1 | #include "mex.h" |
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2 | #include<math.h> |
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3 | #include "../atlalib.c" |
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4 | #include "elempass.h" |
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5 | |
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6 | |
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7 | #define DRIFT1 0.6756035959798286638 |
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8 | #define DRIFT2 -0.1756035959798286639 |
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9 | #define KICK1 1.351207191959657328 |
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10 | #define KICK2 -1.702414383919314656 |
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11 | |
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12 | |
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13 | |
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14 | |
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15 | #define SQR(X) ((X)*(X)) |
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16 | |
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17 | |
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18 | |
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19 | double StrB2perp(double bx, double by, |
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20 | double x, double xpr, double y, double ypr) |
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21 | /* Calculates sqr(|B x e|) , where e is a unit vector in the direction of velocity */ |
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22 | |
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23 | { double v_norm2; |
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24 | v_norm2 = 1/(1 + SQR(xpr) + SQR(ypr)); |
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25 | |
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26 | /* components of the normalized velocity vector |
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27 | double ex, ey, ez; |
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28 | ex = xpr; |
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29 | ey = ypr; |
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30 | ez = 1; |
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31 | */ |
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32 | |
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33 | return((SQR(by) + SQR(bx) + SQR(bx*ypr - by*xpr) )*v_norm2) ; |
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34 | |
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35 | } |
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36 | |
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37 | |
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38 | |
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39 | |
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40 | void strthinkickrad(double* r, double* A, double* B, double L, double E0, int max_order) |
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41 | |
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42 | /***************************************************************************** |
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43 | Calculate and apply |
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44 | (a) multipole kick |
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45 | (b) momentum kick due to classical radiation |
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46 | to a 6-dimentional phase space vector in a straight element ( quadrupole) |
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47 | |
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48 | IMPORTANT !!! |
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49 | The reference coordinate system is straight but the field expansion may still |
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50 | contain dipole terms: PolynomA(1), PolynomB(1) - in MATLAB notation, |
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51 | A[0], B[0] - C,C++ notation |
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52 | |
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53 | |
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54 | Note: According to US convention the transverse multipole field is written as: |
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55 | |
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56 | max_order+1 |
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57 | ---- |
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58 | \ n-1 |
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59 | (B + iB )/ B rho = > (ia + b ) (x + iy) |
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60 | y x / n n |
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61 | ---- |
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62 | n=1 |
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63 | is a polynomial in (x,y) with the highest order = MaxOrder |
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64 | |
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65 | |
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66 | Using different index notation |
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67 | |
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68 | max_order |
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69 | ---- |
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70 | \ n |
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71 | (B + iB )/ B rho = > (iA + B ) (x + iy) |
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72 | y x / n n |
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73 | ---- |
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74 | n=0 |
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75 | |
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76 | A,B: i=0 ... max_order |
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77 | [0] - dipole, [1] - quadrupole, [2] - sextupole ... |
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78 | units for A,B[i] = 1/[m]^(i+1) |
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79 | Coeficients are stroed in the PolynomA, PolynomB field of the element |
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80 | structure in MATLAB |
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81 | |
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82 | A[i] (C++,C) = PolynomA(i+1) (MATLAB) |
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83 | B[i] (C++,C) = PolynomB(i+1) (MATLAB) |
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84 | i = 0 .. MaxOrder |
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85 | |
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86 | ******************************************************************************/ |
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87 | { int i; |
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88 | double ReSumTemp; |
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89 | double ReSum = B[max_order]; |
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90 | double ImSum = A[max_order]; |
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91 | double x ,xpr, y, ypr, p_norm, B2P; |
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92 | |
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93 | #define TWOPI 6.28318530717959 |
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94 | #define CGAMMA 8.846056192e-05 |
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95 | |
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96 | |
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97 | double CRAD = CGAMMA*E0*E0*E0/(TWOPI*1e27); /* [m]/[GeV^3] M.Sands (4.1) */ |
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98 | |
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99 | |
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100 | |
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101 | |
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102 | /* recursively calculate the local transvrese magnetic field |
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103 | Bx = ImSum, By = ReSum |
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104 | */ |
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105 | for(i=max_order-1;i>=0;i--) |
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106 | { ReSumTemp = ReSum*r[0] - ImSum*r[2] + B[i]; |
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107 | ImSum = ImSum*r[0] + ReSum*r[2] + A[i]; |
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108 | ReSum = ReSumTemp; |
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109 | } |
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110 | |
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111 | |
