spectrometer x ray crystalΒΆ
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
spectrometer_x_ray_crystal (alpha) | X-crystal spectrometer diagnostic | |||
spectrometer_x_ray_crystal.channel (alpha) | [1...N] | STRUCT_ARRAY | Measurement channel, composed of a camera, a crystal, and (optional) a set of reflectors. The light coming from the plasma passes through the (optional) set of reflectors, then the crystal and arrives at the camera | |
spectrometer_x_ray_crystal.channel[:].aperture (alpha) | STRUCTURE | Collimating aperture | ||
spectrometer_x_ray_crystal.channel[:].aperture.centre (alpha) | STRUCTURE | If geometry_type=2, coordinates of the centre of the circle. If geometry_type=1 or 3, coordinates of the origin of the local coordinate system (X1,X2,X3) describing the plane detector/aperture. This origin is located within the detector/aperture area. | ||
spectrometer_x_ray_crystal.channel[:].aperture.centre.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle (oriented counter-clockwise when viewing from above) | |
spectrometer_x_ray_crystal.channel[:].aperture.centre.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
spectrometer_x_ray_crystal.channel[:].aperture.centre.z (alpha) | FLT_0D (uncertain) | m | Height | |
spectrometer_x_ray_crystal.channel[:].aperture.geometry_type (alpha) | INT_0D | Type of geometry used to describe the surface of the detector or aperture (1:'outline', 2:'circular', 3:'rectangle'). In case of 'outline', the surface is described by an outline of point in a local coordinate system defined by a centre and three unit vectors X1, X2, X3. Note that there is some flexibility here and the data provider should choose the most convenient coordinate system for the object, respecting the definitions of (X1,X2,X3) indicated below. In case of 'circular', the surface is a circle defined by its centre, radius, and normal vector oriented towards the plasma X3. In case of 'rectangle', the surface is a rectangle defined by its centre, widths in the X1 and X2 directions, and normal vector oriented towards the plasma X3. | ||
spectrometer_x_ray_crystal.channel[:].aperture.outline (alpha) | STRUCTURE | Irregular outline of the detector/aperture in the (X1, X2) coordinate system. Do NOT repeat the first point. | ||
spectrometer_x_ray_crystal.channel[:].aperture.outline.x1 (alpha) | [1...N] | FLT_1D (uncertain) | m | Positions along x1 axis |
spectrometer_x_ray_crystal.channel[:].aperture.outline.x2 (alpha) | [spectrometer_x_ray_crystal.channel[:].aperture.outline.x1] | FLT_1D (uncertain) | m | Positions along x2 axis |
spectrometer_x_ray_crystal.channel[:].aperture.radius (alpha) | FLT_0D (uncertain) | m | Radius of the circle, used only if geometry_type = 2 | |
spectrometer_x_ray_crystal.channel[:].aperture.surface (alpha) | FLT_0D (uncertain) | m^2 | Surface of the detector/aperture, derived from the above geometric data | |
spectrometer_x_ray_crystal.channel[:].aperture.x1_unit_vector (alpha) | STRUCTURE | Components of the X1 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X1 vector is more horizontal than X2 (has a smaller abs(Z) component) and oriented in the positive phi direction (counter-clockwise when viewing from above). | ||
spectrometer_x_ray_crystal.channel[:].aperture.x1_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
spectrometer_x_ray_crystal.channel[:].aperture.x1_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
spectrometer_x_ray_crystal.channel[:].aperture.x1_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
spectrometer_x_ray_crystal.channel[:].aperture.x1_width (alpha) | FLT_0D (uncertain) | m | Full width of the aperture in the X1 direction, used only if geometry_type = 3 | |
spectrometer_x_ray_crystal.channel[:].aperture.x2_unit_vector (alpha) | STRUCTURE | Components of the X2 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X2 axis is orthonormal so that uX2 = uX3 x uX1. | ||
spectrometer_x_ray_crystal.channel[:].aperture.x2_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
spectrometer_x_ray_crystal.channel[:].aperture.x2_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
spectrometer_x_ray_crystal.channel[:].aperture.x2_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
spectrometer_x_ray_crystal.channel[:].aperture.x2_width (alpha) | FLT_0D (uncertain) | m | Full width of the aperture in the X2 direction, used only if geometry_type = 3 | |
spectrometer_x_ray_crystal.channel[:].aperture.x3_unit_vector (alpha) | STRUCTURE | Components of the X3 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X3 axis is normal to the detector/aperture plane and oriented towards the plasma. | ||
spectrometer_x_ray_crystal.channel[:].aperture.x3_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
spectrometer_x_ray_crystal.channel[:].aperture.x3_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
spectrometer_x_ray_crystal.channel[:].aperture.x3_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
spectrometer_x_ray_crystal.channel[:].bin (alpha) | [1...N] | STRUCT_ARRAY | Set of bins (binning in the vertical dimension) defined to increase the signal to noise ratio of the spectra | |
spectrometer_x_ray_crystal.channel[:].bin[:].instrument_function (alpha) | STRUCTURE | Instrument function for this bin (replaces the ../../instrument function in case vertical binning is used), i.e. response of the detector to a monochromatic emission passing through the spectrometer. The resulting image on the detector will be a 2-D distribution of pixel values, for each wavelength. It can be given as explicit values for each detector pixel (values node) or as a parametric function of wavelength (described by the other nodes) | ||
spectrometer_x_ray_crystal.channel[:].bin[:].instrument_function.centre (alpha) | [spectrometer_x_ray_crystal.channel[:].bin[:].instrument_function.wavelengths] | FLT_1D (uncertain) | m | Centre (in terms of absolute wavelength) of instrument function |
spectrometer_x_ray_crystal.channel[:].bin[:].instrument_function.intensity (alpha) | [spectrometer_x_ray_crystal.channel[:].bin[:].instrument_function.wavelengths] | FLT_1D (uncertain) | m | Scaling factor for the instrument function such that convolving the instrument function with an emission spectrum gives the counts per second on the detector |
spectrometer_x_ray_crystal.channel[:].bin[:].instrument_function.scale (alpha) | [spectrometer_x_ray_crystal.channel[:].bin[:].instrument_function.wavelengths] | FLT_1D (uncertain) | m | Scale of Lorentzian instrument function (full width at half height) |
spectrometer_x_ray_crystal.channel[:].bin[:].instrument_function.sigma (alpha) | [spectrometer_x_ray_crystal.channel[:].bin[:].instrument_function.wavelengths] | FLT_1D (uncertain) | m | Standard deviation of Gaussian instrument function |
