Dataset Metadata#
Each ICAT dataset can have metadata associated with it.
ICAT |
Description |
Type |
Units |
NeXus |
|---|---|---|---|---|
datasetName |
Name of the dataset |
NX_CHAR |
title |
|
scanNumber |
Scan number |
NX_CHAR |
scanNumber |
|
proposal |
Proposal code |
NX_CHAR |
proposal |
|
scanType |
Scan type can be ‘step_by_step’ or ‘continuous’ |
NX_CHAR |
dataset_type |
|
location |
Scan starting date |
NX_CHAR |
folder_path |
|
startDate |
Scan starting date |
NX_DATE_TIME |
start_time |
|
endDate |
Scan ending date |
NX_DATE_TIME |
end_time |
|
definition |
Techniques used to collect this dataset |
NX_CHAR |
definition |
|
technique_pid |
List of space-separated techniques identifiers used to collect this dataset, eg. PaNET ids |
NX_CHAR |
technique_pid |
|
DOI_abstract |
Abstract of the DOI |
NX_CHAR |
doi_abstract |
|
DOI_title |
Title fo the DOI |
NX_CHAR |
doi_title |
|
DOI_users |
Users of the DOI. Comma separated string |
NX_CHAR |
doi_users |
|
Project_name |
Name of project |
NX_CHAR |
project_name |
|
machine |
Name of the machine that collects the data |
NX_CHAR |
machine |
|
software |
Name of the software that collects the data |
NX_CHAR |
software |
|
group_by |
Comma separated list of parameters name that will be used to represent the data acquisition as a tree. Mostly for visualization purposes |
NX_CHAR |
group_by |
|
saxs_definition |
Technique used to collect this dataset |
NX_CHAR |
SAXS.definition |
|
saxs_definition.version |
Version |
NX_CHAR |
SAXS.version |
|
SAXS_directory |
Data collection directory |
NX_CHAR |
SAXS.directory |
|
SAXS_experimentType |
Type of experiment |
NX_CHAR |
SAXS.experimentType |
|
SAXS_prefix |
NX_CHAR |
SAXS.prefix |
||
SAXS_maskFile |
NX_CHAR |
SAXS.maskFile |
||
SAXS_numberFrames |
NX_CHAR |
SAXS.numberFrames |
||
SAXS_timePerFrame |
NX_CHAR |
SAXS.timePerFrame |
||
SAXS_concentration |
NX_CHAR |
SAXS.concentration |
||
SAXS_comments |
NX_CHAR |
SAXS.comments |
||
SAXS_code |
NX_CHAR |
SAXS.code |
||
SAXS_detector_distance |
NX_CHAR |
SAXS.detector_distance |
||
SAXS_waveLength |
NX_CHAR |
SAXS.waveLength |
||
SAXS_pixelSizeX |
NX_CHAR |
SAXS.pixelSizeX |
||
SAXS_pixelSizeY |
NX_CHAR |
SAXS.pixelSizeY |
||
SAXS_beam_center_x |
NX_CHAR |
SAXS.beam_center_x |
||
SAXS_beam_center_y |
NX_CHAR |
SAXS.beam_center_y |
||
SAXS_normalisation |
NX_CHAR |
SAXS.normalisation |
||
SAXS_diode_currents |
NX_CHAR |
SAXS.diode_currents |
||
SAXS_acronym |
NX_CHAR |
SAXS.acronym |
||
SAXS_transmission |
NX_CHAR |
SAXS.transmission |
||
SAXS_storage_temperature |
NX_CHAR |
SAXS.storage_temperature |
||
SAXS_exposure_temperature |
NX_CHAR |
SAXS.exposure_temperature |
||
SAXS_column_type |
HPLC column type. [ex. Agilent BioSEC 130] |
NX_CHAR |
SAXS.column_type |
|
SAXS_flow_rate |
NX_CHAR |
SAXS.flow_rate |
||
SAXS_hplc_port |
NX_CHAR |
SAXS.hplc_port |
||
SAXS_sample_type |
It can be buffer or sample |
NX_CHAR |
SAXS.sample_type |
|
SAXS_run_number |
It can be buffer or sample |
NX_CHAR |
SAXS.run_number |
|
SAXS_experiment_type |
It the kind of experiment: sample changer or HPLC |
NX_CHAR |
SAXS.experiment_type |
|
SAXS_guinier_rg |
Guinier radius of giration |
NX_CHAR |
SAXS.guinier_rg |
|
SAXS_guinier_points |
Points of the Guinier region |
NX_CHAR |
SAXS.guinier_points |
|
SAXS_guinier_i0 |
Guinier radius of giration |
NX_CHAR |
SAXS.guinier_i0 |
|
SAXS_rg |
Calculated radious of giration. It can be calculated with Gnom or BIFT |
NX_CHAR |
SAXS.rg |
|
SAXS_total |
NX_CHAR |
SAXS.total |
||
SAXS_d_max |
NX_CHAR |
SAXS.d_max |
||
SAXS_porod_volume |
NX_CHAR |
SAXS.porod_volume |
||
SAXS_porod_MM_volume_estimation |
NX_CHAR |
SAXS.porod_MM_volume_estimation |
||
SAXS_frames_averaged |
NX_CHAR |
SAXS.frames_averaged |
||
MX_aperture |
Aperture size in microns |
NX_CHAR |
MX.aperture |
|
MX_kappa_settings_id |
Identifier used to distinguished between multiple kappa setting within the same data collection |
NX_CHAR |
MX.kappa_settings_id |
|
MX_beamShape |
Beam shape at sample position |
NX_CHAR |
MX.beamShape |
|
MX_beamSizeAtSampleX |
Horizontal beam size in mm at sample position |
NX_CHAR |
mm |
MX.beamSizeAtSampleX |
MX_beamSizeAtSampleY |
Vertical beam size in mm at sample position |
NX_CHAR |
mm |
MX.beamSizeAtSampleY |
MX_dataCollectionId |
ISPyB data collection id |
NX_CHAR |
MX.dataCollectionId |
|
MX_detectorDistance |
Distance from detector to sample position |
NX_CHAR |
mm |
MX.detectorDistance |
MX_directory |
Data collection directory |
NX_CHAR |
MX.directory |
|
MX_exposureTime |
Exposure time per frame |
NX_CHAR |
s |
MX.exposureTime |
MX_flux |
Photon flux at the sample position |
NX_CHAR |
photons/s |
MX.flux |
MX_fluxEnd |
Flux in photon/s before data collection |
NX_CHAR |
MX.fluxEnd |
|
MX_motors_name |
Motor names |
NX_CHAR |
MX.motorsName |
|
MX_motors_value |
Motor positions in mm |
NX_CHAR |
MX.motorsValue |
|
MX_numberOfImages |
Number of images |
NX_CHAR |
MX.numberOfImages |
|
MX_oscillationOverlap |
Overlap between frames |
NX_CHAR |
degrees |
MX.oscillationOverlap |
MX_oscillationRange |
Degrees rotated per frame |
NX_CHAR |
degrees |
MX.oscillationRange |
MX_oscillationStart |
Starting angle of data collection |
NX_CHAR |
degrees |
MX.oscillationStart |
MX_resolution |
Resolution at the edge of the detector |
NX_CHAR |
angstroms |
MX.resolution |
MX_resolution_at_corner |
Resolution at the corner of the detector |
NX_CHAR |
angstroms |
MX.resolution_at_corner |
MX_scanType |
mxCuBE experiment type |
NX_CHAR |
MX.scanType |
|
MX_startImageNumber |
Data collection image start number |
NX_CHAR |
MX.startImageNumber |
|
MX_template |
Image file name template |
NX_CHAR |
MX.template |
|
MX_transmission |
Transmission in % |
NX_CHAR |
MX.transmission |
|
MX_wavelength |
Wavelength in A |
NX_CHAR |
MX.wavelength |
|
MX_xBeam |
Horizontal beam centre in mm |
NX_CHAR |
MX.xBeam |
|
MX_yBeam |
Vertical beam centre in mm |
NX_CHAR |
MX.yBeam |
|
MX_rotation_axis |
Name of the rotation axis |
NX_CHAR |
MX.rotation_axis |
|
MX_axis_range |
Axis range |
NX_CHAR |
MX.axis_range |
|
MX_axis_start |
Rotation start angle |
NX_CHAR |
MX.axis_start |
|
MX_axis_end |
Rotation end angle |
NX_CHAR |
MX.axis_end |
|
MX_position_id |
Identifier of the position within the crystal |
NX_CHAR |
MX.position_id |
|
MX_characterisation_id |
Identifier of the characterisation |
NX_CHAR |
MX.characterisation_id |
|
MX_crystalPositionName |
Centered position, line and grid ID |
NX_CHAR |
MX.crystalPositionName |
|
MXSAD_min_resolution |
SAD minimal resolution |
NX_CHAR |
angstrom |
MX.SAD.min_resolution |
MXSAD_max_resolution |
SAD maximal resolution |
NX_CHAR |
angstrom |
MX.SAD.max_resolution |
MXSAD_enantiomorph |
SAD enantiomorph |
NX_CHAR |
MX.SAD.enantiomorph |
|
MXSAD_space_group |
SAD space group |
NX_CHAR |
MX.SAD.space_group |
|
MXSAD_step |
SAD step |
NX_CHAR |
MX.SAD.step |
|
MXSAD_solvent |
SAD solvent |
NX_CHAR |
MX.SAD.solvent |
|
MXSAD_pseudo_free_cc |
SAD pseudo_free_cc |
NX_CHAR |
MX.SAD.pseudo_free_cc |
|
MXSAD_cc_partial_model |
SAD cc_partial_model |
NX_CHAR |
MX.SAD.cc_partial_model |
|
MXSAD_chain_count |
SAD chain_count |
NX_CHAR |
MX.SAD.chain_count |
|
MXSAD_residues_count |
SAD residues_count |
NX_CHAR |
MX.SAD.residues_count |
|
MXSAD_average_fragment_length |
SAD average_fragment_length |
NX_CHAR |
MX.SAD.average_fragment_length |
|
MXSAD_PDB_file |
SAD PDB file path |
NX_CHAR |
MX.SAD.PDB_file |
|
MXSAD_MTZ_file |
SAD MTZ file path |
NX_CHAR |
MX.SAD.MTZ_file |
|
MXMR_step |
MR Step |
NX_CHAR |
MX.MR.step |
|
MXMR_space_group |
MR space group |
NX_CHAR |
MX.MR.space_group |
|
MXMR_min_resolution |
MR min resolution |
NX_CHAR |
MX.MR.min_resolution |
|
MXMR_max_resolution |
MR max resolution |
NX_CHAR |
MX.MR.max_resolution |
|
MXMRPhasing_source |
Describes the pdb suource: Alphafold, user, unit cell |
NX_CHAR |
MX.MR.Phasing.source |
|
MXMRPhasing_search_model |
Identifier to the search model. It can be a link |
NX_CHAR |
MX.MR.Phasing.search_model |
|
MXMRPhasing_space_group |
Phasing space group |
NX_CHAR |
MX.MR.Phasing.space_group |
|
MXMRPhasing_number_of_search_models_found |
Models found |
NX_CHAR |
MX.MR.Phasing.number_of_search_models_found |
|
MXMRPhasing_best_RFZ |
Best RFZ |
NX_CHAR |
MX.MR.Phasing.best_RFZ |
|
MXMRPhasing_best_TFZ |
Best TTZ |
NX_CHAR |
MX.MR.Phasing.best_TFZ |
|
MXMRPhasing_LLG |
Best LLG |
NX_CHAR |
MX.MR.Phasing.LLG |
|
MXMRPhasing_monomer_form_count |
Number of monomers |
NX_CHAR |
MX.MR.Phasing.monomer_form_count |
|
MXMRPhasing_RFZ_list |
List of RFZ |
NX_CHAR |
MX.MR.Phasing.RFZ_list |
|
MXMRPhasing_TFZ_list |
List of TFZ |
NX_CHAR |
MX.MR.Phasing.TFZ_list |
|
MXMRPhasing_PDB_file |
pdb file path |
NX_CHAR |
MX.MR.Phasing.PDB_file |
|
MXMRPhasing_MTZ_file |
MTZ file path |
NX_CHAR |
MX.MR.Phasing.MTZ_file |
|
MXMRPhasing_MAP_2FOFC |
2FOFC map file path |
NX_CHAR |
MX.MR.Phasing.MAP_2FOFC |
|
MXMRPhasing_MAP_FOFC |
FOFC map file path |
NX_CHAR |
MX.MR.Phasing.MAP_FOFC |
|
MXMRRefinement_R_free |
Free-r |
NX_CHAR |
MX.MR.Refinement.R_free |
|
MXMRRefinement_R_cryst |
R crystal |
NX_CHAR |
MX.MR.Refinement.R_cryst |
|
MXMRRefinement_PDB_file |
List of TFZ |
NX_CHAR |
MX.MR.Refinement.PDB_file |
|
MXMRRefinement_MTZ_file |
List of TFZ |
NX_CHAR |
MX.MR.Refinement.MTZ_file |
|
MXMRRefinement_MAP_FOFC |
MAP_FOFC file path |
NX_CHAR |
MX.MR.Refinement.MAP_FOFC |
|
MXMRRefinement_MAP_2FOFC |
MAP_2FOFC file path |
NX_CHAR |
MX.MR.Refinement.MAP_2FOFC |
|
MXMRLigandFitting_ligand_FOFC_CC |
Ligand FOFC_CC |
NX_CHAR |
MX.MR.LigandFitting.ligand_FOFC_CC |
|
MXMRLigandFitting_R_free |
Free-r |
NX_CHAR |
MX.MR.LigandFitting.R_free |
|
MXMRLigandFitting_R_cryst |
R crystal |
NX_CHAR |
MX.MR.LigandFitting.R_cryst |
|
MXMRLigandFitting_B_factor |
B factor |
NX_CHAR |
MX.MR.LigandFitting.B_factor |
|
MXMRLigandFitting_occupancy |
Occupancy |
NX_CHAR |
MX.MR.LigandFitting.occupancy |
|
MXMRLigandFitting_PDB_file |
pdb file path |
NX_CHAR |
MX.MR.LigandFitting.PDB_file |
|
MXMRLigandFitting_MTZ_file |
mtz file |
NX_CHAR |
MX.MR.LigandFitting.MTZ_file |
|
MXMRLigandFitting_PNG_2FOFC |
snapshot of the ligand in 2FO-FC electron density |
NX_CHAR |
MX.MR.LigandFitting.PNG_2FOFC |
|
MXMRLigandFitting_PNG_FOFC |
snapshot of the ligand in FO-FC electron density |
NX_CHAR |
MX.MR.LigandFitting.PNG_FOFC |
|
MXMRLigandFitting_GIF_file |
animated GIF of the ligand in FO-FC electron density |
NX_CHAR |
MX.MR.LigandFitting.GIF_file |
|
MXMRLigandFitting_ligand_XYZ |
x,y,z coordinates of the ligand |
NX_CHAR |
MX.MR.LigandFitting.ligand_XYZ |
|
MXMRLigandFitting_ligand_name |
name of the ligand |
NX_CHAR |
MX.MR.LigandFitting.ligand_name |
|
MXMRLigandFitting_MAP_FOFC |
MAP_FOFC file path |
NX_CHAR |
MX.MR.LigandFitting.MAP_FOFC |
|
MXMRLigandFitting_MAP_2FOFC |
MAP_2FOFC file path |
NX_CHAR |
MX.MR.LigandFitting.MAP_2FOFC |
|
MXAutoprocIntegration_start_image_number |
First image number of the integration |
NX_CHAR |
MX.AutoprocIntegration.start_image_number |
|
MXAutoprocIntegration_end_image_number |
Last image number of the integration |
NX_CHAR |
MX.AutoprocIntegration.end_image_number |
|
MXAutoprocIntegration_detector_distance |
Refined detector distance |
NX_CHAR |
MX.AutoprocIntegration.detector_distance |
|
MXAutoprocIntegration_beam_x |
Refined beam x |
NX_CHAR |
MX.AutoprocIntegration.beam_x |
|
MXAutoprocIntegration_beam_y |
Refined beam y |
NX_CHAR |
MX.AutoprocIntegration.beam_y |
|
MXAutoprocIntegration_rotation_axis_x |
X position of the rotation axis |
NX_CHAR |
MX.AutoprocIntegration.rotation_axis_x |
|
MXAutoprocIntegration_rotation_axis_y |
Y position of the rotation axis |
NX_CHAR |
MX.AutoprocIntegration.rotation_axis_y |
|
MXAutoprocIntegration_rotation_axis_z |
Z position of the rotation axis |
NX_CHAR |
MX.AutoprocIntegration.rotation_axis_z |
|
MXAutoprocIntegration_beam_vector_x |
Vector X |
NX_CHAR |
MX.AutoprocIntegration.beam_vector_x |
|
MXAutoprocIntegration_beam_vector_y |
Vector Y |
NX_CHAR |
MX.AutoprocIntegration.beam_vector_y |
|
MXAutoprocIntegration_beam_vector_z |
Vector Z |
NX_CHAR |
MX.AutoprocIntegration.beam_vector_z |
|
MXAutoprocIntegration_space_group |
Space group |
NX_CHAR |
MX.AutoprocIntegration.space_group |
|
MXAutoprocIntegration_cell_a |
cell a |
NX_CHAR |
MX.AutoprocIntegration.cell_a |
|
MXAutoprocIntegration_cell_b |
cell b |
NX_CHAR |
MX.AutoprocIntegration.cell_b |
|
MXAutoprocIntegration_cell_c |
cell c |
NX_CHAR |
MX.AutoprocIntegration.cell_c |
|
MXAutoprocIntegration_cell_alpha |
cell alpha |
NX_CHAR |
MX.AutoprocIntegration.cell_alpha |
|
MXAutoprocIntegration_cell_beta |
cell beta |
NX_CHAR |
MX.AutoprocIntegration.cell_beta |
|
MXAutoprocIntegration_cell_gamma |
cell gamma |
NX_CHAR |
MX.AutoprocIntegration.cell_gamma |
|
MXAutoprocIntegration_anomalous |
anomalous |
NX_CHAR |
MX.AutoprocIntegration.anomalous |
|
MXAutoprocIntegrationScaling_overall_resolution_limit_low |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_resolution_limit_low |
||
MXAutoprocIntegrationScaling_overall_resolution_limit_high |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_resolution_limit_high |
||
MXAutoprocIntegrationScaling_overall_r_merge |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_r_merge |
||
MXAutoprocIntegrationScaling_overall_r_meas_within_IPlus_IMinus |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_r_meas_within_IPlus_IMinus |
||
MXAutoprocIntegrationScaling_overall_r_meas_all_IPlus_IMinus |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_r_meas_all_IPlus_IMinus |
||
MXAutoprocIntegrationScaling_overall_r_pim_within_IPlus_IMinus |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_r_pim_within_IPlus_IMinus |
||
MXAutoprocIntegrationScaling_overall_r_pim_all_IPlus_IMinus |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_r_pim_all_IPlus_IMinus |
||
MXAutoprocIntegrationScaling_overall_fractional_partial_bias |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_fractional_partial_bias |
||
MXAutoprocIntegrationScaling_overall_n_total_observations |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_n_total_observations |
||
MXAutoprocIntegrationScaling_overall_n_total_unique_observations |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_n_total_unique_observations |
||
MXAutoprocIntegrationScaling_overall_mean_I_over_sigI |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_mean_I_over_sigI |
||
MXAutoprocIntegrationScaling_overall_completeness |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_completeness |
||
MXAutoprocIntegrationScaling_overall_multiplicity |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_multiplicity |
||
MXAutoprocIntegrationScaling_overall_anomalous_completeness |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_anomalous_completeness |
||
MXAutoprocIntegrationScaling_overall_anomalous_multiplicity |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_anomalous_multiplicity |
||
MXAutoprocIntegrationScaling_overall_anomalous |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_anomalous |
||
MXAutoprocIntegrationScaling_overall_cc_half |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_cc_half |
||
MXAutoprocIntegrationScaling_overall_ccAno |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_ccAno |
||
MXAutoprocIntegrationScaling_overall_sigAno |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_sigAno |
||
MXAutoprocIntegrationScaling_overall_isa |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_isa |
||
MXAutoprocIntegrationScaling_overall_completeness_spherical |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_completeness_spherical |
||
MXAutoprocIntegrationScaling_overall_completeness_ellipsoidal |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_completeness_ellipsoidal |
||
MXAutoprocIntegrationScaling_overall_anomalous_completeness_spherical |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_anomalous_completeness_spherical |
||
MXAutoprocIntegrationScaling_overall_anomalous_completeness_ellipsoidal |
NX_CHAR |
MX.AutoprocIntegration.Scaling.overall_anomalous_completeness_ellipsoidal |
||
MXAutoprocIntegrationScaling_inner_resolution_limit_low |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_resolution_limit_low |
||
MXAutoprocIntegrationScaling_inner_resolution_limit_high |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_resolution_limit_high |
||
MXAutoprocIntegrationScaling_inner_r_merge |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_r_merge |
||
MXAutoprocIntegrationScaling_inner_r_meas_within_IPlus_IMinus |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_r_meas_within_IPlus_IMinus |
||
MXAutoprocIntegrationScaling_inner_r_meas_all_IPlus_IMinus |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_r_meas_all_IPlus_IMinus |
||
MXAutoprocIntegrationScaling_inner_r_pim_within_IPlus_IMinus |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_r_pim_within_IPlus_IMinus |
||
