source: sasview/src/sas/sasgui/perspectives/fitting/media/sm_help.rst @ d85c194

ESS_GUIESS_GUI_DocsESS_GUI_batch_fittingESS_GUI_bumps_abstractionESS_GUI_iss1116ESS_GUI_iss879ESS_GUI_iss959ESS_GUI_openclESS_GUI_orderingESS_GUI_sync_sascalccostrafo411magnetic_scattrelease-4.1.1release-4.1.2release-4.2.2release_4.0.1ticket-1009ticket-1094-headlessticket-1242-2d-resolutionticket-1243ticket-1249ticket885unittest-saveload
Last change on this file since d85c194 was d85c194, checked in by Piotr Rozyczko <piotr.rozyczko@…>, 8 years ago

Remaining modules refactored

  • Property mode set to 100644
File size: 6.8 KB
RevLine 
[da53353]1.. sm_help.rst
2
3.. This is a port of the original SasView html help file to ReSTructured text
4.. by S King, ISIS, during SasView CodeCamp-III in Feb 2015.
5
6.. |beta| unicode:: U+03B2
7.. |gamma| unicode:: U+03B3
8.. |mu| unicode:: U+03BC
9.. |sigma| unicode:: U+03C3
10.. |phi| unicode:: U+03C6
11.. |theta| unicode:: U+03B8
12.. |chi| unicode:: U+03C7
[f256d9b]13.. |bigdelta| unicode:: U+0394
[da53353]14
15.. |inlineimage004| image:: sm_image004.gif
16.. |inlineimage005| image:: sm_image005.gif
17.. |inlineimage008| image:: sm_image008.gif
18.. |inlineimage009| image:: sm_image009.gif
19.. |inlineimage010| image:: sm_image010.gif
20.. |inlineimage011| image:: sm_image011.gif
21.. |inlineimage012| image:: sm_image012.gif
22.. |inlineimage018| image:: sm_image018.gif
23.. |inlineimage019| image:: sm_image019.gif
24
25
26.. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ
27
[f256d9b]28Smearing Functions
29==================
[da53353]30
[f256d9b]31Sometimes it will be necessary to correct reduced experimental data for the
32physical effects of the instrumental geometry in use. This process is called
33*desmearing*. However, calculated/simulated data - which by definition will be
34perfect/exact - can be *smeared* to make it more representative of what might
35actually be measured experimentally.
36
37SasView provides the following three smearing algorithms:
[da53353]38
[a0637de]39*  *Slit Smearing*
40*  *Pinhole Smearing*
41*  *2D Smearing*
[da53353]42
[a0637de]43.. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ
[da53353]44
45Slit Smearing
[f256d9b]46-------------
47
48**This type of smearing is normally only encountered with data from X-ray Kratky**
49**cameras or X-ray/neutron Bonse-Hart USAXS/USANS instruments.**
[da53353]50
[f256d9b]51The slit-smeared scattering intensity is defined by
[da53353]52
53.. image:: sm_image002.gif
54
[f256d9b]55where *Norm* is given by
[da53353]56
57.. image:: sm_image003.gif
58
[f256d9b]59**[Equation 1]**
[da53353]60
61The functions |inlineimage004| and |inlineimage005|
62refer to the slit width weighting function and the slit height weighting
[f256d9b]63determined at the given *q* point, respectively. It is assumed that the weighting
64function is described by a rectangular function, such that
[da53353]65
66.. image:: sm_image006.gif
67
[f256d9b]68**[Equation 2]**
[da53353]69
70and
71
72.. image:: sm_image007.gif
73
[f256d9b]74**[Equation 3]**
[da53353]75
[f256d9b]76so that |inlineimage008| |inlineimage009| for |inlineimage010| and *u*\ .
[da53353]77
[f256d9b]78Here |inlineimage011| and |inlineimage012| stand for
79the slit height (FWHM/2) and the slit width (FWHM/2) in *q* space.
80
81This simplifies the integral in Equation 1 to
[da53353]82
83.. image:: sm_image013.gif
84
[f256d9b]85**[Equation 4]**
86
87which may be solved numerically, depending on the nature of |inlineimage011| and |inlineimage012| .
[da53353]88
[f256d9b]89Solution 1
90^^^^^^^^^^
[da53353]91
[f256d9b]92**For** |inlineimage012| **= 0 and** |inlineimage011| **= constant.**
[da53353]93
94.. image:: sm_image016.gif
95
[f256d9b]96For discrete *q* values, at the *q* values of the data points and at the *q*
97values extended up to *q*\ :sub:`N`\ = *q*\ :sub:`i` + |inlineimage011| the smeared
98intensity can be approximately calculated as
[da53353]99
100.. image:: sm_image017.gif
101
[f256d9b]102**[Equation 5]**
[da53353]103
[f256d9b]104where |inlineimage018| = 0 for *I*\ :sub:`s` when *j* < *i* or *j* > *N-1*.
[da53353]105
[f256d9b]106Solution 2
107^^^^^^^^^^
[da53353]108
[f256d9b]109**For** |inlineimage012| **= constant and** |inlineimage011| **= 0.**
[da53353]110
[f256d9b]111Similar to Case 1
[da53353]112
[f256d9b]113|inlineimage019| for *q*\ :sub:`p` = *q*\ :sub:`i` - |inlineimage012| and *q*\ :sub:`N` = *q*\ :sub:`i` + |inlineimage012|
[da53353]114
[f256d9b]115**[Equation 6]**
