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 | #include "core_shell_cylinder.h" |
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27 | |
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28 | extern "C" { |
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29 | #include "libCylinder.h" |
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30 | #include "libStructureFactor.h" |
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31 | } |
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32 | |
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33 | typedef struct { |
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34 | double scale; |
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35 | double radius; |
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36 | double thickness; |
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37 | double length; |
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38 | double core_sld; |
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39 | double shell_sld; |
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40 | double solvent_sld; |
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41 | double background; |
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42 | double axis_theta; |
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43 | double axis_phi; |
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44 | } CoreShellCylinderParameters; |
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45 | |
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46 | |
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47 | /** |
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48 | * Function to evaluate 2D scattering function |
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49 | * @param pars: parameters of the core-shell cylinder |
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50 | * @param q: q-value |
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51 | * @param q_x: q_x / q |
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52 | * @param q_y: q_y / q |
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53 | * @return: function value |
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54 | */ |
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55 | static double core_shell_cylinder_analytical_2D_scaled(CoreShellCylinderParameters *pars, double q, double q_x, double q_y) { |
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56 | double cyl_x, cyl_y, cyl_z; |
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57 | double q_z; |
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58 | double alpha, vol, cos_val; |
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59 | double answer; |
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60 | //convert angle degree to radian |
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61 | double pi = 4.0*atan(1.0); |
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62 | double theta = pars->axis_theta * pi/180.0; |
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63 | double phi = pars->axis_phi * pi/180.0; |
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64 | |
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65 | // Cylinder orientation |
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66 | cyl_x = sin(theta) * cos(phi); |
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67 | cyl_y = sin(theta) * sin(phi); |
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68 | cyl_z = cos(theta); |
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69 | |
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70 | // q vector |
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71 | q_z = 0; |
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72 | |
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73 | // Compute the angle btw vector q and the |
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74 | // axis of the cylinder |
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75 | cos_val = cyl_x*q_x + cyl_y*q_y + cyl_z*q_z; |
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76 | |
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77 | // The following test should always pass |
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78 | if (fabs(cos_val)>1.0) { |
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79 | printf("core_shell_cylinder_analytical_2D: Unexpected error: cos(alpha)=%g\n", cos_val); |
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80 | return 0; |
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81 | } |
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82 | |
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83 | alpha = acos( cos_val ); |
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84 | |
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85 | // Call the IGOR library function to get the kernel |
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86 | answer = CoreShellCylKernel(q, pars->radius, pars->thickness, |
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87 | pars->core_sld,pars->shell_sld, |
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88 | pars->solvent_sld, pars->length/2.0, alpha) / fabs(sin(alpha)); |
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89 | |
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90 | //normalize by cylinder volume |
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91 | vol=pi*(pars->radius+pars->thickness) |
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92 | *(pars->radius+pars->thickness) |
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93 | *(pars->length+2.0*pars->thickness); |
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94 | answer /= vol; |
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95 | |
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96 | //convert to [cm-1] |
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97 | answer *= 1.0e8; |
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98 | |
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99 | //Scale |
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100 | answer *= pars->scale; |
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101 | |
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102 | // add in the background |
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103 | answer += pars->background; |
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104 | |
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105 | return answer; |
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106 | } |
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107 | |
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108 | /** |
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109 | * Function to evaluate 2D scattering function |
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110 | * @param pars: parameters of the core-shell cylinder |
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111 | * @param q: q-value |
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112 | * @return: function value |
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113 | */ |
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114 | static double core_shell_cylinder_analytical_2DXY(CoreShellCylinderParameters *pars, double qx, double qy) { |
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115 | double q; |
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116 | q = sqrt(qx*qx+qy*qy); |
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117 | return core_shell_cylinder_analytical_2D_scaled(pars, q, qx/q, qy/q); |
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118 | } |
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119 | |
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120 | |
