ReflectometryReductionOneAuto v2¶

Summary¶

Reduces a single TOF/Lambda reflectometry run into a mod Q vs I/I0 workspace attempting to pick instrument parameters for missing properties

Properties¶

Description¶

This algorithm is a facade over ReflectometryReductionOne v2 (see ReflectometryReductionOne v2 for more information on the wrapped algorithm). It optionally corrects the detector position and then pulls numeric parameters out of the instrument parameter file where possible. These automatically applied defaults can be overriden by providing your own values. In addition, it outputs a rebinned workspace in Q, and it optionally performs polarization analysis if the input workspace is a workspace group.

First, if ThetaIn is given the algorithm will try to correct the detector position. For this, it uses ProcessingInstructions, which corresponds to the grouping pattern of workspace indices that define the detectors of interest. Only the detectors of interest will be corrected, the rest of the instrument components will remain in the original position. Note that when ProcessingInstructions is not set, its value is inferred from other properties, depending on the value of AnalysisMode:

• If AnalysisMode = PointDetectorAnalaysis the algorithm will search for PointDetectorStart and PointDetectorStop in the parameter file, and ProcessingInstructions will be set to PointDetectorStart:PointDetectorEnd.
• If AnalysisMode = MultiDetectorAnalaysis the algorithm will search for MultiDetectorStart in the parameter file and all of the spectra from this value onwards will be used.

Note that ProcessingInstructions are workspace indices, not detector IDs. The first few workspaces may correspond to monitors, rather than detectors of interest. For the syntax of this property, see GroupDetectors v2.

Once the algorithm determines the detectors of interest it corrects their positions according to ThetaIn, if given, for which it runs SpecularReflectionPositionCorrect v2. The detectors are moved either by shifting them vertically, or by rotating them around the sample position, as specified by DetectorCorrectionType. If ThetaIn is not set, detectors will not be corrected. However, it is recommended to use this option to ensure that ReflectometryReductionOne v2 is able to convert from wavelength to momentum transfer properly.

Next, the algorithm will try to populate input properties which have not been set. Specifically, it will search for LambdaMin, LambdaMax, I0MonitorIndex, MonitorBackgroundMin, MonitorBackgroundMax, MonitorIntegralMin and MonitorIntegralMin in the parameter file to populate WavelengthMin, WavelengthMax, I0MonitorIndex, MonitorBackgroundWavelengthMin, MonitorBackgroundWavelengthMax, MonitorIntegrationWavelengthMin and MonitorIntegrationWavelengthMax respectively. The first two properties will be used by ReflectometryReductionOne v2 to crop the workspace in wavelength, whereas the rest of the properties refer to monitors and are used to create a temporary monitor workspace by which the detectors of interest will be normalized. Note that there is an additional property referring to monitors, NormalizeByIntegratedMonitors, which can be used to specify whether or not integrated monitors should be considered.

The rest of the input properties are not inferred from the parameter file, and must be specified manually. RegionOfDirectBeam is an optional property that allows users to specify a region of direct beam that will be used to normalize the detector signal. The region of direct beam is specified by workspace indices. For instance, RegionOfDirectBeam='2-3' means that spectra with workspace indices 2 and 3 will be summed and the resulting workspace will be used as the direct beam workspace.

Transmission corrections can be optionally applied by providing either one or two transmission runs or polynomial corrections. Polynomial correction is enabled by setting the CorrectionAlgorithm property. If set to AutoDetect, the algorithm looks at the instrument parameters for the correction parameter. If this parameter is set to polynomial, then polynomial correction is performed using the PolynomialCorrection v1 algorithm, with the polynomial string taken from the instrument’s polystring parameter. If the correction parameter is set to exponential instead, then the ExponentialCorrection v1 algorithm is used, with C0 and C1 taken from the instrument parameters, C0 and C1. All these values can be specified manually by setting the CorrectionAlgorithm to either PolynomialCorrection or ExponentialCorrection and setting Polynomial or C0 and C1 properties accordingly. Note that when using a correction algorithm, monitors will not be integrated, even if NormalizeByIntegratedMonitors was set to true.

Finally, properties MomentumTransferMin, MomentumTransferStep and MomentumTransferMax are used to rebin the output workspace in Q, and ScaleFactor is used to scale the rebinned workspace. When they are not provided the algorithm will attempt to determine the bin width using CalculateResolution v1 (note that, for the latter to run successfully, a slit component with a vertical gap must be defined in the instrument definition file).

See ReflectometryReductionOne v2 for more information on how the input properties are used by the wrapped algorithm.

