Difference between revisions of "Temp"
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A quick reference for the various profile type 3 and 4 terms is given below. Users are ''strongly'' encouraged to read this section of the GSAS manual at least once before (or after) blindly using this guide! | A quick reference for the various profile type 3 and 4 terms is given below. Users are ''strongly'' encouraged to read this section of the GSAS manual at least once before (or after) blindly using this guide! | ||
==Pseudo-Voigt Profile Functions== | == Pseudo-Voigt Profile Functions== | ||
These peak profile functions are a [http://en.wikipedia.org/wiki/Voigt_profile pseudo-Voigt] type, combining Gaussian (G) and Lorentzian (L) components. | These peak profile functions are a [http://en.wikipedia.org/wiki/Voigt_profile pseudo-Voigt] type, combining Gaussian (G) and Lorentzian (L) components. | ||
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The Lorentzian shape is more complex (check the manual), but includes size and strain broadening terms. | The Lorentzian shape is more complex (check the manual), but includes size and strain broadening terms. | ||
==Asymmetry, Zero-Shift and Related Terms== | == Asymmetry, Zero-Shift and Related Terms== | ||
[http://youtu.be/SIz6Ng6UzAw Axial Divergence] (i.e. low angle peak asymmetry) is modeled in GSAS profile types 3 & 4 with the Finger-Cox-Jephcoat model (see GSAS manual). The profile terms ''S/L'' & ''H/L'' describe the ''instrumental'' asymmetry. Most users of 11-BM will not need to refine these terms. | [http://youtu.be/SIz6Ng6UzAw Axial Divergence] (i.e. low angle peak asymmetry) is modeled in GSAS profile types 3 & 4 with the Finger-Cox-Jephcoat model (see GSAS manual). The profile terms ''S/L'' & ''H/L'' describe the ''instrumental'' asymmetry. Most users of 11-BM will not need to refine these terms. | ||
===Sample Transparency=== (''trns'' profile term) | === Sample Transparency=== (''trns'' profile term) | ||
===Sample Transparency=== (''trns'' profile term) | === Sample Transparency=== (''trns'' profile term) | ||
=== Headline text === | === Headline text === |
Revision as of 05:24, 2 May 2012
GSAS offers 5 different Constant Wavelength (CW) X-ray profile functions. They are described in detail within the GSAS technical manual (see page 156). 11-BM users are encouraged to use either profile type 3 or type 4.
A quick reference for the various profile type 3 and 4 terms is given below. Users are strongly encouraged to read this section of the GSAS manual at least once before (or after) blindly using this guide!
Pseudo-Voigt Profile Functions
These peak profile functions are a pseudo-Voigt type, combining Gaussian (G) and Lorentzian (L) components.
The general Gaussian shape (as a function of angle θ) is described by the Cagliotti function
Gaussian Profile ≈ U*tan2θ + V*tanθ + W + P/cos2θ
These U, V, W, and P variables match the GU, GV, GW, and GP profile terms you see below.
The Lorentzian shape is more complex (check the manual), but includes size and strain broadening terms.
Asymmetry, Zero-Shift and Related Terms
Axial Divergence (i.e. low angle peak asymmetry) is modeled in GSAS profile types 3 & 4 with the Finger-Cox-Jephcoat model (see GSAS manual). The profile terms S/L & H/L describe the instrumental asymmetry. Most users of 11-BM will not need to refine these terms.
=== Sample Transparency=== (trns profile term)
=== Sample Transparency=== (trns profile term)
Headline text
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Suggested Profile Types & Terms for Fitting 11-BM Data
11-BM users are encouraged to the GSAS constant wavelength (CW) profile type 3 or type 4. Profile #4 is best for cases in which anisotropic terms are required.
11-BM users will not (usually!) need to change or refine the default 'G' terms given in the instrumental parameter file. For the high-resolution synchrotron powder data collected at 11-BM, the instrumental resolution is well described by Gaussian terms.
On the other hand, sample effects in 11-BM data, such as size and strain broadening are (usually!) best fit and refined using Lorentzian terms. Gaussian sample size broadening is *rarely* observed; this requires a very tight mono-disperse size distribution rarely encountered in powder samples (solid metal samples may be an exception).
Many 11-BM diffraction patterns can then be well fit by refining only the LX (size), LY (strain) and
Type 3
Constant Wavelength X-ray GSAS Profile Type 3
GU = Gaussian U term | GV = Gaussian V term | GW = Gaussian W term |
GP = Gaussian crystallite size broadening | LX = Lorentzian crystallite size broadening | LY = Lorentzian strain broadening |
S/L = Axial Divergence S term | H/L = Axial Divergence H term | trns = Sample 'Transparency' |
shft = Sample 'Displacement' | stec = Lorentzian anisotropic strain broadening ** | ptec = Lorentzian anisotropic crystallite size broadening ** |
sfec = Lorentzian sublattice anisotropic broadening ** | LXX = Anisotropic Lorentzian microstrain ** | LYY = Anisotropic Lorentzian microstrain ** |
- NOTE
Type 4
Constant Wavelength X-ray GSAS Profile Type 4
GU = Gaussian U term | GV = Gaussian V term | GW = Gaussian W term |
GP = Gaussian crystallite size broadening | LX = Lorentzian crystallite size broadening | ptec = anisotropic crystallite size |
trns = Sample 'Transparency' | shft = Sample 'Displacement' | sfec = Lorentzian sublattice anisotropic broadening # |
S/L = Axial Divergence S term | H/L = Axial Divergence H term | eta = mixing factor, from pure Gaussian (0) to pure Lorentzian (1) |
SXXX = Stephens anisotropic microstrain broadening | SYYY = Stephens anisotropic microstrain broadening | SZZZ = Stephens anisotropic microstrain broadening |
- stacking defects (see manual)