spectrometer_x_ray_crystal.channel[:].bin[:].instrument_function.type (alpha) | STRUCTURE | Instrument function type | ||
spectrometer_x_ray_crystal.channel[:].bin[:].instrument_function.type.description (alpha) | STR_0D | Verbose description | ||
spectrometer_x_ray_crystal.channel[:].bin[:].instrument_function.type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
spectrometer_x_ray_crystal.channel[:].bin[:].instrument_function.type.name (alpha) | STR_0D | Short string identifier | ||
spectrometer_x_ray_crystal.channel[:].bin[:].instrument_function.values (alpha) | [1...N, | FLT_2D (uncertain) | sr.m | Explicit instrument function values for the detector. When multiplied by the line-integrated emission spectrum in photons/second/sr/m/m^2 received on a binned pixel of the detector, gives the detector pixel output in counts/seconds. |
spectrometer_x_ray_crystal.channel[:].bin[:].instrument_function.wavelengths (alpha) | [1...N] | FLT_1D (uncertain) | m | Array of wavelengths on which the instrument function is defined |
spectrometer_x_ray_crystal.channel[:].bin[:].line_of_sight (alpha) | STRUCTURE | Description of the line of sight from the crystal to the plasma for this bin, defined by two points | ||
spectrometer_x_ray_crystal.channel[:].bin[:].line_of_sight.first_point (alpha) | STRUCTURE | Position of the first point | ||
spectrometer_x_ray_crystal.channel[:].bin[:].line_of_sight.first_point.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle (oriented counter-clockwise when viewing from above) | |
spectrometer_x_ray_crystal.channel[:].bin[:].line_of_sight.first_point.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
spectrometer_x_ray_crystal.channel[:].bin[:].line_of_sight.first_point.z (alpha) | FLT_0D (uncertain) | m | Height | |
spectrometer_x_ray_crystal.channel[:].bin[:].line_of_sight.second_point (alpha) | STRUCTURE | Position of the second point | ||
spectrometer_x_ray_crystal.channel[:].bin[:].line_of_sight.second_point.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle (oriented counter-clockwise when viewing from above) | |
spectrometer_x_ray_crystal.channel[:].bin[:].line_of_sight.second_point.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
spectrometer_x_ray_crystal.channel[:].bin[:].line_of_sight.second_point.z (alpha) | FLT_0D (uncertain) | m | Height | |
spectrometer_x_ray_crystal.channel[:].bin[:].wavelength (alpha) | [1...N] | FLT_1D (uncertain) | m | Wavelength of incoming photons on each horizontal pixel of this bin. |
spectrometer_x_ray_crystal.channel[:].bin[:].z_pixel_range (alpha) | [1...2] | INT_1D | Vertical pixel index range indicating the corresponding binned detector area | |
spectrometer_x_ray_crystal.channel[:].camera (alpha) | STRUCTURE | Characteristics of the camera used | ||
spectrometer_x_ray_crystal.channel[:].camera.camera_dimensions (alpha) | [1...2] | FLT_1D (uncertain) | m | Total camera dimension in each direction (x1, x2) |
spectrometer_x_ray_crystal.channel[:].camera.centre (alpha) | STRUCTURE | Position of the camera centre | ||
spectrometer_x_ray_crystal.channel[:].camera.centre.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle (oriented counter-clockwise when viewing from above) | |
spectrometer_x_ray_crystal.channel[:].camera.centre.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
spectrometer_x_ray_crystal.channel[:].camera.centre.z (alpha) | FLT_0D (uncertain) | m | Height | |
spectrometer_x_ray_crystal.channel[:].camera.identifier (alpha) | STR_0D | ID of the camera | ||
spectrometer_x_ray_crystal.channel[:].camera.line_of_sight (alpha) | STRUCTURE | Description of the line of sight for each pixel, given by 2 points. For each coordinate : first dimension : line index (x1 axis); second dimension: column index (x2 axis). | ||
spectrometer_x_ray_crystal.channel[:].camera.line_of_sight.first_point (alpha) | STRUCTURE | Position of the first point | ||
spectrometer_x_ray_crystal.channel[:].camera.line_of_sight.first_point.phi (alpha) | [1...N, | FLT_2D (uncertain) | rad | Toroidal angle (oriented counter-clockwise when viewing from above) |
spectrometer_x_ray_crystal.channel[:].camera.line_of_sight.first_point.r (alpha) | [1...N, | FLT_2D (uncertain) | m | Major radius |
spectrometer_x_ray_crystal.channel[:].camera.line_of_sight.first_point.z (alpha) | [1...N, | FLT_2D (uncertain) | m | Height |
spectrometer_x_ray_crystal.channel[:].camera.line_of_sight.second_point (alpha) | STRUCTURE | Position of the second point | ||
spectrometer_x_ray_crystal.channel[:].camera.line_of_sight.second_point.phi (alpha) | [1...N, | FLT_2D (uncertain) | rad | Toroidal angle (oriented counter-clockwise when viewing from above) |
spectrometer_x_ray_crystal.channel[:].camera.line_of_sight.second_point.r (alpha) | [1...N, | FLT_2D (uncertain) | m | Major radius |
spectrometer_x_ray_crystal.channel[:].camera.line_of_sight.second_point.z (alpha) | [1...N, | FLT_2D (uncertain) | m | Height |
spectrometer_x_ray_crystal.channel[:].camera.pixel_dimensions (alpha) | [1...2] | FLT_1D (uncertain) | m | Pixel dimension in each direction (x1, x2) |
spectrometer_x_ray_crystal.channel[:].camera.pixel_position (alpha) | STRUCTURE | Position of the centre of each pixel. First dimension : line index (x1 axis). Second dimension: column index (x2 axis). | ||
spectrometer_x_ray_crystal.channel[:].camera.pixel_position.phi (alpha) | [1...N, | FLT_2D (uncertain) | rad | Toroidal angle (oriented counter-clockwise when viewing from above) |
spectrometer_x_ray_crystal.channel[:].camera.pixel_position.r (alpha) | [1...N, | FLT_2D (uncertain) | m | Major radius |
spectrometer_x_ray_crystal.channel[:].camera.pixel_position.z (alpha) | [1...N, | FLT_2D (uncertain) | m | Height |
spectrometer_x_ray_crystal.channel[:].camera.pixels_n (alpha) | [1...2] | INT_1D | Number of pixels in each direction (x1, x2) | |
spectrometer_x_ray_crystal.channel[:].camera.x1_unit_vector (alpha) | STRUCTURE | Components of the X1 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X1 vector is more horizontal than X2 (has a smaller abs(Z) component) and oriented in the positive phi direction (counter-clockwise when viewing from above). | ||
spectrometer_x_ray_crystal.channel[:].camera.x1_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
spectrometer_x_ray_crystal.channel[:].camera.x1_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
spectrometer_x_ray_crystal.channel[:].camera.x1_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
spectrometer_x_ray_crystal.channel[:].camera.x2_unit_vector (alpha) | STRUCTURE | Components of the X2 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X2 axis is orthonormal so that uX2 = uX3 x uX1. | ||
spectrometer_x_ray_crystal.channel[:].camera.x2_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