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112 | /* calculate angles from momentums */ |
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113 | p_norm = 1/(1+r[4]); |
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114 | x = r[0]; |
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115 | xpr = r[1]*p_norm; |
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116 | y = r[2]; |
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117 | ypr = r[3]*p_norm; |
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118 | |
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119 | /* For instantaneous rate of energy loss due to classical radiation |
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120 | need to calculate |n x B|^2, n unit vector in the direction of velocity |
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121 | */ |
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122 | B2P = StrB2perp(ImSum, ReSum , x , xpr, y ,ypr); |
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123 | |
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124 | |
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125 | r[4] = r[4] - CRAD*(1+r[4])*(1+r[4])*B2P*(1 + (SQR(xpr)+SQR(ypr))/2 )*L; |
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126 | |
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127 | /* recalculate momentums from angles after losing energy for radiation */ |
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128 | p_norm = 1/(1+r[4]); |
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129 | r[1] = xpr/p_norm; |
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130 | r[3] = ypr/p_norm; |
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131 | |
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132 | |
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133 | r[1] -= L*ReSum; |
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134 | r[3] += L*ImSum; |
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135 | |
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136 | } |
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137 | |
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138 | |
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139 | |
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140 | void StrMPoleSymplectic4RadPass(double *r, double le, double *A, double *B, |
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141 | int max_order, int num_int_steps, |
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142 | double *T1, double *T2, |
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143 | double *R1, double *R2, |
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144 | double E0, |
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145 | int num_particles) |
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146 | |
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147 | |
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148 | { int c,m; |
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149 | double *r6; |
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150 | double SL, L1, L2, K1, K2; |
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151 | bool useT1, useT2, useR1, useR2; |
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152 | SL = le/num_int_steps; |
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153 | L1 = SL*DRIFT1; |
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154 | L2 = SL*DRIFT2; |
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155 | K1 = SL*KICK1; |
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156 | K2 = SL*KICK2; |
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157 | |
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158 | |
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159 | if(T1==NULL) |
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160 | useT1=false; |
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161 | else |
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162 | useT1=true; |
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163 | |
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164 | if(T2==NULL) |
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165 | useT2=false; |
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166 | else |
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167 | useT2=true; |
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168 | |
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169 | if(R1==NULL) |
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170 | useR1=false; |
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171 | else |
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172 | useR1=true; |
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173 | |
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174 | if(R2==NULL) |
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175 | useR2=false; |
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176 | else |
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177 | useR2=true; |
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178 | for(c = 0;c<num_particles;c++) /* Loop over particles */ |
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179 | { r6 = r+c*6; |
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180 | if(!mxIsNaN(r6[0])) |
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181 | { |
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182 | |
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183 | /* misalignment at entrance */ |
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184 | if(useT1) |
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185 | ATaddvv(r6,T1); |
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186 | if(useR1) |
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187 | ATmultmv(r6,R1); |
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188 | |
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189 | /* integrator */ |
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190 | for(m=0; m < num_int_steps; m++) /* Loop over slices */ |
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191 | { r6 = r+c*6; |
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192 | |
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193 | ATdrift6(r6,L1); |
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194 | strthinkickrad(r6, A, B, K1, E0, max_order); |
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195 | ATdrift6(r6,L2); |
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196 | strthinkickrad(r6, A, B, K2, E0, max_order); |
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197 | ATdrift6(r6,L2); |
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198 | strthinkickrad(r6, A, B, K1, E0, max_order); |
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199 | ATdrift6(r6,L1); |
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200 | } |
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201 | /* Misalignment at exit */ |
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202 | if(useR2) |
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203 | ATmultmv(r6,R2); |
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204 | if(useT2) |
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205 | ATaddvv(r6,T2); |
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206 | |
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207 | } |
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208 | } |
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209 | } |
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210 | |
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211 | |
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212 | |
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213 | |
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214 | |
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215 | |
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216 | ExportMode int* passFunction(const mxArray *ElemData, int *FieldNumbers, |
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217 | double *r_in, int num_particles, int mode) |
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218 | |
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219 | #define NUM_FIELDS_2_REMEMBER 11 |
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220 | |
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221 | |
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222 | { double *A , *B; |
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223 | double *pr1, *pr2, *pt1, *pt2, *ka; |
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224 | double E0; /* Design energy [eV] */ |
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225 | |
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226 | |
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227 | |
