mhd linear

Path	Dimensions	Type	Units	Description
mhd_linear (alpha)				Magnetohydronamic linear stability
mhd_linear.code (alpha)		STRUCTURE		Generic decription of the code-specific parameters for the code that has produced this IDS
mhd_linear.code.commit (alpha)		STR_0D		Unique commit reference of software
mhd_linear.code.description (alpha)		STR_0D		Short description of the software (type, purpose)
mhd_linear.code.library (alpha)	[1...N]	STRUCT_ARRAY		List of external libraries used by the code that has produced this IDS
mhd_linear.code.library[:].commit (alpha)		STR_0D		Unique commit reference of software
mhd_linear.code.library[:].description (alpha)		STR_0D		Short description of the software (type, purpose)
mhd_linear.code.library[:].name (alpha)		STR_0D		Name of software
mhd_linear.code.library[:].parameters (alpha)		STR_0D		List of the code specific parameters in XML format
mhd_linear.code.library[:].repository (alpha)		STR_0D		URL of software repository
mhd_linear.code.library[:].version (alpha)		STR_0D		Unique version (tag) of software
mhd_linear.code.name (alpha)		STR_0D		Name of software generating IDS
mhd_linear.code.output_flag (alpha)	[mhd_linear.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.
mhd_linear.code.parameters (alpha)		STR_0D		List of the code specific parameters in XML format
mhd_linear.code.repository (alpha)		STR_0D		URL of software repository
mhd_linear.code.version (alpha)		STR_0D		Unique version (tag) of software
mhd_linear.equations (alpha)		STRUCTURE		Type of MHD equations used to populate this IDS 1) reduced : Reduced MHD 11) reduced_kinetic : Reduced MHD and kinetic hybrid 2) full : Full MHD 21) full_kinetic : Full MHD and kinetic hybrid
mhd_linear.equations.description (alpha)		STR_0D		Verbose description
mhd_linear.equations.index (alpha)		INT_0D		Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index.
mhd_linear.equations.name (alpha)		STR_0D		Short string identifier
mhd_linear.fluids_n (alpha)		INT_0D		Number of fluids considered in the model
mhd_linear.ideal_flag (alpha)		INT_0D		1 if ideal MHD is used to populate this IDS, 0 for non-ideal MHD
mhd_linear.ids_properties (alpha)		STRUCTURE		Interface Data Structure properties. This element identifies the node above as an IDS
mhd_linear.ids_properties.comment (alpha)		STR_0D		Any comment describing the content of this IDS
mhd_linear.ids_properties.creation_date (alpha)		STR_0D		Date at which this data has been produced
mhd_linear.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
mhd_linear.ids_properties.name (alpha)		STR_0D		User-defined name for this IDS occurrence
mhd_linear.ids_properties.occurrence		INT_0D
mhd_linear.ids_properties.occurrence_type (alpha)		STRUCTURE		Type of data contained in this occurrence 1) reconstruction : Equilibrium reconstruction 2) prediction_fixed : Equilibrium prediction, fixed boundary 3) prediction_free : Equilibrium prediction, free boundary 4) mapping : Used for mapping equilibrium results from one grid type / resolution to another, or for including variables not present in the first set such as the calculation of magnetic field of other derived parameters
mhd_linear.ids_properties.occurrence_type.description (alpha)		STR_0D		Verbose description
mhd_linear.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.
mhd_linear.ids_properties.occurrence_type.name (alpha)		STR_0D		Short string identifier
mhd_linear.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.
mhd_linear.ids_properties.plugins.infrastructure_get (alpha)		STRUCTURE		Plugin infrastructure used to GET the data
mhd_linear.ids_properties.plugins.infrastructure_get.commit (alpha)		STR_0D		Unique commit reference of software
mhd_linear.ids_properties.plugins.infrastructure_get.description (alpha)		STR_0D		Short description of the software (type, purpose)
mhd_linear.ids_properties.plugins.infrastructure_get.name (alpha)		STR_0D		Name of software used
mhd_linear.ids_properties.plugins.infrastructure_get.repository (alpha)		STR_0D		URL of software repository
mhd_linear.ids_properties.plugins.infrastructure_get.version (alpha)		STR_0D		Unique version (tag) of software
mhd_linear.ids_properties.plugins.infrastructure_put (alpha)		STRUCTURE		Plugin infrastructure used to PUT the data
mhd_linear.ids_properties.plugins.infrastructure_put.commit (alpha)		STR_0D		Unique commit reference of software
mhd_linear.ids_properties.plugins.infrastructure_put.description (alpha)		STR_0D		Short description of the software (type, purpose)
mhd_linear.ids_properties.plugins.infrastructure_put.name (alpha)		STR_0D		Name of software used
mhd_linear.ids_properties.plugins.infrastructure_put.repository (alpha)		STR_0D		URL of software repository
mhd_linear.ids_properties.plugins.infrastructure_put.version (alpha)		STR_0D		Unique version (tag) of software
mhd_linear.ids_properties.plugins.node (alpha)	[1...N]	STRUCT_ARRAY		Set of IDS nodes for which a plugin has been applied
mhd_linear.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.
mhd_linear.ids_properties.plugins.node[:].get_operation[:].commit (alpha)		STR_0D		Unique commit reference of software
mhd_linear.ids_properties.plugins.node[:].get_operation[:].description (alpha)		STR_0D		Short description of the software (type, purpose)
mhd_linear.ids_properties.plugins.node[:].get_operation[:].name (alpha)		STR_0D		Name of software used
mhd_linear.ids_properties.plugins.node[:].get_operation[:].parameters (alpha)		STR_0D		List of the code specific parameters in XML format
mhd_linear.ids_properties.plugins.node[:].get_operation[:].repository (alpha)		STR_0D		URL of software repository
mhd_linear.ids_properties.plugins.node[:].get_operation[:].version (alpha)		STR_0D		Unique version (tag) of software
mhd_linear.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.