spectrometer_x_ray_crystal.channel[:].camera.x2_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
spectrometer_x_ray_crystal.channel[:].camera.x2_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
spectrometer_x_ray_crystal.channel[:].camera.x3_unit_vector (alpha) | STRUCTURE | Components of the X3 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X3 axis is normal to the camera plane and oriented towards the plasma. | ||
spectrometer_x_ray_crystal.channel[:].camera.x3_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
spectrometer_x_ray_crystal.channel[:].camera.x3_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
spectrometer_x_ray_crystal.channel[:].camera.x3_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
spectrometer_x_ray_crystal.channel[:].crystal (alpha) | STRUCTURE | Characteristics of the crystal used | ||
spectrometer_x_ray_crystal.channel[:].crystal.angle_bragg (alpha) | FLT_0D (uncertain) | rad | Bragg angle of the crystal | |
spectrometer_x_ray_crystal.channel[:].crystal.centre (alpha) | STRUCTURE | Coordinates of the origin of the local coordinate system (X1,X2,X3) describing the object. This origin is located within the object area and should be the middle point of the object surface. If geometry_type=2, it's the centre of the circular object. If geometry_type=3, it's the centre of the rectangular object. | ||
spectrometer_x_ray_crystal.channel[:].crystal.centre.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle (oriented counter-clockwise when viewing from above) | |
spectrometer_x_ray_crystal.channel[:].crystal.centre.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
spectrometer_x_ray_crystal.channel[:].crystal.centre.z (alpha) | FLT_0D (uncertain) | m | Height | |
spectrometer_x_ray_crystal.channel[:].crystal.curvature_type (alpha) | STRUCTURE | Curvature of the object. | ||
spectrometer_x_ray_crystal.channel[:].crystal.curvature_type.description (alpha) | STR_0D | Verbose description | ||
spectrometer_x_ray_crystal.channel[:].crystal.curvature_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
spectrometer_x_ray_crystal.channel[:].crystal.curvature_type.name (alpha) | STR_0D | Short string identifier | ||
spectrometer_x_ray_crystal.channel[:].crystal.cut (alpha) | [1...N] | INT_1D | Miller indices characterizing the cut of the crystal (can be of length 3 or 4) | |
spectrometer_x_ray_crystal.channel[:].crystal.geometry_type (alpha) | STRUCTURE | Geometry of the object contour. Note that there is some flexibility in the choice of the local coordinate system (X1,X2,X3). The data provider should choose the most convenient coordinate system for the object, respecting the definitions of (X1,X2,X3) indicated below. | ||
spectrometer_x_ray_crystal.channel[:].crystal.geometry_type.description (alpha) | STR_0D | Verbose description | ||
spectrometer_x_ray_crystal.channel[:].crystal.geometry_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
spectrometer_x_ray_crystal.channel[:].crystal.geometry_type.name (alpha) | STR_0D | Short string identifier | ||
spectrometer_x_ray_crystal.channel[:].crystal.identifier (alpha) | STR_0D | ID of the object | ||
spectrometer_x_ray_crystal.channel[:].crystal.material (alpha) | STRUCTURE | Material of the object | ||
spectrometer_x_ray_crystal.channel[:].crystal.material.description (alpha) | STR_0D | Verbose description | ||
spectrometer_x_ray_crystal.channel[:].crystal.material.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
spectrometer_x_ray_crystal.channel[:].crystal.material.name (alpha) | STR_0D | Short string identifier | ||
spectrometer_x_ray_crystal.channel[:].crystal.mesh_type (alpha) | STRUCTURE | Crystal mesh type | ||
spectrometer_x_ray_crystal.channel[:].crystal.mesh_type.description (alpha) | STR_0D | Verbose description | ||
spectrometer_x_ray_crystal.channel[:].crystal.mesh_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
spectrometer_x_ray_crystal.channel[:].crystal.mesh_type.name (alpha) | STR_0D | Short string identifier | ||
spectrometer_x_ray_crystal.channel[:].crystal.outline (alpha) | STRUCTURE | Irregular outline of the object in the (X1, X2) coordinate system, used only if geometry_type/index=1. Do NOT repeat the first point. | ||
spectrometer_x_ray_crystal.channel[:].crystal.outline.x1 (alpha) | [1...N] | FLT_1D (uncertain) | m | Positions along x1 axis |
spectrometer_x_ray_crystal.channel[:].crystal.outline.x2 (alpha) | [spectrometer_x_ray_crystal.channel[:].crystal.outline.x1] | FLT_1D (uncertain) | m | Positions along x2 axis |
spectrometer_x_ray_crystal.channel[:].crystal.radius (alpha) | FLT_0D (uncertain) | m | Radius of the circle, used only if geometry_type/index = 2 | |
spectrometer_x_ray_crystal.channel[:].crystal.surface (alpha) | FLT_0D (uncertain) | m^2 | Surface of the object, derived from the above geometric data | |
spectrometer_x_ray_crystal.channel[:].crystal.thickness (alpha) | FLT_0D (uncertain) | m | Thickness of the crystal | |
spectrometer_x_ray_crystal.channel[:].crystal.wavelength_bragg (alpha) | FLT_0D (uncertain) | m | Bragg wavelength of the crystal | |
spectrometer_x_ray_crystal.channel[:].crystal.x1_curvature (alpha) | FLT_0D (uncertain) | m | Radius of curvature in the X1 direction, to be filled only for curvature_type/index = 2, 4 or 5 | |
spectrometer_x_ray_crystal.channel[:].crystal.x1_unit_vector (alpha) | STRUCTURE | Components of the X1 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X1 vector is more horizontal than X2 (has a smaller abs(Z) component) and oriented in the positive phi direction (counter-clockwise when viewing from above). | ||
spectrometer_x_ray_crystal.channel[:].crystal.x1_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
spectrometer_x_ray_crystal.channel[:].crystal.x1_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
spectrometer_x_ray_crystal.channel[:].crystal.x1_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
spectrometer_x_ray_crystal.channel[:].crystal.x1_width (alpha) | FLT_0D (uncertain) | m | Full width of the object in the X1 direction, used only if geometry_type/index = 3 | |
spectrometer_x_ray_crystal.channel[:].crystal.x2_curvature (alpha) | FLT_0D (uncertain) | m | Radius of curvature in the X2 direction, to be filled only for curvature_type/index = 3 or 5 | |
spectrometer_x_ray_crystal.channel[:].crystal.x2_unit_vector (alpha) | STRUCTURE | Components of the X2 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X2 axis is orthonormal so that uX2 = uX3 x uX1. | ||
spectrometer_x_ray_crystal.channel[:].crystal.x2_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
spectrometer_x_ray_crystal.channel[:].crystal.x2_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
spectrometer_x_ray_crystal.channel[:].crystal.x2_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
