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Table of contents
There are seven workflow algorithms supporting data reduction at ILL’s time-of-flight instruments. These algorithms are:
The algorithms can be used as flexible building blocks in Python scripts. Not all of them need to be necessarily used in a reduction: the simplest script could call DirectILLCollectData v1 and DirectILLReduction v1 only.
Together with the other algorithms and services provided by the Mantid framework, the reduction algorithms can handle a great number of reduction scenarios. If this proves insufficient, however, the algorithms can be accessed using Python. Before making modifications it is recommended to copy the source files and rename the algorithms as not to break the original behavior.
Additionally, there is an algorithm that streamlines the reduction process, which is the recommended way of performing the reduction:
The DirectILLAutoProcess v1 algorithm calls and properly connects inputs for the algorithms specified above to provide a simplified interface for standard reductions. The number of possible workflows is necessarily more limited than when calls to intermediate algorithms are made individually and from a user-defined script. The individual algorithms should be used only in case when the order of corrections needs changing or any other custom modifications to the standard workflow in the DirectILLAutoProcess v1 are necessary.
This document tries to give an overview on how the algorithms work together via Python examples. Please refer to the algorithm documentation for details of each individual algorithm.
Some algorithm properties have the word ‘AUTO’ in their default value. This means that the default will be chosen according to the instrument by reading the actual default from the instrument parameters. The documentation of the algorithms which have these types of properties includes tables showing the defaults for supported ILL instruments.
Note
To run these usage examples please first download the usage data, and add these to your path. In Mantid this is done using Manage User Directories.
A very basic reduction would include a vanadium reference and a sample and follow the steps:
On instruments like IN4 and IN6, these steps would translate to something like the following simple Python script:
# Uncomment to add a temporary data search directory.
#mantid.config.appendDataSearchDir('/data/')
# Vanadium
DirectILLCollectData(
Run='ILL/IN4/085801-085802.nxs',
OutputWorkspace='vanadium',
OutputEPPWorkspace='vanadium-epps', # Elastic peak positions.
OutputRawWorkspace='vanadium-raw' # 'Raw' data for diagnostics.
)
DirectILLIntegrateVanadium(
InputWorkspace='vanadium',
OutputWorkspace='integrated',
EPPWorkspace='vanadium-epps'
)
DirectILLDiagnostics(
InputWorkspace='vanadium-raw',
OutputWorkspace='diagnostics',
EPPWorkspace='vanadium-epps',
)
# Sample
DirectILLCollectData(
Run='ILL/IN4/087294+087295.nxs',
OutputWorkspace='sample'
)
DirectILLReduction(
InputWorkspace='sample',
OutputWorkspace='SofQW',
IntegratedVanadiumWorkspace='integrated',
DiagnosticsWorkspace='diagnostics'
)
SofQW = mtd['SofQW']
qAxis = SofQW.readX(0) # Vertical axis
eAxis = SofQW.getAxis(1) # Horizontal axis
print('S(Q,W): Q range: {:.3}...{:.3}A; W range {:.3}...{:.3}meV'.format(
qAxis[0], qAxis[-1], eAxis.getMin(), eAxis.getMax()))
Output:
S(Q,W): Q range: 0.0...9.21A; W range -97.0...7.62meV
The basic reduction for IN5 and PANTHER differs slightly with regards to the diagnostics step. In this case, the “raw” workspace is not needed, and it is not necessary to pass the EPP workspace to DirectILLDiagnostics v1:
# Uncomment to add a temporary data search directory.
#mantid.config.appendDataSearchDir('/data/')
# Vanadium
DirectILLCollectData(
Run='085801-085802',
OutputWorkspace='vanadium',
OutputEPPWorkspace='vanadium-epps', # Elastic peak positions.
