edge profilesΒΆ
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
edge_profiles | Edge plasma profiles (includes the scrape-off layer and possibly part of the confined plasma) | |||
edge_profiles.code | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
edge_profiles.code.commit | STR_0D | Unique commit reference of software | ||
edge_profiles.code.description | STR_0D | Short description of the software (type, purpose) | ||
edge_profiles.code.library | [1...N] | STRUCT_ARRAY | List of external libraries used by the code that has produced this IDS | |
edge_profiles.code.library[:].commit | STR_0D | Unique commit reference of software | ||
edge_profiles.code.library[:].description | STR_0D | Short description of the software (type, purpose) | ||
edge_profiles.code.library[:].name | STR_0D | Name of software | ||
edge_profiles.code.library[:].parameters | STR_0D | List of the code specific parameters in XML format | ||
edge_profiles.code.library[:].repository | STR_0D | URL of software repository | ||
edge_profiles.code.library[:].version | STR_0D | Unique version (tag) of software | ||
edge_profiles.code.name | STR_0D | Name of software generating IDS | ||
edge_profiles.code.output_flag | [edge_profiles.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
edge_profiles.code.parameters | STR_0D | List of the code specific parameters in XML format | ||
edge_profiles.code.repository | STR_0D | URL of software repository | ||
edge_profiles.code.version | STR_0D | Unique version (tag) of software | ||
edge_profiles.ggd | [edge_profiles.ggd[:].time] | STRUCT_ARRAY | Edge plasma quantities represented using the general grid description, for various time slices. The timebase of this array of structure must be a subset of the ggd_fast timebase (only if the ggd_fast array of structure is used) | |
edge_profiles.ggd[:].a_field_parallel | [1...N] | STRUCT_ARRAY | T.m | Parallel (to the local magnetic field) component of the magnetic vector potential, given on various grid subsets |
edge_profiles.ggd[:].a_field_parallel[:].coefficients | [edge_profiles.ggd[:].a_field_parallel[:].values, | FLT_2D (uncertain) | T.m | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].a_field_parallel[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].a_field_parallel[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].a_field_parallel[:].values | [1...N] | FLT_1D (uncertain) | T.m | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].e_field | [1...N] | STRUCT_ARRAY | V.m^-1 | Electric field, given on various grid subsets |
edge_profiles.ggd[:].e_field[:].diamagnetic | [1...N] | FLT_1D (uncertain) | V.m^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].e_field[:].diamagnetic_coefficients | [1...N, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].e_field[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].e_field[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].e_field[:].parallel | [1...N] | FLT_1D (uncertain) | V.m^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].e_field[:].parallel_coefficients | [1...N, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].e_field[:].poloidal | [1...N] | FLT_1D (uncertain) | V.m^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].e_field[:].poloidal_coefficients | [1...N, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].e_field[:].r | [1...N] | FLT_1D (uncertain) | V.m^-1 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].e_field[:].r_coefficients | [1...N, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients for the component along the major radius axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].e_field[:].radial | [1...N] | FLT_1D (uncertain) | V.m^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].e_field[:].radial_coefficients | [1...N, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].e_field[:].toroidal | [1...N] | FLT_1D (uncertain) | V.m^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].e_field[:].toroidal_coefficients | [1...N, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].e_field[:].z | [1...N] | FLT_1D (uncertain) | V.m^-1 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].e_field[:].z_coefficients | [1...N, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients for the component along the height axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons | STRUCTURE | Quantities related to the electrons | ||
edge_profiles.ggd[:].electrons.density | [1...N] | STRUCT_ARRAY | m^-3 | Density (thermal+non-thermal), given on various grid subsets |
edge_profiles.ggd[:].electrons.density[:].coefficients | [edge_profiles.ggd[:].electrons.density[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.density[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].electrons.density[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].electrons.density[:].values | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.density_fast | [1...N] | STRUCT_ARRAY | m^-3 | Density of fast (non-thermal) particles, given on various grid subsets |
edge_profiles.ggd[:].electrons.density_fast[:].coefficients | [edge_profiles.ggd[:].electrons.density_fast[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.density_fast[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].electrons.density_fast[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].electrons.density_fast[:].values | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.distribution_function | [1...N] | STRUCT_ARRAY | mixed | Distribution function, given on various grid subsets |
edge_profiles.ggd[:].electrons.distribution_function[:].coefficients | [edge_profiles.ggd[:].electrons.distribution_function[:].values, | FLT_2D (uncertain) | mixed | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.distribution_function[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].electrons.distribution_function[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].electrons.distribution_function[:].values | [1...N] | FLT_1D (uncertain) | mixed | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.pressure | [1...N] | STRUCT_ARRAY | Pa | Pressure, given on various grid subsets |
edge_profiles.ggd[:].electrons.pressure[:].coefficients | [edge_profiles.ggd[:].electrons.pressure[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.pressure[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].electrons.pressure[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].electrons.pressure[:].values | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.pressure_fast_parallel | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) parallel pressure, given on various grid subsets |
edge_profiles.ggd[:].electrons.pressure_fast_parallel[:].coefficients | [edge_profiles.ggd[:].electrons.pressure_fast_parallel[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.pressure_fast_parallel[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].electrons.pressure_fast_parallel[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].electrons.pressure_fast_parallel[:].values | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.pressure_fast_perpendicular | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) perpendicular pressure, given on various grid subsets |
edge_profiles.ggd[:].electrons.pressure_fast_perpendicular[:].coefficients | [edge_profiles.ggd[:].electrons.pressure_fast_perpendicular[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.pressure_fast_perpendicular[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].electrons.pressure_fast_perpendicular[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].electrons.pressure_fast_perpendicular[:].values | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.temperature | [1...N] | STRUCT_ARRAY | eV | Temperature, given on various grid subsets |
edge_profiles.ggd[:].electrons.temperature[:].coefficients | [edge_profiles.ggd[:].electrons.temperature[:].values, | FLT_2D (uncertain) | eV | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.temperature[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].electrons.temperature[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].electrons.temperature[:].values | [1...N] | FLT_1D (uncertain) | eV | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.velocity | [1...N] | STRUCT_ARRAY | m.s^-1 | Velocity, given on various grid subsets |
edge_profiles.ggd[:].electrons.velocity[:].diamagnetic | [1...N] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.velocity[:].diamagnetic_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.velocity[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].electrons.velocity[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].electrons.velocity[:].parallel | [1...N] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.velocity[:].parallel_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.velocity[:].poloidal | [1...N] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.velocity[:].poloidal_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.velocity[:].r | [1...N] | FLT_1D (uncertain) | m.s^-1 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.velocity[:].r_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the component along the major radius axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.velocity[:].radial | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.velocity[:].radial_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.velocity[:].toroidal | [1...N] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.velocity[:].toroidal_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.velocity[:].z | [1...N] | FLT_1D (uncertain) | m.s^-1 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.velocity[:].z_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the component along the height axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion | [1...N] | STRUCT_ARRAY | Quantities related to the different ion species | |
edge_profiles.ggd[:].ion[:].density | [1...N] | STRUCT_ARRAY | m^-3 | Density (thermal+non-thermal) (sum over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].ion[:].density[:].coefficients | [edge_profiles.ggd[:].ion[:].density[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].density[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].density[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].density[:].values | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].density_fast | [1...N] | STRUCT_ARRAY | m^-3 | Density of fast (non-thermal) particles (sum over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].ion[:].density_fast[:].coefficients | [edge_profiles.ggd[:].ion[:].density_fast[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].density_fast[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].density_fast[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].density_fast[:].values | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].element | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
edge_profiles.ggd[:].ion[:].element[:].a | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
edge_profiles.ggd[:].ion[:].element[:].atoms_n | INT_0D | Number of atoms of this element in the molecule | ||
edge_profiles.ggd[:].ion[:].element[:].multiplicity (obsolescent) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
edge_profiles.ggd[:].ion[:].element[:].z_n | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
edge_profiles.ggd[:].ion[:].energy_density_kinetic | [1...N] | STRUCT_ARRAY | J.m^-3 | Kinetic energy density (sum over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].ion[:].energy_density_kinetic[:].coefficients | [edge_profiles.ggd[:].ion[:].energy_density_kinetic[:].values, | FLT_2D (uncertain) | J.m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].energy_density_kinetic[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].energy_density_kinetic[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].energy_density_kinetic[:].values | [1...N] | FLT_1D (uncertain) | J.m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].label | STR_0D | String identifying the species (e.g. H+, D+, T+, He+2, C+, D2, DT, CD4, ...) | ||
edge_profiles.ggd[:].ion[:].multiple_states_flag | INT_0D | Multiple state calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
edge_profiles.ggd[:].ion[:].neutral_index | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
edge_profiles.ggd[:].ion[:].pressure | [1...N] | STRUCT_ARRAY | Pa | Pressure (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].ion[:].pressure[:].coefficients | [edge_profiles.ggd[:].ion[:].pressure[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].pressure[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].pressure[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].pressure[:].values | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].pressure_fast_parallel | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) parallel pressure (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].ion[:].pressure_fast_parallel[:].coefficients | [edge_profiles.ggd[:].ion[:].pressure_fast_parallel[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].pressure_fast_parallel[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].pressure_fast_parallel[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].pressure_fast_parallel[:].values | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].pressure_fast_perpendicular | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) perpendicular pressure (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].ion[:].pressure_fast_perpendicular[:].coefficients | [edge_profiles.ggd[:].ion[:].pressure_fast_perpendicular[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].pressure_fast_perpendicular[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].pressure_fast_perpendicular[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].pressure_fast_perpendicular[:].values | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state | [1...N] | STRUCT_ARRAY | Quantities related to the different states of the species (ionisation, energy, excitation, ...) | |
edge_profiles.ggd[:].ion[:].state[:].density | [1...N] | STRUCT_ARRAY | m^-3 | Density (thermal+non-thermal), given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].density[:].coefficients | [edge_profiles.ggd[:].ion[:].state[:].density[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].density[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].density[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].state[:].density[:].values | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].density_fast | [1...N] | STRUCT_ARRAY | m^-3 | Density of fast (non-thermal) particles, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].density_fast[:].coefficients | [edge_profiles.ggd[:].ion[:].state[:].density_fast[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].density_fast[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].density_fast[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].state[:].density_fast[:].values | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].distribution_function | [1...N] | STRUCT_ARRAY | mixed | Distribution function, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].distribution_function[:].coefficients | [edge_profiles.ggd[:].ion[:].state[:].distribution_function[:].values, | FLT_2D (uncertain) | mixed | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].distribution_function[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].distribution_function[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].state[:].distribution_function[:].values | [1...N] | FLT_1D (uncertain) | mixed | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].electron_configuration | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
edge_profiles.ggd[:].ion[:].state[:].energy_density_kinetic | [1...N] | STRUCT_ARRAY | J.m^-3 | Kinetic energy density, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].energy_density_kinetic[:].coefficients | [edge_profiles.ggd[:].ion[:].state[:].energy_density_kinetic[:].values, | FLT_2D (uncertain) | J.m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].energy_density_kinetic[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].energy_density_kinetic[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].state[:].energy_density_kinetic[:].values | [1...N] | FLT_1D (uncertain) | J.m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].ionisation_potential | [1...N] | STRUCT_ARRAY | Elementary Charge Unit | Cumulative and average ionisation potential to reach a given bundle. Defined as sum (x_z* (sum of Epot from z'=0 to z-1)), where Epot is the ionisation potential of ion Xz_+, and x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].ionisation_potential[:].coefficients | [edge_profiles.ggd[:].ion[:].state[:].ionisation_potential[:].values, | FLT_2D (uncertain) | Elementary Charge Unit | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].ionisation_potential[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].ionisation_potential[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].state[:].ionisation_potential[:].values | [1...N] | FLT_1D (uncertain) | Elementary Charge Unit | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].label | STR_0D | String identifying state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
