[2e44ac7] | 1 | /* |
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| 2 | ########################################################## |
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| 3 | # # |
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| 4 | # !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! # |
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| 5 | # !! !! # |
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| 6 | # !! KEEP THIS CODE CONSISTENT WITH KERNELPY.PY !! # |
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| 7 | # !! !! # |
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| 8 | # !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! # |
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| 9 | # # |
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| 10 | ########################################################## |
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| 11 | */ |
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| 12 | |
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[9ee2756] | 13 | // NOTE: the following macros are defined in generate.py: |
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| 14 | // |
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[6aee3ab] | 15 | // MAX_PD : the maximum number of dispersity loops allowed for this model, |
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| 16 | // which will be at most modelinfo.MAX_PD. |
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[9ee2756] | 17 | // NUM_PARS : the number of parameters in the parameter table |
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| 18 | // NUM_VALUES : the number of values to skip at the start of the |
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| 19 | // values array before you get to the dispersity values. |
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| 20 | // PARAMETER_TABLE : list of parameter declarations used to create the |
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| 21 | // ParameterTable type. |
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| 22 | // KERNEL_NAME : model_Iq, model_Iqxy or model_Imagnetic. This code is |
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| 23 | // included three times, once for each kernel type. |
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[2c108a3] | 24 | // MAGNETIC : defined when the magnetic kernel is being instantiated |
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| 25 | // NUM_MAGNETIC : the number of magnetic parameters |
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[9ee2756] | 26 | // MAGNETIC_PARS : a comma-separated list of indices to the sld |
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| 27 | // parameters in the parameter table. |
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[e44432d] | 28 | // CALL_VOLUME(form, shell, table) : assign form and shell values |
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[a34b811] | 29 | // CALL_RADIUS_EFFECTIVE(mode, table) : call the R_eff function |
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[9ee2756] | 30 | // CALL_IQ(q, table) : call the Iq function for 1D calcs. |
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| 31 | // CALL_IQ_A(q, table) : call the Iq function with |q| for 2D data. |
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[c036ddb] | 32 | // CALL_FQ(q, F1, F2, table) : call the Fq function for 1D calcs. |
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| 33 | // CALL_FQ_A(q, F1, F2, table) : call the Iq function with |q| for 2D data. |
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[9ee2756] | 34 | // CALL_IQ_AC(qa, qc, table) : call the Iqxy function for symmetric shapes |
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| 35 | // CALL_IQ_ABC(qa, qc, table) : call the Iqxy function for asymmetric shapes |
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[108e70e] | 36 | // CALL_IQ_XY(qx, qy, table) : call the Iqxy function for arbitrary models |
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[9ee2756] | 37 | // INVALID(table) : test if the current point is feesible to calculate. This |
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| 38 | // will be defined in the kernel definition file. |
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[ff10479] | 39 | // PROJECTION : equirectangular=1, sinusoidal=2 |
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| 40 | // see explore/jitter.py for definitions. |
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[767dca8] | 41 | |
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[01c8d9e] | 42 | |
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[03cac08] | 43 | #ifndef _PAR_BLOCK_ // protected block so we can include this code twice. |
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| 44 | #define _PAR_BLOCK_ |
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[2e44ac7] | 45 | |
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| 46 | typedef struct { |
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[60eab2a] | 47 | #if MAX_PD > 0 |
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[2c108a3] | 48 | int32_t pd_par[MAX_PD]; // id of the nth dispersity variable |
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| 49 | int32_t pd_length[MAX_PD]; // length of the nth dispersity weight vector |
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[0a7e5eb4] | 50 | int32_t pd_offset[MAX_PD]; // offset of pd weights in the value & weight vector |
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[5cf3c33] | 51 | int32_t pd_stride[MAX_PD]; // stride to move to the next index at this level |
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[60eab2a] | 52 | #endif // MAX_PD > 0 |
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[bde38b5] | 53 | int32_t num_eval; // total number of voxels in hypercube |
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| 54 | int32_t num_weights; // total length of the weights vector |
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[5ff1b03] | 55 | int32_t num_active; // number of non-trivial pd loops |
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[8698a0d] | 56 | int32_t theta_par; // id of first orientation variable |
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[2e44ac7] | 57 | } ProblemDetails; |
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| 58 | |
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[bde38b5] | 59 | // Intel HD 4000 needs private arrays to be a multiple of 4 long |
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[2e44ac7] | 60 | typedef struct { |
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[56547a8] | 61 | PARAMETER_TABLE |
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[bde38b5] | 62 | } ParameterTable; |
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| 63 | typedef union { |
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| 64 | ParameterTable table; |
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| 65 | double vector[4*((NUM_PARS+3)/4)]; |
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[2e44ac7] | 66 | } ParameterBlock; |
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[9eb3632] | 67 | #endif // _PAR_BLOCK_ |
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[03cac08] | 68 | |
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[9ee2756] | 69 | #if defined(MAGNETIC) && NUM_MAGNETIC > 0 |
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| 70 | // ===== Helper functions for magnetism ===== |
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[a4280bd] | 71 | |
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[32e3c9b] | 72 | // Return value restricted between low and high |
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| 73 | static double clip(double value, double low, double high) |
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| 74 | { |
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[b966a96] | 75 | return (value < low ? low : (value > high ? high : value)); |
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[32e3c9b] | 76 | } |
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| 77 | |
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| 78 | // Compute spin cross sections given in_spin and out_spin |
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| 79 | // To convert spin cross sections to sld b: |
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| 80 | // uu * (sld - m_sigma_x); |
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| 81 | // dd * (sld + m_sigma_x); |
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[2c108a3] | 82 | // ud * (m_sigma_y - 1j*m_sigma_z); |
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| 83 | // du * (m_sigma_y + 1j*m_sigma_z); |
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| 84 | // weights for spin crosssections: dd du real, ud real, uu, du imag, ud imag |
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[885753a] | 85 | static void set_spin_weights(double in_spin, double out_spin, double weight[6]) |
