[543d1bd] | 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 "core_shell_bicelle.h" |
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| 27 | |
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| 28 | extern "C" { |
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| 29 | #include "libCylinder.h" |
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| 30 | #include "libStructureFactor.h" |
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| 31 | } |
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| 32 | |
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| 33 | typedef struct { |
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| 34 | double scale; |
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| 35 | double radius; |
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| 36 | double rim_thick; |
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| 37 | double face_thick; |
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| 38 | double length; |
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| 39 | double core_sld; |
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| 40 | double rim_sld; |
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| 41 | double face_sld; |
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| 42 | double solvent_sld; |
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| 43 | double background; |
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| 44 | double axis_theta; |
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| 45 | double axis_phi; |
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| 46 | } CoreShellBicelleParameters; |
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| 47 | |
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| 48 | |
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| 49 | /** |
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| 50 | * Function to evaluate 2D scattering function |
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| 51 | * @param pars: parameters of the core-shell Bicelle |
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| 52 | * @param q: q-value |
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| 53 | * @param q_x: q_x / q |
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| 54 | * @param q_y: q_y / q |
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| 55 | * @return: function value |
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| 56 | */ |
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| 57 | static double core_shell_bicelle_analytical_2D_scaled(CoreShellBicelleParameters *pars, double q, double q_x, double q_y) { |
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| 58 | double cyl_x, cyl_y, cyl_z; |
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| 59 | double q_z; |
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| 60 | double alpha, vol, cos_val; |
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| 61 | double answer; |
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| 62 | //convert angle degree to radian |
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| 63 | double pi = 4.0*atan(1.0); |
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| 64 | double theta = pars->axis_theta * pi/180.0; |
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| 65 | double phi = pars->axis_phi * pi/180.0; |
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| 66 | |
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| 67 | // Cylinder orientation |
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| 68 | cyl_x = sin(theta) * cos(phi); |
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| 69 | cyl_y = sin(theta) * sin(phi); |
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| 70 | cyl_z = cos(theta); |
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| 71 | |
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| 72 | // q vector |
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| 73 | q_z = 0; |
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| 74 | |
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| 75 | // Compute the angle btw vector q and the |
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| 76 | // axis of the cylinder |
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| 77 | cos_val = cyl_x*q_x + cyl_y*q_y + cyl_z*q_z; |
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| 78 | |
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| 79 | // The following test should always pass |
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| 80 | if (fabs(cos_val)>1.0) { |
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| 81 | printf("core_shell_bicelle_analytical_2D: Unexpected error: cos(alpha)=%g\n", cos_val); |
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| 82 | return 0; |
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| 83 | } |
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| 84 | |
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| 85 | alpha = acos( cos_val ); |
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| 86 | |
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| 87 | // Call the IGOR library function to get the kernel |
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| 88 | answer = BicelleKernel(q, pars->radius, pars->rim_thick, pars->face_thick, |
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| 89 | pars->core_sld,pars->face_sld,pars->rim_sld, |
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| 90 | pars->solvent_sld, pars->length/2.0, alpha) / fabs(sin(alpha)); |
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| 91 | |
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| 92 | //normalize by cylinder volume |
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| 93 | vol=pi*(pars->radius+pars->rim_thick) |
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| 94 | *(pars->radius+pars->rim_thick) |
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| 95 | *(pars->length+2.0*pars->face_thick); |
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| 96 | answer /= vol; |
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| 97 | |
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| 98 | //convert to [cm-1] |
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| 99 | answer *= 1.0e8; |
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| 100 | |
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| 101 | //Scale |
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| 102 | answer *= pars->scale; |
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| 103 | |
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| 104 | // add in the background |
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| 105 | answer += pars->background; |
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| 106 | |
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| 107 | return answer; |
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| 108 | } |
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| 109 | |
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| 110 | /** |
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| 111 | * Function to evaluate 2D scattering function |
