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 "GaussWeights.h" |
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30 | #include "barbell.h" |
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31 | } |
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32 | |
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33 | // Convenience parameter structure |
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34 | typedef struct { |
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35 | double scale; |
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36 | double rad_bar; |
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37 | double len_bar; |
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38 | double rad_bell; |
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39 | double sld_barbell; |
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40 | double sld_solv; |
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41 | double background; |
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42 | double theta; |
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43 | double phi; |
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44 | } BarBellParameters; |
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45 | |
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46 | BarBellModel :: BarBellModel() { |
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47 | scale = Parameter(1.0); |
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48 | rad_bar = Parameter(20.0); |
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49 | rad_bar.set_min(0.0); |
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50 | len_bar = Parameter(400.0, true); |
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51 | len_bar.set_min(0.0); |
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52 | rad_bell = Parameter(40.0); |
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53 | rad_bell.set_min(0.0); |
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54 | sld_barbell = Parameter(1.0e-6); |
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55 | sld_solv = Parameter(6.3e-6); |
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56 | background = Parameter(0.0); |
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57 | theta = Parameter(0.0, true); |
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58 | phi = Parameter(0.0, true); |
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59 | } |
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60 | |
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61 | double barbell2d_kernel(double dp[], double q, double alpha) { |
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62 | int j; |
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63 | double Pi; |
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64 | double scale,contr,bkg,sldc,slds; |
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65 | double len,rad,hDist,endRad; |
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66 | int nordj=76; |
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67 | double zi=alpha,yyy,answer; //running tally of integration |
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68 | double summj,vaj,vbj,zij; //for the inner integration |
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69 | double arg1,arg2,inner,be; |
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70 | |
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71 | |
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72 | scale = dp[0]; |
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73 | rad = dp[1]; |
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74 | len = dp[2]; |
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75 | endRad = dp[3]; |
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76 | sldc = dp[4]; |
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77 | slds = dp[5]; |
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78 | bkg = dp[6]; |
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79 | |
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80 | hDist = sqrt(fabs(endRad*endRad-rad*rad)); //by definition for this model |
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81 | |
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82 | contr = sldc-slds; |
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83 | |
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84 | Pi = 4.0*atan(1.0); |
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85 | vaj = -1.0*hDist/endRad; |
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86 | vbj = 1.0; //endpoints of inner integral |
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87 | |
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88 | summj=0.0; |
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89 | |
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90 | for(j=0;j<nordj;j++) { |
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91 | //20 gauss points for the inner integral |
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92 | zij = ( Gauss76Z[j]*(vbj-vaj) + vaj + vbj )/2.0; //the "t" dummy |
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93 | yyy = Gauss76Wt[j] * Dumb_kernel(dp,q,zij,zi); //uses the same Kernel as the Dumbbell, here L>0 |
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94 | summj += yyy; |
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95 | } |
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96 | //now calculate the value of the inner integral |
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97 | inner = (vbj-vaj)/2.0*summj; |
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98 | inner *= 4.0*Pi*endRad*endRad*endRad; |
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99 | |
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100 | //now calculate outer integrand |
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101 | arg1 = q*len/2.0*cos(zi); |
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102 | arg2 = q*rad*sin(zi); |
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103 | yyy = inner; |
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104 | |
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105 | if(arg2 == 0) { |
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106 | be = 0.5; |
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107 | } else { |
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108 | be = NR_BessJ1(arg2)/arg2; |
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109 | } |
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110 | |
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111 | if(arg1 == 0.0) { //limiting value of sinc(0) is 1; sinc is not defined in math.h |
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112 | yyy += Pi*rad*rad*len*2.0*be; |
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113 | } else { |
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114 | yyy += Pi*rad*rad*len*sin(arg1)/arg1*2.0*be; |
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115 | } |
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116 | yyy *= yyy; //sin(zi); |
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117 | answer = yyy; |
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118 | |
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119 | |
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120 | answer /= Pi*rad*rad*len + 2.0*Pi*(2.0*endRad*endRad*endRad/3.0+endRad*endRad*hDist-hDist*hDist*hDist/3.0); //divide by volume |
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121 | answer *= 1.0e8; //convert to cm^-1 |
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122 | answer *= contr*contr; |
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123 | answer *= scale; |
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124 | answer += bkg; |
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125 | |
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126 | return answer; |