)
DirectILLIntegrateVanadium(
InputWorkspace='vanadium',
OutputWorkspace='integrated',
EPPWorkspace='vanadium-epps'
)
DirectILLDiagnostics(
InputWorkspace='vanadium',
OutputWorkspace='diagnostics',
)
# Sample
DirectILLCollectData(
Run='087294+087295',
OutputWorkspace='sample'
)
DirectILLReduction(
InputWorkspace='sample',
OutputWorkspace='SofQW',
IntegratedVanadiumWorkspace='integrated',
DiagnosticsWorkspace='diagnostics'
)
The same effect can be achieved by calling the DirectILLAutoProcess v1 algorithm, and the syntax is the same regardless of the instrument:
# Vanadium
DirectILLAutoProcess(
Runs='085801-085802',
OutputWorkspace='vanadium',
ProcessAs='Vanadium',
ClearCache=True
)
# Sample
DirectILLAutoProcess(
Runs='087294+087295',
OutputWorkspace='sample',
ProcessAs='Sample',
VanadiumWorkspace='vanadium',
ClearCache=True
)
Every DirectILL algorithm has an OutputWorkspace property which provides the main output workspace. Additionally, the algorithms may provide optional output workspaces to be used with other algorithms or for reporting/debugging purposes. The linking of outputs to inputs is an important feature of the DirectILL algorithms and allows for great flexibility in the reduction. An example of the usage of these optional output workspaces is the OutputEPPWorkspace which in the vanadium case above is needed in the integration and diagnostics steps:
...
DirectILLCollectData(
...
OutputEPPWorkspace='epps' # This workspace...
)
DirectILLIntegrateVanadium(
...
EPPWorkspace='epps' # ...is needed here...
)
DirectILLDiagnostics(
...
EPPWorkspace='epps' # ...and here.
)
...
As shown above, these optional outputs are sometimes named similarly the corresponding inputs giving a hint were they are supposed to be used.
The information regarding which numors were loaded by relevant NeXus data loaders to create the current workspace is available in the sample logs under the entry run_list.
In the case of DirectILLAutoProcess v1 the connection of outputs and inputs of the workflow is handled by the algorithm internally.
The flat background subtraction in DirectILLCollectData v1 does not work properly for instruments such as IN5. Another algorithm, DirectILLTubeBackground v1 should be used instead. For this algorithm, one should run DirectILLDiagnostics v1 to utilize the default hard mask and beam stop masking in the background determination.
# Add a temporary data search directory.
mantid.config.appendDataSearchDir('/data/')
# Vanadium
DirectILLCollectData(
Run='0100-0109',
OutputWorkspace='vanadium',
OutputEPPWorkspace='vanadium-epps', # Elastic peak positions.
)
DirectILLDiagnostics(
InputWorkspace='vanadium-raw',
OutputWorkspace='diagnostics',
)
# Determine time-independent background
DirectILLTubeBackground(
InputWorkspace='vanadium',
OutputWorkspace='vanadium-background'
EPPWorkspace='vanadiums-epps',
DiagnosticsWorkspace='diagnostics'
)
# Subtract the background
Subtract(
LHSWorkspace='vanadium'
RHSWorkspace='vanadium-background',
OutputWorkspace='vanadium-bkgsubtr'
)
DirectILLIntegrateVanadium(
InputWorkspace='vanadium-bkgsubtr', # Integrate background subtracted data
OutputWorkspace='integrated',
EPPWorkspace='vanadium-epps'
)
# Sample
DirectILLCollectData(
Run='0201+0205+0209-0210',
OutputWorkspace='sample',
OutputEPPWorkspace='sample-epps'
)
# Determine time-independent background
DirectILLTubeBackground(
InputWorkspace='sample',
OutputWorkspace='sample-background',
EPPWorkspace='sample-epps',
DiagnosticsWorkspace='diagnostics'
)
Subtract(
LHSWorkspace='sample',
RHSWorkspace='sample-background',
OutputWorkspace='sample-bkgsubtr'
)
DirectILLReduction(
InputWorkspace='sample-bkgsubtr',
OutputWorkspace='SofQW',
IntegratedVanadiumWorkspace='integrated'
DiagnosticsWorkspace='diagnostics'
)
A more complete reduction example would include corrections for self-shielding:
The above workflow would translate to this kind of Python script for IN4 and IN6:
# Uncomment to add a temporary data search directory.
#mantid.config.appendDataSearchDir('/data/')
# Vanadium
DirectILLCollectData(
Run='ILL/IN4/085801-085801.nxs',
OutputWorkspace='vanadium',
OutputEPPWorkspace='vanadium-epps', # Elastic peak positions.
OutputRawWorkspace='vanadium-raw' # 'Raw' data for diagnostics.