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228 | int max_order, num_int_steps; |
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229 | double le; |
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230 | int *returnptr; |
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231 | int *NewFieldNumbers, fnum; |
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232 | |
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233 | switch(mode) |
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234 | { case NO_LOCAL_COPY: /* Obsolete in AT1.3 */ |
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235 | { |
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236 | |
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237 | } break; |
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238 | |
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239 | case MAKE_LOCAL_COPY: /* Find field numbers first |
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240 | Save a list of field number in an array |
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241 | and make returnptr point to that array |
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242 | */ |
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243 | { /* Allocate memory for integer array of |
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244 | field numbers for faster futurereference |
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245 | */ |
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246 | NewFieldNumbers = (int*)mxCalloc(NUM_FIELDS_2_REMEMBER,sizeof(int)); |
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247 | |
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248 | /* Populate */ |
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249 | |
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250 | fnum = mxGetFieldNumber(ElemData,"PolynomA"); |
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251 | if(fnum<0) |
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252 | mexErrMsgTxt("Required field 'PolynomA' was not found in the element data structure"); |
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253 | NewFieldNumbers[0] = fnum; |
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254 | A = mxGetPr(mxGetFieldByNumber(ElemData,0,fnum)); |
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255 | |
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256 | |
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257 | fnum = mxGetFieldNumber(ElemData,"PolynomB"); |
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258 | if(fnum<0) |
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259 | mexErrMsgTxt("Required field 'PolynomB' was not found in the element data structure"); |
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260 | NewFieldNumbers[1] = fnum; |
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261 | B = mxGetPr(mxGetFieldByNumber(ElemData,0,fnum)); |
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262 | |
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263 | |
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264 | |
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265 | fnum = mxGetFieldNumber(ElemData,"MaxOrder"); |
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266 | if(fnum<0) |
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267 | mexErrMsgTxt("Required field 'MaxOrder' was not found in the element data structure"); |
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268 | NewFieldNumbers[2] = fnum; |
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269 | max_order = (int)mxGetScalar(mxGetFieldByNumber(ElemData,0,fnum)); |
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270 | |
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271 | |
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272 | fnum = mxGetFieldNumber(ElemData,"NumIntSteps"); |
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273 | if(fnum<0) |
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274 | mexErrMsgTxt("Required field 'NumIntSteps' was not found in the element data structure"); |
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275 | NewFieldNumbers[3] = fnum; |
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276 | num_int_steps = (int)mxGetScalar(mxGetFieldByNumber(ElemData,0,fnum)); |
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277 | |
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278 | |
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279 | fnum = mxGetFieldNumber(ElemData,"Length"); |
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280 | if(fnum<0) |
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281 | mexErrMsgTxt("Required field 'Length' was not found in the element data structure"); |
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282 | NewFieldNumbers[4] = fnum; |
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283 | le = mxGetScalar(mxGetFieldByNumber(ElemData,0,fnum)); |
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284 | |
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285 | fnum = mxGetFieldNumber(ElemData,"Energy"); |
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286 | if(fnum<0) |
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287 | mexErrMsgTxt("Required field 'Energy' was not found in the element data structure"); |
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288 | NewFieldNumbers[5] = fnum; |
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289 | E0 = mxGetScalar(mxGetFieldByNumber(ElemData,0,fnum)); |
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290 | |
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291 | |
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292 | fnum = mxGetFieldNumber(ElemData,"R1"); |
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293 | NewFieldNumbers[6] = fnum; |
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294 | if(fnum<0) |
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295 | pr1 = NULL; |
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296 | else |
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297 | pr1 = mxGetPr(mxGetFieldByNumber(ElemData,0,fnum)); |
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298 | |
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299 | |
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300 | fnum = mxGetFieldNumber(ElemData,"R2"); |
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301 | NewFieldNumbers[7] = fnum; |
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302 | if(fnum<0) |
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303 | pr2 = NULL; |
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304 | else |
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305 | pr2 = mxGetPr(mxGetFieldByNumber(ElemData,0,fnum)); |
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306 | |
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307 | |
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308 | fnum = mxGetFieldNumber(ElemData,"T1"); |
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309 | NewFieldNumbers[8] = fnum; |
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310 | if(fnum<0) |
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311 | pt1 = NULL; |
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312 | else |
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313 | pt1 = mxGetPr(mxGetFieldByNumber(ElemData,0,fnum)); |
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314 | |
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315 | |
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316 | fnum = mxGetFieldNumber(ElemData,"T2"); |
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317 | NewFieldNumbers[9] = fnum; |
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318 | if(fnum<0) |
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319 | pt2 = NULL; |
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320 | else |
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321 | pt2 = mxGetPr(mxGetFieldByNumber(ElemData,0,fnum)); |
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322 | |
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323 | |
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324 | /* Optional: Kick angles, see section below for explanation */ |
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325 | /* Kicks from multipole elements can be specified as angles. This handles the |
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326 | case where corrector coils are used in sextupoles and used for orbit |
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327 | correction. */ |
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328 | fnum = mxGetFieldNumber(ElemData,"KickAngle"); |
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329 | NewFieldNumbers[10] = fnum; |
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330 | if(fnum<0) |
