\(\renewcommand\AA{\unicode{x212B}}\)

CylinderAbsorption v1

../_images/CylinderAbsorption-v1_dlg.png

CylinderAbsorption dialog.

Summary

Calculates bin-by-bin correction factors for attenuation due to absorption and single scattering in a ‘cylindrical’ sample.

See Also

AbsorptionCorrection

Properties

Name

Direction

Type

Default

Description

InputWorkspace

Input

MatrixWorkspace

Mandatory

The X values for the input workspace must be in units of wavelength

OutputWorkspace

Output

MatrixWorkspace

Mandatory

Output workspace name

ScatterFrom

Input

string

Sample

The component to calculate the absorption for (default: Sample). Allowed values: [‘Sample’, ‘Container’, ‘Environment’]

AttenuationXSection

Input

number

Optional

The ABSORPTION cross-section, at 1.8 Angstroms, for the sample material in barns. Column 8 of a table generated from http://www.ncnr.nist.gov/resources/n-lengths/.

ScatteringXSection

Input

number

Optional

The (coherent + incoherent) scattering cross-section for the sample material in barns. Column 7 of a table generated from http://www.ncnr.nist.gov/resources/n-lengths/.

SampleNumberDensity

Input

number

Optional

The number density of the sample in number of atoms per cubic angstrom if not set with SetSampleMaterial

NumberOfWavelengthPoints

Input

number

Optional

The number of wavelength points for which the numerical integral is calculated (default: all points)

ExpMethod

Input

string

Normal

Select the method to use to calculate exponentials, normal or a fast approximation (default: Normal). Allowed values: [‘Normal’, ‘FastApprox’]

EMode

Input

string

Elastic

The energy mode (default: elastic). Allowed values: [‘Elastic’, ‘Direct’, ‘Indirect’]

EFixed

Input

number

0

The value of the initial or final energy, as appropriate, in meV. Will be taken from the instrument definition file, if available.

CylinderSampleHeight

Input

number

Optional

The height of the cylindrical sample in centimetres

CylinderSampleRadius

Input

number

Optional

The radius of the cylindrical sample in centimetres

CylinderAxis

Input

dbl list

0,1,0

A 3D vector specifying the cylindrical sample’s orientation

NumberOfSlices

Input

number

1

The number of slices into which the cylinder is divided for the calculation

NumberOfAnnuli

Input

number

1

The number of annuli into which each slice is divided for the calculation

Description

This algorithm uses a numerical integration method to calculate attenuation factors resulting from absorption and single scattering in a cylindrical sample with the dimensions and material properties given. Factors are calculated for each spectrum (i.e. detector position) and wavelength point, as defined by the input workspace. The sample is divided up into a stack of slices, which are then divided into annuli (rings). These annuli are further divided (see Ref. [2], Appendix A) to give the full set of elements for which a calculation will be carried out. Thus the calculation speed depends linearly on the total number of bins in the workspace and on the number of slices. The dependence on the number of annuli is stronger, going as \(3n ( n+1 )\).

Path lengths through the sample are then calculated for the centre-point of each element and a numerical integration is carried out using these path lengths over the volume elements.

Assumptions

Although no assumptions are made about the beam direction or the sample position, the cylinder will be constructed with its centre at the sample position and it’s axis along the y axis (which in the case of most instruments is the vertical). The sample geometry can also be set using SetSample.

Restrictions on the input workspace

The input workspace must have units of wavelength. The instrument associated with the workspace must be fully defined because detector, source & sample position are needed.

References

The method used here is based upon work presented in the following two papers, although it does not yet fully implement all aspects discussed there (e.g. there’s no multiple scattering and no concentric cylinders).

  1. I.A. Blech & B.L. Averbach, Multiple Scattering of Neutrons in Vanadium and Copper, Phys. Rev. 137 4A (1965) A1113 doi: 10.1103/PhysRev.137.A1113

  2. A.K. Soper & P.A. Egelstaff, Multiple Scattering and Attenuation of Neutrons in Concentric Cylinders, NIM 178 (1980) 415 doi: 10.1016/0029-554X(80)90820-4

Usage

Example - Using a X Section Values

ws = CreateSampleWorkspace()
ws = ConvertUnits(ws,"Wavelength")

wsOut = CylinderAbsorption(ws, AttenuationXSection=5.08,
    ScatteringXSection=5.1,SampleNumberDensity=0.07192,
    NumberOfWavelengthPoints=5, CylinderSampleHeight=4,
    CylinderSampleRadius=0.4, NumberOfSlices=2, NumberOfAnnuli=2)


print ("The Absorption correction is calculated to match the input workspace")
print ("  over %i bins, ranging from  %.2f to %.2f" %
    (wsOut.blocksize(),
    wsOut.readY(0)[0],
    wsOut.readY(0)[wsOut.blocksize()-1]))

Output:

The Absorption correction is calculated to match the input workspace
  over 100 bins, ranging from  0.77 to 0.37

Example - Using a SetSampleMaterial

ws = CreateSampleWorkspace()
ws = ConvertUnits(ws,"Wavelength")
SetSampleMaterial(ws,ChemicalFormula='Cd')

wsOut = CylinderAbsorption(ws,
    NumberOfWavelengthPoints=5, CylinderSampleHeight=4,
    CylinderSampleRadius=0.4, NumberOfSlices=2, NumberOfAnnuli=2)


print ("The Absorption correction is calculated to match the input workspace")
print ("  over %i bins, ranging from  %.2f to %.2f" %
    (wsOut.blocksize(),
    wsOut.readY(0)[0],
    wsOut.readY(0)[wsOut.blocksize()-1]))

Output:

The Absorption correction is calculated to match the input workspace
  over 100 bins, ranging from  0.25 to 0.00

Categories: AlgorithmIndex | CorrectionFunctions\AbsorptionCorrections

Source

C++ header: CylinderAbsorption.h

C++ source: CylinderAbsorption.cpp