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121 | CoreShellCylinderModel :: CoreShellCylinderModel() { |
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122 | scale = Parameter(1.0); |
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123 | radius = Parameter(20.0, true); |
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124 | radius.set_min(0.0); |
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125 | thickness = Parameter(10.0, true); |
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126 | thickness.set_min(0.0); |
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127 | length = Parameter(400.0, true); |
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128 | length.set_min(0.0); |
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129 | core_sld = Parameter(1.e-6); |
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130 | shell_sld = Parameter(4.e-6); |
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131 | solvent_sld= Parameter(1.e-6); |
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132 | background = Parameter(0.0); |
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133 | axis_theta = Parameter(90.0, true); |
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134 | axis_phi = Parameter(0.0, true); |
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135 | } |
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136 | |
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137 | /** |
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138 | * Function to evaluate 1D scattering function |
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139 | * The NIST IGOR library is used for the actual calculation. |
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140 | * @param q: q-value |
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141 | * @return: function value |
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142 | */ |
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143 | double CoreShellCylinderModel :: operator()(double q) { |
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144 | double dp[8]; |
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145 | |
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146 | dp[0] = scale(); |
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147 | dp[1] = radius(); |
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148 | dp[2] = thickness(); |
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149 | dp[3] = length(); |
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150 | dp[4] = core_sld(); |
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151 | dp[5] = shell_sld(); |
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152 | dp[6] = solvent_sld(); |
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153 | dp[7] = 0.0; |
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154 | |
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155 | // Get the dispersion points for the radius |
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156 | vector<WeightPoint> weights_rad; |
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157 | radius.get_weights(weights_rad); |
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158 | |
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159 | // Get the dispersion points for the thickness |
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160 | vector<WeightPoint> weights_thick; |
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161 | thickness.get_weights(weights_thick); |
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162 | |
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163 | // Get the dispersion points for the length |
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164 | vector<WeightPoint> weights_len; |
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165 | length.get_weights(weights_len); |
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166 | |
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167 | // Perform the computation, with all weight points |
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168 | double sum = 0.0; |
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169 | double norm = 0.0; |
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170 | double vol = 0.0; |
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171 | |
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172 | // Loop over radius weight points |
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173 | for(size_t i=0; i<weights_rad.size(); i++) { |
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174 | dp[1] = weights_rad[i].value; |
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175 | |
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176 | // Loop over length weight points |
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177 | for(size_t j=0; j<weights_len.size(); j++) { |
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178 | dp[3] = weights_len[j].value; |
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179 | |
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180 | // Loop over thickness weight points |
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181 | for(size_t k=0; k<weights_thick.size(); k++) { |
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182 | dp[2] = weights_thick[k].value; |
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183 | //Un-normalize by volume |
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184 | sum += weights_rad[i].weight |
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185 | * weights_len[j].weight |
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186 | * weights_thick[k].weight |
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187 | * CoreShellCylinder(dp, q) |
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188 | * pow(weights_rad[i].value+weights_thick[k].value,2) |
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189 | *(weights_len[j].value+2.0*weights_thick[k].value); |
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190 | //Find average volume |
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191 | vol += weights_rad[i].weight |
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192 | * weights_len[j].weight |
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193 | * weights_thick[k].weight |
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194 | * pow(weights_rad[i].value+weights_thick[k].value,2) |
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195 | *(weights_len[j].value+2.0*weights_thick[k].value); |
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196 | norm += weights_rad[i].weight |
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197 | * weights_len[j].weight |
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198 | * weights_thick[k].weight; |
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199 | } |
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200 | } |
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201 | } |
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202 | |
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203 | if (vol != 0.0 && norm != 0.0) { |
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204 | //Re-normalize by avg volume |
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205 | sum = sum/(vol/norm);} |
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206 | |
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207 | return sum/norm + background(); |
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208 | } |
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209 | |
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210 | /** |
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211 | * Function to evaluate 2D scattering function |
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212 | * @param q_x: value of Q along x |