MXAutoprocIntegrationScaling_inner_r_pim_all_IPlus_IMinus |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_r_pim_all_IPlus_IMinus |
||
MXAutoprocIntegrationScaling_inner_fractional_partial_bias |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_fractional_partial_bias |
||
MXAutoprocIntegrationScaling_inner_n_total_observations |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_n_total_observations |
||
MXAutoprocIntegrationScaling_inner_n_total_unique_observations |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_n_total_unique_observations |
||
MXAutoprocIntegrationScaling_inner_mean_I_over_sigI |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_mean_I_over_sigI |
||
MXAutoprocIntegrationScaling_inner_completeness |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_completeness |
||
MXAutoprocIntegrationScaling_inner_multiplicity |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_multiplicity |
||
MXAutoprocIntegrationScaling_inner_anomalous_completeness |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_anomalous_completeness |
||
MXAutoprocIntegrationScaling_inner_anomalous_multiplicity |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_anomalous_multiplicity |
||
MXAutoprocIntegrationScaling_inner_anomalous |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_anomalous |
||
MXAutoprocIntegrationScaling_inner_cc_half |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_cc_half |
||
MXAutoprocIntegrationScaling_inner_ccAno |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_ccAno |
||
MXAutoprocIntegrationScaling_inner_sigAno |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_sigAno |
||
MXAutoprocIntegrationScaling_inner_isa |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_isa |
||
MXAutoprocIntegrationScaling_inner_completeness_spherical |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_completeness_spherical |
||
MXAutoprocIntegrationScaling_inner_completeness_ellipsoidal |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_completeness_ellipsoidal |
||
MXAutoprocIntegrationScaling_inner_anomalous_completeness_spherical |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_anomalous_completeness_spherical |
||
MXAutoprocIntegrationScaling_inner_anomalous_completeness_ellipsoidal |
NX_CHAR |
MX.AutoprocIntegration.Scaling.inner_anomalous_completeness_ellipsoidal |
||
MXAutoprocIntegrationScaling_outer_resolution_limit_low |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_resolution_limit_low |
||
MXAutoprocIntegrationScaling_outer_resolution_limit_high |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_resolution_limit_high |
||
MXAutoprocIntegrationScaling_outer_r_merge |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_r_merge |
||
MXAutoprocIntegrationScaling_outer_r_meas_within_IPlus_IMinus |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_r_meas_within_IPlus_IMinus |
||
MXAutoprocIntegrationScaling_outer_r_meas_all_IPlus_IMinus |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_r_meas_all_IPlus_IMinus |
||
MXAutoprocIntegrationScaling_outer_r_pim_within_IPlus_IMinus |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_r_pim_within_IPlus_IMinus |
||
MXAutoprocIntegrationScaling_outer_r_pim_all_IPlus_IMinus |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_r_pim_all_IPlus_IMinus |
||
MXAutoprocIntegrationScaling_outer_fractional_partial_bias |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_fractional_partial_bias |
||
MXAutoprocIntegrationScaling_outer_n_total_observations |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_n_total_observations |
||
MXAutoprocIntegrationScaling_outer_n_total_unique_observations |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_n_total_unique_observations |
||
MXAutoprocIntegrationScaling_outer_mean_I_over_sigI |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_mean_I_over_sigI |
||
MXAutoprocIntegrationScaling_outer_completeness |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_completeness |
||
MXAutoprocIntegrationScaling_outer_multiplicity |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_multiplicity |
||
MXAutoprocIntegrationScaling_outer_anomalous_completeness |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_anomalous_completeness |
||
MXAutoprocIntegrationScaling_outer_anomalous_multiplicity |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_anomalous_multiplicity |
||
MXAutoprocIntegrationScaling_outer_anomalous |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_anomalous |
||
MXAutoprocIntegrationScaling_outer_cc_half |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_cc_half |
||
MXAutoprocIntegrationScaling_outer_ccAno |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_ccAno |
||
MXAutoprocIntegrationScaling_outer_sigAno |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_sigAno |
||
MXAutoprocIntegrationScaling_outer_isa |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_isa |
||
MXAutoprocIntegrationScaling_outer_completeness_spherical |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_completeness_spherical |
||
MXAutoprocIntegrationScaling_outer_completeness_ellipsoidal |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_completeness_ellipsoidal |
||
MXAutoprocIntegrationScaling_outer_anomalous_completeness_spherical |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_anomalous_completeness_spherical |
||
MXAutoprocIntegrationScaling_outer_anomalous_completeness_ellipsoidal |
NX_CHAR |
MX.AutoprocIntegration.Scaling.outer_anomalous_completeness_ellipsoidal |
||
EM_protein_acronym |
Protein acronym |
NX_CHAR |
EM.protein_acronym |
|
EM_voltage |
Voltage |
NX_CHAR |
EM.voltage |
|
EM_magnification |
Magnification |
NX_CHAR |
EM.magnification |
|
EM_images_count |
Number of images in movie |
NX_CHAR |
EM.images_count |
|
EM_position_x |
Position X |
NX_CHAR |
EM.position_x |
|
EM_position_y |
Position Y |
NX_CHAR |
EM.position_y |
|
EM_dose_initial |
Dose initial |
NX_CHAR |
EM.dose_initial |
|
EM_dose_per_frame |
Dose per frame |
NX_CHAR |
EM.dose_per_frame |
|
EM_spherical_aberration |
Spherical aberration |
NX_CHAR |
EM.spherical_aberration |
|
EM_amplitude_contrast |
Amplitude contrast |
NX_CHAR |
EM.amplitude_contrast |
|
EM_sampling_rate |
samplingRate |
NX_CHAR |
EM.sampling_rate |
|
EM_tilt_angle |
tilt_angle |
NX_CHAR |
EM.tilt_angle |
|
EM_grid_name |
grid_name |
NX_CHAR |
EM.grid_name |
|
EMMotionCorrection_total_motion |
Total motion of the sample |
NX_CHAR |
EM.motioncorrection.total_motion |
|
EMMotionCorrection_average_motion |
Average motion |
NX_CHAR |
EM.motioncorrection.average_motion |
|
EMMotionCorrection_frame_range |
Motion frame range |
NX_CHAR |
EM.motioncorrection.frame_range |
|
EMMotionCorrection_frame_dose |
Dose/frame |
NX_CHAR |
EM.motioncorrection.frame_dose |
|
EMMotionCorrection_total_dose |
Total dose |
NX_CHAR |
EM.motioncorrection.total_dose |
|
EMCTF_resolution_limit |
Limit of the resolution |
NX_CHAR |
EM.ctf.resolution_limit |
|
EMCTF_correlation |
NX_CHAR |
EM.ctf.correlation |
||
EMCTF_defocus_u |
NX_CHAR |
EM.ctf.defocus_u |
||
EMCTF_defocus_v |
NX_CHAR |
EM.ctf.defocus_v |
||
EMCTF_angle |
NX_CHAR |
EM.ctf.angle |
||
EMCTF_estimated_b_factor |
NX_CHAR |
EM.ctf.estimated_b_factor |
||
PTYCHO_propagation |
Propagation may be near or far |
NX_CHAR |
PTYCHO.propagation |
|
PTYCHO_beamSize |
Beam size on the sample in microns |
NX_FLOAT |
micron |
PTYCHO.beamSize |
PTYCHO_stepSize |
Step size during scan |
NX_FLOAT |
micron |
PTYCHO.stepSize |
PTYCHO_focusToDetectorDistance |
Focus to detector distance |
NX_FLOAT |
mm |
PTYCHO.focusToDetectorDistance |
PTYCHO_countTime |
Step size during scan |
NX_FLOAT |
s |
PTYCHO.countTime |
PTYCHO_parameters |
Ptycho parameters |
NX_CHAR |
PTYCHO.parameters |
|
PTYCHO_tomoParameters |
Ptycho tomography parameters |
NX_CHAR |
PTYCHO.tomoParameters |
|
PTYCHO_refN |
Ptycho parameters |
NX_FLOAT |
PTYCHO.refN |
|
PTYCHO_darkN |
Ptycho parameters |
NX_FLOAT |
PTYCHO.darkN |
|
PTYCHO_pixelSize |
Ptycho parameters |
NX_CHAR |
micron |
PTYCHO.pixelSize |
PTYCHO_Axis1_name |
Scan motor in the horizontal direction |
NX_CHAR |
PTYCHO.Axis1.name |
|
PTYCHO_Axis1_range |
Range of the moves in microns |
NX_FLOAT |
micron |
PTYCHO.Axis1.range |
PTYCHO_Axis2_name |
Scan motor in the vertical direction |
NX_CHAR |
PTYCHO.Axis2.name |
|
PTYCHO_Axis2_range |
Range of the moves in microns |
NX_FLOAT |
micron |
PTYCHO.Axis2.range |
FLUO_pixelSize |
NX_FLOAT |
micron |
FLUO.pixelSize |
|
FLUO_dwellTime |
NX_FLOAT |
s |
FLUO.dwellTime |
|
FLUO_scanDim1 |
NX_FLOAT |
FLUO.scanDim_1 |
||
FLUO_scanDim2 |
NX_FLOAT |
FLUO.scanDim_2 |
||
FLUO_scanRange1 |
NX_FLOAT |
micron |
FLUO.scanRange_1 |
|
FLUO_scanRange2 |
NX_FLOAT |
micron |
FLUO.scanRange_2 |
|
FLUO_scanAxis1 |
NX_CHAR |
FLUO.scanAxis_1 |
||
FLUO_scanAxis2 |
NX_CHAR |
FLUO.scanAxis_2 |
||
FLUO_i0 |
Incident intensity |
NX_FLOAT |
FLUO.i0 |
|
FLUO_it |
Transmitted intensity |
NX_FLOAT |
FLUO.it |
|
Source_current_start |
Machine current |
NX_FLOAT64 |
mA |
FLUO.measurement.current_start |
InstrumentSource_current_end |
Machine current |
NX_FLOAT64 |
mA |
FLUO.measurement.current_end |
TOMO_i0_start |
Incident flux |
NX_FLOAT64 |
photons/s |
FLUO.measurement.i0_start |
TOMO_it_start |
Transmitted flux |
NX_FLOAT64 |
photons/s |
FLUO.measurement.it_start |
TOMO_i0_end |
Incident flux |
NX_FLOAT64 |
photons/s |
FLUO.measurement.i0_end |
TOMO_it_end |
Transmitted flux |
NX_FLOAT64 |
photons/s |
FLUO.measurement.it_end |
TOMO_experiment_type |
Type of experiment conducted |
NX_CHAR |
TOMO.experiment_type |
|
TOMO_ftomo_par |
Parameters for Fourier-tomography |
NX_CHAR |
TOMO.ftomo_par |
|
TOMO_xshutter_time |
Shutter closing time for the detector |
NX_FLOAT |
ms |
TOMO.xshutter_time |
TOMO_images_per_step |
Number of images captured per step |
NX_FLOAT |
TOMO.images_per_step |
|
TOMO_interlaced |
Enable interlaced scanning |
NX_FLOAT |
TOMO.interlaced |
|
TOMO_nested |
Enable nested scanning for topotomo |
NX_FLOAT |
TOMO.nested |
|
TOMO_save_separate_dark_image |
Save separate dark field images |
NX_FLOAT |
TOMO.save_separate_dark_image |
|
TOMO_auto_update_ref |
Automatically update references if set |
NX_FLOAT |
TOMO.auto_update_ref |
|
TOMO_images_at_end_as_quali |
Use images at end of scan for quality check |
NX_FLOAT |
TOMO.images_at_end_as_quali |
|
TOMO_live_correction |
Enable live correction of dark fields |
NX_FLOAT |
TOMO.live_correction |
|
TOMO_mono_tune_on_ref |
Tune monochromator before capturing flat images |
NX_FLOAT |
TOMO.mono_tune_on_ref |
|
TOMO_no_accel_corr |
Disable acceleration correction |
NX_FLOAT |
TOMO.no_accel_corr |
|
TOMO_open_slits_on_quali |
Open slits for quality check images |
NX_FLOAT |
TOMO.open_slits_on_quali |
|
TOMO_optics_eye_piece |
Magnification factor from optics |
NX_FLOAT |
TOMO.optics_eye_piece |
|
TOMO_readout_time |
Readout time of the camera |
NX_FLOAT |
s |
TOMO.readout_time |
TOMO_flat_power |
Power of the motor for capturing flat images |
NX_FLOAT |
TOMO.flat_power |
|
TOMO_rounding_correction |
Apply rounding corrections to projections |
NX_FLOAT |
TOMO.rounding_correction |
|
TOMO_safe_time |
Extra time to ensure safe readout |
NX_FLOAT |
s |
TOMO.safe_time |
TOMO_shift_turns |
Number of rotation turns to shift |
NX_FLOAT |
TOMO.shift_turns |
|
TOMO_speed_corr_factor |
Correction factor for rotation speed |
NX_FLOAT |
TOMO.speed_corr_factor |
|
TOMO_mono_tune_on_start |
Tune monochromator before scan starts |
NX_FLOAT |
TOMO.mono_tune_on_start |
|
TOMO_soft_version |
Software version, hostname, and path |
NX_CHAR |
TOMO.soft_version |
|
TOMO_vacuum_value |
Vacuum measurement values |
NX_FLOAT |
TOMO.vacuum_value |
|
TOMO_vacuum_name |
Vacuum measurement names |
NX_CHAR |
TOMO.vacuum_name |
|
TOMO_sx0 |
Focus position on X-axis |
NX_FLOAT |
mm |
TOMO.sx0 |
TOMO_camera_time |
Integration time of the camera |
NX_FLOAT |
s |
TOMO.camera_time |
TOMO_i0 |
Incident beam intensity |
NX_FLOAT |
TOMO.i0 |
|
TOMO_it |
Transmitted beam intensity |
NX_FLOAT |
TOMO.it |
|
TOMO_interlaced_roundtrip |
Interlaced scanning: same or opposite directions |
NX_FLOAT |
TOMO.interlaced_roundtrip |
|
TOMO_scanning_mode |
Mode of scanning |
NX_CHAR |
TOMO.scanning_mode |
|
TOMO_x_pixel_n |
Number of pixels in the x-direction |
NX_FLOAT |
TOMO.x_pixel_n |
|
TOMO_y_pixel_n |
Number of pixels in the y-direction |
NX_FLOAT |
TOMO.y_pixel_n |
|
TOMO_surface_dose |
Radiation dose at the surface |
NX_FLOAT |
Gy/s |
TOMO.surface_dose |
TOMO_voi_dose |
Radiation dose within the volume of interest (VOI) |
NX_FLOAT |
Gy/s |
TOMO.voi_dose |
TOMO_total_voi_dose |
Total accumulated dose within the volume of interest (VOI) |
NX_FLOAT |
kGy |
TOMO.total_voi_dose |
TOMO_reference_description |
Approach used to generate reference frames for flat field subtraction |
NX_CHAR |
TOMO.reference_description |
|
TOMO_subframe_nb |
Number of subframes |
NX_FLOAT |
TOMO.subframe_nb |
|
TOMO_idNames |
Insertion device for ID beamlines |
NX_CHAR |
TOMO.idNames |
|
TOMO_scanRadix |
Common prefix for scan datasets, useful for locating original radiographs |
NX_CHAR |
TOMO.scanRadix |
|
TOMO_propagationDistance |
Distance between the sample and detector |
NX_FLOAT |
mm |
TOMO.propagationDistance |
TOMO_xStages |
Number of scans in x-direction; allows 3D mosaic scans |
NX_FLOAT |
TOMO.xStages |
|
TOMO_yStages |
Number of scans in y-direction; allows 3D mosaic scans |
NX_FLOAT |
TOMO.yStages |
|
TOMO_zStages |
Number of scans in z-direction; allows 3D mosaic scans |
NX_FLOAT |
TOMO.zStages |
|
TOMO_min32to16bits |
Min value for scaling 32-bit float to 16-bit unsigned integer |
NX_FLOAT |
TOMO.min32to16bits |
|
TOMO_max32to16bits |
Max value for scaling 32-bit float to 16-bit unsigned integer |
NX_FLOAT |
TOMO.max32to16bits |
|
TOMO_jp2CompressRatio |
JPEG2000 compression ratio (default ~10x) |
NX_FLOAT |
TOMO.jp2CompressRatio |
|
TOMOAcquisition_technique |
Technique used for hierarchical phase-contrast tomography |
NX_CHAR |
TOMO.acquisition.technique |
|
TOMOAcquisition_proj_n |
Number of projections images |
NX_FLOAT |
TOMO.acquisition.proj_n |
|
TOMOAcquisition_flat_n |
Number of flat field images |
NX_FLOAT |
TOMO.acquisition.flat_n |
|
TOMOAcquisition_dark_n |
Number of dark field images |
NX_FLOAT |
TOMO.acquisition.dark_n |
|
TOMOAcquisition_flat_on |
Interval for capturing flat field images |
NX_FLOAT |
TOMO.acquisition.flat_on |
|
TOMOAcquisition_y_step |
Translation step size in the Y-axis for flat images |
NX_FLOAT |
mm |
TOMO.acquisition.y_step |
TOMOAcquisition_z_step |
Translation step size in the Z-axis for flat images |
NX_FLOAT |
mm |
TOMO.acquisition.z_step |
TOMOAcquisition_start_angle |
Start angle of the tomographic acquisition |
NX_FLOAT |
deg |
TOMO.acquisition.start_angle |
TOMOAcquisition_exposure_time |
Exposure time per projection |
NX_FLOAT |
s |
TOMO.acquisition.exposure_time |
TOMOAcquisition_sample_detector_distance |
Distance between sample and detector |
NX_FLOAT |
mm |
TOMO.acquisition.sample_detector_distance |
TOMOAcquisition_source_sample_distance |
Distance between source and sample |
NX_FLOAT |
mm |
TOMO.acquisition.source_sample_distance |
TOMOAcquisition_energy |
Beam energy |
NX_FLOAT |
keV |
TOMO.acquisition.energy |
TOMOAcquisition_half_acquisition |
Half-acquisition mode enabled |
NX_BOOLEAN |
TOMO.acquisition.half_acquisition |
|
TOMOAcquisition_type |
Acquisition type (e.g., half, full, or quarter acquisition) |
NX_CHAR |
TOMO.acquisition.type |
|
TOMOAcquisition_camera_pixel_size |
Pixel size of the camera hardware |
NX_FLOAT |
micron |
TOMO.acquisition.camera_pixel_size |
TOMOAcquisition_sample_pixel_size |
Pixel size in the sample space after all magnifications |
NX_FLOAT |
micron |
TOMO.acquisition.sample_pixel_size |
TOMOAcquisition_optic_magnified_pixel_size |
Pixel size in the sample space after magnification of the optics |
NX_FLOAT |
micron |
TOMO.acquisition.optic_magnified_pixel_size |
TOMOAcquisition_magnification |
Magnification factor of the optics |
NX_FLOAT |
TOMO.acquisition.magnification |
|
TOMOAcquisition_beam_magnification |
Magnification factor from the beam divergence |
NX_FLOAT |
TOMO.acquisition.beam_magnification |
|
TOMOAcquisition_read_srcur |
Enable real-time beam intensity measurement |
NX_BOOLEAN |
TOMO.acquisition.read_srcur |
|
TOMOAcquisition_srcur_start |
Beam intensity before scan |
NX_FLOAT |
mA |
TOMO.acquisition.srcur_start |
TOMOAcquisition_srcur_stop |
Beam intensity after scan |
NX_FLOAT |
mA |
TOMO.acquisition.srcur_stop |
TOMOAcquisition_scan_range |
Rotation range for tomography |
NX_FLOAT |
deg |
TOMO.acquisition.scan_range |
TOMOAcquisition_scan_type |
Type of scan used for the projection scan (e.g. INTERLACED, STEP, CONTINUOUS) |
NX_CHAR |
TOMO.acquisition.scan_type |
|
TOMOAcquisition_acc_exposure_time |
Accumulated exposure time per frame |
NX_FLOAT |
s |
