[975ec8e] | 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 "libCylinder.h" |
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[5eb9154] | 31 | #include "libStructureFactor.h" |
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[975ec8e] | 32 | #include "spheroid.h" |
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| 33 | } |
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| 34 | |
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[eddff027] | 35 | CoreShellEllipsoidModel :: CoreShellEllipsoidModel() { |
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[975ec8e] | 36 | scale = Parameter(1.0); |
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| 37 | equat_core = Parameter(200.0, true); |
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| 38 | equat_core.set_min(0.0); |
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| 39 | polar_core = Parameter(20.0, true); |
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| 40 | polar_core.set_min(0.0); |
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| 41 | equat_shell = Parameter(250.0, true); |
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| 42 | equat_shell.set_min(0.0); |
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| 43 | polar_shell = Parameter(30.0, true); |
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| 44 | polar_shell.set_min(0.0); |
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| 45 | contrast = Parameter(1e-6); |
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| 46 | sld_solvent = Parameter(6.3e-6); |
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| 47 | background = Parameter(0.0); |
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| 48 | axis_theta = Parameter(0.0, true); |
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| 49 | axis_phi = Parameter(0.0, true); |
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| 50 | |
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| 51 | } |
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| 52 | |
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| 53 | /** |
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| 54 | * Function to evaluate 1D scattering function |
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| 55 | * The NIST IGOR library is used for the actual calculation. |
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| 56 | * @param q: q-value |
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| 57 | * @return: function value |
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| 58 | */ |
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[eddff027] | 59 | double CoreShellEllipsoidModel :: operator()(double q) { |
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[975ec8e] | 60 | double dp[8]; |
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| 61 | |
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| 62 | // Fill parameter array for IGOR library |
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| 63 | // Add the background after averaging |
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| 64 | dp[0] = scale(); |
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| 65 | dp[1] = equat_core(); |
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| 66 | dp[2] = polar_core(); |
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| 67 | dp[3] = equat_shell(); |
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| 68 | dp[4] = polar_shell(); |
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| 69 | dp[5] = contrast(); |
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| 70 | dp[6] = sld_solvent(); |
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| 71 | dp[7] = 0.0; |
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| 72 | |
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| 73 | // Get the dispersion points for the major core |
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| 74 | vector<WeightPoint> weights_equat_core; |
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| 75 | equat_core.get_weights(weights_equat_core); |
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| 76 | |
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| 77 | // Get the dispersion points for the minor core |
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| 78 | vector<WeightPoint> weights_polar_core; |
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| 79 | polar_core.get_weights(weights_polar_core); |
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| 80 | |
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| 81 | // Get the dispersion points for the major shell |
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| 82 | vector<WeightPoint> weights_equat_shell; |
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| 83 | equat_shell.get_weights(weights_equat_shell); |
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| 84 | |
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| 85 | // Get the dispersion points for the minor_shell |
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| 86 | vector<WeightPoint> weights_polar_shell; |
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| 87 | polar_shell.get_weights(weights_polar_shell); |
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| 88 | |
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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 major core weight points |
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| 95 | for(int i=0; i<(int)weights_equat_core.size(); i++) { |
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| 96 | dp[1] = weights_equat_core[i].value; |
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| 97 | |
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| 98 | // Loop over minor core weight points |
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| 99 | for(int j=0; j<(int)weights_polar_core.size(); j++) { |
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| 100 | dp[2] = weights_polar_core[j].value; |
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| 101 | |
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| 102 | // Loop over major shell weight points |
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| 103 | for(int k=0; k<(int)weights_equat_shell.size(); k++) { |
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| 104 | dp[3] = weights_equat_shell[k].value; |
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| 105 | |
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| 106 | // Loop over minor shell weight points |
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| 107 | for(int l=0; l<(int)weights_polar_shell.size(); l++) { |
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| 108 | dp[4] = weights_polar_shell[l].value; |
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| 109 | |
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| 110 | sum += weights_equat_core[i].weight* weights_polar_core[j].weight * weights_equat_shell[k].weight |
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[14c3887] | 111 | * weights_polar_shell[l].weight * ProlateForm(dp, q); |
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[975ec8e] | 112 | norm += weights_equat_core[i].weight* weights_polar_core[j].weight * weights_equat_shell[k].weight |
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| 113 | * weights_polar_shell[l].weight; |
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| 114 | } |
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| 115 | } |
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| 116 | } |
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| 117 | } |
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| 118 | return sum/norm + background(); |
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| 119 | } |
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| 120 | |