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[32e3c9b] | 86 | { |
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[b966a96] | 87 | in_spin = clip(in_spin, 0.0, 1.0); |
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| 88 | out_spin = clip(out_spin, 0.0, 1.0); |
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[7c35fda] | 89 | // Previous version of this function took the square root of the weights, |
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[c036ddb] | 90 | // under the assumption that |
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[7c35fda] | 91 | // |
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[885753a] | 92 | // w*I(q, rho1, rho2, ...) = I(q, sqrt(w)*rho1, sqrt(w)*rho2, ...) |
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[7c35fda] | 93 | // |
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| 94 | // However, since the weights are applied to the final intensity and |
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| 95 | // are not interned inside the I(q) function, we want the full |
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| 96 | // weight and not the square root. Any function using |
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| 97 | // set_spin_weights as part of calculating an amplitude will need to |
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| 98 | // manually take that square root, but there is currently no such |
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| 99 | // function. |
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[84e89cd] | 100 | weight[0] = (1.0-in_spin) * (1.0-out_spin); // dd |
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| 101 | weight[1] = (1.0-in_spin) * out_spin; // du |
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| 102 | weight[2] = in_spin * (1.0-out_spin); // ud |
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| 103 | weight[3] = in_spin * out_spin; // uu |
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[885753a] | 104 | weight[4] = weight[1]; // du.imag |
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| 105 | weight[5] = weight[2]; // ud.imag |
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[a4280bd] | 106 | } |
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| 107 | |
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[9ee2756] | 108 | // Compute the magnetic sld |
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[2c108a3] | 109 | static double mag_sld( |
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[885753a] | 110 | const unsigned int xs, // 0=dd, 1=du.real, 2=ud.real, 3=uu, 4=du.imag, 5=ud.imag |
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[2c108a3] | 111 | const double qx, const double qy, |
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| 112 | const double px, const double py, |
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| 113 | const double sld, |
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| 114 | const double mx, const double my, const double mz |
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| 115 | ) |
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[a4280bd] | 116 | { |
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[2c108a3] | 117 | if (xs < 4) { |
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[a4280bd] | 118 | const double perp = qy*mx - qx*my; |
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[2c108a3] | 119 | switch (xs) { |
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[aadec17] | 120 | default: // keep compiler happy; condition ensures xs in [0,1,2,3] |
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[2c108a3] | 121 | case 0: // uu => sld - D M_perpx |
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| 122 | return sld - px*perp; |
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[885753a] | 123 | case 1: // ud.real => -D M_perpy |
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[2c108a3] | 124 | return py*perp; |
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[885753a] | 125 | case 2: // du.real => -D M_perpy |
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[2c108a3] | 126 | return py*perp; |
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[885753a] | 127 | case 3: // dd => sld + D M_perpx |
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[2c108a3] | 128 | return sld + px*perp; |
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| 129 | } |
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| 130 | } else { |
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| 131 | if (xs== 4) { |
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[885753a] | 132 | return -mz; // du.imag => +D M_perpz |
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[2c108a3] | 133 | } else { // index == 5 |
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[885753a] | 134 | return +mz; // ud.imag => -D M_perpz |
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[2c108a3] | 135 | } |
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| 136 | } |
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[32e3c9b] | 137 | } |
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[9ee2756] | 138 | |
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[2c108a3] | 139 | |
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[9ee2756] | 140 | #endif |
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| 141 | |
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| 142 | // ===== Helper functions for orientation and jitter ===== |
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| 143 | |
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[8698a0d] | 144 | // To change the definition of the angles, run explore/angles.py, which |
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| 145 | // uses sympy to generate the equations. |
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| 146 | |
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[9ee2756] | 147 | #if !defined(_QAC_SECTION) && defined(CALL_IQ_AC) |
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| 148 | #define _QAC_SECTION |
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| 149 | |
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| 150 | typedef struct { |
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| 151 | double R31, R32; |
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| 152 | } QACRotation; |
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| 153 | |
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| 154 | // Fill in the rotation matrix R from the view angles (theta, phi) and the |
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| 155 | // jitter angles (dtheta, dphi). This matrix can be applied to all of the |
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| 156 | // (qx, qy) points in the image to produce R*[qx,qy]' = [qa,qc]' |
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| 157 | static void |
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| 158 | qac_rotation( |
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| 159 | QACRotation *rotation, |
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| 160 | double theta, double phi, |
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| 161 | double dtheta, double dphi) |
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[8698a0d] | 162 | { |
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| 163 | double sin_theta, cos_theta; |
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| 164 | double sin_phi, cos_phi; |
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| 165 | |
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[9ee2756] | 166 | // reverse view matrix |
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[8698a0d] | 167 | SINCOS(theta*M_PI_180, sin_theta, cos_theta); |
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| 168 | SINCOS(phi*M_PI_180, sin_phi, cos_phi); |
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[9ee2756] | 169 | const double V11 = cos_phi*cos_theta; |
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| 170 | const double V12 = sin_phi*cos_theta; |
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| 171 | const double V21 = -sin_phi; |
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| 172 | const double V22 = cos_phi; |
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| 173 | const double V31 = sin_theta*cos_phi; |
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| 174 | const double V32 = sin_phi*sin_theta; |
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[8698a0d] | 175 | |
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[9ee2756] | 176 | // reverse jitter matrix |
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| 177 | SINCOS(dtheta*M_PI_180, sin_theta, cos_theta); |
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| 178 | SINCOS(dphi*M_PI_180, sin_phi, cos_phi); |
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| 179 | const double J31 = sin_theta; |
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| 180 | const double J32 = -sin_phi*cos_theta; |
