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 | */ |
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21 | |
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22 | #include <math.h> |
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23 | #include "parameters.hh" |
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24 | #include <stdio.h> |
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25 | using namespace std; |
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26 | |
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27 | extern "C" { |
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28 | #include "libCylinder.h" |
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29 | #include "libStructureFactor.h" |
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30 | #include "libmultifunc/libfunc.h" |
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31 | } |
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32 | #include "cylinder.h" |
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33 | |
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34 | // Convenience parameter structure |
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35 | typedef struct { |
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36 | double scale; |
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37 | double radius; |
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38 | double length; |
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39 | double sldCyl; |
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40 | double sldSolv; |
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41 | double background; |
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42 | double cyl_theta; |
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43 | double cyl_phi; |
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44 | double M0_sld_cyl; |
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45 | double M_theta_cyl; |
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46 | double M_phi_cyl; |
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47 | double M0_sld_solv; |
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48 | double M_theta_solv; |
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49 | double M_phi_solv; |
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50 | double Up_frac_i; |
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51 | double Up_frac_f; |
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52 | double Up_theta; |
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53 | } CylinderParameters; |
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54 | |
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55 | CylinderModel :: CylinderModel() { |
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56 | scale = Parameter(1.0); |
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57 | radius = Parameter(20.0, true); |
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58 | radius.set_min(0.0); |
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59 | length = Parameter(400.0, true); |
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60 | length.set_min(0.0); |
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61 | sldCyl = Parameter(4.e-6); |
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62 | sldSolv = Parameter(1.e-6); |
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63 | background = Parameter(0.0); |
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64 | cyl_theta = Parameter(0.0, true); |
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65 | cyl_phi = Parameter(0.0, true); |
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66 | M0_sld_cyl = Parameter(0.0e-6); |
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67 | M_theta_cyl = Parameter(0.0); |
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68 | M_phi_cyl = Parameter(0.0); |
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69 | M0_sld_solv = Parameter(0.0e-6); |
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70 | M_theta_solv = Parameter(0.0); |
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71 | M_phi_solv = Parameter(0.0); |
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72 | Up_frac_i = Parameter(0.5); |
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73 | Up_frac_f = Parameter(0.5); |
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74 | Up_theta = Parameter(0.0); |
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75 | } |
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76 | |
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77 | /** |
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78 | * Function to evaluate 1D scattering function |
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79 | * The NIST IGOR library is used for the actual calculation. |
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80 | * @param q: q-value |
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81 | * @return: function value |
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82 | */ |
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83 | double CylinderModel :: operator()(double q) { |
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84 | double dp[6]; |
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85 | |
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86 | // Fill parameter array for IGOR library |
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87 | // Add the background after averaging |
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88 | dp[0] = scale(); |
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89 | dp[1] = radius(); |
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90 | dp[2] = length(); |
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91 | dp[3] = sldCyl(); |
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92 | dp[4] = sldSolv(); |
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93 | dp[5] = 0.0; |
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94 | |
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95 | // Get the dispersion points for the radius |
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96 | vector<WeightPoint> weights_rad; |
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97 | radius.get_weights(weights_rad); |
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98 | |
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99 | // Get the dispersion points for the length |
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100 | vector<WeightPoint> weights_len; |
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101 | length.get_weights(weights_len); |
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102 | |
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103 | // Perform the computation, with all weight points |
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104 | double sum = 0.0; |
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105 | double norm = 0.0; |
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106 | double vol = 0.0; |
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107 | |
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108 | // Loop over radius weight points |
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109 | for(size_t i=0; i<weights_rad.size(); i++) { |
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110 | dp[1] = weights_rad[i].value; |
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111 | |
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112 | // Loop over length weight points |
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113 | for(size_t j=0; j<weights_len.size(); j++) { |
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114 | dp[2] = weights_len[j].value; |
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115 | //Un-normalize by volume |
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116 | sum += weights_rad[i].weight |
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117 | * weights_len[j].weight * CylinderForm(dp, q) |
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118 | *pow(weights_rad[i].value,2)*weights_len[j].value; |
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119 | |
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120 | //Find average volume |
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121 | vol += weights_rad[i].weight |
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122 | * weights_len[j].weight *pow(weights_rad[i].value,2)*weights_len[j].value; |
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123 | norm += weights_rad[i].weight |
