hard x raysΒΆ
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
hard_x_rays (alpha) | Hard X-rays tomography diagnostic | |||
hard_x_rays.channel (alpha) | [1...N] | STRUCT_ARRAY | Set of channels (detector or pixel of a camera) | |
hard_x_rays.channel[:].aperture (alpha) | [1...N] | STRUCT_ARRAY | Description of a set of collimating apertures | |
hard_x_rays.channel[:].aperture[:].centre (alpha) | STRUCTURE | If geometry_type=2, coordinates of the centre of the circle. If geometry_type=1 or 3, coordinates of the origin of the local coordinate system (X1,X2,X3) describing the plane detector/aperture. This origin is located within the detector/aperture area. | ||
hard_x_rays.channel[:].aperture[:].centre.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle (oriented counter-clockwise when viewing from above) | |
hard_x_rays.channel[:].aperture[:].centre.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
hard_x_rays.channel[:].aperture[:].centre.z (alpha) | FLT_0D (uncertain) | m | Height | |
hard_x_rays.channel[:].aperture[:].geometry_type (alpha) | INT_0D | Type of geometry used to describe the surface of the detector or aperture (1:'outline', 2:'circular', 3:'rectangle'). In case of 'outline', the surface is described by an outline of point in a local coordinate system defined by a centre and three unit vectors X1, X2, X3. Note that there is some flexibility here and the data provider should choose the most convenient coordinate system for the object, respecting the definitions of (X1,X2,X3) indicated below. In case of 'circular', the surface is a circle defined by its centre, radius, and normal vector oriented towards the plasma X3. In case of 'rectangle', the surface is a rectangle defined by its centre, widths in the X1 and X2 directions, and normal vector oriented towards the plasma X3. | ||
hard_x_rays.channel[:].aperture[:].outline (alpha) | STRUCTURE | Irregular outline of the detector/aperture in the (X1, X2) coordinate system. Do NOT repeat the first point. | ||
hard_x_rays.channel[:].aperture[:].outline.x1 (alpha) | [1...N] | FLT_1D (uncertain) | m | Positions along x1 axis |
hard_x_rays.channel[:].aperture[:].outline.x2 (alpha) | [hard_x_rays.channel[:].aperture[:].outline.x1] | FLT_1D (uncertain) | m | Positions along x2 axis |
hard_x_rays.channel[:].aperture[:].radius (alpha) | FLT_0D (uncertain) | m | Radius of the circle, used only if geometry_type = 2 | |
hard_x_rays.channel[:].aperture[:].surface (alpha) | FLT_0D (uncertain) | m^2 | Surface of the detector/aperture, derived from the above geometric data | |
hard_x_rays.channel[:].aperture[:].x1_unit_vector (alpha) | STRUCTURE | Components of the X1 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X1 vector is more horizontal than X2 (has a smaller abs(Z) component) and oriented in the positive phi direction (counter-clockwise when viewing from above). | ||
hard_x_rays.channel[:].aperture[:].x1_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
hard_x_rays.channel[:].aperture[:].x1_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
hard_x_rays.channel[:].aperture[:].x1_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
hard_x_rays.channel[:].aperture[:].x1_width (alpha) | FLT_0D (uncertain) | m | Full width of the aperture in the X1 direction, used only if geometry_type = 3 | |
hard_x_rays.channel[:].aperture[:].x2_unit_vector (alpha) | STRUCTURE | Components of the X2 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X2 axis is orthonormal so that uX2 = uX3 x uX1. | ||
hard_x_rays.channel[:].aperture[:].x2_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
hard_x_rays.channel[:].aperture[:].x2_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
hard_x_rays.channel[:].aperture[:].x2_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
hard_x_rays.channel[:].aperture[:].x2_width (alpha) | FLT_0D (uncertain) | m | Full width of the aperture in the X2 direction, used only if geometry_type = 3 | |
hard_x_rays.channel[:].aperture[:].x3_unit_vector (alpha) | STRUCTURE | Components of the X3 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X3 axis is normal to the detector/aperture plane and oriented towards the plasma. | ||