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| 181 | const double J33 = cos_phi*cos_theta; |
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[8698a0d] | 182 | |
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[9ee2756] | 183 | // reverse matrix |
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| 184 | rotation->R31 = J31*V11 + J32*V21 + J33*V31; |
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| 185 | rotation->R32 = J31*V12 + J32*V22 + J33*V32; |
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[8698a0d] | 186 | } |
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| 187 | |
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[9ee2756] | 188 | // Apply the rotation matrix returned from qac_rotation to the point (qx,qy), |
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| 189 | // returning R*[qx,qy]' = [qa,qc]' |
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[d86f0fc] | 190 | static void |
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[9ee2756] | 191 | qac_apply( |
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[ec8d4ac] | 192 | QACRotation *rotation, |
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[9ee2756] | 193 | double qx, double qy, |
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[70530778] | 194 | double *qab_out, double *qc_out) |
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[8698a0d] | 195 | { |
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[9ee2756] | 196 | // Indirect calculation of qab, from qab^2 = |q|^2 - qc^2 |
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[70530778] | 197 | const double dqc = rotation->R31*qx + rotation->R32*qy; |
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| 198 | const double dqab_sq = -dqc*dqc + qx*qx + qy*qy; |
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| 199 | //*qab_out = sqrt(fabs(dqab_sq)); |
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| 200 | *qab_out = dqab_sq > 0.0 ? sqrt(dqab_sq) : 0.0; |
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[9ee2756] | 201 | *qc_out = dqc; |
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[8698a0d] | 202 | } |
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[9ee2756] | 203 | #endif // _QAC_SECTION |
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| 204 | |
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| 205 | #if !defined(_QABC_SECTION) && defined(CALL_IQ_ABC) |
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| 206 | #define _QABC_SECTION |
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| 207 | |
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| 208 | typedef struct { |
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| 209 | double R11, R12; |
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| 210 | double R21, R22; |
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| 211 | double R31, R32; |
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| 212 | } QABCRotation; |
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| 213 | |
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| 214 | // Fill in the rotation matrix R from the view angles (theta, phi, psi) and the |
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| 215 | // jitter angles (dtheta, dphi, dpsi). This matrix can be applied to all of the |
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| 216 | // (qx, qy) points in the image to produce R*[qx,qy]' = [qa,qb,qc]' |
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[8698a0d] | 217 | static void |
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[9ee2756] | 218 | qabc_rotation( |
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| 219 | QABCRotation *rotation, |
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[8698a0d] | 220 | double theta, double phi, double psi, |
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[9ee2756] | 221 | double dtheta, double dphi, double dpsi) |
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[8698a0d] | 222 | { |
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| 223 | double sin_theta, cos_theta; |
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| 224 | double sin_phi, cos_phi; |
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| 225 | double sin_psi, cos_psi; |
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| 226 | |
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| 227 | // reverse view matrix |
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| 228 | SINCOS(theta*M_PI_180, sin_theta, cos_theta); |
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| 229 | SINCOS(phi*M_PI_180, sin_phi, cos_phi); |
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| 230 | SINCOS(psi*M_PI_180, sin_psi, cos_psi); |
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[9ee2756] | 231 | const double V11 = -sin_phi*sin_psi + cos_phi*cos_psi*cos_theta; |
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| 232 | const double V12 = sin_phi*cos_psi*cos_theta + sin_psi*cos_phi; |
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| 233 | const double V21 = -sin_phi*cos_psi - sin_psi*cos_phi*cos_theta; |
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| 234 | const double V22 = -sin_phi*sin_psi*cos_theta + cos_phi*cos_psi; |
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[8698a0d] | 235 | const double V31 = sin_theta*cos_phi; |
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| 236 | const double V32 = sin_phi*sin_theta; |
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| 237 | |
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| 238 | // reverse jitter matrix |
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[9ee2756] | 239 | SINCOS(dtheta*M_PI_180, sin_theta, cos_theta); |
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| 240 | SINCOS(dphi*M_PI_180, sin_phi, cos_phi); |
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| 241 | SINCOS(dpsi*M_PI_180, sin_psi, cos_psi); |
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[8698a0d] | 242 | const double J11 = cos_psi*cos_theta; |
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[9ee2756] | 243 | const double J12 = sin_phi*sin_theta*cos_psi + sin_psi*cos_phi; |
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| 244 | const double J13 = sin_phi*sin_psi - sin_theta*cos_phi*cos_psi; |
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| 245 | const double J21 = -sin_psi*cos_theta; |
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| 246 | const double J22 = -sin_phi*sin_psi*sin_theta + cos_phi*cos_psi; |
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| 247 | const double J23 = sin_phi*cos_psi + sin_psi*sin_theta*cos_phi; |
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[8698a0d] | 248 | const double J31 = sin_theta; |
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| 249 | const double J32 = -sin_phi*cos_theta; |
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| 250 | const double J33 = cos_phi*cos_theta; |
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| 251 | |
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| 252 | // reverse matrix |
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[9ee2756] | 253 | rotation->R11 = J11*V11 + J12*V21 + J13*V31; |
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| 254 | rotation->R12 = J11*V12 + J12*V22 + J13*V32; |
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| 255 | rotation->R21 = J21*V11 + J22*V21 + J23*V31; |
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| 256 | rotation->R22 = J21*V12 + J22*V22 + J23*V32; |
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| 257 | rotation->R31 = J31*V11 + J32*V21 + J33*V31; |
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| 258 | rotation->R32 = J31*V12 + J32*V22 + J33*V32; |
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[8698a0d] | 259 | } |
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| 260 | |
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[9ee2756] | 261 | // Apply the rotation matrix returned from qabc_rotation to the point (qx,qy), |
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| 262 | // returning R*[qx,qy]' = [qa,qb,qc]' |
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[d86f0fc] | 263 | static void |
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[9ee2756] | 264 | qabc_apply( |
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[ec8d4ac] | 265 | QABCRotation *rotation, |
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[9ee2756] | 266 | double qx, double qy, |
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| 267 | double *qa_out, double *qb_out, double *qc_out) |
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[8698a0d] | 268 | { |
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[ec8d4ac] | 269 | *qa_out = rotation->R11*qx + rotation->R12*qy; |
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| 270 | *qb_out = rotation->R21*qx + rotation->R22*qy; |
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| 271 | *qc_out = rotation->R31*qx + rotation->R32*qy; |
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[8698a0d] | 272 | } |