edge_profiles.ggd[:].ion[:].state[:].pressure | [1...N] | STRUCT_ARRAY | Pa | Pressure, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].pressure[:].coefficients | [edge_profiles.ggd[:].ion[:].state[:].pressure[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].pressure[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].pressure[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].state[:].pressure[:].values | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_parallel | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) parallel pressure, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_parallel[:].coefficients | [edge_profiles.ggd[:].ion[:].state[:].pressure_fast_parallel[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_parallel[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_parallel[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_parallel[:].values | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_perpendicular | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) perpendicular pressure, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_perpendicular[:].coefficients | [edge_profiles.ggd[:].ion[:].state[:].pressure_fast_perpendicular[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_perpendicular[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_perpendicular[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_perpendicular[:].values | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].temperature | [1...N] | STRUCT_ARRAY | eV | Temperature, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].temperature[:].coefficients | [edge_profiles.ggd[:].ion[:].state[:].temperature[:].values, | FLT_2D (uncertain) | eV | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].temperature[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].temperature[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].state[:].temperature[:].values | [1...N] | FLT_1D (uncertain) | eV | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity | [1...N] | STRUCT_ARRAY | m.s^-1 | Velocity, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].diamagnetic | [1...N] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].diamagnetic_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].velocity[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].state[:].velocity[:].parallel | [1...N] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].parallel_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].poloidal | [1...N] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].poloidal_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].r | [1...N] | FLT_1D (uncertain) | m.s^-1 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].r_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the component along the major radius axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].radial | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].radial_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].toroidal | [1...N] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].toroidal_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].z | [1...N] | FLT_1D (uncertain) | m.s^-1 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].z_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the component along the height axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic | [1...N] | STRUCT_ARRAY | m.s^-1 | Velocity due to the diamagnetic drift, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].diamagnetic | [1...N] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].diamagnetic_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].parallel | [1...N] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].parallel_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].poloidal | [1...N] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].poloidal_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].r | [1...N] | FLT_1D (uncertain) | m.s^-1 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].r_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the component along the major radius axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].radial | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].radial_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].toroidal | [1...N] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].toroidal_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].z | [1...N] | FLT_1D (uncertain) | m.s^-1 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].z_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the component along the height axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb | [1...N] | STRUCT_ARRAY | m.s^-1 | Velocity due to the ExB drift, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].diamagnetic | [1...N] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].diamagnetic_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].parallel | [1...N] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].parallel_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].poloidal | [1...N] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].poloidal_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].r | [1...N] | FLT_1D (uncertain) | m.s^-1 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].r_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the component along the major radius axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].radial | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].radial_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].toroidal | [1...N] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].toroidal_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].z | [1...N] | FLT_1D (uncertain) | m.s^-1 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].z_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the component along the height axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].vibrational_level | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
edge_profiles.ggd[:].ion[:].state[:].vibrational_mode | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
edge_profiles.ggd[:].ion[:].state[:].z_average | [1...N] | STRUCT_ARRAY | Elementary Charge Unit | Average Z of the state bundle (equal to z_min if no bundle), = sum (Z*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].z_average[:].coefficients | [edge_profiles.ggd[:].ion[:].state[:].z_average[:].values, | FLT_2D (uncertain) | Elementary Charge Unit | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].z_average[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].z_average[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].state[:].z_average[:].values | [1...N] | FLT_1D (uncertain) | Elementary Charge Unit | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].z_max | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the state bundle (equal to z_min if no bundle) | |
edge_profiles.ggd[:].ion[:].state[:].z_min | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the state bundle (z_min = z_max = 0 for a neutral) | |
edge_profiles.ggd[:].ion[:].state[:].z_square_average | [1...N] | STRUCT_ARRAY | Elementary Charge Unit | Average Z square of the state bundle (equal to z_min if no bundle), = sum (Z^2*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].z_square_average[:].coefficients | [edge_profiles.ggd[:].ion[:].state[:].z_square_average[:].values, | FLT_2D (uncertain) | Elementary Charge Unit | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].z_square_average[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].z_square_average[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].state[:].z_square_average[:].values | [1...N] | FLT_1D (uncertain) | Elementary Charge Unit | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].temperature | [1...N] | STRUCT_ARRAY | eV | Temperature (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].ion[:].temperature[:].coefficients | [edge_profiles.ggd[:].ion[:].temperature[:].values, | FLT_2D (uncertain) | eV | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].temperature[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].temperature[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].temperature[:].values | [1...N] | FLT_1D (uncertain) | eV | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].velocity | [1...N] | STRUCT_ARRAY | m.s^-1 | Velocity (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].ion[:].velocity[:].diamagnetic | [1...N] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].velocity[:].diamagnetic_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].velocity[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].velocity[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].ion[:].velocity[:].parallel | [1...N] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].velocity[:].parallel_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].velocity[:].poloidal | [1...N] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].velocity[:].poloidal_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].velocity[:].r | [1...N] | FLT_1D (uncertain) | m.s^-1 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].velocity[:].r_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the component along the major radius axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].velocity[:].radial | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].velocity[:].radial_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].velocity[:].toroidal | [1...N] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].velocity[:].toroidal_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].velocity[:].z | [1...N] | FLT_1D (uncertain) | m.s^-1 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].velocity[:].z_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the component along the height axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].z_ion | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed). | |
edge_profiles.ggd[:].j_anomalous | [1...N] | STRUCT_ARRAY | A.m^-2 | Anomalous current density, given on various grid subsets |
edge_profiles.ggd[:].j_anomalous[:].diamagnetic | [1...N] | FLT_1D (uncertain) | A.m^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_anomalous[:].diamagnetic_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_anomalous[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].j_anomalous[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].j_anomalous[:].parallel | [1...N] | FLT_1D (uncertain) | A.m^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_anomalous[:].parallel_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_anomalous[:].poloidal | [1...N] | FLT_1D (uncertain) | A.m^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_anomalous[:].poloidal_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_anomalous[:].r | [1...N] | FLT_1D (uncertain) | A.m^-2 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_anomalous[:].r_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the component along the major radius axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_anomalous[:].radial | [1...N] | FLT_1D (uncertain) | A.m^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_anomalous[:].radial_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_anomalous[:].toroidal | [1...N] | FLT_1D (uncertain) | A.m^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_anomalous[:].toroidal_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_anomalous[:].z | [1...N] | FLT_1D (uncertain) | A.m^-2 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_anomalous[:].z_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the component along the height axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_diamagnetic | [1...N] | STRUCT_ARRAY | A.m^-2 | Current density due to the diamgnetic drift, given on various grid subsets |
edge_profiles.ggd[:].j_diamagnetic[:].diamagnetic | [1...N] | FLT_1D (uncertain) | A.m^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_diamagnetic[:].diamagnetic_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_diamagnetic[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].j_diamagnetic[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].j_diamagnetic[:].parallel | [1...N] | FLT_1D (uncertain) | A.m^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_diamagnetic[:].parallel_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_diamagnetic[:].poloidal | [1...N] | FLT_1D (uncertain) | A.m^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_diamagnetic[:].poloidal_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_diamagnetic[:].r | [1...N] | FLT_1D (uncertain) | A.m^-2 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_diamagnetic[:].r_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the component along the major radius axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_diamagnetic[:].radial | [1...N] | FLT_1D (uncertain) | A.m^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_diamagnetic[:].radial_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_diamagnetic[:].toroidal | [1...N] | FLT_1D (uncertain) | A.m^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_diamagnetic[:].toroidal_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_diamagnetic[:].z | [1...N] | FLT_1D (uncertain) | A.m^-2 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_diamagnetic[:].z_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the component along the height axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_heat_viscosity | [1...N] | STRUCT_ARRAY | A.m^-2 | Current density due to the heat viscosity, given on various grid subsets |
edge_profiles.ggd[:].j_heat_viscosity[:].diamagnetic | [1...N] | FLT_1D (uncertain) | A.m^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_heat_viscosity[:].diamagnetic_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_heat_viscosity[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].j_heat_viscosity[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].j_heat_viscosity[:].parallel | [1...N] | FLT_1D (uncertain) | A.m^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_heat_viscosity[:].parallel_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_heat_viscosity[:].poloidal | [1...N] | FLT_1D (uncertain) | A.m^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_heat_viscosity[:].poloidal_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_heat_viscosity[:].r | [1...N] | FLT_1D (uncertain) | A.m^-2 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_heat_viscosity[:].r_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the component along the major radius axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_heat_viscosity[:].radial | [1...N] | FLT_1D (uncertain) | A.m^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_heat_viscosity[:].radial_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_heat_viscosity[:].toroidal | [1...N] | FLT_1D (uncertain) | A.m^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_heat_viscosity[:].toroidal_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_heat_viscosity[:].z | [1...N] | FLT_1D (uncertain) | A.m^-2 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_heat_viscosity[:].z_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the component along the height axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_inertial | [1...N] | STRUCT_ARRAY | A.m^-2 | Inertial current density, given on various grid subsets |
