core_profiles¶
Core plasma profiles
Maximum occurrences (MDS+ backend only): 15
New in version 3.1.0: lifecycle status active
Changed in version 4.2.0.
ids_propertiesstructure¶
See common IDS structure reference: ids_properties.
profiles_1d(itime)AoS¶Core plasma radial profiles for various time slices
Core plasma radial profiles for various time slices
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profiles_1d(itime)/gridstructure¶Radial grid
Radial grid
profiles_1d(itime)/grid/rho_tor_norm(:) ⇹1FLT_1D¶Normalized toroidal flux coordinate. […] (click to expand)
Normalized toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation, see time_slice/boundary/b_flux_pol_norm in the equilibrium IDS)
Alternatives for this coordinate
The following items may be used as a coordinate instead of rho_tor_norm:
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profiles_1d(itime)/grid/rho_tor(:) ⇹mFLT_1D¶Toroidal flux coordinate = sqrt(phi/(pi\*b0)), where the toroidal […] (click to expand)
Toroidal flux coordinate = sqrt(phi/(pi*b0)), where the toroidal magnetic field, b0, corresponds to that stored in vacuum_toroidal_field/b0 and pi can be found in the IMAS constants
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profiles_1d(itime)/grid/rho_pol_norm(:) ⇹1FLT_1D¶Normalized poloidal flux coordinate = sqrt((psi(rho)-psi(magnetic_axis)) […] (click to expand)
Normalized poloidal flux coordinate = sqrt((psi(rho)-psi(magnetic_axis)) / (psi(LCFS)-psi(magnetic_axis)))
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profiles_1d(itime)/grid/psi(:) ⇹WbFLT_1D¶Poloidal magnetic flux. […] (click to expand)
Poloidal magnetic flux. Integral of magnetic field passing through a contour defined by the intersection of a flux surface passing through the point of interest and a Z=constant plane. If the integration surface is flat, the surface normal vector is in the increasing vertical coordinate direction, Z, namely upwards.
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profiles_1d(itime)/grid/volume(:) ⇹m^3FLT_1D¶Volume enclosed inside the magnetic surface
Volume enclosed inside the magnetic surface
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profiles_1d(itime)/grid/area(:) ⇹m^2FLT_1D¶Cross-sectional area of the flux surface
Cross-sectional area of the flux surface
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profiles_1d(itime)/grid/surface(:) ⇹m^2FLT_1D¶Surface area of the toroidal flux surface
Surface area of the toroidal flux surface
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profiles_1d(itime)/grid/psi_magnetic_axis ⇹WbFLT_0D¶Value of the poloidal magnetic flux at the magnetic axis (useful […] (click to expand)
Value of the poloidal magnetic flux at the magnetic axis (useful to normalize the psi array values when the radial grid doesn’t go from the magnetic axis to the plasma boundary)
profiles_1d(itime)/grid/psi_boundary ⇹WbFLT_0D¶Value of the poloidal magnetic flux at the plasma boundary (useful […] (click to expand)
Value of the poloidal magnetic flux at the plasma boundary (useful to normalize the psi array values when the radial grid doesn’t go from the magnetic axis to the plasma boundary)
profiles_1d(itime)/electronsstructure¶Quantities related to the electrons
Quantities related to the electrons
profiles_1d(itime)/electrons/temperature_validityINT_0D¶Indicator of the validity of the temperature profile. […] (click to expand)
Indicator of the validity of the temperature profile. 0: valid from automated processing, 1: valid and certified by the RO; - 1 means problem identified in the data processing (request verification by the RO), -2: invalid data, should not be used
profiles_1d(itime)/electrons/temperature_fiteVstructure¶Information on the fit used to obtain the temperature profile
Information on the fit used to obtain the temperature profile
profiles_1d(itime)/electrons/temperature_fit/measured(:) ⇹mixedFLT_1D¶Measured values
Measured values
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profiles_1d(itime)/electrons/temperature_fit/source(:)STR_1D¶Path to the source data for each measurement in the IMAS data […] (click to expand)
Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS
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profiles_1d(itime)/electrons/temperature_fit/time_measurement(:) ⇹sFLT_1D¶Exact time slices used from the time array of the measurement […] (click to expand)
Exact time slices used from the time array of the measurement source data. The time slice is indicated for each measurement point considered in the fit since measurements may come from different and thus asynchronous diagnostics. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used
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profiles_1d(itime)/electrons/temperature_fit/time_measurement_slice_methodstructure¶Method used to slice the data : index = 0 means using exact time […] (click to expand)
Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, …
profiles_1d(itime)/electrons/temperature_fit/time_measurement_slice_method/nameSTR_0D¶Short string identifier
Short string identifier
profiles_1d(itime)/electrons/temperature_fit/time_measurement_width(:) ⇹sFLT_1D¶In case the measurements are averaged over a time interval, this […] (click to expand)
In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn’t use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement.
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profiles_1d(itime)/electrons/temperature_fit/local(:)INT_1D¶Integer flag : 1 means local measurement, 0 means line-integrated […] (click to expand)
Integer flag : 1 means local measurement, 0 means line-integrated measurement
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profiles_1d(itime)/electrons/temperature_fit/rho_tor_norm(:) ⇹1FLT_1D¶Normalized toroidal flux coordinate of each measurement (local […] (click to expand)
Normalized toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
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profiles_1d(itime)/electrons/temperature_fit/rho_pol_norm(:) ⇹1FLT_1D¶Normalized poloidal flux coordinate of each measurement (local […] (click to expand)
Normalized poloidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
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New in version >4.1.1.
profiles_1d(itime)/electrons/temperature_fit/weight(:) ⇹1FLT_1D¶Weight given to each measured value
Weight given to each measured value
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profiles_1d(itime)/electrons/temperature_fit/sigma(:) ⇹mixedFLT_1D¶Standard deviation of the measurement error
Standard deviation of the measurement error
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New in version >4.1.1.
profiles_1d(itime)/electrons/temperature_fit/reconstructed(:) ⇹mixedFLT_1D¶Value reconstructed from the fit
Value reconstructed from the fit
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profiles_1d(itime)/electrons/temperature_fit/chi_squared(:) ⇹1FLT_1D¶Squared error normalized by the weighted standard deviation considered […] (click to expand)
Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error
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profiles_1d(itime)/electrons/density(:) ⇹m^-3FLT_1D¶Density (thermal+non-thermal)
Density (thermal+non-thermal)
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profiles_1d(itime)/electrons/density_validityINT_0D¶Indicator of the validity of the density profile. […] (click to expand)
Indicator of the validity of the density profile. 0: valid from automated processing, 1: valid and certified by the RO; - 1 means problem identified in the data processing (request verification by the RO), -2: invalid data, should not be used
profiles_1d(itime)/electrons/density_fitm^-3structure¶Information on the fit used to obtain the density profile
Information on the fit used to obtain the density profile
profiles_1d(itime)/electrons/density_fit/measured(:) ⇹mixedFLT_1D¶Measured values
Measured values
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profiles_1d(itime)/electrons/density_fit/source(:)STR_1D¶Path to the source data for each measurement in the IMAS data […] (click to expand)
Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS
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profiles_1d(itime)/electrons/density_fit/time_measurement(:) ⇹sFLT_1D¶Exact time slices used from the time array of the measurement […] (click to expand)
Exact time slices used from the time array of the measurement source data. The time slice is indicated for each measurement point considered in the fit since measurements may come from different and thus asynchronous diagnostics. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used
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profiles_1d(itime)/electrons/density_fit/time_measurement_slice_methodstructure¶Method used to slice the data : index = 0 means using exact time […] (click to expand)
Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, …
profiles_1d(itime)/electrons/density_fit/time_measurement_slice_method/nameSTR_0D¶Short string identifier
Short string identifier
profiles_1d(itime)/electrons/density_fit/time_measurement_width(:) ⇹sFLT_1D¶In case the measurements are averaged over a time interval, this […] (click to expand)
In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn’t use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement.
