Status:
base class, extends NXobject, version 1.1
Description:
Template of a detector, detector bank, or multidetector.
Symbols:
These symbols will be used below to coordinate datasets with the same shape.
np: number of scan points (only present in scanning measurements)
i: number of detector pixels in the first (X, slowest) direction
j: number of detector pixels in the second (Y, faster) direction
k: number of detector pixels in the third (Z, if necessary, fastest) direction
tof: number of bins in the time-of-flight histogram
Structure:
time_of_flight[tof+1]: NX_FLOAT {units=NX_TIME_OF_FLIGHT}
raw_time_of_flight[tof+1]: NX_INT {units=NX_PULSES}
detector_number[i, j]: NX_INT
Identifier for detectordata[np, i, j, tof]: NX_NUMBER {units=NX_ANY}
Data values from the detector.
@signal: NX_POSINT
Obligatory value: 1@axes: NX_CHAR
[number of scan points,x_offset?,y_offset?,time_of_flight?]@long_name: NX_CHAR
Title of measurement@check_sum: NX_INT
Integral of data as check of data integrity@link: NX_CHAR
absolute path to location in NXdetectordata_error[np, i, j, tof]: NX_NUMBER {units=NX_ANY}
x_pixel_offset[i, j]: NX_FLOAT {units=NX_LENGTH}
y_pixel_offset[i, j]: NX_FLOAT {units=NX_LENGTH}
distance[np, i, j]: NX_FLOAT {units=NX_LENGTH}
TODO: need documentationpolar_angle[np, i, j]: NX_FLOAT {units=NX_ANGLE}
TODO: need documentationazimuthal_angle[np, i, j]: NX_FLOAT {units=NX_ANGLE}
TODO: need documentationdescription: NX_CHAR
name/manufacturer/model/etc. informationlocal_name: NX_CHAR
Local name for the detectorsolid_angle[i, j]: NX_FLOAT {units=NX_SOLID_ANGLE}
Solid angle subtended by the detector at the samplex_pixel_size[i, j]: NX_FLOAT {units=NX_LENGTH}
Size of each detector pixel. If it is scalar all pixels are the same size.y_pixel_size[i, j]: NX_FLOAT {units=NX_LENGTH}
Size of each detector pixel. If it is scalar all pixels are the same sizedead_time[np, i, j]: NX_FLOAT {units=NX_TIME}
Detector dead timegas_pressure[i, j]: NX_FLOAT {units=NX_PRESSURE}
Detector gas pressuredetection_gas_path: NX_FLOAT {units=NX_LENGTH}
maximum drift space dimensioncrate[i, j]: NX_INT
slot[i, j]: NX_INT
input[i, j]: NX_INT
type: NX_CHAR
Description of type such as He3 gas cylinder, He3 PSD, scintillator, fission chamber, proportion counter, ion chamber, ccd, pixel, image plate, CMOS, ...calibration_date: NX_DATE_TIME
date of last calibration (geometry and/or efficiency) measurementslayout: NX_CHAR
How the detector is represented
Any of these values: point | linear | area
count_time[np]: NX_NUMBER {units=NX_TIME}
Elapsed actual counting timesequence_number[nBrightFrames]: NX_CHAR
In order to properly sort the order of the images taken in (for example) a tomography experiment, a sequence number is stored with each image.beam_center_x: NX_FLOAT {units=NX_LENGTH}
This is the x position where the direct beam would hit the detector. This is a length, not a pixel position, and can be outside of the actual detector.beam_center_y: NX_FLOAT {units=NX_LENGTH}
This is the y position where the direct beam would hit the detector. This is a length, not a pixel position, and can be outside of the actual detector.frame_start_number: NX_INT
This is the start number of the first frame of a scan. In PX one often scans a couple of frames on a give sample, then does something else, then returns to the same sample and scans some more frames. Each time with a new data file. This number helps concatenating such measurements.diameter: NX_FLOAT {units=NX_LENGTH}
The diameter of a cylindrical detectoracquisition_mode: NX_CHAR
The acquisition mode of the detector.