mhd_linear.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)
mhd_linear.ids_properties.plugins.node[:].put_operation[:].commit (alpha)		STR_0D		Unique commit reference of software
mhd_linear.ids_properties.plugins.node[:].put_operation[:].description (alpha)		STR_0D		Short description of the software (type, purpose)
mhd_linear.ids_properties.plugins.node[:].put_operation[:].name (alpha)		STR_0D		Name of software used
mhd_linear.ids_properties.plugins.node[:].put_operation[:].parameters (alpha)		STR_0D		List of the code specific parameters in XML format
mhd_linear.ids_properties.plugins.node[:].put_operation[:].repository (alpha)		STR_0D		URL of software repository
mhd_linear.ids_properties.plugins.node[:].put_operation[:].version (alpha)		STR_0D		Unique version (tag) of software
mhd_linear.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)
mhd_linear.ids_properties.plugins.node[:].readback[:].commit (alpha)		STR_0D		Unique commit reference of software
mhd_linear.ids_properties.plugins.node[:].readback[:].description (alpha)		STR_0D		Short description of the software (type, purpose)
mhd_linear.ids_properties.plugins.node[:].readback[:].name (alpha)		STR_0D		Name of software used
mhd_linear.ids_properties.plugins.node[:].readback[:].parameters (alpha)		STR_0D		List of the code specific parameters in XML format
mhd_linear.ids_properties.plugins.node[:].readback[:].repository (alpha)		STR_0D		URL of software repository
mhd_linear.ids_properties.plugins.node[:].readback[:].version (alpha)		STR_0D		Unique version (tag) of software
mhd_linear.ids_properties.provenance (alpha)		STRUCTURE		Provenance information about this IDS
mhd_linear.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
mhd_linear.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.
mhd_linear.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.
mhd_linear.ids_properties.provider (alpha)		STR_0D		Name of the person in charge of producing this data
mhd_linear.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.
mhd_linear.ids_properties.version_put (alpha)		STRUCTURE		Version of the access layer package used to PUT this IDS
mhd_linear.ids_properties.version_put.access_layer (alpha)		STR_0D		Version of Access Layer used to PUT this IDS
mhd_linear.ids_properties.version_put.access_layer_language (alpha)		STR_0D		Programming language of the Access Layer high level API used to PUT this IDS
mhd_linear.ids_properties.version_put.data_dictionary (alpha)		STR_0D		Version of Data Dictionary used to PUT this IDS
mhd_linear.model_type (alpha)		STRUCTURE		Type of model used to populate this IDS 1) global : Global calculation 2) local : Local calculation 3) analytical : Analytical estimate
mhd_linear.model_type.description (alpha)		STR_0D		Verbose description
mhd_linear.model_type.index (alpha)		INT_0D		Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index.
mhd_linear.model_type.name (alpha)		STR_0D		Short string identifier
mhd_linear.time (alpha)	[1...N]	FLT_1D_TYPE	s	Generic time
mhd_linear.time_slice (alpha)	[mhd_linear.time_slice[:].time]	STRUCT_ARRAY		Core plasma radial profiles for various time slices
mhd_linear.time_slice[:].time (alpha)		FLT_0D	s	Time
mhd_linear.time_slice[:].toroidal_mode (alpha)	[1...N]	STRUCT_ARRAY		Vector of toroidal modes. Each mode is described as exp(i(n_tor.phi - m_pol.theta - 2.pi.frequency.t - phase))
mhd_linear.time_slice[:].toroidal_mode[:].amplitude_multiplier (alpha)		FLT_0D (uncertain)	mixed	Multiplier that is needed to convert the linear mode structures to the amplitude of a non-linearly saturated mode in physical units. If empty, it means that the structures contains no information about non-linearly saturated mode
mhd_linear.time_slice[:].toroidal_mode[:].ballooning_type (alpha)		STRUCTURE		Ballooning type of the mode : ballooning 0; anti-ballooning:1; flute-like:2 1) TAE : Toroidal Alfven Eigenmode 2) EAE : Ellipticity-induced Alfven Eigenmode 3) NAE : Non-circular triangularity induced Alfven Eigenmode 4) RSAE : Reversed Shear Alfven Eigenmode 5) BAE : Beta induced Alfven Eigenmode 6) BAAE : Beta induced Alfven Acoustic Eigenmode 7) EPM : Energetic particle mode, outside any shear Alfven gap 8) GAE : Global Alfven Eingenmode 9) GAM : Geodesic Acoustic Mode 10) EGAM : Energetic particle-driven Geodesic Acoustic Mode 11) iKINK : Internal KINK mode 12) eKINK : External KINK mode 13) Tearing : Tearing mode 14) Double_Tearing : Double Tearing mode
mhd_linear.time_slice[:].toroidal_mode[:].ballooning_type.description (alpha)		STR_0D		Verbose description
mhd_linear.time_slice[:].toroidal_mode[:].ballooning_type.index (alpha)		INT_0D		Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index.