)
DirectILLIntegrateVanadium(
InputWorkspace='vanadium',
OutputWorkspace='integrated',
EPPWorkspace='vanadium-epps'
)
DirectILLDiagnostics(
InputWorkspace='vanadium-raw', # For IN5/PANTHER, 'vanadium' could be used
OutputWorkspace='diagnostics',
EPPWorkspace='vanadium-epps', # Can be omitted for IN5/PANTHER
)
# Sample
DirectILLCollectData(
Run='ILL/IN4/087294+087295.nxs',
OutputWorkspace='sample',
)
geometry = {
'Shape': 'FlatPlate',
'Width': 4.0,
'Height': 5.0,
'Thick': 0.1,
'Center': [0.0, 0.0, 0.0],
'Angle': 45.0
}
material = {
'ChemicalFormula': 'Cd S',
'SampleNumberDensity': 0.01
}
SetSample(
InputWorkspace='sample',
Geometry=geometry,
Material=material
)
DirectILLSelfShielding(
InputWorkspace='sample',
OutputWorkspace='corrections',
EventsPerPoint=10000
)
DirectILLApplySelfShielding(
InputWorkspace='sample',
OutputWorkspace='sample-corrected',
SelfShieldingCorrectionWorkspace='corrections',
)
DirectILLReduction(
InputWorkspace='sample-corrected',
OutputWorkspace='SofQW',
IntegratedVanadiumWorkspace='integrated',
DiagnosticsWorkspace='diagnostics'
)
SofQW = mtd['SofQW']
qAxis = SofQW.readX(0) # Vertical axis
eAxis = SofQW.getAxis(1) # Horizontal axis
print('S(Q,W): Q range: {:.3}...{:.3}A; W range {:.3}...{:.3}meV'.format(
qAxis[0], qAxis[-1], eAxis.getMin(), eAxis.getMax()))
Output:
S(Q,W): Q range: 0.0...9.21A; W range -97.0...7.62meV
In the case of DirectILLAutoProcess v1, the self-attenuation correction is handled internally when the AbsorptionCorrection property is set to either Fast or Full, which denote the granularity of the geometry to be used for calculations. Another property, SelfAbsorptionCorrection allows to choose whether to use Monte Carlo or numerical integration methods. Similarly to the case presented above, at least the geometry and material of the sample need of the provided as input, via SampleMaterial and SampleGeometry properties.
Mantid can be picky with binning when doing arithmetics between workspaces. This is an issue for the time-of-flight instruments at ILL as the time axis needs to be corrected to correspond to a physical flight distance. Even thought data is recorded with the same nominal wavelength, the actual value written in the NeXus files may differ between runs. Incident energy calibration further complicates matters. As the correction to the time-of-flight axis depends on the wavelength, two datasets loaded into Mantid with DirectILLCollectData v1 may have slightly different time-of-flight axis. This prevents arithmetics between the workspaces. The situation is most often encountered between a sample and the corresponding empty container.
To alleviate the situation, the output workspaces of DirectILLCollectData v1 can be forced to use the same wavelength. The following Python script shows how to propagate the calibrated incident energy from the first loaded workspace into the rest:
# Sample
DirectILLCollectData(
Run='ILL/IN4/087294-087295.nxs',
OutputWorkspace='sample',
OutputIncidentEnergyWorkspace='Ei' # Get a common incident energy.
)
# Empty container.
DirectILLCollectData(
Run='ILL/IN4/087306-087309.nxs',
OutputWorkspace='container',
IncidentEnergyWorkspace='Ei' # Ensure same TOF binning.
)
x_sample = mtd['sample'].readX(0)
x_container = mtd['container'].readX(0)
print("Sample's TOF axis starts at {:.4}mus, container's at {:.4}mus".format(
x_sample[0], x_container[0]))
Output:
Sample's TOF axis starts at 965.4mus, container's at 965.7mus
The container subtraction is done perhaps a bit counterintuitively in DirectILLApplySelfShielding v1. At the moment the self-shielding corrections and the empty container data do not have much to do with each other but this may change in the future if the so called Paalman-Pings corrections are used.
With empty container data, the steps to reduce the experimental data might look like this:
A corresponding Python script follows.
