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 "bcc.h" |
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27 | |
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28 | extern "C" { |
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29 | #include "libSphere.h" |
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30 | } |
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31 | |
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32 | // Convenience structure |
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33 | typedef struct { |
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34 | double scale; |
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35 | double dnn; |
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36 | double d_factor; |
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37 | double radius; |
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38 | double sldSph; |
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39 | double sldSolv; |
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40 | double background; |
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41 | double theta; |
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42 | double phi; |
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43 | double psi; |
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44 | |
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45 | } BCParameters; |
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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 BCCCrystalModel |
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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 bc_analytical_2D_scaled(BCParameters *pars, double q, double q_x, double q_y) { |
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56 | double b3_x, b3_y, b1_x, b1_y, b2_x, b2_y; //b3_z, |
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57 | double q_z; |
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58 | double cos_val_b3, cos_val_b2, cos_val_b1; |
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59 | double a1_dot_q, a2_dot_q,a3_dot_q; |
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60 | double answer; |
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61 | double Pi = 4.0*atan(1.0); |
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62 | double aa, Da, qDa_2, latticeScale, Zq, Fkq, Fkq_2; |
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63 | |
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64 | //convert angle degree to radian |
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65 | double pi = 4.0*atan(1.0); |
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66 | double theta = pars->theta * pi/180.0; |
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67 | double phi = pars->phi * pi/180.0; |
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68 | double psi = pars->psi * pi/180.0; |
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69 | |
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70 | double dp[5]; |
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71 | dp[0] = 1.0; |
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72 | dp[1] = pars->radius; |
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73 | dp[2] = pars->sldSph; |
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74 | dp[3] = pars->sldSolv; |
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75 | dp[4] = 0.0; |
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76 | |
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77 | aa = pars->dnn; |
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78 | Da = pars->d_factor*aa; |
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79 | qDa_2 = pow(q*Da,2.0); |
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80 | |
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81 | //the occupied volume of the lattice |
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82 | latticeScale = 2.0*(4.0/3.0)*Pi*(dp[1]*dp[1]*dp[1])/pow(aa/sqrt(3.0/4.0),3.0); |
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83 | // q vector |
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84 | q_z = 0.0; // for SANS; assuming qz is negligible |
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85 | /// Angles here are respect to detector coordinate |
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86 | /// instead of against q coordinate(PRB 36(46), 3(6), 1754(3854)) |
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87 | // b3 axis orientation |
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88 | b3_x = cos(theta) * cos(phi); |
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89 | b3_y = sin(theta); |
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90 | //b3_z = -cos(theta) * sin(phi); |
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91 | cos_val_b3 = b3_x*q_x + b3_y*q_y;// + b3_z*q_z; |
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92 | |
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93 | //alpha = acos(cos_val_b3); |
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94 | // b1 axis orientation |
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95 | b1_x = -cos(phi)*sin(psi) * sin(theta)+sin(phi)*cos(psi); |
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96 | b1_y = sin(psi)*cos(theta); |
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97 | cos_val_b1 = b1_x*q_x + b1_y*q_y; |
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98 | // b2 axis orientation |
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99 | b2_x = -sin(theta)*cos(psi)*cos(phi)-sin(psi)*sin(phi); |
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100 | b2_y = cos(theta)*cos(psi); |
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101 | cos_val_b2 = b2_x*q_x + b2_y*q_y; |
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102 | |
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103 | // The following test should always pass |
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104 | if (fabs(cos_val_b3)>1.0) { |
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105 | //printf("bcc_ana_2D: Unexpected error: cos()>1\n"); |
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106 | cos_val_b3 = 1.0; |
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107 | } |
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108 | if (fabs(cos_val_b2)>1.0) { |
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109 | //printf("bcc_ana_2D: Unexpected error: cos()>1\n"); |
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110 | cos_val_b2 = 1.0; |
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111 | } |
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112 | if (fabs(cos_val_b1)>1.0) { |
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113 | //printf("bcc_ana_2D: Unexpected error: cos()>1\n"); |
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114 | cos_val_b1 = 1.0; |
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115 | } |
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116 | // Compute the angle btw vector q and the a3 axis |
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117 | a3_dot_q = 0.5*aa*q*(cos_val_b2+cos_val_b1-cos_val_b3); |
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118 | |
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119 | // a1 axis |
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120 | a1_dot_q = 0.5*aa*q*(cos_val_b3+cos_val_b2-cos_val_b1); |
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121 | |
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122 | // a2 axis |
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123 | a2_dot_q = 0.5*aa*q*(cos_val_b3+cos_val_b1-cos_val_b2); |
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124 | |
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125 | |
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126 | // Get Fkq and Fkq_2 |
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127 | Fkq = exp(-0.5*pow(Da/aa,2.0)*(a1_dot_q*a1_dot_q+a2_dot_q*a2_dot_q+a3_dot_q*a3_dot_q)); |
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128 | Fkq_2 = Fkq*Fkq; |
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129 | // Call Zq=Z1*Z2*Z3 |
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130 | Zq = (1.0-Fkq_2)/(1.0-2.0*Fkq*cos(a1_dot_q)+Fkq_2); |
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131 | Zq *= (1.0-Fkq_2)/(1.0-2.0*Fkq*cos(a2_dot_q)+Fkq_2); |
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132 | Zq *= (1.0-Fkq_2)/(1.0-2.0*Fkq*cos(a3_dot_q)+Fkq_2); |
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133 | |
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134 | // Use SphereForm directly from libigor |
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135 | answer = SphereForm(dp,q)*Zq; |
