source: sasview/src/sas/sasgui/perspectives/fitting/media/sm_help.rst @ 20cfa23

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[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.. |inlineimage004| image:: sm_image004.gif
7.. |inlineimage005| image:: sm_image005.gif
8.. |inlineimage008| image:: sm_image008.gif
9.. |inlineimage009| image:: sm_image009.gif
10.. |inlineimage010| image:: sm_image010.gif
11.. |inlineimage011| image:: sm_image011.gif
12.. |inlineimage012| image:: sm_image012.gif
13.. |inlineimage018| image:: sm_image018.gif
14.. |inlineimage019| image:: sm_image019.gif
15
16
17.. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ
18
[f256d9b]19Smearing Functions
20==================
[da53353]21
[f256d9b]22Sometimes it will be necessary to correct reduced experimental data for the
23physical effects of the instrumental geometry in use. This process is called
24*desmearing*. However, calculated/simulated data - which by definition will be
25perfect/exact - can be *smeared* to make it more representative of what might
26actually be measured experimentally.
27
28SasView provides the following three smearing algorithms:
[da53353]29
[a0637de]30*  *Slit Smearing*
31*  *Pinhole Smearing*
32*  *2D Smearing*
[da53353]33
[a0637de]34.. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ
[da53353]35
36Slit Smearing
[f256d9b]37-------------
38
39**This type of smearing is normally only encountered with data from X-ray Kratky**
40**cameras or X-ray/neutron Bonse-Hart USAXS/USANS instruments.**
[da53353]41
[f256d9b]42The slit-smeared scattering intensity is defined by
[da53353]43
44.. image:: sm_image002.gif
45
[f256d9b]46where *Norm* is given by
[da53353]47
48.. image:: sm_image003.gif
49
[f256d9b]50**[Equation 1]**
[da53353]51
52The functions |inlineimage004| and |inlineimage005|
53refer to the slit width weighting function and the slit height weighting
[f256d9b]54determined at the given *q* point, respectively. It is assumed that the weighting
55function is described by a rectangular function, such that
[da53353]56
57.. image:: sm_image006.gif
58
[f256d9b]59**[Equation 2]**
[da53353]60
61and
62
63.. image:: sm_image007.gif
64
[f256d9b]65**[Equation 3]**
[da53353]66
[f256d9b]67so that |inlineimage008| |inlineimage009| for |inlineimage010| and *u*\ .
[da53353]68
[f256d9b]69Here |inlineimage011| and |inlineimage012| stand for
70the slit height (FWHM/2) and the slit width (FWHM/2) in *q* space.
71
72This simplifies the integral in Equation 1 to
[da53353]73
74.. image:: sm_image013.gif
75
[f256d9b]76**[Equation 4]**
77
78which may be solved numerically, depending on the nature of |inlineimage011| and |inlineimage012| .
[da53353]79
[f256d9b]80Solution 1
81^^^^^^^^^^
[da53353]82
[f256d9b]83**For** |inlineimage012| **= 0 and** |inlineimage011| **= constant.**
[da53353]84
85.. image:: sm_image016.gif
86
[f256d9b]87For discrete *q* values, at the *q* values of the data points and at the *q*
88values extended up to *q*\ :sub:`N`\ = *q*\ :sub:`i` + |inlineimage011| the smeared
89intensity can be approximately calculated as
[da53353]90
91.. image:: sm_image017.gif
92
[f256d9b]93**[Equation 5]**
[da53353]94
[f256d9b]95where |inlineimage018| = 0 for *I*\ :sub:`s` when *j* < *i* or *j* > *N-1*.
[da53353]96
[f256d9b]97Solution 2
98^^^^^^^^^^
[da53353]99
[f256d9b]100**For** |inlineimage012| **= constant and** |inlineimage011| **= 0.**
[da53353]101
[f256d9b]102Similar to Case 1
[da53353]103
[f256d9b]104|inlineimage019| for *q*\ :sub:`p` = *q*\ :sub:`i` - |inlineimage012| and *q*\ :sub:`N` = *q*\ :sub:`i` + |inlineimage012|
[da53353]105
[f256d9b]106**[Equation 6]**
[da53353]107
[f256d9b]108where |inlineimage018| = 0 for *I*\ :sub:`s` when *j* < *p* or *j* > *N-1*.