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127 | } |
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128 | |
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129 | /** |
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130 | * Function to evaluate 2D scattering function |
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131 | * @param pars: parameters of the BarBell |
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132 | * @param q: q-value |
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133 | * @param q_x: q_x / q |
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134 | * @param q_y: q_y / q |
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135 | * @return: function value |
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136 | */ |
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137 | static double barbell_analytical_2D_scaled(BarBellParameters *pars, double q, double q_x, double q_y) { |
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138 | double cyl_x, cyl_y;//, cyl_z; |
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139 | //double q_z; |
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140 | double alpha, cos_val; |
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141 | double answer; |
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142 | double dp[7]; |
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143 | //convert angle degree to radian |
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144 | double pi = 4.0*atan(1.0); |
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145 | double theta = pars->theta * pi/180.0; |
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146 | double phi = pars->phi * pi/180.0; |
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147 | |
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148 | dp[0] = pars->scale; |
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149 | dp[1] = pars->rad_bar; |
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150 | dp[2] = pars->len_bar; |
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151 | dp[3] = pars->rad_bell; |
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152 | dp[4] = pars->sld_barbell; |
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153 | dp[5] = pars->sld_solv; |
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154 | dp[6] = pars->background; |
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155 | |
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156 | |
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157 | //double Pi = 4.0*atan(1.0); |
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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 | |
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163 | // q vector |
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164 | //q_z = 0; |
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165 | |
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166 | // Compute the angle btw vector q and the |
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167 | // axis of the cylinder |
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168 | cos_val = cyl_x*q_x + cyl_y*q_y;// + cyl_z*q_z; |
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169 | |
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170 | // The following test should always pass |
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171 | if (fabs(cos_val)>1.0) { |
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172 | printf("cyl_ana_2D: Unexpected error: cos(alpha)>1\n"); |
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173 | return 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 | |
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180 | answer = barbell2d_kernel(dp, q, alpha); |
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181 | |
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182 | |
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183 | return answer; |
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184 | |
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185 | } |
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186 | |
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187 | /** |
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188 | * Function to evaluate 2D scattering function |
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189 | * @param pars: parameters of the BarBell |
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190 | * @param q: q-value |
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191 | * @return: function value |
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192 | */ |
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193 | static double barbell_analytical_2DXY(BarBellParameters *pars, double qx, double qy){ |
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194 | double q; |
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195 | q = sqrt(qx*qx+qy*qy); |
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196 | return barbell_analytical_2D_scaled(pars, q, qx/q, qy/q); |
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197 | } |
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198 | |
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199 | /** |
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200 | * Function to evaluate 1D scattering function |
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201 | * The NIST IGOR library is used for the actual calculation. |
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202 | * @param q: q-value |
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203 | * @return: function value |
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204 | */ |
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205 | double BarBellModel :: operator()(double q) { |
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206 | double dp[7]; |
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207 | |
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208 | // Fill parameter array for IGOR library |
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209 | // Add the background after averaging |
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210 | dp[0] = scale(); |
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211 | dp[1] = rad_bar(); |
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212 | dp[2] = len_bar(); |
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213 | dp[3] = rad_bell(); |
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214 | dp[4] = sld_barbell(); |
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215 | dp[5] = sld_solv(); |
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216 | dp[6] = 0.0; |
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217 | |
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218 | // Get the dispersion points for the rad_bar |
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219 | vector<WeightPoint> weights_rad_bar; |
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220 | rad_bar.get_weights(weights_rad_bar); |
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221 | // Get the dispersion points for the len_bar |
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222 | vector<WeightPoint> weights_len_bar; |
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223 | len_bar.get_weights(weights_len_bar); |
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224 | // Get the dispersion points for the rad_bell |
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225 | vector<WeightPoint> weights_rad_bell; |
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226 | rad_bell.get_weights(weights_rad_bell); |
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227 | |
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228 | // Perform the computation, with all weight points |
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229 | double sum = 0.0; |
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230 | double norm = 0.0; |