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profiles_1d(itime)/electrons/density_fit/local(:)INT_1D¶Integer flag : 1 means local measurement, 0 means line-integrated […] (click to expand)
Integer flag : 1 means local measurement, 0 means line-integrated measurement
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profiles_1d(itime)/electrons/density_fit/rho_tor_norm(:) ⇹1FLT_1D¶Normalized toroidal flux coordinate of each measurement (local […] (click to expand)
Normalized toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
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profiles_1d(itime)/electrons/density_fit/rho_pol_norm(:) ⇹1FLT_1D¶Normalized poloidal flux coordinate of each measurement (local […] (click to expand)
Normalized poloidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
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New in version >4.1.1.
profiles_1d(itime)/electrons/density_fit/weight(:) ⇹1FLT_1D¶Weight given to each measured value
Weight given to each measured value
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profiles_1d(itime)/electrons/density_fit/sigma(:) ⇹mixedFLT_1D¶Standard deviation of the measurement error
Standard deviation of the measurement error
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New in version >4.1.1.
profiles_1d(itime)/electrons/density_fit/reconstructed(:) ⇹mixedFLT_1D¶Value reconstructed from the fit
Value reconstructed from the fit
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profiles_1d(itime)/electrons/density_fit/chi_squared(:) ⇹1FLT_1D¶Squared error normalized by the weighted standard deviation considered […] (click to expand)
Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error
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profiles_1d(itime)/electrons/density_thermal(:) ⇹m^-3FLT_1D¶Density of thermal particles
Density of thermal particles
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profiles_1d(itime)/electrons/density_fast(:) ⇹m^-3FLT_1D¶Density of fast (non-thermal) particles
Density of fast (non-thermal) particles
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profiles_1d(itime)/electrons/pressure(:) ⇹PaFLT_1D¶Pressure (thermal+non-thermal)
Pressure (thermal+non-thermal)
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profiles_1d(itime)/electrons/pressure_thermal(:) ⇹PaFLT_1D¶Pressure (thermal) associated with random motion ~average((v-average(v))^2)
Pressure (thermal) associated with random motion ~average((v-average(v))^2)
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profiles_1d(itime)/electrons/pressure_fast_perpendicular(:) ⇹PaFLT_1D¶Fast (non-thermal) perpendicular pressure
Fast (non-thermal) perpendicular pressure
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profiles_1d(itime)/electrons/pressure_fast_parallel(:) ⇹PaFLT_1D¶Fast (non-thermal) parallel pressure
Fast (non-thermal) parallel pressure
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profiles_1d(itime)/ion(i1)AoS¶Quantities related to the different ion species, in the sense […] (click to expand)
Quantities related to the different ion species, in the sense of isonuclear or isomolecular sequences. Ionization states (or other types of states) must be differentiated at the state level below
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profiles_1d(itime)/ion(i1)/element(i2)AoS¶List of elements forming the atom or molecule
List of elements forming the atom or molecule
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profiles_1d(itime)/ion(i1)/z_ion ⇹eFLT_0D¶Ion charge (of the dominant ionization state; lumped ions are […] (click to expand)
Ion charge (of the dominant ionization state; lumped ions are allowed), volume averaged over plasma radius
profiles_1d(itime)/ion(i1)/nameSTR_0D¶String identifying ion (e.g. […] (click to expand)
String identifying ion (e.g. H, D, T, He, C, D2, …)
Changed in version 3.42.0: Renamed from label
profiles_1d(itime)/ion(i1)/neutral_indexINT_0D¶Index of the corresponding neutral species in the ../../neutral […] (click to expand)
Index of the corresponding neutral species in the ../../neutral array
profiles_1d(itime)/ion(i1)/z_ion_1d(:) ⇹1FLT_1D¶Average charge of the ion species (sum of states charge weighted […] (click to expand)
Average charge of the ion species (sum of states charge weighted by state density and divided by ion density)
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profiles_1d(itime)/ion(i1)/z_ion_square_1d(:) ⇹1FLT_1D¶Average square charge of the ion species (sum of states square […] (click to expand)
Average square charge of the ion species (sum of states square charge weighted by state density and divided by ion density)
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profiles_1d(itime)/ion(i1)/temperature(:) ⇹eVFLT_1D¶Temperature (average over charge states when multiple charge […] (click to expand)
Temperature (average over charge states when multiple charge states are considered)
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profiles_1d(itime)/ion(i1)/temperature_validityINT_0D¶Indicator of the validity of the temperature profile. […] (click to expand)
Indicator of the validity of the temperature profile. 0: valid from automated processing, 1: valid and certified by the RO; - 1 means problem identified in the data processing (request verification by the RO), -2: invalid data, should not be used
profiles_1d(itime)/ion(i1)/temperature_fiteVstructure¶Information on the fit used to obtain the temperature profile
Information on the fit used to obtain the temperature profile
profiles_1d(itime)/ion(i1)/temperature_fit/measured(:) ⇹mixedFLT_1D¶Measured values
Measured values
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profiles_1d(itime)/ion(i1)/temperature_fit/source(:)STR_1D¶Path to the source data for each measurement in the IMAS data […] (click to expand)
Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS
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profiles_1d(itime)/ion(i1)/temperature_fit/time_measurement(:) ⇹sFLT_1D¶Exact time slices used from the time array of the measurement […] (click to expand)
Exact time slices used from the time array of the measurement source data. The time slice is indicated for each measurement point considered in the fit since measurements may come from different and thus asynchronous diagnostics. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used
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profiles_1d(itime)/ion(i1)/temperature_fit/time_measurement_slice_methodstructure¶Method used to slice the data : index = 0 means using exact time […] (click to expand)
Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, …
profiles_1d(itime)/ion(i1)/temperature_fit/time_measurement_slice_method/nameSTR_0D¶Short string identifier
Short string identifier
profiles_1d(itime)/ion(i1)/temperature_fit/time_measurement_width(:) ⇹sFLT_1D¶In case the measurements are averaged over a time interval, this […] (click to expand)
In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn’t use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement.
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profiles_1d(itime)/ion(i1)/temperature_fit/local(:)INT_1D¶Integer flag : 1 means local measurement, 0 means line-integrated […] (click to expand)
Integer flag : 1 means local measurement, 0 means line-integrated measurement
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profiles_1d(itime)/ion(i1)/temperature_fit/rho_tor_norm(:) ⇹1FLT_1D¶Normalized toroidal flux coordinate of each measurement (local […] (click to expand)
Normalized toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
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profiles_1d(itime)/ion(i1)/temperature_fit/rho_pol_norm(:) ⇹1FLT_1D¶Normalized poloidal flux coordinate of each measurement (local […] (click to expand)
Normalized poloidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
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New in version >4.1.1.
profiles_1d(itime)/ion(i1)/temperature_fit/weight(:) ⇹1FLT_1D¶Weight given to each measured value
Weight given to each measured value
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profiles_1d(itime)/ion(i1)/temperature_fit/sigma(:) ⇹mixedFLT_1D¶Standard deviation of the measurement error
Standard deviation of the measurement error
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New in version >4.1.1.
profiles_1d(itime)/ion(i1)/temperature_fit/reconstructed(:) ⇹mixedFLT_1D¶Value reconstructed from the fit
Value reconstructed from the fit
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profiles_1d(itime)/ion(i1)/temperature_fit/chi_squared(:) ⇹1FLT_1D¶Squared error normalized by the weighted standard deviation considered […] (click to expand)
Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error
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profiles_1d(itime)/ion(i1)/density(:) ⇹m^-3FLT_1D¶Density (thermal+non-thermal) (sum over charge states when multiple […] (click to expand)
Density (thermal+non-thermal) (sum over charge states when multiple charge states are considered)
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profiles_1d(itime)/ion(i1)/density_validityINT_0D¶Indicator of the validity of the density profile. […] (click to expand)
Indicator of the validity of the density profile. 0: valid from automated processing, 1: valid and certified by the RO; - 1 means problem identified in the data processing (request verification by the RO), -2: invalid data, should not be used
profiles_1d(itime)/ion(i1)/density_fitm^-3structure¶Information on the fit used to obtain the density profile
Information on the fit used to obtain the density profile
profiles_1d(itime)/ion(i1)/density_fit/measured(:) ⇹mixedFLT_1D¶Measured values
Measured values
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profiles_1d(itime)/ion(i1)/density_fit/source(:)STR_1D¶Path to the source data for each measurement in the IMAS data […] (click to expand)
Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS
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profiles_1d(itime)/ion(i1)/density_fit/time_measurement(:) ⇹sFLT_1D¶Exact time slices used from the time array of the measurement […] (click to expand)
Exact time slices used from the time array of the measurement source data. The time slice is indicated for each measurement point considered in the fit since measurements may come from different and thus asynchronous diagnostics. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used
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profiles_1d(itime)/ion(i1)/density_fit/time_measurement_slice_methodstructure¶Method used to slice the data : index = 0 means using exact time […] (click to expand)
Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, …
profiles_1d(itime)/ion(i1)/density_fit/time_measurement_slice_method/nameSTR_0D¶Short string identifier
Short string identifier
profiles_1d(itime)/ion(i1)/density_fit/time_measurement_width(:) ⇹sFLT_1D¶In case the measurements are averaged over a time interval, this […] (click to expand)
In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn’t use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement.