edge_profiles.ggd[:].j_inertial[:].diamagnetic | [1...N] | FLT_1D (uncertain) | A.m^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_inertial[:].diamagnetic_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_inertial[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].j_inertial[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].j_inertial[:].parallel | [1...N] | FLT_1D (uncertain) | A.m^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_inertial[:].parallel_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_inertial[:].poloidal | [1...N] | FLT_1D (uncertain) | A.m^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_inertial[:].poloidal_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_inertial[:].r | [1...N] | FLT_1D (uncertain) | A.m^-2 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_inertial[:].r_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the component along the major radius axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_inertial[:].radial | [1...N] | FLT_1D (uncertain) | A.m^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_inertial[:].radial_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_inertial[:].toroidal | [1...N] | FLT_1D (uncertain) | A.m^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_inertial[:].toroidal_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_inertial[:].z | [1...N] | FLT_1D (uncertain) | A.m^-2 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_inertial[:].z_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the component along the height axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_ion_neutral_friction | [1...N] | STRUCT_ARRAY | A.m^-2 | Current density due to ion neutral friction, given on various grid subsets |
edge_profiles.ggd[:].j_ion_neutral_friction[:].diamagnetic | [1...N] | FLT_1D (uncertain) | A.m^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_ion_neutral_friction[:].diamagnetic_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_ion_neutral_friction[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].j_ion_neutral_friction[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].j_ion_neutral_friction[:].parallel | [1...N] | FLT_1D (uncertain) | A.m^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_ion_neutral_friction[:].parallel_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_ion_neutral_friction[:].poloidal | [1...N] | FLT_1D (uncertain) | A.m^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_ion_neutral_friction[:].poloidal_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_ion_neutral_friction[:].r | [1...N] | FLT_1D (uncertain) | A.m^-2 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_ion_neutral_friction[:].r_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the component along the major radius axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_ion_neutral_friction[:].radial | [1...N] | FLT_1D (uncertain) | A.m^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_ion_neutral_friction[:].radial_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_ion_neutral_friction[:].toroidal | [1...N] | FLT_1D (uncertain) | A.m^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_ion_neutral_friction[:].toroidal_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_ion_neutral_friction[:].z | [1...N] | FLT_1D (uncertain) | A.m^-2 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_ion_neutral_friction[:].z_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the component along the height axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_parallel | [1...N] | STRUCT_ARRAY | A.m^-2 | Current due to parallel electric and thermo-electric conductivity and potential and electron temperature gradients along the field line, differences away from ambipolar flow in the parallel direction between ions and electrons (this is not the parallel component of j_total) |
edge_profiles.ggd[:].j_parallel[:].coefficients | [edge_profiles.ggd[:].j_parallel[:].values, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_parallel[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].j_parallel[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].j_parallel[:].values | [1...N] | FLT_1D (uncertain) | A.m^-2 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_parallel_viscosity | [1...N] | STRUCT_ARRAY | A.m^-2 | Current density due to the parallel viscosity, given on various grid subsets |
edge_profiles.ggd[:].j_parallel_viscosity[:].diamagnetic | [1...N] | FLT_1D (uncertain) | A.m^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_parallel_viscosity[:].diamagnetic_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_parallel_viscosity[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].j_parallel_viscosity[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].j_parallel_viscosity[:].parallel | [1...N] | FLT_1D (uncertain) | A.m^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_parallel_viscosity[:].parallel_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_parallel_viscosity[:].poloidal | [1...N] | FLT_1D (uncertain) | A.m^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_parallel_viscosity[:].poloidal_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_parallel_viscosity[:].r | [1...N] | FLT_1D (uncertain) | A.m^-2 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_parallel_viscosity[:].r_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the component along the major radius axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_parallel_viscosity[:].radial | [1...N] | FLT_1D (uncertain) | A.m^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_parallel_viscosity[:].radial_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_parallel_viscosity[:].toroidal | [1...N] | FLT_1D (uncertain) | A.m^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_parallel_viscosity[:].toroidal_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_parallel_viscosity[:].z | [1...N] | FLT_1D (uncertain) | A.m^-2 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_parallel_viscosity[:].z_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the component along the height axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_perpendicular_viscosity | [1...N] | STRUCT_ARRAY | A.m^-2 | Current density due to the perpendicular viscosity, given on various grid subsets |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].diamagnetic | [1...N] | FLT_1D (uncertain) | A.m^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].diamagnetic_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].j_perpendicular_viscosity[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].j_perpendicular_viscosity[:].parallel | [1...N] | FLT_1D (uncertain) | A.m^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].parallel_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].poloidal | [1...N] | FLT_1D (uncertain) | A.m^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].poloidal_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].r | [1...N] | FLT_1D (uncertain) | A.m^-2 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].r_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the component along the major radius axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].radial | [1...N] | FLT_1D (uncertain) | A.m^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].radial_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].toroidal | [1...N] | FLT_1D (uncertain) | A.m^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].toroidal_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].z | [1...N] | FLT_1D (uncertain) | A.m^-2 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].z_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the component along the height axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_pfirsch_schlueter | [1...N] | STRUCT_ARRAY | A.m^-2 | Current density due to Pfirsch-SchlΓΌter effects, given on various grid subsets |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].diamagnetic | [1...N] | FLT_1D (uncertain) | A.m^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].diamagnetic_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].j_pfirsch_schlueter[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].j_pfirsch_schlueter[:].parallel | [1...N] | FLT_1D (uncertain) | A.m^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].parallel_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].poloidal | [1...N] | FLT_1D (uncertain) | A.m^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].poloidal_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].r | [1...N] | FLT_1D (uncertain) | A.m^-2 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].r_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the component along the major radius axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].radial | [1...N] | FLT_1D (uncertain) | A.m^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].radial_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].toroidal | [1...N] | FLT_1D (uncertain) | A.m^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].toroidal_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].z | [1...N] | FLT_1D (uncertain) | A.m^-2 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].z_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the component along the height axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_total | [1...N] | STRUCT_ARRAY | A.m^-2 | Total current density, given on various grid subsets |
edge_profiles.ggd[:].j_total[:].diamagnetic | [1...N] | FLT_1D (uncertain) | A.m^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_total[:].diamagnetic_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_total[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].j_total[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].j_total[:].parallel | [1...N] | FLT_1D (uncertain) | A.m^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_total[:].parallel_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_total[:].poloidal | [1...N] | FLT_1D (uncertain) | A.m^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_total[:].poloidal_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_total[:].r | [1...N] | FLT_1D (uncertain) | A.m^-2 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_total[:].r_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the component along the major radius axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_total[:].radial | [1...N] | FLT_1D (uncertain) | A.m^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_total[:].radial_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_total[:].toroidal | [1...N] | FLT_1D (uncertain) | A.m^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_total[:].toroidal_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_total[:].z | [1...N] | FLT_1D (uncertain) | A.m^-2 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_total[:].z_coefficients | [1...N, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the component along the height axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].n_i_total_over_n_e | [1...N] | STRUCT_ARRAY | - | Ratio of total ion density (sum over ion species) over electron density. (thermal+non-thermal), given on various grid subsets |
edge_profiles.ggd[:].n_i_total_over_n_e[:].coefficients | [edge_profiles.ggd[:].n_i_total_over_n_e[:].values, | FLT_2D (uncertain) | - | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].n_i_total_over_n_e[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].n_i_total_over_n_e[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].n_i_total_over_n_e[:].values | [1...N] | FLT_1D (uncertain) | - | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral | [1...N] | STRUCT_ARRAY | Quantities related to the different neutral species | |
edge_profiles.ggd[:].neutral[:].density | [1...N] | STRUCT_ARRAY | m^-3 | Density (thermal+non-thermal) (sum over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].neutral[:].density[:].coefficients | [edge_profiles.ggd[:].neutral[:].density[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].density[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].density[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].neutral[:].density[:].values | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].density_fast | [1...N] | STRUCT_ARRAY | m^-3 | Density of fast (non-thermal) particles (sum over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].neutral[:].density_fast[:].coefficients | [edge_profiles.ggd[:].neutral[:].density_fast[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].density_fast[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].density_fast[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].neutral[:].density_fast[:].values | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].element | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
edge_profiles.ggd[:].neutral[:].element[:].a | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
edge_profiles.ggd[:].neutral[:].element[:].atoms_n | INT_0D | Number of atoms of this element in the molecule | ||
edge_profiles.ggd[:].neutral[:].element[:].multiplicity (obsolescent) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
edge_profiles.ggd[:].neutral[:].element[:].z_n | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
edge_profiles.ggd[:].neutral[:].energy_density_kinetic | [1...N] | STRUCT_ARRAY | J.m^-3 | Kinetic energy density (sum over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].neutral[:].energy_density_kinetic[:].coefficients | [edge_profiles.ggd[:].neutral[:].energy_density_kinetic[:].values, | FLT_2D (uncertain) | J.m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].energy_density_kinetic[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].energy_density_kinetic[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].neutral[:].energy_density_kinetic[:].values | [1...N] | FLT_1D (uncertain) | J.m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].ion_index | INT_0D | Index of the corresponding ion species in the ../../ion array | ||
edge_profiles.ggd[:].neutral[:].label | STR_0D | String identifying the species (e.g. H, D, T, He, C, D2, DT, CD4, ...) | ||
edge_profiles.ggd[:].neutral[:].multiple_states_flag | INT_0D | Multiple state calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
edge_profiles.ggd[:].neutral[:].pressure | [1...N] | STRUCT_ARRAY | Pa | Pressure (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].neutral[:].pressure[:].coefficients | [edge_profiles.ggd[:].neutral[:].pressure[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].pressure[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].pressure[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].neutral[:].pressure[:].values | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].pressure_fast_parallel | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) parallel pressure (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].neutral[:].pressure_fast_parallel[:].coefficients | [edge_profiles.ggd[:].neutral[:].pressure_fast_parallel[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].pressure_fast_parallel[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].pressure_fast_parallel[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].neutral[:].pressure_fast_parallel[:].values | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].pressure_fast_perpendicular | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) perpendicular pressure (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].neutral[:].pressure_fast_perpendicular[:].coefficients | [edge_profiles.ggd[:].neutral[:].pressure_fast_perpendicular[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].pressure_fast_perpendicular[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].pressure_fast_perpendicular[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].neutral[:].pressure_fast_perpendicular[:].values | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state | [1...N] | STRUCT_ARRAY | Quantities related to the different states of the species (energy, excitation, ...) | |
edge_profiles.ggd[:].neutral[:].state[:].density | [1...N] | STRUCT_ARRAY | m^-3 | Density (thermal+non-thermal), given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].density[:].coefficients | [edge_profiles.ggd[:].neutral[:].state[:].density[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].density[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].density[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].neutral[:].state[:].density[:].values | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].density_fast | [1...N] | STRUCT_ARRAY | m^-3 | Density of fast (non-thermal) particles, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].density_fast[:].coefficients | [edge_profiles.ggd[:].neutral[:].state[:].density_fast[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].density_fast[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].density_fast[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].neutral[:].state[:].density_fast[:].values | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].distribution_function | [1...N] | STRUCT_ARRAY | mixed | Distribution function, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].distribution_function[:].coefficients | [edge_profiles.ggd[:].neutral[:].state[:].distribution_function[:].values, | FLT_2D (uncertain) | mixed | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].distribution_function[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].distribution_function[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].neutral[:].state[:].distribution_function[:].values | [1...N] | FLT_1D (uncertain) | mixed | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].electron_configuration | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