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| 273 | |
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[9ee2756] | 274 | #endif // _QABC_SECTION |
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| 275 | |
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| 276 | // ==================== KERNEL CODE ======================== |
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[03cac08] | 277 | kernel |
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| 278 | void KERNEL_NAME( |
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[07646b6] | 279 | int32_t nq, // number of q values |
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| 280 | const int32_t pd_start, // where we are in the dispersity loop |
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| 281 | const int32_t pd_stop, // where we are stopping in the dispersity loop |
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[74e9b5f] | 282 | pglobal const ProblemDetails *details, |
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[07646b6] | 283 | pglobal const double *values, // parameter values and distributions |
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| 284 | pglobal const double *q, // nq q values, with padding to boundary |
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| 285 | pglobal double *result, // nq+1 return values, again with padding |
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| 286 | const double cutoff, // cutoff in the dispersity weight product |
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[a34b811] | 287 | int32_t radius_effective_mode // which effective radius to compute |
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[2e44ac7] | 288 | ) |
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| 289 | { |
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[0db7dbd] | 290 | #if defined(USE_GPU) |
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[9ee2756] | 291 | // who we are and what element we are working with |
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[0db7dbd] | 292 | #if defined(USE_OPENCL) |
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[9ee2756] | 293 | const int q_index = get_global_id(0); |
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[0db7dbd] | 294 | #else // USE_CUDA |
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| 295 | const int q_index = threadIdx.x + blockIdx.x * blockDim.x; |
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| 296 | #endif |
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[9ee2756] | 297 | if (q_index >= nq) return; |
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| 298 | #else |
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| 299 | // Define q_index here so that debugging statements can be written to work |
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| 300 | // for both OpenCL and DLL using: |
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| 301 | // if (q_index == 0) {printf(...);} |
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| 302 | int q_index = 0; |
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| 303 | #endif |
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| 304 | |
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[6aee3ab] | 305 | // ** Fill in the local values table ** |
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| 306 | // Storage for the current parameter values. |
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| 307 | // These will be updated as we walk the dispersity mesh. |
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[9eb3632] | 308 | ParameterBlock local_values; |
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[6aee3ab] | 309 | // values[0] is scale |
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| 310 | // values[1] is background |
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| 311 | #ifdef USE_OPENMP |
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| 312 | #pragma omp parallel for |
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| 313 | #endif |
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| 314 | for (int i=0; i < NUM_PARS; i++) { |
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| 315 | local_values.vector[i] = values[2+i]; |
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| 316 | //if (q_index==0) printf("p%d = %g\n",i, local_values.vector[i]); |
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| 317 | } |
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| 318 | //if (q_index==0) printf("NUM_VALUES:%d NUM_PARS:%d MAX_PD:%d\n", NUM_VALUES, NUM_PARS, MAX_PD); |
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| 319 | //if (q_index==0) printf("start:%d stop:%d\n", pd_start, pd_stop); |
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[2e44ac7] | 320 | |
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[6aee3ab] | 321 | // ** Precompute magnatism values ** |
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[a4280bd] | 322 | #if defined(MAGNETIC) && NUM_MAGNETIC>0 |
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[bde38b5] | 323 | // Location of the sld parameters in the parameter vector. |
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[9eb3632] | 324 | // These parameters are updated with the effective sld due to magnetism. |
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| 325 | const int32_t slds[] = { MAGNETIC_PARS }; |
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[32e3c9b] | 326 | |
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| 327 | // Interpret polarization cross section. |
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[a4280bd] | 328 | // up_frac_i = values[NUM_PARS+2]; |
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| 329 | // up_frac_f = values[NUM_PARS+3]; |
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| 330 | // up_angle = values[NUM_PARS+4]; |
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[9ee2756] | 331 | // TODO: could precompute more magnetism parameters before calling the kernel. |
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[885753a] | 332 | double xs_weights[8]; // uu, ud real, du real, dd, ud imag, du imag, fill, fill |
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[32e3c9b] | 333 | double cos_mspin, sin_mspin; |
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[885753a] | 334 | set_spin_weights(values[NUM_PARS+2], values[NUM_PARS+3], xs_weights); |
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[a4280bd] | 335 | SINCOS(-values[NUM_PARS+4]*M_PI_180, sin_mspin, cos_mspin); |
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[9eb3632] | 336 | #endif // MAGNETIC |
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[3044216] | 337 | |
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[6aee3ab] | 338 | // ** Fill in the initial results ** |
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[9ee2756] | 339 | // If pd_start is zero that means that we are starting a new calculation, |
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| 340 | // and must initialize the result to zero. Otherwise, we are restarting |
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| 341 | // the calculation from somewhere in the middle of the dispersity mesh, |
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| 342 | // and we update the value rather than reset it. Similarly for the |
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| 343 | // normalization factor, which is stored as the final value in the |
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| 344 | // results vector (one past the number of q values). |
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| 345 | // |
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| 346 | // The code differs slightly between opencl and dll since opencl is only |
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[07646b6] | 347 | // seeing one q value (stored in the variable "this_F2") while the dll |
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[c036ddb] | 348 | // version must loop over all q. |
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[07646b6] | 349 | #if defined(CALL_FQ) |
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| 350 | double weight_norm = (pd_start == 0 ? 0.0 : result[2*nq]); |
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| 351 | double weighted_form = (pd_start == 0 ? 0.0 : result[2*nq+1]); |
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| 352 | double weighted_shell = (pd_start == 0 ? 0.0 : result[2*nq+2]); |
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| 353 | double weighted_radius = (pd_start == 0 ? 0.0 : result[2*nq+3]); |
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| 354 | #else |
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| 355 | double weight_norm = (pd_start == 0 ? 0.0 : result[nq]); |
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| 356 | double weighted_form = (pd_start == 0 ? 0.0 : result[nq+1]); |
