[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 | |
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| 27 | extern "C" { |
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| 28 | #include "GaussWeights.h" |
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| 29 | #include "libCylinder.h" |
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| 30 | } |
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| 31 | #include "capcyl.h" |
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| 32 | |
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| 33 | // Convenience parameter structure |
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| 34 | typedef struct { |
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| 35 | double scale; |
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| 36 | double rad_cyl; |
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| 37 | double len_cyl; |
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| 38 | double rad_cap; |
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| 39 | double sld_capcyl; |
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| 40 | double sld_solv; |
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| 41 | double background; |
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| 42 | double theta; |
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| 43 | double phi; |
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| 44 | } CapCylParameters; |
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| 45 | |
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| 46 | CappedCylinderModel :: CappedCylinderModel() { |
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| 47 | scale = Parameter(1.0); |
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| 48 | rad_cyl = Parameter(20.0); |
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| 49 | rad_cyl.set_min(0.0); |
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| 50 | len_cyl = Parameter(400.0, true); |
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| 51 | len_cyl.set_min(0.0); |
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| 52 | rad_cap = Parameter(40.0); |
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| 53 | rad_cap.set_min(0.0); |
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| 54 | sld_capcyl = Parameter(1.0e-6); |
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| 55 | sld_solv = Parameter(6.3e-6); |
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| 56 | background = Parameter(0.0); |
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| 57 | theta = Parameter(0.0, true); |
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| 58 | phi = Parameter(0.0, true); |
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| 59 | } |
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| 60 | |
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| 61 | static double capcyl2d_kernel(double dp[], double q, double alpha) { |
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| 62 | int j; |
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| 63 | double Pi; |
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| 64 | double scale,contr,bkg,sldc,slds; |
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| 65 | double len,rad,hDist,endRad; |
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| 66 | int nordj=76; |
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| 67 | double zi=alpha,yyy,answer; //running tally of integration |
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| 68 | double summj,vaj,vbj,zij; //for the inner integration |
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| 69 | double arg1,arg2,inner,be; |
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| 70 | |
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| 71 | |
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| 72 | scale = dp[0]; |
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| 73 | rad = dp[1]; |
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| 74 | len = dp[2]; |
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| 75 | endRad = dp[3]; |
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| 76 | sldc = dp[4]; |
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| 77 | slds = dp[5]; |
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| 78 | bkg = dp[6]; |
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| 79 | |
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| 80 | hDist = -1.0*sqrt(fabs(endRad*endRad-rad*rad)); //by definition for this model |
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| 81 | |
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| 82 | contr = sldc-slds; |
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| 83 | |
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| 84 | Pi = 4.0*atan(1.0); |
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| 85 | vaj = -1.0*hDist/endRad; |
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| 86 | vbj = 1.0; //endpoints of inner integral |
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| 87 | |
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| 88 | summj=0.0; |
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| 89 | |
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| 90 | for(j=0;j<nordj;j++) { |
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| 91 | //20 gauss points for the inner integral |
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| 92 | zij = ( Gauss76Z[j]*(vbj-vaj) + vaj + vbj )/2.0; //the "t" dummy |
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| 93 | yyy = Gauss76Wt[j] * ConvLens_kernel(dp,q,zij,zi); //uses the same Kernel as the Dumbbell, here L>0 |
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| 94 | summj += yyy; |
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| 95 | } |
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| 96 | //now calculate the value of the inner integral |
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| 97 | inner = (vbj-vaj)/2.0*summj; |
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| 98 | inner *= 4.0*Pi*endRad*endRad*endRad; |
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| 99 | |
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| 100 | //now calculate outer integrand |
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| 101 | arg1 = q*len/2.0*cos(zi); |
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| 102 | arg2 = q*rad*sin(zi); |
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| 103 | yyy = inner; |
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| 104 | |
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| 105 | if(arg2 == 0) { |
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| 106 | be = 0.5; |
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| 107 | } else { |
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| 108 | be = NR_BessJ1(arg2)/arg2; |
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| 109 | } |
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| 110 | |
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| 111 | if(arg1 == 0.0) { //limiting value of sinc(0) is 1; sinc is not defined in math.h |
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| 112 | yyy += Pi*rad*rad*len*2.0*be; |
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| 113 | } else { |
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| 114 | yyy += Pi*rad*rad*len*sin(arg1)/arg1*2.0*be; |
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| 115 | } |
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| 116 | yyy *= yyy; //sin(zi); |
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| 117 | answer = yyy; |
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| 118 | |
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| 119 | |
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| 120 | answer /= Pi*rad*rad*len + 2.0*Pi*(2.0*endRad*endRad*endRad/3.0+endRad*endRad*hDist-hDist*hDist*hDist/3.0); //divide by volume |
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| 121 | answer *= 1.0e8; //convert to cm^-1 |
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| 122 | answer *= contr*contr; |
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| 123 | answer *= scale; |