# Uncomment to add a temporary data search directory.
#mantid.config.appendDataSearchDir('/data/')
# Vanadium
DirectILLCollectData(
Run='ILL/IN4/085801-085802.nxs',
OutputWorkspace='vanadium',
OutputEPPWorkspace='vanadium-epps',
OutputRawWorkspace='vanadium-raw' # Can be omitted for IN5/PANTHER
)
DirectILLIntegrateVanadium(
InputWorkspace='vanadium',
OutputWorkspace='integrated',
EPPWorkspace='vanadium-epps'
)
DirectILLDiagnostics(
InputWorkspace='vanadium-raw', # IN5/PANTHER can use 'vanadium'
OutputWorkspace='diagnostics',
EPPWorkspace='vanadium-epps', # Can be omitted for IN5/PANTHER
)
# Sample
DirectILLCollectData(
Run='ILL/IN4/087294+087295.nxs',
OutputWorkspace='sample',
OutputIncidentEnergyWorkspace='Ei' # For empty container
)
# Container
DirectILLCollectData(
Run='ILL/IN4/087306-087309.nxs',
OutputWorkspace='container',
IncidentEnergyWorkspace='Ei' # Ensure common TOF axis
)
# Sample self-shielding and container subtraction.
geometry = {
'Shape': 'HollowCylinder',
'Height': 4.0,
'InnerRadius': 1.9,
'OuterRadius': 2.0,
'Center': [0.0, 0.0, 0.0]
}
material = {
'ChemicalFormula': 'Cd S',
'SampleNumberDensity': 0.01
}
SetSample('sample', geometry, material)
DirectILLSelfShielding(
InputWorkspace='sample',
OutputWorkspace='sample-corrections',
EventsPerPoint=10000
)
DirectILLApplySelfShielding(
InputWorkspace='sample',
OutputWorkspace='sample-corrected',
SelfShieldingCorrectionWorkspace='sample-corrections',
EmptyContainerWorkspace='container' # Also subtract container
)
DirectILLReduction(
InputWorkspace='sample-corrected',
OutputWorkspace='SofQW',
IntegratedVanadiumWorkspace='integrated',
DiagnosticsWorkspace='diagnostics'
)
SofQW = mtd['SofQW']
qAxis = SofQW.readX(0) # Vertical axis
eAxis = SofQW.getAxis(1) # Horizontal axis
print('S(Q,W): Q range: {:.3}...{:.3}A; W range {:.3}...{:.3}meV'.format(
qAxis[0], qAxis[-1], eAxis.getMin(), eAxis.getMax()))
Output:
S(Q,W): Q range: 0.0...9.21A; W range -97.0...7.62meV
Container subtraction is handled internally by the DirectILLAutoProcess v1 algorithm, provided the X-axis binning is compatible between the current sample and the empty container workspace. For the correction to be taken into account, the EmptyContainerWorkspace needs to be pointed to the empty container workspace.
Sometimes the empty container is not measured at all the experiment’s temperature points. One can use Mantid’s workspace arithmetics to perform simple linear interpolation in temperature:
import numpy
DirectILLCollectData(
Run='ILL/IN4/087283-087290.nxs',
OutputWorkspace='sample_50K',
OutputIncidentEnergyWorkspace='E_i'
)
DirectILLCollectData(
Run='ILL/IN4/087306-087309.nxs',
OutputWorkspace='container_1.5K',
IncidentEnergyWorkspace='E_i'
)
DirectILLCollectData(
Run='ILL/IN4/087311-087314.nxs',
OutputWorkspace='container_100K',
IncidentEnergyWorkspace='E_i'
)
# Container measurement temperatures.
T0 = 1.5
T1 = 100.0
DT = T1 - T0
# Target sample temperature.
Ts = 50.0
# Linear interpolation.
RebinToWorkspace(
WorkspaceToRebin='container_100K',
WorkspaceToMatch='container_1.5K',
OutputWorkspace='container_100K_rebinned1p5K'
)
container_50K = (T1 - Ts) / DT * mtd['container_1.5K'] + (Ts - T0) / DT * mtd['container_100K_rebinned1p5K']
T_sample_logs = container_50K.run().getProperty('sample.temperature').value
mean_T = numpy.mean(T_sample_logs)
print('Note, that the mean temperature from the sample logs is {:.4}K, a bit off.'.format(mean_T))
Output:
Note, that the mean temperature from the sample logs is 51.0K, a bit off.
As usual, care should be taken when extrapolating the container data outside the measured range.
The reduction algorithms do not produce much output to Mantid logs by default. Also, none of the intermediate workspaces generated during the run of the DirectILL algorithms will show up in the analysis data service. Both behaviors can be controlled by the SubalgorithmLogging and Cleanup properties. Enabling SubalgorithmLogging will log all messages from child algorithms to Mantid’s logs. Disabling Cleanup will unhide the intermediate workspaces created during the algorithm run and disable their deletion.