spectrometer_x_ray_crystal.channel[:].crystal.x2_width (alpha) | FLT_0D (uncertain) | m | Full width of the object in the X2 direction, used only if geometry_type/index = 3 | |
spectrometer_x_ray_crystal.channel[:].crystal.x3_unit_vector (alpha) | STRUCTURE | Components of the X3 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X3 axis is normal to the object surface and oriented towards the plasma. | ||
spectrometer_x_ray_crystal.channel[:].crystal.x3_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
spectrometer_x_ray_crystal.channel[:].crystal.x3_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
spectrometer_x_ray_crystal.channel[:].crystal.x3_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
spectrometer_x_ray_crystal.channel[:].detection_efficiency (alpha) | [spectrometer_x_ray_crystal.channel[:].energies] | FLT_1D (uncertain) | - | Probability of detection of a photon impacting the detector as a function of its energy |
spectrometer_x_ray_crystal.channel[:].energies (alpha) | [1...N] | FLT_1D (uncertain) | eV | Array of energy values for tabulation of the detection efficiency |
spectrometer_x_ray_crystal.channel[:].energy_bound_lower (alpha) | [1...N, | FLT_2D (uncertain) | eV | Lower energy bound for the photon detection, for each pixel (horizontal, vertical) |
spectrometer_x_ray_crystal.channel[:].energy_bound_upper (alpha) | [1...N, | FLT_2D (uncertain) | eV | Upper energy bound for the photon detection, for each pixel (horizontal, vertical) |
spectrometer_x_ray_crystal.channel[:].exposure_time (alpha) | FLT_0D (uncertain) | s | Exposure time of the measurement | |
spectrometer_x_ray_crystal.channel[:].filter_window (alpha) | [1...N] | STRUCT_ARRAY | Set of filter windows | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].centre (alpha) | STRUCTURE | Coordinates of the origin of the local coordinate system (X1,X2,X3) describing the filter. This origin is located within the filter area and should be the middle point of the filter surface. If geometry_type=2, it's the centre of the circular filter. If geometry_type=3, it's the centre of the rectangular filter. | ||
spectrometer_x_ray_crystal.channel[:].filter_window[:].centre.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle (oriented counter-clockwise when viewing from above) | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].centre.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].centre.z (alpha) | FLT_0D (uncertain) | m | Height | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].curvature_type (alpha) | STRUCTURE | Curvature of the filter. | ||
spectrometer_x_ray_crystal.channel[:].filter_window[:].curvature_type.description (alpha) | STR_0D | Verbose description | ||
spectrometer_x_ray_crystal.channel[:].filter_window[:].curvature_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
spectrometer_x_ray_crystal.channel[:].filter_window[:].curvature_type.name (alpha) | STR_0D | Short string identifier | ||
spectrometer_x_ray_crystal.channel[:].filter_window[:].geometry_type (alpha) | STRUCTURE | Geometry of the filter contour. Note that there is some flexibility in the choice of the local coordinate system (X1,X2,X3). The data provider should choose the most convenient coordinate system for the filter, respecting the definitions of (X1,X2,X3) indicated below. | ||
spectrometer_x_ray_crystal.channel[:].filter_window[:].geometry_type.description (alpha) | STR_0D | Verbose description | ||
spectrometer_x_ray_crystal.channel[:].filter_window[:].geometry_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
spectrometer_x_ray_crystal.channel[:].filter_window[:].geometry_type.name (alpha) | STR_0D | Short string identifier | ||
spectrometer_x_ray_crystal.channel[:].filter_window[:].identifier (alpha) | STR_0D | ID of the filter | ||
spectrometer_x_ray_crystal.channel[:].filter_window[:].material (alpha) | STRUCTURE | Material of the filter window | ||
spectrometer_x_ray_crystal.channel[:].filter_window[:].material.description (alpha) | STR_0D | Verbose description | ||
spectrometer_x_ray_crystal.channel[:].filter_window[:].material.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
spectrometer_x_ray_crystal.channel[:].filter_window[:].material.name (alpha) | STR_0D | Short string identifier | ||
spectrometer_x_ray_crystal.channel[:].filter_window[:].outline (alpha) | STRUCTURE | Irregular outline of the filter in the (X1, X2) coordinate system, used only if geometry_type/index=1. Do NOT repeat the first point. | ||
spectrometer_x_ray_crystal.channel[:].filter_window[:].outline.x1 (alpha) | [1...N] | FLT_1D (uncertain) | m | Positions along x1 axis |
spectrometer_x_ray_crystal.channel[:].filter_window[:].outline.x2 (alpha) | [spectrometer_x_ray_crystal.channel[:].filter_window[:].outline.x1] | FLT_1D (uncertain) | m | Positions along x2 axis |
spectrometer_x_ray_crystal.channel[:].filter_window[:].photon_absorption (alpha) | [spectrometer_x_ray_crystal.channel[:].filter_window[:].wavelengths] | FLT_1D (uncertain) | - | Probability of absorbing a photon passing through the filter as a function of its wavelength |
spectrometer_x_ray_crystal.channel[:].filter_window[:].radius (alpha) | FLT_0D (uncertain) | m | Radius of the circle, used only if geometry_type/index = 2 | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].surface (alpha) | FLT_0D (uncertain) | m^2 | Surface of the filter, derived from the above geometric data | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].thickness (alpha) | FLT_0D (uncertain) | m | Thickness of the filter window | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].wavelength_lower (alpha) | FLT_0D (uncertain) | m | Lower bound of the filter wavelength range | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].wavelength_upper (alpha) | FLT_0D (uncertain) | m | Upper bound of the filter wavelength range | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].wavelengths (alpha) | [1...N] | FLT_1D (uncertain) | m | Array of wavelength values |
spectrometer_x_ray_crystal.channel[:].filter_window[:].x1_curvature (alpha) | FLT_0D (uncertain) | m | Radius of curvature in the X1 direction, to be filled only for curvature_type/index = 2, 4 or 5 | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].x1_unit_vector (alpha) | STRUCTURE | Components of the X1 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X1 vector is more horizontal than X2 (has a smaller abs(Z) component) and oriented in the positive phi direction (counter-clockwise when viewing from above). | ||