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profiles_1d(itime)/ion(i1)/density_fit/local(:)INT_1D¶Integer flag : 1 means local measurement, 0 means line-integrated […] (click to expand)
Integer flag : 1 means local measurement, 0 means line-integrated measurement
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profiles_1d(itime)/ion(i1)/density_fit/rho_tor_norm(:) ⇹1FLT_1D¶Normalized toroidal flux coordinate of each measurement (local […] (click to expand)
Normalized toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
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profiles_1d(itime)/ion(i1)/density_fit/rho_pol_norm(:) ⇹1FLT_1D¶Normalized poloidal flux coordinate of each measurement (local […] (click to expand)
Normalized poloidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
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New in version >4.1.1.
profiles_1d(itime)/ion(i1)/density_fit/weight(:) ⇹1FLT_1D¶Weight given to each measured value
Weight given to each measured value
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profiles_1d(itime)/ion(i1)/density_fit/sigma(:) ⇹mixedFLT_1D¶Standard deviation of the measurement error
Standard deviation of the measurement error
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New in version >4.1.1.
profiles_1d(itime)/ion(i1)/density_fit/reconstructed(:) ⇹mixedFLT_1D¶Value reconstructed from the fit
Value reconstructed from the fit
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profiles_1d(itime)/ion(i1)/density_fit/chi_squared(:) ⇹1FLT_1D¶Squared error normalized by the weighted standard deviation considered […] (click to expand)
Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error
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profiles_1d(itime)/ion(i1)/density_thermal(:) ⇹m^-3FLT_1D¶Density (thermal) (sum over charge states when multiple charge […] (click to expand)
Density (thermal) (sum over charge states when multiple charge states are considered)
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profiles_1d(itime)/ion(i1)/density_fast(:) ⇹m^-3FLT_1D¶Density of fast (non-thermal) particles (sum over charge states […] (click to expand)
Density of fast (non-thermal) particles (sum over charge states when multiple charge states are considered)
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profiles_1d(itime)/ion(i1)/pressure(:) ⇹PaFLT_1D¶Pressure (thermal+non-thermal) (sum over charge states when multiple […] (click to expand)
Pressure (thermal+non-thermal) (sum over charge states when multiple charge states are considered)
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profiles_1d(itime)/ion(i1)/pressure_thermal(:) ⇹PaFLT_1D¶Pressure (thermal) associated with random motion ~average((v-average(v))^2) […] (click to expand)
Pressure (thermal) associated with random motion ~average((v-average(v))^2) (sum over charge states when multiple charge states are considered)
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profiles_1d(itime)/ion(i1)/pressure_fast_perpendicular(:) ⇹PaFLT_1D¶Fast (non-thermal) perpendicular pressure (sum over charge states […] (click to expand)
Fast (non-thermal) perpendicular pressure (sum over charge states when multiple charge states are considered)
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profiles_1d(itime)/ion(i1)/pressure_fast_parallel(:) ⇹PaFLT_1D¶Fast (non-thermal) parallel pressure (sum over charge states […] (click to expand)
Fast (non-thermal) parallel pressure (sum over charge states when multiple charge states are considered)
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profiles_1d(itime)/ion(i1)/rotation_frequency_tor(:) ⇹rad.s^-1FLT_1D¶Toroidal rotation frequency (i.e. […] (click to expand)
Toroidal rotation frequency (i.e. toroidal velocity divided by the major radius at which the toroidal velocity is taken) (average over charge states when multiple charge states are considered)
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profiles_1d(itime)/ion(i1)/velocitym.s^-1structure¶Velocity (average over charge states when multiple charge states […] (click to expand)
Velocity (average over charge states when multiple charge states are considered) at the position of maximum major radius on every flux surface
profiles_1d(itime)/ion(i1)/velocity/diamagnetic(:) ⇹m.s^-1FLT_1D¶Diamagnetic component
Diamagnetic component
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profiles_1d(itime)/ion(i1)/velocity/parallel(:) ⇹m.s^-1FLT_1D¶Parallel component
Parallel component
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profiles_1d(itime)/ion(i1)/velocity/poloidal(:) ⇹m.s^-1FLT_1D¶Poloidal component
Poloidal component
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profiles_1d(itime)/ion(i1)/multiple_states_flagINT_0D¶Multiple states calculation flag : 0-Only the ‘ion’ level is […] (click to expand)
Multiple states calculation flag : 0-Only the ‘ion’ level is considered and the ‘state’ array of structure is empty; 1-Ion states are considered and are described in the ‘state’ array of structure
profiles_1d(itime)/ion(i1)/state(i2)AoS¶Quantities related to the different states of the species (ionization, […] (click to expand)
Quantities related to the different states of the species (ionization, energy, excitation, …)
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profiles_1d(itime)/ion(i1)/state(i2)/z_min ⇹eFLT_0D¶Minimum Z of the charge state bundle
Minimum Z of the charge state bundle
profiles_1d(itime)/ion(i1)/state(i2)/z_max ⇹eFLT_0D¶Maximum Z of the charge state bundle (equal to z_min if no bundle)
Maximum Z of the charge state bundle (equal to z_min if no bundle)
profiles_1d(itime)/ion(i1)/state(i2)/z_average ⇹eFLT_0D¶Average Z of the charge state bundle, volume averaged over the […] (click to expand)
Average Z of the charge state bundle, volume averaged over the plasma radius (equal to z_min if no bundle), = sum (Z*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle.
profiles_1d(itime)/ion(i1)/state(i2)/z_square_average ⇹eFLT_0D¶Average Z square of the charge state bundle, volume averaged […] (click to expand)
Average Z square of the charge state bundle, volume averaged over the plasma radius (equal to z_min squared if no bundle), = sum (Z^2*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle.
profiles_1d(itime)/ion(i1)/state(i2)/z_average_1d(:) ⇹1FLT_1D¶Average charge profile of the charge state bundle (equal to z_min […] (click to expand)
Average charge profile of the charge state bundle (equal to z_min if no bundle), = sum (Z*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle.
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profiles_1d(itime)/ion(i1)/state(i2)/z_average_square_1d(:) ⇹1FLT_1D¶Average square charge profile of the charge state bundle (equal […] (click to expand)
Average square charge profile of the charge state bundle (equal to z_min squared if no bundle), = sum (Z^2*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle.
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profiles_1d(itime)/ion(i1)/state(i2)/ionization_potential ⇹eVFLT_0D¶Cumulative and average ionization potential to reach a given […] (click to expand)
Cumulative and average ionization potential to reach a given bundle. Defined as sum (x_z* (sum of Epot from z’=0 to z-1)), where Epot is the ionization potential of ion Xz’+, and x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle.
Changed in version 4.0.0: Renamed from ionisation_potential
profiles_1d(itime)/ion(i1)/state(i2)/nameSTR_0D¶String identifying state (e.g. […] (click to expand)
String identifying state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, …)
Changed in version 3.42.0: Renamed from label
profiles_1d(itime)/ion(i1)/state(i2)/electron_configurationSTR_0D¶Configuration of atomic orbitals of this state, e.g. […] (click to expand)
Configuration of atomic orbitals of this state, e.g. 1s2-2s1
profiles_1d(itime)/ion(i1)/state(i2)/vibrational_level ⇹eFLT_0D¶Vibrational level (can be bundled)
Vibrational level (can be bundled)
profiles_1d(itime)/ion(i1)/state(i2)/vibrational_modeSTR_0D¶Vibrational mode of this state, e.g. […] (click to expand)
Vibrational mode of this state, e.g. “A_g”. Need to define, or adopt a standard nomenclature.
profiles_1d(itime)/ion(i1)/state(i2)/rotation_frequency_tor(:) ⇹rad.s^-1FLT_1D¶Toroidal rotation frequency (i.e. […] (click to expand)
Toroidal rotation frequency (i.e. toroidal velocity divided by the major radius at which the toroidal velocity is taken)
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profiles_1d(itime)/ion(i1)/state(i2)/velocitym.s^-1structure¶Velocity at the position of maximum major radius on every flux […] (click to expand)
Velocity at the position of maximum major radius on every flux surface
New in version >4.0.0.