TOMO.acquisition.acc_exposure_time |
TOMOAcquisition_acc_frames_count |
Number of frames in accumulation mode |
NX_FLOAT |
TOMO.acquisition.acc_frames_count |
|
TOMOAcquisition_accel_disp |
Acceleration displacement for the rotation stage |
NX_FLOAT |
mm |
TOMO.acquisition.accel_disp |
TOMOAcquisition_beam_check |
Suspend scan if no beam is detected |
NX_BOOLEAN |
TOMO.acquisition.beam_check |
|
TOMOAcquisition_camera_x_mot |
Motor for moving the camera along the beam axis |
NX_CHAR |
TOMO.acquisition.camera_x_mot |
|
TOMOAcquisition_camera_acq_mode |
Acquisition mode of the camera |
NX_CHAR |
TOMO.acquisition.camera_acq_mode |
|
TOMOAcquisition_camera_flip_horz |
Horizontal flip of the camera (left-right) |
NX_BOOLEAN |
TOMO.acquisition.camera_flip_horz |
|
TOMOAcquisition_camera_flip_vert |
Vertical flip of the camera (up-down) |
NX_BOOLEAN |
TOMO.acquisition.camera_flip_vert |
|
TOMOAcquisition_latency_time |
Extra readout time for the camera |
NX_FLOAT |
s |
TOMO.acquisition.latency_time |
TOMOAcquisition_no_images_at_end |
Capture of images at the end of scan disabled |
NX_BOOLEAN |
TOMO.acquisition.no_images_at_end |
|
TOMOAcquisition_no_flat_at_end |
Capture of flat images at the end of scan disabled |
NX_BOOLEAN |
TOMO.acquisition.no_flat_at_end |
|
TOMOAcquisition_optic_name |
Name of optic used |
NX_CHAR |
TOMO.acquisition.optic_name |
|
TOMOAcquisition_optic_type |
Type of optic used |
NX_CHAR |
TOMO.acquisition.optic_type |
|
TOMOAcquisition_scintillator |
Name of the scintillator used |
NX_CHAR |
TOMO.acquisition.scintillator |
|
TOMOAcquisition_duration |
Time it took for the acquisition sequence to run |
NX_FLOAT |
s |
TOMO.acquisition.duration |
TOMOAcquisition_comment |
Additional comments |
NX_CHAR |
TOMO.acquisition.comment |
|
TOMOAcquisitionZseries_z_mot |
Motor mnemonic for Z-axis |
NX_CHAR |
TOMO.acquisition.zseries.z_mot |
|
TOMOAcquisitionZseries_z_start |
Initial position of the motor on the Z-axis (first stage) |
NX_FLOAT |
mm |
TOMO.acquisition.zseries.z_start |
TOMOAcquisitionZseries_z_delta |
Incremental value for the Z-axis stage |
NX_FLOAT |
mm |
TOMO.acquisition.zseries.z_delta |
TOMOAcquisitionZseries_z_n_steps |
Number of steps for the Z-axis stage |
NX_FLOAT |
TOMO.acquisition.zseries.z_n_steps |
|
TOMOAcquisitionZseries_duration |
Time it took for the acquisition z-series sequence to run |
NX_FLOAT |
s |
TOMO.acquisition.zseries.duration |
TOMOReconstruction_angle_offset |
Angle offset for the reconstruction in degrees |
NX_FLOAT |
degree |
TOMO.reconstruction.angle_offset |
TOMOReconstruction_angles_file |
File path for angles used in reconstruction |
NX_CHAR |
TOMO.reconstruction.angles_file |
|
TOMOReconstruction_axis_correction_file |
File path for axis correction data |
NX_CHAR |
TOMO.reconstruction.axis_correction_file |
|
TOMOReconstruction_centered_axis |
Whether the reconstruction is centered on the axis |
NX_BOOLEAN |
TOMO.reconstruction.centered_axis |
|
TOMOReconstruction_clip_outer_circle |
Whether to clip the outer circle of the reconstruction |
NX_BOOLEAN |
TOMO.reconstruction.clip_outer_circle |
|
TOMOReconstruction_cor_options |
Options for center of rotation correction |
NX_CHAR |
TOMO.reconstruction.cor_options |
|
TOMOReconstruction_enable_halftomo |
Enable half-tomography mode |
NX_BOOLEAN |
TOMO.reconstruction.enable_halftomo |
|
TOMOReconstruction_end_x |
End X coordinate (in pixels) for reconstruction |
NX_INT |
TOMO.reconstruction.end_x |
|
TOMOReconstruction_end_y |
End Y coordinate (in pixels) for reconstruction |
NX_INT |
TOMO.reconstruction.end_y |
|
TOMOReconstruction_end_z |
End Z coordinate (in pixels) for reconstruction |
NX_INT |
TOMO.reconstruction.end_z |
|
TOMOReconstruction_fbp_filter_cutoff |
Cutoff frequency for the FBP filter |
NX_FLOAT |
TOMO.reconstruction.fbp_filter_cutoff |
|
TOMOReconstruction_fbp_filter_type |
Type of FBP filter used |
NX_CHAR |
TOMO.reconstruction.fbp_filter_type |
|
TOMOReconstruction_method |
Reconstruction method used (e.g., FBP, SIRT) |
NX_CHAR |
TOMO.reconstruction.method |
|
TOMOReconstruction_optim_algorithm |
Optimization algorithm used for reconstruction |
NX_CHAR |
TOMO.reconstruction.optim_algorithm |
|
TOMOReconstruction_padding_type |
Padding type for reconstruction |
NX_CHAR |
TOMO.reconstruction.padding_type |
|
TOMOReconstruction_preconditioning_filter |
Preconditioning filter applied to the reconstruction |
NX_CHAR |
TOMO.reconstruction.preconditioning_filter |
|
TOMOReconstruction_rotation_axis_position |
Position of the rotation axis in pixels |
NX_FLOAT |
TOMO.reconstruction.rotation_axis_position |
|
TOMOReconstruction_start_x |
Start X coordinate (in pixels) for reconstruction |
NX_INT |
TOMO.reconstruction.start_x |
|
TOMOReconstruction_start_y |
Start Y coordinate (in pixels) for reconstruction |
NX_INT |
TOMO.reconstruction.start_y |
|
TOMOReconstruction_start_z |
Start Z coordinate (in pixels) for reconstruction |
NX_INT |
TOMO.reconstruction.start_z |
|
TOMOReconstruction_translation_movements_file |
File path for translation movements data |
NX_CHAR |
TOMO.reconstruction.translation_movements_file |
|
TOMOReconstruction_weight_tv |
Total variation weight for reconstruction |
NX_FLOAT |
TOMO.reconstruction.weight_tv |
|
TOMOReconstruction_voxel_size_x |
Voxel size in X direction |
NX_FLOAT |
micron |
TOMO.reconstruction.voxel_size_x |
TOMOReconstruction_voxel_size_y |
Voxel size in Y direction |
NX_FLOAT |
micron |
TOMO.reconstruction.voxel_size_y |
TOMOReconstruction_voxel_size_z |
Voxel size in Z direction |
NX_FLOAT |
micron |
TOMO.reconstruction.voxel_size_z |
TOMOReconstructionPhase_ctf_advanced_params |
Advanced parameters for CTF phase retrieval |
NX_CHAR |
TOMO.reconstruction.phase.ctf_advanced_params |
|
TOMOReconstructionPhase_ctf_geometry |
CTF phase retrieval geometry |
NX_CHAR |
TOMO.reconstruction.phase.ctf_geometry |
|
TOMOReconstructionPhase_delta_beta |
Delta-beta ratio for phase retrieval |
NX_FLOAT |
TOMO.reconstruction.phase.delta_beta |
|
TOMOReconstructionPhase_detector_sample_distance |
Detector-sample distance for phase retrieval |
NX_FLOAT |
mm |
TOMO.reconstruction.phase.detector_sample_distance |
TOMOReconstructionPhase_method |
Phase retrieval method used |
NX_CHAR |
TOMO.reconstruction.phase.method |
|
TOMOReconstructionPhase_padding_type |
Padding type for phase retrieval |
NX_CHAR |
TOMO.reconstruction.phase.padding_type |
|
TOMOReconstructionPhase_unsharp_coeff |
Unsharp coefficient for phase retrieval |
NX_FLOAT |
TOMO.reconstruction.phase.unsharp_coeff |
|
TOMOReconstructionPhase_unsharp_method |
Unsharp method used for phase retrieval |
NX_CHAR |
TOMO.reconstruction.phase.unsharp_method |
|
TOMOReconstructionPhase_unsharp_sigma |
Unsharp sigma for phase retrieval |
NX_FLOAT |
TOMO.reconstruction.phase.unsharp_sigma |
|
TOMOReconstruction_nb_voxel_x |
Reconstructed volume length in pixels (x-direction) |
NX_FLOAT |
TOMO.reconstruction.phase.nb_voxel_x |
|
TOMOReconstruction_nb_voxel_y |
Reconstructed volume length in pixels (y-direction) |
NX_FLOAT |
TOMO.reconstruction.phase.nb_voxel_y |
|
TOMOReconstruction_nb_voxel_z |
Reconstructed volume length in pixels (z-direction) |
NX_FLOAT |
TOMO.reconstruction.phase.nb_voxel_z |
|
MRT_mscType |
Multislit Type |
NX_CHAR |
MRT.mscType |
|
MRT_doseRate |
Dose Rate |
NX_CHAR |
Gy/s/mA |
MRT.doseRate |
MRT_ctcMot |
C-to-C Motor |
NX_CHAR |
MRT.ctcMot |
|
MRT_ctcSpacing |
C-to-C Spacing |
NX_CHAR |
micron |
MRT.ctcSpacing |
MRT_ctcN |
Number of Irradiations |
NX_CHAR |
MRT.ctcN |
|
MRT_crossMot |
Crossfiring Motor |
NX_CHAR |
MRT.crossMot |
|
MRT_crossAngle |
Crossfiring Angle |
NX_CHAR |
deg |
MRT.crossAngle |
MRT_crossN |
Number of Crossfiring |
NX_CHAR |
MRT.crossN |
|
MRT_intlcdMot |
Interlaced Motor |
NX_CHAR |
MRT.intlcdMot |
|
MRT_intlcdOff |
Interlaced Offset |
NX_CHAR |
micron |
MRT.intlcdOff |
MRT_expoStart |
Z Start Position |
NX_CHAR |
mm |
MRT.expoStart |
MRT_expoStop |
Z Stop Position |
NX_CHAR |
mm |
MRT.expoStop |
MRT_expoSpeed |
Z Last Speed |
NX_CHAR |
mm/s |
MRT.expoSpeed |
MRT_IC01 |
Counts on ION chamber 0-1 |
NX_CHAR |
MRT.IC01 |
|
MRT_IC02 |
Counts on ION chamber 0-2 |
NX_CHAR |
MRT.IC02 |
|
MRT_IC0MU1 |
Counts on ION MUSST chamber 0-1 |
NX_CHAR |
MRT.IC0MU1 |
|
MRT_IC0MU2 |
Counts on ION MUSST chamber 0-2 |
NX_CHAR |
MRT.IC0MU2 |
|
MRT_IONCH1 |
Counts on ION chamber 1 |
NX_CHAR |
MRT.IONCH1 |
|
MRT_IONCH2 |
Counts on ION chamber 2 |
NX_CHAR |
MRT.IONCH2 |
|
MRT_dose |
Dose Planned |
NX_CHAR |
Gy |
MRT.dose |
MRT_beamHeight |
Beam Vertical Width |
NX_CHAR |
microns |
MRT.beamHeight |
MRT_beamSize |
Microbeam Width |
NX_CHAR |
microns |
MRT.beamSize |
HOLO_N |
Number of planes for holography |
NX_FLOAT |
HOLO.n |
|
HOLO_holoSampleDetectorDistances |
Sample/detector distances for all planes used |
NX_CHAR |
HOLO.sampleDetectorDistances |
|
HOLO_holoSourceSampleDistances |
Source/sample distances for all planes used |
NX_CHAR |
HOLO.sourceSampleDistances |
|
HOLO_im01_num_end |
Index of last sample image in plane 1 |
NX_FLOAT |
HOLO.im01NumEnd |
|
HOLO_im01_num_start |
Index of first sample image in plane 1 |
NX_FLOAT |
HOLO.im01NumStart |
|
HOLO_im02_num_end |
Index of last sample image in plane 2 |
NX_FLOAT |
HOLO.im02NumEnd |
|
HOLO_im02_num_start |
Index of first sample image in plane 2 |
NX_FLOAT |
HOLO.im02NumStart |
|
HOLO_im03_num_end |
Index of last sample image in plane 3 |
NX_FLOAT |
HOLO.im03NumEnd |
|
HOLO_im03_num_start |
Index of first sample image in plane 3 |
NX_FLOAT |
HOLO.im03NumStart |
|
HOLO_im04_num_end |
Index of last sample image in plane 4 |
NX_FLOAT |
HOLO.im04NumEnd |
|
HOLO_im04_num_start |
Index of first sample image in plane 4 |
NX_FLOAT |
HOLO.im04NumStart |
|
HOLO_ref01_num_end |
Index of last reference image in plane 1 |
NX_FLOAT |
HOLO.ref01NumEnd |
|
HOLO_ref02_num_end |
Index of last reference image in plane 2 |
NX_FLOAT |
HOLO.ref02NumEnd |
|
HOLO_ref02_num_start |
Index of first reference image in plane 2 |
NX_FLOAT |
HOLO.ref02NumStart |
|
HOLO_ref03_num_end |
Index of last reference image in plane 3 |
NX_FLOAT |
HOLO.ref03NumEnd |
|
HOLO_ref03_num_start |
Index of first reference image in plane 3 |
NX_FLOAT |
HOLO.ref03NumStart |
|
HOLO_ref04_num_end |
Index of last reference image in plane 4 |
NX_FLOAT |
HOLO.ref04NumEnd |
|
HOLO_ref04_num_start |
Index of first reference image in plane 4 |
NX_FLOAT |
HOLO.ref04NumStart |
|
HOLO_dark_num_start |
Index of first dark image |
NX_FLOAT |
HOLO.darkNumStart |
|
HOLO_dark_num_end |
Index of last dark image |
NX_FLOAT |
HOLO.darkNumEnd |
|
HOLO_pixelSize |
Pixel size of first distance in micron |
NX_FLOAT |
s |
HOLO.pixelSize |
SSXJet_speed |
Jet’s speed |
NX_CHAR |
SSX.jet.speed |
|
SSXJet_size |
Jet’s size |
NX_CHAR |
SSX.jet.size |
|
SSXChip_horizontal_spacing |
NX_CHAR |
SSX.chip.horizontal_spacing |
||
SSXChip_vertical_spacing |
NX_CHAR |
SSX.chip.vertical_spacing |
||
SSXChip_row_number |
NX_CHAR |
SSX.chip.row_number |
||
SSXChip_column_number |
NX_CHAR |
SSX.chip.column_number |
||
SSXChip_model |
NX_CHAR |
SSX.chip.model |
||
xrf_definition |
Technique used to collect this dataset |
NX_CHAR |
WAXS.definition |
|
HTXRPD_energy |
Beam energy |
NX_FLOAT |
keV |
HTXRPD.energy |
HTXRPD_exposureTime |
Requested exposure time per diffraction pattern |
NX_FLOAT |
s |
HTXRPD.exposureTime |
HTXRPD_distance |
The perpendicular sample-detector distance |
NX_FLOAT |
mm |
HTXRPD.distance |
HTXRPD_sampleVibration |
The vibration speed of the powder sample (0-100 %) |
NX_FLOAT |
HTXRPD.sampleVibration |
|
SXDM_beamSizeVertical |
Vertical beam size on the sample in microns |
NX_FLOAT |
micron |
SXDM.beamSizeVertical |
SXDM_beamSizeHorizontal |
Horizontal beam size on the sample in microns |
NX_FLOAT |
micron |
SXDM.beamSizeHorizontal |
BCDI_beamSizeVertical |
Vertical beam size on the sample in microns |
NX_FLOAT |
micron |
BCDI.beamSizeVertical |
BCDI_beamSizeHorizontal |
Horizontal beam size on the sample in microns |
NX_FLOAT |
micron |
BCDI.beamSizeHorizontal |
Sample_name |
Name of the sample |
NX_CHAR |
sample.name |
|
Sample_description |
Description of the sample |
NX_CHAR |
sample.description |
|
Sample_distance |
Translation of the sample along the Z-direction of the laboratory coordinate system |
NX_CHAR |
sample.distance |
|
Sample_support |
Name of the support used to collect the sample. It can be a chip, plate, jet, etc… |
NX_CHAR |
sample.support |
|
Sample_situation |
The atmosphere will be one of the components, which is where its details will be stored; the relevant components will be indicated by the entry in the sample_component member. |
NX_CHAR |
sample.situation |
|
Sample_ub_matrix |
UB matrix of single crystal sample using Busing-Levy convention: W. R. Busing and H. A. Levy (1967). Acta Cryst. 22, 457-464. This is the multiplication of the orientation_matrix, given above, with the BB matrix which can be derived from the lattice constants. |
NX_CHAR |
sample.ub_matrix |
|
Sample_temperature_env |
Additional sample temperature environment information |
NX_CHAR |
sample.temperature_env |
|
Sample_chemical_formula |
Chemical formula of the sample |
NX_CHAR |
sample.chemical_formula |
|
Sample_notes |
NX_CHAR |
sample.notes.notes |
||
SamplePositioners_name |
NX_CHAR |
sample.positioners.name |
||
SamplePositioners_value |
NX_CHAR |
sample.positioners.value |
||
SampleProtein_acronym |
Acronym of the protein |
NX_CHAR |
sample.protein.acronym |
|
SampleProtein_name |
Acronym of the protein |
NX_CHAR |
sample.protein.name |
|
SampleChanger_position |
Sample changer position |
NX_CHAR |
sample.changer.position |
|
SamplePatient_institute |
Institute of origin of the patient |
NX_CHAR |
sample.patient.institute |
|
SamplePatient_number |
Number of the patient |
NX_CHAR |
sample.patient.number |
|
SamplePatient_age |
Age of the patient |
NX_CHAR |
years |
sample.patient.age |
SamplePatient_sex |
Sex of the patient |
NX_CHAR |
sample.patient.sex |
|
SamplePatient_weight |
Weight of the patient |
NX_CHAR |
kg |
sample.patient.weight |
SamplePatient_size |
Size of the patient |
NX_CHAR |
cm |
sample.patient.size |
SamplePatient_info |
Information about the patient |
NX_CHAR |
sample.patient.info |
|
SamplePatient_organ_name |
Name of the organ |
NX_CHAR |
sample.patient.organ_name |
|
SamplePatient_organ_description |
Name of the organ |
NX_CHAR |
sample.patient.organ_description |
|
SampleEnvironment_name |
Apparatus identification code/model number; e.g. OC100 011 |
NX_CHAR |
sample.environment.name |
|
SampleEnvironment_type |
Type of apparatus. This could be the SE codes in scheduling database; e.g. OC/100 |
NX_CHAR |
sample.environment.type |
|
SampleEnvironment_description |
Description of the apparatus; e.g. 100mm bore orange cryostat with Roots pump |
NX_CHAR |
sample.environment.description |
|
SampleEnvironmentSensors_name |
NX_CHAR |
sample.environment.sensors.name |
||
SampleEnvironmentSensors_value |
NX_CHAR |
sample.environment.sensors.value |
||
SampleTrackingShipment_id |
Identifier of the shipment |
NX_CHAR |
sample.tracking.shipment.id |
|
SampleTrackingShipment_name |
Name of the shipment |
NX_CHAR |
sample.tracking.shipment.name |
|
SampleTrackingParcel_storage_condition |
Storage conditions of the parcel. Example: -80 degrees |
NX_CHAR |
sample.tracking.parcel.id |
|
SampleTrackingContainer_type |
Type of container. Example: unipuck, spinepuck, etc… |
NX_CHAR |
sample.tracking.container.type |
|
SampleTrackingContainer_capaticy |
Total capacity of the container |
NX_CHAR |
sample.tracking.container.capacity |
|
SampleTrackingContainer_position |
Position of the sample within the container |
NX_CHAR |
sample.tracking.container.position |
|
SampleTrackingContainer_id |
Identifier of the container |
NX_CHAR |
sample.tracking.container.id |
|
SampleLocalisation_name |
Name of the localisation |
NX_CHAR |
sample.localisation.name |
|
SampleLocalisation_country |
Country |
NX_CHAR |
sample.localisation.country |
|
SampleLocalisation_continental_region |
Continental region |
NX_CHAR |
sample.localisation.continental_region |
|
SamplePaleo_scientific_domain |
Scientific domain |
NX_CHAR |
sample.paleo.scientific_domain |
|
SamplePaleo_repository_institution |
Repository institution |
NX_CHAR |
sample.paleo.repository_institution |
|
SamplePaleo_collection_number |
Collection number in the repository institution |
NX_CHAR |
sample.paleo.collection_number |
|
SamplePaleoGeologicalTime_formation |
Formation |
NX_CHAR |
sample.paleo.geological_time.formation |
|
SamplePaleoGeologicalTime_era |
Era |
NX_CHAR |
sample.paleo.geological_time.era |
|
SamplePaleoGeologicalTime_period |
Period |
NX_CHAR |
sample.paleo.geological_time.period |
|
SamplePaleoGeologicalTime_epoch |
Epoch |
NX_CHAR |
sample.paleo.geological_time.epoch |
|
SamplePaleoClassification_species |
Species |
NX_CHAR |
sample.paleo.classification.species |
|
SamplePaleoClassification_material_type |