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124 | * weights_len[j].weight; |
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125 | } |
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126 | } |
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127 | if (vol != 0.0 && norm != 0.0) { |
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128 | //Re-normalize by avg volume |
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129 | sum = sum/(vol/norm);} |
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130 | |
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131 | return sum/norm + background(); |
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132 | } |
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133 | |
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134 | /** |
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135 | * Function to evaluate 2D scattering function |
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136 | * @param pars: parameters of the cylinder |
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137 | * @param q: q-value |
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138 | * @param q_x: q_x / q |
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139 | * @param q_y: q_y / q |
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140 | * @return: function value |
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141 | */ |
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142 | static double cylinder_analytical_2D_scaled(CylinderParameters *pars, double q, double q_x, double q_y) { |
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143 | double cyl_x, cyl_y;//, cyl_z; |
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144 | //double q_z; |
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145 | double alpha, vol, cos_val; |
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146 | double answer = 0.0; |
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147 | double form = 0.0; |
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148 | //convert angle degree to radian |
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149 | double pi = 4.0*atan(1.0); |
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150 | double theta = pars->cyl_theta * pi/180.0; |
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151 | double phi = pars->cyl_phi * pi/180.0; |
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152 | double sld_solv = pars->sldSolv; |
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153 | double sld_cyl = pars->sldCyl; |
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154 | double m_max = pars->M0_sld_cyl; |
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155 | double m_max_solv = pars->M0_sld_solv; |
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156 | double contrast = 0.0; |
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157 | |
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158 | // Cylinder orientation |
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159 | cyl_x = cos(theta) * cos(phi); |
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160 | cyl_y = sin(theta); |
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161 | //cyl_z = -cos(theta) * sin(phi); |
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162 | // q vector |
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163 | //q_z = 0.0; |
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164 | |
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165 | // Compute the angle btw vector q and the |
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166 | // axis of the cylinder |
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167 | cos_val = cyl_x*q_x + cyl_y*q_y;// + cyl_z*q_z; |
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168 | |
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169 | // The following test should always pass |
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170 | if (fabs(cos_val)>1.0) { |
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171 | printf("cyl_ana_2D: Unexpected error: |cos(alpha)=%g|>1\n", cos_val); |
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172 | printf("cyl_ana_2D: at theta=%g and phi=%g.", theta, phi); |
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173 | return 1.0; |
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174 | } |
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175 | |
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176 | // Note: cos(alpha) = 0 and 1 will get an |
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177 | // undefined value from CylKernel |
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178 | alpha = acos( cos_val ); |
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179 | if (alpha == 0.0){ |
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180 | alpha = 1.0e-26; |
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181 | } |
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182 | // Call the IGOR library function to get the kernel |
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183 | //answer = CylKernel(q, pars->radius, pars->length/2.0, alpha) / sin(alpha); |
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184 | |
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185 | // Call the IGOR library function to get the kernel |
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186 | form = CylKernel(q, pars->radius, pars->length/2.0, alpha) / sin(alpha); |
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187 | |
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188 | if (m_max < 1.0e-32 && m_max_solv < 1.0e-32){ |
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189 | // Multiply by contrast^2 |
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190 | contrast = (pars->sldCyl - pars->sldSolv); |
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191 | answer = contrast * contrast * form; |
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192 | } |
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193 | else{ |
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194 | double qx = q_x; |
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195 | double qy = q_y; |
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196 | double s_theta = pars->Up_theta; |
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197 | double m_phi = pars->M_phi_cyl; |
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198 | double m_theta = pars->M_theta_cyl; |
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199 | double m_phi_solv = pars->M_phi_solv; |
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200 | double m_theta_solv = pars->M_theta_solv; |
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201 | double in_spin = pars->Up_frac_i; |
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202 | double out_spin = pars->Up_frac_f; |
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203 | polar_sld p_sld; |
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204 | polar_sld p_sld_solv; |
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205 | p_sld = cal_msld(1, qx, qy, sld_cyl, m_max, m_theta, m_phi, |
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206 | in_spin, out_spin, s_theta); |
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207 | p_sld_solv = cal_msld(1, qx, qy, sld_solv, m_max_solv, m_theta_solv, m_phi_solv, |
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208 | in_spin, out_spin, s_theta); |
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209 | //up_up |
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210 | if (in_spin > 0.0 && out_spin > 0.0){ |
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211 | answer += ((p_sld.uu- p_sld_solv.uu) * (p_sld.uu- p_sld_solv.uu) * form); |
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212 | } |
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213 | //down_down |
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214 | if (in_spin < 1.0 && out_spin < 1.0){ |
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215 | answer += ((p_sld.dd - p_sld_solv.dd) * (p_sld.dd - p_sld_solv.dd) * form); |
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216 | } |
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217 | //up_down |
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218 | if (in_spin > 0.0 && out_spin < 1.0){ |
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219 | answer += ((p_sld.re_ud - p_sld_solv.re_ud) * (p_sld.re_ud - p_sld_solv.re_ud) * form); |
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220 | answer += ((p_sld.im_ud - p_sld_solv.im_ud) * (p_sld.im_ud - p_sld_solv.im_ud) * form); |