profiles_1d(itime)/ion(i1)/state(i2)/velocity/radial(:) ⇹m.s^-1FLT_1D¶Radial component
Radial component
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profiles_1d(itime)/ion(i1)/state(i2)/velocity/diamagnetic(:) ⇹m.s^-1FLT_1D¶Diamagnetic component
Diamagnetic component
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profiles_1d(itime)/ion(i1)/state(i2)/velocity/parallel(:) ⇹m.s^-1FLT_1D¶Parallel component
Parallel component
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profiles_1d(itime)/ion(i1)/state(i2)/velocity/poloidal(:) ⇹m.s^-1FLT_1D¶Poloidal component
Poloidal component
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profiles_1d(itime)/ion(i1)/state(i2)/density(:) ⇹m^-3FLT_1D¶Density (thermal+non-thermal)
Density (thermal+non-thermal)
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profiles_1d(itime)/ion(i1)/state(i2)/density_fitm^-3structure¶Information on the fit used to obtain the density profile
Information on the fit used to obtain the density profile
profiles_1d(itime)/ion(i1)/state(i2)/density_fit/measured(:) ⇹mixedFLT_1D¶Measured values
Measured values
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profiles_1d(itime)/ion(i1)/state(i2)/density_fit/source(:)STR_1D¶Path to the source data for each measurement in the IMAS data […] (click to expand)
Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS
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profiles_1d(itime)/ion(i1)/state(i2)/density_fit/time_measurement(:) ⇹sFLT_1D¶Exact time slices used from the time array of the measurement […] (click to expand)
Exact time slices used from the time array of the measurement source data. The time slice is indicated for each measurement point considered in the fit since measurements may come from different and thus asynchronous diagnostics. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used
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profiles_1d(itime)/ion(i1)/state(i2)/density_fit/time_measurement_slice_methodstructure¶Method used to slice the data : index = 0 means using exact time […] (click to expand)
Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, …
profiles_1d(itime)/ion(i1)/state(i2)/density_fit/time_measurement_slice_method/nameSTR_0D¶Short string identifier
Short string identifier
profiles_1d(itime)/ion(i1)/state(i2)/density_fit/time_measurement_width(:) ⇹sFLT_1D¶In case the measurements are averaged over a time interval, this […] (click to expand)
In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn’t use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement.
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profiles_1d(itime)/ion(i1)/state(i2)/density_fit/local(:)INT_1D¶Integer flag : 1 means local measurement, 0 means line-integrated […] (click to expand)
Integer flag : 1 means local measurement, 0 means line-integrated measurement
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profiles_1d(itime)/ion(i1)/state(i2)/density_fit/rho_tor_norm(:) ⇹1FLT_1D¶Normalized toroidal flux coordinate of each measurement (local […] (click to expand)
Normalized toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
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profiles_1d(itime)/ion(i1)/state(i2)/density_fit/rho_pol_norm(:) ⇹1FLT_1D¶Normalized poloidal flux coordinate of each measurement (local […] (click to expand)
Normalized poloidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
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New in version >4.1.1.
profiles_1d(itime)/ion(i1)/state(i2)/density_fit/weight(:) ⇹1FLT_1D¶Weight given to each measured value
Weight given to each measured value
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profiles_1d(itime)/ion(i1)/state(i2)/density_fit/sigma(:) ⇹mixedFLT_1D¶Standard deviation of the measurement error
Standard deviation of the measurement error
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New in version >4.1.1.
profiles_1d(itime)/ion(i1)/state(i2)/density_fit/reconstructed(:) ⇹mixedFLT_1D¶Value reconstructed from the fit
Value reconstructed from the fit
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profiles_1d(itime)/ion(i1)/state(i2)/density_fit/chi_squared(:) ⇹1FLT_1D¶Squared error normalized by the weighted standard deviation considered […] (click to expand)
Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error
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profiles_1d(itime)/ion(i1)/state(i2)/density_thermal(:) ⇹m^-3FLT_1D¶Density of thermal particles
Density of thermal particles
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profiles_1d(itime)/ion(i1)/state(i2)/density_fast(:) ⇹m^-3FLT_1D¶Density of fast (non-thermal) particles
Density of fast (non-thermal) particles
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profiles_1d(itime)/ion(i1)/state(i2)/pressure(:) ⇹PaFLT_1D¶Pressure (thermal+non-thermal)
Pressure (thermal+non-thermal)
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profiles_1d(itime)/ion(i1)/state(i2)/pressure_thermal(:) ⇹PaFLT_1D¶Pressure (thermal) associated with random motion ~average((v-average(v))^2)
Pressure (thermal) associated with random motion ~average((v-average(v))^2)
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profiles_1d(itime)/ion(i1)/state(i2)/pressure_fast_perpendicular(:) ⇹PaFLT_1D¶Fast (non-thermal) perpendicular pressure
Fast (non-thermal) perpendicular pressure
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profiles_1d(itime)/neutral(i1)AoS¶Quantities related to the different neutral species
Quantities related to the different neutral species
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profiles_1d(itime)/neutral(i1)/element(i2)AoS¶List of elements forming the atom or molecule
List of elements forming the atom or molecule
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profiles_1d(itime)/neutral(i1)/nameSTR_0D¶String identifying the species (e.g. […] (click to expand)
String identifying the species (e.g. H, D, T, He, C, D2, DT, CD4, …)
Changed in version 3.42.0: Renamed from label
profiles_1d(itime)/neutral(i1)/ion_indexINT_0D¶Index of the corresponding ion species in the ../../ion array
Index of the corresponding ion species in the ../../ion array
profiles_1d(itime)/neutral(i1)/temperature(:) ⇹eVFLT_1D¶Temperature (average over charge states when multiple charge […] (click to expand)
Temperature (average over charge states when multiple charge states are considered)
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profiles_1d(itime)/neutral(i1)/density(:) ⇹m^-3FLT_1D¶Density (thermal+non-thermal) (sum over charge states when multiple […] (click to expand)
Density (thermal+non-thermal) (sum over charge states when multiple charge states are considered)
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profiles_1d(itime)/neutral(i1)/density_thermal(:) ⇹m^-3FLT_1D¶Density (thermal) (sum over charge states when multiple charge […] (click to expand)
Density (thermal) (sum over charge states when multiple charge states are considered)
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profiles_1d(itime)/neutral(i1)/density_fast(:) ⇹m^-3FLT_1D¶Density of fast (non-thermal) particles (sum over charge states […] (click to expand)
Density of fast (non-thermal) particles (sum over charge states when multiple charge states are considered)
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profiles_1d(itime)/neutral(i1)/pressure(:) ⇹PaFLT_1D¶Pressure (thermal+non-thermal) (sum over charge states when multiple […] (click to expand)
Pressure (thermal+non-thermal) (sum over charge states when multiple charge states are considered)
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profiles_1d(itime)/neutral(i1)/pressure_thermal(:) ⇹PaFLT_1D¶Pressure (thermal) associated with random motion ~average((v-average(v))^2) […] (click to expand)
Pressure (thermal) associated with random motion ~average((v-average(v))^2) (sum over charge states when multiple charge states are considered)
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profiles_1d(itime)/neutral(i1)/pressure_fast_perpendicular(:) ⇹PaFLT_1D¶Fast (non-thermal) perpendicular pressure (sum over charge states […] (click to expand)
Fast (non-thermal) perpendicular pressure (sum over charge states when multiple charge states are considered)
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profiles_1d(itime)/neutral(i1)/pressure_fast_parallel(:) ⇹PaFLT_1D¶Fast (non-thermal) parallel pressure (sum over charge states […] (click to expand)
Fast (non-thermal) parallel pressure (sum over charge states when multiple charge states are considered)
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profiles_1d(itime)/neutral(i1)/multiple_states_flagINT_0D¶Multiple states calculation flag : 0-Only one state is considered; […] (click to expand)
Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure
profiles_1d(itime)/neutral(i1)/state(i2)AoS¶Quantities related to the different states of the species (energy, […] (click to expand)
Quantities related to the different states of the species (energy, excitation, …)
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profiles_1d(itime)/neutral(i1)/state(i2)/nameSTR_0D¶String identifying state
String identifying state
Changed in version 3.42.0: Renamed from label
profiles_1d(itime)/neutral(i1)/state(i2)/electron_configurationSTR_0D¶Configuration of atomic orbitals of this state, e.g. […] (click to expand)
Configuration of atomic orbitals of this state, e.g. 1s2-2s1
profiles_1d(itime)/neutral(i1)/state(i2)/vibrational_level ⇹eFLT_0D¶Vibrational level (can be bundled)
Vibrational level (can be bundled)
profiles_1d(itime)/neutral(i1)/state(i2)/vibrational_modeSTR_0D¶Vibrational mode of this state, e.g. […] (click to expand)
Vibrational mode of this state, e.g. “A_g”. Need to define, or adopt a standard nomenclature.