edge_profiles.ggd[:].neutral[:].state[:].energy_density_kinetic | [1...N] | STRUCT_ARRAY | J.m^-3 | Kinetic energy density, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].energy_density_kinetic[:].coefficients | [edge_profiles.ggd[:].neutral[:].state[:].energy_density_kinetic[:].values, | FLT_2D (uncertain) | J.m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].energy_density_kinetic[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].energy_density_kinetic[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].neutral[:].state[:].energy_density_kinetic[:].values | [1...N] | FLT_1D (uncertain) | J.m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].label | STR_0D | String identifying state | ||
edge_profiles.ggd[:].neutral[:].state[:].neutral_type | STRUCTURE | Neutral type, in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI | ||
edge_profiles.ggd[:].neutral[:].state[:].neutral_type.description | STR_0D | Verbose description | ||
edge_profiles.ggd[:].neutral[:].state[:].neutral_type.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_profiles.ggd[:].neutral[:].state[:].neutral_type.name | STR_0D | Short string identifier | ||
edge_profiles.ggd[:].neutral[:].state[:].pressure | [1...N] | STRUCT_ARRAY | Pa | Pressure, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].pressure[:].coefficients | [edge_profiles.ggd[:].neutral[:].state[:].pressure[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].pressure[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].pressure[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].neutral[:].state[:].pressure[:].values | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_parallel | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) parallel pressure, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_parallel[:].coefficients | [edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_parallel[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_parallel[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_parallel[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_parallel[:].values | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_perpendicular | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) perpendicular pressure, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_perpendicular[:].coefficients | [edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_perpendicular[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_perpendicular[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_perpendicular[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_perpendicular[:].values | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].temperature | [1...N] | STRUCT_ARRAY | eV | Temperature, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].temperature[:].coefficients | [edge_profiles.ggd[:].neutral[:].state[:].temperature[:].values, | FLT_2D (uncertain) | eV | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].temperature[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].temperature[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].neutral[:].state[:].temperature[:].values | [1...N] | FLT_1D (uncertain) | eV | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity | [1...N] | STRUCT_ARRAY | m.s^-1 | Velocity, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].diamagnetic | [1...N] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].diamagnetic_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].parallel | [1...N] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].parallel_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].poloidal | [1...N] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].poloidal_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].r | [1...N] | FLT_1D (uncertain) | m.s^-1 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].r_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the component along the major radius axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].radial | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].radial_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].toroidal | [1...N] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].toroidal_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].z | [1...N] | FLT_1D (uncertain) | m.s^-1 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].z_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the component along the height axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic | [1...N] | STRUCT_ARRAY | m.s^-1 | Velocity due to the diamagnetic drift, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].diamagnetic | [1...N] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].diamagnetic_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].parallel | [1...N] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].parallel_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].poloidal | [1...N] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].poloidal_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].r | [1...N] | FLT_1D (uncertain) | m.s^-1 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].r_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the component along the major radius axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].radial | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].radial_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].toroidal | [1...N] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].toroidal_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].z | [1...N] | FLT_1D (uncertain) | m.s^-1 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].z_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the component along the height axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb | [1...N] | STRUCT_ARRAY | m.s^-1 | Velocity due to the ExB drift, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].diamagnetic | [1...N] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].diamagnetic_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].parallel | [1...N] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].parallel_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].poloidal | [1...N] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].poloidal_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].r | [1...N] | FLT_1D (uncertain) | m.s^-1 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].r_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the component along the major radius axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].radial | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].radial_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].toroidal | [1...N] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].toroidal_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].z | [1...N] | FLT_1D (uncertain) | m.s^-1 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].z_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the component along the height axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].vibrational_level | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
edge_profiles.ggd[:].neutral[:].state[:].vibrational_mode | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
edge_profiles.ggd[:].neutral[:].temperature | [1...N] | STRUCT_ARRAY | eV | Temperature (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].neutral[:].temperature[:].coefficients | [edge_profiles.ggd[:].neutral[:].temperature[:].values, | FLT_2D (uncertain) | eV | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].temperature[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].temperature[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].neutral[:].temperature[:].values | [1...N] | FLT_1D (uncertain) | eV | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].velocity | [1...N] | STRUCT_ARRAY | m.s^-1 | Velocity (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].neutral[:].velocity[:].diamagnetic | [1...N] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].velocity[:].diamagnetic_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].velocity[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].velocity[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].neutral[:].velocity[:].parallel | [1...N] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].velocity[:].parallel_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].velocity[:].poloidal | [1...N] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].velocity[:].poloidal_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].velocity[:].r | [1...N] | FLT_1D (uncertain) | m.s^-1 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].velocity[:].r_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the component along the major radius axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].velocity[:].radial | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].velocity[:].radial_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].velocity[:].toroidal | [1...N] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].velocity[:].toroidal_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].velocity[:].z | [1...N] | FLT_1D (uncertain) | m.s^-1 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].velocity[:].z_coefficients | [1...N, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the component along the height axis, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].phi_potential | [1...N] | STRUCT_ARRAY | V | Electric potential, given on various grid subsets |
edge_profiles.ggd[:].phi_potential[:].coefficients | [edge_profiles.ggd[:].phi_potential[:].values, | FLT_2D (uncertain) | V | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].phi_potential[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].phi_potential[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].phi_potential[:].values | [1...N] | FLT_1D (uncertain) | V | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].pressure_parallel | [1...N] | STRUCT_ARRAY | Pa | Total parallel pressure (electrons+ions, thermal+non-thermal), given on various grid subsets |
edge_profiles.ggd[:].pressure_parallel[:].coefficients | [edge_profiles.ggd[:].pressure_parallel[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].pressure_parallel[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].pressure_parallel[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].pressure_parallel[:].values | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].pressure_perpendicular | [1...N] | STRUCT_ARRAY | Pa | Total perpendicular pressure (electrons+ions, thermal+non-thermal), given on various grid subsets |
edge_profiles.ggd[:].pressure_perpendicular[:].coefficients | [edge_profiles.ggd[:].pressure_perpendicular[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].pressure_perpendicular[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].pressure_perpendicular[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].pressure_perpendicular[:].values | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].pressure_thermal | [1...N] | STRUCT_ARRAY | Pa | Thermal pressure (electrons+ions), given on various grid subsets |
edge_profiles.ggd[:].pressure_thermal[:].coefficients | [edge_profiles.ggd[:].pressure_thermal[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].pressure_thermal[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].pressure_thermal[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].pressure_thermal[:].values | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].t_i_average | [1...N] | STRUCT_ARRAY | eV | Ion temperature (averaged on ion species), given on various grid subsets |
edge_profiles.ggd[:].t_i_average[:].coefficients | [edge_profiles.ggd[:].t_i_average[:].values, | FLT_2D (uncertain) | eV | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].t_i_average[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].t_i_average[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].t_i_average[:].values | [1...N] | FLT_1D (uncertain) | eV | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].time | FLT_0D | s | Time | |
edge_profiles.ggd[:].zeff | [1...N] | STRUCT_ARRAY | - | Effective charge, given on various grid subsets |
edge_profiles.ggd[:].zeff[:].coefficients | [edge_profiles.ggd[:].zeff[:].values, | FLT_2D (uncertain) | - | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].zeff[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].zeff[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd[:].zeff[:].values | [1...N] | FLT_1D (uncertain) | - | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd_fast | [edge_profiles.ggd_fast[:].time] | STRUCT_ARRAY | Quantities provided at a faster sampling rate than the full ggd quantities. These are either integrated quantities or local quantities provided on a reduced set of positions. Positions and integration domains are described by a set of grid_subsets (of size 1 for a position). | |
edge_profiles.ggd_fast[:].electrons | STRUCTURE | Quantities related to the electrons | ||
edge_profiles.ggd_fast[:].electrons.density | [1...N] | STRUCT_ARRAY | m^-3 | Density (thermal+non-thermal), given at various positions (grid subset of size 1) |
edge_profiles.ggd_fast[:].electrons.density[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd_fast[:].electrons.density[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd_fast[:].electrons.density[:].value | FLT_0D (uncertain) | m^-3 | Scalar value of the quantity on the grid subset (corresponding to a single local position or to an integrated value over the subset) | |
edge_profiles.ggd_fast[:].electrons.temperature | [1...N] | STRUCT_ARRAY | eV | Temperature, given at various positions (grid subset of size 1) |
edge_profiles.ggd_fast[:].electrons.temperature[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd_fast[:].electrons.temperature[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd_fast[:].electrons.temperature[:].value | FLT_0D (uncertain) | eV | Scalar value of the quantity on the grid subset (corresponding to a single local position or to an integrated value over the subset) | |
edge_profiles.ggd_fast[:].energy_thermal | [1...N] | STRUCT_ARRAY | J | Plasma energy content = 3/2 * integral over the volume of the grid subset of the thermal pressure (summed over all species), for various grid subsets |
edge_profiles.ggd_fast[:].energy_thermal[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd_fast[:].energy_thermal[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd_fast[:].energy_thermal[:].value | FLT_0D (uncertain) | J | Scalar value of the quantity on the grid subset (corresponding to a single local position or to an integrated value over the subset) | |
edge_profiles.ggd_fast[:].ion | [1...N] | STRUCT_ARRAY | Quantities related to the different ion species | |
edge_profiles.ggd_fast[:].ion[:].content | [1...N] | STRUCT_ARRAY | - | Particle content = total number of particles for this ion species in the volume of the grid subset, for various grid subsets |
edge_profiles.ggd_fast[:].ion[:].content[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd_fast[:].ion[:].content[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd_fast[:].ion[:].content[:].value | FLT_0D (uncertain) | - | Scalar value of the quantity on the grid subset (corresponding to a single local position or to an integrated value over the subset) | |
edge_profiles.ggd_fast[:].ion[:].density | [1...N] | STRUCT_ARRAY | m^-3 | Density (thermal+non-thermal) (sum over states when multiple states are considered), given at various positions (grid subset of size 1) |
edge_profiles.ggd_fast[:].ion[:].density[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd_fast[:].ion[:].density[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd_fast[:].ion[:].density[:].value | FLT_0D (uncertain) | m^-3 | Scalar value of the quantity on the grid subset (corresponding to a single local position or to an integrated value over the subset) | |
edge_profiles.ggd_fast[:].ion[:].element | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
edge_profiles.ggd_fast[:].ion[:].element[:].a | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
edge_profiles.ggd_fast[:].ion[:].element[:].atoms_n | INT_0D | Number of atoms of this element in the molecule | ||
edge_profiles.ggd_fast[:].ion[:].element[:].multiplicity (obsolescent) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
edge_profiles.ggd_fast[:].ion[:].element[:].z_n | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
