[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 | #include <stdlib.h> |
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| 26 | using namespace std; |
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| 27 | #include "elliptical_cylinder.h" |
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| 28 | |
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| 29 | extern "C" { |
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| 30 | #include "libCylinder.h" |
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| 31 | #include "libStructureFactor.h" |
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| 32 | } |
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| 33 | |
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| 34 | typedef struct { |
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| 35 | double scale; |
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| 36 | double r_minor; |
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| 37 | double r_ratio; |
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| 38 | double length; |
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| 39 | double sldCyl; |
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| 40 | double sldSolv; |
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| 41 | double background; |
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| 42 | double cyl_theta; |
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| 43 | double cyl_phi; |
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| 44 | double cyl_psi; |
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| 45 | } EllipticalCylinderParameters; |
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| 46 | |
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| 47 | |
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| 48 | static double elliptical_cylinder_kernel(EllipticalCylinderParameters *pars, double q, double cos_val, double cos_nu, double cos_mu) { |
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| 49 | double qr; |
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| 50 | double qL; |
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| 51 | double Be,Si; |
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| 52 | double r_major; |
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| 53 | double kernel; |
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| 54 | |
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| 55 | r_major = pars->r_ratio * pars->r_minor; |
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| 56 | |
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| 57 | qr = q*sqrt( r_major*r_major*cos_nu*cos_nu + pars->r_minor*pars->r_minor*cos_mu*cos_mu ); |
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| 58 | qL = q*pars->length*cos_val/2.0; |
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| 59 | |
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| 60 | if (qr==0){ |
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| 61 | Be = 0.5; |
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| 62 | }else{ |
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| 63 | Be = NR_BessJ1(qr)/qr; |
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| 64 | } |
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| 65 | if (qL==0){ |
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| 66 | Si = 1.0; |
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| 67 | }else{ |
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| 68 | Si = sin(qL)/qL; |
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| 69 | } |
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| 70 | |
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| 71 | |
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| 72 | kernel = 2.0*Be * Si; |
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| 73 | return kernel*kernel; |
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| 74 | } |
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| 75 | |
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| 76 | /** |
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| 77 | * Function to evaluate 2D scattering function |
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| 78 | * @param pars: parameters of the cylinder |
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| 79 | * @param q: q-value |
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| 80 | * @param q_x: q_x / q |
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| 81 | * @param q_y: q_y / q |
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| 82 | * @return: function value |
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| 83 | */ |
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| 84 | static double elliptical_cylinder_analytical_2D_scaled(EllipticalCylinderParameters *pars, double q, double q_x, double q_y) { |
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| 85 | double cyl_x, cyl_y;//, cyl_z; |
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| 86 | double ella_x, ella_y, ellb_x, ellb_y; |
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| 87 | //double q_z; |
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| 88 | double vol, cos_val; |
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| 89 | double cos_mu, cos_nu; |
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| 90 | double answer; |
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| 91 | //convert angle degree to radian |
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| 92 | double pi = 4.0*atan(1.0); |
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| 93 | double theta = pars->cyl_theta * pi/180.0; |
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| 94 | double phi = pars->cyl_phi * pi/180.0; |
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| 95 | double psi = pars->cyl_psi * pi/180.0; |
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| 96 | |
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| 97 | //Cylinder orientation |
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| 98 | cyl_x = cos(theta) * cos(phi); |
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| 99 | cyl_y = sin(theta); |
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| 100 | //cyl_z = -cos(theta) * sin(phi); |
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| 101 | |
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| 102 | // q vector |
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| 103 | //q_z = 0; |
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| 104 | |
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| 105 | // Note: cos(alpha) = 0 and 1 will get an |
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| 106 | // undefined value from CylKernel |
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| 107 | //alpha = acos( cos_val ); |
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| 108 | |
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| 109 | //ellipse orientation: |
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| 110 | // the elliptical corss section was transformed and projected |
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| 111 | // into the detector plane already through sin(alpha)and furthermore psi remains as same |
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| 112 | // on the detector plane. |
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| 113 | // So, all we need is to calculate the angle (nu) of the minor axis of the ellipse wrt |
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| 114 | // the wave vector q. |
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| 115 | |
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| 116 | //x- y- component on the detector plane. |