profiles_1d(itime)/neutral(i1)/state(i2)/neutral_typestructure¶Neutral type (if the considered state is a neutral), in terms […] (click to expand)
Neutral type (if the considered state is a neutral), in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI
This is an identifier. See neutrals_identifier for the available options.
profiles_1d(itime)/neutral(i1)/state(i2)/neutral_type/nameSTR_0D¶Short string identifier
Short string identifier
profiles_1d(itime)/neutral(i1)/state(i2)/density(:) ⇹m^-3FLT_1D¶Density (thermal+non-thermal)
Density (thermal+non-thermal)
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profiles_1d(itime)/neutral(i1)/state(i2)/density_thermal(:) ⇹m^-3FLT_1D¶Density of thermal particles
Density of thermal particles
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profiles_1d(itime)/neutral(i1)/state(i2)/density_fast(:) ⇹m^-3FLT_1D¶Density of fast (non-thermal) particles
Density of fast (non-thermal) particles
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profiles_1d(itime)/neutral(i1)/state(i2)/pressure(:) ⇹PaFLT_1D¶Pressure (thermal+non-thermal)
Pressure (thermal+non-thermal)
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profiles_1d(itime)/neutral(i1)/state(i2)/pressure_thermal(:) ⇹PaFLT_1D¶Pressure (thermal) associated with random motion ~average((v-average(v))^2)
Pressure (thermal) associated with random motion ~average((v-average(v))^2)
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profiles_1d(itime)/neutral(i1)/state(i2)/pressure_fast_perpendicular(:) ⇹PaFLT_1D¶Fast (non-thermal) perpendicular pressure
Fast (non-thermal) perpendicular pressure
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profiles_1d(itime)/t_i_average(:) ⇹eVFLT_1D¶Ion temperature (averaged on charge states and ion species)
Ion temperature (averaged on charge states and ion species)
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profiles_1d(itime)/t_i_average_fiteVstructure¶Information on the fit used to obtain the t_i_average profile
Information on the fit used to obtain the t_i_average profile
profiles_1d(itime)/t_i_average_fit/source(:)STR_1D¶Path to the source data for each measurement in the IMAS data […] (click to expand)
Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS
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profiles_1d(itime)/t_i_average_fit/time_measurement(:) ⇹sFLT_1D¶Exact time slices used from the time array of the measurement […] (click to expand)
Exact time slices used from the time array of the measurement source data. The time slice is indicated for each measurement point considered in the fit since measurements may come from different and thus asynchronous diagnostics. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used
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profiles_1d(itime)/t_i_average_fit/time_measurement_slice_methodstructure¶Method used to slice the data : index = 0 means using exact time […] (click to expand)
Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, …
profiles_1d(itime)/t_i_average_fit/time_measurement_slice_method/nameSTR_0D¶Short string identifier
Short string identifier
profiles_1d(itime)/t_i_average_fit/time_measurement_width(:) ⇹sFLT_1D¶In case the measurements are averaged over a time interval, this […] (click to expand)
In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn’t use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement.
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profiles_1d(itime)/t_i_average_fit/local(:)INT_1D¶Integer flag : 1 means local measurement, 0 means line-integrated […] (click to expand)
Integer flag : 1 means local measurement, 0 means line-integrated measurement
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profiles_1d(itime)/t_i_average_fit/rho_tor_norm(:) ⇹1FLT_1D¶Normalized toroidal flux coordinate of each measurement (local […] (click to expand)
Normalized toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
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profiles_1d(itime)/t_i_average_fit/rho_pol_norm(:) ⇹1FLT_1D¶Normalized poloidal flux coordinate of each measurement (local […] (click to expand)
Normalized poloidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
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New in version >4.1.1.
profiles_1d(itime)/t_i_average_fit/weight(:) ⇹1FLT_1D¶Weight given to each measured value
Weight given to each measured value
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profiles_1d(itime)/t_i_average_fit/sigma(:) ⇹mixedFLT_1D¶Standard deviation of the measurement error
Standard deviation of the measurement error
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New in version >4.1.1.
profiles_1d(itime)/t_i_average_fit/reconstructed(:) ⇹mixedFLT_1D¶Value reconstructed from the fit
Value reconstructed from the fit
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profiles_1d(itime)/t_i_average_fit/chi_squared(:) ⇹1FLT_1D¶Squared error normalized by the weighted standard deviation considered […] (click to expand)
Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error
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profiles_1d(itime)/n_i_total_over_n_e(:) ⇹1FLT_1D¶Ratio of total ion density (sum over species and charge states) […] (click to expand)
Ratio of total ion density (sum over species and charge states) over electron density. (thermal+non-thermal)
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profiles_1d(itime)/n_i_thermal_total(:) ⇹m^-3FLT_1D¶Total ion thermal density (sum over species and charge states)
Total ion thermal density (sum over species and charge states)
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profiles_1d(itime)/momentum_phi(:) ⇹kg.m^-1.s^-1FLT_1D¶Total plasma toroidal momentum, summed over ion species and electrons […] (click to expand)
Total plasma toroidal momentum, summed over ion species and electrons weighted by their density and major radius, i.e. sum_over_species(n*R*m*Vphi)
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Changed in version 3.42.0: Renamed from momentum_tor
profiles_1d(itime)/zeff_fit1structure¶Information on the fit used to obtain the zeff profile
Information on the fit used to obtain the zeff profile
profiles_1d(itime)/zeff_fit/source(:)STR_1D¶Path to the source data for each measurement in the IMAS data […] (click to expand)
Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS
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profiles_1d(itime)/zeff_fit/time_measurement(:) ⇹sFLT_1D¶Exact time slices used from the time array of the measurement […] (click to expand)
Exact time slices used from the time array of the measurement source data. The time slice is indicated for each measurement point considered in the fit since measurements may come from different and thus asynchronous diagnostics. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used
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profiles_1d(itime)/zeff_fit/time_measurement_slice_methodstructure¶Method used to slice the data : index = 0 means using exact time […] (click to expand)
Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, …
profiles_1d(itime)/zeff_fit/time_measurement_slice_method/nameSTR_0D¶Short string identifier
Short string identifier
profiles_1d(itime)/zeff_fit/time_measurement_width(:) ⇹sFLT_1D¶In case the measurements are averaged over a time interval, this […] (click to expand)
In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn’t use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement.
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profiles_1d(itime)/zeff_fit/local(:)INT_1D¶Integer flag : 1 means local measurement, 0 means line-integrated […] (click to expand)
Integer flag : 1 means local measurement, 0 means line-integrated measurement
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profiles_1d(itime)/zeff_fit/rho_tor_norm(:) ⇹1FLT_1D¶Normalized toroidal flux coordinate of each measurement (local […] (click to expand)
Normalized toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
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profiles_1d(itime)/zeff_fit/rho_pol_norm(:) ⇹1FLT_1D¶Normalized poloidal flux coordinate of each measurement (local […] (click to expand)
Normalized poloidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
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New in version >4.1.1.
profiles_1d(itime)/zeff_fit/weight(:) ⇹1FLT_1D¶Weight given to each measured value
Weight given to each measured value
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profiles_1d(itime)/zeff_fit/sigma(:) ⇹mixedFLT_1D¶Standard deviation of the measurement error
Standard deviation of the measurement error
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New in version >4.1.1.