Workspace Groups¶

If a workspace group is provided as input, each workspace in the group will be reduced independently and sequentially using ReflectometryReductionOne v2. Each of these individual reductions will produce three output workspaces: an output workspace in wavelength, an output workspace in Q with native binning, and a rebinned workspace in Q. Output workspaces in wavelength will be grouped together to produce an output workspace group in wavelength, and output workspaces in Q will be grouped together to produce an output workspace group in Q. The diagram below illustrates this process (note that, for the sake of clarity, the rebinned output workspace in Q, OutputWorkspaceBinned, is not represented but it is handled analogously to OutputWorkspace and OutputWorkspaceWavelength):

Polarization Analysis Off¶

If PolarizationAnalysis = None the reduction stops here. Note that if transmission runs are given in the form of a workspace group, each member in the transmission group will be associated to the corresponding member in the input workspace group, i.e., the first item in the transmission group will be used as the transmission run for the first workspace in the input workspace group, the second element in the transmission group will be used as the transmission run for the second workspace in the input workspace group, etc. This is also illustrated in the diagram above, where [0] represents the first element in a workspace group, [1] the second element, etc. If transmission runs are provided as matrix workspaces the specified runs will be used for all members of the input workspace group.

Polarization Analysis On¶

If PolarizationAnalysis is set to PA or PNR the reduction continues and polarization corrections will be applied to the output workspace in wavelength. The algorithm will use the properties PolarizationAnalysis, CPp, CAp, CRho and CAlpha to run PolarizationCorrection v1. The result will be a new workspace in wavelength, which will override the previous one, that will be used as input to ReflectometryReductionOne v2 to calculate the new output workspaces in Q, which in turn will override the existing workspaces in Q. Note that if transmission runs are provided in the form of workspace groups, the individual workspaces will be summed to produce a matrix workspace that will be used as the transmission run for all items in the input workspace group, as illustrated in the diagram below (note that, for the sake of clarity, the rebinned output workspace in Q, OutputWorkspaceBinned, is not represented but it is handled analogously to OutputWorkspace).

Previous Versions¶

This is version 2 of the algorithm. For version 1, please see here.

Usage¶

Example - Basic reduction with no transmission run, polynomial corrections will be automatically applied

run = Load(Filename='INTER00013460.nxs')
IvsQ, IvsQ_unbinned, IvsLam = ReflectometryReductionOneAuto(InputWorkspace=run, ThetaIn=0.7)

print "%.5f" % (IvsLam.readY(0)[175])
print "%.5f" % (IvsLam.readY(0)[176])
print "%.5f" % (IvsQ_unbinned.readY(0)[106])
print "%.5f" % (IvsQ_unbinned.readY(0)[107])
print "%.5f" % (IvsQ.readY(0)[13])
print "%.5f" % (IvsQ.readY(0)[14])

Output:

0.00441
0.00462
0.63441
0.41079
0.44780
0.23690

Example - Basic reduction with a transmission run

run = Load(Filename='INTER00013460.nxs')
trans = Load(Filename='INTER00013463.nxs')
IvsQ, IvsQ_unbinned, IvsLam = ReflectometryReductionOneAuto(InputWorkspace=run, FirstTransmissionRun=trans, ThetaIn=0.7)

print "%.5f" % (IvsLam.readY(0)[164])
print "%.5f" % (IvsLam.readY(0)[164])
print "%.5f" % (IvsQ_unbinned.readY(0)[96])
print "%.5f" % (IvsQ_unbinned.readY(0)[97])
print "%.5f" % (IvsQ.readY(0)[5])
print "%.5f" % (IvsQ.readY(0)[6])

Output:

0.00338
0.00338
1.16756
0.89144
1.46645
1.41351

Example - Reduction overriding some default values

run = Load(Filename='INTER00013460.nxs')
IvsQ, IvsQ_unbinned, IvsLam = ReflectometryReductionOneAuto(InputWorkspace=run, ThetaIn=0.7, DetectorCorrectionType="RotateAroundSample", MonitorBackgroundWavelengthMin=0.0, MonitorBackgroundWavelengthMax=1.0)

print "%.5f" % (IvsLam.readY(0)[175])
print "%.5f" % (IvsLam.readY(0)[176])
print "%.5f" % (IvsQ_unbinned.readY(0)[106])
print "%.5f" % (IvsQ_unbinned.readY(0)[107])
print "%.5f" % (IvsQ.readY(0)[5])
print "%.5f" % (IvsQ.readY(0)[6])

Output:

0.00441
0.00462
0.64241
0.41453
0.51028
0.52241

Categories: Algorithms | Reflectometry\ISIS

Source¶

C++ source: ReflectometryReductionOneAuto2.cpp

C++ header: ReflectometryReductionOneAuto2.h