edge_profiles.ggd_fast[:].ion[:].label | STR_0D | String identifying the species (e.g. H+, D+, T+, He+2, C+, D2, DT, CD4, ...) | ||
edge_profiles.ggd_fast[:].ion[:].neutral_index | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
edge_profiles.ggd_fast[:].ion[:].temperature | [1...N] | STRUCT_ARRAY | eV | Temperature (average over states when multiple states are considered), given at various positions (grid subset of size 1) |
edge_profiles.ggd_fast[:].ion[:].temperature[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd_fast[:].ion[:].temperature[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.ggd_fast[:].ion[:].temperature[:].value | FLT_0D (uncertain) | eV | Scalar value of the quantity on the grid subset (corresponding to a single local position or to an integrated value over the subset) | |
edge_profiles.ggd_fast[:].ion[:].z_ion | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed). | |
edge_profiles.ggd_fast[:].time | FLT_0D | s | Time | |
edge_profiles.grid_ggd | [edge_profiles.grid_ggd[:].time] | STRUCT_ARRAY | Grid (using the Generic Grid Description), for various time slices. The timebase of this array of structure must be a subset of the ggd timebase | |
edge_profiles.grid_ggd[:].grid_subset | [1...N] | STRUCT_ARRAY | Grid subsets | |
edge_profiles.grid_ggd[:].grid_subset[:].base | [1...N] | STRUCT_ARRAY | Set of bases for the grid subset. For each base, the structure describes the projection of the base vectors on the canonical frame of the grid. | |
edge_profiles.grid_ggd[:].grid_subset[:].base[:].jacobian | [edge_profiles.grid_ggd[:].grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
edge_profiles.grid_ggd[:].grid_subset[:].base[:].tensor_contravariant | [edge_profiles.grid_ggd[:].grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
edge_profiles.grid_ggd[:].grid_subset[:].base[:].tensor_covariant | [edge_profiles.grid_ggd[:].grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
edge_profiles.grid_ggd[:].grid_subset[:].dimension | INT_0D | Space dimension of the grid subset elements. This must be equal to the sum of the dimensions of the individual objects forming the element. | ||
edge_profiles.grid_ggd[:].grid_subset[:].element | [1...N] | STRUCT_ARRAY | Set of elements defining the grid subset. An element is defined by a combination of objects from potentially all spaces | |
edge_profiles.grid_ggd[:].grid_subset[:].element[:].object | [1...N] | STRUCT_ARRAY | Set of objects defining the element | |
edge_profiles.grid_ggd[:].grid_subset[:].element[:].object[:].dimension | INT_0D | Dimension of the object | ||
edge_profiles.grid_ggd[:].grid_subset[:].element[:].object[:].index | INT_0D | Object index | ||
edge_profiles.grid_ggd[:].grid_subset[:].element[:].object[:].space | INT_0D | Index of the space from which that object is taken | ||
edge_profiles.grid_ggd[:].grid_subset[:].identifier | STRUCTURE | Grid subset identifier | ||
edge_profiles.grid_ggd[:].grid_subset[:].identifier.description | STR_0D | Verbose description | ||
edge_profiles.grid_ggd[:].grid_subset[:].identifier.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_profiles.grid_ggd[:].grid_subset[:].identifier.name | STR_0D | Short string identifier | ||
edge_profiles.grid_ggd[:].grid_subset[:].metric | STRUCTURE | Metric of the canonical frame onto Cartesian coordinates | ||
edge_profiles.grid_ggd[:].grid_subset[:].metric.jacobian | [edge_profiles.grid_ggd[:].grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
edge_profiles.grid_ggd[:].grid_subset[:].metric.tensor_contravariant | [edge_profiles.grid_ggd[:].grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
edge_profiles.grid_ggd[:].grid_subset[:].metric.tensor_covariant | [edge_profiles.grid_ggd[:].grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
edge_profiles.grid_ggd[:].identifier | STRUCTURE | Grid identifier | ||
edge_profiles.grid_ggd[:].identifier.description | STR_0D | Verbose description | ||
edge_profiles.grid_ggd[:].identifier.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_profiles.grid_ggd[:].identifier.name | STR_0D | Short string identifier | ||
edge_profiles.grid_ggd[:].path | STR_0D | Path of the grid, including the IDS name, in case of implicit reference to a grid_ggd node described in another IDS. To be filled only if the grid is not described explicitly in this grid_ggd structure. Example syntax: IDS::wall/0/description_ggd(1)/grid_ggd, means that the grid is located in the wall IDS, occurrence 0, with relative path description_ggd(1)/grid_ggd, using Fortran index convention (here : first index of the array) | ||
edge_profiles.grid_ggd[:].space | [1...N] | STRUCT_ARRAY | Set of grid spaces | |
edge_profiles.grid_ggd[:].space[:].coordinates_type | [1...N] | INT_1D | Type of coordinates describing the physical space, for every coordinate of the space. The size of this node therefore defines the dimension of the space. The meaning of these predefined integer constants can be found in the Data Dictionary under utilities/coordinate_identifier.xml | |
edge_profiles.grid_ggd[:].space[:].geometry_type | STRUCTURE | Type of space geometry (0: standard, 1:Fourier, >1: Fourier with periodicity) | ||
edge_profiles.grid_ggd[:].space[:].geometry_type.description | STR_0D | Verbose description | ||
edge_profiles.grid_ggd[:].space[:].geometry_type.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_profiles.grid_ggd[:].space[:].geometry_type.name | STR_0D | Short string identifier | ||
edge_profiles.grid_ggd[:].space[:].identifier | STRUCTURE | Space identifier | ||
edge_profiles.grid_ggd[:].space[:].identifier.description | STR_0D | Verbose description | ||
edge_profiles.grid_ggd[:].space[:].identifier.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_profiles.grid_ggd[:].space[:].identifier.name | STR_0D | Short string identifier | ||
edge_profiles.grid_ggd[:].space[:].objects_per_dimension | [1...N] | STRUCT_ARRAY | Definition of the space objects for every dimension (from one to the dimension of the highest-dimensional objects). The index correspond to 1=nodes, 2=edges, 3=faces, 4=cells/volumes, .... For every index, a collection of objects of that dimension is described. | |
edge_profiles.grid_ggd[:].space[:].objects_per_dimension[:].geometry_content | STRUCTURE | Content of the ../object/geometry node for this dimension | ||
edge_profiles.grid_ggd[:].space[:].objects_per_dimension[:].geometry_content.description | STR_0D | Verbose description | ||
edge_profiles.grid_ggd[:].space[:].objects_per_dimension[:].geometry_content.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_profiles.grid_ggd[:].space[:].objects_per_dimension[:].geometry_content.name | STR_0D | Short string identifier | ||
edge_profiles.grid_ggd[:].space[:].objects_per_dimension[:].object | [1...N] | STRUCT_ARRAY | Set of objects for a given dimension | |
edge_profiles.grid_ggd[:].space[:].objects_per_dimension[:].object[:].boundary | [1...N] | STRUCT_ARRAY | Set of (n-1)-dimensional objects defining the boundary of this n-dimensional object | |
edge_profiles.grid_ggd[:].space[:].objects_per_dimension[:].object[:].boundary[:].index | INT_0D | Index of this (n-1)-dimensional boundary object | ||
edge_profiles.grid_ggd[:].space[:].objects_per_dimension[:].object[:].boundary[:].neighbours | [1...N] | INT_1D | List of indices of the n-dimensional objects adjacent to the given n-dimensional object. An object can possibly have multiple neighbours on a boundary | |
edge_profiles.grid_ggd[:].space[:].objects_per_dimension[:].object[:].geometry | [1...N] | FLT_1D (uncertain) | mixed | Geometry data associated with the object, its detailed content is defined by ../../geometry_content. Its dimension depends on the type of object, geometry and coordinate considered. |
edge_profiles.grid_ggd[:].space[:].objects_per_dimension[:].object[:].geometry_2d | [1...N, | FLT_2D (uncertain) | mixed | 2D geometry data associated with the object. Its dimension depends on the type of object, geometry and coordinate considered. Typically, the first dimension represents the object coordinates, while the second dimension would represent the values of the various degrees of freedom of the finite element attached to the object. |
edge_profiles.grid_ggd[:].space[:].objects_per_dimension[:].object[:].measure | FLT_0D (uncertain) | m^dimension | Measure of the space object, i.e. physical size (length for 1d, area for 2d, volume for 3d objects,...) | |
edge_profiles.grid_ggd[:].space[:].objects_per_dimension[:].object[:].nodes | [1...N] | INT_1D | List of nodes forming this object (indices to objects_per_dimension(1)%object(:) in Fortran notation) | |
edge_profiles.grid_ggd[:].time | FLT_0D | s | Time | |
edge_profiles.ids_properties | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
edge_profiles.ids_properties.comment | STR_0D | Any comment describing the content of this IDS | ||
edge_profiles.ids_properties.creation_date | STR_0D | Date at which this data has been produced | ||
edge_profiles.ids_properties.homogeneous_time | INT_0D | This node must be filled (with 0, 1, or 2) for the IDS to be valid. If 1, the time of this IDS is homogeneous, i.e. the time values for this IDS are stored in the time node just below the root of this IDS. If 0, the time values are stored in the various time fields at lower levels in the tree. In the case only constant or static nodes are filled within the IDS, homogeneous_time must be set to 2 | ||
edge_profiles.ids_properties.name | STR_0D | User-defined name for this IDS occurrence | ||
edge_profiles.ids_properties.occurrence | INT_0D | |||
edge_profiles.ids_properties.occurrence_type | STRUCTURE | Type of data contained in this occurrence | ||
edge_profiles.ids_properties.occurrence_type.description | STR_0D | Verbose description | ||
edge_profiles.ids_properties.occurrence_type.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_profiles.ids_properties.occurrence_type.name | STR_0D | Short string identifier | ||
edge_profiles.ids_properties.plugins (alpha) | STRUCTURE | Information about the plugins used to write/read this IDS. This structure is filled automatically by the Access Layer at GET/PUT time, no need to fill it via a user program. | ||
edge_profiles.ids_properties.plugins.infrastructure_get (alpha) | STRUCTURE | Plugin infrastructure used to GET the data | ||
edge_profiles.ids_properties.plugins.infrastructure_get.commit (alpha) | STR_0D | Unique commit reference of software | ||
edge_profiles.ids_properties.plugins.infrastructure_get.description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
edge_profiles.ids_properties.plugins.infrastructure_get.name (alpha) | STR_0D | Name of software used | ||
edge_profiles.ids_properties.plugins.infrastructure_get.repository (alpha) | STR_0D | URL of software repository | ||
edge_profiles.ids_properties.plugins.infrastructure_get.version (alpha) | STR_0D | Unique version (tag) of software | ||
edge_profiles.ids_properties.plugins.infrastructure_put (alpha) | STRUCTURE | Plugin infrastructure used to PUT the data | ||
edge_profiles.ids_properties.plugins.infrastructure_put.commit (alpha) | STR_0D | Unique commit reference of software | ||
edge_profiles.ids_properties.plugins.infrastructure_put.description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
edge_profiles.ids_properties.plugins.infrastructure_put.name (alpha) | STR_0D | Name of software used | ||
edge_profiles.ids_properties.plugins.infrastructure_put.repository (alpha) | STR_0D | URL of software repository | ||
edge_profiles.ids_properties.plugins.infrastructure_put.version (alpha) | STR_0D | Unique version (tag) of software | ||
edge_profiles.ids_properties.plugins.node (alpha) | [1...N] | STRUCT_ARRAY | Set of IDS nodes for which a plugin has been applied | |
edge_profiles.ids_properties.plugins.node[:].get_operation (alpha) | [1...N] | STRUCT_ARRAY | Plugins actually used to read back a node (potentially, multiple plugins can be applied, listed in reverse order of application). This information is filled by the plugin infrastructure during the GET operation. | |
edge_profiles.ids_properties.plugins.node[:].get_operation[:].commit (alpha) | STR_0D | Unique commit reference of software | ||
edge_profiles.ids_properties.plugins.node[:].get_operation[:].description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
edge_profiles.ids_properties.plugins.node[:].get_operation[:].name (alpha) | STR_0D | Name of software used | ||
edge_profiles.ids_properties.plugins.node[:].get_operation[:].parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
edge_profiles.ids_properties.plugins.node[:].get_operation[:].repository (alpha) | STR_0D | URL of software repository | ||
edge_profiles.ids_properties.plugins.node[:].get_operation[:].version (alpha) | STR_0D | Unique version (tag) of software | ||
edge_profiles.ids_properties.plugins.node[:].path (alpha) | STR_0D | Path of the node within the IDS, following the syntax given in the link below. If empty, means the plugin applies to the whole IDS. | ||
edge_profiles.ids_properties.plugins.node[:].put_operation (alpha) | [1...N] | STRUCT_ARRAY | Plugins used to PUT a node (potentially, multiple plugins can be applied, if so they are listed by order of application) | |
edge_profiles.ids_properties.plugins.node[:].put_operation[:].commit (alpha) | STR_0D | Unique commit reference of software | ||
edge_profiles.ids_properties.plugins.node[:].put_operation[:].description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
edge_profiles.ids_properties.plugins.node[:].put_operation[:].name (alpha) | STR_0D | Name of software used | ||
edge_profiles.ids_properties.plugins.node[:].put_operation[:].parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
edge_profiles.ids_properties.plugins.node[:].put_operation[:].repository (alpha) | STR_0D | URL of software repository | ||
edge_profiles.ids_properties.plugins.node[:].put_operation[:].version (alpha) | STR_0D | Unique version (tag) of software | ||
edge_profiles.ids_properties.plugins.node[:].readback (alpha) | [1...N] | STRUCT_ARRAY | Plugins to be used to read back a node (potentially, multiple plugins can be applied, listed in reverse order of application) | |
edge_profiles.ids_properties.plugins.node[:].readback[:].commit (alpha) | STR_0D | Unique commit reference of software | ||
edge_profiles.ids_properties.plugins.node[:].readback[:].description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
edge_profiles.ids_properties.plugins.node[:].readback[:].name (alpha) | STR_0D | Name of software used | ||
edge_profiles.ids_properties.plugins.node[:].readback[:].parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
edge_profiles.ids_properties.plugins.node[:].readback[:].repository (alpha) | STR_0D | URL of software repository | ||
edge_profiles.ids_properties.plugins.node[:].readback[:].version (alpha) | STR_0D | Unique version (tag) of software | ||
edge_profiles.ids_properties.provenance (alpha) | STRUCTURE | Provenance information about this IDS | ||
edge_profiles.ids_properties.provenance.node (alpha) | [1...N] | STRUCT_ARRAY | Set of IDS nodes for which the provenance is given. The provenance information applies to the whole structure below the IDS node. For documenting provenance information for the whole IDS, set the size of this array of structure to 1 and leave the child "path" node empty | |
edge_profiles.ids_properties.provenance.node[:].path (alpha) | STR_0D | Path of the node within the IDS, following the syntax given in the link below. If empty, means the provenance information applies to the whole IDS. | ||
edge_profiles.ids_properties.provenance.node[:].sources (alpha) | [1...N] | STR_1D | List of sources used to import or calculate this node, identified as explained below. In case the node is the result of of a calculation / data processing, the source is an input to the process described in the "code" structure at the root of the IDS. The source can be an IDS (identified by a URI or a persitent identifier, see syntax in the link below) or non-IDS data imported directly from an non-IMAS database (identified by the command used to import the source, or the persistent identifier of the data source). Often data are obtained by a chain of processes, however only the last process input are recorded here. The full chain of provenance has then to be reconstructed recursively from the provenance information contained in the data sources. | |
edge_profiles.ids_properties.provider | STR_0D | Name of the person in charge of producing this data | ||
edge_profiles.ids_properties.source (obsolescent) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...). Superseeded by the new provenance structure. | ||
edge_profiles.ids_properties.version_put | STRUCTURE | Version of the access layer package used to PUT this IDS | ||
edge_profiles.ids_properties.version_put.access_layer | STR_0D | Version of Access Layer used to PUT this IDS | ||