[da53353]109
[f256d9b]110Solution 3
111^^^^^^^^^^
112
113**For** |inlineimage011| **= constant and** |inlineimage011| **= constant.**
114
115In this case, the best way is to perform the integration of Equation 1
116numerically for both slit height and slit width. However, the numerical
117integration is imperfect unless a large number of iterations, say, at
118least 10000 by 10000 for each element of the matrix *W*, is performed.
119This is usually too slow for routine use.
120
121An alternative approach is used in SasView which assumes
122slit width << slit height. This method combines Solution 1 with the
123numerical integration for the slit width. Then
[da53353]124
125.. image:: sm_image020.gif
126
[f256d9b]127**[Equation 7]**
128
129for *q*\ :sub:`p` = *q*\ :sub:`i` - |inlineimage012| and *q*\ :sub:`N` = *q*\ :sub:`i` + |inlineimage012|
[da53353]130
[f256d9b]131where |inlineimage018| = 0 for *I*\ :sub:`s` when *j* < *p* or *j* > *N-1*.
[da53353]132
[a0637de]133.. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ
[da53353]134
135Pinhole Smearing
[f256d9b]136----------------
[da53353]137
[f256d9b]138**This is the type of smearing normally encountered with data from synchrotron**
139**SAXS cameras and SANS instruments.**
[da53353]140
[f256d9b]141The pinhole smearing computation is performed in a similar fashion to the slit-
142smeared case above except that the weight function used is a Gaussian. Thus
143Equation 6 becomes
[da53353]144
[f256d9b]145.. image:: sm_image021.gif
[da53353]146
[f256d9b]147**[Equation 8]**
[da53353]148
[a0637de]149.. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ
[da53353]150
1512D Smearing
[f256d9b]152-----------
[da53353]153
[f256d9b]154The 2D smearing computation is performed in a similar fashion to the 1D pinhole
155smearing above except that the weight function used is a 2D elliptical Gaussian.
156Thus
[da53353]157
158.. image:: sm_image022.gif
159
[f256d9b]160**[Equation 9]**
[da53353]161
[f256d9b]162In Equation 9, *x*\ :sub:`0` = *q* cos(|theta|), *y*\ :sub:`0` = *q* sin(|theta|), and
163the primed axes, are all in the coordinate rotated by an angle |theta| about
164the z-axis (see the figure below) so that *x'*\ :sub:`0` = *x*\ :sub:`0` cos(|theta|) +
165*y*\ :sub:`0` sin(|theta|) and *y'*\ :sub:`0` = -*x*\ :sub:`0` sin(|theta|) +
166*y*\ :sub:`0` cos(|theta|). Note that the rotation angle is zero for a x-y symmetric
167elliptical Gaussian distribution. The *A* is a normalization factor.
[da53353]168
169.. image:: sm_image023.gif
170
[f256d9b]171Now we consider a numerical integration where each of the bins in |theta| and *R* are
172*evenly* (this is to simplify the equation below) distributed by |bigdelta|\ |theta|
173and |bigdelta|\ R, respectively, and it is further assumed that *I(x',y')* is constant
174within the bins. Then
[da53353]175
176.. image:: sm_image024.gif
177
[f256d9b]178**[Equation 10]**
179
180Since the weighting factor on each of the bins is known, it is convenient to
181transform *x'-y'* back to *x-y* coordinates (by rotating it by -|theta| around the
182*z* axis).
[da53353]183
[f256d9b]184Then, for a polar symmetric smear
[da53353]185
186.. image:: sm_image025.gif
187
[f256d9b]188**[Equation 11]**
[da53353]189
190where
191
192.. image:: sm_image026.gif
193
[f256d9b]194while for a *x-y* symmetric smear
[da53353]195
196.. image:: sm_image027.gif
197
[f256d9b]198**[Equation 12]**
[da53353]199
200where
201
202.. image:: sm_image028.gif
203
[f256d9b]204The current version of the SasView uses Equation 11 for 2D smearing, assuming
205that all the Gaussian weighting functions are aligned in the polar coordinate.
[da53353]206
[f256d9b]207.. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ
208
209Weighting & Normalization
210-------------------------
211
212In all the cases above, the weighting matrix *W* is calculated on the first call
213to a smearing function, and includes ~60 *q* values (finely and evenly binned)
214below (>0) and above the *q* range of data in order to smear all data points for
215a given model and slit/pinhole size. The *Norm*  factor is found numerically with the
216weighting matrix and applied on the computation of *I*\ :sub:`s`.
[da53353]217
218.. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ
[f256d9b]219
220.. note::  This help document was last changed by Steve King, 01May2015
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