profiles_1d(itime)/zeff_fit/reconstructed(:) ⇹mixedFLT_1D¶Value reconstructed from the fit
Value reconstructed from the fit
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profiles_1d(itime)/zeff_fit/chi_squared(:) ⇹1FLT_1D¶Squared error normalized by the weighted standard deviation considered […] (click to expand)
Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error
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profiles_1d(itime)/pressure_ion_total(:) ⇹PaFLT_1D¶Total (sum over ion species) thermal ion pressure
Total (sum over ion species) thermal ion pressure
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profiles_1d(itime)/pressure_thermal(:) ⇹PaFLT_1D¶Thermal pressure (electrons+ions)
Thermal pressure (electrons+ions)
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profiles_1d(itime)/pressure_perpendicular(:) ⇹PaFLT_1D¶Total perpendicular pressure (electrons+ions, thermal+non-thermal)
Total perpendicular pressure (electrons+ions, thermal+non-thermal)
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profiles_1d(itime)/pressure_parallel(:) ⇹PaFLT_1D¶Total parallel pressure (electrons+ions, thermal+non-thermal)
Total parallel pressure (electrons+ions, thermal+non-thermal)
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profiles_1d(itime)/j_total(:) ⇹A.m^-2FLT_1D¶Total parallel current density = average(jtot.B) / B0, where […] (click to expand)
Total parallel current density = average(jtot.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0
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profiles_1d(itime)/current_parallel_inside(:) ⇹AFLT_1D¶Parallel current driven inside the flux surface. […] (click to expand)
Parallel current driven inside the flux surface. Cumulative surface integral of j_total
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profiles_1d(itime)/j_phi(:) ⇹A.m^-2FLT_1D¶Total toroidal current density = average(J_phi/R) / average(1/R)
Total toroidal current density = average(J_phi/R) / average(1/R)
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Changed in version 3.42.0: Renamed from j_tor
profiles_1d(itime)/j_ohmic(:) ⇹A.m^-2FLT_1D¶Ohmic parallel current density = average(J_Ohmic.B) / B0, where […] (click to expand)
Ohmic parallel current density = average(J_Ohmic.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0
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profiles_1d(itime)/j_non_inductive(:) ⇹A.m^-2FLT_1D¶Non-inductive (includes bootstrap) parallel current density = […] (click to expand)
Non-inductive (includes bootstrap) parallel current density = average(jni.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0
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profiles_1d(itime)/j_bootstrap(:) ⇹A.m^-2FLT_1D¶Bootstrap current density = average(J_Bootstrap.B) / B0, where […] (click to expand)
Bootstrap current density = average(J_Bootstrap.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0
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profiles_1d(itime)/conductivity_parallel(:) ⇹ohm^-1.m^-1FLT_1D¶Parallel conductivity
Parallel conductivity
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profiles_1d(itime)/e_fieldV.m^-1structure¶Electric field, averaged on the magnetic surface. […] (click to expand)
Electric field, averaged on the magnetic surface. E.g for the parallel component, average(E.B) / B0, using core_profiles/vacuum_toroidal_field/b0
profiles_1d(itime)/e_field/diamagnetic(:) ⇹V.m^-1FLT_1D¶Diamagnetic component
Diamagnetic component
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profiles_1d(itime)/phi_potential(:) ⇹VFLT_1D¶Electrostatic potential, averaged on the magnetic flux surface
Electrostatic potential, averaged on the magnetic flux surface
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profiles_1d(itime)/rotation_frequency_tor_sonic(:) ⇹s^-1FLT_1D¶Derivative of the flux surface averaged electrostatic potential […] (click to expand)
Derivative of the flux surface averaged electrostatic potential with respect to the poloidal flux, multiplied by (1/2pi). This quantity is the toroidal angular rotation frequency due to the ExB drift, introduced in formula (43) of Hinton and Wong, Physics of Fluids 3082 (1985), also referred to as sonic flow in regimes in which the toroidal velocity is dominant over the poloidal velocity
Click here for further documentation.
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profiles_1d(itime)/q(:) ⇹1FLT_1D¶Safety factor (only positive when toroidal current and magnetic […] (click to expand)
Safety factor (only positive when toroidal current and magnetic field are in same direction)
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profiles_2d(itime)AoS¶Core plasma quantities in a poloidal cross section, for various […] (click to expand)
Core plasma quantities in a poloidal cross section, for various time slices
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New in version 3.39.0: lifecycle status alpha
New in version >3.38.1.
profiles_2d(itime)/grid_typestructure¶Selection of one of a set of grid types
Selection of one of a set of grid types
This is an identifier. See poloidal_plane_coordinates_identifier for the available options.
profiles_2d(itime)/gridstructure¶Definition of the 2D grid (the content of dim1 and dim2 is defined […] (click to expand)
Definition of the 2D grid (the content of dim1 and dim2 is defined by the selected grid_type)
profiles_2d(itime)/grid/dim2(:) ⇹mixedFLT_1D¶Second dimension values
Second dimension values
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profiles_2d(itime)/grid/volume_element(:,:) ⇹m^3FLT_2D¶Elementary plasma volume of plasma enclosed in the cell formed […] (click to expand)
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)]
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profiles_2d(itime)/ion(i1)AoS¶2D quantities related to the different ion species, in the sense […] (click to expand)
2D quantities related to the different ion species, in the sense of isonuclear or isomolecular sequences. Ionization states (or other types of states) must be differentiated at the state level below. This array doesn’t necessarily have the same size as the profiles_1d/ion array, since 2D data may be relevant only for a subset of ion species.
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profiles_2d(itime)/ion(i1)/element(i2)AoS¶List of elements forming the atom or molecule
List of elements forming the atom or molecule
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profiles_2d(itime)/ion(i1)/z_ion ⇹eFLT_0D¶Ion charge (of the dominant ionization state; lumped ions are […] (click to expand)
Ion charge (of the dominant ionization state; lumped ions are allowed), volume averaged over plasma radius
profiles_2d(itime)/ion(i1)/nameSTR_0D¶String identifying ion (e.g. […] (click to expand)
String identifying ion (e.g. H, D, T, He, C, D2, …)
Changed in version 3.42.0: Renamed from label
profiles_2d(itime)/ion(i1)/ion_indexINT_0D¶Index of the corresponding ion species in the ../../../profiles_1d/ion […] (click to expand)
Index of the corresponding ion species in the ../../../profiles_1d/ion array
profiles_2d(itime)/ion(i1)/temperature(:,:) ⇹eVFLT_2D¶Temperature (average over charge states when multiple charge […] (click to expand)
Temperature (average over charge states when multiple charge states are considered)
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profiles_2d(itime)/ion(i1)/density(:,:) ⇹m^-3FLT_2D¶Density (thermal+non-thermal) (sum over charge states when multiple […] (click to expand)
Density (thermal+non-thermal) (sum over charge states when multiple charge states are considered)
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profiles_2d(itime)/ion(i1)/density_thermal(:,:) ⇹m^-3FLT_2D¶Density (thermal) (sum over charge states when multiple charge […] (click to expand)
Density (thermal) (sum over charge states when multiple charge states are considered)
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profiles_2d(itime)/ion(i1)/density_fast(:,:) ⇹m^-3FLT_2D¶Density of fast (non-thermal) particles (sum over charge states […] (click to expand)
Density of fast (non-thermal) particles (sum over charge states when multiple charge states are considered)
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profiles_2d(itime)/ion(i1)/pressure(:,:) ⇹PaFLT_2D¶Pressure (thermal+non-thermal) (sum over charge states when multiple […] (click to expand)
Pressure (thermal+non-thermal) (sum over charge states when multiple charge states are considered)
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profiles_2d(itime)/ion(i1)/pressure_thermal(:,:) ⇹PaFLT_2D¶Pressure (thermal) associated with random motion ~average((v-average(v))^2) […] (click to expand)
Pressure (thermal) associated with random motion ~average((v-average(v))^2) (sum over charge states when multiple charge states are considered)
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profiles_2d(itime)/ion(i1)/pressure_fast_perpendicular(:,:) ⇹PaFLT_2D¶Fast (non-thermal) perpendicular pressure (sum over charge states […] (click to expand)
Fast (non-thermal) perpendicular pressure (sum over charge states when multiple charge states are considered)
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profiles_2d(itime)/ion(i1)/pressure_fast_parallel(:,:) ⇹PaFLT_2D¶Fast (non-thermal) parallel pressure (sum over charge states […] (click to expand)
Fast (non-thermal) parallel pressure (sum over charge states when multiple charge states are considered)
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profiles_2d(itime)/ion(i1)/rotation_frequency_tor(:,:) ⇹rad.s^-1FLT_2D¶Toroidal rotation frequency (i.e. […] (click to expand)
Toroidal rotation frequency (i.e. toroidal velocity divided by the major radius at which the toroidal velocity is taken) (average over charge states when multiple charge states are considered)
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profiles_2d(itime)/ion(i1)/velocitym.s^-1structure¶Velocity (average over charge states when multiple charge states […] (click to expand)
Velocity (average over charge states when multiple charge states are considered) at the position of maximum major radius on every flux surface
profiles_2d(itime)/ion(i1)/velocity/diamagnetic(:,:) ⇹m.s^-1FLT_2D¶Diamagnetic component
Diamagnetic component
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profiles_2d(itime)/ion(i1)/velocity/parallel(:,:) ⇹m.s^-1FLT_2D¶Parallel component
Parallel component
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profiles_2d(itime)/ion(i1)/velocity/poloidal(:,:) ⇹m.s^-1FLT_2D¶Poloidal component
Poloidal component
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profiles_2d(itime)/ion(i1)/multiple_states_flagINT_0D¶Multiple states calculation flag : 0-Only the ‘ion’ level is […] (click to expand)
Multiple states calculation flag : 0-Only the ‘ion’ level is considered and the ‘state’ array of structure is empty; 1-Ion states are considered and are described in the ‘state’ array of structure
profiles_2d(itime)/ion(i1)/state(i2)AoS¶Quantities related to the different states of the species (ionization, […] (click to expand)
Quantities related to the different states of the species (ionization, energy, excitation, …)
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profiles_2d(itime)/ion(i1)/state(i2)/z_min ⇹eFLT_0D¶Minimum Z of the charge state bundle
Minimum Z of the charge state bundle
profiles_2d(itime)/ion(i1)/state(i2)/z_max ⇹eFLT_0D¶Maximum Z of the charge state bundle (equal to z_min if no bundle)
Maximum Z of the charge state bundle (equal to z_min if no bundle)
profiles_2d(itime)/ion(i1)/state(i2)/z_average ⇹eFLT_0D¶Average Z of the charge state bundle, volume averaged over the […] (click to expand)
Average Z of the charge state bundle, volume averaged over the plasma radius (equal to z_min if no bundle), = sum (Z*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle.
