[5068697] | 1 | /** |
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| 2 | * Scattering model for a cylinder |
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| 3 | * @author: Mathieu Doucet / UTK |
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| 4 | */ |
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| 5 | |
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| 6 | #include "triaxial_ellipsoid.h" |
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| 7 | #include <math.h> |
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| 8 | #include "libCylinder.h" |
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| 9 | #include <stdio.h> |
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| 10 | #include <stdlib.h> |
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| 11 | |
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| 12 | |
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| 13 | /** |
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| 14 | * Function to evaluate 1D scattering function |
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| 15 | * @param pars: parameters of the triaxial ellipsoid |
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| 16 | * @param q: q-value |
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| 17 | * @return: function value |
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| 18 | */ |
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| 19 | double triaxial_ellipsoid_analytical_1D(TriaxialEllipsoidParameters *pars, double q) { |
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[34c3020] | 20 | double dp[6]; |
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[975ec8e] | 21 | |
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[5068697] | 22 | // Fill paramater array |
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| 23 | dp[0] = pars->scale; |
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| 24 | dp[1] = pars->semi_axisA; |
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| 25 | dp[2] = pars->semi_axisB; |
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| 26 | dp[3] = pars->semi_axisC; |
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| 27 | dp[4] = pars->contrast; |
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| 28 | dp[5] = pars->background; |
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[975ec8e] | 29 | |
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[5068697] | 30 | // Call library function to evaluate model |
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[975ec8e] | 31 | return TriaxialEllipsoid(dp, q); |
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| 32 | } |
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| 33 | |
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| 34 | double triaxial_ellipsoid_kernel(TriaxialEllipsoidParameters *pars, double q, double alpha, double nu) { |
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| 35 | double t,a,b,c; |
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| 36 | double kernel; |
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[3c102d4] | 37 | double pi = 4.0*atan(1.0); |
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[975ec8e] | 38 | |
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| 39 | a = pars->semi_axisA ; |
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| 40 | b = pars->semi_axisB ; |
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| 41 | c = pars->semi_axisC ; |
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| 42 | |
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| 43 | t = q * sqrt(a*a*cos(nu)*cos(nu)+b*b*sin(nu)*sin(nu)*sin(alpha)*sin(alpha)+c*c*cos(alpha)*cos(alpha)); |
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[3c102d4] | 44 | if (t==0.0){ |
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[975ec8e] | 45 | kernel = 1.0; |
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| 46 | }else{ |
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[3c102d4] | 47 | kernel = 3.0*(sin(t)-t*cos(t))/(t*t*t); |
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[975ec8e] | 48 | } |
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| 49 | return kernel*kernel; |
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[5068697] | 50 | } |
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| 51 | |
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[975ec8e] | 52 | |
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[5068697] | 53 | /** |
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| 54 | * Function to evaluate 2D scattering function |
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| 55 | * @param pars: parameters of the triaxial ellipsoid |
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| 56 | * @param q: q-value |
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| 57 | * @return: function value |
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| 58 | */ |
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| 59 | double triaxial_ellipsoid_analytical_2DXY(TriaxialEllipsoidParameters *pars, double qx, double qy) { |
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| 60 | double q; |
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| 61 | q = sqrt(qx*qx+qy*qy); |
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| 62 | return triaxial_ellipsoid_analytical_2D_scaled(pars, q, qx/q, qy/q); |
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[975ec8e] | 63 | } |
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[5068697] | 64 | |
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| 65 | |
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| 66 | /** |
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| 67 | * Function to evaluate 2D scattering function |
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| 68 | * @param pars: parameters of the triaxial ellipsoid |
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| 69 | * @param q: q-value |
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| 70 | * @param phi: angle phi |
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| 71 | * @return: function value |
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| 72 | */ |
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| 73 | double triaxial_ellipsoid_analytical_2D(TriaxialEllipsoidParameters *pars, double q, double phi) { |
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| 74 | return triaxial_ellipsoid_analytical_2D_scaled(pars, q, cos(phi), sin(phi)); |
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[975ec8e] | 75 | } |
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| 76 | |
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[5068697] | 77 | /** |
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| 78 | * Function to evaluate 2D scattering function |