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| 121 | /** |
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| 122 | * Function to evaluate 2D scattering function |
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| 123 | * @param q_x: value of Q along x |
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| 124 | * @param q_y: value of Q along y |
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| 125 | * @return: function value |
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| 126 | */ |
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| 127 | /* |
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| 128 | double OblateModel :: operator()(double qx, double qy) { |
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| 129 | double q = sqrt(qx*qx + qy*qy); |
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| 130 | |
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| 131 | return (*this).operator()(q); |
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| 132 | } |
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| 133 | */ |
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| 134 | |
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| 135 | /** |
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| 136 | * Function to evaluate 2D scattering function |
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| 137 | * @param pars: parameters of the oblate |
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| 138 | * @param q: q-value |
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| 139 | * @param phi: angle phi |
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| 140 | * @return: function value |
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| 141 | */ |
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[eddff027] | 142 | double CoreShellEllipsoidModel :: evaluate_rphi(double q, double phi) { |
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[5eb9154] | 143 | double qx = q*cos(phi); |
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| 144 | double qy = q*sin(phi); |
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| 145 | return (*this).operator()(qx, qy); |
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[975ec8e] | 146 | } |
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| 147 | |
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[5eb9154] | 148 | /** |
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| 149 | * Function to evaluate 2D scattering function |
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| 150 | * @param q_x: value of Q along x |
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| 151 | * @param q_y: value of Q along y |
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| 152 | * @return: function value |
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| 153 | */ |
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[eddff027] | 154 | double CoreShellEllipsoidModel :: operator()(double qx, double qy) { |
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[975ec8e] | 155 | SpheroidParameters dp; |
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| 156 | // Fill parameter array |
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| 157 | dp.scale = scale(); |
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| 158 | dp.equat_core = equat_core(); |
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| 159 | dp.polar_core = polar_core(); |
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| 160 | dp.equat_shell = equat_shell(); |
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| 161 | dp.polar_shell = polar_shell(); |
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| 162 | dp.contrast = contrast(); |
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| 163 | dp.sld_solvent = sld_solvent(); |
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[5eb9154] | 164 | dp.background = 0.0; |
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[975ec8e] | 165 | dp.axis_theta = axis_theta(); |
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| 166 | dp.axis_phi = axis_phi(); |
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| 167 | |
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| 168 | // Get the dispersion points for the major core |
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| 169 | vector<WeightPoint> weights_equat_core; |
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| 170 | equat_core.get_weights(weights_equat_core); |
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| 171 | |
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| 172 | // Get the dispersion points for the minor core |
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| 173 | vector<WeightPoint> weights_polar_core; |
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| 174 | polar_core.get_weights(weights_polar_core); |
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| 175 | |
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| 176 | // Get the dispersion points for the major shell |
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| 177 | vector<WeightPoint> weights_equat_shell; |
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| 178 | equat_shell.get_weights(weights_equat_shell); |
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| 179 | |
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| 180 | // Get the dispersion points for the minor shell |
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| 181 | vector<WeightPoint> weights_polar_shell; |
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| 182 | polar_shell.get_weights(weights_polar_shell); |
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| 183 | |
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| 184 | |
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| 185 | // Get angular averaging for theta |
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| 186 | vector<WeightPoint> weights_theta; |
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| 187 | axis_theta.get_weights(weights_theta); |
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| 188 | |
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| 189 | // Get angular averaging for phi |
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| 190 | vector<WeightPoint> weights_phi; |
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| 191 | axis_phi.get_weights(weights_phi); |
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| 192 | |
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| 193 | // Perform the computation, with all weight points |
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| 194 | double sum = 0.0; |
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| 195 | double norm = 0.0; |
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| 196 | |
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| 197 | // Loop over major core weight points |
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| 198 | for(int i=0; i< (int)weights_equat_core.size(); i++) { |
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| 199 | dp.equat_core = weights_equat_core[i].value; |
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| 200 | |
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| 201 | // Loop over minor core weight points |
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| 202 | for(int j=0; j< (int)weights_polar_core.size(); j++) { |
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| 203 | dp.polar_core = weights_polar_core[j].value; |
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| 204 | |
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| 205 | // Loop over major shell weight points |
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| 206 | for(int k=0; k< (int)weights_equat_shell.size(); k++) { |