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| 124 | answer += bkg; |
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| 125 | |
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| 126 | return answer; |
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| 127 | } |
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| 128 | |
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| 129 | /** |
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| 130 | * Function to evaluate 2D scattering function |
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| 131 | * @param pars: parameters of the BarBell |
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| 132 | * @param q: q-value |
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| 133 | * @param q_x: q_x / q |
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| 134 | * @param q_y: q_y / q |
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| 135 | * @return: function value |
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| 136 | */ |
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| 137 | static double capcyl_analytical_2D_scaled(CapCylParameters *pars, double q, double q_x, double q_y) { |
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| 138 | double cyl_x, cyl_y;//, cyl_z; |
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| 139 | //double q_z; |
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| 140 | double alpha, cos_val; |
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| 141 | double answer; |
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| 142 | double dp[7]; |
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| 143 | //convert angle degree to radian |
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| 144 | double pi = 4.0*atan(1.0); |
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| 145 | double theta = pars->theta * pi/180.0; |
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| 146 | double phi = pars->phi * pi/180.0; |
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| 147 | |
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| 148 | dp[0] = pars->scale; |
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| 149 | dp[1] = pars->rad_cyl; |
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| 150 | dp[2] = pars->len_cyl; |
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| 151 | dp[3] = pars->rad_cap; |
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| 152 | dp[4] = pars->sld_capcyl; |
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| 153 | dp[5] = pars->sld_solv; |
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| 154 | dp[6] = pars->background; |
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| 155 | |
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| 156 | |
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| 157 | //double Pi = 4.0*atan(1.0); |
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| 158 | // Cylinder orientation |
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| 159 | cyl_x = cos(theta) * cos(phi); |
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| 160 | cyl_y = sin(theta); |
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| 161 | //cyl_z = -cos(theta) * sin(phi); |
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| 162 | |
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| 163 | // q vector |
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| 164 | //q_z = 0; |
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| 165 | |
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| 166 | // Compute the angle btw vector q and the |
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| 167 | // axis of the cylinder |
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| 168 | cos_val = cyl_x*q_x + cyl_y*q_y;// + cyl_z*q_z; |
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| 169 | |
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| 170 | // The following test should always pass |
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| 171 | if (fabs(cos_val)>1.0) { |
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| 172 | printf("cyl_ana_2D: Unexpected error: cos(alpha)>1\n"); |
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| 173 | return 0; |
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| 174 | } |
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| 175 | |
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| 176 | // Note: cos(alpha) = 0 and 1 will get an |
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| 177 | // undefined value from CylKernel |
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| 178 | alpha = acos( cos_val ); |
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| 179 | |
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| 180 | // Call the IGOR library function to get the kernel |
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| 181 | answer = capcyl2d_kernel(dp, q, alpha)/sin(alpha); |
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| 182 | |
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| 183 | |
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| 184 | return answer; |
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| 185 | |
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| 186 | } |
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| 187 | |
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| 188 | /** |
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| 189 | * Function to evaluate 2D scattering function |
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| 190 | * @param pars: parameters of the BarBell |
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| 191 | * @param q: q-value |
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| 192 | * @return: function value |
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| 193 | */ |
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| 194 | static double capcyl_analytical_2DXY(CapCylParameters *pars, double qx, double qy){ |
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| 195 | double q; |
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| 196 | q = sqrt(qx*qx+qy*qy); |
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| 197 | return capcyl_analytical_2D_scaled(pars, q, qx/q, qy/q); |
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| 198 | } |
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| 199 | |
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| 200 | /** |
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| 201 | * Function to evaluate 1D scattering function |
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| 202 | * The NIST IGOR library is used for the actual calculation. |
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| 203 | * @param q: q-value |
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| 204 | * @return: function value |
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| 205 | */ |
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| 206 | double CappedCylinderModel :: operator()(double q) { |
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| 207 | double dp[7]; |
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| 208 | |
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| 209 | // Fill parameter array for IGOR library |
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| 210 | // Add the background after averaging |
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| 211 | dp[0] = scale(); |
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| 212 | dp[1] = rad_cyl(); |
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| 213 | dp[2] = len_cyl(); |
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| 214 | dp[3] = rad_cap(); |
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| 215 | dp[4] = sld_capcyl(); |
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| 216 | dp[5] = sld_solv(); |
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| 217 | dp[6] = 0.0; |
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| 218 | |
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| 219 | // Get the dispersion points for the rad_cyl |