[da53353]116
[f256d9b]117where |inlineimage018| = 0 for *I*\ :sub:`s` when *j* < *p* or *j* > *N-1*.
[da53353]118
[f256d9b]119Solution 3
120^^^^^^^^^^
121
122**For** |inlineimage011| **= constant and** |inlineimage011| **= constant.**
123
124In this case, the best way is to perform the integration of Equation 1
125numerically for both slit height and slit width. However, the numerical
126integration is imperfect unless a large number of iterations, say, at
127least 10000 by 10000 for each element of the matrix *W*, is performed.
128This is usually too slow for routine use.
129
130An alternative approach is used in SasView which assumes
131slit width << slit height. This method combines Solution 1 with the
132numerical integration for the slit width. Then
[da53353]133
134.. image:: sm_image020.gif
135
[f256d9b]136**[Equation 7]**
137
138for *q*\ :sub:`p` = *q*\ :sub:`i` - |inlineimage012| and *q*\ :sub:`N` = *q*\ :sub:`i` + |inlineimage012|
[da53353]139
[f256d9b]140where |inlineimage018| = 0 for *I*\ :sub:`s` when *j* < *p* or *j* > *N-1*.
[da53353]141
[a0637de]142.. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ
[da53353]143
144Pinhole Smearing
[f256d9b]145----------------
[da53353]146
[f256d9b]147**This is the type of smearing normally encountered with data from synchrotron**
148**SAXS cameras and SANS instruments.**
[da53353]149
[f256d9b]150The pinhole smearing computation is performed in a similar fashion to the slit-
151smeared case above except that the weight function used is a Gaussian. Thus
152Equation 6 becomes
[da53353]153
[f256d9b]154.. image:: sm_image021.gif
[da53353]155
[f256d9b]156**[Equation 8]**
[da53353]157
[a0637de]158.. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ
[da53353]159
1602D Smearing
[f256d9b]161-----------
[da53353]162
[f256d9b]163The 2D smearing computation is performed in a similar fashion to the 1D pinhole
164smearing above except that the weight function used is a 2D elliptical Gaussian.
165Thus
[da53353]166
167.. image:: sm_image022.gif
168
[f256d9b]169**[Equation 9]**
[da53353]170
[f256d9b]171In Equation 9, *x*\ :sub:`0` = *q* cos(|theta|), *y*\ :sub:`0` = *q* sin(|theta|), and
172the primed axes, are all in the coordinate rotated by an angle |theta| about
173the z-axis (see the figure below) so that *x'*\ :sub:`0` = *x*\ :sub:`0` cos(|theta|) +
174*y*\ :sub:`0` sin(|theta|) and *y'*\ :sub:`0` = -*x*\ :sub:`0` sin(|theta|) +
175*y*\ :sub:`0` cos(|theta|). Note that the rotation angle is zero for a x-y symmetric
176elliptical Gaussian distribution. The *A* is a normalization factor.
[da53353]177
178.. image:: sm_image023.gif
179
[f256d9b]180Now we consider a numerical integration where each of the bins in |theta| and *R* are
181*evenly* (this is to simplify the equation below) distributed by |bigdelta|\ |theta|
182and |bigdelta|\ R, respectively, and it is further assumed that *I(x',y')* is constant
183within the bins. Then
[da53353]184
185.. image:: sm_image024.gif
186
[f256d9b]187**[Equation 10]**
188
189Since the weighting factor on each of the bins is known, it is convenient to
190transform *x'-y'* back to *x-y* coordinates (by rotating it by -|theta| around the
191*z* axis).
[da53353]192
[f256d9b]193Then, for a polar symmetric smear
[da53353]194
195.. image:: sm_image025.gif
196
[f256d9b]197**[Equation 11]**
[da53353]198
199where
200
201.. image:: sm_image026.gif
202
[f256d9b]203while for a *x-y* symmetric smear
[da53353]204
205.. image:: sm_image027.gif
206
[f256d9b]207**[Equation 12]**
[da53353]208
209where
210
211.. image:: sm_image028.gif
212
[f256d9b]213The current version of the SasView uses Equation 11 for 2D smearing, assuming
214that all the Gaussian weighting functions are aligned in the polar coordinate.
[da53353]215
[f256d9b]216.. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ
217
218Weighting & Normalization
219-------------------------
220
221In all the cases above, the weighting matrix *W* is calculated on the first call
222to a smearing function, and includes ~60 *q* values (finely and evenly binned)
223below (>0) and above the *q* range of data in order to smear all data points for
224a given model and slit/pinhole size. The *Norm*  factor is found numerically with the
225weighting matrix and applied on the computation of *I*\ :sub:`s`.
[da53353]226
227.. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ
[f256d9b]228
229.. note::  This help document was last changed by Steve King, 01May2015
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