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136 | |
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137 | //consider scales |
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138 | answer *= latticeScale * pars->scale; |
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139 | |
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140 | // This FIXES a singualrity the kernel in libigor. |
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141 | if ( answer == INFINITY || answer == NAN){ |
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142 | answer = 0.0; |
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143 | } |
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144 | |
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145 | // add background |
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146 | answer += pars->background; |
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147 | |
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148 | return answer; |
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149 | } |
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150 | |
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151 | /** |
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152 | * Function to evaluate 2D scattering function |
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153 | * @param pars: parameters of the BCC_ParaCrystal |
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154 | * @param q: q-value |
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155 | * @return: function value |
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156 | */ |
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157 | static double bc_analytical_2DXY(BCParameters *pars, double qx, double qy){ |
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158 | double q; |
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159 | q = sqrt(qx*qx+qy*qy); |
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160 | return bc_analytical_2D_scaled(pars, q, qx/q, qy/q); |
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161 | } |
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162 | |
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163 | BCCrystalModel :: BCCrystalModel() { |
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164 | scale = Parameter(1.0); |
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165 | dnn = Parameter(220.0); |
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166 | d_factor = Parameter(0.06); |
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167 | radius = Parameter(40.0, true); |
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168 | radius.set_min(0.0); |
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169 | sldSph = Parameter(3.0e-6); |
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170 | sldSolv = Parameter(6.3e-6); |
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171 | background = Parameter(0.0); |
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172 | theta = Parameter(0.0, true); |
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173 | phi = Parameter(0.0, true); |
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174 | psi = Parameter(0.0, true); |
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175 | } |
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176 | |
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177 | /** |
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178 | * Function to evaluate 1D scattering function |
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179 | * The NIST IGOR library is used for the actual calculation. |
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180 | * @param q: q-value |
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181 | * @return: function value |
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182 | */ |
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183 | double BCCrystalModel :: operator()(double q) { |
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184 | double dp[7]; |
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185 | |
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186 | // Fill parameter array for IGOR library |
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187 | // Add the background after averaging |
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188 | dp[0] = scale(); |
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189 | dp[1] = dnn(); |
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190 | dp[2] = d_factor(); |
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191 | dp[3] = radius(); |
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192 | dp[4] = sldSph(); |
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193 | dp[5] = sldSolv(); |
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194 | dp[6] = 0.0; |
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195 | |
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196 | // Get the dispersion points for the radius |
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197 | vector<WeightPoint> weights_rad; |
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198 | radius.get_weights(weights_rad); |
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199 | |
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200 | // Perform the computation, with all weight points |
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201 | double sum = 0.0; |
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202 | double norm = 0.0; |
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203 | double vol = 0.0; |
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204 | double result; |
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205 | |
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206 | // Loop over radius weight points |
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207 | for(size_t i=0; i<weights_rad.size(); i++) { |
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208 | dp[3] = weights_rad[i].value; |
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209 | |
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210 | //Un-normalize SphereForm by volume |
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211 | result = BCC_ParaCrystal(dp, q) * pow(weights_rad[i].value,3); |
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212 | // This FIXES a singualrity in the kernel in libigor. |
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213 | if ( result == INFINITY || result == NAN){ |
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214 | result = 0.0; |
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215 | } |
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216 | sum += weights_rad[i].weight |
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217 | * result; |
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218 | //Find average volume |
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219 | vol += weights_rad[i].weight |
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220 | * pow(weights_rad[i].value,3); |
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221 | |
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222 | norm += weights_rad[i].weight; |
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223 | } |
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224 | |
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225 | if (vol != 0.0 && norm != 0.0) { |
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226 | //Re-normalize by avg volume |
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227 | sum = sum/(vol/norm);} |
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228 | return sum/norm + background(); |
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229 | } |
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230 | |
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231 | /** |
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232 | * Function to evaluate 2D scattering function |
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233 | * @param q_x: value of Q along x |
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234 | * @param q_y: value of Q along y |
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235 | * @return: function value |
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236 | */ |
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237 | double BCCrystalModel :: operator()(double qx, double qy) { |
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238 | BCParameters dp; |
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239 | dp.scale = scale(); |
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240 | dp.dnn = dnn(); |
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241 | dp.d_factor = d_factor(); |