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| 220 | vector<WeightPoint> weights_rad_cyl; |
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| 221 | rad_cyl.get_weights(weights_rad_cyl); |
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| 222 | // Get the dispersion points for the len_cyl |
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| 223 | vector<WeightPoint> weights_len_cyl; |
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| 224 | len_cyl.get_weights(weights_len_cyl); |
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| 225 | // Get the dispersion points for the rad_cap |
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| 226 | vector<WeightPoint> weights_rad_cap; |
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| 227 | rad_cap.get_weights(weights_rad_cap); |
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| 228 | |
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| 229 | // Perform the computation, with all weight points |
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| 230 | double sum = 0.0; |
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| 231 | double norm = 0.0; |
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| 232 | double vol = 0.0; |
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| 233 | double pi,hDist,result; |
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| 234 | double vol_i = 0.0; |
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| 235 | pi = 4.0*atan(1.0); |
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| 236 | // Loop over radius weight points |
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| 237 | for(size_t i=0; i<weights_rad_cyl.size(); i++) { |
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| 238 | dp[1] = weights_rad_cyl[i].value; |
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| 239 | for(size_t j=0; j<weights_len_cyl.size(); j++) { |
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| 240 | dp[2] = weights_len_cyl[j].value; |
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| 241 | for(size_t k=0; k<weights_rad_cap.size(); k++) { |
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| 242 | dp[3] = weights_rad_cap[k].value; |
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| 243 | |
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| 244 | //Un-normalize SphereForm by volume |
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| 245 | hDist = -1.0*sqrt(fabs(dp[3]*dp[3]-dp[1]*dp[1])); |
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| 246 | vol_i = pi*dp[1]*dp[1]*dp[2]+2.0*pi/3.0*((dp[3]-hDist)*(dp[3]-hDist)* |
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| 247 | (2.0*(dp[3]+hDist))); |
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| 248 | result = CappedCylinder(dp, q) * vol_i; |
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| 249 | // This FIXES a singualrity the kernel in libigor. |
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| 250 | if ( result == INFINITY || result == NAN){ |
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| 251 | result = 0.0; |
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| 252 | } |
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| 253 | sum += weights_rad_cyl[i].weight*weights_len_cyl[j].weight*weights_rad_cap[k].weight |
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| 254 | * result; |
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| 255 | //Find average volume |
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| 256 | vol += weights_rad_cyl[i].weight*weights_len_cyl[j].weight*weights_rad_cap[k].weight |
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| 257 | * vol_i; |
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| 258 | |
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| 259 | norm += weights_rad_cyl[i].weight*weights_len_cyl[j].weight*weights_rad_cap[k].weight; |
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| 260 | } |
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| 261 | } |
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| 262 | } |
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| 263 | |
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| 264 | if (vol != 0.0 && norm != 0.0) { |
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| 265 | //Re-normalize by avg volume |
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| 266 | sum = sum/(vol/norm);} |
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| 267 | return sum/norm + background(); |
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| 268 | } |
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| 269 | |
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| 270 | /** |
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| 271 | * Function to evaluate 2D scattering function |
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| 272 | * @param q_x: value of Q along x |
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| 273 | * @param q_y: value of Q along y |
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| 274 | * @return: function value |
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| 275 | */ |
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| 276 | double CappedCylinderModel :: operator()(double qx, double qy) { |
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| 277 | CapCylParameters dp; |
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| 278 | |
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| 279 | dp.scale = scale(); |
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| 280 | dp.rad_cyl = rad_cyl(); |
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| 281 | dp.len_cyl = len_cyl(); |
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| 282 | dp.rad_cap = rad_cap(); |
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| 283 | dp.sld_capcyl = sld_capcyl(); |
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| 284 | dp.sld_solv = sld_solv(); |
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| 285 | dp.background = 0.0; |
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| 286 | dp.theta = theta(); |
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| 287 | dp.phi = phi(); |
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| 288 | |
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| 289 | // Get the dispersion points for the rad_bar |
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| 290 | vector<WeightPoint> weights_rad_cyl; |
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| 291 | rad_cyl.get_weights(weights_rad_cyl); |
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| 292 | |
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| 293 | // Get the dispersion points for the len_bar |
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| 294 | vector<WeightPoint> weights_len_cyl; |
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| 295 | len_cyl.get_weights(weights_len_cyl); |
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| 296 | |
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| 297 | // Get the dispersion points for the rad_bell |
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| 298 | vector<WeightPoint> weights_rad_cap; |
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| 299 | rad_cap.get_weights(weights_rad_cap); |
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| 300 | |
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| 301 | // Get angular averaging for theta |
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| 302 | vector<WeightPoint> weights_theta; |
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| 303 | theta.get_weights(weights_theta); |
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| 304 | |
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| 305 | // Get angular averaging for phi |
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| 306 | vector<WeightPoint> weights_phi; |
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| 307 | phi.get_weights(weights_phi); |
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| 308 | |
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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,hDist; |
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| 316 | double vol_i = 0.0; |