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| 117 | ella_x = -cos(phi)*sin(psi) * sin(theta)+sin(phi)*cos(psi); |
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| 118 | ella_y = sin(psi)*cos(theta); |
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| 119 | ellb_x = -sin(theta)*cos(psi)*cos(phi)-sin(psi)*sin(phi); |
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| 120 | ellb_y = cos(theta)*cos(psi); |
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| 121 | |
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| 122 | // Compute the angle btw vector q and the |
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| 123 | // axis of the cylinder |
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| 124 | cos_val = cyl_x*q_x + cyl_y*q_y;// + cyl_z*q_z; |
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| 125 | |
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| 126 | // calculate the axis of the ellipse wrt q-coord. |
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| 127 | cos_nu = ella_x*q_x + ella_y*q_y; |
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| 128 | cos_mu = ellb_x*q_x + ellb_y*q_y; |
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| 129 | |
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| 130 | // The following test should always pass |
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| 131 | if (fabs(cos_val)>1.0) { |
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| 132 | //printf("cyl_ana_2D: Unexpected error: cos(alpha)>1\n"); |
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| 133 | cos_val = 1.0; |
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| 134 | } |
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| 135 | if (fabs(cos_nu)>1.0) { |
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| 136 | //printf("cyl_ana_2D: Unexpected error: cos(nu)>1\n"); |
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| 137 | cos_nu = 1.0; |
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| 138 | } |
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| 139 | if (fabs(cos_mu)>1.0) { |
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| 140 | //printf("cyl_ana_2D: Unexpected error: cos(nu)>1\n"); |
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| 141 | cos_mu = 1.0; |
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| 142 | } |
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| 143 | answer = elliptical_cylinder_kernel(pars, q, cos_val, cos_nu, cos_mu); |
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| 144 | |
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| 145 | // Multiply by contrast^2 |
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| 146 | answer *= (pars->sldCyl - pars->sldSolv) * (pars->sldCyl - pars->sldSolv); |
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| 147 | |
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| 148 | //normalize by cylinder volume |
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| 149 | //NOTE that for this (Fournet) definition of the integral, one must MULTIPLY by Vcyl |
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| 150 | vol = acos(-1.0) * pars->r_minor * pars->r_minor * pars->r_ratio * pars->length; |
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| 151 | answer *= vol; |
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| 152 | |
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| 153 | //convert to [cm-1] |
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| 154 | answer *= 1.0e8; |
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| 155 | |
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| 156 | //Scale |
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| 157 | answer *= pars->scale; |
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| 158 | |
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| 159 | // add in the background |
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| 160 | answer += pars->background; |
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| 161 | |
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| 162 | return answer; |
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| 163 | } |
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| 164 | |
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| 165 | |
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| 166 | /** |
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| 167 | * Function to evaluate 2D scattering function |
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| 168 | * @param pars: parameters of the cylinder |
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| 169 | * @param q: q-value |
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| 170 | * @return: function value |
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| 171 | */ |
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| 172 | static double elliptical_cylinder_analytical_2DXY(EllipticalCylinderParameters *pars, double qx, double qy) { |
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| 173 | double q; |
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| 174 | q = sqrt(qx*qx+qy*qy); |
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| 175 | return elliptical_cylinder_analytical_2D_scaled(pars, q, qx/q, qy/q); |
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| 176 | } |
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| 177 | |
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| 178 | EllipticalCylinderModel :: EllipticalCylinderModel() { |
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| 179 | scale = Parameter(1.0); |
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| 180 | r_minor = Parameter(20.0, true); |
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| 181 | r_minor.set_min(0.0); |
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| 182 | r_ratio = Parameter(1.5, true); |
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| 183 | r_ratio.set_min(0.0); |
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| 184 | length = Parameter(400.0, true); |
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| 185 | length.set_min(0.0); |
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| 186 | sldCyl = Parameter(4.e-6); |
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| 187 | sldSolv = Parameter(1.e-6); |
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| 188 | background = Parameter(0.0); |
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| 189 | cyl_theta = Parameter(57.325, true); |
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| 190 | cyl_phi = Parameter(0.0, true); |
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| 191 | cyl_psi = Parameter(0.0, true); |
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| 192 | } |
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| 193 | |
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| 194 | /** |
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| 195 | * Function to evaluate 1D scattering function |
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| 196 | * The NIST IGOR library is used for the actual calculation. |
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| 197 | * @param q: q-value |
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| 198 | * @return: function value |
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| 199 | */ |
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| 200 | double EllipticalCylinderModel :: operator()(double q) { |
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| 201 | double dp[7]; |
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| 202 | |
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| 203 | dp[0] = scale(); |