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| 112 | * @param pars: parameters of the core-shell cylinder |
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| 113 | * @param q: q-value |
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| 114 | * @return: function value |
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| 115 | */ |
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| 116 | static double core_shell_bicelle_analytical_2DXY(CoreShellBicelleParameters *pars, double qx, double qy) { |
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| 117 | double q; |
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| 118 | q = sqrt(qx*qx+qy*qy); |
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| 119 | return core_shell_bicelle_analytical_2D_scaled(pars, q, qx/q, qy/q); |
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| 120 | } |
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| 121 | |
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| 122 | |
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| 123 | CoreShellBicelleModel :: CoreShellBicelleModel() { |
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| 124 | scale = Parameter(1.0); |
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| 125 | radius = Parameter(20.0, true); |
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| 126 | radius.set_min(0.0); |
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| 127 | face_thick = Parameter(10.0, true); |
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| 128 | face_thick.set_min(0.0); |
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| 129 | rim_thick = Parameter(10.0, true); |
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| 130 | rim_thick.set_min(0.0); |
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| 131 | length = Parameter(400.0, true); |
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| 132 | length.set_min(0.0); |
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| 133 | core_sld = Parameter(1.e-6); |
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| 134 | face_sld = Parameter(4.e-6); |
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| 135 | rim_sld = Parameter(4.e-6); |
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| 136 | solvent_sld= Parameter(1.e-6); |
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| 137 | background = Parameter(0.0); |
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| 138 | axis_theta = Parameter(90.0, true); |
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| 139 | axis_phi = Parameter(0.0, true); |
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| 140 | } |
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| 141 | |
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| 142 | /** |
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| 143 | * Function to evaluate 1D scattering function |
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| 144 | * The NIST IGOR library is used for the actual calculation. |
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| 145 | * @param q: q-value |
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| 146 | * @return: function value |
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| 147 | */ |
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| 148 | double CoreShellBicelleModel :: operator()(double q) { |
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| 149 | double dp[10]; |
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| 150 | |
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| 151 | dp[0] = scale(); |
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| 152 | dp[1] = radius(); |
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| 153 | dp[2] = rim_thick(); |
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| 154 | dp[3] = face_thick(); |
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| 155 | dp[4] = length(); |
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| 156 | dp[5] = core_sld(); |
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| 157 | dp[6] = face_sld(); |
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| 158 | dp[7] = rim_sld(); |
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| 159 | dp[8] = solvent_sld(); |
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| 160 | dp[9] = 0.0; |
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| 161 | double pi = 4.0*atan(1.0); |
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| 162 | // Get the dispersion points for the radius |
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| 163 | vector<WeightPoint> weights_rad; |
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| 164 | radius.get_weights(weights_rad); |
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| 165 | |
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| 166 | // Get the dispersion points for the thickness |
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| 167 | vector<WeightPoint> weights_rthick; |
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| 168 | rim_thick.get_weights(weights_rthick); |
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| 169 | |
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| 170 | // Get the dispersion points for the thickness |
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| 171 | vector<WeightPoint> weights_fthick; |
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| 172 | face_thick.get_weights(weights_fthick); |
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| 173 | |
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| 174 | // Get the dispersion points for the length |
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| 175 | vector<WeightPoint> weights_len; |
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| 176 | length.get_weights(weights_len); |
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| 177 | |
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| 178 | // Perform the computation, with all weight points |
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| 179 | double sum = 0.0; |
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| 180 | double norm = 0.0; |
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| 181 | double vol = 0.0; |
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| 182 | |
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| 183 | // Loop over radius weight points |
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| 184 | for(size_t i=0; i<weights_rad.size(); i++) { |
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| 185 | dp[1] = weights_rad[i].value; |
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| 186 | |
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| 187 | // Loop over length weight points |
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| 188 | for(size_t j=0; j<weights_len.size(); j++) { |
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| 189 | dp[4] = weights_len[j].value; |
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| 190 | |
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| 191 | // Loop over thickness weight points |
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| 192 | for(size_t k=0; k<weights_rthick.size(); k++) { |