mhd_linear.time_slice[:].toroidal_mode[:].ballooning_type.name (alpha)		STR_0D		Short string identifier
mhd_linear.time_slice[:].toroidal_mode[:].energy_perturbed (alpha)		FLT_0D (uncertain)	J	Perturbed energy associated to the mode
mhd_linear.time_slice[:].toroidal_mode[:].frequency (alpha)		FLT_0D (uncertain)	Hz	Frequency of the mode
mhd_linear.time_slice[:].toroidal_mode[:].growthrate (alpha)		FLT_0D (uncertain)	Hz	Linear growthrate of the mode
mhd_linear.time_slice[:].toroidal_mode[:].m_pol_dominant (alpha)		FLT_0D (uncertain)	-	Dominant poloidal mode number defining the mode rational surface; for TAEs the lower of the two main m's has to be specified
mhd_linear.time_slice[:].toroidal_mode[:].n_tor (alpha)		INT_0D		Toroidal mode number of the MHD mode
mhd_linear.time_slice[:].toroidal_mode[:].perturbation_type (alpha)		STRUCTURE		Type of the perturbation 1) TAE : Toroidal Alfven Eigenmode 2) EAE : Ellipticity-induced Alfven Eigenmode 3) NAE : Non-circular triangularity induced Alfven Eigenmode 4) RSAE : Reversed Shear Alfven Eigenmode 5) BAE : Beta induced Alfven Eigenmode 6) BAAE : Beta induced Alfven Acoustic Eigenmode 7) EPM : Energetic particle mode, outside any shear Alfven gap 8) GAE : Global Alfven Eingenmode 9) GAM : Geodesic Acoustic Mode 10) EGAM : Energetic particle-driven Geodesic Acoustic Mode 11) iKINK : Internal KINK mode 12) eKINK : External KINK mode 13) Tearing : Tearing mode 14) Double_Tearing : Double Tearing mode
mhd_linear.time_slice[:].toroidal_mode[:].perturbation_type.description (alpha)		STR_0D		Verbose description
mhd_linear.time_slice[:].toroidal_mode[:].perturbation_type.index (alpha)		INT_0D		Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index.
mhd_linear.time_slice[:].toroidal_mode[:].perturbation_type.name (alpha)		STR_0D		Short string identifier
mhd_linear.time_slice[:].toroidal_mode[:].phase (alpha)		FLT_0D (uncertain)	rad	Additional phase offset of mode
mhd_linear.time_slice[:].toroidal_mode[:].plasma (alpha)		STRUCTURE		MHD modes in the confined plasma
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed (alpha)		STRUCTURE	T.m	Pertubed vector potential for given toroidal mode number
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate1 (alpha)		STRUCTURE	T.m	First coordinate (radial)
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate1.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	T.m	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate1.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	T.m	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate1.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	T.m	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate1.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	T.m	Real part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate2 (alpha)		STRUCTURE	T.m	Second coordinate (poloidal)
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate2.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	T.m	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate2.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	T.m	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate2.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	T.m	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate2.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	T.m	Real part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate3 (alpha)		STRUCTURE	T.m	Third coordinate (toroidal)
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate3.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	T.m	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate3.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	T.m	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate3.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	T.m	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate3.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	T.m	Real part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.alfven_frequency_spectrum (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1]	STRUCT_ARRAY		Local shear Alfven spectrum as a function of radius (only in case grid/dim1 is a radial coordinate)
mhd_linear.time_slice[:].toroidal_mode[:].plasma.alfven_frequency_spectrum[:].imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.alfven_frequency_spectrum[:].real]	FLT_1D (uncertain)	s^-1	Imaginary part of the frequency, for a given radial position and every root found at this position
mhd_linear.time_slice[:].toroidal_mode[:].plasma.alfven_frequency_spectrum[:].real (alpha)	[1...N]	FLT_1D (uncertain)	s^-1	Real part of the frequency, for a given radial position and every root found at this position
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed (alpha)		STRUCTURE	T	Pertubed magnetic field for given toroidal mode number
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate1 (alpha)		STRUCTURE	T	First coordinate (radial)
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate1.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	T	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate1.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	T	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate1.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	T	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate1.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	T	Real part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate2 (alpha)		STRUCTURE	T	Second coordinate (poloidal)
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate2.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	T	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate2.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	T	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate2.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	T	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate2.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	T	Real part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate3 (alpha)		STRUCTURE	T	Third coordinate (toroidal)
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate3.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	T	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate3.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	T	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate3.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	T	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate3.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	T	Real part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system (alpha)		STRUCTURE		Flux surface coordinate system of the equilibrium used for the MHD calculation on a square grid of flux and poloidal angle
mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid (alpha)		STRUCTURE		Definition of the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid.dim1 (alpha)	[1...N]	FLT_1D (uncertain)	mixed	First dimension values
mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid.dim2 (alpha)	[1...N]	FLT_1D (uncertain)	mixed	Second dimension values
mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid.volume_element (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid.dim2]	FLT_2D (uncertain)	m^3	Elementary plasma volume of plasma enclosed in the cell formed by the nodes [dim1(i) dim2(j)], [dim1(i+1) dim2(j)], [dim1(i) dim2(j+1)] and [dim1(i+1) dim2(j+1)]
mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid_type (alpha)		STRUCTURE		Selection of one of a set of grid types 1) rectangular : Cylindrical R,Z ala eqdsk (R=dim1, Z=dim2). In this case the position arrays should not be filled since they are redundant with grid/dim1 and dim2. 2) inverse : Rhopolar_polar 2D polar coordinates (rho=dim1, theta=dim2) with magnetic axis as centre of grid; theta and values following the COCOS=11 convention; the polar angle is theta=atan2(z-zaxis,r-raxis) 11) inverse_psi_straight_field_line : Flux surface type with psi as radial label (dim1) and the straight-field line poloidal angle (mod(index,10)=1) (dim2); could be non-equidistant; magnetic axis as centre of grid; following the COCOS=11 convention 12) inverse_psi_equal_arc : Flux surface type with psi as radial label (dim1) and the equal arc poloidal angle (mod(index,10)=2) (dim2) 13) inverse_psi_polar : Flux surface type with psi as radial label (dim1) and the polar poloidal angle (mod(index,10)=3) (dim2); could be non-equidistant 14) inverse_psi_straight_field_line_fourier : Flux surface type with psi as radial label (dim1) and Fourier modes in the straight-field line poloidal angle (mod(index,10)=4) (dim2), could be non-equidistant; magnetic axis as centre of grid; following the COCOS=11 convention 15) inverse_psi_equal_arc_fourier : Flux surface type with psi as radial label (dim1) and Fourier modes in the equal arc poloidal angle (mod(index,10)=5) (dim2) 16) inverse_psi_polar_fourier : Flux surface type with psi as radial label (dim1) and Fourier modes in the polar poloidal angle (mod(index,10)=6) (dim2); could be non-equidistant 21) inverse_rhopolnorm_straight_field_line : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and the straight-field line poloidal angle (dim2) 22) inverse_rhopolnorm_equal_arc : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and the equal arc poloidal angle (dim2) 23) inverse_rhopolnorm_polar : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and the polar poloidal angle (dim2) 24) inverse_rhopolnorm_straight_field_line_fourier : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and Fourier modes in the straight-field line poloidal angle (dim2) 25) inverse_rhopolnorm_equal_arc_fourier : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and Fourier modes in the equal arc poloidal angle (dim2) 26) inverse_rhopolnorm_polar_fourier : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and Fourier modes in the polar poloidal angle (dim2) 31) inverse_rhotornorm_straight_field_line : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the straight-field line poloidal angle (dim2) 32) inverse_rhotornorm_equal_arc : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the equal arc poloidal angle (dim2) 33) inverse_rhotornorm_polar : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the polar poloidal angle (dim2) 34) inverse_rhotornorm_straight_field_line_fourier : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in the straight-field line poloidal angle (dim2) 35) inverse_rhotornorm_equal_arc_fourier : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in the equal arc poloidal angle (dim2) 36) inverse_rhotornorm_polar_fourier : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in the polar poloidal angle (dim2) 41) inverse_rhopol_straight_field_line : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the straight-field line poloidal angle (dim2) 42) inverse_rhopol_equal_arc : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the equal arc poloidal angle (dim2) 43) inverse_rhopol_polar : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the polar poloidal angle (dim2) 44) inverse_rhopol_straight_field_line_fourier : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in the straight-field line poloidal angle (dim2) 45) inverse_rhopol_equal_arc_fourier : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in the equal arc poloidal angle (dim2) 46) inverse_rhopol_polar_fourier : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in the polar poloidal angle (dim2) 51) inverse_rhotor_straight_field_line : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and the straight-field line poloidal angle (dim2) 52) inverse_rhotor_equal_arc : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and the equal arc poloidal angle (dim2) 53) inverse_rhotor_polar : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and the polar poloidal angle (dim2) 54) inverse_rhotor_straight_field_line_fourier : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and Fourier modes in the straight-field line poloidal angle (dim2) 55) inverse_rhotor_equal_arc_fourier : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and Fourier modes in the equal arc poloidal angle (dim2) 56) inverse_rhotor_polar_fourier : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and Fourier modes in the polar poloidal angle (dim2) 91) irregular_rz_na : Irregular grid, thus give list of vertices in dim1(1:ndim1), dim2(1:ndim1) and then all fields are on values(1:ndim1,1)
mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid_type.description (alpha)		STR_0D		Verbose description
mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid_type.index (alpha)		INT_0D		Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index.
mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid_type.name (alpha)		STR_0D		Short string identifier
mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.jacobian (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid.dim2]	FLT_2D (uncertain)	mixed	Absolute value of the jacobian of the coordinate system
mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.r (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid.dim2]	FLT_2D (uncertain)	m	Values of the major radius on the grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.tensor_contravariant (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid.dim2, 1...3, 1...3]	FLT_4D (uncertain)	mixed	Contravariant metric tensor on every point of the grid described by grid_type
mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.tensor_covariant (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid.dim2, 1...3, 1...3]	FLT_4D (uncertain)	mixed	Covariant metric tensor on every point of the grid described by grid_type
mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.z (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.coordinate_system.grid.dim2]	FLT_2D (uncertain)	m	Values of the Height on the grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.displacement_parallel (alpha)		STRUCTURE	m	Parallel displacement of the modes
mhd_linear.time_slice[:].toroidal_mode[:].plasma.displacement_parallel.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	m	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.displacement_parallel.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	m	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.displacement_parallel.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	m	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.displacement_parallel.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	m	Real part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.displacement_perpendicular (alpha)		STRUCTURE	m	Perpendicular displacement of the modes
mhd_linear.time_slice[:].toroidal_mode[:].plasma.displacement_perpendicular.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	m	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.displacement_perpendicular.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	m	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.displacement_perpendicular.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	m	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.displacement_perpendicular.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	m	Real part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid (alpha)		STRUCTURE		Definition of the 2D grid (the content of dim1 and dim2 is defined by the selected grid_type)
mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1 (alpha)	[1...N]	FLT_1D (uncertain)	mixed	First dimension values
mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2 (alpha)	[1...N]	FLT_1D (uncertain)	mixed	Second dimension values
mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.volume_element (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	m^3	Elementary plasma volume of plasma enclosed in the cell formed by the nodes [dim1(i) dim2(j)], [dim1(i+1) dim2(j)], [dim1(i) dim2(j+1)] and [dim1(i+1) dim2(j+1)]
mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid_type (alpha)		STRUCTURE		Selection of one of a set of grid types 1) rectangular : Cylindrical R,Z ala eqdsk (R=dim1, Z=dim2). In this case the position arrays should not be filled since they are redundant with grid/dim1 and dim2. 2) inverse : Rhopolar_polar 2D polar coordinates (rho=dim1, theta=dim2) with magnetic axis as centre of grid; theta and values following the COCOS=11 convention; the polar angle is theta=atan2(z-zaxis,r-raxis) 11) inverse_psi_straight_field_line : Flux surface type with psi as radial label (dim1) and the straight-field line poloidal angle (mod(index,10)=1) (dim2); could be non-equidistant; magnetic axis as centre of grid; following the COCOS=11 convention 12) inverse_psi_equal_arc : Flux surface type with psi as radial label (dim1) and the equal arc poloidal angle (mod(index,10)=2) (dim2) 13) inverse_psi_polar : Flux surface type with psi as radial label (dim1) and the polar poloidal angle (mod(index,10)=3) (dim2); could be non-equidistant 14) inverse_psi_straight_field_line_fourier : Flux surface type with psi as radial label (dim1) and Fourier modes in the straight-field line poloidal angle (mod(index,10)=4) (dim2), could be non-equidistant; magnetic axis as centre of grid; following the COCOS=11 convention 15) inverse_psi_equal_arc_fourier : Flux surface type with psi as radial label (dim1) and Fourier modes in the equal arc poloidal angle (mod(index,10)=5) (dim2) 16) inverse_psi_polar_fourier : Flux surface type with psi as radial label (dim1) and Fourier modes in the polar poloidal angle (mod(index,10)=6) (dim2); could be non-equidistant 21) inverse_rhopolnorm_straight_field_line : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and the straight-field line poloidal angle (dim2) 22) inverse_rhopolnorm_equal_arc : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and the equal arc poloidal angle (dim2) 23) inverse_rhopolnorm_polar : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and the polar poloidal angle (dim2) 24) inverse_rhopolnorm_straight_field_line_fourier : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and Fourier modes in the straight-field line poloidal angle (dim2) 25) inverse_rhopolnorm_equal_arc_fourier : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and Fourier modes in the equal arc poloidal angle (dim2) 26) inverse_rhopolnorm_polar_fourier : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and Fourier modes in the polar poloidal angle (dim2) 31) inverse_rhotornorm_straight_field_line : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the straight-field line poloidal angle (dim2) 32) inverse_rhotornorm_equal_arc : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the equal arc poloidal angle (dim2) 33) inverse_rhotornorm_polar : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the polar poloidal angle (dim2) 34) inverse_rhotornorm_straight_field_line_fourier : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in the straight-field line poloidal angle (dim2) 35) inverse_rhotornorm_equal_arc_fourier : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in the equal arc poloidal angle (dim2) 36) inverse_rhotornorm_polar_fourier : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in the polar poloidal angle (dim2) 41) inverse_rhopol_straight_field_line : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the straight-field line poloidal angle (dim2) 42) inverse_rhopol_equal_arc : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the equal arc poloidal angle (dim2) 43) inverse_rhopol_polar : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the polar poloidal angle (dim2) 44) inverse_rhopol_straight_field_line_fourier : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in the straight-field line poloidal angle (dim2) 45) inverse_rhopol_equal_arc_fourier : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in the equal arc poloidal angle (dim2) 46) inverse_rhopol_polar_fourier : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in the polar poloidal angle (dim2) 51) inverse_rhotor_straight_field_line : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and the straight-field line poloidal angle (dim2) 52) inverse_rhotor_equal_arc : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and the equal arc poloidal angle (dim2) 53) inverse_rhotor_polar : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and the polar poloidal angle (dim2) 54) inverse_rhotor_straight_field_line_fourier : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and Fourier modes in the straight-field line poloidal angle (dim2) 55) inverse_rhotor_equal_arc_fourier : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and Fourier modes in the equal arc poloidal angle (dim2) 56) inverse_rhotor_polar_fourier : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and Fourier modes in the polar poloidal angle (dim2) 91) irregular_rz_na : Irregular grid, thus give list of vertices in dim1(1:ndim1), dim2(1:ndim1) and then all fields are on values(1:ndim1,1)
mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid_type.description (alpha)		STR_0D		Verbose description
mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid_type.index (alpha)		INT_0D		Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index.
mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid_type.name (alpha)		STR_0D		Short string identifier
mhd_linear.time_slice[:].toroidal_mode[:].plasma.mass_density_perturbed (alpha)		STRUCTURE	kg.m^-3	Perturbed mass density for given toroidal mode number
mhd_linear.time_slice[:].toroidal_mode[:].plasma.mass_density_perturbed.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	kg.m^-3	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.mass_density_perturbed.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	kg.m^-3	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.mass_density_perturbed.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	kg.m^-3	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.mass_density_perturbed.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	kg.m^-3	Real part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.ntv (alpha)		STRUCTURE		Neoclassical toroidal viscosity tensor
mhd_linear.time_slice[:].toroidal_mode[:].plasma.ntv.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, 1...N, 1...N]	FLT_3D (uncertain)	N.m^-2	Imaginary part of the stress tensor, for various radial positions
mhd_linear.time_slice[:].toroidal_mode[:].plasma.ntv.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, 1...N, 1...N]	FLT_3D (uncertain)	N.m^-2	Real part of the stress tensor, for various radial positions
mhd_linear.time_slice[:].toroidal_mode[:].plasma.phi_potential_perturbed (alpha)		STRUCTURE	V	Perturbed electrostatic potential for given toroidal mode number
mhd_linear.time_slice[:].toroidal_mode[:].plasma.phi_potential_perturbed.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	V	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.phi_potential_perturbed.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	V	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.phi_potential_perturbed.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	V	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.phi_potential_perturbed.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	V	Real part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.pressure_perturbed (alpha)		STRUCTURE	Pa	Perturbed pressure for given toroidal mode number
mhd_linear.time_slice[:].toroidal_mode[:].plasma.pressure_perturbed.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	Pa	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.pressure_perturbed.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	Pa	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.pressure_perturbed.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	Pa	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.pressure_perturbed.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	Pa	Real part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.psi_potential_perturbed (alpha)		STRUCTURE	V	Perturbed electromagnetic super-potential for given toroidal mode number, see ref [Antonsen/Lane Phys Fluids 23(6) 1980, formula 34], so that A_field_parallel=1/(i*2pi*frequency) (grad psi_potential)_parallel