spectrometer_x_ray_crystal.channel[:].filter_window[:].x1_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].x1_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].x1_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].x1_width (alpha) | FLT_0D (uncertain) | m | Full width of the filter in the X1 direction, used only if geometry_type/index = 3 | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].x2_curvature (alpha) | FLT_0D (uncertain) | m | Radius of curvature in the X2 direction, to be filled only for curvature_type/index = 3 or 5 | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].x2_unit_vector (alpha) | STRUCTURE | Components of the X2 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X2 axis is orthonormal so that uX2 = uX3 x uX1. | ||
spectrometer_x_ray_crystal.channel[:].filter_window[:].x2_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].x2_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].x2_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].x2_width (alpha) | FLT_0D (uncertain) | m | Full width of the filter in the X2 direction, used only if geometry_type/index = 3 | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].x3_unit_vector (alpha) | STRUCTURE | Components of the X3 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X3 axis is normal to the filter surface and oriented towards the plasma. | ||
spectrometer_x_ray_crystal.channel[:].filter_window[:].x3_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].x3_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
spectrometer_x_ray_crystal.channel[:].filter_window[:].x3_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
spectrometer_x_ray_crystal.channel[:].frame (alpha) | [spectrometer_x_ray_crystal.channel[:].frame[:].time] | STRUCT_ARRAY | Set of frames | |
spectrometer_x_ray_crystal.channel[:].frame[:].counts_bin_n (alpha) | [1...N, | FLT_2D (uncertain) | - | Number of counts detected on each pixel/bin of the binned frame during one exposure time |
spectrometer_x_ray_crystal.channel[:].frame[:].counts_n (alpha) | [1...N, | FLT_2D (uncertain) | - | Number of counts detected on each pixel of the frame during one exposure time |
spectrometer_x_ray_crystal.channel[:].frame[:].time (alpha) | FLT_0D | s | Time | |
spectrometer_x_ray_crystal.channel[:].instrument_function (alpha) | STRUCTURE | Instrument function (to be used in case vertical binning is not used), i.e. response of the detector to a monochromatic emission passing through the spectrometer. The resulting image on the detector will be a 2-D distribution of pixel values, for each wavelength. It can be given as explicit values for each detector pixel (values node) or as a parametric function of wavelength (described by the other nodes) | ||
spectrometer_x_ray_crystal.channel[:].instrument_function.centre (alpha) | [spectrometer_x_ray_crystal.channel[:].z_frames, | FLT_2D (uncertain) | m | Centre (in terms of absolute wavelength) of instrument function |
spectrometer_x_ray_crystal.channel[:].instrument_function.intensity (alpha) | [spectrometer_x_ray_crystal.channel[:].z_frames, | FLT_2D (uncertain) | m | Scaling factor for the instrument function such that convolving the instrument function with an emission spectrum gives the counts per second on the detector |
spectrometer_x_ray_crystal.channel[:].instrument_function.scale (alpha) | [spectrometer_x_ray_crystal.channel[:].z_frames, | FLT_2D (uncertain) | m | Scale of Lorentzian instrument function (full width at half height) |
spectrometer_x_ray_crystal.channel[:].instrument_function.sigma (alpha) | [spectrometer_x_ray_crystal.channel[:].z_frames, | FLT_2D (uncertain) | m | Standard deviation of Gaussian instrument function |
spectrometer_x_ray_crystal.channel[:].instrument_function.type (alpha) | STRUCTURE | Instrument function type | ||
spectrometer_x_ray_crystal.channel[:].instrument_function.type.description (alpha) | STR_0D | Verbose description | ||
spectrometer_x_ray_crystal.channel[:].instrument_function.type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
spectrometer_x_ray_crystal.channel[:].instrument_function.type.name (alpha) | STR_0D | Short string identifier | ||
spectrometer_x_ray_crystal.channel[:].instrument_function.values (alpha) | [1...N, | FLT_3D (uncertain) | sr.m | Explicit instrument function values for the detector. When multiplied by the line-integrated emission spectrum in photons/second/sr/m/m^2 received on a pixel of the detector, gives the detector pixel output in counts/seconds. |
spectrometer_x_ray_crystal.channel[:].instrument_function.wavelengths (alpha) | [1...N] | FLT_1D (uncertain) | m | Array of wavelengths on which the instrument function is defined |
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated (alpha) | STRUCTURE | Profiles proxies are given in the vertical direction of the detector. They are estimated directly from the camera, without tomographic inversion. Binning is allowed so the number of profile points may be lower than the length of z_frames. Physical quantities deduced from the measured spectra are given for each profile point. They correspond to the spectra integrated along lines of sight, defined by a first point given by the centre of the crystal and a second point (depending on the profile point) described below. | ||
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.lines_of_sight_rho_tor_norm (alpha) | [spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.lines_of_sight_second_point.r] | STRUCTURE | - | Shortest distance in rho_tor_norm between lines of sight and magnetic axis, signed with following convention : positive (resp. negative) means the point of shortest distance is above (resp. below) the magnetic axis |
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.lines_of_sight_rho_tor_norm.data (alpha) | [1...N, | FLT_2D (uncertain) | - | Data |
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.lines_of_sight_rho_tor_norm.validity (alpha) | INT_0D | Indicator of the validity of the data for the whole acquisition period. 0: valid from automated processing, 1: valid and certified by the diagnostic RO; - 1 means problem identified in the data processing (request verification by the diagnostic RO), -2: invalid data, should not be used (values lower than -2 have a code-specific meaning detailing the origin of their invalidity) | ||
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.lines_of_sight_rho_tor_norm.validity_timed (alpha) | [spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.time] | INT_1D | Indicator of the validity of the data for each time slice. 0: valid from automated processing, 1: valid and certified by the diagnostic RO; - 1 means problem identified in the data processing (request verification by the diagnostic RO), -2: invalid data, should not be used (values lower than -2 have a code-specific meaning detailing the origin of their invalidity) | |
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.lines_of_sight_second_point (alpha) | STRUCTURE | For each profile point, a line of sight is defined by a first point given by the centre of the crystal and a second point described here. | ||