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242 | dp.radius = radius(); |
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243 | dp.sldSph = sldSph(); |
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244 | dp.sldSolv = sldSolv(); |
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245 | dp.background = 0.0; |
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246 | dp.theta = theta(); |
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247 | dp.phi = phi(); |
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248 | dp.psi = psi(); |
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249 | double pi = 4.0*atan(1.0); |
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250 | // Get the dispersion points for the radius |
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251 | vector<WeightPoint> weights_rad; |
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252 | radius.get_weights(weights_rad); |
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253 | |
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254 | // Get angular averaging for theta |
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255 | vector<WeightPoint> weights_theta; |
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256 | theta.get_weights(weights_theta); |
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257 | |
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258 | // Get angular averaging for phi |
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259 | vector<WeightPoint> weights_phi; |
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260 | phi.get_weights(weights_phi); |
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261 | |
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262 | // Get angular averaging for psi |
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263 | vector<WeightPoint> weights_psi; |
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264 | psi.get_weights(weights_psi); |
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265 | |
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266 | // Perform the computation, with all weight points |
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267 | double sum = 0.0; |
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268 | double norm = 0.0; |
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269 | double norm_vol = 0.0; |
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270 | double vol = 0.0; |
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271 | |
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272 | // Loop over radius weight points |
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273 | for(size_t i=0; i<weights_rad.size(); i++) { |
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274 | dp.radius = weights_rad[i].value; |
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275 | // Average over theta distribution |
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276 | for(size_t j=0; j< weights_theta.size(); j++) { |
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277 | dp.theta = weights_theta[j].value; |
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278 | // Average over phi distribution |
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279 | for(size_t k=0; k< weights_phi.size(); k++) { |
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280 | dp.phi = weights_phi[k].value; |
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281 | // Average over phi distribution |
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282 | for(size_t l=0; l< weights_psi.size(); l++) { |
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283 | dp.psi = weights_psi[l].value; |
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284 | //Un-normalize SphereForm by volume |
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285 | double _ptvalue = weights_rad[i].weight |
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286 | * weights_theta[j].weight |
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287 | * weights_phi[k].weight |
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288 | * weights_psi[l].weight |
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289 | * bc_analytical_2DXY(&dp, qx, qy); |
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290 | //* pow(weights_rad[i].value,3.0); |
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291 | // Consider when there is infinity or nan. |
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292 | // Actual value for this singular point are typically zero. |
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293 | if ( _ptvalue == INFINITY || _ptvalue == NAN){ |
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294 | _ptvalue = 0.0; |
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295 | } |
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296 | if (weights_theta.size()>1) { |
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297 | _ptvalue *= fabs(cos(weights_theta[j].value*pi/180.0)); |
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298 | } |
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299 | sum += _ptvalue; |
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300 | // This model dose not need the volume of spheres correction!!! |
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301 | norm += weights_rad[i].weight |
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302 | * weights_theta[j].weight |
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303 | * weights_phi[k].weight |
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304 | * weights_psi[l].weight; |
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305 | } |
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306 | } |
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307 | } |
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308 | } |
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309 | // Averaging in theta needs an extra normalization |
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310 | // factor to account for the sin(theta) term in the |
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311 | // integration (see documentation). |
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312 | if (weights_theta.size()>1) norm = norm / asin(1.0); |
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313 | |
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314 | if (vol != 0.0 && norm_vol != 0.0) { |
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315 | //Re-normalize by avg volume |
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316 | sum = sum/(vol/norm_vol);} |
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317 | |
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318 | return sum/norm + background(); |
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319 | } |
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320 | |
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321 | /** |
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322 | * Function to evaluate 2D scattering function |
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323 | * @param pars: parameters of the BCCCrystal |
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324 | * @param q: q-value |
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325 | * @param phi: angle phi |
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326 | * @return: function value |
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327 | */ |
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328 | double BCCrystalModel :: evaluate_rphi(double q, double phi) { |
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329 | return (*this).operator()(q); |
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330 | } |
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331 | |
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332 | /** |
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333 | * Function to calculate effective radius |
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334 | * @return: effective radius value |
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335 | */ |
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336 | double BCCrystalModel :: calculate_ER() { |
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337 | //NOT implemented yet!!! |
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338 | return 0.0; |
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339 | } |
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340 | double BCCrystalModel :: calculate_VR() { |
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341 | return 1.0; |
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342 | } |
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