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213 | * @param q_y: value of Q along y |
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214 | * @return: function value |
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215 | */ |
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216 | double CoreShellCylinderModel :: operator()(double qx, double qy) { |
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217 | CoreShellCylinderParameters dp; |
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218 | // Fill parameter array |
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219 | dp.scale = scale(); |
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220 | dp.radius = radius(); |
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221 | dp.thickness = thickness(); |
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222 | dp.length = length(); |
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223 | dp.core_sld = core_sld(); |
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224 | dp.shell_sld = shell_sld(); |
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225 | dp.solvent_sld= solvent_sld(); |
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226 | dp.background = 0.0; |
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227 | dp.axis_theta = axis_theta(); |
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228 | dp.axis_phi = axis_phi(); |
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229 | |
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230 | // Get the dispersion points for the radius |
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231 | vector<WeightPoint> weights_rad; |
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232 | radius.get_weights(weights_rad); |
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233 | |
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234 | // Get the dispersion points for the thickness |
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235 | vector<WeightPoint> weights_thick; |
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236 | thickness.get_weights(weights_thick); |
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237 | |
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238 | // Get the dispersion points for the length |
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239 | vector<WeightPoint> weights_len; |
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240 | length.get_weights(weights_len); |
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241 | |
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242 | // Get angular averaging for theta |
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243 | vector<WeightPoint> weights_theta; |
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244 | axis_theta.get_weights(weights_theta); |
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245 | |
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246 | // Get angular averaging for phi |
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247 | vector<WeightPoint> weights_phi; |
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248 | axis_phi.get_weights(weights_phi); |
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249 | |
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250 | // Perform the computation, with all weight points |
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251 | double sum = 0.0; |
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252 | double norm = 0.0; |
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253 | double norm_vol = 0.0; |
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254 | double vol = 0.0; |
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255 | double pi = 4.0*atan(1.0); |
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256 | // Loop over radius weight points |
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257 | for(size_t i=0; i<weights_rad.size(); i++) { |
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258 | dp.radius = weights_rad[i].value; |
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259 | |
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260 | |
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261 | // Loop over length weight points |
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262 | for(size_t j=0; j<weights_len.size(); j++) { |
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263 | dp.length = weights_len[j].value; |
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264 | |
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265 | // Loop over thickness weight points |
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266 | for(size_t m=0; m<weights_thick.size(); m++) { |
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267 | dp.thickness = weights_thick[m].value; |
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268 | |
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269 | // Average over theta distribution |
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270 | for(size_t k=0; k<weights_theta.size(); k++) { |
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271 | dp.axis_theta = weights_theta[k].value; |
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272 | |
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273 | // Average over phi distribution |
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274 | for(size_t l=0; l<weights_phi.size(); l++) { |
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275 | dp.axis_phi = weights_phi[l].value; |
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276 | //Un-normalize by volume |
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277 | double _ptvalue = weights_rad[i].weight |
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278 | * weights_len[j].weight |
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279 | * weights_thick[m].weight |
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280 | * weights_theta[k].weight |
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281 | * weights_phi[l].weight |
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282 | * core_shell_cylinder_analytical_2DXY(&dp, qx, qy) |
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283 | * pow(weights_rad[i].value+weights_thick[m].value,2) |
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284 | *(weights_len[j].value+2.0*weights_thick[m].value); |
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285 | |
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286 | if (weights_theta.size()>1) { |
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287 | _ptvalue *= fabs(sin(weights_theta[k].value*pi/180.0)); |
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288 | } |
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289 | sum += _ptvalue; |
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290 | |
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291 | //Find average volume |
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292 | vol += weights_rad[i].weight |
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293 | * weights_len[j].weight |
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294 | * weights_thick[m].weight |
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295 | * pow(weights_rad[i].value+weights_thick[m].value,2) |
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296 | *(weights_len[j].value+2.0*weights_thick[m].value); |
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297 | //Find norm for volume |
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298 | norm_vol += weights_rad[i].weight |
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299 | * weights_len[j].weight |
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300 | * weights_thick[m].weight; |
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301 | |