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221 | } |
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222 | //down_up |
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223 | if (in_spin < 1.0 && out_spin > 0.0){ |
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224 | answer += ((p_sld.re_du - p_sld_solv.re_du) * (p_sld.re_du - p_sld_solv.re_du) * form); |
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225 | answer += ((p_sld.im_du - p_sld_solv.im_du) * (p_sld.im_du - p_sld_solv.im_du) * form); |
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226 | } |
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227 | } |
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228 | |
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229 | //normalize by cylinder volume |
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230 | //NOTE that for this (Fournet) definition of the integral, one must MULTIPLY by Vcyl |
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231 | vol = acos(-1.0) * pars->radius * pars->radius * pars->length; |
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232 | answer *= vol; |
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233 | |
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234 | //convert to [cm-1] |
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235 | answer *= 1.0e8; |
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236 | |
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237 | //Scale |
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238 | answer *= pars->scale; |
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239 | |
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240 | // add in the background |
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241 | answer += pars->background; |
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242 | |
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243 | return answer; |
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244 | } |
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245 | |
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246 | /** |
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247 | * Function to evaluate 2D scattering function |
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248 | * @param pars: parameters of the cylinder |
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249 | * @param q: q-value |
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250 | * @return: function value |
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251 | */ |
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252 | static double cylinder_analytical_2DXY(CylinderParameters *pars, double qx, double qy) { |
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253 | double q; |
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254 | q = sqrt(qx*qx+qy*qy); |
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255 | return cylinder_analytical_2D_scaled(pars, q, qx/q, qy/q); |
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256 | } |
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257 | |
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258 | /** |
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259 | * Function to evaluate 2D scattering function |
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260 | * @param q_x: value of Q along x |
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261 | * @param q_y: value of Q along y |
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262 | * @return: function value |
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263 | */ |
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264 | double CylinderModel :: operator()(double qx, double qy) { |
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265 | CylinderParameters dp; |
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266 | // Fill parameter array |
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267 | dp.scale = scale(); |
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268 | dp.radius = radius(); |
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269 | dp.length = length(); |
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270 | dp.sldCyl = sldCyl(); |
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271 | dp.sldSolv = sldSolv(); |
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272 | dp.background = 0.0; |
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273 | dp.cyl_theta = cyl_theta(); |
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274 | dp.cyl_phi = cyl_phi(); |
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275 | dp.Up_theta = Up_theta(); |
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276 | dp.M_phi_cyl = M_phi_cyl(); |
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277 | dp.M_theta_cyl = M_theta_cyl(); |
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278 | dp.M0_sld_cyl = M0_sld_cyl(); |
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279 | dp.M_phi_solv = M_phi_solv(); |
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280 | dp.M_theta_solv = M_theta_solv(); |
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281 | dp.M0_sld_solv = M0_sld_solv(); |
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282 | dp.Up_frac_i = Up_frac_i(); |
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283 | dp.Up_frac_f = Up_frac_f(); |
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284 | |
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285 | // Get the dispersion points for the radius |
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286 | vector<WeightPoint> weights_rad; |
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287 | radius.get_weights(weights_rad); |
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288 | |
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289 | // Get the dispersion points for the length |
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290 | vector<WeightPoint> weights_len; |
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291 | length.get_weights(weights_len); |
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292 | |
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293 | // Get angular averaging for theta |
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294 | vector<WeightPoint> weights_theta; |
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295 | cyl_theta.get_weights(weights_theta); |
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296 | |
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297 | // Get angular averaging for phi |
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298 | vector<WeightPoint> weights_phi; |
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299 | cyl_phi.get_weights(weights_phi); |
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300 | |
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301 | // Perform the computation, with all weight points |
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302 | double sum = 0.0; |
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303 | double norm = 0.0; |
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304 | double norm_vol = 0.0; |
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305 | double vol = 0.0; |
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306 | double pi = 4.0*atan(1.0); |
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307 | // Loop over radius weight points |
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308 | for(size_t i=0; i<weights_rad.size(); i++) { |
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309 | dp.radius = weights_rad[i].value; |
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310 | |
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311 | |
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312 | // Loop over length weight points |
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313 | for(size_t j=0; j<weights_len.size(); j++) { |
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314 | dp.length = weights_len[j].value; |
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315 | |
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316 | // Average over theta distribution |
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317 | for(size_t k=0; k<weights_theta.size(); k++) { |
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318 | dp.cyl_theta = weights_theta[k].value; |
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319 | |
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320 | // Average over phi distribution |