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| 317 | pi = 4.0*atan(1.0); |
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| 318 | |
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| 319 | // Loop over radius weight points |
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| 320 | for(size_t i=0; i<weights_rad_cyl.size(); i++) { |
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| 321 | dp.rad_cyl = weights_rad_cyl[i].value; |
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| 322 | for(size_t j=0; j<weights_len_cyl.size(); j++) { |
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| 323 | dp.len_cyl = weights_len_cyl[j].value; |
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| 324 | for(size_t k=0; k<weights_rad_cap.size(); k++) { |
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| 325 | dp.rad_cap = weights_rad_cap[k].value; |
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| 326 | // Average over theta distribution |
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| 327 | for(size_t l=0; l< weights_theta.size(); l++) { |
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| 328 | dp.theta = weights_theta[l].value; |
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| 329 | // Average over phi distribution |
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| 330 | for(size_t m=0; m< weights_phi.size(); m++) { |
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| 331 | dp.phi = weights_phi[m].value; |
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| 332 | //Un-normalize Form by volume |
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| 333 | hDist = -1.0*sqrt(fabs(dp.rad_cap*dp.rad_cap-dp.rad_cyl*dp.rad_cyl)); |
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| 334 | vol_i = pi*dp.rad_cyl*dp.rad_cyl*dp.len_cyl+2.0*pi/3.0*((dp.rad_cap-hDist)*(dp.rad_cap-hDist)* |
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| 335 | (2*dp.rad_cap+hDist)); |
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| 336 | |
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| 337 | double _ptvalue = weights_rad_cyl[i].weight |
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| 338 | * weights_len_cyl[j].weight |
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| 339 | * weights_rad_cap[k].weight |
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| 340 | * weights_theta[l].weight |
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| 341 | * weights_phi[m].weight |
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| 342 | * vol_i |
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| 343 | * capcyl_analytical_2DXY(&dp, qx, qy); |
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| 344 | //* pow(weights_rad[i].value,3.0); |
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| 345 | // Consider when there is infinte or nan. |
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| 346 | if ( _ptvalue == INFINITY || _ptvalue == NAN){ |
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| 347 | _ptvalue = 0.0; |
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| 348 | } |
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| 349 | if (weights_theta.size()>1) { |
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| 350 | _ptvalue *= fabs(cos(weights_theta[l].value*pi/180.0)); |
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| 351 | } |
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| 352 | sum += _ptvalue; |
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| 353 | // This model dose not need the volume of spheres correction!!! |
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| 354 | //Find average volume |
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| 355 | vol += weights_rad_cyl[i].weight |
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| 356 | * weights_len_cyl[j].weight |
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| 357 | * weights_rad_cap[k].weight |
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| 358 | * vol_i; |
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| 359 | //Find norm for volume |
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| 360 | norm_vol += weights_rad_cyl[i].weight |
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| 361 | * weights_len_cyl[j].weight |
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| 362 | * weights_rad_cap[k].weight; |
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| 363 | |
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| 364 | norm += weights_rad_cyl[i].weight |
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| 365 | * weights_len_cyl[j].weight |
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| 366 | * weights_rad_cap[k].weight |
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| 367 | * weights_theta[l].weight |
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| 368 | * weights_phi[m].weight; |
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| 369 | } |
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| 370 | } |
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| 371 | } |
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| 372 | } |
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| 373 | } |
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| 374 | // Averaging in theta needs an extra normalization |
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| 375 | // factor to account for the sin(theta) term in the |
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| 376 | // integration (see documentation). |
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| 377 | if (weights_theta.size()>1) norm = norm / asin(1.0); |
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| 378 | |
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| 379 | if (vol != 0.0 && norm_vol != 0.0) { |
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| 380 | //Re-normalize by avg volume |
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| 381 | sum = sum/(vol/norm_vol);} |
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| 382 | |
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| 383 | return sum/norm + background(); |
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| 384 | } |
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| 385 | |
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| 386 | /** |
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| 387 | * Function to evaluate 2D scattering function |
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| 388 | * @param pars: parameters of the SCCrystal |
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| 389 | * @param q: q-value |
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| 390 | * @param phi: angle phi |
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| 391 | * @return: function value |
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| 392 | */ |
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| 393 | double CappedCylinderModel :: evaluate_rphi(double q, double phi) { |
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| 394 | return (*this).operator()(q); |
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| 395 | } |
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| 396 | |
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| 397 | /** |
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| 398 | * Function to calculate effective radius |
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| 399 | * @return: effective radius value |
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| 400 | */ |
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| 401 | double CappedCylinderModel :: calculate_ER() { |
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| 402 | //NOT implemented yet!!! |
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| 403 | return 0.0; |
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| 404 | } |
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| 405 | double CappedCylinderModel :: calculate_VR() { |
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| 406 | return 1.0; |
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| 407 | } |
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