profiles_2d(itime)/ion(i1)/state(i2)/z_square_average ⇹eFLT_0D¶Average Z square of the charge state bundle, volume averaged […] (click to expand)
Average Z square of the charge state bundle, volume averaged over the plasma radius (equal to z_min squared if no bundle), = sum (Z^2*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle.
profiles_2d(itime)/ion(i1)/state(i2)/ionization_potential ⇹eVFLT_0D¶Cumulative and average ionization potential to reach a given […] (click to expand)
Cumulative and average ionization potential to reach a given bundle. Defined as sum (x_z* (sum of Epot from z’=0 to z-1)), where Epot is the ionization potential of ion Xz’+, and x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle.
Changed in version 4.0.0: Renamed from ionisation_potential
profiles_2d(itime)/ion(i1)/state(i2)/nameSTR_0D¶String identifying state (e.g. […] (click to expand)
String identifying state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, …)
Changed in version 3.42.0: Renamed from label
profiles_2d(itime)/ion(i1)/state(i2)/electron_configurationSTR_0D¶Configuration of atomic orbitals of this state, e.g. […] (click to expand)
Configuration of atomic orbitals of this state, e.g. 1s2-2s1
profiles_2d(itime)/ion(i1)/state(i2)/vibrational_level ⇹eFLT_0D¶Vibrational level (can be bundled)
Vibrational level (can be bundled)
profiles_2d(itime)/ion(i1)/state(i2)/vibrational_modeSTR_0D¶Vibrational mode of this state, e.g. […] (click to expand)
Vibrational mode of this state, e.g. “A_g”. Need to define, or adopt a standard nomenclature.
profiles_2d(itime)/ion(i1)/state(i2)/rotation_frequency_tor(:,:) ⇹rad.s^-1FLT_2D¶Toroidal rotation frequency (i.e. […] (click to expand)
Toroidal rotation frequency (i.e. toroidal velocity divided by the major radius at which the toroidal velocity is taken)
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profiles_2d(itime)/ion(i1)/state(i2)/density(:,:) ⇹m^-3FLT_2D¶Density (thermal+non-thermal)
Density (thermal+non-thermal)
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profiles_2d(itime)/ion(i1)/state(i2)/density_thermal(:,:) ⇹m^-3FLT_2D¶Density of thermal particles
Density of thermal particles
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profiles_2d(itime)/ion(i1)/state(i2)/density_fast(:,:) ⇹m^-3FLT_2D¶Density of fast (non-thermal) particles
Density of fast (non-thermal) particles
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profiles_2d(itime)/ion(i1)/state(i2)/pressure(:,:) ⇹PaFLT_2D¶Pressure (thermal+non-thermal)
Pressure (thermal+non-thermal)
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profiles_2d(itime)/ion(i1)/state(i2)/pressure_thermal(:,:) ⇹PaFLT_2D¶Pressure (thermal) associated with random motion ~average((v-average(v))^2)
Pressure (thermal) associated with random motion ~average((v-average(v))^2)
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profiles_2d(itime)/ion(i1)/state(i2)/pressure_fast_perpendicular(:,:) ⇹PaFLT_2D¶Fast (non-thermal) perpendicular pressure
Fast (non-thermal) perpendicular pressure
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profiles_2d(itime)/t_i_average(:,:) ⇹eVFLT_2D¶Ion temperature (averaged on states and ion species)
Ion temperature (averaged on states and ion species)
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profiles_2d(itime)/n_i_total_over_n_e(:,:) ⇹1FLT_2D¶Ratio of total ion density (sum over species and charge states) […] (click to expand)
Ratio of total ion density (sum over species and charge states) over electron density. (thermal+non-thermal)
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profiles_2d(itime)/n_i_thermal_total(:,:) ⇹m^-3FLT_2D¶Total ion thermal density (sum over species and charge states)
Total ion thermal density (sum over species and charge states)
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profiles_2d(itime)/momentum_phi(:,:) ⇹kg.m^-1.s^-1FLT_2D¶Total plasma toroidal momentum, summed over ion species and electrons […] (click to expand)
Total plasma toroidal momentum, summed over ion species and electrons weighted by their density and major radius, i.e. sum_over_species(n*R*m*Vphi)
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Changed in version 3.42.0: Renamed from momentum_tor
profiles_2d(itime)/pressure_ion_total(:,:) ⇹PaFLT_2D¶Total (sum over ion species) thermal ion pressure
Total (sum over ion species) thermal ion pressure
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profiles_2d(itime)/pressure_thermal(:,:) ⇹PaFLT_2D¶Thermal pressure (electrons+ions)
Thermal pressure (electrons+ions)
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profiles_2d(itime)/pressure_perpendicular(:,:) ⇹PaFLT_2D¶Total perpendicular pressure (electrons+ions, thermal+non-thermal)
Total perpendicular pressure (electrons+ions, thermal+non-thermal)
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global_quantitiesstructure¶Various global quantities derived from the profiles
Various global quantities derived from the profiles
global_quantities/ip(:) ⇹AFLT_1D¶Total plasma current (toroidal component). […] (click to expand)
Total plasma current (toroidal component). Positive sign means anti-clockwise when viewed from above.
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global_quantities/current_non_inductive(:) ⇹AFLT_1D¶Total non-inductive current (toroidal component). […] (click to expand)
Total non-inductive current (toroidal component). Positive sign means anti-clockwise when viewed from above.
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global_quantities/current_bootstrap(:) ⇹AFLT_1D¶Bootstrap current (toroidal component). […] (click to expand)
Bootstrap current (toroidal component). Positive sign means anti-clockwise when viewed from above.
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global_quantities/v_loop(:) ⇹VFLT_1D¶LCFS loop voltage (positive value drives positive ohmic current […] (click to expand)
LCFS loop voltage (positive value drives positive ohmic current that flows anti-clockwise when viewed from above)
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global_quantities/li_3(:) ⇹1FLT_1D¶Internal inductance. […] (click to expand)
Internal inductance. The li_3 definition is used, i.e. li_3 = 2/R0/mu0^2/Ip^2 * int(Bp^2 dV).
