source: sasmodels/doc/guide/sesans/sans_to_sesans.rst @ a03fad8

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Last change on this file since a03fad8 was 8ae8532, checked in by Paul Kienzle <pkienzle@…>, 8 years ago

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[8ae8532]1.. currentmodule:: sasmodels
2.. Wim Bouwman, DUT, written at codecamp-V, Oct2016
3
4.. _SESANS:
5
6SANS to SESANS conversion
7=========================
8
9The conversion from SANS into SESANS in absolute units is a simple Hankel
10transformation when all the small-angle scattered neutrons are detected.
11First we calculate the Hankel transform including the absolute intensities by
12
13.. math:: G(\delta) = 2 \pi \int_0^{\infty} J_0(Q \delta) \frac{d \Sigma}{d \Omega} (Q) Q dQ \!,
14
15in which :math:`J_0` is the zeroth order Bessel function, :math:`\delta`
16the spin-echo length, :math:`Q` the wave vector transfer and :math:`\frac{d \Sigma}{d \Omega} (Q)`
17the scattering cross section in absolute units. This is a 1-dimensional
18integral, which can be rather fast. In the numerical calculation we integrate
19from :math:`Q_{min} = 0.1 \times 2 \pi / R_{max}` in which :math:`R_{max}`
20will be model dependent. We determined the factor 0.1 by varying its value
21until the value of the integral was stable. This happened at a value of 0.3.
22The have a safety margin of a factor of three we have choosen the value 0.1.
23For the solid sphere we took 3 times the radius for :math:`R_{max}`. The real
24integration is performed to :math:`Q_{max}` which is an instrumental parameter
25that is read in from the measurement file. From the equation above we can
26calculate the polarisation that we measure in a SESANS experiment:
27
28.. math:: P(\delta) = e^{t \left( \frac{ \lambda}{2 \pi} \right)^2 \left(G(\delta) - G(0) \right)} \!,
29
30in which :math:`t` is the thickness of the sample and :math:`\lambda` is
31the wavelength of the neutrons.
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