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| 357 | double weighted_shell = (pd_start == 0 ? 0.0 : result[nq+2]); |
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| 358 | double weighted_radius = (pd_start == 0 ? 0.0 : result[nq+3]); |
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| 359 | #endif |
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[0db7dbd] | 360 | #if defined(USE_GPU) |
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[e44432d] | 361 | #if defined(CALL_FQ) |
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[6e7ba14] | 362 | double this_F2 = (pd_start == 0 ? 0.0 : result[2*q_index+0]); |
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| 363 | double this_F1 = (pd_start == 0 ? 0.0 : result[2*q_index+1]); |
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[c036ddb] | 364 | #else |
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[07646b6] | 365 | double this_F2 = (pd_start == 0 ? 0.0 : result[q_index]); |
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[c036ddb] | 366 | #endif |
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[0db7dbd] | 367 | #else // !USE_GPU |
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[9ee2756] | 368 | if (pd_start == 0) { |
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| 369 | #ifdef USE_OPENMP |
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| 370 | #pragma omp parallel for |
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| 371 | #endif |
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[e44432d] | 372 | #if defined(CALL_FQ) |
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[6e7ba14] | 373 | // 2*nq for F^2,F pairs |
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| 374 | for (int q_index=0; q_index < 2*nq; q_index++) result[q_index] = 0.0; |
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[c036ddb] | 375 | #else |
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| 376 | for (int q_index=0; q_index < nq; q_index++) result[q_index] = 0.0; |
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[01c8d9e] | 377 | #endif |
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[9ee2756] | 378 | } |
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[6aee3ab] | 379 | //if (q_index==0) printf("start %d %g %g\n", pd_start, pd_norm, result[0]); |
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[0db7dbd] | 380 | #endif // !USE_GPU |
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[9ee2756] | 381 | |
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| 382 | |
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| 383 | // ====== macros to set up the parts of the loop ======= |
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| 384 | /* |
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| 385 | Based on the level of the loop, uses C preprocessor magic to construct |
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| 386 | level-specific looping variables, including these from loop level 3: |
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| 387 | |
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| 388 | int n3 : length of loop for mesh level 3 |
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| 389 | int i3 : current position in the loop for level 3, which is calculated |
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| 390 | from a combination of pd_start, pd_stride[3] and pd_length[3]. |
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| 391 | int p3 : is the index into the parameter table for mesh level 3 |
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| 392 | double v3[] : pointer into dispersity array to values for loop 3 |
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| 393 | double w3[] : pointer into dispersity array to weights for loop 3 |
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| 394 | double weight3 : the product of weights from levels 3 and up, computed |
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| 395 | as weight5*weight4*w3[i3]. Note that we need an outermost |
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| 396 | value weight5 set to 1.0 for this to work properly. |
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| 397 | |
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| 398 | After expansion, the loop struction will look like the following: |
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| 399 | |
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| 400 | // --- PD_INIT(4) --- |
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| 401 | const int n4 = pd_length[4]; |
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| 402 | const int p4 = pd_par[4]; |
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[74e9b5f] | 403 | pglobal const double *v4 = pd_value + pd_offset[4]; |
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| 404 | pglobal const double *w4 = pd_weight + pd_offset[4]; |
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[9ee2756] | 405 | int i4 = (pd_start/pd_stride[4])%n4; // position in level 4 at pd_start |
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| 406 | |
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| 407 | // --- PD_INIT(3) --- |
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| 408 | const int n3 = pd_length[3]; |
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| 409 | ... |
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| 410 | int i3 = (pd_start/pd_stride[3])%n3; // position in level 3 at pd_start |
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| 411 | |
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| 412 | PD_INIT(2) |
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| 413 | PD_INIT(1) |
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| 414 | PD_INIT(0) |
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| 415 | |
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| 416 | // --- PD_OUTERMOST_WEIGHT(5) --- |
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| 417 | const double weight5 = 1.0; |
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| 418 | |
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| 419 | // --- PD_OPEN(4,5) --- |
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| 420 | while (i4 < n4) { |
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| 421 | parameter[p4] = v4[i4]; // set the value for pd parameter 4 at this mesh point |
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| 422 | const double weight4 = w4[i4] * weight5; |
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| 423 | |
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| 424 | // from PD_OPEN(3,4) |
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| 425 | while (i3 < n3) { |
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| 426 | parameter[p3] = v3[i3]; // set the value for pd parameter 3 at this mesh point |
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| 427 | const double weight3 = w3[i3] * weight4; |
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| 428 | |
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| 429 | PD_OPEN(3,2) |
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| 430 | PD_OPEN(2,1) |
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| 431 | PD_OPEN(0,1) |
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| 432 | |
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[6aee3ab] | 433 | // ... main loop body ... |
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| 434 | APPLY_PROJECTION // convert jitter values to spherical coords |
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| 435 | BUILD_ROTATION // construct the rotation matrix qxy => qabc |
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| 436 | for each q |
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| 437 | FETCH_Q // set qx,qy from the q input vector |
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| 438 | APPLY_ROTATION // convert qx,qy to qa,qb,qc |
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[07646b6] | 439 | CALL_KERNEL // F2 = Iqxy(qa, qb, qc, p1, p2, ...) |
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[9ee2756] | 440 | |
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| 441 | ++step; // increment counter representing position in dispersity mesh |
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| 442 | |
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| 443 | PD_CLOSE(0) |
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| 444 | PD_CLOSE(1) |
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| 445 | PD_CLOSE(2) |
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| 446 | |
---|
| 447 | // --- PD_CLOSE(3) --- |
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| 448 | if (step >= pd_stop) break; |
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| 449 | ++i3; |
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| 450 | } |
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| 451 | i3 = 0; // reset loop counter for next round through the loop |
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| 452 | |
---|
| 453 | // --- PD_CLOSE(4) --- |