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| 204 | dp[1] = r_minor(); |
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| 205 | dp[2] = r_ratio(); |
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| 206 | dp[3] = length(); |
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| 207 | dp[4] = sldCyl(); |
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| 208 | dp[5] = sldSolv(); |
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| 209 | dp[6] = 0.0; |
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| 210 | |
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| 211 | // Get the dispersion points for the r_minor |
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| 212 | vector<WeightPoint> weights_rad; |
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| 213 | r_minor.get_weights(weights_rad); |
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| 214 | |
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| 215 | // Get the dispersion points for the r_ratio |
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| 216 | vector<WeightPoint> weights_rat; |
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| 217 | r_ratio.get_weights(weights_rat); |
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| 218 | |
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| 219 | // Get the dispersion points for the length |
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| 220 | vector<WeightPoint> weights_len; |
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| 221 | length.get_weights(weights_len); |
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| 222 | |
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| 223 | // Perform the computation, with all weight points |
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| 224 | double sum = 0.0; |
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| 225 | double norm = 0.0; |
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| 226 | double vol = 0.0; |
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| 227 | |
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| 228 | // Loop over r_minor weight points |
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| 229 | for(size_t i=0; i<weights_rad.size(); i++) { |
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| 230 | dp[1] = weights_rad[i].value; |
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| 231 | |
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| 232 | // Loop over r_ratio weight points |
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| 233 | for(size_t j=0; j<weights_rat.size(); j++) { |
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| 234 | dp[2] = weights_rat[j].value; |
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| 235 | |
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| 236 | // Loop over length weight points |
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| 237 | for(size_t k=0; k<weights_len.size(); k++) { |
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| 238 | dp[3] = weights_len[k].value; |
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| 239 | //Un-normalize by volume |
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| 240 | sum += weights_rad[i].weight |
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| 241 | * weights_len[k].weight |
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| 242 | * weights_rat[j].weight |
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| 243 | * EllipCyl20(dp, q) |
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| 244 | * pow(weights_rad[i].value,2) * weights_rat[j].value |
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| 245 | * weights_len[k].value; |
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| 246 | //Find average volume |
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| 247 | vol += weights_rad[i].weight |
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| 248 | * weights_len[k].weight |
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| 249 | * weights_rat[j].weight |
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| 250 | * pow(weights_rad[i].value,2) * weights_rat[j].value |
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| 251 | * weights_len[k].value; |
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| 252 | norm += weights_rad[i].weight |
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| 253 | * weights_len[k].weight |
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| 254 | * weights_rat[j].weight; |
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| 255 | } |
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| 256 | } |
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| 257 | } |
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| 258 | |
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| 259 | if (vol != 0.0 && norm != 0.0) { |
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| 260 | //Re-normalize by avg volume |
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| 261 | sum = sum/(vol/norm);} |
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| 262 | |
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| 263 | return sum/norm + background(); |
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| 264 | } |
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| 265 | |
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| 266 | /** |
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| 267 | * Function to evaluate 2D scattering function |
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| 268 | * @param q_x: value of Q along x |
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| 269 | * @param q_y: value of Q along y |
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| 270 | * @return: function value |
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| 271 | */ |
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| 272 | double EllipticalCylinderModel :: operator()(double qx, double qy) { |
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| 273 | EllipticalCylinderParameters dp; |
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| 274 | // Fill parameter array |
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| 275 | dp.scale = scale(); |
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| 276 | dp.r_minor = r_minor(); |
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| 277 | dp.r_ratio = r_ratio(); |
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| 278 | dp.length = length(); |
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| 279 | dp.sldCyl = sldCyl(); |
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| 280 | dp.sldSolv = sldSolv(); |
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| 281 | dp.background = 0.0; |
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| 282 | dp.cyl_theta = cyl_theta(); |
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| 283 | dp.cyl_phi = cyl_phi(); |
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| 284 | dp.cyl_psi = cyl_psi(); |
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| 285 | |
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| 286 | // Get the dispersion points for the r_minor |
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| 287 | vector<WeightPoint> weights_rad; |
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| 288 | r_minor.get_weights(weights_rad); |
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| 289 | |
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| 290 | // Get the dispersion points for the r_ratio |
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| 291 | vector<WeightPoint> weights_rat; |
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| 292 | r_ratio.get_weights(weights_rat); |