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321 | for(size_t l=0; l<weights_phi.size(); l++) { |
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322 | dp.cyl_phi = weights_phi[l].value; |
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323 | //Un-normalize by volume |
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324 | double _ptvalue = weights_rad[i].weight |
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325 | * weights_len[j].weight |
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326 | * weights_theta[k].weight |
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327 | * weights_phi[l].weight |
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328 | * cylinder_analytical_2DXY(&dp, qx, qy) |
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329 | *pow(weights_rad[i].value,2)*weights_len[j].value; |
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330 | if (weights_theta.size()>1) { |
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331 | _ptvalue *= fabs(cos(weights_theta[k].value*pi/180.0)); |
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332 | } |
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333 | sum += _ptvalue; |
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334 | //Find average volume |
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335 | vol += weights_rad[i].weight |
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336 | * weights_len[j].weight |
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337 | * pow(weights_rad[i].value,2)*weights_len[j].value; |
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338 | //Find norm for volume |
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339 | norm_vol += weights_rad[i].weight |
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340 | * weights_len[j].weight; |
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341 | |
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342 | norm += weights_rad[i].weight |
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343 | * weights_len[j].weight |
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344 | * weights_theta[k].weight |
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345 | * weights_phi[l].weight; |
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346 | |
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347 | } |
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348 | } |
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349 | } |
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350 | } |
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351 | // Averaging in theta needs an extra normalization |
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352 | // factor to account for the sin(theta) term in the |
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353 | // integration (see documentation). |
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354 | if (weights_theta.size()>1) norm = norm / asin(1.0); |
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355 | if (vol != 0.0 && norm_vol != 0.0) { |
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356 | //Re-normalize by avg volume |
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357 | sum = sum/(vol/norm_vol);} |
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358 | |
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359 | return sum/norm + background(); |
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360 | } |
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361 | |
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362 | /** |
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363 | * Function to evaluate 2D scattering function |
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364 | * @param pars: parameters of the cylinder |
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365 | * @param q: q-value |
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366 | * @param phi: angle phi |
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367 | * @return: function value |
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368 | */ |
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369 | double CylinderModel :: evaluate_rphi(double q, double phi) { |
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370 | double qx = q*cos(phi); |
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371 | double qy = q*sin(phi); |
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372 | return (*this).operator()(qx, qy); |
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373 | } |
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374 | /** |
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375 | * Function to calculate effective radius |
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376 | * @return: effective radius value |
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377 | */ |
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378 | double CylinderModel :: calculate_ER() { |
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379 | CylinderParameters dp; |
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380 | |
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381 | dp.radius = radius(); |
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382 | dp.length = length(); |
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383 | double rad_out = 0.0; |
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384 | |
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385 | // Perform the computation, with all weight points |
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386 | double sum = 0.0; |
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387 | double norm = 0.0; |
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388 | |
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389 | // Get the dispersion points for the major shell |
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390 | vector<WeightPoint> weights_length; |
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391 | length.get_weights(weights_length); |
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392 | |
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393 | // Get the dispersion points for the minor shell |
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394 | vector<WeightPoint> weights_radius ; |
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395 | radius.get_weights(weights_radius); |
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396 | |
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397 | // Loop over major shell weight points |
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398 | for(int i=0; i< (int)weights_length.size(); i++) { |
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399 | dp.length = weights_length[i].value; |
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400 | for(int k=0; k< (int)weights_radius.size(); k++) { |
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401 | dp.radius = weights_radius[k].value; |
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402 | //Note: output of "DiamCyl(dp.length,dp.radius)" is DIAMETER. |
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403 | sum +=weights_length[i].weight |
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404 | * weights_radius[k].weight*DiamCyl(dp.length,dp.radius)/2.0; |
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405 | norm += weights_length[i].weight* weights_radius[k].weight; |
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406 | } |
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407 | } |
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408 | if (norm != 0){ |
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409 | //return the averaged value |
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410 | rad_out = sum/norm;} |
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411 | else{ |
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412 | //return normal value |
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413 | //Note: output of "DiamCyl(dp.length,dp.radius)" is DIAMETER. |
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414 | rad_out = DiamCyl(dp.length,dp.radius)/2.0;} |
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415 | |
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416 | return rad_out; |
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417 | } |
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418 | double CylinderModel :: calculate_VR() { |
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419 | return 1.0; |
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420 | } |
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