Any of these values:
- gated
- triggered
- summed
- event
- histogrammed
angular_calibration_applied: NX_BOOLEAN
True when the angular calibration has been applied in the electronics, false otherwise.angular_calibration[i, j]: NX_FLOAT
Angular calibration data.flatfield_applied: NX_BOOLEAN
True when the flat field correction has been applied in the electronics, false otherwise.flatfield[i, j]: NX_FLOAT
Flat field correction data.flatfield_error[i, j]: NX_FLOAT
Errors of the flat field correction data.pixel_mask_applied: NX_BOOLEAN
True when the pixel mask correction has been applied in the electronics, false otherwise.pixel_mask[i, j]: NX_INT
The 32-bit pixel mask for the detector. Contains a bit field for each pixel to signal dead, blind or high or otherwise unwanted or undesirable pixels. They have the following meaning:
- bit 0: gap (pixel with no sensor)
- bit 1: dead
- bit 2: under responding
- bit 3: over responding
- bit 4: noisy
- bit 5: -undefined-
- bit 6: pixel is part of a cluster of problematic pixels (bit set in addition to others)
- bit 7: -undefined-
- bit 8: user defined mask (e.g. around beamstop)
- bits 9-30: -undefined-
- bit 31: virtual pixel (corner pixel with interpolated value)
The normal data analysis software would not take pixels into account when a bit in (mask & 0x00FF) is set. Tag bit in the upper two bytes would indicate special pixel properties that normally would not be a sole reason to reject the intensity value (unless lower bits are set as well of course).
countrate_correction__applied: NX_BOOLEAN
True when a count-rate correction has already been applied in the electronics, false otherwise.bit_depth_readout: NX_INT
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, ...detector_readout_time: NX_FLOAT {units=NX_TIME}
Time it takes to read the detector (typically milliseconds). This is important to know for time resolved experiments.trigger_delay_time: NX_FLOAT {units=NX_TIME}
Time it takes to start exposure after a trigger signal has been received. This is important to know for time resolved experiments.trigger_dead_time: NX_FLOAT {units=NX_TIME}
Time during which no new trigger signal can be accepted. Typically this is the trigger_delay_time + exposure_time + readout_time. This is important to know for time resolved experiments.frame_time[NP]: NX_FLOAT {units=NX_TIME}
This is time for each frame. This is exposure_time + readout time.gain_setting: NX_CHAR
The gain setting of the detector. This influences background etc.
Any of these values: high | standard | fast | auto
saturation_value: NX_INT
The value at which the detector goes into saturation. Especially common to CCD detectors, the data is known to be invalid above this value.number_of_cycles: NX_INT
CCD images are sometimes constructed by summing together multiple short exposures in the electronics. This reduces background etc. This is the number of short exposures used to sum images for an image.sensor_material: NX_CHAR
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.sensor_thickness: NX_FLOAT {units=NX_LENGTH}
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 thickness of this converter material.threshold_energy: NX_FLOAT {units=NX_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.(geometry): NXgeometry
Position and orientation of detectorefficiency: NXdata
Spectral efficiency of detector with respect to e.g. wavelength
efficiency[i, j, k]: NX_FLOAT {units=NX_DIMENSIONLESS}
efficiency of the detectorwavelength[i, j, k]: NX_FLOAT {units=NX_WAVELENGTH}
TODO: need documentationstart_time[np]: NX_FLOAT {units=NX_TIME}
start time for each frame, with the start attribute as absolute reference
@start: NX_DATE_TIME
stop_time[np]: NX_FLOAT {units=NX_TIME}
stop time for each frame, with the start attribute as absolute reference
@start: NX_DATE_TIME
real_time[i, j, k]: NX_NUMBER {units=NX_TIME}
real-time of the exposure (use this if exposure time varies for each array element, otherwise use count_time field)calibration_method: NXnote
summary of conversion of array data to pixels (e.g. polynomial approximations) and location of details of the calibrationsdata_file: NXnote
(characterization): NXcharacterization
deprecated, use NXcollection instead
for more details, see https://github.com/nexusformat/definitions/issues/177
(collection): NXcollection
Use this group to provide other data related to this NXdetector group.(detector_module): NXdetector_module
For use in special cases where the data in NXdetector is represented in several parts, each with a separate geometry.
Use one or more instances of the NXdetector_module group to declare regions of interest or some other subdivision of a detector.