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global_quantities/beta_tor(:) ⇹1FLT_1D¶Toroidal beta, defined as the volume-averaged total perpendicular […] (click to expand)
Toroidal beta, defined as the volume-averaged total perpendicular pressure divided by (B0^2/(2*mu0)), i.e. beta_toroidal = 2 mu0 int(p dV) / V / B0^2
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global_quantities/beta_tor_norm(:) ⇹1FLT_1D¶Normalized toroidal beta, defined as 100 \* beta_tor \* a[m] […] (click to expand)
Normalized toroidal beta, defined as 100 * beta_tor * a[m] * B0 [T] / ip [MA]
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global_quantities/beta_pol(:) ⇹1FLT_1D¶Poloidal beta. […] (click to expand)
Poloidal beta. Defined as betap = 4 int(p dV) / [R_0 * mu_0 * Ip^2]
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global_quantities/energy_diamagnetic(:) ⇹JFLT_1D¶Plasma energy content = 3/2 \* integral over the plasma volume […] (click to expand)
Plasma energy content = 3/2 * integral over the plasma volume of the total perpendicular pressure
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global_quantities/z_eff_resistive(:) ⇹1FLT_1D¶Volume average plasma effective charge, estimated from the flux […] (click to expand)
Volume average plasma effective charge, estimated from the flux consumption in the ohmic phase
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global_quantities/t_e_peaking(:) ⇹1FLT_1D¶Electron temperature peaking factor, defined as the Te value […] (click to expand)
Electron temperature peaking factor, defined as the Te value at the magnetic axis divided by the volume averaged Te (average over the plasma volume up to the LCFS)
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global_quantities/t_i_average_peaking(:) ⇹1FLT_1D¶Ion temperature (averaged over ion species and states) peaking […] (click to expand)
Ion temperature (averaged over ion species and states) peaking factor, defined as the Ti value at the magnetic axis divided by the volume averaged Ti (average over the plasma volume up to the LCFS)
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global_quantities/resistive_psi_losses(:) ⇹WbFLT_1D¶Resistive part of the poloidal flux losses, defined as the volume-averaged […] (click to expand)
Resistive part of the poloidal flux losses, defined as the volume-averaged scalar product of the electric field and the ohmic current density, normalized by the plasma current and integrated in time from the beginning of the plasma discharge: int ( (int(E_field_tor.j_ohm_tor) dV) / Ip ) dt)
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global_quantities/ejima(:) ⇹1FLT_1D¶Ejima coefficient : resistive psi losses divided by (mu0\*R\*Ip). […] (click to expand)
Ejima coefficient : resistive psi losses divided by (mu0*R*Ip). See S. Ejima et al, Nuclear Fusion, Vol.22, No.10 (1982), 1313
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global_quantities/t_e_volume_average(:) ⇹eVFLT_1D¶Volume averaged electron temperature (average over the plasma […] (click to expand)
Volume averaged electron temperature (average over the plasma volume up to the LCFS)
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New in version >3.33.0.
global_quantities/n_e_volume_average(:) ⇹m^-3FLT_1D¶Volume averaged electron density (average over the plasma volume […] (click to expand)
Volume averaged electron density (average over the plasma volume up to the LCFS)
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New in version >3.33.0.
global_quantities/ion(i1)AoS¶Quantities related to the different ion species, in the sense […] (click to expand)
Quantities related to the different ion species, in the sense of isonuclear or isomolecular sequences. The set of ion species of this array must be the same as the one defined in profiles_1d/ion, at the time slice indicated in ion_time_slice
Maximum occurrences (MDS+ backend only): 20
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New in version >3.33.0.
global_quantities/ion(i1)/t_i_volume_average(:) ⇹eVFLT_1D¶Volume averaged temperature of this ion species (averaged over […] (click to expand)
Volume averaged temperature of this ion species (averaged over the plasma volume up to the LCFS)
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vacuum_toroidal_fieldstructure¶Characteristics of the vacuum toroidal field (used in rho_tor […] (click to expand)
Characteristics of the vacuum toroidal field (used in rho_tor definition and in the normalization of current densities)
vacuum_toroidal_field/r0 ⇹mFLT_0D¶Reference major radius where the vacuum toroidal magnetic field […] (click to expand)
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)
vacuum_toroidal_field/b0(:) ⇹TFLT_1D¶Vacuum toroidal field at R0 [T]; Positive sign means anti-clockwise […] (click to expand)
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.
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covariancestructure¶User defined covariance matrix. […] (click to expand)
User defined covariance matrix. The covariance of various quantities can be stored here, these quantities are referred to by giving their IDS path in the rows_uri list
New in version 3.40.0: lifecycle status alpha
New in version >3.39.0.
covariance/descriptionSTR_0D¶Description of this covariance matrix
Description of this covariance matrix
covariance/rows_uri(:)STR_1D¶List of URIs corresponding to the rows (1st dimension) of the […] (click to expand)
List of URIs corresponding to the rows (1st dimension) of the covariance matrix. If not all indices of a given node are used, they must be listed explicitly e.g. rows_uri(i) = pf_active:1/coil(i) will refer to a list of indices of the occurrence 1 of the pf_active IDS of this data entry. If the rows correspond to all indices of a given vector it is sufficient to give a single URI where this vector is denoted using the (:) implicit notation, e.g. rows_uri(1) = /grid_ggd(3)/grid_subset(2)/elements(:).
Click here for further documentation.
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statistics(itime)AoS¶Statistics for various time slices
Statistics for various time slices
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New in version 3.40.0: lifecycle status alpha
New in version >3.39.0.
statistics(itime)/quantity_2d(i1)AoS¶Set of 2D quantities on which statistics are provided. […] (click to expand)
Set of 2D quantities on which statistics are provided. 2D means 1D+time dimension, so either a 1D quantity within a dynamic array of structure, or a 2D dynamic quantity outside of an array of structure. Therefore the resulting statistical value is 1D for a given statistics time slice.
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statistics(itime)/quantity_2d(i1)/pathSTR_0D¶Path of the quantity within the IDS, following the syntax given […] (click to expand)
Path of the quantity within the IDS, following the syntax given in the link below
statistics(itime)/quantity_2d(i1)/statistics_type(i2)AoS¶Set of statistics types applied to the quantity
Set of statistics types applied to the quantity
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statistics(itime)/quantity_2d(i1)/statistics_type(i2)/identifierstructure¶Identifier of the statistics type
Identifier of the statistics type
This is an identifier. See statistics_type_identifier for the available options.
statistics(itime)/quantity_2d(i1)/statistics_type(i2)/identifier/nameSTR_0D¶Short string identifier
Short string identifier
statistics(itime)/quantity_2d(i1)/statistics_type(i2)/value(:) ⇹mixedFLT_1D¶Value of the statistics for that quantity, the array corresponding […] (click to expand)
Value of the statistics for that quantity, the array corresponding to the first dimension of the original 2D quantity
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statistics(itime)/quantity_2d(i1)/statistics_type(i2)/grid_subset_indexINT_0D¶Only if the statistics value is given on a different GGD grid […] (click to expand)
Only if the statistics value is given on a different GGD grid subset than the original quantity (e.g. if the statistics has worked over a dimension of the GGD), index of the new grid subset the statistics value is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index
statistics(itime)/quantity_2d(i1)/statistics_type(i2)/grid_indexINT_0D¶Only if the statistics value is given on a different GGD grid […] (click to expand)
Only if the statistics value is given on a different GGD grid subset than the original quantity (e.g. if the statistics has worked over a dimension of the GGD), index of the grid used to represent the statistics value
statistics(itime)/quantity_2d(i1)/distributionstructure¶Probability distribution function of the quantity
Probability distribution function of the quantity
statistics(itime)/quantity_2d(i1)/distribution/bins(:,:) ⇹mixedFLT_2D¶Bins of quantitiy values, defined for each element (first dimension) […] (click to expand)
Bins of quantitiy values, defined for each element (first dimension) corresponding to the first dimension of the original 2D quantity
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statistics(itime)/quantity_2d(i1)/distribution/probability(:,:) ⇹1FLT_2D¶Probability to have a value of the quantity between bins(n) and […] (click to expand)
Probability to have a value of the quantity between bins(n) and bins(n+1) (thus the size of its second dimension is the size of the second dimension of the bins array - 1). The first dimension correspond to the first dimension of the original 2D quantity
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statistics(itime)/uq_input_2d(i1)AoS¶If the statistics are based on an uncertainty quantification […] (click to expand)
If the statistics are based on an uncertainty quantification process, set of 2D input quantities that are varied
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statistics(itime)/uq_input_2d(i1)/pathSTR_0D¶Path of the quantity within the IDS, following the syntax given […] (click to expand)
Path of the quantity within the IDS, following the syntax given in the link below
statistics(itime)/uq_input_2d(i1)/distributionstructure¶Probability distribution function of the quantity
Probability distribution function of the quantity
statistics(itime)/uq_input_2d(i1)/distribution/bins(:,:) ⇹mixedFLT_2D¶Bins of quantitiy values, defined for each element (first dimension) […] (click to expand)
Bins of quantitiy values, defined for each element (first dimension) corresponding to the first dimension of the original 2D quantity
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statistics(itime)/uq_input_2d(i1)/distribution/probability(:,:) ⇹1FLT_2D¶Probability to have a value of the quantity between bins(n) and […] (click to expand)
Probability to have a value of the quantity between bins(n) and bins(n+1) (thus the size of its second dimension is the size of the second dimension of the bins array - 1). The first dimension correspond to the first dimension of the original 2D quantity
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