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231 | double vol = 0.0; |
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232 | double pi,hDist,result; |
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233 | double vol_i = 0.0; |
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234 | pi = 4.0*atan(1.0); |
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235 | // Loop over radius weight points |
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236 | for(size_t i=0; i<weights_rad_bar.size(); i++) { |
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237 | dp[1] = weights_rad_bar[i].value; |
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238 | for(size_t j=0; j<weights_len_bar.size(); j++) { |
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239 | dp[2] = weights_len_bar[j].value; |
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240 | for(size_t k=0; k<weights_rad_bell.size(); k++) { |
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241 | dp[3] = weights_rad_bell[k].value; |
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242 | |
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243 | //Un-normalize SphereForm by volume |
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244 | hDist = sqrt(fabs(dp[3]*dp[3]-dp[1]*dp[1])); |
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245 | vol_i = pi*dp[1]*dp[1]*dp[2]+2.0*pi*(2.0*dp[3]*dp[3]*dp[3]/3.0 |
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246 | +dp[3]*dp[3]*hDist-hDist*hDist*hDist/3.0); |
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247 | result = Barbell(dp, q) * vol_i; |
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248 | // This FIXES a singualrity the kernel in libigor. |
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249 | if ( result == INFINITY || result == NAN){ |
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250 | result = 0.0; |
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251 | } |
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252 | sum += weights_rad_bar[i].weight*weights_len_bar[j].weight*weights_rad_bell[k].weight |
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253 | * result; |
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254 | //Find average volume |
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255 | vol += weights_rad_bar[i].weight*weights_len_bar[j].weight*weights_rad_bell[k].weight |
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256 | * vol_i; |
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257 | |
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258 | norm += weights_rad_bar[i].weight*weights_len_bar[j].weight*weights_rad_bell[k].weight; |
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259 | } |
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260 | } |
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261 | } |
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262 | |
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263 | if (vol != 0.0 && norm != 0.0) { |
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264 | //Re-normalize by avg volume |
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265 | sum = sum/(vol/norm);} |
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266 | return sum/norm + background(); |
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267 | } |
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268 | |
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269 | /** |
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270 | * Function to evaluate 2D scattering function |
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271 | * @param q_x: value of Q along x |
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272 | * @param q_y: value of Q along y |
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273 | * @return: function value |
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274 | */ |
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275 | double BarBellModel :: operator()(double qx, double qy) { |
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276 | BarBellParameters dp; |
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277 | |
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278 | // Fill parameter array for IGOR library |
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279 | // Add the background after averaging |
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280 | dp.scale = scale(); |
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281 | dp.rad_bar = rad_bar(); |
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282 | dp.len_bar = len_bar(); |
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283 | dp.rad_bell = rad_bell(); |
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284 | dp.sld_barbell = sld_barbell(); |
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285 | dp.sld_solv = sld_solv(); |
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286 | dp.background = 0.0; |
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287 | dp.theta = theta(); |
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288 | dp.phi = phi(); |
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289 | |
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290 | // Get the dispersion points for the rad_bar |
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291 | vector<WeightPoint> weights_rad_bar; |
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292 | rad_bar.get_weights(weights_rad_bar); |
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293 | |
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294 | // Get the dispersion points for the len_bar |
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295 | vector<WeightPoint> weights_len_bar; |
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296 | len_bar.get_weights(weights_len_bar); |
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297 | |
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298 | // Get the dispersion points for the rad_bell |
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299 | vector<WeightPoint> weights_rad_bell; |
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300 | rad_bell.get_weights(weights_rad_bell); |
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301 | |
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302 | // Get angular averaging for theta |
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303 | vector<WeightPoint> weights_theta; |
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304 | theta.get_weights(weights_theta); |
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305 | |
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306 | // Get angular averaging for phi |
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307 | vector<WeightPoint> weights_phi; |
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308 | phi.get_weights(weights_phi); |
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309 | |
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310 | |
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311 | // Perform the computation, with all weight points |
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312 | double sum = 0.0; |
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313 | double norm = 0.0; |
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314 | double norm_vol = 0.0; |
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315 | double vol = 0.0; |
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316 | double pi,hDist; |
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317 | double vol_i = 0.0; |
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318 | pi = 4.0*atan(1.0); |
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319 | |
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320 | // Loop over radius weight points |
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321 | for(size_t i=0; i<weights_rad_bar.size(); i++) { |
