[230f479] | 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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