hard_x_rays.channel[:].aperture[:].x3_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
hard_x_rays.channel[:].aperture[:].x3_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
hard_x_rays.channel[:].aperture[:].x3_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
hard_x_rays.channel[:].detector (alpha) | STRUCTURE | Detector description | ||
hard_x_rays.channel[:].detector.centre (alpha) | STRUCTURE | If geometry_type=2, coordinates of the centre of the circle. If geometry_type=1 or 3, coordinates of the origin of the local coordinate system (X1,X2,X3) describing the plane detector/aperture. This origin is located within the detector/aperture area. | ||
hard_x_rays.channel[:].detector.centre.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle (oriented counter-clockwise when viewing from above) | |
hard_x_rays.channel[:].detector.centre.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
hard_x_rays.channel[:].detector.centre.z (alpha) | FLT_0D (uncertain) | m | Height | |
hard_x_rays.channel[:].detector.geometry_type (alpha) | INT_0D | Type of geometry used to describe the surface of the detector or aperture (1:'outline', 2:'circular', 3:'rectangle'). In case of 'outline', the surface is described by an outline of point in a local coordinate system defined by a centre and three unit vectors X1, X2, X3. Note that there is some flexibility here and the data provider should choose the most convenient coordinate system for the object, respecting the definitions of (X1,X2,X3) indicated below. In case of 'circular', the surface is a circle defined by its centre, radius, and normal vector oriented towards the plasma X3. In case of 'rectangle', the surface is a rectangle defined by its centre, widths in the X1 and X2 directions, and normal vector oriented towards the plasma X3. | ||
hard_x_rays.channel[:].detector.outline (alpha) | STRUCTURE | Irregular outline of the detector/aperture in the (X1, X2) coordinate system. Do NOT repeat the first point. | ||
hard_x_rays.channel[:].detector.outline.x1 (alpha) | [1...N] | FLT_1D (uncertain) | m | Positions along x1 axis |
hard_x_rays.channel[:].detector.outline.x2 (alpha) | [hard_x_rays.channel[:].detector.outline.x1] | FLT_1D (uncertain) | m | Positions along x2 axis |
hard_x_rays.channel[:].detector.radius (alpha) | FLT_0D (uncertain) | m | Radius of the circle, used only if geometry_type = 2 | |
hard_x_rays.channel[:].detector.surface (alpha) | FLT_0D (uncertain) | m^2 | Surface of the detector/aperture, derived from the above geometric data | |
hard_x_rays.channel[:].detector.x1_unit_vector (alpha) | STRUCTURE | Components of the X1 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X1 vector is more horizontal than X2 (has a smaller abs(Z) component) and oriented in the positive phi direction (counter-clockwise when viewing from above). | ||
hard_x_rays.channel[:].detector.x1_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
hard_x_rays.channel[:].detector.x1_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
hard_x_rays.channel[:].detector.x1_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
hard_x_rays.channel[:].detector.x1_width (alpha) | FLT_0D (uncertain) | m | Full width of the aperture in the X1 direction, used only if geometry_type = 3 | |
hard_x_rays.channel[:].detector.x2_unit_vector (alpha) | STRUCTURE | Components of the X2 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X2 axis is orthonormal so that uX2 = uX3 x uX1. | ||
hard_x_rays.channel[:].detector.x2_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
hard_x_rays.channel[:].detector.x2_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
hard_x_rays.channel[:].detector.x2_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
hard_x_rays.channel[:].detector.x2_width (alpha) | FLT_0D (uncertain) | m | Full width of the aperture in the X2 direction, used only if geometry_type = 3 | |