Material Type |
NX_CHAR |
sample.paleo.classification.material_type |
|
SamplePaleoClassification_clade1 |
Clade 1 |
NX_CHAR |
sample.paleo.classification.clade1 |
|
SamplePaleoClassification_clade2 |
Clade 2 |
NX_CHAR |
sample.paleo.classification.clade2 |
|
SamplePaleoClassification_clade3 |
Clade 3 |
NX_CHAR |
sample.paleo.classification.clade3 |
|
SamplePaleoClassification_clade4 |
Clade 4 |
NX_CHAR |
sample.paleo.classification.clade4 |
|
SamplePaleoClassification_clade5 |
Clade 5 |
NX_CHAR |
sample.paleo.classification.clade5 |
|
SamplePaleoClassification_clade6 |
Clade 6 |
NX_CHAR |
sample.paleo.classification.clade6 |
|
Fresnel_zone_plate_outer_diameter |
NX_CHAR |
fresnel_zone_plate.outer_diameter |
||
Fresnel_zone_plate_outermost_zone_width |
NX_CHAR |
fresnel_zone_plate.outermost_zone_width |
||
Fresnel_zone_plate_central_stop_diameter |
NX_CHAR |
fresnel_zone_plate.central_stop_diameter |
||
Fresnel_zone_plate_fabrication |
how the zone plate was manufactured. Any of these values: etched | plated | zone doubled | other |
NX_CHAR |
fresnel_zone_plate.fabrication |
|
Fresnel_zone_plate_zone_height |
NX_CHAR |
fresnel_zone_plate.zone_height |
||
Fresnel_zone_plate_zone_material |
NX_CHAR |
fresnel_zone_plate.zone_material |
||
Fresnel_zone_plate_zone_support_material |
Material present between the zones. This is usually only present for the “zone doubled” fabrication process |
NX_CHAR |
fresnel_zone_plate.zone_support_material |
|
Fresnel_zone_plate_central_stop_material |
NX_CHAR |
fresnel_zone_plate.central_stop_material |
||
Fresnel_zone_plate_central_stop_thickness |
NX_CHAR |
fresnel_zone_plate.central_stop_thickness |
||
Fresnel_zone_plate_support_membrane_material |
NX_CHAR |
fresnel_zone_plate.support_membrane_material |
||
Fresnel_zone_plate_distance |
NX_CHAR |
fresnel_zone_plate.distance |
||
Fresnel_zone_plate_component_index |
NX_CHAR |
fresnel_zone_plate.component_index |
||
Aperture_description |
Declares which child group contains a path leading to a NXdata group. It is recommended (as of NIAC2014) to use this attribute to help define the path to the default dataset to be plotted. See https://www.nexusformat.org/2014_How_to_find_default_data.html for a summary of the discussion. |
NX_CHAR |
aperture.description |
|
Aperture_material |
Absorbing material of the aperture |
NX_CHAR |
aperture.material |
|
ApertureGeometry_vertical |
Optional description/label. Probably only present if we are an additional reference point for components rather than the location of a real component. |
NX_CHAR |
aperture.geometry.vertical |
|
ApertureGeometry_horizontal |
NX_CHAR |
aperture.geometry.horizontal |
||
ApertureGeometry_transformation |
NX_CHAR |
aperture.geometry.transformation |
||
ApertureGeometry_distance |
NX_CHAR |
aperture.geometry.distance |
||
ApertureGeometry_component_index |
Position of the component along the beam path. The sample is at 0, components upstream have negative component_index, components downstream have positive component_index. |
NX_CHAR |
aperture.geometry.component_index |
|
Mirror_type |
Any of these values: single: mirror with a single material as a reflecting surface, multi: mirror with stacked, multiple layers as a reflecting surface |
NX_CHAR |
mirror.type |
|
Mirror_description |
description of this mirror |
NX_CHAR |
mirror.description |
|
Mirror_interior_atmosphere |
Any of these values: vacuum | helium | argon |
NX_CHAR |
mirror.interior_atmosphere |
|
Mirror_substrate_material |
NX_CHAR |
mirror.substrate_material |
||
Mirror_coating_material |
NX_CHAR |
mirror.coating_material |
||
MirrorGeometry_vertical |
Optional description/label. Probably only present if we are an additional reference point for components rather than the location of a real component. |
NX_CHAR |
mirror.geometry.vertical |
|
MirrorGeometry_horizontal |
NX_CHAR |
mirror.geometry.horizontal |
||
MirrorGeometry_transformation |
NX_CHAR |
mirror.geometry.transformation |
||
MirrorGeometry_distance |
NX_CHAR |
mirror.geometry.distance |
||
MirrorGeometry_component_index |
Position of the component along the beam path. The sample is at 0, components upstream have negative component_index, components downstream have positive component_index. |
NX_CHAR |
mirror.geometry.component_index |
|
beamlineID |
ID of the beamline |
NX_CHAR |
instrument.name |
|
InstrumentVariables_name |
NX_CHAR |
instrument.variables.name |
||
InstrumentVariables_value |
NX_CHAR |
instrument.variables.value |
||
InstrumentPositioners_name |
NX_CHAR |
instrument.positioners.name |
||
InstrumentPositioners_value |
NX_CHAR |
instrument.positioners.value |
||
InstrumentBeam_incident_beam_divergence |
Beam crossfire in degrees parallel to the laboratory X axis |
NX_CHAR |
instrument.beam.incident_beam_divergence |
|
InstrumentBeam_horizontal_incident_beam_divergence |
Horizontal beam crossfire in degrees parallel to the laboratory X axis |
NX_CHAR |
instrument.beam.horizontal_incident_beam_divergence |
|
InstrumentBeam_vertical_incident_beam_divergence |
Vertical beam crossfire in degrees parallel to the laboratory X axis |
NX_CHAR |
instrument.beam.vertical_incident_beam_divergence |
|
InstrumentBeam_final_polarization |
Polarization vector on leaving beamline component using Stokes notation (see incident_polarization_stokes). |
NX_CHAR |
instrument.beam.final_polarization |
|
InstrumentMonochromator_name |
NX_CHAR |
instrument.monochromator.name |
||
InstrumentMonochromator_energy |
NX_CHAR |
instrument.monochromator.energy |
||
InstrumentMonochromator_wavelength |
NX_CHAR |
instrument.monochromator.wavelength |
||
InstrumentMonochromatorCrystal_usage |
NX_CHAR |
instrument.monochromator.crystal.usage |
||
InstrumentMonochromatorCrystal_d_spacing |
NX_CHAR |
instrument.monochromator.crystal.d_spacing |
||
InstrumentMonochromatorCrystal_type |
NX_CHAR |
instrument.monochromator.crystal.type |
||
InstrumentMonochromatorCrystal_reflection |
NX_CHAR |
instrument.monochromator.crystal.reflection |
||
InstrumentSource_mode |
NX_CHAR |
instrument.source.mode |
||
InstrumentSource_current |
NX_CHAR |
instrument.source.current |
||
InstrumentSource_distance |
Effective distance from sample Distance as seen by radiation from sample. This number should be negative to signify that it is upstream of the sample. |
NX_CHAR |
instrument.source.distance |
|
InstrumentSource_name |
Name of source |
NX_CHAR |
instrument.source.name |
|
InstrumentSource_type |
type of radiation source (pick one from the enumerated list and spell exactly). Spallation Neutron Source, Pulsed Reactor Neutron Source, Reactor Neutron Source, Synchrotron X-ray Source, Pulsed Muon Source, Rotating Anode X-ray,Fixed Tube X-ray,UV Laser,Free-Electron Laser,Optical Laser,Ion Source,UV Plasma Source |
NX_CHAR |
instrument.source.type |
|
InstrumentSource_probe |
type of radiation probe |
NX_CHAR |
instrument.source.probe |
|
InstrumentSource_emittance_x |
Source emittance (nm-rad) in X (horizontal) direction. |
NX_CHAR |
instrument.source.emittance_x |
|
InstrumentSource_emittance_y |
Source emittance (nm-rad) in Y (horizontal) direction. |
NX_CHAR |
instrument.source.emittance_y |
|
InstrumentLaser01_name |
https://manual.nexusformat.org/classes/base_classes/NXsource.html#nxsource-name-field |
NX_CHAR |
instrument.laser01.name |
|
InstrumentLaser01_type |
Type of source. https://manual.nexusformat.org/classes/base_classes/NXsource.html#nxsource-type-field |
NX_CHAR |
instrument.laser01.type |
|
InstrumentLaser01_probe |
Type of radiation. https://manual.nexusformat.org/classes/base_classes/NXsource.html#nxsource-probe-field |
NX_CHAR |
instrument.laser01.probe |
|
InstrumentLaser01_energy |
Energy emitted in a single pulse. https://manual.nexusformat.org/classes/base_classes/NXsource.html#nxsource-energy-field |
NX_FLOAT |
instrument.laser01.energy |
|
InstrumentLaser01_wavelength |
Wavelength emitted in a single pulse. |
NX_FLOAT |
m |
instrument.laser01.wavelength |
InstrumentLaser01_repetition_rate |
Pulse Repetition Frequency. |
NX_FLOAT |
instrument.laser01.repetition_rate |
|
InstrumentLaser01_pulse_width |
Time between the start and end of a single pulse. https://manual.nexusformat.org/classes/base_classes/NXsource.html#nxsource-pulse-width-field |
NX_FLOAT |
s |
instrument.laser01.pulse_width |
InstrumentLaser01_delay |
The time of the start of the laser pulse with respect to the start of the measurement (T=0) |
NX_FLOAT |
s |
instrument.laser01.delay |
InstrumentLaser02_name |
https://manual.nexusformat.org/classes/base_classes/NXsource.html#nxsource-name-field |
NX_CHAR |
instrument.laser02.name |
|
InstrumentLaser02_type |
Type of source. https://manual.nexusformat.org/classes/base_classes/NXsource.html#nxsource-type-field |
NX_CHAR |
instrument.laser02.type |
|
InstrumentLaser02_probe |
Type of radiation. https://manual.nexusformat.org/classes/base_classes/NXsource.html#nxsource-probe-field |
NX_CHAR |
instrument.laser02.probe |
|
InstrumentLaser02_energy |
Energy emitted in a single pulse. https://manual.nexusformat.org/classes/base_classes/NXsource.html#nxsource-energy-field |
NX_FLOAT |
J |
instrument.laser02.energy |
InstrumentLaser02_wavelength |
Wavelength emitted in a single pulse. |
NX_FLOAT |
m |
instrument.laser02.wavelength |
InstrumentLaser02_repetition_rate |
Pulse Repetition Frequency. |
NX_FLOAT |
instrument.laser02.repetition_rate |
|
InstrumentLaser02_pulse_width |
Time between the start and end of a single pulse. https://manual.nexusformat.org/classes/base_classes/NXsource.html#nxsource-pulse-width-field |
NX_FLOAT |
s |
instrument.laser02.pulse_width |
InstrumentLaser02_delay |
The time of the start of the laser pulse with respect to the start of the measurement (T=0) |
NX_FLOAT |
s |
instrument.laser02.delay |
InstrumentSlitPrimary_name |
NX_CHAR |
instrument.primary_slit.name |
||
InstrumentSlitPrimary_vertical_gap |
NX_CHAR |
instrument.primary_slit.vertical_gap |
||
InstrumentSlitPrimary_vertical_offset |
NX_CHAR |
instrument.primary_slit.vertical_offset |
||
InstrumentSlitPrimary_horizontal_gap |
NX_CHAR |
instrument.primary_slit.horizontal_gap |
||
InstrumentSlitPrimary_horizontal_offset |
NX_CHAR |
instrument.primary_slit.horizontal_offset |
||
InstrumentSlitPrimary_blade_up |
NX_CHAR |
instrument.primary_slit.blade_up |
||
InstrumentSlitPrimary_blade_down |
NX_CHAR |
instrument.primary_slit.blade_down |
||
InstrumentSlitPrimary_blade_front |
NX_CHAR |
instrument.primary_slit.blade_front |
||
InstrumentSlitPrimary_blade_back |
NX_CHAR |
instrument.primary_slit.blade_back |
||
InstrumentSlitSecondary_name |
NX_CHAR |
instrument.secondary_slit.name |
||
InstrumentSlitSecondary_vertical_gap |
NX_CHAR |
instrument.secondary_slit.vertical_gap |
||
InstrumentSlitSecondary_vertical_offset |
NX_CHAR |
instrument.secondary_slit.vertical_offset |
||
InstrumentSlitSecondary_horizontal_gap |
NX_CHAR |
instrument.secondary_slit.horizontal_gap |
||
InstrumentSlitSecondary_horizontal_offset |
NX_CHAR |
instrument.secondary_slit.horizontal_offset |
||
InstrumentSlitSecondary_blade_up |
NX_CHAR |
instrument.secondary_slit.blade_up |
||
InstrumentSlitSecondary_blade_down |
NX_CHAR |
instrument.secondary_slit.blade_down |
||
InstrumentSlitSecondary_blade_front |
NX_CHAR |
instrument.secondary_slit.blade_front |
||
InstrumentSlitSecondary_blade_back |
NX_CHAR |
instrument.secondary_slit.blade_back |
||
InstrumentSlits_name |
NX_CHAR |
instrument.slits.name |
||
InstrumentSlits_vertical_gap |
NX_CHAR |
instrument.slits.vertical_gap |
||
InstrumentSlits_vertical_offset |
NX_CHAR |
instrument.slits.vertical_offset |
||
InstrumentSlits_horizontal_gap |
NX_CHAR |
instrument.slits.horizontal_gap |
||
InstrumentSlits_horizontal_offset |
NX_CHAR |
instrument.slits.horizontal_offset |
||
InstrumentSlits_blade_up |
NX_CHAR |
instrument.slits.blade_up |
||
InstrumentSlits_blade_down |
NX_CHAR |
instrument.slits.blade_down |
||
InstrumentSlits_blade_front |
NX_CHAR |
instrument.slits.blade_front |
||
InstrumentSlits_blade_back |
NX_CHAR |
instrument.slits.blade_back |
||
InstrumentXraylens01_lens_geometry |
Geometry of the lens. Any of these values:paraboloid,spherical,elliptical,hyperbolical |
NX_CHAR |
instrument.xraylens01.lens_geometry |
|
InstrumentXraylens01_focus_type |
The type of focus of the lens. Any of these values:line,point |
NX_CHAR |
instrument.xraylens01.focus_type |
|
InstrumentXraylens01_lens_thickness |
Thickness of the lens |
NX_CHAR |
instrument.xraylens01.lens_thickness |
|
InstrumentXraylens01_lens_length |
Length of the lens |
NX_CHAR |
instrument.xraylens01.lens_length |
|
InstrumentXraylens01_curvature |
Radius of the curvature as measured in the middle of the lens |
NX_CHAR |
instrument.xraylens01.curvature |
|
InstrumentXraylens01_aperture |
Diameter of the lens |
NX_CHAR |
instrument.xraylens01.aperture |
|
InstrumentXraylens01_number_of_lenses |
Number of lenses that make up the compound lens |
NX_CHAR |
instrument.xraylens01.number_of_lenses |
|
InstrumentXraylens01_lens_material |
Material used to make the lens |
NX_CHAR |
instrument.xraylens01.lens_material |
|
InstrumentXraylens02_lens_geometry |
Geometry of the lens. Any of these values:paraboloid,spherical,elliptical,hyperbolical |
NX_CHAR |
instrument.xraylens02.lens_geometry |
|
InstrumentXraylens02_focus_type |
The type of focus of the lens. Any of these values:line,point |
NX_CHAR |
instrument.xraylens02.focus_type |
|
InstrumentXraylens02_lens_thickness |
Thickness of the lens |
NX_CHAR |
instrument.xraylens02.lens_thickness |
|
InstrumentXraylens02_lens_length |
Length of the lens |
NX_CHAR |
instrument.xraylens02.lens_length |
|
InstrumentXraylens02_curvature |
Radius of the curvature as measured in the middle of the lens |
NX_CHAR |
instrument.xraylens02.curvature |
|
InstrumentXraylens02_aperture |
Diameter of the lens |
NX_CHAR |
instrument.xraylens02.aperture |
|
InstrumentXraylens02_number_of_lenses |
Number of lenses that make up the compound lens |
NX_CHAR |
instrument.xraylens02.number_of_lenses |
|
InstrumentXraylens02_lens_material |
Material used to make the lens |
NX_CHAR |
instrument.xraylens02.lens_material |
|
InstrumentXraylens03_lens_geometry |
Geometry of the lens. Any of these values:paraboloid,spherical,elliptical,hyperbolical |
NX_CHAR |
instrument.xraylens03.lens_geometry |
|
InstrumentXraylens03_focus_type |
The type of focus of the lens. Any of these values:line,point |
NX_CHAR |
instrument.xraylens03.focus_type |
|
InstrumentXraylens03_lens_thickness |
Thickness of the lens |
NX_CHAR |
instrument.xraylens03.lens_thickness |
|
InstrumentXraylens03_lens_length |
Length of the lens |
NX_CHAR |
instrument.xraylens03.lens_length |
|
InstrumentXraylens03_curvature |
Radius of the curvature as measured in the middle of the lens |
NX_CHAR |
instrument.xraylens03.curvature |
|
InstrumentXraylens03_aperture |
Diameter of the lens |
NX_CHAR |
instrument.xraylens03.aperture |
|
InstrumentXraylens03_number_of_lenses |
Number of lenses that make up the compound lens |
NX_CHAR |
instrument.xraylens03.number_of_lenses |
|
InstrumentXraylens03_lens_material |
Material used to make the lens |
NX_CHAR |
instrument.xraylens03.lens_material |
|
InstrumentXraylens04_lens_geometry |
Geometry of the lens. Any of these values:paraboloid,spherical,elliptical,hyperbolical |
NX_CHAR |
instrument.xraylens04.lens_geometry |
|
InstrumentXraylens04_focus_type |
The type of focus of the lens. Any of these values:line,point |
NX_CHAR |
instrument.xraylens04.focus_type |
|
InstrumentXraylens04_lens_thickness |
Thickness of the lens |
NX_CHAR |
instrument.xraylens04.lens_thickness |
|
InstrumentXraylens04_lens_length |
Length of the lens |
NX_CHAR |
instrument.xraylens04.lens_length |
|
InstrumentXraylens04_curvature |
Radius of the curvature as measured in the middle of the lens |
NX_CHAR |
instrument.xraylens04.curvature |
|
InstrumentXraylens04_aperture |
Diameter of the lens |
NX_CHAR |
instrument.xraylens04.aperture |
|
InstrumentXraylens04_number_of_lenses |
Number of lenses that make up the compound lens |
NX_CHAR |
instrument.xraylens04.number_of_lenses |
|
InstrumentXraylens04_lens_material |
Material used to make the lens |
NX_CHAR |
instrument.xraylens04.lens_material |
|
InstrumentXraylens05_lens_geometry |
Geometry of the lens. Any of these values:paraboloid,spherical,elliptical,hyperbolical |
NX_CHAR |
instrument.xraylens05.lens_geometry |
|
InstrumentXraylens05_focus_type |
The type of focus of the lens. Any of these values:line,point |
NX_CHAR |
instrument.xraylens05.focus_type |
|
InstrumentXraylens05_lens_thickness |
Thickness of the lens |
NX_CHAR |
instrument.xraylens05.lens_thickness |
|
InstrumentXraylens05_lens_length |
Length of the lens |
NX_CHAR |
instrument.xraylens05.lens_length |
|
InstrumentXraylens05_curvature |
Radius of the curvature as measured in the middle of the lens |
NX_CHAR |