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302 | norm += weights_rad[i].weight |
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303 | * weights_len[j].weight |
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304 | * weights_thick[m].weight |
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305 | * weights_theta[k].weight |
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306 | * weights_phi[l].weight; |
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307 | |
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308 | } |
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309 | } |
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310 | } |
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311 | } |
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312 | } |
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313 | // Averaging in theta needs an extra normalization |
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314 | // factor to account for the sin(theta) term in the |
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315 | // integration (see documentation). |
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316 | if (weights_theta.size()>1) norm = norm / asin(1.0); |
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317 | |
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318 | if (vol != 0.0 && norm_vol != 0.0) { |
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319 | //Re-normalize by avg volume |
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320 | sum = sum/(vol/norm_vol);} |
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321 | |
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322 | return sum/norm + background(); |
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323 | } |
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324 | |
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325 | /** |
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326 | * Function to evaluate 2D scattering function |
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327 | * @param pars: parameters of the cylinder |
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328 | * @param q: q-value |
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329 | * @param phi: angle phi |
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330 | * @return: function value |
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331 | */ |
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332 | double CoreShellCylinderModel :: evaluate_rphi(double q, double phi) { |
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333 | double qx = q*cos(phi); |
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334 | double qy = q*sin(phi); |
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335 | return (*this).operator()(qx, qy); |
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336 | } |
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337 | /** |
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338 | * Function to calculate effective radius |
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339 | * @return: effective radius value |
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340 | */ |
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341 | double CoreShellCylinderModel :: calculate_ER() { |
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342 | CoreShellCylinderParameters dp; |
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343 | |
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344 | dp.radius = radius(); |
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345 | dp.thickness = thickness(); |
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346 | dp.length = length(); |
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347 | double rad_out = 0.0; |
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348 | |
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349 | // Perform the computation, with all weight points |
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350 | double sum = 0.0; |
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351 | double norm = 0.0; |
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352 | |
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353 | // Get the dispersion points for the length |
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354 | vector<WeightPoint> weights_length; |
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355 | length.get_weights(weights_length); |
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356 | |
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357 | // Get the dispersion points for the thickness |
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358 | vector<WeightPoint> weights_thickness; |
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359 | thickness.get_weights(weights_thickness); |
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360 | |
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361 | // Get the dispersion points for the radius |
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362 | vector<WeightPoint> weights_radius ; |
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363 | radius.get_weights(weights_radius); |
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364 | |
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365 | // Loop over major shell weight points |
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366 | for(int i=0; i< (int)weights_length.size(); i++) { |
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367 | dp.length = weights_length[i].value; |
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368 | for(int j=0; j< (int)weights_thickness.size(); j++) { |
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369 | dp.thickness = weights_thickness[j].value; |
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370 | for(int k=0; k< (int)weights_radius.size(); k++) { |
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371 | dp.radius = weights_radius[k].value; |
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372 | //Note: output of "DiamCyl( )" is DIAMETER. |
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373 | sum +=weights_length[i].weight * weights_thickness[j].weight |
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374 | * weights_radius[k].weight*DiamCyl(dp.length+2.0*dp.thickness,dp.radius+dp.thickness)/2.0; |
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375 | norm += weights_length[i].weight* weights_thickness[j].weight* weights_radius[k].weight; |
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376 | } |
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377 | } |
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378 | } |
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379 | if (norm != 0){ |
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380 | //return the averaged value |
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381 | rad_out = sum/norm;} |
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382 | else{ |
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383 | //return normal value |
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384 | //Note: output of "DiamCyl()" is DIAMETER. |
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385 | rad_out = DiamCyl(dp.length+2.0*dp.thickness,dp.radius+dp.thickness)/2.0;} |
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386 | |
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387 | return rad_out; |
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388 | } |
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389 | double CoreShellCylinderModel :: calculate_VR() { |
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390 | return 1.0; |
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391 | } |
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