mhd_linear.time_slice[:].toroidal_mode[:].plasma.psi_potential_perturbed.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	V	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.psi_potential_perturbed.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	V	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.psi_potential_perturbed.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	V	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.psi_potential_perturbed.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	V	Real part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.stress_maxwell (alpha)		STRUCTURE		Maxwell stress tensor
mhd_linear.time_slice[:].toroidal_mode[:].plasma.stress_maxwell.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, 1...N, 1...N]	FLT_3D (uncertain)	N.m^-2	Imaginary part of the stress tensor, for various radial positions
mhd_linear.time_slice[:].toroidal_mode[:].plasma.stress_maxwell.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, 1...N, 1...N]	FLT_3D (uncertain)	N.m^-2	Real part of the stress tensor, for various radial positions
mhd_linear.time_slice[:].toroidal_mode[:].plasma.stress_reynolds (alpha)		STRUCTURE		Reynolds stress tensor
mhd_linear.time_slice[:].toroidal_mode[:].plasma.stress_reynolds.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, 1...N, 1...N]	FLT_3D (uncertain)	N.m^-2	Imaginary part of the stress tensor, for various radial positions
mhd_linear.time_slice[:].toroidal_mode[:].plasma.stress_reynolds.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, 1...N, 1...N]	FLT_3D (uncertain)	N.m^-2	Real part of the stress tensor, for various radial positions
mhd_linear.time_slice[:].toroidal_mode[:].plasma.tau_alfven (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1]	FLT_1D (uncertain)	s	Alven time=R/vA=R0 sqrt(mi ni(rho))/B0
mhd_linear.time_slice[:].toroidal_mode[:].plasma.tau_resistive (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1]	FLT_1D (uncertain)	s	Resistive time = mu_0 rho*rho/1.22/eta_neo
mhd_linear.time_slice[:].toroidal_mode[:].plasma.temperature_perturbed (alpha)		STRUCTURE	eV	Perturbed temperature for given toroidal mode number
mhd_linear.time_slice[:].toroidal_mode[:].plasma.temperature_perturbed.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	eV	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.temperature_perturbed.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	eV	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.temperature_perturbed.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	eV	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.temperature_perturbed.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	eV	Real part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed (alpha)		STRUCTURE	m/s	Pertubed velocity for given toroidal mode number
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate1 (alpha)		STRUCTURE	m/s	First coordinate (radial)
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate1.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	m/s	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate1.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	m/s	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate1.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	m/s	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate1.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	m/s	Real part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate2 (alpha)		STRUCTURE	m/s	Second coordinate (poloidal)
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate2.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	m/s	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate2.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	m/s	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate2.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	m/s	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate2.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	m/s	Real part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate3 (alpha)		STRUCTURE	m/s	Third coordinate (toroidal)
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate3.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	m/s	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate3.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2, 1...N]	FLT_3D (uncertain)	m/s	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate3.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	m/s	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate3.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2]	FLT_2D (uncertain)	m/s	Real part
mhd_linear.time_slice[:].toroidal_mode[:].radial_mode_number (alpha)		FLT_0D (uncertain)	-	Radial mode number
mhd_linear.time_slice[:].toroidal_mode[:].vacuum (alpha)		STRUCTURE		MHD modes in the vacuum
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.a_field_perturbed (alpha)		STRUCTURE	T.m	Pertubed vector potential for given toroidal mode number
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.a_field_perturbed.coordinate1 (alpha)		STRUCTURE	T.m	First coordinate (radial)
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.a_field_perturbed.coordinate1.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2, 1...N]	FLT_3D (uncertain)	T.m	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.a_field_perturbed.coordinate1.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2, 1...N]	FLT_3D (uncertain)	T.m	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.a_field_perturbed.coordinate1.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2]	FLT_2D (uncertain)	T.m	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.a_field_perturbed.coordinate1.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2]	FLT_2D (uncertain)	T.m	Real part
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.a_field_perturbed.coordinate2 (alpha)		STRUCTURE	T.m	Second coordinate (poloidal)
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.a_field_perturbed.coordinate2.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2, 1...N]	FLT_3D (uncertain)	T.m	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.a_field_perturbed.coordinate2.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2, 1...N]	FLT_3D (uncertain)	T.m	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.a_field_perturbed.coordinate2.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2]	FLT_2D (uncertain)	T.m	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.a_field_perturbed.coordinate2.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2]	FLT_2D (uncertain)	T.m	Real part
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.a_field_perturbed.coordinate3 (alpha)		STRUCTURE	T.m	Third coordinate (toroidal)
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.a_field_perturbed.coordinate3.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2, 1...N]	FLT_3D (uncertain)	T.m	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.a_field_perturbed.coordinate3.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2, 1...N]	FLT_3D (uncertain)	T.m	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.a_field_perturbed.coordinate3.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2]	FLT_2D (uncertain)	T.m	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.a_field_perturbed.coordinate3.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2]	FLT_2D (uncertain)	T.m	Real part
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.b_field_perturbed (alpha)		STRUCTURE	T	Pertubed magnetic field for given toroidal mode number
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.b_field_perturbed.coordinate1 (alpha)		STRUCTURE	T	First coordinate (radial)
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.b_field_perturbed.coordinate1.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2, 1...N]	FLT_3D (uncertain)	T	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.b_field_perturbed.coordinate1.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2, 1...N]	FLT_3D (uncertain)	T	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.b_field_perturbed.coordinate1.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2]	FLT_2D (uncertain)	T	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.b_field_perturbed.coordinate1.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2]	FLT_2D (uncertain)	T	Real part