instrument.xraylens05.curvature |
|
InstrumentXraylens05_aperture |
Diameter of the lens |
NX_CHAR |
instrument.xraylens05.aperture |
|
InstrumentXraylens05_number_of_lenses |
Number of lenses that make up the compound lens |
NX_CHAR |
instrument.xraylens05.number_of_lenses |
|
InstrumentXraylens05_lens_material |
Material used to make the lens |
NX_CHAR |
instrument.xraylens05.lens_material |
|
InstrumentXraylens06_lens_geometry |
Geometry of the lens. Any of these values:paraboloid,spherical,elliptical,hyperbolical |
NX_CHAR |
instrument.xraylens06.lens_geometry |
|
InstrumentXraylens06_focus_type |
The type of focus of the lens. Any of these values:line,point |
NX_CHAR |
instrument.xraylens06.focus_type |
|
InstrumentXraylens06_lens_thickness |
Thickness of the lens |
NX_CHAR |
instrument.xraylens06.lens_thickness |
|
InstrumentXraylens06_lens_length |
Length of the lens |
NX_CHAR |
instrument.xraylens06.lens_length |
|
InstrumentXraylens06_curvature |
Radius of the curvature as measured in the middle of the lens |
NX_CHAR |
instrument.xraylens06.curvature |
|
InstrumentXraylens06_aperture |
Diameter of the lens |
NX_CHAR |
instrument.xraylens06.aperture |
|
InstrumentXraylens06_number_of_lenses |
Number of lenses that make up the compound lens |
NX_CHAR |
instrument.xraylens06.number_of_lenses |
|
InstrumentXraylens06_lens_material |
Material used to make the lens |
NX_CHAR |
instrument.xraylens06.lens_material |
|
InstrumentXraylens07_lens_geometry |
Geometry of the lens. Any of these values:paraboloid,spherical,elliptical,hyperbolical |
NX_CHAR |
instrument.xraylens07.lens_geometry |
|
InstrumentXraylens07_focus_type |
The type of focus of the lens. Any of these values:line,point |
NX_CHAR |
instrument.xraylens07.focus_type |
|
InstrumentXraylens07_lens_thickness |
Thickness of the lens |
NX_CHAR |
instrument.xraylens07.lens_thickness |
|
InstrumentXraylens07_lens_length |
Length of the lens |
NX_CHAR |
instrument.xraylens07.lens_length |
|
InstrumentXraylens07_curvature |
Radius of the curvature as measured in the middle of the lens |
NX_CHAR |
instrument.xraylens07.curvature |
|
InstrumentXraylens07_aperture |
Diameter of the lens |
NX_CHAR |
instrument.xraylens07.aperture |
|
InstrumentXraylens07_number_of_lenses |
Number of lenses that make up the compound lens |
NX_CHAR |
instrument.xraylens07.number_of_lenses |
|
InstrumentXraylens07_lens_material |
Material used to make the lens |
NX_CHAR |
instrument.xraylens07.lens_material |
|
InstrumentXraylens08_lens_geometry |
Geometry of the lens. Any of these values:paraboloid,spherical,elliptical,hyperbolical |
NX_CHAR |
instrument.xraylens08.lens_geometry |
|
InstrumentXraylens08_focus_type |
The type of focus of the lens. Any of these values:line,point |
NX_CHAR |
instrument.xraylens08.focus_type |
|
InstrumentXraylens08_lens_thickness |
Thickness of the lens |
NX_CHAR |
instrument.xraylens08.lens_thickness |
|
InstrumentXraylens08_lens_length |
Length of the lens |
NX_CHAR |
instrument.xraylens08.lens_length |
|
InstrumentXraylens08_curvature |
Radius of the curvature as measured in the middle of the lens |
NX_CHAR |
instrument.xraylens08.curvature |
|
InstrumentXraylens08_aperture |
Diameter of the lens |
NX_CHAR |
instrument.xraylens08.aperture |
|
InstrumentXraylens08_number_of_lenses |
Number of lenses that make up the compound lens |
NX_CHAR |
instrument.xraylens08.number_of_lenses |
|
InstrumentXraylens08_lens_material |
Material used to make the lens |
NX_CHAR |
instrument.xraylens08.lens_material |
|
InstrumentXraylens09_lens_geometry |
Geometry of the lens. Any of these values:paraboloid,spherical,elliptical,hyperbolical |
NX_CHAR |
instrument.xraylens09.lens_geometry |
|
InstrumentXraylens09_focus_type |
The type of focus of the lens. Any of these values:line,point |
NX_CHAR |
instrument.xraylens09.focus_type |
|
InstrumentXraylens09_lens_thickness |
Thickness of the lens |
NX_CHAR |
instrument.xraylens09.lens_thickness |
|
InstrumentXraylens09_lens_length |
Length of the lens |
NX_CHAR |
instrument.xraylens09.lens_length |
|
InstrumentXraylens09_curvature |
Radius of the curvature as measured in the middle of the lens |
NX_CHAR |
instrument.xraylens09.curvature |
|
InstrumentXraylens09_aperture |
Diameter of the lens |
NX_CHAR |
instrument.xraylens09.aperture |
|
InstrumentXraylens09_number_of_lenses |
Number of lenses that make up the compound lens |
NX_CHAR |
instrument.xraylens09.number_of_lenses |
|
InstrumentXraylens09_lens_material |
Material used to make the lens |
NX_CHAR |
instrument.xraylens09.lens_material |
|
InstrumentXraylens10_lens_geometry |
Geometry of the lens. Any of these values:paraboloid,spherical,elliptical,hyperbolical |
NX_CHAR |
instrument.xraylens10.lens_geometry |
|
InstrumentXraylens10_focus_type |
The type of focus of the lens. Any of these values:line,point |
NX_CHAR |
instrument.xraylens10.focus_type |
|
InstrumentXraylens10_lens_thickness |
Thickness of the lens |
NX_CHAR |
instrument.xraylens10.lens_thickness |
|
InstrumentXraylens10_lens_length |
Length of the lens |
NX_CHAR |
instrument.xraylens10.lens_length |
|
InstrumentXraylens10_curvature |
Radius of the curvature as measured in the middle of the lens |
NX_CHAR |
instrument.xraylens10.curvature |
|
InstrumentXraylens10_aperture |
Diameter of the lens |
NX_CHAR |
instrument.xraylens10.aperture |
|
InstrumentXraylens10_number_of_lenses |
Number of lenses that make up the compound lens |
NX_CHAR |
instrument.xraylens10.number_of_lenses |
|
InstrumentXraylens10_lens_material |
Material used to make the lens |
NX_CHAR |
instrument.xraylens10.lens_material |
|
InstrumentAttenuator01_description |
NX_CHAR |
instrument.attenuator01.description |
||
InstrumentAttenuator01_type |
NX_CHAR |
instrument.attenuator01.type |
||
InstrumentAttenuator01_thickness |
NX_CHAR |
instrument.attenuator01.thickness |
||
InstrumentAttenuator01_status |
NX_CHAR |
instrument.attenuator01.status |
||
InstrumentAttenuator01_distance |
NX_CHAR |
instrument.attenuator01.distance |
||
InstrumentAttenuator01Positioners_name |
NX_CHAR |
instrument.attenuator01.positioners.name |
||
InstrumentAttenuator01Positioners_value |
NX_CHAR |
instrument.attenuator01.positioners.value |
||
InstrumentAttenuator02_type |
NX_CHAR |
instrument.attenuator02.type |
||
InstrumentAttenuator02_thickness |
NX_CHAR |
instrument.attenuator02.thickness |
||
InstrumentAttenuator02_status |
NX_CHAR |
instrument.attenuator02.status |
||
InstrumentAttenuator02_distance |
NX_CHAR |
instrument.attenuator02.distance |
||
InstrumentAttenuator02Positioners_name |
NX_CHAR |
instrument.attenuator02.positioners.name |
||
InstrumentAttenuator02Positioners_value |
NX_CHAR |
instrument.attenuator02.positioners.value |
||
InstrumentAttenuator03_type |
NX_CHAR |
instrument.attenuator03.type |
||
InstrumentAttenuator03_thickness |
NX_CHAR |
instrument.attenuator03.thickness |
||
InstrumentAttenuator03_status |
NX_CHAR |
instrument.attenuator03.status |
||
InstrumentAttenuator03_distance |
NX_CHAR |
instrument.attenuator03.distance |
||
InstrumentAttenuator03Positioners_name |
NX_CHAR |
instrument.attenuator03.positioners.name |
||
InstrumentAttenuator03Positioners_value |
NX_CHAR |
instrument.attenuator03.positioners.value |
||
InstrumentAttenuator04_type |
NX_CHAR |
instrument.attenuator04.type |
||
InstrumentAttenuator04_thickness |
NX_CHAR |
instrument.attenuator04.thickness |
||
InstrumentAttenuator04_status |
NX_CHAR |
instrument.attenuator04.status |
||
InstrumentAttenuator04_distance |
NX_CHAR |
instrument.attenuator04.distance |
||
InstrumentAttenuator04Positioners_name |
NX_CHAR |
instrument.attenuator04.positioners.name |
||
InstrumentAttenuator04Positioners_value |
NX_CHAR |
instrument.attenuator04.positioners.value |
||
InstrumentAttenuator05_type |
NX_CHAR |
instrument.attenuator05.type |
||
InstrumentAttenuator05_thickness |
NX_CHAR |
instrument.attenuator05.thickness |
||
InstrumentAttenuator05_status |
NX_CHAR |
instrument.attenuator05.status |
||
InstrumentAttenuator05_distance |
NX_CHAR |
instrument.attenuator05.distance |
||
InstrumentAttenuator05Positioners_name |
NX_CHAR |
instrument.attenuator05.positioners.name |
||
InstrumentAttenuator05Positioners_value |
NX_CHAR |
instrument.attenuator05.positioners.value |
||
InstrumentAttenuator06_type |
NX_CHAR |
instrument.attenuator06.type |
||
InstrumentAttenuator06_thickness |
NX_CHAR |
instrument.attenuator06.thickness |
||
InstrumentAttenuator06_status |
NX_CHAR |
instrument.attenuator06.status |
||
InstrumentAttenuator06_distance |
NX_CHAR |
instrument.attenuator06.distance |
||
InstrumentAttenuator06Positioners_name |
NX_CHAR |
instrument.attenuator06.positioners.name |
||
InstrumentAttenuator06Positioners_value |
NX_CHAR |
instrument.attenuator06.positioners.value |
||
InstrumentAttenuator07_type |
NX_CHAR |
instrument.attenuator07.type |
||
InstrumentAttenuator07_thickness |
NX_CHAR |
instrument.attenuator07.thickness |
||
InstrumentAttenuator07_status |
NX_CHAR |
instrument.attenuator07.status |
||
InstrumentAttenuator07_distance |
NX_CHAR |
instrument.attenuator07.distance |
||
InstrumentAttenuator07Positioners_name |
NX_CHAR |
instrument.attenuator07.positioners.name |
||
InstrumentAttenuator07Positioners_value |
NX_CHAR |
instrument.attenuator07.positioners.value |
||
InstrumentAttenuator08_type |
NX_CHAR |
instrument.attenuator08.type |
||
InstrumentAttenuator08_thickness |
NX_CHAR |
instrument.attenuator08.thickness |
||
InstrumentAttenuator08_status |
NX_CHAR |
instrument.attenuator08.status |
||
InstrumentAttenuator08_distance |
NX_CHAR |
instrument.attenuator08.distance |
||
InstrumentAttenuator08Positioners_name |
NX_CHAR |
instrument.attenuator08.positioners.name |
||
InstrumentAttenuator08Positioners_value |
NX_CHAR |
instrument.attenuator08.positioners.value |
||
InstrumentAttenuator09_type |
NX_CHAR |
instrument.attenuator09.type |
||
InstrumentAttenuator09_thickness |
NX_CHAR |
instrument.attenuator09.thickness |
||
InstrumentAttenuator09_status |
NX_CHAR |
instrument.attenuator09.status |
||
InstrumentAttenuator09_distance |
NX_CHAR |
instrument.attenuator09.distance |
||
InstrumentAttenuator09Positioners_name |
NX_CHAR |
instrument.attenuator09.positioners.name |
||
InstrumentAttenuator09Positioners_value |
NX_CHAR |
instrument.attenuator09.positioners.value |
||
InstrumentAttenuator10_type |
NX_CHAR |
instrument.attenuator10.type |
||
InstrumentAttenuator10_thickness |
NX_CHAR |
instrument.attenuator10.thickness |
||
InstrumentAttenuator10_status |
NX_CHAR |
instrument.attenuator10.status |
||
InstrumentAttenuator10_distance |
NX_CHAR |
instrument.attenuator10.distance |
||
InstrumentAttenuator10Positioners_name |
NX_CHAR |
instrument.attenuator10.positioners.name |
||
InstrumentAttenuator10Positioners_value |
NX_CHAR |
instrument.attenuator10.positioners.value |
||
InstrumentAttenuator11_type |
NX_CHAR |
instrument.attenuator11.type |
||
InstrumentAttenuator11_thickness |
NX_CHAR |
instrument.attenuator11.thickness |
||
InstrumentAttenuator11_status |
NX_CHAR |
instrument.attenuator11.status |
||
InstrumentAttenuator11_distance |
NX_CHAR |
instrument.attenuator11.distance |
||
InstrumentAttenuator11Positioners_name |
NX_CHAR |
instrument.attenuator11.positioners.name |
||
InstrumentAttenuator11Positioners_value |
NX_CHAR |
instrument.attenuator11.positioners.value |
||
InstrumentAttenuator12_type |
NX_CHAR |
instrument.attenuator12.type |
||
InstrumentAttenuator12_thickness |
NX_CHAR |
instrument.attenuator12.thickness |
||
InstrumentAttenuator12_status |
NX_CHAR |
instrument.attenuator12.status |
||
InstrumentAttenuator12_distance |
NX_CHAR |
instrument.attenuator12.distance |
||
InstrumentAttenuator12Positioners_name |
NX_CHAR |
instrument.attenuator12.positioners.name |
||
InstrumentAttenuator12Positioners_value |
NX_CHAR |
instrument.attenuator12.positioners.value |
||
InstrumentAttenuator13_type |
NX_CHAR |
instrument.attenuator13.type |
||
InstrumentAttenuator13_thickness |
NX_CHAR |
instrument.attenuator13.thickness |
||
InstrumentAttenuator13_status |
NX_CHAR |
instrument.attenuator13.status |
||
InstrumentAttenuator13_distance |
NX_CHAR |
instrument.attenuator13.distance |
||
InstrumentAttenuator13Positioners_name |
NX_CHAR |
instrument.attenuator13.positioners.name |
||
InstrumentAttenuator13Positioners_value |
NX_CHAR |
instrument.attenuator13.positioners.value |
||
InstrumentAttenuator14_type |
NX_CHAR |
instrument.attenuator14.type |
||
InstrumentAttenuator14_thickness |
NX_CHAR |
instrument.attenuator14.thickness |
||
InstrumentAttenuator14_status |
NX_CHAR |
instrument.attenuator14.status |
||
InstrumentAttenuator14_distance |
NX_CHAR |
instrument.attenuator14.distance |
||
InstrumentAttenuator14Positioners_name |
NX_CHAR |
instrument.attenuator14.positioners.name |
||
InstrumentAttenuator14Positioners_value |
NX_CHAR |
instrument.attenuator14.positioners.value |
||
InstrumentAttenuator15_type |
NX_CHAR |
instrument.attenuator15.type |
||
InstrumentAttenuator15_thickness |
NX_CHAR |
instrument.attenuator15.thickness |
||
InstrumentAttenuator15_status |
NX_CHAR |
instrument.attenuator15.status |
||
InstrumentAttenuator15_distance |
NX_CHAR |
instrument.attenuator15.distance |
||
InstrumentAttenuator15Positioners_name |
NX_CHAR |
instrument.attenuator15.positioners.name |
||
InstrumentAttenuator15Positioners_value |
NX_CHAR |
instrument.attenuator15.positioners.value |
||
InstrumentInsertionDevice_gap_name |
NX_CHAR |
instrument.insertion_device.gap.name |
||
InstrumentInsertionDevice_gap_value |
NX_CHAR |
instrument.insertion_device.gap.value |
||
InstrumentInsertionDevice_taper_name |
NX_CHAR |
instrument.insertion_device.taper.name |
||
InstrumentInsertionDevice_taper_value |
NX_CHAR |
instrument.insertion_device.taper.value |
||
InstrumentOpticsPositioners_name |
NX_CHAR |
instrument.optics.positioners.name |
||
InstrumentOpticsPositioners_value |
NX_CHAR |
instrument.optics.positioners.value |
||
InstrumentEnvironmentSensors_name |
NX_CHAR |
instrument.environment.sensors.name |
||
InstrumentEnvironmentSensors_value |
NX_CHAR |
instrument.environment.sensors.value |
||
InstrumentDetector01_name |
Name of the detector |
NX_CHAR |
instrument.detector01.name |
|
InstrumentDetector01_type |
Description of type such as He3 gas cylinder, He3 PSD, scintillator, fission chamber, proportion counter, ion chamber, ccd, pixel, image plate, CMOS, … |
NX_CHAR |
instrument.detector01.type |
|
InstrumentDetector01_manufacturer |
Name of the manufacturer of the detector. Example: Dectris |
NX_CHAR |
instrument.detector01.manufacturer |
|
InstrumentDetector01_model |
Model of the detector. Example: Pilatus3_6M |
NX_CHAR |
instrument.detector01.model |
|
InstrumentDetector01_preset_time |
Desired measuring time |
NX_FLOAT |
instrument.detector01.preset_time |
|
InstrumentDetector01_elapsed_live_time |
Time the detector has been actually measuring (elapsed_time - dead_time) |
NX_FLOAT |
instrument.detector01.live_time |
|
InstrumentDetector01_elapsed_real_time |
Time elapsed between start and stop of the measurement |
NX_FLOAT |
instrument.detector01.elapsed_time |
|
InstrumentDetector01_calibration |
For MCA detectors, coefficients a, b, c to compute a scale based on channel number as a + b * x + c * x * x |
NX_CHAR |
instrument.detector01.calibration |
|
InstrumentDetector01_description |
name/manufacturer/model/etc. information |
NX_CHAR |
instrument.detector01.description |
|
InstrumentDetector01_local_name |
Local name for the detector |
NX_CHAR |
instrument.detector01.local_name |
|
InstrumentDetector01_x_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector01.x_pixel_size |
|
InstrumentDetector01_y_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector01.y_pixel_size |
|
InstrumentDetector01_calibration_date |
NX_CHAR |
instrument.detector01.calibration_date |
||
InstrumentDetector01_layout |
How the detector is represented. Any of these values: point | linear | area |
NX_CHAR |
instrument.detector01.layout |
|
InstrumentDetector01_beam_center_x |
This is the x position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector01.beam_center_x |
|
InstrumentDetector01_beam_center_y |
This is the y position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector01.beam_center_y |
|
InstrumentDetector01_flat_field_applied |
True when the flat field correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector01.flatfield_applied |
|
InstrumentDetector01_pixel_mask |
The 32-bit pixel mask for the detector |
NX_CHAR |
instrument.detector01.pixel_mask |
|
InstrumentDetector01_pixel_mask_applied |
True when the pixel mask correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector01.pixel_mask_applied |
|
InstrumentDetector01_countrate_correction_applied |
Counting detectors usually are not able to measure all incoming particles, especially at higher count-rates. Count-rate correction is applied to account for these errors. |