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.lines_of_sight_second_point.phi (alpha) | [spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.lines_of_sight_second_point.r] | FLT_1D (uncertain) | rad | Toroidal angle (oriented counter-clockwise when viewing from above) |
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.lines_of_sight_second_point.r (alpha) | [1...N] | FLT_1D (uncertain) | m | Major radius |
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.lines_of_sight_second_point.z (alpha) | [spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.lines_of_sight_second_point.r] | FLT_1D (uncertain) | m | Height |
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.t_e (alpha) | [spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.lines_of_sight_second_point.r] | STRUCTURE | eV | Electron temperature (estimated from a spectral fit directly on the output line-integrated signal, without tomographic inversion) |
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.t_e.data (alpha) | [1...N, | FLT_2D (uncertain) | eV | Data |
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.t_e.validity (alpha) | INT_0D | Indicator of the validity of the data for the whole acquisition period. 0: valid from automated processing, 1: valid and certified by the diagnostic RO; - 1 means problem identified in the data processing (request verification by the diagnostic RO), -2: invalid data, should not be used (values lower than -2 have a code-specific meaning detailing the origin of their invalidity) | ||
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.t_e.validity_timed (alpha) | [spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.time] | INT_1D | Indicator of the validity of the data for each time slice. 0: valid from automated processing, 1: valid and certified by the diagnostic RO; - 1 means problem identified in the data processing (request verification by the diagnostic RO), -2: invalid data, should not be used (values lower than -2 have a code-specific meaning detailing the origin of their invalidity) | |
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.t_i (alpha) | [spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.lines_of_sight_second_point.r] | STRUCTURE | eV | Ion temperature (estimated from a spectral fit directly on the output line-integrated signal, without tomographic inversion) |
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.t_i.data (alpha) | [1...N, | FLT_2D (uncertain) | eV | Data |
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.t_i.validity (alpha) | INT_0D | Indicator of the validity of the data for the whole acquisition period. 0: valid from automated processing, 1: valid and certified by the diagnostic RO; - 1 means problem identified in the data processing (request verification by the diagnostic RO), -2: invalid data, should not be used (values lower than -2 have a code-specific meaning detailing the origin of their invalidity) | ||
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.t_i.validity_timed (alpha) | [spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.time] | INT_1D | Indicator of the validity of the data for each time slice. 0: valid from automated processing, 1: valid and certified by the diagnostic RO; - 1 means problem identified in the data processing (request verification by the diagnostic RO), -2: invalid data, should not be used (values lower than -2 have a code-specific meaning detailing the origin of their invalidity) | |
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.time (alpha) | [1...N] | FLT_1D_TYPE | s | Timebase for the dynamic nodes of this probe located at this level of the IDS structure |
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.velocity_tor (alpha) | [spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.lines_of_sight_second_point.r] | STRUCTURE | m.s^-1 | Toroidal velocity (estimated from a spectral fit directly on the output line-integrated signal, without tomographic inversion) |
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.velocity_tor.data (alpha) | [1...N, | FLT_2D (uncertain) | m.s^-1 | Data |
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.velocity_tor.validity (alpha) | INT_0D | Indicator of the validity of the data for the whole acquisition period. 0: valid from automated processing, 1: valid and certified by the diagnostic RO; - 1 means problem identified in the data processing (request verification by the diagnostic RO), -2: invalid data, should not be used (values lower than -2 have a code-specific meaning detailing the origin of their invalidity) | ||
spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.velocity_tor.validity_timed (alpha) | [spectrometer_x_ray_crystal.channel[:].profiles_line_integrated.time] | INT_1D | Indicator of the validity of the data for each time slice. 0: valid from automated processing, 1: valid and certified by the diagnostic RO; - 1 means problem identified in the data processing (request verification by the diagnostic RO), -2: invalid data, should not be used (values lower than -2 have a code-specific meaning detailing the origin of their invalidity) | |
spectrometer_x_ray_crystal.channel[:].reflector (alpha) | [1...N] | STRUCT_ARRAY | Set of reflectors (optional) reflecting the light coming from the plasma towards the crystal. If empty, means that the plasma light directly arrives on the crystal. | |
spectrometer_x_ray_crystal.channel[:].reflector[:].centre (alpha) | STRUCTURE | Coordinates of the origin of the local coordinate system (X1,X2,X3) describing the object. This origin is located within the object area and should be the middle point of the object surface. If geometry_type=2, it's the centre of the circular object. If geometry_type=3, it's the centre of the rectangular object. | ||
spectrometer_x_ray_crystal.channel[:].reflector[:].centre.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle (oriented counter-clockwise when viewing from above) | |
spectrometer_x_ray_crystal.channel[:].reflector[:].centre.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
spectrometer_x_ray_crystal.channel[:].reflector[:].centre.z (alpha) | FLT_0D (uncertain) | m | Height | |
spectrometer_x_ray_crystal.channel[:].reflector[:].curvature_type (alpha) | STRUCTURE | Curvature of the object. | ||
spectrometer_x_ray_crystal.channel[:].reflector[:].curvature_type.description (alpha) | STR_0D | Verbose description | ||
spectrometer_x_ray_crystal.channel[:].reflector[:].curvature_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
spectrometer_x_ray_crystal.channel[:].reflector[:].curvature_type.name (alpha) | STR_0D | Short string identifier | ||