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.b_field_perturbed.coordinate2 (alpha)		STRUCTURE	T	Second coordinate (poloidal)
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.b_field_perturbed.coordinate2.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2, 1...N]	FLT_3D (uncertain)	T	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.b_field_perturbed.coordinate2.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2, 1...N]	FLT_3D (uncertain)	T	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.b_field_perturbed.coordinate2.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2]	FLT_2D (uncertain)	T	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.b_field_perturbed.coordinate2.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2]	FLT_2D (uncertain)	T	Real part
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.b_field_perturbed.coordinate3 (alpha)		STRUCTURE	T	Third coordinate (toroidal)
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.b_field_perturbed.coordinate3.coefficients_imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2, 1...N]	FLT_3D (uncertain)	T	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.b_field_perturbed.coordinate3.coefficients_real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2, 1...N]	FLT_3D (uncertain)	T	Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.b_field_perturbed.coordinate3.imaginary (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2]	FLT_2D (uncertain)	T	Imaginary part
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.b_field_perturbed.coordinate3.real (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2]	FLT_2D (uncertain)	T	Real part
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system (alpha)		STRUCTURE		Flux surface coordinate system of the equilibrium used for the MHD calculation on a square grid of flux and poloidal angle
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid (alpha)		STRUCTURE		Definition of the 2D grid
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid.dim1 (alpha)	[1...N]	FLT_1D (uncertain)	mixed	First dimension values
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid.dim2 (alpha)	[1...N]	FLT_1D (uncertain)	mixed	Second dimension values
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid.volume_element (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid.dim2]	FLT_2D (uncertain)	m^3	Elementary plasma volume of plasma enclosed in the cell formed by the nodes [dim1(i) dim2(j)], [dim1(i+1) dim2(j)], [dim1(i) dim2(j+1)] and [dim1(i+1) dim2(j+1)]
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid_type (alpha)		STRUCTURE		Selection of one of a set of grid types 1) rectangular : Cylindrical R,Z ala eqdsk (R=dim1, Z=dim2). In this case the position arrays should not be filled since they are redundant with grid/dim1 and dim2. 2) inverse : Rhopolar_polar 2D polar coordinates (rho=dim1, theta=dim2) with magnetic axis as centre of grid; theta and values following the COCOS=11 convention; the polar angle is theta=atan2(z-zaxis,r-raxis) 11) inverse_psi_straight_field_line : Flux surface type with psi as radial label (dim1) and the straight-field line poloidal angle (mod(index,10)=1) (dim2); could be non-equidistant; magnetic axis as centre of grid; following the COCOS=11 convention 12) inverse_psi_equal_arc : Flux surface type with psi as radial label (dim1) and the equal arc poloidal angle (mod(index,10)=2) (dim2) 13) inverse_psi_polar : Flux surface type with psi as radial label (dim1) and the polar poloidal angle (mod(index,10)=3) (dim2); could be non-equidistant 14) inverse_psi_straight_field_line_fourier : Flux surface type with psi as radial label (dim1) and Fourier modes in the straight-field line poloidal angle (mod(index,10)=4) (dim2), could be non-equidistant; magnetic axis as centre of grid; following the COCOS=11 convention 15) inverse_psi_equal_arc_fourier : Flux surface type with psi as radial label (dim1) and Fourier modes in the equal arc poloidal angle (mod(index,10)=5) (dim2) 16) inverse_psi_polar_fourier : Flux surface type with psi as radial label (dim1) and Fourier modes in the polar poloidal angle (mod(index,10)=6) (dim2); could be non-equidistant 21) inverse_rhopolnorm_straight_field_line : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and the straight-field line poloidal angle (dim2) 22) inverse_rhopolnorm_equal_arc : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and the equal arc poloidal angle (dim2) 23) inverse_rhopolnorm_polar : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and the polar poloidal angle (dim2) 24) inverse_rhopolnorm_straight_field_line_fourier : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and Fourier modes in the straight-field line poloidal angle (dim2) 25) inverse_rhopolnorm_equal_arc_fourier : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and Fourier modes in the equal arc poloidal angle (dim2) 26) inverse_rhopolnorm_polar_fourier : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and Fourier modes in the polar poloidal angle (dim2) 31) inverse_rhotornorm_straight_field_line : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the straight-field line poloidal angle (dim2) 32) inverse_rhotornorm_equal_arc : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the equal arc poloidal angle (dim2) 33) inverse_rhotornorm_polar : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the polar poloidal angle (dim2) 34) inverse_rhotornorm_straight_field_line_fourier : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in the straight-field line poloidal angle (dim2) 35) inverse_rhotornorm_equal_arc_fourier : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in the equal arc poloidal angle (dim2) 36) inverse_rhotornorm_polar_fourier : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in the polar poloidal angle (dim2) 41) inverse_rhopol_straight_field_line : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the straight-field line poloidal angle (dim2) 42) inverse_rhopol_equal_arc : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the equal arc poloidal angle (dim2) 43) inverse_rhopol_polar : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the polar poloidal angle (dim2) 44) inverse_rhopol_straight_field_line_fourier : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in the straight-field line poloidal angle (dim2) 45) inverse_rhopol_equal_arc_fourier : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in the equal arc poloidal angle (dim2) 46) inverse_rhopol_polar_fourier : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in the polar poloidal angle (dim2) 51) inverse_rhotor_straight_field_line : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and the straight-field line poloidal angle (dim2) 52) inverse_rhotor_equal_arc : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and the equal arc poloidal angle (dim2) 53) inverse_rhotor_polar : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and the polar poloidal angle (dim2) 54) inverse_rhotor_straight_field_line_fourier : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and Fourier modes in the straight-field line poloidal angle (dim2) 55) inverse_rhotor_equal_arc_fourier : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and Fourier modes in the equal arc poloidal angle (dim2) 56) inverse_rhotor_polar_fourier : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and Fourier modes in the polar poloidal angle (dim2) 91) irregular_rz_na : Irregular grid, thus give list of vertices in dim1(1:ndim1), dim2(1:ndim1) and then all fields are on values(1:ndim1,1)
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid_type.description (alpha)		STR_0D		Verbose description
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid_type.index (alpha)		INT_0D		Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index.