NX_CHAR |
instrument.detector01.countrate_correction_applied |
|
InstrumentDetector01_saturation_value |
The value at which the detector goes into saturation. Especially common to CCD detectors, the data is known to be invalid above this value. |
NX_CHAR |
instrument.detector01.saturation_value |
|
InstrumentDetector01_threshold_energy |
Single photon counter detectors can be adjusted for a certain energy range in which they work optimally. This is the energy setting for this. |
NX_CHAR |
instrument.detector01.threshold_energy |
|
InstrumentDetector01_sensor_thickness |
NX_CHAR |
instrument.detector01.sensor_thickness |
||
InstrumentDetector01_sensor_material |
At times, radiation is not directly sensed by the detector. Rather, the detector might sense the output from some converter like a scintillator. This is the name of this converter material. |
NX_CHAR |
instrument.detector01.sensor_material |
|
InstrumentDetector01_bit_depth_readout |
How many bits the electronics reads per pixel. With CCD’s and single photon counting detectors, this must not align with traditional integer sizes. This can be 4, 8, 12, 14, 16, |
NX_CHAR |
instrument.detector01.bit_depth_readout |
|
InstrumentDetector01_distance |
This is the distance to the previous component in the instrument; most often the sample. The usage depends on the nature of the detector: Most often it is the distance of the detector assembly. But there are irregular detectors. In this case the distance must be specified for each detector pixel. |
NX_CHAR |
instrument.detector01.distance |
|
InstrumentDetector01_frame_time |
This is time for each frame. This is exposure_time + readout time. |
NX_CHAR |
instrument.detector01.frame_time |
|
InstrumentDetector01_acquisition_mode |
The acquisition mode of the detector. Any of these values: gated,triggered,summed,event,histogrammed,decimated |
NX_CHAR |
instrument.detector01.acquisition_mode |
|
InstrumentDetector01Positioners_name |
NX_CHAR |
instrument.detector01.positioners.name |
||
InstrumentDetector01Positioners_value |
NX_CHAR |
instrument.detector01.positioners.value |
||
InstrumentDetector01Rois_name |
NX_CHAR |
instrument.detector01.rois.name |
||
InstrumentDetector01Rois_value |
Parameters defining the ROI. Format: R1P1,R1P2 R2P1,R2P2 … RnP1,RnP2 |
NX_CHAR |
instrument.detector01.rois.value |
|
InstrumentDetector02_name |
Name of the detector |
NX_CHAR |
instrument.detector02.name |
|
InstrumentDetector02_type |
Description of type such as He3 gas cylinder, He3 PSD, scintillator, fission chamber, proportion counter, ion chamber, ccd, pixel, image plate, CMOS, … |
NX_CHAR |
instrument.detector02.type |
|
InstrumentDetector02_manufacturer |
Name of the manufacturer of the detector. Example: Dectris |
NX_CHAR |
instrument.detector02.manufacturer |
|
InstrumentDetector02_model |
Model of the detector. Example: Pilatus3_6M |
NX_CHAR |
instrument.detector02.model |
|
InstrumentDetector02_preset_time |
Desired measuring time |
NX_FLOAT |
instrument.detector02.preset_time |
|
InstrumentDetector02_elapsed_live_time |
Time the detector has been actually measuring (elapsed_time - dead_time) |
NX_FLOAT |
instrument.detector02.live_time |
|
InstrumentDetector02_elapsed_real_time |
Time elapsed between start and stop of the measurement |
NX_FLOAT |
instrument.detector02.elapsed_time |
|
InstrumentDetector02_calibration |
For MCA detectors, coefficients a, b, c to compute a scale based on channel number as a + b * x + c * x * x |
NX_CHAR |
instrument.detector02.calibration |
|
InstrumentDetector02_description |
name/manufacturer/model/etc. information |
NX_CHAR |
instrument.detector02.description |
|
InstrumentDetector02_local_name |
Local name for the detector |
NX_CHAR |
instrument.detector02.local_name |
|
InstrumentDetector02_x_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector02.x_pixel_size |
|
InstrumentDetector02_y_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector02.y_pixel_size |
|
InstrumentDetector02_calibration_date |
NX_CHAR |
instrument.detector02.calibration_date |
||
InstrumentDetector02_layout |
How the detector is represented. Any of these values: point | linear | area |
NX_CHAR |
instrument.detector02.layout |
|
InstrumentDetector02_beam_center_x |
This is the x position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector02.beam_center_x |
|
InstrumentDetector02_beam_center_y |
This is the y position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector02.beam_center_y |
|
InstrumentDetector02_flat_field_applied |
True when the flat field correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector02.flatfield_applied |
|
InstrumentDetector02_pixel_mask |
The 32-bit pixel mask for the detector |
NX_CHAR |
instrument.detector02.pixel_mask |
|
InstrumentDetector02_pixel_mask_applied |
True when the pixel mask correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector02.pixel_mask_applied |
|
InstrumentDetector02_countrate_correction_applied |
Counting detectors usually are not able to measure all incoming particles, especially at higher count-rates. Count-rate correction is applied to account for these errors. |
NX_CHAR |
instrument.detector02.countrate_correction_applied |
|
InstrumentDetector02_saturation_value |
The value at which the detector goes into saturation. Especially common to CCD detectors, the data is known to be invalid above this value. |
NX_CHAR |
instrument.detector02.saturation_value |
|
InstrumentDetector02_threshold_energy |
Single photon counter detectors can be adjusted for a certain energy range in which they work optimally. This is the energy setting for this. |
NX_CHAR |
instrument.detector02.threshold_energy |
|
InstrumentDetector02_sensor_thickness |
NX_CHAR |
instrument.detector02.sensor_thickness |
||
InstrumentDetector02_sensor_material |
At times, radiation is not directly sensed by the detector. Rather, the detector might sense the output from some converter like a scintillator. This is the name of this converter material. |
NX_CHAR |
instrument.detector02.sensor_material |
|
InstrumentDetector02_bit_depth_readout |
How many bits the electronics reads per pixel. With CCD’s and single photon counting detectors, this must not align with traditional integer sizes. This can be 4, 8, 12, 14, 16, |
NX_CHAR |
instrument.detector02.bit_depth_readout |
|
InstrumentDetector02_distance |
This is the distance to the previous component in the instrument; most often the sample. The usage depends on the nature of the detector: Most often it is the distance of the detector assembly. But there are irregular detectors. In this case the distance must be specified for each detector pixel. |
NX_CHAR |
instrument.detector02.distance |
|
InstrumentDetector02_frame_time |
This is time for each frame. This is exposure_time + readout time. |
NX_CHAR |
instrument.detector02.frame_time |
|
InstrumentDetector02_acquisition_mode |
The acquisition mode of the detector. Any of these values: gated,triggered,summed,event,histogrammed,decimated |
NX_CHAR |
instrument.detector02.acquisition_mode |
|
InstrumentDetector02Positioners_name |
NX_CHAR |
instrument.detector02.positioners.name |
||
InstrumentDetector02Positioners_value |
NX_CHAR |
instrument.detector02.positioners.value |
||
InstrumentDetector02Rois_name |
NX_CHAR |
instrument.detector02.rois.name |
||
InstrumentDetector02Rois_value |
Parameters defining the ROI. Format: R1P1,R1P2 R2P1,R2P2 … RnP1,RnP2 |
NX_CHAR |
instrument.detector02.rois.value |
|
InstrumentDetector03_name |
Name of the detector |
NX_CHAR |
instrument.detector03.name |
|
InstrumentDetector03_type |
Description of type such as He3 gas cylinder, He3 PSD, scintillator, fission chamber, proportion counter, ion chamber, ccd, pixel, image plate, CMOS, … |
NX_CHAR |
instrument.detector03.type |
|
InstrumentDetector03_manufacturer |
Name of the manufacturer of the detector. Example: Dectris |
NX_CHAR |
instrument.detector03.manufacturer |
|
InstrumentDetector03_model |
Model of the detector. Example: Pilatus3_6M |
NX_CHAR |
instrument.detector03.model |
|
InstrumentDetector03_preset_time |
Desired measuring time |
NX_FLOAT |
instrument.detector03.preset_time |
|
InstrumentDetector03_elapsed_live_time |
Time the detector has been actually measuring (elapsed_time - dead_time) |
NX_FLOAT |
instrument.detector03.live_time |
|
InstrumentDetector03_elapsed_real_time |
Time elapsed between start and stop of the measurement |
NX_FLOAT |
instrument.detector03.elapsed_time |
|
InstrumentDetector03_calibration |
For MCA detectors, coefficients a, b, c to compute a scale based on channel number as a + b * x + c * x * x |
NX_CHAR |
instrument.detector03.calibration |
|
InstrumentDetector03_description |
name/manufacturer/model/etc. information |
NX_CHAR |
instrument.detector03.description |
|
InstrumentDetector03_local_name |
Local name for the detector |
NX_CHAR |
instrument.detector03.local_name |
|
InstrumentDetector03_x_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector03.x_pixel_size |
|
InstrumentDetector03_y_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector03.y_pixel_size |
|
InstrumentDetector03_calibration_date |
NX_CHAR |
instrument.detector03.calibration_date |
||
InstrumentDetector03_layout |
How the detector is represented. Any of these values: point | linear | area |
NX_CHAR |
instrument.detector03.layout |
|
InstrumentDetector03_beam_center_x |
This is the x position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector03.beam_center_x |
|
InstrumentDetector03_beam_center_y |
This is the y position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector03.beam_center_y |
|
InstrumentDetector03_flat_field_applied |
True when the flat field correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector03.flatfield_applied |
|
InstrumentDetector03_pixel_mask |
The 32-bit pixel mask for the detector |
NX_CHAR |
instrument.detector03.pixel_mask |
|
InstrumentDetector03_pixel_mask_applied |
True when the pixel mask correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector03.pixel_mask_applied |
|
InstrumentDetector03_countrate_correction_applied |
Counting detectors usually are not able to measure all incoming particles, especially at higher count-rates. Count-rate correction is applied to account for these errors. |
NX_CHAR |
instrument.detector03.countrate_correction_applied |
|
InstrumentDetector03_saturation_value |
The value at which the detector goes into saturation. Especially common to CCD detectors, the data is known to be invalid above this value. |
NX_CHAR |
instrument.detector03.saturation_value |
|
InstrumentDetector03_threshold_energy |
Single photon counter detectors can be adjusted for a certain energy range in which they work optimally. This is the energy setting for this. |
NX_CHAR |
instrument.detector03.threshold_energy |
|
InstrumentDetector03_sensor_thickness |
NX_CHAR |
instrument.detector03.sensor_thickness |
||
InstrumentDetector03_sensor_material |
At times, radiation is not directly sensed by the detector. Rather, the detector might sense the output from some converter like a scintillator. This is the name of this converter material. |
NX_CHAR |
instrument.detector03.sensor_material |
|
InstrumentDetector03_bit_depth_readout |
How many bits the electronics reads per pixel. With CCD’s and single photon counting detectors, this must not align with traditional integer sizes. This can be 4, 8, 12, 14, 16, |
NX_CHAR |
instrument.detector03.bit_depth_readout |
|
InstrumentDetector03_distance |
This is the distance to the previous component in the instrument; most often the sample. The usage depends on the nature of the detector: Most often it is the distance of the detector assembly. But there are irregular detectors. In this case the distance must be specified for each detector pixel. |
NX_CHAR |
instrument.detector03.distance |
|
InstrumentDetector03_frame_time |
This is time for each frame. This is exposure_time + readout time. |
NX_CHAR |
instrument.detector03.frame_time |
|
InstrumentDetector03_acquisition_mode |
The acquisition mode of the detector. Any of these values: gated,triggered,summed,event,histogrammed,decimated |
NX_CHAR |
instrument.detector03.acquisition_mode |
|
InstrumentDetector03Positioners_name |
NX_CHAR |
instrument.detector03.positioners.name |
||
InstrumentDetector03Positioners_value |
NX_CHAR |
instrument.detector03.positioners.value |
||
InstrumentDetector03Rois_name |
NX_CHAR |
instrument.detector03.rois.name |
||
InstrumentDetector03Rois_value |
Parameters defining the ROI. Format: R1P1,R1P2 R2P1,R2P2 … RnP1,RnP2 |
NX_CHAR |
instrument.detector03.rois.value |
|
InstrumentDetector04_name |
Name of the detector |
NX_CHAR |
instrument.detector04.name |
|
InstrumentDetector04_type |
Description of type such as He3 gas cylinder, He3 PSD, scintillator, fission chamber, proportion counter, ion chamber, ccd, pixel, image plate, CMOS, … |
NX_CHAR |
instrument.detector04.type |
|
InstrumentDetector04_manufacturer |
Name of the manufacturer of the detector. Example: Dectris |
NX_CHAR |
instrument.detector04.manufacturer |
|
InstrumentDetector04_model |
Model of the detector. Example: Pilatus3_6M |
NX_CHAR |
instrument.detector04.model |
|
InstrumentDetector04_preset_time |
Desired measuring time |
NX_FLOAT |
instrument.detector04.preset_time |
|
InstrumentDetector04_elapsed_live_time |
Time the detector has been actually measuring (elapsed_time - dead_time) |
NX_FLOAT |
instrument.detector04.live_time |
|
InstrumentDetector04_elapsed_real_time |
Time elapsed between start and stop of the measurement |
NX_FLOAT |
instrument.detector04.elapsed_time |
|
InstrumentDetector04_calibration |
For MCA detectors, coefficients a, b, c to compute a scale based on channel number as a + b * x + c * x * x |
NX_CHAR |
instrument.detector04.calibration |
|
InstrumentDetector04_description |
name/manufacturer/model/etc. information |
NX_CHAR |
instrument.detector04.description |
|
InstrumentDetector04_local_name |
Local name for the detector |
NX_CHAR |
instrument.detector04.local_name |
|
InstrumentDetector04_x_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector04.x_pixel_size |
|
InstrumentDetector04_y_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector04.y_pixel_size |
|
InstrumentDetector04_calibration_date |
NX_CHAR |
instrument.detector04.calibration_date |
||
InstrumentDetector04_layout |
How the detector is represented. Any of these values: point | linear | area |
NX_CHAR |
instrument.detector04.layout |
|
InstrumentDetector04_beam_center_x |
This is the x position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector04.beam_center_x |
|
InstrumentDetector04_beam_center_y |
This is the y position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector04.beam_center_y |
|
InstrumentDetector04_flat_field_applied |
True when the flat field correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector04.flatfield_applied |
|
InstrumentDetector04_pixel_mask |
The 32-bit pixel mask for the detector |
NX_CHAR |
instrument.detector04.pixel_mask |
|
InstrumentDetector04_pixel_mask_applied |
True when the pixel mask correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector04.pixel_mask_applied |
|
InstrumentDetector04_countrate_correction_applied |
Counting detectors usually are not able to measure all incoming particles, especially at higher count-rates. Count-rate correction is applied to account for these errors. |
NX_CHAR |
instrument.detector04.countrate_correction_applied |
|
InstrumentDetector04_saturation_value |
The value at which the detector goes into saturation. Especially common to CCD detectors, the data is known to be invalid above this value. |
NX_CHAR |
instrument.detector04.saturation_value |
|
InstrumentDetector04_threshold_energy |
Single photon counter detectors can be adjusted for a certain energy range in which they work optimally. This is the energy setting for this. |
NX_CHAR |
instrument.detector04.threshold_energy |
|
InstrumentDetector04_sensor_thickness |
NX_CHAR |
instrument.detector04.sensor_thickness |
||
InstrumentDetector04_sensor_material |
At times, radiation is not directly sensed by the detector. Rather, the detector might sense the output from some converter like a scintillator. This is the name of this converter material. |
NX_CHAR |
instrument.detector04.sensor_material |
|
InstrumentDetector04_bit_depth_readout |
How many bits the electronics reads per pixel. With CCD’s and single photon counting detectors, this must not align with traditional integer sizes. This can be 4, 8, 12, 14, 16, |
NX_CHAR |
instrument.detector04.bit_depth_readout |
|
InstrumentDetector04_distance |
This is the distance to the previous component in the instrument; most often the sample. The usage depends on the nature of the detector: Most often it is the distance of the detector assembly. But there are irregular detectors. In this case the distance must be specified for each detector pixel. |