spectrometer_x_ray_crystal.channel[:].reflector[:].geometry_type (alpha) | STRUCTURE | Geometry of the object contour. Note that there is some flexibility in the choice of the local coordinate system (X1,X2,X3). The data provider should choose the most convenient coordinate system for the object, respecting the definitions of (X1,X2,X3) indicated below. | ||
spectrometer_x_ray_crystal.channel[:].reflector[:].geometry_type.description (alpha) | STR_0D | Verbose description | ||
spectrometer_x_ray_crystal.channel[:].reflector[:].geometry_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
spectrometer_x_ray_crystal.channel[:].reflector[:].geometry_type.name (alpha) | STR_0D | Short string identifier | ||
spectrometer_x_ray_crystal.channel[:].reflector[:].identifier (alpha) | STR_0D | ID of the object | ||
spectrometer_x_ray_crystal.channel[:].reflector[:].material (alpha) | STRUCTURE | Material of the object | ||
spectrometer_x_ray_crystal.channel[:].reflector[:].material.description (alpha) | STR_0D | Verbose description | ||
spectrometer_x_ray_crystal.channel[:].reflector[:].material.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
spectrometer_x_ray_crystal.channel[:].reflector[:].material.name (alpha) | STR_0D | Short string identifier | ||
spectrometer_x_ray_crystal.channel[:].reflector[:].outline (alpha) | STRUCTURE | Irregular outline of the object in the (X1, X2) coordinate system, used only if geometry_type/index=1. Do NOT repeat the first point. | ||
spectrometer_x_ray_crystal.channel[:].reflector[:].outline.x1 (alpha) | [1...N] | FLT_1D (uncertain) | m | Positions along x1 axis |
spectrometer_x_ray_crystal.channel[:].reflector[:].outline.x2 (alpha) | [spectrometer_x_ray_crystal.channel[:].reflector[:].outline.x1] | FLT_1D (uncertain) | m | Positions along x2 axis |
spectrometer_x_ray_crystal.channel[:].reflector[:].radius (alpha) | FLT_0D (uncertain) | m | Radius of the circle, used only if geometry_type/index = 2 | |
spectrometer_x_ray_crystal.channel[:].reflector[:].surface (alpha) | FLT_0D (uncertain) | m^2 | Surface of the object, derived from the above geometric data | |
spectrometer_x_ray_crystal.channel[:].reflector[:].x1_curvature (alpha) | FLT_0D (uncertain) | m | Radius of curvature in the X1 direction, to be filled only for curvature_type/index = 2, 4 or 5 | |
spectrometer_x_ray_crystal.channel[:].reflector[:].x1_unit_vector (alpha) | STRUCTURE | Components of the X1 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X1 vector is more horizontal than X2 (has a smaller abs(Z) component) and oriented in the positive phi direction (counter-clockwise when viewing from above). | ||
spectrometer_x_ray_crystal.channel[:].reflector[:].x1_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
spectrometer_x_ray_crystal.channel[:].reflector[:].x1_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
spectrometer_x_ray_crystal.channel[:].reflector[:].x1_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
spectrometer_x_ray_crystal.channel[:].reflector[:].x1_width (alpha) | FLT_0D (uncertain) | m | Full width of the object in the X1 direction, used only if geometry_type/index = 3 | |
spectrometer_x_ray_crystal.channel[:].reflector[:].x2_curvature (alpha) | FLT_0D (uncertain) | m | Radius of curvature in the X2 direction, to be filled only for curvature_type/index = 3 or 5 | |
spectrometer_x_ray_crystal.channel[:].reflector[:].x2_unit_vector (alpha) | STRUCTURE | Components of the X2 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X2 axis is orthonormal so that uX2 = uX3 x uX1. | ||
spectrometer_x_ray_crystal.channel[:].reflector[:].x2_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
spectrometer_x_ray_crystal.channel[:].reflector[:].x2_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
spectrometer_x_ray_crystal.channel[:].reflector[:].x2_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
spectrometer_x_ray_crystal.channel[:].reflector[:].x2_width (alpha) | FLT_0D (uncertain) | m | Full width of the object in the X2 direction, used only if geometry_type/index = 3 | |
spectrometer_x_ray_crystal.channel[:].reflector[:].x3_unit_vector (alpha) | STRUCTURE | Components of the X3 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. The X3 axis is normal to the object surface and oriented towards the plasma. | ||
spectrometer_x_ray_crystal.channel[:].reflector[:].x3_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
spectrometer_x_ray_crystal.channel[:].reflector[:].x3_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
spectrometer_x_ray_crystal.channel[:].reflector[:].x3_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
spectrometer_x_ray_crystal.channel[:].wavelength_frames (alpha) | [1...N, | FLT_2D (uncertain) | m | Wavelength of incoming photons on each pixel of the frames, mainly varying accross the horizontal dimension of the frame. However a 2D map of the wavelength is given since it is not constant vertically due to the elliptical curvature of the photon iso-surfaces |
spectrometer_x_ray_crystal.channel[:].z_frames (alpha) | [1...N] | FLT_1D (uncertain) | m | Height of the observed zone at the focal plane in the plasma, corresponding to the vertical dimension of the frame |
spectrometer_x_ray_crystal.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
spectrometer_x_ray_crystal.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
spectrometer_x_ray_crystal.code.description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
spectrometer_x_ray_crystal.code.library (alpha) | [1...N] | STRUCT_ARRAY | List of external libraries used by the code that has produced this IDS | |
spectrometer_x_ray_crystal.code.library[:].commit (alpha) | STR_0D | Unique commit reference of software | ||
spectrometer_x_ray_crystal.code.library[:].description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
spectrometer_x_ray_crystal.code.library[:].name (alpha) | STR_0D | Name of software | ||
spectrometer_x_ray_crystal.code.library[:].parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
spectrometer_x_ray_crystal.code.library[:].repository (alpha) | STR_0D | URL of software repository | ||
spectrometer_x_ray_crystal.code.library[:].version (alpha) | STR_0D | Unique version (tag) of software | ||
spectrometer_x_ray_crystal.code.name (alpha) | STR_0D | Name of software generating IDS | ||
spectrometer_x_ray_crystal.code.output_flag (alpha) | [spectrometer_x_ray_crystal.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. | |
spectrometer_x_ray_crystal.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
spectrometer_x_ray_crystal.code.repository (alpha) | STR_0D | URL of software repository | ||
spectrometer_x_ray_crystal.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
spectrometer_x_ray_crystal.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
spectrometer_x_ray_crystal.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
spectrometer_x_ray_crystal.ids_properties.creation_date (alpha) | STR_0D | Date at which this data has been produced | ||