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| 193 | dp[2] = weights_rthick[k].value; |
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| 194 | for(size_t l=0; l<weights_fthick.size(); l++) { |
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| 195 | dp[3] = weights_fthick[l].value; |
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| 196 | //Un-normalize by volume |
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| 197 | sum += weights_rad[i].weight |
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| 198 | * weights_len[j].weight |
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| 199 | * weights_rthick[k].weight |
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| 200 | * weights_fthick[l].weight |
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| 201 | * BicelleIntegration(q, dp[1],dp[2], dp[3], |
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| 202 | dp[5],dp[6],dp[7],dp[8], dp[4]); |
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| 203 | //* pow(weights_rad[i].value+weights_rthick[k].value,2) |
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| 204 | //*(weights_len[j].value+2.0*weights_fthick[k].value); |
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| 205 | //Find average volume |
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| 206 | vol += weights_rad[i].weight |
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| 207 | * weights_len[j].weight |
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| 208 | * weights_rthick[k].weight |
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| 209 | * weights_fthick[l].weight |
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| 210 | * pi * pow(weights_rad[i].value+weights_rthick[k].value,2) |
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| 211 | *(weights_len[j].value+2.0*weights_fthick[l].value); |
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| 212 | norm += weights_rad[i].weight |
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| 213 | * weights_len[j].weight |
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| 214 | * weights_rthick[k].weight |
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| 215 | * weights_fthick[l].weight; |
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| 216 | } |
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| 217 | } |
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| 218 | } |
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| 219 | } |
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| 220 | |
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| 221 | if (vol != 0.0 && norm != 0.0) { |
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| 222 | //Re-normalize by avg volume |
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| 223 | sum = sum/(vol/norm);} |
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| 224 | //convert to [cm-1] |
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| 225 | sum *= 1.0e8; |
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[02bdfc5] | 226 | sum *= dp[0]; |
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[543d1bd] | 227 | return sum/norm + background(); |
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| 228 | } |
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| 229 | |
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| 230 | /** |
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| 231 | * Function to evaluate 2D scattering function |
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| 232 | * @param q_x: value of Q along x |
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| 233 | * @param q_y: value of Q along y |
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| 234 | * @return: function value |
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| 235 | */ |
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| 236 | double CoreShellBicelleModel :: operator()(double qx, double qy) { |
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| 237 | CoreShellBicelleParameters dp; |
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| 238 | // Fill parameter array |
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| 239 | dp.scale = scale(); |
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| 240 | dp.radius = radius(); |
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| 241 | dp.rim_thick = rim_thick(); |
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| 242 | dp.face_thick = face_thick(); |
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| 243 | dp.length = length(); |
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| 244 | dp.core_sld = core_sld(); |
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| 245 | dp.rim_sld = rim_sld(); |
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| 246 | dp.face_sld = face_sld(); |
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| 247 | dp.solvent_sld= solvent_sld(); |
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| 248 | dp.background = 0.0; |
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| 249 | dp.axis_theta = axis_theta(); |
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| 250 | dp.axis_phi = axis_phi(); |
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| 251 | |
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| 252 | // Get the dispersion points for the radius |
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| 253 | vector<WeightPoint> weights_rad; |
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| 254 | radius.get_weights(weights_rad); |
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| 255 | |
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| 256 | // Get the dispersion points for the thickness |
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| 257 | vector<WeightPoint> weights_rthick; |
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| 258 | rim_thick.get_weights(weights_rthick); |
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| 259 | |
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| 260 | // Get the dispersion points for the thickness |
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| 261 | vector<WeightPoint> weights_fthick; |
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| 262 | face_thick.get_weights(weights_fthick); |
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| 263 | |
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| 264 | // Get the dispersion points for the length |
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| 265 | vector<WeightPoint> weights_len; |
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| 266 | length.get_weights(weights_len); |
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| 267 | |
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| 268 | // Get angular averaging for theta |
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| 269 | vector<WeightPoint> weights_theta; |
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| 270 | axis_theta.get_weights(weights_theta); |
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| 271 | |
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| 272 | // Get angular averaging for phi |
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| 273 | vector<WeightPoint> weights_phi; |