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| 293 | |
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| 294 | // Get the dispersion points for the length |
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| 295 | vector<WeightPoint> weights_len; |
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| 296 | length.get_weights(weights_len); |
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| 297 | |
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| 298 | // Get angular averaging for theta |
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| 299 | vector<WeightPoint> weights_theta; |
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| 300 | cyl_theta.get_weights(weights_theta); |
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| 301 | |
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| 302 | // Get angular averaging for phi |
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| 303 | vector<WeightPoint> weights_phi; |
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| 304 | cyl_phi.get_weights(weights_phi); |
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| 305 | |
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| 306 | // Get angular averaging for psi |
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| 307 | vector<WeightPoint> weights_psi; |
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| 308 | cyl_psi.get_weights(weights_psi); |
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| 309 | |
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| 310 | // Perform the computation, with all weight points |
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| 311 | double sum = 0.0; |
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| 312 | double norm = 0.0; |
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| 313 | double norm_vol = 0.0; |
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| 314 | double vol = 0.0; |
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| 315 | double pi = 4.0*atan(1.0); |
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| 316 | // Loop over minor radius weight points |
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| 317 | for(size_t i=0; i<weights_rad.size(); i++) { |
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| 318 | dp.r_minor = weights_rad[i].value; |
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| 319 | |
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| 320 | |
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| 321 | // Loop over length weight points |
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| 322 | for(size_t j=0; j<weights_len.size(); j++) { |
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| 323 | dp.length = weights_len[j].value; |
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| 324 | |
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| 325 | // Loop over r_ration weight points |
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| 326 | for(size_t m=0; m<weights_rat.size(); m++) { |
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| 327 | dp.r_ratio = weights_rat[m].value; |
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| 328 | |
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| 329 | // Average over theta distribution |
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| 330 | for(size_t k=0; k<weights_theta.size(); k++) { |
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| 331 | dp.cyl_theta = weights_theta[k].value; |
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| 332 | |
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| 333 | // Average over phi distribution |
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| 334 | for(size_t l=0; l<weights_phi.size(); l++) { |
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| 335 | dp.cyl_phi = weights_phi[l].value; |
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| 336 | |
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| 337 | // Average over phi distribution |
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| 338 | for(size_t o=0; o<weights_psi.size(); o++) { |
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| 339 | dp.cyl_psi = weights_psi[o].value; |
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| 340 | //Un-normalize by volume |
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| 341 | double _ptvalue = weights_rad[i].weight |
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| 342 | * weights_len[j].weight |
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| 343 | * weights_rat[m].weight |
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| 344 | * weights_theta[k].weight |
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| 345 | * weights_phi[l].weight |
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| 346 | * weights_psi[o].weight |
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| 347 | * elliptical_cylinder_analytical_2DXY(&dp, qx, qy) |
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| 348 | * pow(weights_rad[i].value,2) |
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| 349 | * weights_len[j].value |
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| 350 | * weights_rat[m].value; |
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| 351 | if (weights_theta.size()>1) { |
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| 352 | _ptvalue *= fabs(cos(weights_theta[k].value*pi/180.0)); |
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| 353 | } |
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| 354 | sum += _ptvalue; |
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| 355 | //Find average volume |
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| 356 | vol += weights_rad[i].weight |
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| 357 | * weights_len[j].weight |
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| 358 | * weights_rat[m].weight |
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| 359 | * pow(weights_rad[i].value,2) |
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| 360 | * weights_len[j].value |
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| 361 | * weights_rat[m].value; |
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| 362 | //Find norm for volume |
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| 363 | norm_vol += weights_rad[i].weight |
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| 364 | * weights_len[j].weight |
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| 365 | * weights_rat[m].weight; |
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| 366 | |
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| 367 | norm += weights_rad[i].weight |
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| 368 | * weights_len[j].weight |
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| 369 | * weights_rat[m].weight |
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| 370 | * weights_theta[k].weight |
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| 371 | * weights_phi[l].weight |
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| 372 | * weights_psi[o].weight; |
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| 373 | |
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| 374 | } |
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| 375 | } |
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| 376 | } |
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| 377 | } |
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| 378 | } |
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| 379 | } |
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| 380 | // Averaging in theta needs an extra normalization |
