[318b5bbb] | 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 <iostream> |
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| 26 | using namespace std; |
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| 27 | #include "TwoYukawa.h" |
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| 28 | |
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| 29 | extern "C" { |
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| 30 | #include "2Y_TwoYukawa.h" |
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| 31 | } |
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| 32 | |
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| 33 | TwoYukawaModel :: TwoYukawaModel() { |
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| 34 | // Model parameters |
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| 35 | volfraction = Parameter(0.2, true); |
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| 36 | effect_radius = Parameter(50.0, true); |
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| 37 | effect_radius.set_min(0.0); |
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| 38 | scale_K1 = Parameter(6.0); |
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| 39 | decayConst_Z1 = Parameter(10.0); |
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| 40 | scale_K2 = Parameter(-1.0); |
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| 41 | decayConst_Z2 = Parameter(2.0); |
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| 42 | } |
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| 43 | |
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| 44 | /** |
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| 45 | * Function to evaluate 1D scattering function |
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| 46 | * The NIST IGOR library is used for the actual calculation. |
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| 47 | * @param q: q-value |
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| 48 | * @return: function value |
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| 49 | */ |
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| 50 | double TwoYukawaModel :: operator()(double q) |
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| 51 | { |
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| 52 | double dp[6]; |
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| 53 | // Fill parameter array for IGOR library |
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| 54 | // Add the background after averaging |
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| 55 | dp[0] = volfraction(); |
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| 56 | dp[1] = effect_radius(); |
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| 57 | dp[2] = scale_K1(); |
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| 58 | dp[3] = decayConst_Z1(); |
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| 59 | dp[4] = scale_K2(); |
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| 60 | dp[5] = decayConst_Z2(); |
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| 61 | |
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| 62 | double ZERO = 1.0e-24; |
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| 63 | if (fabs(dp[2]) < 0.001){ |
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| 64 | return ZERO; |
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| 65 | } |
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| 66 | if (fabs(dp[3]) < 0.001){ |
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| 67 | return ZERO; |
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| 68 | } |
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| 69 | if (fabs(dp[4]) < 0.001){ |
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| 70 | return ZERO; |
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| 71 | } |
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| 72 | if (fabs(dp[5]) < 0.001){ |
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| 73 | return ZERO; |
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| 74 | } |
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| 75 | |
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| 76 | double a, b, c1, c2, d1, d2; |
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| 77 | int check = 1; |
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| 78 | double x_in = q * dp[1] *2.0; |
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| 79 | int ok = 0; |
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| 80 | |
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| 81 | ok = TY_SolveEquations(dp[3], dp[5], dp[2], dp[4], dp[0], &a, &b, &c1, &c2, &d1, &d2, 0); |
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| 82 | if (ok > 0 ){ |
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| 83 | //check = TY_CheckSolution(dp[3], dp[5], dp[2], dp[4], dp[0], &a, &b, &c1, &c2, &d1, &d2); |
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| 84 | if (check > 0){ |
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| 85 | return SqTwoYukawa(x_in, dp[3], dp[5], dp[2], dp[4], dp[0], a, b, c1, c2, d1, d2); |
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| 86 | } |
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| 87 | else{ |
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| 88 | return ZERO; |
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| 89 | } |
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| 90 | } |
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| 91 | else{ |
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| 92 | return ZERO; |
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| 93 | } |
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| 94 | } |
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| 95 | |
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| 96 | /** |
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| 97 | * Function to evaluate 2D scattering function |
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| 98 | * @param q_x: value of Q along x |
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| 99 | * @param q_y: value of Q along y |
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| 100 | * @return: function value |
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| 101 | */ |
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| 102 | double TwoYukawaModel :: operator()(double qx, double qy) |
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| 103 | { |
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| 104 | double q = sqrt(qx*qx + qy*qy); |
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| 105 | return (*this).operator()(q); |
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| 106 | } |
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| 107 | |
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| 108 | /** |
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| 109 | * Function to evaluate 2D scattering function |
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| 110 | * @param pars: parameters of the cylinder |
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| 111 | * @param q: q-value |
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| 112 | * @param phi: angle phi |
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| 113 | * @return: function value |
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| 114 | */ |
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| 115 | double TwoYukawaModel :: evaluate_rphi(double q, double phi) |
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| 116 | { |
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| 117 | double qx = q*cos(phi); |
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| 118 | double qy = q*sin(phi); |
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| 119 | return (*this).operator()(qx, qy); |
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| 120 | } |
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| 121 | /** |
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| 122 | * Function to calculate effective radius |
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| 123 | * @return: effective radius value |
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| 124 | */ |
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| 125 | double TwoYukawaModel :: calculate_ER() |
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| 126 | { |
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| 127 | return effect_radius(); |
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| 128 | } |
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| 129 | double TwoYukawaModel :: calculate_VR() |
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| 130 | { |
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| 131 | return 1.0; |
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| 132 | } |
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| 133 | |
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