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| 274 | axis_phi.get_weights(weights_phi); |
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| 275 | |
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| 276 | // Perform the computation, with all weight points |
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| 277 | double sum = 0.0; |
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| 278 | double norm = 0.0; |
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| 279 | double norm_vol = 0.0; |
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| 280 | double vol = 0.0; |
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| 281 | double pi = 4.0*atan(1.0); |
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| 282 | // Loop over radius weight points |
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| 283 | for(size_t i=0; i<weights_rad.size(); i++) { |
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| 284 | dp.radius = weights_rad[i].value; |
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| 285 | |
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| 286 | // Loop over length weight points |
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| 287 | for(size_t j=0; j<weights_len.size(); j++) { |
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| 288 | dp.length = weights_len[j].value; |
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| 289 | |
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| 290 | // Loop over thickness weight points |
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| 291 | for(size_t m=0; m<weights_rthick.size(); m++) { |
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| 292 | dp.rim_thick = weights_rthick[m].value; |
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| 293 | |
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| 294 | // Loop over thickness weight points |
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| 295 | for(size_t n=0; n<weights_fthick.size(); n++) { |
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| 296 | dp.face_thick = weights_fthick[n].value; |
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| 297 | |
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| 298 | // Average over theta distribution |
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| 299 | for(size_t k=0; k<weights_theta.size(); k++) { |
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| 300 | dp.axis_theta = weights_theta[k].value; |
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| 301 | |
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| 302 | // Average over phi distribution |
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| 303 | for(size_t l=0; l<weights_phi.size(); l++) { |
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| 304 | dp.axis_phi = weights_phi[l].value; |
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| 305 | //Un-normalize by volume |
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| 306 | double _ptvalue = weights_rad[i].weight |
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| 307 | * weights_len[j].weight |
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| 308 | * weights_rthick[m].weight |
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| 309 | * weights_fthick[n].weight |
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| 310 | * weights_theta[k].weight |
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| 311 | * weights_phi[l].weight |
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| 312 | * core_shell_bicelle_analytical_2DXY(&dp, qx, qy) |
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| 313 | * pow(weights_rad[i].value+weights_rthick[m].value,2) |
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| 314 | *(weights_len[j].value+2.0*weights_fthick[n].value); |
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| 315 | |
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| 316 | if (weights_theta.size()>1) { |
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| 317 | _ptvalue *= fabs(sin(weights_theta[k].value*pi/180.0)); |
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| 318 | } |
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| 319 | sum += _ptvalue; |
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| 320 | |
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| 321 | //Find average volume |
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| 322 | vol += weights_rad[i].weight |
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| 323 | * weights_len[j].weight |
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| 324 | * weights_rthick[m].weight |
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| 325 | * weights_fthick[n].weight |
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| 326 | * pow(weights_rad[i].value+weights_rthick[m].value,2) |
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| 327 | *(weights_len[j].value+2.0*weights_fthick[n].value); |
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| 328 | //Find norm for volume |
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| 329 | norm_vol += weights_rad[i].weight |
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| 330 | * weights_len[j].weight |
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| 331 | * weights_rthick[m].weight |
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| 332 | * weights_fthick[n].weight; |
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| 333 | |
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| 334 | norm += weights_rad[i].weight |
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| 335 | * weights_len[j].weight |
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| 336 | * weights_rthick[m].weight |
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| 337 | * weights_fthick[n].weight |
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| 338 | * weights_theta[k].weight |
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| 339 | * weights_phi[l].weight; |
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| 340 | |
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| 341 | } |
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| 342 | } |
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| 343 | } |
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| 344 | } |
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| 345 | } |
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| 346 | } |
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| 347 | // Averaging in theta needs an extra normalization |
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| 348 | // factor to account for the sin(theta) term in the |
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| 349 | // integration (see documentation). |
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| 350 | if (weights_theta.size()>1) norm = norm / asin(1.0); |
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| 351 | |
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| 352 | if (vol != 0.0 && norm_vol != 0.0) { |
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| 353 | //Re-normalize by avg volume |
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| 354 | sum = sum/(vol/norm_vol);} |