edge_profiles.ids_properties.version_put.access_layer_language | STR_0D | Programming language of the Access Layer high level API used to PUT this IDS | ||
edge_profiles.ids_properties.version_put.data_dictionary | STR_0D | Version of Data Dictionary used to PUT this IDS | ||
edge_profiles.midplane | STRUCTURE | Choice of midplane definition (use the lowest index number if more than one value is relevant) | ||
edge_profiles.midplane.description | STR_0D | Verbose description | ||
edge_profiles.midplane.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_profiles.midplane.name | STR_0D | Short string identifier | ||
edge_profiles.profiles_1d | [edge_profiles.profiles_1d[:].time] | STRUCT_ARRAY | SOL radial profiles for various time slices, taken on outboard equatorial mid-plane | |
edge_profiles.profiles_1d[:].conductivity_parallel | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | ohm^-1.m^-1 | Parallel conductivity |
edge_profiles.profiles_1d[:].current_parallel_inside | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | A | Parallel current driven inside the flux surface. Cumulative surface integral of j_total |
edge_profiles.profiles_1d[:].e_field | STRUCTURE | V.m^-1 | Electric field, averaged on the magnetic surface. E.g for the parallel component, average(E.B) / B0, using edge_profiles/vacuum_toroidal_field/b0 | |
edge_profiles.profiles_1d[:].e_field.diamagnetic | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | V.m^-1 | Diamagnetic component |
edge_profiles.profiles_1d[:].e_field.parallel | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | V.m^-1 | Parallel component |
edge_profiles.profiles_1d[:].e_field.poloidal | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | V.m^-1 | Poloidal component |
edge_profiles.profiles_1d[:].e_field.radial | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | V.m^-1 | Radial component |
edge_profiles.profiles_1d[:].e_field.toroidal | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | V.m^-1 | Toroidal component |
edge_profiles.profiles_1d[:].e_field_parallel (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | V.m^-1 | Parallel electric field = average(E.B) / B0, where edge_profiles/Vacuum_Toroidal_Field/ B0 |
edge_profiles.profiles_1d[:].electrons | STRUCTURE | Quantities related to the electrons | ||
edge_profiles.profiles_1d[:].electrons.collisionality_norm | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | - | Collisionality normalised to the bounce frequency |
edge_profiles.profiles_1d[:].electrons.density | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
edge_profiles.profiles_1d[:].electrons.density_fast | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles |
edge_profiles.profiles_1d[:].electrons.density_fit | STRUCTURE | m^-3 | Information on the fit used to obtain the density profile | |
edge_profiles.profiles_1d[:].electrons.density_fit.chi_squared | [edge_profiles.profiles_1d[:].electrons.density_fit.measured] | FLT_1D (uncertain) | - | Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error |
edge_profiles.profiles_1d[:].electrons.density_fit.local | [edge_profiles.profiles_1d[:].electrons.density_fit.measured] | INT_1D | Integer flag : 1 means local measurement, 0 means line-integrated measurement | |
edge_profiles.profiles_1d[:].electrons.density_fit.measured | [1...N] | FLT_1D (uncertain) | m^-3 | Measured values |
edge_profiles.profiles_1d[:].electrons.density_fit.parameters | STR_0D | List of the fit specific parameters in XML format | ||
edge_profiles.profiles_1d[:].electrons.density_fit.reconstructed | [edge_profiles.profiles_1d[:].electrons.density_fit.measured] | FLT_1D (uncertain) | m^-3 | Value reconstructed from the fit |
edge_profiles.profiles_1d[:].electrons.density_fit.rho_pol_norm | [edge_profiles.profiles_1d[:].electrons.density_fit.measured] | FLT_1D (uncertain) | - | Normalised poloidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement) |
edge_profiles.profiles_1d[:].electrons.density_fit.rho_tor_norm | [edge_profiles.profiles_1d[:].electrons.density_fit.measured] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement) |
edge_profiles.profiles_1d[:].electrons.density_fit.source | [edge_profiles.profiles_1d[:].electrons.density_fit.measured] | STR_1D | Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS | |
edge_profiles.profiles_1d[:].electrons.density_fit.time_measurement | [edge_profiles.profiles_1d[:].electrons.density_fit.measured] | FLT_1D (uncertain) | s | Exact time slices used from the time array of the measurement source data. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used |
edge_profiles.profiles_1d[:].electrons.density_fit.time_measurement_slice_method | STRUCTURE | Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, ... | ||
edge_profiles.profiles_1d[:].electrons.density_fit.time_measurement_slice_method.description | STR_0D | Verbose description | ||
edge_profiles.profiles_1d[:].electrons.density_fit.time_measurement_slice_method.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_profiles.profiles_1d[:].electrons.density_fit.time_measurement_slice_method.name | STR_0D | Short string identifier | ||
edge_profiles.profiles_1d[:].electrons.density_fit.time_measurement_width | [edge_profiles.profiles_1d[:].electrons.density_fit.measured] | FLT_1D (uncertain) | s | In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn't use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement. |
edge_profiles.profiles_1d[:].electrons.density_fit.weight | [edge_profiles.profiles_1d[:].electrons.density_fit.measured] | FLT_1D (uncertain) | - | Weight given to each measured value |
edge_profiles.profiles_1d[:].electrons.density_thermal | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m^-3 | Density of thermal particles |
edge_profiles.profiles_1d[:].electrons.density_validity | INT_0D | Indicator of the validity of the density profile. 0: valid from automated processing, 1: valid and certified by the RO; - 1 means problem identified in the data processing (request verification by the RO), -2: invalid data, should not be used | ||
edge_profiles.profiles_1d[:].electrons.pressure | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) |
edge_profiles.profiles_1d[:].electrons.pressure_fast_parallel | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure |
edge_profiles.profiles_1d[:].electrons.pressure_fast_perpendicular | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure |
edge_profiles.profiles_1d[:].electrons.pressure_thermal | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal) associated with random motion ~average((v-average(v))^2) |
edge_profiles.profiles_1d[:].electrons.temperature | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | eV | Temperature |
edge_profiles.profiles_1d[:].electrons.temperature_fit | STRUCTURE | eV | Information on the fit used to obtain the temperature profile | |
edge_profiles.profiles_1d[:].electrons.temperature_fit.chi_squared | [edge_profiles.profiles_1d[:].electrons.temperature_fit.measured] | FLT_1D (uncertain) | - | Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error |
edge_profiles.profiles_1d[:].electrons.temperature_fit.local | [edge_profiles.profiles_1d[:].electrons.temperature_fit.measured] | INT_1D | Integer flag : 1 means local measurement, 0 means line-integrated measurement | |
edge_profiles.profiles_1d[:].electrons.temperature_fit.measured | [1...N] | FLT_1D (uncertain) | eV | Measured values |
edge_profiles.profiles_1d[:].electrons.temperature_fit.parameters | STR_0D | List of the fit specific parameters in XML format | ||
edge_profiles.profiles_1d[:].electrons.temperature_fit.reconstructed | [edge_profiles.profiles_1d[:].electrons.temperature_fit.measured] | FLT_1D (uncertain) | eV | Value reconstructed from the fit |
edge_profiles.profiles_1d[:].electrons.temperature_fit.rho_pol_norm | [edge_profiles.profiles_1d[:].electrons.temperature_fit.measured] | FLT_1D (uncertain) | - | Normalised poloidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement) |
edge_profiles.profiles_1d[:].electrons.temperature_fit.rho_tor_norm | [edge_profiles.profiles_1d[:].electrons.temperature_fit.measured] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement) |
edge_profiles.profiles_1d[:].electrons.temperature_fit.source | [edge_profiles.profiles_1d[:].electrons.temperature_fit.measured] | STR_1D | Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS | |
edge_profiles.profiles_1d[:].electrons.temperature_fit.time_measurement | [edge_profiles.profiles_1d[:].electrons.temperature_fit.measured] | FLT_1D (uncertain) | s | Exact time slices used from the time array of the measurement source data. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used |
edge_profiles.profiles_1d[:].electrons.temperature_fit.time_measurement_slice_method | STRUCTURE | Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, ... | ||
edge_profiles.profiles_1d[:].electrons.temperature_fit.time_measurement_slice_method.description | STR_0D | Verbose description | ||
edge_profiles.profiles_1d[:].electrons.temperature_fit.time_measurement_slice_method.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_profiles.profiles_1d[:].electrons.temperature_fit.time_measurement_slice_method.name | STR_0D | Short string identifier | ||
edge_profiles.profiles_1d[:].electrons.temperature_fit.time_measurement_width | [edge_profiles.profiles_1d[:].electrons.temperature_fit.measured] | FLT_1D (uncertain) | s | In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn't use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement. |
edge_profiles.profiles_1d[:].electrons.temperature_fit.weight | [edge_profiles.profiles_1d[:].electrons.temperature_fit.measured] | FLT_1D (uncertain) | - | Weight given to each measured value |
edge_profiles.profiles_1d[:].electrons.temperature_validity | INT_0D | Indicator of the validity of the temperature profile. 0: valid from automated processing, 1: valid and certified by the RO; - 1 means problem identified in the data processing (request verification by the RO), -2: invalid data, should not be used | ||
edge_profiles.profiles_1d[:].electrons.velocity (obsolescent) | STRUCTURE | m.s^-1 | Velocity | |
edge_profiles.profiles_1d[:].electrons.velocity.diamagnetic (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
edge_profiles.profiles_1d[:].electrons.velocity.parallel (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
edge_profiles.profiles_1d[:].electrons.velocity.poloidal (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
edge_profiles.profiles_1d[:].electrons.velocity.radial (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
edge_profiles.profiles_1d[:].electrons.velocity.toroidal (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
edge_profiles.profiles_1d[:].electrons.velocity_pol (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal velocity |
edge_profiles.profiles_1d[:].electrons.velocity_tor (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal velocity |
edge_profiles.profiles_1d[:].grid | STRUCTURE | Radial grid | ||
edge_profiles.profiles_1d[:].grid.area | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m^2 | Cross-sectional area of the flux surface |
edge_profiles.profiles_1d[:].grid.psi | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
edge_profiles.profiles_1d[:].grid.psi_boundary | FLT_0D (uncertain) | Wb | Value of the poloidal magnetic flux at the plasma boundary (useful to normalize the psi array values when the radial grid doesn't go from the magnetic axis to the plasma boundary) | |
edge_profiles.profiles_1d[:].grid.psi_magnetic_axis | FLT_0D (uncertain) | Wb | Value of the poloidal magnetic flux at the magnetic axis (useful to normalize the psi array values when the radial grid doesn't go from the magnetic axis to the plasma boundary) | |
edge_profiles.profiles_1d[:].grid.rho_pol_norm | [1...N] | FLT_1D (uncertain) | - | Normalised poloidal flux coordinate = sqrt((psi(rho)-psi(magnetic_axis) / (psi(LCFS)-psi(magnetic_axis))) |
edge_profiles.profiles_1d[:].grid.rho_tor | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m | Toroidal flux coordinate. rho_tor = sqrt(b_flux_tor/(pi*b0)) ~ sqrt(pi*r^2*b0/(pi*b0)) ~ r [m]. The toroidal field used in its definition is indicated under vacuum_toroidal_field/b0 |
edge_profiles.profiles_1d[:].grid.rho_tor_norm | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation, see time_slice/boundary/b_flux_pol_norm in the equilibrium IDS) |
edge_profiles.profiles_1d[:].grid.volume | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m^3 | Volume enclosed inside the magnetic surface |
edge_profiles.profiles_1d[:].ion | [1...N] | STRUCT_ARRAY | Quantities related to the different ion species, in the sense of isonuclear or isomolecular sequences. Ionisation states (and other types of states) must be differentiated at the state level below | |
edge_profiles.profiles_1d[:].ion[:].density | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].ion[:].density_fast | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].ion[:].density_fit | STRUCTURE | m^-3 | Information on the fit used to obtain the density profile | |
edge_profiles.profiles_1d[:].ion[:].density_fit.chi_squared | [edge_profiles.profiles_1d[:].ion[:].density_fit.measured] | FLT_1D (uncertain) | - | Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error |
edge_profiles.profiles_1d[:].ion[:].density_fit.local | [edge_profiles.profiles_1d[:].ion[:].density_fit.measured] | INT_1D | Integer flag : 1 means local measurement, 0 means line-integrated measurement | |
edge_profiles.profiles_1d[:].ion[:].density_fit.measured | [1...N] | FLT_1D (uncertain) | m^-3 | Measured values |
edge_profiles.profiles_1d[:].ion[:].density_fit.parameters | STR_0D | List of the fit specific parameters in XML format | ||
edge_profiles.profiles_1d[:].ion[:].density_fit.reconstructed | [edge_profiles.profiles_1d[:].ion[:].density_fit.measured] | FLT_1D (uncertain) | m^-3 | Value reconstructed from the fit |
edge_profiles.profiles_1d[:].ion[:].density_fit.rho_pol_norm | [edge_profiles.profiles_1d[:].ion[:].density_fit.measured] | FLT_1D (uncertain) | - | Normalised poloidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement) |
edge_profiles.profiles_1d[:].ion[:].density_fit.rho_tor_norm | [edge_profiles.profiles_1d[:].ion[:].density_fit.measured] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement) |
edge_profiles.profiles_1d[:].ion[:].density_fit.source | [edge_profiles.profiles_1d[:].ion[:].density_fit.measured] | STR_1D | Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS | |
edge_profiles.profiles_1d[:].ion[:].density_fit.time_measurement | [edge_profiles.profiles_1d[:].ion[:].density_fit.measured] | FLT_1D (uncertain) | s | Exact time slices used from the time array of the measurement source data. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used |
edge_profiles.profiles_1d[:].ion[:].density_fit.time_measurement_slice_method | STRUCTURE | Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, ... | ||
edge_profiles.profiles_1d[:].ion[:].density_fit.time_measurement_slice_method.description | STR_0D | Verbose description | ||
edge_profiles.profiles_1d[:].ion[:].density_fit.time_measurement_slice_method.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_profiles.profiles_1d[:].ion[:].density_fit.time_measurement_slice_method.name | STR_0D | Short string identifier | ||
edge_profiles.profiles_1d[:].ion[:].density_fit.time_measurement_width | [edge_profiles.profiles_1d[:].ion[:].density_fit.measured] | FLT_1D (uncertain) | s | In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn't use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement. |
edge_profiles.profiles_1d[:].ion[:].density_fit.weight | [edge_profiles.profiles_1d[:].ion[:].density_fit.measured] | FLT_1D (uncertain) | - | Weight given to each measured value |
edge_profiles.profiles_1d[:].ion[:].density_thermal | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal) (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].ion[:].density_validity | INT_0D | Indicator of the validity of the density profile. 0: valid from automated processing, 1: valid and certified by the RO; - 1 means problem identified in the data processing (request verification by the RO), -2: invalid data, should not be used | ||
edge_profiles.profiles_1d[:].ion[:].element | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
edge_profiles.profiles_1d[:].ion[:].element[:].a | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
edge_profiles.profiles_1d[:].ion[:].element[:].atoms_n | INT_0D | Number of atoms of this element in the molecule | ||
edge_profiles.profiles_1d[:].ion[:].element[:].multiplicity (obsolescent) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