hard_x_rays.channel[:].detector.x3_unit_vector (alpha) | STRUCTURE | Components of the X3 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X3 axis is normal to the detector/aperture plane and oriented towards the plasma. | ||
hard_x_rays.channel[:].detector.x3_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
hard_x_rays.channel[:].detector.x3_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
hard_x_rays.channel[:].detector.x3_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
hard_x_rays.channel[:].energy_band (alpha) | [1...N] | STRUCT_ARRAY | Set of energy bands in which photons are counted by the detector | |
hard_x_rays.channel[:].energy_band[:].detection_efficiency (alpha) | [hard_x_rays.channel[:].energy_band[:].energies] | FLT_1D (uncertain) | - | Probability of detection of a photon impacting the detector as a function of its energy |
hard_x_rays.channel[:].energy_band[:].energies (alpha) | [1...N] | FLT_1D (uncertain) | eV | Array of discrete energy values inside the band |
hard_x_rays.channel[:].energy_band[:].lower_bound (alpha) | FLT_0D (uncertain) | eV | Lower bound of the energy band | |
hard_x_rays.channel[:].energy_band[:].upper_bound (alpha) | FLT_0D (uncertain) | eV | Upper bound of the energy band | |
hard_x_rays.channel[:].etendue (alpha) | FLT_0D (uncertain) | m^2.str | Etendue (geometric extent) of the channel's optical system | |
hard_x_rays.channel[:].etendue_method (alpha) | STRUCTURE | Method used to calculate the etendue. Index = 0 : exact calculation with a 4D integral; 1 : approximation with first order formula (detector surface times solid angle subtended by the apertures); 2 : other methods | ||
hard_x_rays.channel[:].etendue_method.description (alpha) | STR_0D | Verbose description | ||
hard_x_rays.channel[:].etendue_method.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
hard_x_rays.channel[:].etendue_method.name (alpha) | STR_0D | Short string identifier | ||
hard_x_rays.channel[:].filter_window (alpha) | [1...N] | STRUCT_ARRAY | Set of filter windows | |
hard_x_rays.channel[:].filter_window[:].centre (alpha) | STRUCTURE | Coordinates of the origin of the local coordinate system (X1,X2,X3) describing the filter. This origin is located within the filter area and should be the middle point of the filter surface. If geometry_type=2, it's the centre of the circular filter. If geometry_type=3, it's the centre of the rectangular filter. | ||
hard_x_rays.channel[:].filter_window[:].centre.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle (oriented counter-clockwise when viewing from above) | |
hard_x_rays.channel[:].filter_window[:].centre.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
hard_x_rays.channel[:].filter_window[:].centre.z (alpha) | FLT_0D (uncertain) | m | Height | |
hard_x_rays.channel[:].filter_window[:].curvature_type (alpha) | STRUCTURE | Curvature of the filter. | ||
hard_x_rays.channel[:].filter_window[:].curvature_type.description (alpha) | STR_0D | Verbose description | ||
hard_x_rays.channel[:].filter_window[:].curvature_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
hard_x_rays.channel[:].filter_window[:].curvature_type.name (alpha) | STR_0D | Short string identifier | ||
hard_x_rays.channel[:].filter_window[:].geometry_type (alpha) | STRUCTURE | Geometry of the filter contour. Note that there is some flexibility in the choice of the local coordinate system (X1,X2,X3). The data provider should choose the most convenient coordinate system for the filter, respecting the definitions of (X1,X2,X3) indicated below. | ||
hard_x_rays.channel[:].filter_window[:].geometry_type.description (alpha) | STR_0D | Verbose description | ||
hard_x_rays.channel[:].filter_window[:].geometry_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
hard_x_rays.channel[:].filter_window[:].geometry_type.name (alpha) | STR_0D | Short string identifier | ||
hard_x_rays.channel[:].filter_window[:].identifier (alpha) | STR_0D | ID of the filter | ||
hard_x_rays.channel[:].filter_window[:].material (alpha) | STRUCTURE | Material of the filter window | ||
hard_x_rays.channel[:].filter_window[:].material.description (alpha) | STR_0D | Verbose description | ||