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid_type.name (alpha)		STR_0D		Short string identifier
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.jacobian (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid.dim2]	FLT_2D (uncertain)	mixed	Absolute value of the jacobian of the coordinate system
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.r (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid.dim2]	FLT_2D (uncertain)	m	Values of the major radius on the grid
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.tensor_contravariant (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid.dim2, 1...3, 1...3]	FLT_4D (uncertain)	mixed	Contravariant metric tensor on every point of the grid described by grid_type
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.tensor_covariant (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid.dim2, 1...3, 1...3]	FLT_4D (uncertain)	mixed	Covariant metric tensor on every point of the grid described by grid_type
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.z (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.coordinate_system.grid.dim2]	FLT_2D (uncertain)	m	Values of the Height on the grid
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid (alpha)		STRUCTURE		Definition of the 2D grid (the content of dim1 and dim2 is defined by the selected grid_type)
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1 (alpha)	[1...N]	FLT_1D (uncertain)	mixed	First dimension values
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2 (alpha)	[1...N]	FLT_1D (uncertain)	mixed	Second dimension values
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.volume_element (alpha)	[mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim1, mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid.dim2]	FLT_2D (uncertain)	m^3	Elementary plasma volume of plasma enclosed in the cell formed by the nodes [dim1(i) dim2(j)], [dim1(i+1) dim2(j)], [dim1(i) dim2(j+1)] and [dim1(i+1) dim2(j+1)]
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid_type (alpha)		STRUCTURE		Selection of one of a set of grid types 1) rectangular : Cylindrical R,Z ala eqdsk (R=dim1, Z=dim2). In this case the position arrays should not be filled since they are redundant with grid/dim1 and dim2. 2) inverse : Rhopolar_polar 2D polar coordinates (rho=dim1, theta=dim2) with magnetic axis as centre of grid; theta and values following the COCOS=11 convention; the polar angle is theta=atan2(z-zaxis,r-raxis) 11) inverse_psi_straight_field_line : Flux surface type with psi as radial label (dim1) and the straight-field line poloidal angle (mod(index,10)=1) (dim2); could be non-equidistant; magnetic axis as centre of grid; following the COCOS=11 convention 12) inverse_psi_equal_arc : Flux surface type with psi as radial label (dim1) and the equal arc poloidal angle (mod(index,10)=2) (dim2) 13) inverse_psi_polar : Flux surface type with psi as radial label (dim1) and the polar poloidal angle (mod(index,10)=3) (dim2); could be non-equidistant 14) inverse_psi_straight_field_line_fourier : Flux surface type with psi as radial label (dim1) and Fourier modes in the straight-field line poloidal angle (mod(index,10)=4) (dim2), could be non-equidistant; magnetic axis as centre of grid; following the COCOS=11 convention 15) inverse_psi_equal_arc_fourier : Flux surface type with psi as radial label (dim1) and Fourier modes in the equal arc poloidal angle (mod(index,10)=5) (dim2) 16) inverse_psi_polar_fourier : Flux surface type with psi as radial label (dim1) and Fourier modes in the polar poloidal angle (mod(index,10)=6) (dim2); could be non-equidistant 21) inverse_rhopolnorm_straight_field_line : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and the straight-field line poloidal angle (dim2) 22) inverse_rhopolnorm_equal_arc : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and the equal arc poloidal angle (dim2) 23) inverse_rhopolnorm_polar : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and the polar poloidal angle (dim2) 24) inverse_rhopolnorm_straight_field_line_fourier : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and Fourier modes in the straight-field line poloidal angle (dim2) 25) inverse_rhopolnorm_equal_arc_fourier : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and Fourier modes in the equal arc poloidal angle (dim2) 26) inverse_rhopolnorm_polar_fourier : Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1) and Fourier modes in the polar poloidal angle (dim2) 31) inverse_rhotornorm_straight_field_line : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the straight-field line poloidal angle (dim2) 32) inverse_rhotornorm_equal_arc : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the equal arc poloidal angle (dim2) 33) inverse_rhotornorm_polar : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the polar poloidal angle (dim2) 34) inverse_rhotornorm_straight_field_line_fourier : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in the straight-field line poloidal angle (dim2) 35) inverse_rhotornorm_equal_arc_fourier : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in the equal arc poloidal angle (dim2) 36) inverse_rhotornorm_polar_fourier : Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in the polar poloidal angle (dim2) 41) inverse_rhopol_straight_field_line : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the straight-field line poloidal angle (dim2) 42) inverse_rhopol_equal_arc : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the equal arc poloidal angle (dim2) 43) inverse_rhopol_polar : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the polar poloidal angle (dim2) 44) inverse_rhopol_straight_field_line_fourier : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in the straight-field line poloidal angle (dim2) 45) inverse_rhopol_equal_arc_fourier : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in the equal arc poloidal angle (dim2) 46) inverse_rhopol_polar_fourier : Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in the polar poloidal angle (dim2) 51) inverse_rhotor_straight_field_line : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and the straight-field line poloidal angle (dim2) 52) inverse_rhotor_equal_arc : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and the equal arc poloidal angle (dim2) 53) inverse_rhotor_polar : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and the polar poloidal angle (dim2) 54) inverse_rhotor_straight_field_line_fourier : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and Fourier modes in the straight-field line poloidal angle (dim2) 55) inverse_rhotor_equal_arc_fourier : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and Fourier modes in the equal arc poloidal angle (dim2) 56) inverse_rhotor_polar_fourier : Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux, and Fourier modes in the polar poloidal angle (dim2) 91) irregular_rz_na : Irregular grid, thus give list of vertices in dim1(1:ndim1), dim2(1:ndim1) and then all fields are on values(1:ndim1,1)
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid_type.description (alpha)		STR_0D		Verbose description
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid_type.index (alpha)		INT_0D		Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index.
mhd_linear.time_slice[:].toroidal_mode[:].vacuum.grid_type.name (alpha)		STR_0D		Short string identifier
mhd_linear.vacuum_toroidal_field (alpha)		STRUCTURE		Characteristics of the vacuum toroidal field (used in rho_tor definition and in the normalization of current densities)
mhd_linear.vacuum_toroidal_field.b0 (alpha)	[mhd_linear.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.
mhd_linear.vacuum_toroidal_field.r0 (alpha)		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)