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| 381 | // factor to account for the sin(theta) term in the |
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| 382 | // integration (see documentation). |
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| 383 | if (weights_theta.size()>1) norm = norm / asin(1.0); |
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| 384 | |
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| 385 | if (vol != 0.0 && norm_vol != 0.0) { |
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| 386 | //Re-normalize by avg volume |
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| 387 | sum = sum/(vol/norm_vol);} |
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| 388 | |
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| 389 | return sum/norm + background(); |
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| 390 | |
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| 391 | } |
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| 392 | |
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| 393 | /** |
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| 394 | * Function to evaluate 2D scattering function |
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| 395 | * @param pars: parameters of the cylinder |
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| 396 | * @param q: q-value |
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| 397 | * @param phi: angle phi |
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| 398 | * @return: function value |
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| 399 | */ |
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| 400 | double EllipticalCylinderModel :: evaluate_rphi(double q, double phi) { |
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| 401 | double qx = q*cos(phi); |
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| 402 | double qy = q*sin(phi); |
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| 403 | return (*this).operator()(qx, qy); |
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| 404 | } |
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| 405 | /** |
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| 406 | * Function to calculate effective radius |
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| 407 | * @return: effective radius value |
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| 408 | */ |
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| 409 | double EllipticalCylinderModel :: calculate_ER() { |
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| 410 | EllipticalCylinderParameters dp; |
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| 411 | dp.r_minor = r_minor(); |
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| 412 | dp.r_ratio = r_ratio(); |
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| 413 | dp.length = length(); |
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| 414 | double rad_out = 0.0; |
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| 415 | double suf_rad = sqrt(dp.r_minor*dp.r_minor*dp.r_ratio); |
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| 416 | |
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| 417 | // Perform the computation, with all weight points |
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| 418 | double sum = 0.0; |
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| 419 | double norm = 0.0; |
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| 420 | |
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| 421 | // Get the dispersion points for the r_minor |
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| 422 | vector<WeightPoint> weights_rad; |
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| 423 | r_minor.get_weights(weights_rad); |
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| 424 | |
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| 425 | // Get the dispersion points for the r_ratio |
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| 426 | vector<WeightPoint> weights_rat; |
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| 427 | r_ratio.get_weights(weights_rat); |
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| 428 | |
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| 429 | // Get the dispersion points for the length |
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| 430 | vector<WeightPoint> weights_len; |
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| 431 | length.get_weights(weights_len); |
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| 432 | |
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| 433 | // Loop over minor radius weight points |
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| 434 | for(size_t i=0; i<weights_rad.size(); i++) { |
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| 435 | dp.r_minor = weights_rad[i].value; |
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| 436 | |
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| 437 | // Loop over length weight points |
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| 438 | for(size_t j=0; j<weights_len.size(); j++) { |
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| 439 | dp.length = weights_len[j].value; |
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| 440 | |
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| 441 | // Loop over r_ration weight points |
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| 442 | for(size_t m=0; m<weights_rat.size(); m++) { |
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| 443 | dp.r_ratio = weights_rat[m].value; |
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| 444 | //Calculate surface averaged radius |
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| 445 | suf_rad = sqrt(dp.r_minor * dp.r_minor * dp.r_ratio); |
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| 446 | |
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| 447 | //Note: output of "DiamCyl(dp.length,dp.radius)" is DIAMETER. |
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| 448 | sum +=weights_rad[i].weight *weights_len[j].weight |
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| 449 | * weights_rat[m].weight*DiamCyl(dp.length, suf_rad)/2.0; |
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| 450 | norm += weights_rad[i].weight *weights_len[j].weight* weights_rat[m].weight; |
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| 451 | } |
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| 452 | } |
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| 453 | } |
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| 454 | if (norm != 0){ |
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| 455 | //return the averaged value |
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| 456 | rad_out = sum/norm;} |
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| 457 | else{ |
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| 458 | //return normal value |
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| 459 | //Note: output of "DiamCyl(dp.length,dp.radius)" is DIAMETER. |
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| 460 | rad_out = DiamCyl(dp.length, suf_rad)/2.0;} |
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| 461 | |
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| 462 | return rad_out; |
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| 463 | } |
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| 464 | double EllipticalCylinderModel :: calculate_VR() { |
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| 465 | return 1.0; |
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| 466 | } |
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