edge_profiles.profiles_1d[:].ion[:].element[:].z_n | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
edge_profiles.profiles_1d[:].ion[:].label | STR_0D | String identifying ion (e.g. H, D, T, He, C, D2, ...) | ||
edge_profiles.profiles_1d[:].ion[:].multiple_states_flag | INT_0D | Multiple states calculation flag : 0-Only the 'ion' level is considered and the 'state' array of structure is empty; 1-Ion states are considered and are described in the 'state' array of structure | ||
edge_profiles.profiles_1d[:].ion[:].neutral_index | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
edge_profiles.profiles_1d[:].ion[:].pressure | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].ion[:].pressure_fast_parallel | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].ion[:].pressure_fast_perpendicular | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].ion[:].pressure_thermal | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal) associated with random motion ~average((v-average(v))^2) (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].ion[:].rotation_frequency_tor | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | rad.s^-1 | Toroidal rotation frequency (i.e. toroidal velocity divided by the major radius at which the toroidal velocity is taken) (average over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].ion[:].state | [1...N] | STRUCT_ARRAY | Quantities related to the different states of the species (ionisation, energy, excitation, ...) | |
edge_profiles.profiles_1d[:].ion[:].state[:].density | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
edge_profiles.profiles_1d[:].ion[:].state[:].density_fast | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles |
edge_profiles.profiles_1d[:].ion[:].state[:].density_fit | STRUCTURE | m^-3 | Information on the fit used to obtain the density profile | |
edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.chi_squared | [edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.measured] | FLT_1D (uncertain) | - | Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error |
edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.local | [edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.measured] | INT_1D | Integer flag : 1 means local measurement, 0 means line-integrated measurement | |
edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.measured | [1...N] | FLT_1D (uncertain) | m^-3 | Measured values |
edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.parameters | STR_0D | List of the fit specific parameters in XML format | ||
edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.reconstructed | [edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.measured] | FLT_1D (uncertain) | m^-3 | Value reconstructed from the fit |
edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.rho_pol_norm | [edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.measured] | FLT_1D (uncertain) | - | Normalised poloidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement) |
edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.rho_tor_norm | [edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.measured] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement) |
edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.source | [edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.measured] | STR_1D | Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS | |
edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.time_measurement | [edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.measured] | FLT_1D (uncertain) | s | Exact time slices used from the time array of the measurement source data. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used |
edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.time_measurement_slice_method | STRUCTURE | Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, ... | ||
edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.time_measurement_slice_method.description | STR_0D | Verbose description | ||
edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.time_measurement_slice_method.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.time_measurement_slice_method.name | STR_0D | Short string identifier | ||
edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.time_measurement_width | [edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.measured] | FLT_1D (uncertain) | s | In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn't use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement. |
edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.weight | [edge_profiles.profiles_1d[:].ion[:].state[:].density_fit.measured] | FLT_1D (uncertain) | - | Weight given to each measured value |
edge_profiles.profiles_1d[:].ion[:].state[:].density_thermal | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m^-3 | Density of thermal particles |
edge_profiles.profiles_1d[:].ion[:].state[:].electron_configuration | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
edge_profiles.profiles_1d[:].ion[:].state[:].ionisation_potential | FLT_0D (uncertain) | eV | Cumulative and average ionisation potential to reach a given bundle. Defined as sum (x_z* (sum of Epot from z'=0 to z-1)), where Epot is the ionisation potential of ion Xz_+, and x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle. | |
edge_profiles.profiles_1d[:].ion[:].state[:].label | STR_0D | String identifying state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
edge_profiles.profiles_1d[:].ion[:].state[:].pressure | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) |
edge_profiles.profiles_1d[:].ion[:].state[:].pressure_fast_parallel | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure |
edge_profiles.profiles_1d[:].ion[:].state[:].pressure_fast_perpendicular | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure |
edge_profiles.profiles_1d[:].ion[:].state[:].pressure_thermal | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal) associated with random motion ~average((v-average(v))^2) |
edge_profiles.profiles_1d[:].ion[:].state[:].rotation_frequency_tor | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | rad.s^-1 | Toroidal rotation frequency (i.e. toroidal velocity divided by the major radius at which the toroidal velocity is taken) |
edge_profiles.profiles_1d[:].ion[:].state[:].temperature | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | eV | Temperature |
edge_profiles.profiles_1d[:].ion[:].state[:].velocity (obsolescent) | STRUCTURE | m.s^-1 | Velocity | |
edge_profiles.profiles_1d[:].ion[:].state[:].velocity.diamagnetic (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
edge_profiles.profiles_1d[:].ion[:].state[:].velocity.parallel (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
edge_profiles.profiles_1d[:].ion[:].state[:].velocity.poloidal (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
edge_profiles.profiles_1d[:].ion[:].state[:].velocity.radial (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
edge_profiles.profiles_1d[:].ion[:].state[:].velocity.toroidal (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
edge_profiles.profiles_1d[:].ion[:].state[:].vibrational_level | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
edge_profiles.profiles_1d[:].ion[:].state[:].vibrational_mode | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
edge_profiles.profiles_1d[:].ion[:].state[:].z_average | FLT_0D (uncertain) | Elementary Charge Unit | Average Z of the charge state bundle, volume averaged over the plasma radius (equal to z_min if no bundle), = sum (Z*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle. | |
edge_profiles.profiles_1d[:].ion[:].state[:].z_average_1d | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | - | Average charge profile of the charge state bundle (equal to z_min if no bundle), = sum (Z*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle. |
edge_profiles.profiles_1d[:].ion[:].state[:].z_average_square_1d | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | - | Average square charge profile of the charge state bundle (equal to z_min squared if no bundle), = sum (Z^2*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle. |
edge_profiles.profiles_1d[:].ion[:].state[:].z_max | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
edge_profiles.profiles_1d[:].ion[:].state[:].z_min | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle | |
edge_profiles.profiles_1d[:].ion[:].state[:].z_square_average | FLT_0D (uncertain) | Elementary Charge Unit | Average Z square of the charge state bundle, volume averaged over the plasma radius (equal to z_min squared if no bundle), = sum (Z^2*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle. | |
edge_profiles.profiles_1d[:].ion[:].temperature | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | eV | Temperature (average over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].ion[:].temperature_fit | STRUCTURE | eV | Information on the fit used to obtain the temperature profile | |
edge_profiles.profiles_1d[:].ion[:].temperature_fit.chi_squared | [edge_profiles.profiles_1d[:].ion[:].temperature_fit.measured] | FLT_1D (uncertain) | - | Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error |
edge_profiles.profiles_1d[:].ion[:].temperature_fit.local | [edge_profiles.profiles_1d[:].ion[:].temperature_fit.measured] | INT_1D | Integer flag : 1 means local measurement, 0 means line-integrated measurement | |
edge_profiles.profiles_1d[:].ion[:].temperature_fit.measured | [1...N] | FLT_1D (uncertain) | eV | Measured values |
edge_profiles.profiles_1d[:].ion[:].temperature_fit.parameters | STR_0D | List of the fit specific parameters in XML format | ||
edge_profiles.profiles_1d[:].ion[:].temperature_fit.reconstructed | [edge_profiles.profiles_1d[:].ion[:].temperature_fit.measured] | FLT_1D (uncertain) | eV | Value reconstructed from the fit |
edge_profiles.profiles_1d[:].ion[:].temperature_fit.rho_pol_norm | [edge_profiles.profiles_1d[:].ion[:].temperature_fit.measured] | FLT_1D (uncertain) | - | Normalised poloidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement) |
edge_profiles.profiles_1d[:].ion[:].temperature_fit.rho_tor_norm | [edge_profiles.profiles_1d[:].ion[:].temperature_fit.measured] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement) |
edge_profiles.profiles_1d[:].ion[:].temperature_fit.source | [edge_profiles.profiles_1d[:].ion[:].temperature_fit.measured] | STR_1D | Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS | |
edge_profiles.profiles_1d[:].ion[:].temperature_fit.time_measurement | [edge_profiles.profiles_1d[:].ion[:].temperature_fit.measured] | FLT_1D (uncertain) | s | Exact time slices used from the time array of the measurement source data. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used |
edge_profiles.profiles_1d[:].ion[:].temperature_fit.time_measurement_slice_method | STRUCTURE | Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, ... | ||
edge_profiles.profiles_1d[:].ion[:].temperature_fit.time_measurement_slice_method.description | STR_0D | Verbose description | ||
edge_profiles.profiles_1d[:].ion[:].temperature_fit.time_measurement_slice_method.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_profiles.profiles_1d[:].ion[:].temperature_fit.time_measurement_slice_method.name | STR_0D | Short string identifier | ||
edge_profiles.profiles_1d[:].ion[:].temperature_fit.time_measurement_width | [edge_profiles.profiles_1d[:].ion[:].temperature_fit.measured] | FLT_1D (uncertain) | s | In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn't use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement. |
edge_profiles.profiles_1d[:].ion[:].temperature_fit.weight | [edge_profiles.profiles_1d[:].ion[:].temperature_fit.measured] | FLT_1D (uncertain) | - | Weight given to each measured value |
edge_profiles.profiles_1d[:].ion[:].temperature_validity | INT_0D | Indicator of the validity of the temperature profile. 0: valid from automated processing, 1: valid and certified by the RO; - 1 means problem identified in the data processing (request verification by the RO), -2: invalid data, should not be used | ||
edge_profiles.profiles_1d[:].ion[:].velocity | STRUCTURE | m.s^-1 | Velocity (average over charge states when multiple charge states are considered) at the position of maximum major radius on every flux surface | |
edge_profiles.profiles_1d[:].ion[:].velocity.diamagnetic | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
edge_profiles.profiles_1d[:].ion[:].velocity.parallel | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
edge_profiles.profiles_1d[:].ion[:].velocity.poloidal | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
edge_profiles.profiles_1d[:].ion[:].velocity.radial | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
edge_profiles.profiles_1d[:].ion[:].velocity.toroidal | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
edge_profiles.profiles_1d[:].ion[:].velocity_pol (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal velocity (average over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].ion[:].velocity_tor (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal velocity (average over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].ion[:].z_ion | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed), volume averaged over plasma radius | |
edge_profiles.profiles_1d[:].ion[:].z_ion_1d | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | - | Average charge of the ion species (sum of states charge weighted by state density and divided by ion density) |
edge_profiles.profiles_1d[:].ion[:].z_ion_square_1d | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | - | Average square charge of the ion species (sum of states square charge weighted by state density and divided by ion density) |
edge_profiles.profiles_1d[:].j_bootstrap | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | A/m^2 | Bootstrap current density = average(J_Bootstrap.B) / B0, where B0 = edge_profiles/Vacuum_Toroidal_Field/ B0 |
edge_profiles.profiles_1d[:].j_non_inductive | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | A/m^2 | Non-inductive (includes bootstrap) parallel current density = average(jni.B) / B0, where B0 = edge_profiles/Vacuum_Toroidal_Field/ B0 |
edge_profiles.profiles_1d[:].j_ohmic | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | A/m^2 | Ohmic parallel current density = average(J_Ohmic.B) / B0, where B0 = edge_profiles/Vacuum_Toroidal_Field/ B0 |
edge_profiles.profiles_1d[:].j_tor | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | A/m^2 | Total toroidal current density = average(J_Tor/R) / average(1/R) |
edge_profiles.profiles_1d[:].j_total | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | A/m^2 | Total parallel current density = average(jtot.B) / B0, where B0 = edge_profiles/Vacuum_Toroidal_Field/ B0 |
edge_profiles.profiles_1d[:].magnetic_shear | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | - | Magnetic shear, defined as rho_tor/q . dq/drho_tor |
edge_profiles.profiles_1d[:].momentum_tor | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | kg.m^-1.s^-1 | Total plasma toroidal momentum, summed over ion species and electrons weighted by their density and major radius, i.e. sum_over_species(n*R*m*Vphi) |
edge_profiles.profiles_1d[:].n_i_thermal_total | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m^-3 | Total ion thermal density (sum over species and charge states) |
edge_profiles.profiles_1d[:].n_i_total_over_n_e | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | - | Ratio of total ion density (sum over species and charge states) over electron density. (thermal+non-thermal) |
edge_profiles.profiles_1d[:].neutral | [1...N] | STRUCT_ARRAY | Quantities related to the different neutral species | |
edge_profiles.profiles_1d[:].neutral[:].density | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].neutral[:].density_fast | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].neutral[:].density_thermal | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal) (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].neutral[:].element | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
edge_profiles.profiles_1d[:].neutral[:].element[:].a | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
edge_profiles.profiles_1d[:].neutral[:].element[:].atoms_n | INT_0D | Number of atoms of this element in the molecule | ||
edge_profiles.profiles_1d[:].neutral[:].element[:].multiplicity (obsolescent) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
edge_profiles.profiles_1d[:].neutral[:].element[:].z_n | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
edge_profiles.profiles_1d[:].neutral[:].ion_index | INT_0D | Index of the corresponding ion species in the ../../ion array | ||
edge_profiles.profiles_1d[:].neutral[:].label | STR_0D | String identifying the species (e.g. H, D, T, He, C, D2, DT, CD4, ...) | ||
