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33 | <div class="header"><h1 class="heading"><a href="../index.html"> |
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34 | <span>Home</span></a></h1> |
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35 | <h2 class="heading"><span>1. Introduction</span></h2> |
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40 | «  <a href="index.html">2. SAS Model Reference</a> |
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51 | <div class="section" id="introduction"> |
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52 | <span id="models-intro"></span><h1>1. Introduction<a class="headerlink" href="#introduction" title="Permalink to this headline">¶</a></h1> |
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53 | <p>Many of our models use the form factor calculations implemented in a c-library provided by the NIST Center for Neutron |
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54 | Research and thus some content and figures in this document are originated from or shared with the NIST SANS Igor-based |
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55 | analysis package.</p> |
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56 | <p>This software provides form factors for various particle shapes. After giving a mathematical definition of each model, |
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57 | we show the list of parameters available to the user. Validation plots for each model are also presented.</p> |
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58 | <p>Instructions on how to use SasView itself are available separately.</p> |
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59 | <p>To easily compare to the scattering intensity measured in experiments, we normalize the form factors by the volume of |
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60 | the particle</p> |
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61 | <div class="math"> |
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62 | \[P(\vec q) = \frac{P_o(\vec q)}{V} = \frac{1}{V} F(\vec q) F^*(\vec q)\]</div> |
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63 | <p>with</p> |
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64 | <blockquote> |
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65 | <div>F(vec q) = intintint dVrho(vec r) e^{-ivec q cdot vec r}</div></blockquote> |
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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 |
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67 | point in space and the integration is done over the volume <span class="math">\(V\)</span> of the scatterer.</p> |
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68 | <p>For systems without inter-particle interference, the form factors we provide can be related to the scattering intensity |
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69 | by the particle volume fraction</p> |
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70 | <div class="math"> |
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71 | \[I(\vec q) = \Phi P(\vec q)\]</div> |
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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 |
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73 | that case, the scattering intensity only depends on the length of <span class="math">\(Q\)</span> . The intensity measured on the plane of the SAS |
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74 | detector will have an azimuthal symmetry around <span class="math">\(Q=0\)</span>.</p> |
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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 |
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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 |
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77 | ($x$) axis of the plane of the detector.</p> |
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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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86 | «  <a href="index.html">2. SAS Model Reference</a> |
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88 | <a class="uplink" href="../index.html">Contents</a> |
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89 |   ::   |
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90 | <a href="models/index.html">2. Model Functions</a>  Â» |
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