NX_CHAR |
instrument.detector04.distance |
|
InstrumentDetector04_frame_time |
This is time for each frame. This is exposure_time + readout time. |
NX_CHAR |
instrument.detector04.frame_time |
|
InstrumentDetector04_acquisition_mode |
The acquisition mode of the detector. Any of these values: gated,triggered,summed,event,histogrammed,decimated |
NX_CHAR |
instrument.detector04.acquisition_mode |
|
InstrumentDetector04Positioners_name |
NX_CHAR |
instrument.detector04.positioners.name |
||
InstrumentDetector04Positioners_value |
NX_CHAR |
instrument.detector04.positioners.value |
||
InstrumentDetector04Rois_name |
NX_CHAR |
instrument.detector04.rois.name |
||
InstrumentDetector04Rois_value |
Parameters defining the ROI. Format: R1P1,R1P2 R2P1,R2P2 … RnP1,RnP2 |
NX_CHAR |
instrument.detector04.rois.value |
|
InstrumentDetector05_name |
Name of the detector |
NX_CHAR |
instrument.detector05.name |
|
InstrumentDetector05_type |
Description of type such as He3 gas cylinder, He3 PSD, scintillator, fission chamber, proportion counter, ion chamber, ccd, pixel, image plate, CMOS, … |
NX_CHAR |
instrument.detector05.type |
|
InstrumentDetector05_manufacturer |
Name of the manufacturer of the detector. Example: Dectris |
NX_CHAR |
instrument.detector05.manufacturer |
|
InstrumentDetector05_model |
Model of the detector. Example: Pilatus3_6M |
NX_CHAR |
instrument.detector05.model |
|
InstrumentDetector05_preset_time |
Desired measuring time |
NX_FLOAT |
instrument.detector05.preset_time |
|
InstrumentDetector05_elapsed_live_time |
Time the detector has been actually measuring (elapsed_time - dead_time) |
NX_FLOAT |
instrument.detector05.live_time |
|
InstrumentDetector05_elapsed_real_time |
Time elapsed between start and stop of the measurement |
NX_FLOAT |
instrument.detector05.elapsed_time |
|
InstrumentDetector05_calibration |
For MCA detectors, coefficients a, b, c to compute a scale based on channel number as a + b * x + c * x * x |
NX_CHAR |
instrument.detector05.calibration |
|
InstrumentDetector05_description |
name/manufacturer/model/etc. information |
NX_CHAR |
instrument.detector05.description |
|
InstrumentDetector05_local_name |
Local name for the detector |
NX_CHAR |
instrument.detector05.local_name |
|
InstrumentDetector05_x_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector05.x_pixel_size |
|
InstrumentDetector05_y_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector05.y_pixel_size |
|
InstrumentDetector05_calibration_date |
NX_CHAR |
instrument.detector05.calibration_date |
||
InstrumentDetector05_layout |
How the detector is represented. Any of these values: point | linear | area |
NX_CHAR |
instrument.detector05.layout |
|
InstrumentDetector05_beam_center_x |
This is the x position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector05.beam_center_x |
|
InstrumentDetector05_beam_center_y |
This is the y position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector05.beam_center_y |
|
InstrumentDetector05_flat_field_applied |
True when the flat field correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector05.flatfield_applied |
|
InstrumentDetector05_pixel_mask |
The 32-bit pixel mask for the detector |
NX_CHAR |
instrument.detector05.pixel_mask |
|
InstrumentDetector05_pixel_mask_applied |
True when the pixel mask correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector05.pixel_mask_applied |
|
InstrumentDetector05_countrate_correction_applied |
Counting detectors usually are not able to measure all incoming particles, especially at higher count-rates. Count-rate correction is applied to account for these errors. |
NX_CHAR |
instrument.detector05.countrate_correction_applied |
|
InstrumentDetector05_saturation_value |
The value at which the detector goes into saturation. Especially common to CCD detectors, the data is known to be invalid above this value. |
NX_CHAR |
instrument.detector05.saturation_value |
|
InstrumentDetector05_threshold_energy |
Single photon counter detectors can be adjusted for a certain energy range in which they work optimally. This is the energy setting for this. |
NX_CHAR |
instrument.detector05.threshold_energy |
|
InstrumentDetector05_sensor_thickness |
NX_CHAR |
instrument.detector05.sensor_thickness |
||
InstrumentDetector05_sensor_material |
At times, radiation is not directly sensed by the detector. Rather, the detector might sense the output from some converter like a scintillator. This is the name of this converter material. |
NX_CHAR |
instrument.detector05.sensor_material |
|
InstrumentDetector05_bit_depth_readout |
How many bits the electronics reads per pixel. With CCD’s and single photon counting detectors, this must not align with traditional integer sizes. This can be 4, 8, 12, 14, 16, |
NX_CHAR |
instrument.detector05.bit_depth_readout |
|
InstrumentDetector05_distance |
This is the distance to the previous component in the instrument; most often the sample. The usage depends on the nature of the detector: Most often it is the distance of the detector assembly. But there are irregular detectors. In this case the distance must be specified for each detector pixel. |
NX_CHAR |
instrument.detector05.distance |
|
InstrumentDetector05_frame_time |
This is time for each frame. This is exposure_time + readout time. |
NX_CHAR |
instrument.detector05.frame_time |
|
InstrumentDetector05_acquisition_mode |
The acquisition mode of the detector. Any of these values: gated,triggered,summed,event,histogrammed,decimated |
NX_CHAR |
instrument.detector05.acquisition_mode |
|
InstrumentDetector05Positioners_name |
NX_CHAR |
instrument.detector05.positioners.name |
||
InstrumentDetector05Positioners_value |
NX_CHAR |
instrument.detector05.positioners.value |
||
InstrumentDetector05Rois_name |
NX_CHAR |
instrument.detector05.rois.name |
||
InstrumentDetector05Rois_value |
Parameters defining the ROI. Format: R1P1,R1P2 R2P1,R2P2 … RnP1,RnP2 |
NX_CHAR |
instrument.detector05.rois.value |
|
InstrumentDetector06_name |
Name of the detector |
NX_CHAR |
instrument.detector06.name |
|
InstrumentDetector06_type |
Description of type such as He3 gas cylinder, He3 PSD, scintillator, fission chamber, proportion counter, ion chamber, ccd, pixel, image plate, CMOS, … |
NX_CHAR |
instrument.detector06.type |
|
InstrumentDetector06_manufacturer |
Name of the manufacturer of the detector. Example: Dectris |
NX_CHAR |
instrument.detector06.manufacturer |
|
InstrumentDetector06_model |
Model of the detector. Example: Pilatus3_6M |
NX_CHAR |
instrument.detector06.model |
|
InstrumentDetector06_preset_time |
Desired measuring time |
NX_FLOAT |
instrument.detector06.preset_time |
|
InstrumentDetector06_elapsed_live_time |
Time the detector has been actually measuring (elapsed_time - dead_time) |
NX_FLOAT |
instrument.detector06.live_time |
|
InstrumentDetector06_elapsed_real_time |
Time elapsed between start and stop of the measurement |
NX_FLOAT |
instrument.detector06.elapsed_time |
|
InstrumentDetector06_calibration |
For MCA detectors, coefficients a, b, c to compute a scale based on channel number as a + b * x + c * x * x |
NX_CHAR |
instrument.detector06.calibration |
|
InstrumentDetector06_description |
name/manufacturer/model/etc. information |
NX_CHAR |
instrument.detector06.description |
|
InstrumentDetector06_local_name |
Local name for the detector |
NX_CHAR |
instrument.detector06.local_name |
|
InstrumentDetector06_x_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector06.x_pixel_size |
|
InstrumentDetector06_y_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector06.y_pixel_size |
|
InstrumentDetector06_calibration_date |
NX_CHAR |
instrument.detector06.calibration_date |
||
InstrumentDetector06_layout |
How the detector is represented. Any of these values: point | linear | area |
NX_CHAR |
instrument.detector06.layout |
|
InstrumentDetector06_beam_center_x |
This is the x position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector06.beam_center_x |
|
InstrumentDetector06_beam_center_y |
This is the y position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector06.beam_center_y |
|
InstrumentDetector06_flat_field_applied |
True when the flat field correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector06.flatfield_applied |
|
InstrumentDetector06_pixel_mask |
The 32-bit pixel mask for the detector |
NX_CHAR |
instrument.detector06.pixel_mask |
|
InstrumentDetector06_pixel_mask_applied |
True when the pixel mask correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector06.pixel_mask_applied |
|
InstrumentDetector06_countrate_correction_applied |
Counting detectors usually are not able to measure all incoming particles, especially at higher count-rates. Count-rate correction is applied to account for these errors. |
NX_CHAR |
instrument.detector06.countrate_correction_applied |
|
InstrumentDetector06_saturation_value |
The value at which the detector goes into saturation. Especially common to CCD detectors, the data is known to be invalid above this value. |
NX_CHAR |
instrument.detector06.saturation_value |
|
InstrumentDetector06_threshold_energy |
Single photon counter detectors can be adjusted for a certain energy range in which they work optimally. This is the energy setting for this. |
NX_CHAR |
instrument.detector06.threshold_energy |
|
InstrumentDetector06_sensor_thickness |
NX_CHAR |
instrument.detector06.sensor_thickness |
||
InstrumentDetector06_sensor_material |
At times, radiation is not directly sensed by the detector. Rather, the detector might sense the output from some converter like a scintillator. This is the name of this converter material. |
NX_CHAR |
instrument.detector06.sensor_material |
|
InstrumentDetector06_bit_depth_readout |
How many bits the electronics reads per pixel. With CCD’s and single photon counting detectors, this must not align with traditional integer sizes. This can be 4, 8, 12, 14, 16, |
NX_CHAR |
instrument.detector06.bit_depth_readout |
|
InstrumentDetector06_distance |
This is the distance to the previous component in the instrument; most often the sample. The usage depends on the nature of the detector: Most often it is the distance of the detector assembly. But there are irregular detectors. In this case the distance must be specified for each detector pixel. |
NX_CHAR |
instrument.detector06.distance |
|
InstrumentDetector06_frame_time |
This is time for each frame. This is exposure_time + readout time. |
NX_CHAR |
instrument.detector06.frame_time |
|
InstrumentDetector06_acquisition_mode |
The acquisition mode of the detector. Any of these values: gated,triggered,summed,event,histogrammed,decimated |
NX_CHAR |
instrument.detector06.acquisition_mode |
|
InstrumentDetector06Positioners_name |
NX_CHAR |
instrument.detector06.positioners.name |
||
InstrumentDetector06Positioners_value |
NX_CHAR |
instrument.detector06.positioners.value |
||
InstrumentDetector06Rois_name |
NX_CHAR |
instrument.detector06.rois.name |
||
InstrumentDetector06Rois_value |
Parameters defining the ROI. Format: R1P1,R1P2 R2P1,R2P2 … RnP1,RnP2 |
NX_CHAR |
instrument.detector06.rois.value |
|
InstrumentDetector07_name |
Name of the detector |
NX_CHAR |
instrument.detector07.name |
|
InstrumentDetector07_type |
Description of type such as He3 gas cylinder, He3 PSD, scintillator, fission chamber, proportion counter, ion chamber, ccd, pixel, image plate, CMOS, … |
NX_CHAR |
instrument.detector07.type |
|
InstrumentDetector07_manufacturer |
Name of the manufacturer of the detector. Example: Dectris |
NX_CHAR |
instrument.detector07.manufacturer |
|
InstrumentDetector07_model |
Model of the detector. Example: Pilatus3_6M |
NX_CHAR |
instrument.detector07.model |
|
InstrumentDetector07_preset_time |
Desired measuring time |
NX_FLOAT |
instrument.detector07.preset_time |
|
InstrumentDetector07_elapsed_live_time |
Time the detector has been actually measuring (elapsed_time - dead_time) |
NX_FLOAT |
instrument.detector07.live_time |
|
InstrumentDetector07_elapsed_real_time |
Time elapsed between start and stop of the measurement |
NX_FLOAT |
instrument.detector07.elapsed_time |
|
InstrumentDetector07_calibration |
For MCA detectors, coefficients a, b, c to compute a scale based on channel number as a + b * x + c * x * x |
NX_CHAR |
instrument.detector07.calibration |
|
InstrumentDetector07_description |
name/manufacturer/model/etc. information |
NX_CHAR |
instrument.detector07.description |
|
InstrumentDetector07_local_name |
Local name for the detector |
NX_CHAR |
instrument.detector07.local_name |
|
InstrumentDetector07_x_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector07.x_pixel_size |
|
InstrumentDetector07_y_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector07.y_pixel_size |
|
InstrumentDetector07_calibration_date |
NX_CHAR |
instrument.detector07.calibration_date |
||
InstrumentDetector07_layout |
How the detector is represented. Any of these values: point | linear | area |
NX_CHAR |
instrument.detector07.layout |
|
InstrumentDetector07_beam_center_x |
This is the x position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector07.beam_center_x |
|
InstrumentDetector07_beam_center_y |
This is the y position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector07.beam_center_y |
|
InstrumentDetector07_flat_field_applied |
True when the flat field correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector07.flatfield_applied |
|
InstrumentDetector07_pixel_mask |
The 32-bit pixel mask for the detector |
NX_CHAR |
instrument.detector07.pixel_mask |
|
InstrumentDetector07_pixel_mask_applied |
True when the pixel mask correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector07.pixel_mask_applied |
|
InstrumentDetector07_countrate_correction_applied |
Counting detectors usually are not able to measure all incoming particles, especially at higher count-rates. Count-rate correction is applied to account for these errors. |
NX_CHAR |
instrument.detector07.countrate_correction_applied |
|
InstrumentDetector07_saturation_value |
The value at which the detector goes into saturation. Especially common to CCD detectors, the data is known to be invalid above this value. |
NX_CHAR |
instrument.detector07.saturation_value |
|
InstrumentDetector07_threshold_energy |
Single photon counter detectors can be adjusted for a certain energy range in which they work optimally. This is the energy setting for this. |
NX_CHAR |
instrument.detector07.threshold_energy |
|
InstrumentDetector07_sensor_thickness |
NX_CHAR |
instrument.detector07.sensor_thickness |
||
InstrumentDetector07_sensor_material |
At times, radiation is not directly sensed by the detector. Rather, the detector might sense the output from some converter like a scintillator. This is the name of this converter material. |
NX_CHAR |
instrument.detector07.sensor_material |
|
InstrumentDetector07_bit_depth_readout |
How many bits the electronics reads per pixel. With CCD’s and single photon counting detectors, this must not align with traditional integer sizes. This can be 4, 8, 12, 14, 16, |
NX_CHAR |
instrument.detector07.bit_depth_readout |
|
InstrumentDetector07_distance |
This is the distance to the previous component in the instrument; most often the sample. The usage depends on the nature of the detector: Most often it is the distance of the detector assembly. But there are irregular detectors. In this case the distance must be specified for each detector pixel. |
NX_CHAR |
instrument.detector07.distance |
|
InstrumentDetector07_frame_time |
This is time for each frame. This is exposure_time + readout time. |
NX_CHAR |
instrument.detector07.frame_time |
|
InstrumentDetector07_acquisition_mode |
The acquisition mode of the detector. Any of these values: gated,triggered,summed,event,histogrammed,decimated |
NX_CHAR |
instrument.detector07.acquisition_mode |
|
InstrumentDetector07Positioners_name |
NX_CHAR |
instrument.detector07.positioners.name |
||
InstrumentDetector07Positioners_value |
NX_CHAR |
instrument.detector07.positioners.value |
||
InstrumentDetector07Rois_name |
NX_CHAR |
instrument.detector07.rois.name |
||
InstrumentDetector07Rois_value |
Parameters defining the ROI. Format: R1P1,R1P2 R2P1,R2P2 … RnP1,RnP2 |
NX_CHAR |
instrument.detector07.rois.value |
|
InstrumentDetector08_name |
Name of the detector |
NX_CHAR |
instrument.detector08.name |
|
InstrumentDetector08_type |
Description of type such as He3 gas cylinder, He3 PSD, scintillator, fission chamber, proportion counter, ion chamber, ccd, pixel, image plate, CMOS, … |
NX_CHAR |
instrument.detector08.type |
|
InstrumentDetector08_manufacturer |
Name of the manufacturer of the detector. Example: Dectris |
NX_CHAR |
instrument.detector08.manufacturer |
|
InstrumentDetector08_model |