Note, that disabling Cleanup might produce a large number of workspaces and cause the computer to run out of memory.
The intensities of individual pixels on position sensitive detectors are very low. This makes the fitting procedure employed by FindEPP v2 to work unreliably or fail altogether. Because of this, DirectILLCollectData v1 will use CreateEPP v1 instead by default for IN5 and PANTHER. CreateEPP v1 produces an artificial EPP workspace based on the instrument geometry. This should be accurate enough for vanadium integration and diagnostics.
The elastic peak and background diagnostics are turned off by default for IN5 and PANTHER as it makes no sense to mask individual pixels based on them.
When working on memory constrained systems, it is recommended to manually delete the workspaces which are not needed anymore in the reduction script. The SaveNexus v1 can be used to save the data to disk.
Lets put it all together into a complex Python script. The script below reduces the following dataset:
# Uncomment to add a temporary data search directory.
#mantid.config.appendDataSearchDir('/data/')
# Vanadium
DirectILLCollectData(
Run='ILL/IN4/085801-085802.nxs',
OutputWorkspace='vanadium',
OutputEPPWorkspace='vanadium-epps',
OutputRawWorkspace='vanadium-raw' # Can be omitted for IN5/PANTHER
)
DirectILLIntegrateVanadium(
InputWorkspace='vanadium',
OutputWorkspace='integrated',
EPPWorkspace='vanadium-epps'
)
DirectILLDiagnostics(
InputWorkspace='vanadium-raw', # IN5/PANTHER can use 'vanadium'
OutputWorkspace='diagnostics',
EPPWorkspace='vanadium-epps', # Can be omitted for IN5/PANTHER
)
# Samples
DirectILLCollectData(
Run='ILL/IN4/087294+087295.nxs',
OutputWorkspace='sample_1.5K',
OutputIncidentEnergyWorkspace='Ei', # For other datasets
OutputFlatBkgWorkspace='bkgs' # For sample at 50K
)
DirectILLCollectData(
Run='ILL/IN4/087283-087290.nxs',
OutputWorkspace='sample_50K',
IncidentEnergyWorkspace='Ei', # Ensure common TOF axis
FlatBkgWorkspace='bkgs' # Use flat backgrounds from 1.5K
)
# Containers
DirectILLCollectData(
Run='ILL/IN4/087306-087309.nxs',
OutputWorkspace='container_1.5K',
IncidentEnergyWorkspace='Ei' # Ensure common TOF axis
)
DirectILLCollectData(
Run='ILL/IN4/087311-087314.nxs',
OutputWorkspace='container_100K',
IncidentEnergyWorkspace='Ei' # Ensure common TOF axis
)
# Sample self-shielding and container subtraction.
geometry = {
'Shape': 'HollowCylinder',
'Height': 4.0,
'InnerRadius': 1.9,
'OuterRadius': 2.0,
'Center': [0.0, 0.0, 0.0]
}
material = {
'ChemicalFormula': 'Cd S',
'SampleNumberDensity': 0.01
}
SetSample('sample_1.5K', geometry, material)
SetSample('sample_50K', geometry, material)