hard_x_rays.channel[:].filter_window[:].material.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
hard_x_rays.channel[:].filter_window[:].material.name (alpha) | STR_0D | Short string identifier | ||
hard_x_rays.channel[:].filter_window[:].outline (alpha) | STRUCTURE | Irregular outline of the filter in the (X1, X2) coordinate system, used only if geometry_type/index=1. Do NOT repeat the first point. | ||
hard_x_rays.channel[:].filter_window[:].outline.x1 (alpha) | [1...N] | FLT_1D (uncertain) | m | Positions along x1 axis |
hard_x_rays.channel[:].filter_window[:].outline.x2 (alpha) | [hard_x_rays.channel[:].filter_window[:].outline.x1] | FLT_1D (uncertain) | m | Positions along x2 axis |
hard_x_rays.channel[:].filter_window[:].photon_absorption (alpha) | [hard_x_rays.channel[:].filter_window[:].wavelengths] | FLT_1D (uncertain) | - | Probability of absorbing a photon passing through the filter as a function of its wavelength |
hard_x_rays.channel[:].filter_window[:].radius (alpha) | FLT_0D (uncertain) | m | Radius of the circle, used only if geometry_type/index = 2 | |
hard_x_rays.channel[:].filter_window[:].surface (alpha) | FLT_0D (uncertain) | m^2 | Surface of the filter, derived from the above geometric data | |
hard_x_rays.channel[:].filter_window[:].thickness (alpha) | FLT_0D (uncertain) | m | Thickness of the filter window | |
hard_x_rays.channel[:].filter_window[:].wavelength_lower (alpha) | FLT_0D (uncertain) | m | Lower bound of the filter wavelength range | |
hard_x_rays.channel[:].filter_window[:].wavelength_upper (alpha) | FLT_0D (uncertain) | m | Upper bound of the filter wavelength range | |
hard_x_rays.channel[:].filter_window[:].wavelengths (alpha) | [1...N] | FLT_1D (uncertain) | m | Array of wavelength values |
hard_x_rays.channel[:].filter_window[:].x1_curvature (alpha) | FLT_0D (uncertain) | m | Radius of curvature in the X1 direction, to be filled only for curvature_type/index = 2, 4 or 5 | |
hard_x_rays.channel[:].filter_window[:].x1_unit_vector (alpha) | STRUCTURE | Components of the X1 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X1 vector is more horizontal than X2 (has a smaller abs(Z) component) and oriented in the positive phi direction (counter-clockwise when viewing from above). | ||
hard_x_rays.channel[:].filter_window[:].x1_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
hard_x_rays.channel[:].filter_window[:].x1_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
hard_x_rays.channel[:].filter_window[:].x1_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
hard_x_rays.channel[:].filter_window[:].x1_width (alpha) | FLT_0D (uncertain) | m | Full width of the filter in the X1 direction, used only if geometry_type/index = 3 | |
hard_x_rays.channel[:].filter_window[:].x2_curvature (alpha) | FLT_0D (uncertain) | m | Radius of curvature in the X2 direction, to be filled only for curvature_type/index = 3 or 5 | |
hard_x_rays.channel[:].filter_window[:].x2_unit_vector (alpha) | STRUCTURE | Components of the X2 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X2 axis is orthonormal so that uX2 = uX3 x uX1. | ||
hard_x_rays.channel[:].filter_window[:].x2_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
hard_x_rays.channel[:].filter_window[:].x2_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
hard_x_rays.channel[:].filter_window[:].x2_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
hard_x_rays.channel[:].filter_window[:].x2_width (alpha) | FLT_0D (uncertain) | m | Full width of the filter in the X2 direction, used only if geometry_type/index = 3 | |
hard_x_rays.channel[:].filter_window[:].x3_unit_vector (alpha) | STRUCTURE | Components of the X3 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X3 axis is normal to the filter surface and oriented towards the plasma. | ||
hard_x_rays.channel[:].filter_window[:].x3_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
hard_x_rays.channel[:].filter_window[:].x3_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