spectrometer_x_ray_crystal.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 | ||
spectrometer_x_ray_crystal.ids_properties.name (alpha) | STR_0D | User-defined name for this IDS occurrence | ||
spectrometer_x_ray_crystal.ids_properties.occurrence | INT_0D | |||
spectrometer_x_ray_crystal.ids_properties.occurrence_type (alpha) | STRUCTURE | Type of data contained in this occurrence | ||
spectrometer_x_ray_crystal.ids_properties.occurrence_type.description (alpha) | STR_0D | Verbose description | ||
spectrometer_x_ray_crystal.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. | ||
spectrometer_x_ray_crystal.ids_properties.occurrence_type.name (alpha) | STR_0D | Short string identifier | ||
spectrometer_x_ray_crystal.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. | ||
spectrometer_x_ray_crystal.ids_properties.plugins.infrastructure_get (alpha) | STRUCTURE | Plugin infrastructure used to GET the data | ||
spectrometer_x_ray_crystal.ids_properties.plugins.infrastructure_get.commit (alpha) | STR_0D | Unique commit reference of software | ||
spectrometer_x_ray_crystal.ids_properties.plugins.infrastructure_get.description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
spectrometer_x_ray_crystal.ids_properties.plugins.infrastructure_get.name (alpha) | STR_0D | Name of software used | ||
spectrometer_x_ray_crystal.ids_properties.plugins.infrastructure_get.repository (alpha) | STR_0D | URL of software repository | ||
spectrometer_x_ray_crystal.ids_properties.plugins.infrastructure_get.version (alpha) | STR_0D | Unique version (tag) of software | ||
spectrometer_x_ray_crystal.ids_properties.plugins.infrastructure_put (alpha) | STRUCTURE | Plugin infrastructure used to PUT the data | ||
spectrometer_x_ray_crystal.ids_properties.plugins.infrastructure_put.commit (alpha) | STR_0D | Unique commit reference of software | ||
spectrometer_x_ray_crystal.ids_properties.plugins.infrastructure_put.description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
spectrometer_x_ray_crystal.ids_properties.plugins.infrastructure_put.name (alpha) | STR_0D | Name of software used | ||
spectrometer_x_ray_crystal.ids_properties.plugins.infrastructure_put.repository (alpha) | STR_0D | URL of software repository | ||
spectrometer_x_ray_crystal.ids_properties.plugins.infrastructure_put.version (alpha) | STR_0D | Unique version (tag) of software | ||
spectrometer_x_ray_crystal.ids_properties.plugins.node (alpha) | [1...N] | STRUCT_ARRAY | Set of IDS nodes for which a plugin has been applied | |
spectrometer_x_ray_crystal.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. | |
spectrometer_x_ray_crystal.ids_properties.plugins.node[:].get_operation[:].commit (alpha) | STR_0D | Unique commit reference of software | ||
spectrometer_x_ray_crystal.ids_properties.plugins.node[:].get_operation[:].description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
spectrometer_x_ray_crystal.ids_properties.plugins.node[:].get_operation[:].name (alpha) | STR_0D | Name of software used | ||
spectrometer_x_ray_crystal.ids_properties.plugins.node[:].get_operation[:].parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
spectrometer_x_ray_crystal.ids_properties.plugins.node[:].get_operation[:].repository (alpha) | STR_0D | URL of software repository | ||
spectrometer_x_ray_crystal.ids_properties.plugins.node[:].get_operation[:].version (alpha) | STR_0D | Unique version (tag) of software | ||
spectrometer_x_ray_crystal.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. | ||
spectrometer_x_ray_crystal.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) | |
spectrometer_x_ray_crystal.ids_properties.plugins.node[:].put_operation[:].commit (alpha) | STR_0D | Unique commit reference of software | ||
spectrometer_x_ray_crystal.ids_properties.plugins.node[:].put_operation[:].description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
spectrometer_x_ray_crystal.ids_properties.plugins.node[:].put_operation[:].name (alpha) | STR_0D | Name of software used | ||
spectrometer_x_ray_crystal.ids_properties.plugins.node[:].put_operation[:].parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
spectrometer_x_ray_crystal.ids_properties.plugins.node[:].put_operation[:].repository (alpha) | STR_0D | URL of software repository | ||
spectrometer_x_ray_crystal.ids_properties.plugins.node[:].put_operation[:].version (alpha) | STR_0D | Unique version (tag) of software | ||
spectrometer_x_ray_crystal.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) | |
spectrometer_x_ray_crystal.ids_properties.plugins.node[:].readback[:].commit (alpha) | STR_0D | Unique commit reference of software | ||
spectrometer_x_ray_crystal.ids_properties.plugins.node[:].readback[:].description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
spectrometer_x_ray_crystal.ids_properties.plugins.node[:].readback[:].name (alpha) | STR_0D | Name of software used | ||
spectrometer_x_ray_crystal.ids_properties.plugins.node[:].readback[:].parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
spectrometer_x_ray_crystal.ids_properties.plugins.node[:].readback[:].repository (alpha) | STR_0D | URL of software repository | ||
spectrometer_x_ray_crystal.ids_properties.plugins.node[:].readback[:].version (alpha) | STR_0D | Unique version (tag) of software | ||
spectrometer_x_ray_crystal.ids_properties.provenance (alpha) | STRUCTURE | Provenance information about this IDS | ||
spectrometer_x_ray_crystal.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 | |
spectrometer_x_ray_crystal.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. | ||
spectrometer_x_ray_crystal.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. | |
spectrometer_x_ray_crystal.ids_properties.provider (alpha) | STR_0D | Name of the person in charge of producing this data | ||
spectrometer_x_ray_crystal.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. | ||
spectrometer_x_ray_crystal.ids_properties.version_put (alpha) | STRUCTURE | Version of the access layer package used to PUT this IDS | ||
spectrometer_x_ray_crystal.ids_properties.version_put.access_layer (alpha) | STR_0D | Version of Access Layer used to PUT this IDS | ||
spectrometer_x_ray_crystal.ids_properties.version_put.access_layer_language (alpha) | STR_0D | Programming language of the Access Layer high level API used to PUT this IDS | ||
spectrometer_x_ray_crystal.ids_properties.version_put.data_dictionary (alpha) | STR_0D | Version of Data Dictionary used to PUT this IDS | ||
spectrometer_x_ray_crystal.latency (alpha) | FLT_0D (uncertain) | s | Upper bound of the delay between physical information received by the detector and data available on the real-time (RT) network. | |
spectrometer_x_ray_crystal.time (alpha) | [1...N] | FLT_1D_TYPE | s | Generic time |