# Self-shielding corrections need to be calculated only once.
DirectILLSelfShielding(
InputWorkspace='sample_1.5K',
OutputWorkspace='corrections',
EventsPerPoint=10000
)
DirectILLApplySelfShielding(
InputWorkspace='sample_1.5K',
OutputWorkspace='corrected_1.5K',
SelfShieldingCorrectionWorkspace='corrections',
EmptyContainerWorkspace='container_1.5K'
)
# Need to interpolate container to 50K
T0 = 1.5
T1 = 100.0
DT = T1 - T0
Ts = 50.0 # Target T
RebinToWorkspace(
WorkspaceToRebin='container_100K',
WorkspaceToMatch='container_1.5K',
OutputWorkspace='container_100K_rebinned1p5K'
)
container_50K = (T1 - Ts) / DT * mtd['container_1.5K'] + (Ts - T0) / DT * mtd['container_100K_rebinned1p5K']
DirectILLApplySelfShielding(
InputWorkspace='sample_50K',
OutputWorkspace='corrected_50K',
SelfShieldingCorrectionWorkspace='corrections',
EmptyContainerWorkspace=container_50K
)
DirectILLReduction(
InputWorkspace='corrected_1.5K',
OutputWorkspace='SofQW_1.5K',
IntegratedVanadiumWorkspace='integrated',
DiagnosticsWorkspace='diagnostics'
)
DirectILLReduction(
InputWorkspace='corrected_50K',
OutputWorkspace='SofQW_50K',
IntegratedVanadiumWorkspace='integrated',
DiagnosticsWorkspace='diagnostics'
)
outputs = ['SofQW_1.5K', 'SofQW_50K']
for output in outputs:
SofQW = mtd[output]
qAxis = SofQW.readX(0) # Vertical axis
eAxis = SofQW.getAxis(1) # Horizontal axis
print('{}: Q range: {:.3}...{:.3}A; W range {:.3}...{:.3}meV'.format(
output, qAxis[0], qAxis[-1], eAxis.getMin(), eAxis.getMax()))
Output:
SofQW_1.5K: Q range: 0.0...9.21A; W range -97.0...7.62meV
SofQW_50K: Q range: 0.0...9.19A; W range -96.6...7.62meV
And the same reduction, but with the use of the DirectILLAutoProcess v1:
vanadium_runs = '085801-085802'
sample_runs = '087294+087295,087283-087290'
container_runs = '087306-087309,087311-087314'
vanadium_ws = 'vanadium_auto'
container_ws = 'container'
sample_ws = 'sample'
# Sample self-shielding and container subtraction.
geometry = {
'Shape': 'HollowCylinder',
'Height': 4.0,
'InnerRadius': 1.9,
'OuterRadius': 2.0,
'Center': [0.0, 0.0, 0.0]
}
material = {
'ChemicalFormula': 'Cd S',
'SampleNumberDensity': 0.01
}
Ei = 8.804337831263577
DirectILLAutoProcess(
Runs=vanadium_runs,
OutputWorkspace=vanadium_ws,
ProcessAs='Vanadium',
ReductionType='Powder',
FlatBkg = 'Flat Bkg ON',
ElasticChannel='Elastic Channel AUTO',
EPPCreationMethod='Fit EPP'
)
DirectILLAutoProcess(
Runs=container_runs,
OutputWorkspace=container_ws,
ProcessAs='Empty',
ReductionType='Powder',
IncidentEnergyCalibration="Energy Calibration ON",
IncidentEnergy=Ei
)
# Need to interpolate container to 50K
T0 = 1.5
T1 = 100.0
DT = T1 - T0
Ts = 50.0 # Target T
RebinToWorkspace(
WorkspaceToRebin='container_087311_Ei9meV_T100.0K',
WorkspaceToMatch='container_087306_Ei9meV_T1.5K',
OutputWorkspace='container_087311_Ei9meV_T100.0K'
)
container_Ei9meV_50K = (T1 - Ts) / DT * mtd['container_087306_Ei9meV_T1.5K'] + (Ts - T0) / DT * mtd['container_087311_Ei9meV_T100.0K']
mtd[container_ws].add('container_Ei9meV_50K')
DirectILLAutoProcess(
Runs=sample_runs,
OutputWorkspace=sample_ws,
ProcessAs='Sample',
ReductionType='Powder',
VanadiumWorkspace=vanadium_ws,
EmptyContainerWorkspace=container_ws,
IncidentEnergyCalibration="Energy Calibration ON",
IncidentEnergy=Ei,
SampleMaterial=material,
SampleGeometry=geometry,
SaveOutput=False,
ClearCache=True,
)
outputs = ['sample_SofQW_087294_Ei9meV_T1.5K', 'sample_SofQW_087283_Ei9meV_T50.0K']
for output in outputs:
SofQW = mtd[output]
qAxis = SofQW.readX(0) # Vertical axis
eAxis = SofQW.getAxis(1) # Horizontal axis
print('{}: Q range: {:.3}...{:.3}A; W range {:.3}...{:.3}meV'.format(
output, qAxis[0], qAxis[-1], eAxis.getMin(), eAxis.getMax()))
Output:
sample_SofQW_087294_Ei9meV_T1.5K: Q range: 0.0...9.21A; W range -97.0...7.62meV
sample_SofQW_087283_Ei9meV_T50.0K: Q range: 0.0...9.19A; W range -96.6...7.62meV
Category: Techniques