hard_x_rays.channel[:].filter_window[:].x3_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
hard_x_rays.channel[:].identifier (alpha) | STR_0D | ID of the channel | ||
hard_x_rays.channel[:].line_of_sight (alpha) | STRUCTURE | Description of the line of sight of the channel, given by 2 points | ||
hard_x_rays.channel[:].line_of_sight.first_point (alpha) | STRUCTURE | Position of the first point | ||
hard_x_rays.channel[:].line_of_sight.first_point.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle (oriented counter-clockwise when viewing from above) | |
hard_x_rays.channel[:].line_of_sight.first_point.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
hard_x_rays.channel[:].line_of_sight.first_point.z (alpha) | FLT_0D (uncertain) | m | Height | |
hard_x_rays.channel[:].line_of_sight.second_point (alpha) | STRUCTURE | Position of the second point | ||
hard_x_rays.channel[:].line_of_sight.second_point.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle (oriented counter-clockwise when viewing from above) | |
hard_x_rays.channel[:].line_of_sight.second_point.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
hard_x_rays.channel[:].line_of_sight.second_point.z (alpha) | FLT_0D (uncertain) | m | Height | |
hard_x_rays.channel[:].name (alpha) | STR_0D | Name of the channel | ||
hard_x_rays.channel[:].radiance (alpha) | [hard_x_rays.channel[:].energy_band, | STRUCTURE | (photons).s^-1.m^-2.sr^-1 | Photons received by the detector per unit time, per unit solid angle and per unit area (i.e. photon flux divided by the etendue), in multiple energy bands if available from the detector |
hard_x_rays.channel[:].radiance.data (alpha) | [1...N, | FLT_2D (uncertain) | (photons).s^-1.m^-2.sr^-1 | Data |
hard_x_rays.channel[:].radiance.time (alpha) | [1...N] | FLT_1D_TYPE | s | Time |
hard_x_rays.channel[:].radiance.validity (alpha) | INT_0D | Indicator of the validity of the data for the whole acquisition period. 0: valid from automated processing, 1: valid and certified by the diagnostic RO; - 1 means problem identified in the data processing (request verification by the diagnostic RO), -2: invalid data, should not be used (values lower than -2 have a code-specific meaning detailing the origin of their invalidity) | ||
hard_x_rays.channel[:].radiance.validity_timed (alpha) | [hard_x_rays.channel[:].radiance.time] | INT_1D | Indicator of the validity of the data for each time slice. 0: valid from automated processing, 1: valid and certified by the diagnostic RO; - 1 means problem identified in the data processing (request verification by the diagnostic RO), -2: invalid data, should not be used (values lower than -2 have a code-specific meaning detailing the origin of their invalidity) | |
hard_x_rays.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
hard_x_rays.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
hard_x_rays.code.description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
hard_x_rays.code.library (alpha) | [1...N] | STRUCT_ARRAY | List of external libraries used by the code that has produced this IDS | |
hard_x_rays.code.library[:].commit (alpha) | STR_0D | Unique commit reference of software | ||
hard_x_rays.code.library[:].description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
hard_x_rays.code.library[:].name (alpha) | STR_0D | Name of software | ||
hard_x_rays.code.library[:].parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
hard_x_rays.code.library[:].repository (alpha) | STR_0D | URL of software repository | ||
hard_x_rays.code.library[:].version (alpha) | STR_0D | Unique version (tag) of software | ||
hard_x_rays.code.name (alpha) | STR_0D | Name of software generating IDS | ||
hard_x_rays.code.output_flag (alpha) | [hard_x_rays.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. | |
hard_x_rays.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
hard_x_rays.code.repository (alpha) | STR_0D | URL of software repository | ||
hard_x_rays.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
hard_x_rays.emissivity_profile_1d (alpha) | [1...N] | STRUCT_ARRAY | Emissivity profile per energy band (assumed common to all channels used in the profile reconstruction) | |