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| 207 | dp.equat_shell = weights_equat_shell[i].value; |
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| 208 | |
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| 209 | // Loop over minor shell weight points |
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| 210 | for(int l=0; l< (int)weights_polar_shell.size(); l++) { |
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| 211 | dp.polar_shell = weights_polar_shell[l].value; |
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| 212 | |
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| 213 | // Average over theta distribution |
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| 214 | for(int m=0; m< (int)weights_theta.size(); m++) { |
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| 215 | dp.axis_theta = weights_theta[m].value; |
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| 216 | |
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| 217 | // Average over phi distribution |
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| 218 | for(int n=0; n< (int)weights_phi.size(); n++) { |
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| 219 | dp.axis_phi = weights_phi[n].value; |
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| 220 | |
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| 221 | double _ptvalue = weights_equat_core[i].weight *weights_polar_core[j].weight |
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| 222 | * weights_equat_shell[k].weight * weights_polar_shell[l].weight |
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| 223 | * weights_theta[m].weight |
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| 224 | * weights_phi[n].weight |
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| 225 | * spheroid_analytical_2DXY(&dp, qx, qy); |
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| 226 | if (weights_theta.size()>1) { |
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| 227 | _ptvalue *= sin(weights_theta[m].value); |
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| 228 | } |
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| 229 | sum += _ptvalue; |
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| 230 | |
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| 231 | norm += weights_equat_core[i].weight *weights_polar_core[j].weight |
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| 232 | * weights_equat_shell[k].weight * weights_polar_shell[l].weight |
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| 233 | * weights_theta[m].weight * weights_phi[n].weight; |
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| 234 | } |
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| 235 | } |
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| 236 | } |
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| 237 | } |
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| 238 | } |
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| 239 | } |
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| 240 | // Averaging in theta needs an extra normalization |
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| 241 | // factor to account for the sin(theta) term in the |
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| 242 | // integration (see documentation). |
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| 243 | if (weights_theta.size()>1) norm = norm / asin(1.0); |
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| 244 | return sum/norm + background(); |
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| 245 | } |
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| 246 | |
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[5eb9154] | 247 | /** |
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| 248 | * Function to calculate effective radius |
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| 249 | * @return: effective radius value |
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| 250 | */ |
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| 251 | double CoreShellEllipsoidModel :: calculate_ER() { |
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| 252 | SpheroidParameters dp; |
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| 253 | |
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| 254 | dp.equat_shell = equat_shell(); |
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| 255 | dp.polar_shell = polar_shell(); |
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| 256 | |
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| 257 | double rad_out = 0.0; |
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| 258 | |
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| 259 | // Perform the computation, with all weight points |
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| 260 | double sum = 0.0; |
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| 261 | double norm = 0.0; |
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| 262 | |
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| 263 | // Get the dispersion points for the major shell |
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| 264 | vector<WeightPoint> weights_equat_shell; |
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| 265 | equat_shell.get_weights(weights_equat_shell); |
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| 266 | |
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| 267 | // Get the dispersion points for the minor shell |
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| 268 | vector<WeightPoint> weights_polar_shell; |
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| 269 | polar_shell.get_weights(weights_polar_shell); |
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| 270 | |
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| 271 | // Loop over major shell weight points |
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| 272 | for(int i=0; i< (int)weights_equat_shell.size(); i++) { |
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| 273 | dp.equat_shell = weights_equat_shell[i].value; |
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| 274 | for(int k=0; k< (int)weights_polar_shell.size(); k++) { |
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| 275 | dp.polar_shell = weights_polar_shell[k].value; |
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| 276 | //Note: output of "DiamEllip(dp.polar_shell,dp.equat_shell)" is DIAMETER. |
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| 277 | sum +=weights_equat_shell[i].weight |
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| 278 | * weights_polar_shell[k].weight*DiamEllip(dp.polar_shell,dp.equat_shell)/2.0; |
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| 279 | norm += weights_equat_shell[i].weight* weights_polar_shell[k].weight; |
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| 280 | } |
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| 281 | } |
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| 282 | if (norm != 0){ |
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| 283 | //return the averaged value |
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| 284 | rad_out = sum/norm;} |
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| 285 | else{ |
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| 286 | //return normal value |
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| 287 | //Note: output of "DiamEllip(dp.polar_shell,dp.equat_shell)" is DIAMETER. |
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| 288 | rad_out = DiamEllip(dp.polar_shell,dp.equat_shell)/2.0;} |
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| 289 | |
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| 290 | return rad_out; |
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| 291 | } |
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