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322 | dp.rad_bar = weights_rad_bar[i].value; |
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323 | for(size_t j=0; j<weights_len_bar.size(); j++) { |
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324 | dp.len_bar = weights_len_bar[j].value; |
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325 | for(size_t k=0; k<weights_rad_bell.size(); k++) { |
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326 | dp.rad_bell = weights_rad_bell[k].value; |
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327 | // Average over theta distribution |
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328 | for(size_t l=0; l< weights_theta.size(); l++) { |
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329 | dp.theta = weights_theta[l].value; |
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330 | // Average over phi distribution |
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331 | for(size_t m=0; m< weights_phi.size(); m++) { |
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332 | dp.phi = weights_phi[m].value; |
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333 | //Un-normalize Form by volume |
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334 | hDist = -sqrt(fabs(dp.rad_bell*dp.rad_bell-dp.rad_bar*dp.rad_bar)); |
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335 | vol_i = pi*dp.rad_bar*dp.rad_bar*dp.len_bar+2.0*pi/3.0*((dp.rad_bell-hDist)*(dp.rad_bell-hDist)* |
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336 | (2*dp.rad_bell+hDist)); |
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337 | double _ptvalue = weights_rad_bar[i].weight |
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338 | * weights_len_bar[j].weight |
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339 | * weights_rad_bell[k].weight |
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340 | * weights_theta[l].weight |
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341 | * weights_phi[m].weight |
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342 | * vol_i |
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343 | * barbell_analytical_2DXY(&dp, qx, qy); |
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344 | //* output; |
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345 | //* pow(weights_rad[i].value,3.0); |
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346 | |
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347 | // Consider when there is infinte or nan. |
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348 | if ( _ptvalue == INFINITY || _ptvalue == NAN){ |
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349 | _ptvalue = 0.0; |
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350 | } |
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351 | if (weights_theta.size()>1) { |
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352 | _ptvalue *= fabs(cos(weights_theta[l].value*pi/180.0)); |
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353 | } |
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354 | sum += _ptvalue; |
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355 | // This model dose not need the volume of spheres correction!!! |
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356 | //Find average volume |
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357 | vol += weights_rad_bar[i].weight |
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358 | * weights_len_bar[j].weight |
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359 | * weights_rad_bell[k].weight |
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360 | * vol_i; |
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361 | //Find norm for volume |
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362 | norm_vol += weights_rad_bar[i].weight |
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363 | * weights_len_bar[j].weight |
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364 | * weights_rad_bell[k].weight; |
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365 | |
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366 | norm += weights_rad_bar[i].weight |
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367 | * weights_len_bar[j].weight |
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368 | * weights_rad_bell[k].weight |
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369 | * weights_theta[l].weight |
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370 | * weights_phi[m].weight; |
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371 | } |
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372 | } |
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373 | } |
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374 | } |
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375 | } |
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376 | // Averaging in theta needs an extra normalization |
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377 | // factor to account for the sin(theta) term in the |
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378 | // integration (see documentation). |
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379 | if (weights_theta.size()>1) norm = norm / asin(1.0); |
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380 | |
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381 | if (vol != 0.0 && norm_vol != 0.0) { |
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382 | //Re-normalize by avg volume |
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383 | sum = sum/(vol/norm_vol);} |
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384 | |
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385 | return sum/norm + background(); |
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386 | } |
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387 | |
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388 | /** |
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389 | * Function to evaluate 2D scattering function |
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390 | * @param pars: parameters of the SCCrystal |
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391 | * @param q: q-value |
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392 | * @param phi: angle phi |
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393 | * @return: function value |
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394 | */ |
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395 | double BarBellModel :: evaluate_rphi(double q, double phi) { |
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396 | return (*this).operator()(q); |
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397 | } |
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398 | |
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399 | /** |
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400 | * Function to calculate effective radius |
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401 | * @return: effective radius value |
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402 | */ |
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403 | double BarBellModel :: calculate_ER() { |
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404 | //NOT implemented yet!!! |
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405 | return 0.0; |
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406 | } |
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407 | /** |
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408 | * Function to calculate volf_ratio for shell/tot |
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409 | * @return: volf_ratio value |
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410 | */ |
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411 | double BarBellModel :: calculate_VR() { |
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412 | return 1.0; |
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413 | } |
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