[25579e8] | 1 | /** |
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| 2 | This software was developed by the University of Tennessee as part of the |
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| 3 | Distributed Data Analysis of Neutron Scattering Experiments (DANSE) |
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| 4 | project funded by the US National Science Foundation. |
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| 5 | |
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| 6 | If you use DANSE applications to do scientific research that leads to |
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| 7 | publication, we ask that you acknowledge the use of the software with the |
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| 8 | following sentence: |
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| 9 | |
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| 10 | "This work benefited from DANSE software developed under NSF award DMR-0520547." |
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| 11 | |
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| 12 | copyright 2008, University of Tennessee |
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| 13 | */ |
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| 14 | |
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| 15 | /** |
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| 16 | * Scattering model classes |
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| 17 | * The classes use the IGOR library found in |
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| 18 | * sansmodels/src/libigor |
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| 19 | * |
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| 20 | * TODO: refactor so that we pull in the old sansmodels.c_extensions |
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| 21 | */ |
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| 22 | |
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| 23 | #include <math.h> |
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| 24 | #include "models.hh" |
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| 25 | #include "parameters.hh" |
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| 26 | #include <stdio.h> |
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| 27 | using namespace std; |
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| 28 | |
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| 29 | extern "C" { |
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| 30 | #include "libStructureFactor.h" |
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| 31 | #include "Hardsphere.h" |
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| 32 | } |
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| 33 | |
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| 34 | HardsphereStructure :: HardsphereStructure() { |
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| 35 | radius = Parameter(50.0, true); |
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| 36 | radius.set_min(0.0); |
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| 37 | volfraction = Parameter(0.20, true); |
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| 38 | volfraction.set_min(0.0); |
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| 39 | } |
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| 40 | |
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| 41 | /** |
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| 42 | * Function to evaluate 1D scattering function |
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| 43 | * The NIST IGOR library is used for the actual calculation. |
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| 44 | * @param q: q-value |
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| 45 | * @return: function value |
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| 46 | */ |
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| 47 | double HardsphereStructure :: operator()(double q) { |
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| 48 | double dp[2]; |
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| 49 | |
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| 50 | // Fill parameter array for IGOR library |
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| 51 | // Add the background after averaging |
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| 52 | dp[0] = radius(); |
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| 53 | dp[1] = volfraction(); |
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| 54 | |
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| 55 | // Get the dispersion points for the radius |
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| 56 | vector<WeightPoint> weights_rad; |
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| 57 | radius.get_weights(weights_rad); |
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| 58 | |
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| 59 | // Perform the computation, with all weight points |
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| 60 | double sum = 0.0; |
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| 61 | double norm = 0.0; |
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| 62 | |
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| 63 | // Loop over radius weight points |
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| 64 | for(int i=0; i<weights_rad.size(); i++) { |
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| 65 | dp[0] = weights_rad[i].value; |
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| 66 | |
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| 67 | sum += weights_rad[i].weight |
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| 68 | * HardSphereStruct(dp, q); |
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| 69 | norm += weights_rad[i].weight; |
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| 70 | } |
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| 71 | return sum/norm ; |
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| 72 | } |
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| 73 | |
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| 74 | /** |
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| 75 | * Function to evaluate 2D scattering function |
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| 76 | * @param q_x: value of Q along x |
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| 77 | * @param q_y: value of Q along y |
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| 78 | * @return: function value |
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| 79 | */ |
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| 80 | double HardsphereStructure :: operator()(double qx, double qy) { |
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| 81 | HardsphereParameters dp; |
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| 82 | // Fill parameter array |
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| 83 | dp.radius = radius(); |
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| 84 | dp.volfraction = volfraction(); |
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| 85 | |
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| 86 | // Get the dispersion points for the radius |
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| 87 | vector<WeightPoint> weights_rad; |
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| 88 | radius.get_weights(weights_rad); |
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| 89 | |
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| 90 | // Perform the computation, with all weight points |
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| 91 | double sum = 0.0; |
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| 92 | double norm = 0.0; |
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| 93 | |
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| 94 | // Loop over radius weight points |
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| 95 | for(int i=0; i<weights_rad.size(); i++) { |
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| 96 | dp.radius = weights_rad[i].value; |
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| 97 | |
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| 98 | double _ptvalue = weights_rad[i].weight |
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| 99 | * Hardsphere_analytical_2DXY(&dp, qx, qy); |
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| 100 | sum += _ptvalue; |
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| 101 | |
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| 102 | norm += weights_rad[i].weight; |
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| 103 | } |
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| 104 | // Averaging in theta needs an extra normalization |
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| 105 | // factor to account for the sin(theta) term in the |
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| 106 | // integration (see documentation). |
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| 107 | return sum/norm; |
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| 108 | } |
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| 109 | |
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| 110 | /** |
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| 111 | * Function to evaluate 2D scattering function |
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| 112 | * @param pars: parameters of the cylinder |
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| 113 | * @param q: q-value |
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| 114 | * @param phi: angle phi |
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| 115 | * @return: function value |
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| 116 | */ |
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| 117 | double HardsphereStructure :: evaluate_rphi(double q, double phi) { |
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| 118 | double qx = q*cos(phi); |
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| 119 | double qy = q*sin(phi); |
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| 120 | return (*this).operator()(qx, qy); |
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| 121 | } |
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