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| 454 | if (step >= pd_stop) break; |
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| 455 | ++i4; |
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[2e44ac7] | 456 | } |
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[9ee2756] | 457 | i4 = 0; // reset loop counter even though no more rounds through the loop |
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| 458 | |
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| 459 | */ |
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| 460 | |
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| 461 | |
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[6aee3ab] | 462 | // ** prepare inner loops ** |
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[9ee2756] | 463 | |
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| 464 | // Depending on the shape type (radial, axial, triaxial), the variables |
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[6aee3ab] | 465 | // and calling parameters in the loop body will be slightly different. |
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| 466 | // Macros capture the differences in one spot so the rest of the code |
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| 467 | // is easier to read. The code below both declares variables for the |
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| 468 | // inner loop and defines the macros that use them. |
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[ff10479] | 469 | |
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[01c8d9e] | 470 | |
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[c036ddb] | 471 | #if defined(CALL_FQ) // COMPUTE_F1_F2 is true |
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| 472 | // unoriented 1D returning <F> and <F^2> |
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[12f4c19] | 473 | // Note that F1 and F2 are returned from CALL_FQ by reference, and the |
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| 474 | // user of the CALL_KERNEL macro below is assuming that F1 and F2 are defined. |
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[9ee2756] | 475 | double qk; |
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[c036ddb] | 476 | double F1, F2; |
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| 477 | #define FETCH_Q() do { qk = q[q_index]; } while (0) |
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| 478 | #define BUILD_ROTATION() do {} while(0) |
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| 479 | #define APPLY_ROTATION() do {} while(0) |
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| 480 | #define CALL_KERNEL() CALL_FQ(qk,F1,F2,local_values.table) |
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| 481 | |
---|
| 482 | #elif defined(CALL_FQ_A) |
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| 483 | // unoriented 2D return <F> and <F^2> |
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[12f4c19] | 484 | // Note that the CALL_FQ_A macro is computing _F1_slot and _F2_slot by |
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| 485 | // reference then returning _F2_slot. We are calling them _F1_slot and |
---|
| 486 | // _F2_slot here so they don't conflict with _F1 and _F2 in the macro |
---|
| 487 | // expansion, or with the use of F2 = CALL_KERNEL() when it is used below. |
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[c036ddb] | 488 | double qx, qy; |
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[12f4c19] | 489 | double _F1_slot, _F2_slot; |
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[c036ddb] | 490 | #define FETCH_Q() do { qx = q[2*q_index]; qy = q[2*q_index+1]; } while (0) |
---|
| 491 | #define BUILD_ROTATION() do {} while(0) |
---|
| 492 | #define APPLY_ROTATION() do {} while(0) |
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[12f4c19] | 493 | #define CALL_KERNEL() CALL_FQ_A(sqrt(qx*qx+qy*qy),_F1_slot,_F2_slot,local_values.table) |
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[c036ddb] | 494 | |
---|
| 495 | #elif defined(CALL_IQ) |
---|
| 496 | // unoriented 1D return <F^2> |
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| 497 | double qk; |
---|
| 498 | #define FETCH_Q() do { qk = q[q_index]; } while (0) |
---|
| 499 | #define BUILD_ROTATION() do {} while(0) |
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| 500 | #define APPLY_ROTATION() do {} while(0) |
---|
| 501 | #define CALL_KERNEL() CALL_IQ(qk,local_values.table) |
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[9ee2756] | 502 | |
---|
| 503 | #elif defined(CALL_IQ_A) |
---|
| 504 | // unoriented 2D |
---|
| 505 | double qx, qy; |
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[2c108a3] | 506 | #define FETCH_Q() do { qx = q[2*q_index]; qy = q[2*q_index+1]; } while (0) |
---|
| 507 | #define BUILD_ROTATION() do {} while(0) |
---|
| 508 | #define APPLY_ROTATION() do {} while(0) |
---|
| 509 | #define CALL_KERNEL() CALL_IQ_A(sqrt(qx*qx+qy*qy), local_values.table) |
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[9ee2756] | 510 | |
---|
| 511 | #elif defined(CALL_IQ_AC) |
---|
| 512 | // oriented symmetric 2D |
---|
| 513 | double qx, qy; |
---|
[2c108a3] | 514 | #define FETCH_Q() do { qx = q[2*q_index]; qy = q[2*q_index+1]; } while (0) |
---|
[9ee2756] | 515 | double qa, qc; |
---|
| 516 | QACRotation rotation; |
---|
[ff10479] | 517 | // theta, phi, dtheta, dphi are defined below in projection to avoid repeated code. |
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[767dca8] | 518 | #define BUILD_ROTATION() qac_rotation(&rotation, theta, phi, dtheta, dphi); |
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[ec8d4ac] | 519 | #define APPLY_ROTATION() qac_apply(&rotation, qx, qy, &qa, &qc) |
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[2c108a3] | 520 | #define CALL_KERNEL() CALL_IQ_AC(qa, qc, local_values.table) |
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[9ee2756] | 521 | |
---|
| 522 | #elif defined(CALL_IQ_ABC) |
---|
| 523 | // oriented asymmetric 2D |
---|
| 524 | double qx, qy; |
---|
[2c108a3] | 525 | #define FETCH_Q() do { qx = q[2*q_index]; qy = q[2*q_index+1]; } while (0) |
---|
[9ee2756] | 526 | double qa, qb, qc; |
---|
| 527 | QABCRotation rotation; |
---|
[ff10479] | 528 | // theta, phi, dtheta, dphi are defined below in projection to avoid repeated code. |
---|
| 529 | // psi and dpsi are only for IQ_ABC, so they are processed here. |
---|
| 530 | const double psi = values[details->theta_par+4]; |
---|
[6aee3ab] | 531 | local_values.table.psi = 0.; |
---|
[ff10479] | 532 | #define BUILD_ROTATION() qabc_rotation(&rotation, theta, phi, psi, dtheta, dphi, local_values.table.psi) |
---|
[ec8d4ac] | 533 | #define APPLY_ROTATION() qabc_apply(&rotation, qx, qy, &qa, &qb, &qc) |
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[ff10479] | 534 | #define CALL_KERNEL() CALL_IQ_ABC(qa, qb, qc, local_values.table) |
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[c036ddb] | 535 | |
---|
[108e70e] | 536 | #elif defined(CALL_IQ_XY) |
---|
| 537 | // direct call to qx,qy calculator |
---|
| 538 | double qx, qy; |
---|
| 539 | #define FETCH_Q() do { qx = q[2*q_index]; qy = q[2*q_index+1]; } while (0) |
---|
| 540 | #define BUILD_ROTATION() do {} while(0) |
---|
| 541 | #define APPLY_ROTATION() do {} while(0) |
---|
| 542 | #define CALL_KERNEL() CALL_IQ_XY(qx, qy, local_values.table) |
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[ff10479] | 543 | #endif |
---|
| 544 | |
---|
[2a7e20e] | 545 | // Define APPLY_PROJECTION depending on model symmetries. We do this outside |
---|
| 546 | // the previous if block so that we don't need to repeat the identical |
---|
| 547 | // logic in the IQ_AC and IQ_ABC branches. This will become more important |
---|
| 548 | // if we implement more projections, or more complicated projections. |
---|
[c036ddb] | 549 | #if defined(CALL_IQ) || defined(CALL_IQ_A) || defined(CALL_FQ) || defined(CALL_FQ_A) |
---|
| 550 | // no orientation |
---|
[ff10479] | 551 | #define APPLY_PROJECTION() const double weight=weight0 |
---|
[2a7e20e] | 552 | #elif defined(CALL_IQ_XY) // pass orientation to the model |
---|
[108e70e] | 553 | // CRUFT: support oriented model which define Iqxy rather than Iqac or Iqabc |
---|
| 554 | // Need to plug the values for the orientation angles back into parameter |
---|
| 555 | // table in case they were overridden by the orientation offset. This |
---|
| 556 | // means that orientation dispersity will not work for these models, but |
---|
| 557 | // it was broken anyway, so no matter. Still want to provide Iqxy in case |
---|
| 558 | // the user model wants full control of orientation/magnetism. |
---|
| 559 | #if defined(HAVE_PSI) |
---|
| 560 | const double theta = values[details->theta_par+2]; |
---|
| 561 | const double phi = values[details->theta_par+3]; |
---|
| 562 | const double psi = values[details->theta_par+4]; |
---|
| 563 | double weight; |
---|
| 564 | #define APPLY_PROJECTION() do { \ |
---|
| 565 | local_values.table.theta = theta; \ |
---|
| 566 | local_values.table.phi = phi; \ |