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| 355 | |
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| 356 | return sum/norm + background(); |
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| 357 | } |
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| 358 | |
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| 359 | /** |
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| 360 | * Function to evaluate 2D scattering function |
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| 361 | * @param pars: parameters of the cylinder |
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| 362 | * @param q: q-value |
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| 363 | * @param phi: angle phi |
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| 364 | * @return: function value |
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| 365 | */ |
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| 366 | double CoreShellBicelleModel :: evaluate_rphi(double q, double phi) { |
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| 367 | double qx = q*cos(phi); |
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| 368 | double qy = q*sin(phi); |
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| 369 | return (*this).operator()(qx, qy); |
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| 370 | } |
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| 371 | /** |
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| 372 | * Function to calculate effective radius |
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| 373 | * @return: effective radius value |
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| 374 | */ |
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| 375 | double CoreShellBicelleModel :: calculate_ER() { |
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| 376 | CoreShellBicelleParameters dp; |
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| 377 | |
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| 378 | dp.radius = radius(); |
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| 379 | dp.rim_thick = rim_thick(); |
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| 380 | dp.face_thick = face_thick(); |
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| 381 | dp.length = length(); |
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| 382 | double rad_out = 0.0; |
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| 383 | |
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| 384 | // Perform the computation, with all weight points |
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| 385 | double sum = 0.0; |
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| 386 | double norm = 0.0; |
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| 387 | |
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| 388 | // Get the dispersion points for the length |
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| 389 | vector<WeightPoint> weights_length; |
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| 390 | length.get_weights(weights_length); |
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| 391 | |
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| 392 | // Get the dispersion points for the thickness |
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| 393 | vector<WeightPoint> weights_rthick; |
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| 394 | rim_thick.get_weights(weights_rthick); |
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| 395 | |
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| 396 | // Get the dispersion points for the thickness |
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| 397 | vector<WeightPoint> weights_fthick; |
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| 398 | face_thick.get_weights(weights_fthick); |
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| 399 | |
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| 400 | // Get the dispersion points for the radius |
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| 401 | vector<WeightPoint> weights_radius ; |
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| 402 | radius.get_weights(weights_radius); |
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| 403 | |
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| 404 | // Loop over major shell weight points |
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| 405 | for(int i=0; i< (int)weights_length.size(); i++) { |
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| 406 | dp.length = weights_length[i].value; |
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| 407 | for(int j=0; j< (int)weights_rthick.size(); j++) { |
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| 408 | dp.rim_thick = weights_rthick[j].value; |
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| 409 | for(int l=0; l< (int)weights_fthick.size(); l++) { |
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| 410 | dp.face_thick = weights_fthick[l].value; |
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| 411 | for(int k=0; k< (int)weights_radius.size(); k++) { |
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| 412 | dp.radius = weights_radius[k].value; |
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| 413 | //Note: output of "DiamCyl( )" is DIAMETER. |
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| 414 | sum +=weights_length[i].weight * weights_rthick[j].weight * weights_fthick[l].weight |
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| 415 | * weights_radius[k].weight*DiamCyl(dp.length+2.0*dp.face_thick,dp.radius+dp.rim_thick)/2.0; |
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| 416 | norm += weights_length[i].weight* weights_rthick[j].weight * weights_fthick[l].weight* weights_radius[k].weight; |
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| 417 | } |
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| 418 | } |
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| 419 | } |
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| 420 | } |
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| 421 | if (norm != 0){ |
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| 422 | //return the averaged value |
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| 423 | rad_out = sum/norm;} |
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| 424 | else{ |
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| 425 | //return normal value |
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| 426 | //Note: output of "DiamCyl()" is DIAMETER. |
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| 427 | rad_out = DiamCyl(dp.length+2.0*dp.face_thick,dp.radius+dp.rim_thick)/2.0;} |
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| 428 | |
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| 429 | return rad_out; |
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| 430 | } |
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[e08bd5b] | 431 | double CoreShellBicelleModel :: calculate_VR() { |
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| 432 | return 1.0; |
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| 433 | } |
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