hard_x_rays.emissivity_profile_1d[:].emissivity (alpha) | [hard_x_rays.emissivity_profile_1d[:].rho_tor_norm, | FLT_2D (uncertain) | (photons).m^-3.str^-1.s^-1 | Radial profile of the plasma emissivity in this energy band |
hard_x_rays.emissivity_profile_1d[:].half_width_external (alpha) | [hard_x_rays.emissivity_profile_1d[:].time] | FLT_1D (uncertain) | - | External (towards separatrix) half width of the emissivity peak (in normalised toroidal flux) |
hard_x_rays.emissivity_profile_1d[:].half_width_internal (alpha) | [hard_x_rays.emissivity_profile_1d[:].time] | FLT_1D (uncertain) | - | Internal (towards magnetic axis) half width of the emissivity peak (in normalised toroidal flux) |
hard_x_rays.emissivity_profile_1d[:].lower_bound (alpha) | FLT_0D (uncertain) | eV | Lower bound of the energy band | |
hard_x_rays.emissivity_profile_1d[:].peak_position (alpha) | [hard_x_rays.emissivity_profile_1d[:].time] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate position at which the emissivity peaks |
hard_x_rays.emissivity_profile_1d[:].rho_tor_norm (alpha) | [1...N] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate grid |
hard_x_rays.emissivity_profile_1d[:].time (alpha) | [1...N] | FLT_1D_TYPE | s | Time |
hard_x_rays.emissivity_profile_1d[:].upper_bound (alpha) | FLT_0D (uncertain) | eV | Upper bound of the energy band | |
hard_x_rays.emissivity_profile_1d[:].validity_timed (alpha) | [hard_x_rays.emissivity_profile_1d[:].time] | INT_1D | Indicator of the validity of the emissivity profile data for each time slice. 0: valid from automated processing, 1: valid and certified by the diagnostic RO; - 1 means problem identified in the data processing (request verification by the diagnostic RO), -2: invalid data, should not be used (values lower than -2 have a code-specific meaning detailing the origin of their invalidity) | |
hard_x_rays.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
hard_x_rays.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
hard_x_rays.ids_properties.creation_date (alpha) | STR_0D | Date at which this data has been produced | ||
hard_x_rays.ids_properties.homogeneous_time (alpha) | 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 | ||
hard_x_rays.ids_properties.name (alpha) | STR_0D | User-defined name for this IDS occurrence | ||
hard_x_rays.ids_properties.occurrence | INT_0D | |||
hard_x_rays.ids_properties.occurrence_type (alpha) | STRUCTURE | Type of data contained in this occurrence | ||
hard_x_rays.ids_properties.occurrence_type.description (alpha) | STR_0D | Verbose description | ||
hard_x_rays.ids_properties.occurrence_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
hard_x_rays.ids_properties.occurrence_type.name (alpha) | STR_0D | Short string identifier | ||
hard_x_rays.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. | ||
hard_x_rays.ids_properties.plugins.infrastructure_get (alpha) | STRUCTURE | Plugin infrastructure used to GET the data | ||
hard_x_rays.ids_properties.plugins.infrastructure_get.commit (alpha) | STR_0D | Unique commit reference of software | ||
hard_x_rays.ids_properties.plugins.infrastructure_get.description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
hard_x_rays.ids_properties.plugins.infrastructure_get.name (alpha) | STR_0D | Name of software used | ||
hard_x_rays.ids_properties.plugins.infrastructure_get.repository (alpha) | STR_0D | URL of software repository | ||
hard_x_rays.ids_properties.plugins.infrastructure_get.version (alpha) | STR_0D | Unique version (tag) of software | ||
hard_x_rays.ids_properties.plugins.infrastructure_put (alpha) | STRUCTURE | Plugin infrastructure used to PUT the data | ||
hard_x_rays.ids_properties.plugins.infrastructure_put.commit (alpha) | STR_0D | Unique commit reference of software | ||
hard_x_rays.ids_properties.plugins.infrastructure_put.description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
hard_x_rays.ids_properties.plugins.infrastructure_put.name (alpha) | STR_0D | Name of software used | ||