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| 79 | * @param pars: parameters of the triaxial ellipsoid |
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| 80 | * @param q: q-value |
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| 81 | * @param q_x: q_x / q |
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| 82 | * @param q_y: q_y / q |
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| 83 | * @return: function value |
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| 84 | */ |
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| 85 | double triaxial_ellipsoid_analytical_2D_scaled(TriaxialEllipsoidParameters *pars, double q, double q_x, double q_y) { |
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[975ec8e] | 86 | double cyl_x, cyl_y, cyl_z, ell_x, ell_y; |
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[5068697] | 87 | double q_z; |
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[975ec8e] | 88 | double cos_nu,nu; |
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[5068697] | 89 | double alpha, vol, cos_val; |
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| 90 | double answer; |
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| 91 | double pi = acos(-1.0); |
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| 92 | // Cylinder orientation |
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| 93 | cyl_x = sin(pars->axis_theta) * cos(pars->axis_phi); |
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| 94 | cyl_y = sin(pars->axis_theta) * sin(pars->axis_phi); |
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| 95 | cyl_z = cos(pars->axis_theta); |
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[975ec8e] | 96 | |
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[5068697] | 97 | // q vector |
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| 98 | q_z = 0; |
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[975ec8e] | 99 | |
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| 100 | //dx = 1.0; |
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| 101 | //dy = 1.0; |
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[5068697] | 102 | // Compute the angle btw vector q and the |
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| 103 | // axis of the cylinder |
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| 104 | cos_val = cyl_x*q_x + cyl_y*q_y + cyl_z*q_z; |
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[975ec8e] | 105 | |
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[5068697] | 106 | // The following test should always pass |
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| 107 | if (fabs(cos_val)>1.0) { |
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| 108 | printf("cyl_ana_2D: Unexpected error: cos(alpha)>1\n"); |
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| 109 | return 0; |
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| 110 | } |
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[975ec8e] | 111 | |
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[5068697] | 112 | // Note: cos(alpha) = 0 and 1 will get an |
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| 113 | // undefined value from CylKernel |
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| 114 | alpha = acos( cos_val ); |
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[975ec8e] | 115 | |
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| 116 | //ellipse orientation: |
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| 117 | // the elliptical corss section was transformed and projected |
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| 118 | // into the detector plane already through sin(alpha)and furthermore psi remains as same |
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| 119 | // on the detector plane. |
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| 120 | // So, all we need is to calculate the angle (nu) of the minor axis of the ellipse wrt |
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| 121 | // the wave vector q. |
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| 122 | |
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| 123 | //x- y- component on the detector plane. |
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| 124 | ell_x = cos(pars->axis_psi); |
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| 125 | ell_y = sin(pars->axis_psi); |
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| 126 | |
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| 127 | // calculate the axis of the ellipse wrt q-coord. |
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| 128 | cos_nu = ell_x*q_x + ell_y*q_y; |
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| 129 | nu = acos(cos_nu); |
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| 130 | |
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[5068697] | 131 | // Call the IGOR library function to get the kernel |
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[975ec8e] | 132 | answer = triaxial_ellipsoid_kernel(pars, q, alpha, nu); |
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| 133 | |
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[5068697] | 134 | // Multiply by contrast^2 |
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| 135 | answer *= pars->contrast*pars->contrast; |
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[975ec8e] | 136 | |
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[5068697] | 137 | //normalize by cylinder volume |
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| 138 | //NOTE that for this (Fournet) definition of the integral, one must MULTIPLY by Vcyl |
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[3c102d4] | 139 | vol = 4.0* pi/3.0 * pars->semi_axisA * pars->semi_axisB * pars->semi_axisC; |
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[5068697] | 140 | answer *= vol; |
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| 141 | //convert to [cm-1] |
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| 142 | answer *= 1.0e8; |
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| 143 | //Scale |
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| 144 | answer *= pars->scale; |
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[975ec8e] | 145 | |
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[5068697] | 146 | // add in the background |
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| 147 | answer += pars->background; |
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[975ec8e] | 148 | |
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[5068697] | 149 | return answer; |
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| 150 | } |
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