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34          <span>Home</span></a></h1>
35        <h2 class="heading"><span>1. Introduction</span></h2>
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51  <div class="section" id="introduction">
52<span id="models-intro"></span><h1>1. Introduction<a class="headerlink" href="#introduction" title="Permalink to this headline">¶</a></h1>
53<p>Many of our models use the form factor calculations implemented in a c-library provided by the NIST Center for Neutron
54Research and thus some content and figures in this document are originated from or shared with the NIST SANS Igor-based
55analysis package.</p>
56<p>This software provides form factors for various particle shapes. After giving a mathematical definition of each model,
57we show the list of parameters available to the user. Validation plots for each model are also presented.</p>
58<p>Instructions on how to use SasView itself are available separately.</p>
59<p>To easily compare to the scattering intensity measured in experiments, we normalize the form factors by the volume of
60the particle</p>
61<div class="math">
62\[P(\vec q) = \frac{P_o(\vec q)}{V} = \frac{1}{V} F(\vec q) F^*(\vec q)\]</div>
63<p>with</p>
64<blockquote>
65<div>F(vec q) = intintint dVrho(vec r) e^{-ivec q cdot vec r}</div></blockquote>
66<p>where <span class="math">\(P_0(\vec q)\)</span> is the un-normalized form factor, <span class="math">\(\rho(\vec r)\)</span> is the scattering length density at a given
67point in space and the integration is done over the volume <span class="math">\(V\)</span> of the scatterer.</p>
68<p>For systems without inter-particle interference, the form factors we provide can be related to the scattering intensity
69by the particle volume fraction</p>
70<div class="math">
71\[I(\vec q) = \Phi P(\vec q)\]</div>
72<p>Our so-called 1D scattering intensity functions provide <span class="math">\(P(Q)\)</span> for the case where the scatterer is randomly oriented. In
73that case, the scattering intensity only depends on the length of <span class="math">\(Q\)</span> . The intensity measured on the plane of the SAS
74detector will have an azimuthal symmetry around <span class="math">\(Q=0\)</span>.</p>
75<p>Our so-called 2D scattering intensity functions provide <span class="math">\(P(Q,\phi)\)</span> for an oriented system as a function of a
76<span class="math">\(q\)</span> vector in the plane of the detector. We define the angle <span class="math">\(\phi\)</span> as the angle between the <span class="math">\(q\)</span> vector and the horizontal
77($x$) axis of the plane of the detector.</p>
78<p>For information about polarised and magnetic scattering, see <a class="reference external" href="polar_mag_help.html">here</a>.</p>
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