hard_x_rays.ids_properties.plugins.infrastructure_put.repository (alpha) | STR_0D | URL of software repository | ||
hard_x_rays.ids_properties.plugins.infrastructure_put.version (alpha) | STR_0D | Unique version (tag) of software | ||
hard_x_rays.ids_properties.plugins.node (alpha) | [1...N] | STRUCT_ARRAY | Set of IDS nodes for which a plugin has been applied | |
hard_x_rays.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. | |
hard_x_rays.ids_properties.plugins.node[:].get_operation[:].commit (alpha) | STR_0D | Unique commit reference of software | ||
hard_x_rays.ids_properties.plugins.node[:].get_operation[:].description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
hard_x_rays.ids_properties.plugins.node[:].get_operation[:].name (alpha) | STR_0D | Name of software used | ||
hard_x_rays.ids_properties.plugins.node[:].get_operation[:].parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
hard_x_rays.ids_properties.plugins.node[:].get_operation[:].repository (alpha) | STR_0D | URL of software repository | ||
hard_x_rays.ids_properties.plugins.node[:].get_operation[:].version (alpha) | STR_0D | Unique version (tag) of software | ||
hard_x_rays.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. | ||
hard_x_rays.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) | |
hard_x_rays.ids_properties.plugins.node[:].put_operation[:].commit (alpha) | STR_0D | Unique commit reference of software | ||
hard_x_rays.ids_properties.plugins.node[:].put_operation[:].description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
hard_x_rays.ids_properties.plugins.node[:].put_operation[:].name (alpha) | STR_0D | Name of software used | ||
hard_x_rays.ids_properties.plugins.node[:].put_operation[:].parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
hard_x_rays.ids_properties.plugins.node[:].put_operation[:].repository (alpha) | STR_0D | URL of software repository | ||
hard_x_rays.ids_properties.plugins.node[:].put_operation[:].version (alpha) | STR_0D | Unique version (tag) of software | ||
hard_x_rays.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) | |
hard_x_rays.ids_properties.plugins.node[:].readback[:].commit (alpha) | STR_0D | Unique commit reference of software | ||
hard_x_rays.ids_properties.plugins.node[:].readback[:].description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
hard_x_rays.ids_properties.plugins.node[:].readback[:].name (alpha) | STR_0D | Name of software used | ||
hard_x_rays.ids_properties.plugins.node[:].readback[:].parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
hard_x_rays.ids_properties.plugins.node[:].readback[:].repository (alpha) | STR_0D | URL of software repository | ||
hard_x_rays.ids_properties.plugins.node[:].readback[:].version (alpha) | STR_0D | Unique version (tag) of software | ||
hard_x_rays.ids_properties.provenance (alpha) | STRUCTURE | Provenance information about this IDS | ||
hard_x_rays.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 | |
hard_x_rays.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. | ||
hard_x_rays.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. | |
hard_x_rays.ids_properties.provider (alpha) | STR_0D | Name of the person in charge of producing this data | ||
hard_x_rays.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. | ||
hard_x_rays.ids_properties.version_put (alpha) | STRUCTURE | Version of the access layer package used to PUT this IDS | ||
hard_x_rays.ids_properties.version_put.access_layer (alpha) | STR_0D | Version of Access Layer used to PUT this IDS | ||
hard_x_rays.ids_properties.version_put.access_layer_language (alpha) | STR_0D | Programming language of the Access Layer high level API used to PUT this IDS | ||
hard_x_rays.ids_properties.version_put.data_dictionary (alpha) | STR_0D | Version of Data Dictionary used to PUT this IDS | ||
hard_x_rays.latency (alpha) | FLT_0D (uncertain) | s | Upper bound of the delay between physical information received by the detector and data available on the real-time (RT) network. | |
hard_x_rays.time (alpha) | [1...N] | FLT_1D_TYPE | s | Generic time |