---|
| 567 | local_values.table.psi = psi; \ |
---|
| 568 | weight=weight0; \ |
---|
| 569 | } while (0) |
---|
| 570 | #elif defined(HAVE_THETA) |
---|
| 571 | const double theta = values[details->theta_par+2]; |
---|
| 572 | const double phi = values[details->theta_par+3]; |
---|
| 573 | double weight; |
---|
| 574 | #define APPLY_PROJECTION() do { \ |
---|
| 575 | local_values.table.theta = theta; \ |
---|
| 576 | local_values.table.phi = phi; \ |
---|
| 577 | weight=weight0; \ |
---|
| 578 | } while (0) |
---|
| 579 | #else |
---|
| 580 | #define APPLY_PROJECTION() const double weight=weight0 |
---|
| 581 | #endif |
---|
[2a7e20e] | 582 | #else // apply jitter and view before calling the model |
---|
[9ee2756] | 583 | // Grab the "view" angles (theta, phi, psi) from the initial parameter table. |
---|
| 584 | const double theta = values[details->theta_par+2]; |
---|
| 585 | const double phi = values[details->theta_par+3]; |
---|
[6aee3ab] | 586 | // Make sure jitter angle defaults to zero if there is no jitter distribution |
---|
| 587 | local_values.table.theta = 0.; |
---|
| 588 | local_values.table.phi = 0.; |
---|
[ff10479] | 589 | // The "jitter" angles (dtheta, dphi, dpsi) are stored with the |
---|
| 590 | // dispersity values and copied to the local parameter table as |
---|
| 591 | // we go through the mesh. |
---|
| 592 | double dtheta, dphi, weight; |
---|
[2a7e20e] | 593 | #if PROJECTION == 1 // equirectangular |
---|
[ff10479] | 594 | #define APPLY_PROJECTION() do { \ |
---|
[767dca8] | 595 | dtheta = local_values.table.theta; \ |
---|
| 596 | dphi = local_values.table.phi; \ |
---|
[ff10479] | 597 | weight = fabs(cos(dtheta*M_PI_180)) * weight0; \ |
---|
[767dca8] | 598 | } while (0) |
---|
[2a7e20e] | 599 | #elif PROJECTION == 2 // sinusoidal |
---|
[ff10479] | 600 | #define APPLY_PROJECTION() do { \ |
---|
[767dca8] | 601 | dtheta = local_values.table.theta; \ |
---|
| 602 | dphi = local_values.table.phi; \ |
---|
[ff10479] | 603 | weight = weight0; \ |
---|
| 604 | if (dtheta != 90.0) dphi /= cos(dtheta*M_PI_180); \ |
---|
| 605 | else if (dphi != 0.0) weight = 0.; \ |
---|
| 606 | if (fabs(dphi) >= 180.) weight = 0.; \ |
---|
[767dca8] | 607 | } while (0) |
---|
| 608 | #endif |
---|
[2a7e20e] | 609 | #endif // done defining APPLY_PROJECTION |
---|
[9ee2756] | 610 | |
---|
[6aee3ab] | 611 | // ** define looping macros ** |
---|
| 612 | |
---|
| 613 | // Define looping variables |
---|
| 614 | #define PD_INIT(_LOOP) \ |
---|
| 615 | const int n##_LOOP = details->pd_length[_LOOP]; \ |
---|
| 616 | const int p##_LOOP = details->pd_par[_LOOP]; \ |
---|
[74e9b5f] | 617 | pglobal const double *v##_LOOP = pd_value + details->pd_offset[_LOOP]; \ |
---|
| 618 | pglobal const double *w##_LOOP = pd_weight + details->pd_offset[_LOOP]; \ |
---|
[6aee3ab] | 619 | int i##_LOOP = (pd_start/details->pd_stride[_LOOP])%n##_LOOP; |
---|
| 620 | |
---|
| 621 | // Jump into the middle of the dispersity loop |
---|
| 622 | #define PD_OPEN(_LOOP,_OUTER) \ |
---|
| 623 | while (i##_LOOP < n##_LOOP) { \ |
---|
| 624 | local_values.vector[p##_LOOP] = v##_LOOP[i##_LOOP]; \ |
---|
| 625 | const double weight##_LOOP = w##_LOOP[i##_LOOP] * weight##_OUTER; |
---|
| 626 | |
---|
| 627 | // create the variable "weight#=1.0" where # is the outermost level+1 (=MAX_PD). |
---|
| 628 | #define _PD_OUTERMOST_WEIGHT(_n) const double weight##_n = 1.0; |
---|
| 629 | #define PD_OUTERMOST_WEIGHT(_n) _PD_OUTERMOST_WEIGHT(_n) |
---|
| 630 | |
---|
| 631 | // Close out the loop |
---|
| 632 | #define PD_CLOSE(_LOOP) \ |
---|
| 633 | if (step >= pd_stop) break; \ |
---|
| 634 | ++i##_LOOP; \ |
---|
| 635 | } \ |
---|
| 636 | i##_LOOP = 0; |
---|
[9eb3632] | 637 | |
---|
[9ee2756] | 638 | // ====== construct the loops ======= |
---|
| 639 | |
---|
| 640 | // Pointers to the start of the dispersity and weight vectors, if needed. |
---|
[7b7da6b] | 641 | #if MAX_PD>0 |
---|
[74e9b5f] | 642 | pglobal const double *pd_value = values + NUM_VALUES; |
---|
| 643 | pglobal const double *pd_weight = pd_value + details->num_weights; |
---|
[7b7da6b] | 644 | #endif |
---|
[9eb3632] | 645 | |
---|
[9ee2756] | 646 | // The variable "step" is the current position in the dispersity loop. |
---|
| 647 | // It will be incremented each time a new point in the mesh is accumulated, |
---|
| 648 | // and used to test whether we have reached pd_stop. |
---|
| 649 | int step = pd_start; |
---|
| 650 | |
---|
[6aee3ab] | 651 | // *** define loops for each of 0, 1, 2, ..., modelinfo.MAX_PD-1 *** |
---|
| 652 | |
---|
[9ee2756] | 653 | // define looping variables |
---|
[9eb3632] | 654 | #if MAX_PD>4 |
---|
[9ee2756] | 655 | PD_INIT(4) |
---|
[9eb3632] | 656 | #endif |
---|
| 657 | #if MAX_PD>3 |
---|
[9ee2756] | 658 | PD_INIT(3) |
---|
[9eb3632] | 659 | #endif |
---|
| 660 | #if MAX_PD>2 |
---|
[9ee2756] | 661 | PD_INIT(2) |
---|
[9eb3632] | 662 | #endif |
---|
| 663 | #if MAX_PD>1 |
---|
[9ee2756] | 664 | PD_INIT(1) |
---|
[9eb3632] | 665 | #endif |
---|
| 666 | #if MAX_PD>0 |
---|
[9ee2756] | 667 | PD_INIT(0) |
---|
[9eb3632] | 668 | #endif |
---|
[2e44ac7] | 669 | |
---|
[9ee2756] | 670 | // open nested loops |
---|
| 671 | PD_OUTERMOST_WEIGHT(MAX_PD) |
---|
[9eb3632] | 672 | #if MAX_PD>4 |
---|
[9ee2756] | 673 | PD_OPEN(4,5) |
---|
[9eb3632] | 674 | #endif |
---|
| 675 | #if MAX_PD>3 |
---|
[9ee2756] | 676 | PD_OPEN(3,4) |
---|
[9eb3632] | 677 | #endif |
---|
| 678 | #if MAX_PD>2 |
---|
[9ee2756] | 679 | PD_OPEN(2,3) |
---|
[9eb3632] | 680 | #endif |
---|
| 681 | #if MAX_PD>1 |
---|
[9ee2756] | 682 | PD_OPEN(1,2) |
---|
[9eb3632] | 683 | #endif |
---|
| 684 | #if MAX_PD>0 |
---|
[9ee2756] | 685 | PD_OPEN(0,1) |
---|
[9eb3632] | 686 | #endif |
---|
[5ff1b03] | 687 | |
---|
[9ee2756] | 688 | //if (q_index==0) {printf("step:%d of %d, pars:",step,pd_stop); for (int i=0; i < NUM_PARS; i++) printf("p%d=%g ",i, local_values.vector[i]); printf("\n");} |
---|
| 689 | |
---|
| 690 | // ====== loop body ======= |
---|
| 691 | #ifdef INVALID |
---|
| 692 | if (!INVALID(local_values.table)) |
---|
| 693 | #endif |
---|
| 694 | { |
---|
[ff10479] | 695 | APPLY_PROJECTION(); |
---|
| 696 | |
---|
[9ee2756] | 697 | // Accumulate I(q) |
---|
| 698 | // Note: weight==0 must always be excluded |
---|
[767dca8] | 699 | if (weight > cutoff) { |
---|
[e44432d] | 700 | double form, shell; |
---|
| 701 | CALL_VOLUME(form, shell, local_values.table); |
---|
[c036ddb] | 702 | weight_norm += weight; |
---|
[e44432d] | 703 | weighted_form += weight * form; |
---|
| 704 | weighted_shell += weight * shell; |
---|
[a34b811] | 705 | if (radius_effective_mode != 0) { |
---|
| 706 | weighted_radius += weight * CALL_RADIUS_EFFECTIVE(radius_effective_mode, local_values.table); |
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[6e7ba14] | 707 | } |
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[2c108a3] | 708 | BUILD_ROTATION(); |
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[c036ddb] | 709 | |
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[0db7dbd] | 710 | #if !defined(USE_GPU) |
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[9ee2756] | 711 | // DLL needs to explicitly loop over the q values. |
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| 712 | #ifdef USE_OPENMP |
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| 713 | #pragma omp parallel for |
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| 714 | #endif |
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| 715 | for (q_index=0; q_index<nq; q_index++) |
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[0db7dbd] | 716 | #endif // !USE_GPU |
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[9ee2756] | 717 | { |
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| 718 | |
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[2c108a3] | 719 | FETCH_Q(); |
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| 720 | APPLY_ROTATION(); |
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[9ee2756] | 721 | |
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| 722 | // ======= COMPUTE SCATTERING ========== |
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| 723 | #if defined(MAGNETIC) && NUM_MAGNETIC > 0 |
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[2c108a3] | 724 | // Compute the scattering from the magnetic cross sections. |
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[07646b6] | 725 | double F2 = 0.0; |
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[2c108a3] | 726 | const double qsq = qx*qx + qy*qy; |
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| 727 | if (qsq > 1.e-16) { |
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| 728 | // TODO: what is the magnetic scattering at q=0 |
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| 729 | const double px = (qy*cos_mspin + qx*sin_mspin)/qsq; |
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| 730 | const double py = (qy*sin_mspin - qx*cos_mspin)/qsq; |
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| 731 | |
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| 732 | // loop over uu, ud real, du real, dd, ud imag, du imag |