Model of the detector. Example: Pilatus3_6M |
NX_CHAR |
instrument.detector08.model |
|
InstrumentDetector08_preset_time |
Desired measuring time |
NX_FLOAT |
instrument.detector08.preset_time |
|
InstrumentDetector08_elapsed_live_time |
Time the detector has been actually measuring (elapsed_time - dead_time) |
NX_FLOAT |
instrument.detector08.live_time |
|
InstrumentDetector08_elapsed_real_time |
Time elapsed between start and stop of the measurement |
NX_FLOAT |
instrument.detector08.elapsed_time |
|
InstrumentDetector08_calibration |
For MCA detectors, coefficients a, b, c to compute a scale based on channel number as a + b * x + c * x * x |
NX_CHAR |
instrument.detector08.calibration |
|
InstrumentDetector08_description |
name/manufacturer/model/etc. information |
NX_CHAR |
instrument.detector08.description |
|
InstrumentDetector08_local_name |
Local name for the detector |
NX_CHAR |
instrument.detector08.local_name |
|
InstrumentDetector08_x_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector08.x_pixel_size |
|
InstrumentDetector08_y_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector08.y_pixel_size |
|
InstrumentDetector08_calibration_date |
NX_CHAR |
instrument.detector08.calibration_date |
||
InstrumentDetector08_layout |
How the detector is represented. Any of these values: point | linear | area |
NX_CHAR |
instrument.detector08.layout |
|
InstrumentDetector08_beam_center_x |
This is the x position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector08.beam_center_x |
|
InstrumentDetector08_beam_center_y |
This is the y position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector08.beam_center_y |
|
InstrumentDetector08_flat_field_applied |
True when the flat field correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector08.flatfield_applied |
|
InstrumentDetector08_pixel_mask |
The 32-bit pixel mask for the detector |
NX_CHAR |
instrument.detector08.pixel_mask |
|
InstrumentDetector08_pixel_mask_applied |
True when the pixel mask correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector08.pixel_mask_applied |
|
InstrumentDetector08_countrate_correction_applied |
Counting detectors usually are not able to measure all incoming particles, especially at higher count-rates. Count-rate correction is applied to account for these errors. |
NX_CHAR |
instrument.detector08.countrate_correction_applied |
|
InstrumentDetector08_saturation_value |
The value at which the detector goes into saturation. Especially common to CCD detectors, the data is known to be invalid above this value. |
NX_CHAR |
instrument.detector08.saturation_value |
|
InstrumentDetector08_threshold_energy |
Single photon counter detectors can be adjusted for a certain energy range in which they work optimally. This is the energy setting for this. |
NX_CHAR |
instrument.detector08.threshold_energy |
|
InstrumentDetector08_sensor_thickness |
NX_CHAR |
instrument.detector08.sensor_thickness |
||
InstrumentDetector08_sensor_material |
At times, radiation is not directly sensed by the detector. Rather, the detector might sense the output from some converter like a scintillator. This is the name of this converter material. |
NX_CHAR |
instrument.detector08.sensor_material |
|
InstrumentDetector08_bit_depth_readout |
How many bits the electronics reads per pixel. With CCD’s and single photon counting detectors, this must not align with traditional integer sizes. This can be 4, 8, 12, 14, 16, |
NX_CHAR |
instrument.detector08.bit_depth_readout |
|
InstrumentDetector08_distance |
This is the distance to the previous component in the instrument; most often the sample. The usage depends on the nature of the detector: Most often it is the distance of the detector assembly. But there are irregular detectors. In this case the distance must be specified for each detector pixel. |
NX_CHAR |
instrument.detector08.distance |
|
InstrumentDetector08_frame_time |
This is time for each frame. This is exposure_time + readout time. |
NX_CHAR |
instrument.detector08.frame_time |
|
InstrumentDetector08_acquisition_mode |
The acquisition mode of the detector. Any of these values: gated,triggered,summed,event,histogrammed,decimated |
NX_CHAR |
instrument.detector08.acquisition_mode |
|
InstrumentDetector08Positioners_name |
NX_CHAR |
instrument.detector08.positioners.name |
||
InstrumentDetector08Positioners_value |
NX_CHAR |
instrument.detector08.positioners.value |
||
InstrumentDetector08Rois_name |
NX_CHAR |
instrument.detector08.rois.name |
||
InstrumentDetector08Rois_value |
Parameters defining the ROI. Format: R1P1,R1P2 R2P1,R2P2 … RnP1,RnP2 |
NX_CHAR |
instrument.detector08.rois.value |
|
InstrumentDetector09_name |
Name of the detector |
NX_CHAR |
instrument.detector09.name |
|
InstrumentDetector09_type |
Description of type such as He3 gas cylinder, He3 PSD, scintillator, fission chamber, proportion counter, ion chamber, ccd, pixel, image plate, CMOS, … |
NX_CHAR |
instrument.detector09.type |
|
InstrumentDetector09_manufacturer |
Name of the manufacturer of the detector. Example: Dectris |
NX_CHAR |
instrument.detector09.manufacturer |
|
InstrumentDetector09_model |
Model of the detector. Example: Pilatus3_6M |
NX_CHAR |
instrument.detector09.model |
|
InstrumentDetector09_preset_time |
Desired measuring time |
NX_FLOAT |
instrument.detector09.preset_time |
|
InstrumentDetector09_elapsed_live_time |
Time the detector has been actually measuring (elapsed_time - dead_time) |
NX_FLOAT |
instrument.detector09.live_time |
|
InstrumentDetector09_elapsed_real_time |
Time elapsed between start and stop of the measurement |
NX_FLOAT |
instrument.detector09.elapsed_time |
|
InstrumentDetector09_calibration |
For MCA detectors, coefficients a, b, c to compute a scale based on channel number as a + b * x + c * x * x |
NX_CHAR |
instrument.detector09.calibration |
|
InstrumentDetector09_description |
name/manufacturer/model/etc. information |
NX_CHAR |
instrument.detector09.description |
|
InstrumentDetector09_local_name |
Local name for the detector |
NX_CHAR |
instrument.detector09.local_name |
|
InstrumentDetector09_x_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector09.x_pixel_size |
|
InstrumentDetector09_y_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector09.y_pixel_size |
|
InstrumentDetector09_calibration_date |
NX_CHAR |
instrument.detector09.calibration_date |
||
InstrumentDetector09_layout |
How the detector is represented. Any of these values: point | linear | area |
NX_CHAR |
instrument.detector09.layout |
|
InstrumentDetector09_beam_center_x |
This is the x position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector09.beam_center_x |
|
InstrumentDetector09_beam_center_y |
This is the y position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector09.beam_center_y |
|
InstrumentDetector09_flat_field_applied |
True when the flat field correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector09.flatfield_applied |
|
InstrumentDetector09_pixel_mask |
The 32-bit pixel mask for the detector |
NX_CHAR |
instrument.detector09.pixel_mask |
|
InstrumentDetector09_pixel_mask_applied |
True when the pixel mask correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector09.pixel_mask_applied |
|
InstrumentDetector09_countrate_correction_applied |
Counting detectors usually are not able to measure all incoming particles, especially at higher count-rates. Count-rate correction is applied to account for these errors. |
NX_CHAR |
instrument.detector09.countrate_correction_applied |
|
InstrumentDetector09_saturation_value |
The value at which the detector goes into saturation. Especially common to CCD detectors, the data is known to be invalid above this value. |
NX_CHAR |
instrument.detector09.saturation_value |
|
InstrumentDetector09_threshold_energy |
Single photon counter detectors can be adjusted for a certain energy range in which they work optimally. This is the energy setting for this. |
NX_CHAR |
instrument.detector09.threshold_energy |
|
InstrumentDetector09_sensor_thickness |
NX_CHAR |
instrument.detector09.sensor_thickness |
||
InstrumentDetector09_sensor_material |
At times, radiation is not directly sensed by the detector. Rather, the detector might sense the output from some converter like a scintillator. This is the name of this converter material. |
NX_CHAR |
instrument.detector09.sensor_material |
|
InstrumentDetector09_bit_depth_readout |
How many bits the electronics reads per pixel. With CCD’s and single photon counting detectors, this must not align with traditional integer sizes. This can be 4, 8, 12, 14, 16, |
NX_CHAR |
instrument.detector09.bit_depth_readout |
|
InstrumentDetector09_distance |
This is the distance to the previous component in the instrument; most often the sample. The usage depends on the nature of the detector: Most often it is the distance of the detector assembly. But there are irregular detectors. In this case the distance must be specified for each detector pixel. |
NX_CHAR |
instrument.detector09.distance |
|
InstrumentDetector09_frame_time |
This is time for each frame. This is exposure_time + readout time. |
NX_CHAR |
instrument.detector09.frame_time |
|
InstrumentDetector09_acquisition_mode |
The acquisition mode of the detector. Any of these values: gated,triggered,summed,event,histogrammed,decimated |
NX_CHAR |
instrument.detector09.acquisition_mode |
|
InstrumentDetector09Positioners_name |
NX_CHAR |
instrument.detector09.positioners.name |
||
InstrumentDetector09Positioners_value |
NX_CHAR |
instrument.detector09.positioners.value |
||
InstrumentDetector09Rois_name |
NX_CHAR |
instrument.detector09.rois.name |
||
InstrumentDetector09Rois_value |
Parameters defining the ROI. Format: R1P1,R1P2 R2P1,R2P2 … RnP1,RnP2 |
NX_CHAR |
instrument.detector09.rois.value |
|
InstrumentDetector10_name |
Name of the detector |
NX_CHAR |
instrument.detector10.name |
|
InstrumentDetector10_type |
Description of type such as He3 gas cylinder, He3 PSD, scintillator, fission chamber, proportion counter, ion chamber, ccd, pixel, image plate, CMOS, … |
NX_CHAR |
instrument.detector10.type |
|
InstrumentDetector10_manufacturer |
Name of the manufacturer of the detector. Example: Dectris |
NX_CHAR |
instrument.detector10.manufacturer |
|
InstrumentDetector10_model |
Model of the detector. Example: Pilatus3_6M |
NX_CHAR |
instrument.detector10.model |
|
InstrumentDetector10_preset_time |
Desired measuring time |
NX_FLOAT |
instrument.detector10.preset_time |
|
InstrumentDetector10_elapsed_live_time |
Time the detector has been actually measuring (elapsed_time - dead_time) |
NX_FLOAT |
instrument.detector10.live_time |
|
InstrumentDetector10_elapsed_real_time |
Time elapsed between start and stop of the measurement |
NX_FLOAT |
instrument.detector10.elapsed_time |
|
InstrumentDetector10_calibration |
For MCA detectors, coefficients a, b, c to compute a scale based on channel number as a + b * x + c * x * x |
NX_CHAR |
instrument.detector10.calibration |
|
InstrumentDetector10_description |
name/manufacturer/model/etc. information |
NX_CHAR |
instrument.detector10.description |
|
InstrumentDetector10_local_name |
Local name for the detector |
NX_CHAR |
instrument.detector10.local_name |
|
InstrumentDetector10_x_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector10.x_pixel_size |
|
InstrumentDetector10_y_pixel_size |
Size of each detector pixel. If it is scalar all pixels are the same size. |
NX_CHAR |
instrument.detector10.y_pixel_size |
|
InstrumentDetector10_calibration_date |
NX_CHAR |
instrument.detector10.calibration_date |
||
InstrumentDetector10_layout |
How the detector is represented. Any of these values: point | linear | area |
NX_CHAR |
instrument.detector10.layout |
|
InstrumentDetector10_beam_center_x |
This is the x position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector10.beam_center_x |
|
InstrumentDetector10_beam_center_y |
This is the y position where the direct beam would hit the detector. This is a length and can be outside of the actual detector. The length can be in physical units or pixels as documented by the units attribute. |
NX_CHAR |
instrument.detector10.beam_center_y |
|
InstrumentDetector10_flat_field_applied |
True when the flat field correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector10.flatfield_applied |
|
InstrumentDetector10_pixel_mask |
The 32-bit pixel mask for the detector |
NX_CHAR |
instrument.detector10.pixel_mask |
|
InstrumentDetector10_pixel_mask_applied |
True when the pixel mask correction has been applied in the electronics, false otherwise. |
NX_CHAR |
instrument.detector10.pixel_mask_applied |
|
InstrumentDetector10_countrate_correction_applied |
Counting detectors usually are not able to measure all incoming particles, especially at higher count-rates. Count-rate correction is applied to account for these errors. |
NX_CHAR |
instrument.detector10.countrate_correction_applied |
|
InstrumentDetector10_saturation_value |
The value at which the detector goes into saturation. Especially common to CCD detectors, the data is known to be invalid above this value. |
NX_CHAR |
instrument.detector10.saturation_value |
|
InstrumentDetector10_threshold_energy |
Single photon counter detectors can be adjusted for a certain energy range in which they work optimally. This is the energy setting for this. |
NX_CHAR |
instrument.detector10.threshold_energy |
|
InstrumentDetector10_sensor_thickness |
NX_CHAR |
instrument.detector10.sensor_thickness |
||
InstrumentDetector10_sensor_material |
At times, radiation is not directly sensed by the detector. Rather, the detector might sense the output from some converter like a scintillator. This is the name of this converter material. |
NX_CHAR |
instrument.detector10.sensor_material |
|
InstrumentDetector10_bit_depth_readout |
How many bits the electronics reads per pixel. With CCD’s and single photon counting detectors, this must not align with traditional integer sizes. This can be 4, 8, 12, 14, 16, |
NX_CHAR |
instrument.detector10.bit_depth_readout |
|
InstrumentDetector10_distance |
This is the distance to the previous component in the instrument; most often the sample. The usage depends on the nature of the detector: Most often it is the distance of the detector assembly. But there are irregular detectors. In this case the distance must be specified for each detector pixel. |
NX_CHAR |
instrument.detector10.distance |
|
InstrumentDetector10_frame_time |
This is time for each frame. This is exposure_time + readout time. |
NX_CHAR |
instrument.detector10.frame_time |
|
InstrumentDetector10_acquisition_mode |
The acquisition mode of the detector. Any of these values: gated,triggered,summed,event,histogrammed,decimated |
NX_CHAR |
instrument.detector10.acquisition_mode |
|
InstrumentDetector10Positioners_name |
NX_CHAR |
instrument.detector10.positioners.name |
||
InstrumentDetector10Positioners_value |
NX_CHAR |
instrument.detector10.positioners.value |
||
InstrumentDetector10Rois_name |
NX_CHAR |
instrument.detector10.rois.name |
||
InstrumentDetector10Rois_value |
Parameters defining the ROI. Format: R1P1,R1P2 R2P1,R2P2 … RnP1,RnP2 |
NX_CHAR |
instrument.detector10.rois.value |
|
Notes_note_00 |
NX_CHAR |
notes.note_00 |
||
Notes_note_01 |
NX_CHAR |
notes.note_01 |
||
Notes_note_02 |
NX_CHAR |
notes.note_02 |
||
Notes_note_03 |
NX_CHAR |
notes.note_03 |
||
Notes_note_04 |
NX_CHAR |
notes.note_04 |
||
Notes_note_05 |
NX_CHAR |
notes.note_05 |
||
Notes_note_06 |
NX_CHAR |
notes.note_06 |
||
Notes_note_07 |
NX_CHAR |
notes.note_07 |
||
Notes_note_08 |
NX_CHAR |
notes.note_08 |
||
Notes_note_09 |
NX_CHAR |
notes.note_09 |
||
Process_program |
NX_CHAR |
process.program |
||
Process_sequence_index |
NX_CHAR |
process.sequence_index |
||
Process_version |
NX_CHAR |
process.version |
||
Process_note |
NX_CHAR |
process.note |
||
Process_triggering |
Defines how the process has been launched. Values are MANUAL, AUTOMATIC |
NX_CHAR |
process.triggering |
|
Workflow_name |
NX_CHAR |
workflow.name |
||
Workflow_id |
NX_CHAR |
workflow.id |
||
Workflow_type |
NX_CHAR |
workflow.type |
||
Workflow_status |
NX_CHAR |
workflow.status |
||
ExternalReferences_neuroglancer |
NX_CHAR |
external_references.neuroglancer |
||
ExternalReferencesPublication_doi |
NX_CHAR |
external_references.publication.doi |
||
ExternalReferencesPublication_endnote |
NX_CHAR |
external_references.publication.endnote |
||
ExternalReferencesDatacollector_endnote |
NX_CHAR |
external_references.datacollector.endnote |
Relation to NeXus#
To save all possible ICAT dataset metadata fields in a NeXus-compliant HDF5 file
icat-nexus-definitions [--filename=icat.h5] [--url https://...]
By default the definitions from the locally installed icat-esrf-definitions are used but a URL to the ICAT definitions XML file can be provided.
An example HDF5 file can be found here.