edge_profiles.profiles_1d[:].neutral[:].multiple_states_flag | INT_0D | Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
edge_profiles.profiles_1d[:].neutral[:].pressure | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].neutral[:].pressure_fast_parallel | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].neutral[:].pressure_fast_perpendicular | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].neutral[:].pressure_thermal | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal) associated with random motion ~average((v-average(v))^2) (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].neutral[:].state | [1...N] | STRUCT_ARRAY | Quantities related to the different states of the species (energy, excitation, ...) | |
edge_profiles.profiles_1d[:].neutral[:].state[:].density | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
edge_profiles.profiles_1d[:].neutral[:].state[:].density_fast | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles |
edge_profiles.profiles_1d[:].neutral[:].state[:].density_thermal | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m^-3 | Density of thermal particles |
edge_profiles.profiles_1d[:].neutral[:].state[:].electron_configuration | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
edge_profiles.profiles_1d[:].neutral[:].state[:].label | STR_0D | String identifying state | ||
edge_profiles.profiles_1d[:].neutral[:].state[:].neutral_type | STRUCTURE | Neutral type (if the considered state is a neutral), in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI | ||
edge_profiles.profiles_1d[:].neutral[:].state[:].neutral_type.description | STR_0D | Verbose description | ||
edge_profiles.profiles_1d[:].neutral[:].state[:].neutral_type.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_profiles.profiles_1d[:].neutral[:].state[:].neutral_type.name | STR_0D | Short string identifier | ||
edge_profiles.profiles_1d[:].neutral[:].state[:].pressure | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) |
edge_profiles.profiles_1d[:].neutral[:].state[:].pressure_fast_parallel | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure |
edge_profiles.profiles_1d[:].neutral[:].state[:].pressure_fast_perpendicular | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure |
edge_profiles.profiles_1d[:].neutral[:].state[:].pressure_thermal | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal) associated with random motion ~average((v-average(v))^2) |
edge_profiles.profiles_1d[:].neutral[:].state[:].temperature | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | eV | Temperature |
edge_profiles.profiles_1d[:].neutral[:].state[:].velocity (obsolescent) | STRUCTURE | m.s^-1 | Velocity | |
edge_profiles.profiles_1d[:].neutral[:].state[:].velocity.diamagnetic (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
edge_profiles.profiles_1d[:].neutral[:].state[:].velocity.parallel (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
edge_profiles.profiles_1d[:].neutral[:].state[:].velocity.poloidal (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
edge_profiles.profiles_1d[:].neutral[:].state[:].velocity.radial (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
edge_profiles.profiles_1d[:].neutral[:].state[:].velocity.toroidal (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
edge_profiles.profiles_1d[:].neutral[:].state[:].vibrational_level | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
edge_profiles.profiles_1d[:].neutral[:].state[:].vibrational_mode | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
edge_profiles.profiles_1d[:].neutral[:].temperature | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | eV | Temperature (average over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].neutral[:].velocity (obsolescent) | STRUCTURE | m.s^-1 | Velocity (average over charge states when multiple charge states are considered) | |
edge_profiles.profiles_1d[:].neutral[:].velocity.diamagnetic (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
edge_profiles.profiles_1d[:].neutral[:].velocity.parallel (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
edge_profiles.profiles_1d[:].neutral[:].velocity.poloidal (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
edge_profiles.profiles_1d[:].neutral[:].velocity.radial (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
edge_profiles.profiles_1d[:].neutral[:].velocity.toroidal (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
edge_profiles.profiles_1d[:].phi_potential | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | V | Electrostatic potential, averaged on the magnetic flux surface |
edge_profiles.profiles_1d[:].pressure_ion_total | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Total (sum over ion species) thermal ion pressure |
edge_profiles.profiles_1d[:].pressure_parallel | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Total parallel pressure (electrons+ions, thermal+non-thermal) |
edge_profiles.profiles_1d[:].pressure_perpendicular | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Total perpendicular pressure (electrons+ions, thermal+non-thermal) |
edge_profiles.profiles_1d[:].pressure_thermal | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | Pa | Thermal pressure (electrons+ions) |
edge_profiles.profiles_1d[:].q | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | - | Safety factor |
edge_profiles.profiles_1d[:].rotation_frequency_tor_sonic | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | s^-1 | Derivative of the flux surface averaged electrostatic potential with respect to the poloidal flux, multiplied by -1. This quantity is the toroidal angular rotation frequency due to the ExB drift, introduced in formula (43) of Hinton and Wong, Physics of Fluids 3082 (1985), also referred to as sonic flow in regimes in which the toroidal velocity is dominant over the poloidal velocity |
edge_profiles.profiles_1d[:].t_i_average | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | eV | Ion temperature (averaged on charge states and ion species) |
edge_profiles.profiles_1d[:].t_i_average_fit | STRUCTURE | eV | Information on the fit used to obtain the t_i_average profile | |
edge_profiles.profiles_1d[:].t_i_average_fit.chi_squared | [edge_profiles.profiles_1d[:].t_i_average_fit.measured] | FLT_1D (uncertain) | - | Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error |
edge_profiles.profiles_1d[:].t_i_average_fit.local | [edge_profiles.profiles_1d[:].t_i_average_fit.measured] | INT_1D | Integer flag : 1 means local measurement, 0 means line-integrated measurement | |
edge_profiles.profiles_1d[:].t_i_average_fit.measured | [1...N] | FLT_1D (uncertain) | eV | Measured values |
edge_profiles.profiles_1d[:].t_i_average_fit.parameters | STR_0D | List of the fit specific parameters in XML format | ||
edge_profiles.profiles_1d[:].t_i_average_fit.reconstructed | [edge_profiles.profiles_1d[:].t_i_average_fit.measured] | FLT_1D (uncertain) | eV | Value reconstructed from the fit |
edge_profiles.profiles_1d[:].t_i_average_fit.rho_pol_norm | [edge_profiles.profiles_1d[:].t_i_average_fit.measured] | FLT_1D (uncertain) | - | Normalised poloidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement) |
edge_profiles.profiles_1d[:].t_i_average_fit.rho_tor_norm | [edge_profiles.profiles_1d[:].t_i_average_fit.measured] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement) |
edge_profiles.profiles_1d[:].t_i_average_fit.source | [edge_profiles.profiles_1d[:].t_i_average_fit.measured] | STR_1D | Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS | |
edge_profiles.profiles_1d[:].t_i_average_fit.time_measurement | [edge_profiles.profiles_1d[:].t_i_average_fit.measured] | FLT_1D (uncertain) | s | Exact time slices used from the time array of the measurement source data. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used |
edge_profiles.profiles_1d[:].t_i_average_fit.time_measurement_slice_method | STRUCTURE | Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, ... | ||
edge_profiles.profiles_1d[:].t_i_average_fit.time_measurement_slice_method.description | STR_0D | Verbose description | ||
edge_profiles.profiles_1d[:].t_i_average_fit.time_measurement_slice_method.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_profiles.profiles_1d[:].t_i_average_fit.time_measurement_slice_method.name | STR_0D | Short string identifier | ||
edge_profiles.profiles_1d[:].t_i_average_fit.time_measurement_width | [edge_profiles.profiles_1d[:].t_i_average_fit.measured] | FLT_1D (uncertain) | s | In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn't use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement. |
edge_profiles.profiles_1d[:].t_i_average_fit.weight | [edge_profiles.profiles_1d[:].t_i_average_fit.measured] | FLT_1D (uncertain) | - | Weight given to each measured value |
edge_profiles.profiles_1d[:].time | FLT_0D | s | Time | |
edge_profiles.profiles_1d[:].zeff | [edge_profiles.profiles_1d[:].grid.rho_pol_norm] | FLT_1D (uncertain) | - | Effective charge |
edge_profiles.profiles_1d[:].zeff_fit | STRUCTURE | - | Information on the fit used to obtain the zeff profile | |
edge_profiles.profiles_1d[:].zeff_fit.chi_squared | [edge_profiles.profiles_1d[:].zeff_fit.measured] | FLT_1D (uncertain) | - | Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error |
edge_profiles.profiles_1d[:].zeff_fit.local | [edge_profiles.profiles_1d[:].zeff_fit.measured] | INT_1D | Integer flag : 1 means local measurement, 0 means line-integrated measurement | |
edge_profiles.profiles_1d[:].zeff_fit.measured | [1...N] | FLT_1D (uncertain) | - | Measured values |
edge_profiles.profiles_1d[:].zeff_fit.parameters | STR_0D | List of the fit specific parameters in XML format | ||
edge_profiles.profiles_1d[:].zeff_fit.reconstructed | [edge_profiles.profiles_1d[:].zeff_fit.measured] | FLT_1D (uncertain) | - | Value reconstructed from the fit |
edge_profiles.profiles_1d[:].zeff_fit.rho_pol_norm | [edge_profiles.profiles_1d[:].zeff_fit.measured] | FLT_1D (uncertain) | - | Normalised poloidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement) |
edge_profiles.profiles_1d[:].zeff_fit.rho_tor_norm | [edge_profiles.profiles_1d[:].zeff_fit.measured] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement) |
edge_profiles.profiles_1d[:].zeff_fit.source | [edge_profiles.profiles_1d[:].zeff_fit.measured] | STR_1D | Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS | |
edge_profiles.profiles_1d[:].zeff_fit.time_measurement | [edge_profiles.profiles_1d[:].zeff_fit.measured] | FLT_1D (uncertain) | s | Exact time slices used from the time array of the measurement source data. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used |
edge_profiles.profiles_1d[:].zeff_fit.time_measurement_slice_method | STRUCTURE | Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, ... | ||
edge_profiles.profiles_1d[:].zeff_fit.time_measurement_slice_method.description | STR_0D | Verbose description | ||
edge_profiles.profiles_1d[:].zeff_fit.time_measurement_slice_method.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_profiles.profiles_1d[:].zeff_fit.time_measurement_slice_method.name | STR_0D | Short string identifier | ||
edge_profiles.profiles_1d[:].zeff_fit.time_measurement_width | [edge_profiles.profiles_1d[:].zeff_fit.measured] | FLT_1D (uncertain) | s | In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn't use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement. |
edge_profiles.profiles_1d[:].zeff_fit.weight | [edge_profiles.profiles_1d[:].zeff_fit.measured] | FLT_1D (uncertain) | - | Weight given to each measured value |
edge_profiles.statistics (alpha) | [edge_profiles.statistics[:].time] | STRUCT_ARRAY | Statistics for various time slices | |
edge_profiles.statistics[:].quantity_2d (alpha) | [1...N] | STRUCT_ARRAY | Set of 2D quantities on which statistics are provided. 2D means 1D+time dimension, so either a 1D quantity within a dynamic array of structure, or a 2D dynamic quantity outside of an array of structure. Therefore the resulting statistical value is 1D for a given statistics time slice. | |
edge_profiles.statistics[:].quantity_2d[:].distribution (alpha) | STRUCTURE | Probability distribution function of the quantity | ||
edge_profiles.statistics[:].quantity_2d[:].distribution.bins (alpha) | [1...N, | FLT_2D (uncertain) | mixed | Bins of quantitiy values, defined for each element (first dimension) corresponding to the first dimension of the original 2D quantity |
edge_profiles.statistics[:].quantity_2d[:].distribution.probability (alpha) | [1...N, | FLT_2D (uncertain) | - | Probability to have a value of the quantity between bins(n) and bins(n+1) (thus the size of its second dimension is the size of the second dimension of the bins array - 1). The first dimension correspond to the first dimension of the original 2D quantity |
edge_profiles.statistics[:].quantity_2d[:].path (alpha) | STR_0D | Path of the quantity within the IDS, following the syntax given in the link below | ||
edge_profiles.statistics[:].quantity_2d[:].statistics_type (alpha) | [1...N] | STRUCT_ARRAY | Set of statistics types applied to the quantity | |
edge_profiles.statistics[:].quantity_2d[:].statistics_type[:].grid_index (alpha) | INT_0D | Only if the statistics value is given on a different GGD grid subset than the original quantity (e.g. if the statistics has worked over a dimension of the GGD), index of the grid used to represent the statistics value | ||
edge_profiles.statistics[:].quantity_2d[:].statistics_type[:].grid_subset_index (alpha) | INT_0D | Only if the statistics value is given on a different GGD grid subset than the original quantity (e.g. if the statistics has worked over a dimension of the GGD), index of the new grid subset the statistics value is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_profiles.statistics[:].quantity_2d[:].statistics_type[:].identifier (alpha) | STRUCTURE | Identifier of the statistics type | ||
edge_profiles.statistics[:].quantity_2d[:].statistics_type[:].identifier.description (alpha) | STR_0D | Verbose description | ||
edge_profiles.statistics[:].quantity_2d[:].statistics_type[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_profiles.statistics[:].quantity_2d[:].statistics_type[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
edge_profiles.statistics[:].quantity_2d[:].statistics_type[:].uq_input_path (alpha) | INT_0D | For Sobol index only, path to the related the uq_input quantity, e.g. ../../../uq_input_2d(3) | ||
edge_profiles.statistics[:].quantity_2d[:].statistics_type[:].value (alpha) | [1...N] | FLT_1D (uncertain) | mixed | Value of the statistics for that quantity, the array corresponding to the first dimension of the original 2D quantity |
edge_profiles.statistics[:].time (alpha) | FLT_0D | s | Time | |
edge_profiles.statistics[:].time_width (alpha) | FLT_0D (uncertain) | s | Width of the time interval over which the statistics have been calculated. By convention, the time interval starts at time-time_width and ends at time. | |
edge_profiles.statistics[:].uq_input_2d (alpha) | [1...N] | STRUCT_ARRAY | If the statistics are based on an uncertainty quantification process, set of 2D input quantities that are varied | |
edge_profiles.statistics[:].uq_input_2d[:].distribution (alpha) | STRUCTURE | Probability distribution function of the quantity | ||
edge_profiles.statistics[:].uq_input_2d[:].distribution.bins (alpha) | [1...N, | FLT_2D (uncertain) | mixed | Bins of quantitiy values, defined for each element (first dimension) corresponding to the first dimension of the original 2D quantity |
edge_profiles.statistics[:].uq_input_2d[:].distribution.probability (alpha) | [1...N, | FLT_2D (uncertain) | - | Probability to have a value of the quantity between bins(n) and bins(n+1) (thus the size of its second dimension is the size of the second dimension of the bins array - 1). The first dimension correspond to the first dimension of the original 2D quantity |
edge_profiles.statistics[:].uq_input_2d[:].path (alpha) | STR_0D | Path of the quantity within the IDS, following the syntax given in the link below | ||
edge_profiles.time | [1...N] | FLT_1D_TYPE | s | Generic time |
edge_profiles.vacuum_toroidal_field | STRUCTURE | Characteristics of the vacuum toroidal field (used in rho_tor definition and in the normalization of current densities) | ||
edge_profiles.vacuum_toroidal_field.b0 | [edge_profiles.time] | FLT_1D (uncertain) | T | Vacuum toroidal field at R0 [T]; Positive sign means anti-clockwise when viewing from above. The product R0B0 must be consistent with the b_tor_vacuum_r field of the tf IDS. |
edge_profiles.vacuum_toroidal_field.r0 | FLT_0D (uncertain) | m | Reference major radius where the vacuum toroidal magnetic field is given (usually a fixed position such as the middle of the vessel at the equatorial midplane) |