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[aadec17] | 733 | for (unsigned int xs=0; xs<6; xs++) { |
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[885753a] | 734 | const double xs_weight = xs_weights[xs]; |
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[2c108a3] | 735 | if (xs_weight > 1.e-8) { |
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| 736 | // Since the cross section weight is significant, set the slds |
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| 737 | // to the effective slds for this cross section, call the |
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| 738 | // kernel, and add according to weight. |
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| 739 | for (int sk=0; sk<NUM_MAGNETIC; sk++) { |
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| 740 | const int32_t mag_index = NUM_PARS+5 + 3*sk; |
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| 741 | const int32_t sld_index = slds[sk]; |
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| 742 | const double mx = values[mag_index]; |
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| 743 | const double my = values[mag_index+1]; |
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| 744 | const double mz = values[mag_index+2]; |
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| 745 | local_values.vector[sld_index] = |
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| 746 | mag_sld(xs, qx, qy, px, py, values[sld_index+2], mx, my, mz); |
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[885753a] | 747 | //if (q_index==0) printf("%d: (qx,qy)=(%g,%g) xs=%d sld%d=%g p=(%g,%g) m=(%g,%g,%g)\n", |
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[dc6f601] | 748 | // q_index, qx, qy, xs, sk, local_values.vector[sld_index], px, py, mx, my, mz); |
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[2c108a3] | 749 | } |
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[07646b6] | 750 | F2 += xs_weight * CALL_KERNEL(); |
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[a4280bd] | 751 | } |
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[9eb3632] | 752 | } |
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[32e3c9b] | 753 | } |
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[9ee2756] | 754 | #else // !MAGNETIC |
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[e44432d] | 755 | #if defined(CALL_FQ) |
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[c036ddb] | 756 | CALL_KERNEL(); // sets F1 and F2 by reference |
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[01c8d9e] | 757 | #else |
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[07646b6] | 758 | const double F2 = CALL_KERNEL(); |
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[01c8d9e] | 759 | #endif |
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[9ee2756] | 760 | #endif // !MAGNETIC |
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[07646b6] | 761 | //printf("q_index:%d %g %g %g %g\n", q_index, F2, weight0); |
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[9ee2756] | 762 | |
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[0db7dbd] | 763 | #if defined(USE_GPU) |
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[e44432d] | 764 | #if defined(CALL_FQ) |
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[c036ddb] | 765 | this_F2 += weight * F2; |
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[6e7ba14] | 766 | this_F1 += weight * F1; |
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[c036ddb] | 767 | #else |
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[07646b6] | 768 | this_F2 += weight * F2; |
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[01c8d9e] | 769 | #endif |
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[9ee2756] | 770 | #else // !USE_OPENCL |
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[e44432d] | 771 | #if defined(CALL_FQ) |
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[6e7ba14] | 772 | result[2*q_index+0] += weight * F2; |
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| 773 | result[2*q_index+1] += weight * F1; |
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[c036ddb] | 774 | #else |
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[07646b6] | 775 | result[q_index] += weight * F2; |
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[01c8d9e] | 776 | #endif |
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[9ee2756] | 777 | #endif // !USE_OPENCL |
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[3044216] | 778 | } |
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[03cac08] | 779 | } |
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[2e44ac7] | 780 | } |
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[9ee2756] | 781 | // close nested loops |
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| 782 | ++step; |
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| 783 | #if MAX_PD>0 |
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| 784 | PD_CLOSE(0) |
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[9eb3632] | 785 | #endif |
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| 786 | #if MAX_PD>1 |
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[9ee2756] | 787 | PD_CLOSE(1) |
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[9eb3632] | 788 | #endif |
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| 789 | #if MAX_PD>2 |
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[9ee2756] | 790 | PD_CLOSE(2) |
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[9eb3632] | 791 | #endif |
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| 792 | #if MAX_PD>3 |
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[9ee2756] | 793 | PD_CLOSE(3) |
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[9eb3632] | 794 | #endif |
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| 795 | #if MAX_PD>4 |
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[9ee2756] | 796 | PD_CLOSE(4) |
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[9eb3632] | 797 | #endif |
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[f2f67a6] | 798 | |
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[07646b6] | 799 | // Remember the results and the updated norm. |
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[0db7dbd] | 800 | #if defined(USE_GPU) |
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[e44432d] | 801 | #if defined(CALL_FQ) |
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[07646b6] | 802 | result[2*q_index+0] = this_F2; |
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| 803 | result[2*q_index+1] = this_F1; |
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[c036ddb] | 804 | #else |
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[07646b6] | 805 | result[q_index] = this_F2; |
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[01c8d9e] | 806 | #endif |
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[07646b6] | 807 | if (q_index == 0) |
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| 808 | #endif |
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| 809 | { |
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| 810 | #if defined(CALL_FQ) |
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[6e7ba14] | 811 | result[2*nq] = weight_norm; |
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[e44432d] | 812 | result[2*nq+1] = weighted_form; |
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| 813 | result[2*nq+2] = weighted_shell; |
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| 814 | result[2*nq+3] = weighted_radius; |
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[07646b6] | 815 | #else |
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[6e7ba14] | 816 | result[nq] = weight_norm; |
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[e44432d] | 817 | result[nq+1] = weighted_form; |
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| 818 | result[nq+2] = weighted_shell; |
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| 819 | result[nq+3] = weighted_radius; |
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[07646b6] | 820 | #endif |
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| 821 | } |
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[2c108a3] | 822 | |
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[6aee3ab] | 823 | // ** clear the macros in preparation for the next kernel ** |
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[2c108a3] | 824 | #undef PD_INIT |
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| 825 | #undef PD_OPEN |
---|
| 826 | #undef PD_CLOSE |
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| 827 | #undef FETCH_Q |
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[ff10479] | 828 | #undef APPLY_PROJECTION |
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[2c108a3] | 829 | #undef BUILD_ROTATION |
---|
| 830 | #undef APPLY_ROTATION |
---|
| 831 | #undef CALL_KERNEL |
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[2e44ac7] | 832 | } |
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