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331 | ka = NULL; |
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332 | else |
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333 | ka = mxGetPr(mxGetFieldByNumber(ElemData,0,fnum)); |
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334 | |
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335 | |
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336 | returnptr = NewFieldNumbers; |
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337 | |
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338 | } break; |
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339 | |
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340 | case USE_LOCAL_COPY: /* Get fields from MATLAB using field numbers |
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341 | The second argument ponter to the array of field |
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342 | numbers is previously created with |
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343 | QuadLinPass( ..., MAKE_LOCAL_COPY) |
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344 | */ |
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345 | |
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346 | { A = mxGetPr(mxGetFieldByNumber(ElemData,0,FieldNumbers[0])); |
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347 | B = mxGetPr(mxGetFieldByNumber(ElemData,0,FieldNumbers[1])); |
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348 | max_order = (int)mxGetScalar(mxGetFieldByNumber(ElemData,0,FieldNumbers[2])); |
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349 | num_int_steps = (int)mxGetScalar(mxGetFieldByNumber(ElemData,0,FieldNumbers[3])); |
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350 | le = mxGetScalar(mxGetFieldByNumber(ElemData,0,FieldNumbers[4])); |
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351 | E0 = mxGetScalar(mxGetFieldByNumber(ElemData,0,FieldNumbers[5])); |
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352 | |
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353 | |
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354 | /* Optional fields */ |
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355 | if(FieldNumbers[6]<0) |
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356 | pr1 = NULL; |
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357 | else |
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358 | pr1 = mxGetPr(mxGetFieldByNumber(ElemData,0,FieldNumbers[6])); |
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359 | |
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360 | if(FieldNumbers[7]<0) |
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361 | pr2 = NULL; |
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362 | else |
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363 | pr2 = mxGetPr(mxGetFieldByNumber(ElemData,0,FieldNumbers[7])); |
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364 | |
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365 | |
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366 | if(FieldNumbers[8]<0) |
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367 | pt1 = NULL; |
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368 | else |
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369 | pt1 = mxGetPr(mxGetFieldByNumber(ElemData,0,FieldNumbers[8])); |
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370 | |
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371 | if(FieldNumbers[9]<0) |
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372 | pt2 = NULL; |
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373 | else |
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374 | pt2 = mxGetPr(mxGetFieldByNumber(ElemData,0,FieldNumbers[9])); |
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375 | |
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376 | if(FieldNumbers[10]<0) |
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377 | ka = NULL; |
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378 | else |
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379 | ka = mxGetPr(mxGetFieldByNumber(ElemData,0,FieldNumbers[9])); |
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380 | |
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381 | returnptr = FieldNumbers; |
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382 | |
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383 | } break; |
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384 | default: |
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385 | { mexErrMsgTxt("No match for calling mode in function StrMPoleSymplectic4RadPass\n"); |
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386 | } |
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387 | } |
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388 | |
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389 | |
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390 | if(ka!=NULL) |
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391 | { |
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392 | /* Positive angle must correspond to -ve B field since +ve B field corresponds |
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393 | to a bend with the same curvature as the bend magnets. |
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394 | */ |
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395 | B[0] -= sin(ka[0])/le; |
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396 | A[0] += sin(ka[1])/le; |
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397 | } |
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398 | |
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399 | StrMPoleSymplectic4RadPass(r_in, le, A, B, max_order, num_int_steps,pt1, pt2, pr1, pr2, E0, num_particles); |
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400 | |
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401 | if(ka!=NULL) |
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402 | { |
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403 | B[0] += sin(ka[0])/le; |
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404 | A[0] -= sin(ka[1])/le; |
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405 | } |
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406 | |
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407 | return(returnptr); |
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408 | |
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409 | } |
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410 | |
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411 | |
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412 | |
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413 | |
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414 | |
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415 | |
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416 | |
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417 | |
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418 | |
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419 | void mexFunction( int nlhs, mxArray *plhs[], int nrhs, const mxArray *prhs[]) |
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420 | { int m,n; |
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421 | double *r_in; |
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422 | double le, *A, *B; |
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423 | int max_order, num_int_steps; |
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424 | double *pr1, *pr2, *pt1, *pt2, *ka; |
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425 | mxArray *tmpmxptr; |
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426 | double E0; /* Design energy [eV] */ |
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427 | |
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428 | |
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429 | if(nrhs) |
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430 | { |
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431 | /* ALLOCATE memory for the output array of the same size as the input */ |
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432 | m = mxGetM(prhs[1]); |
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433 | n = mxGetN(prhs[1]); |
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434 | if(m!=6) |
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435 | mexErrMsgTxt("Second argument must be a 6 x N matrix"); |
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436 | |
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437 | |
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438 | |
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439 | tmpmxptr =mxGetField(prhs[0],0,"PolynomA"); |
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440 | if(tmpmxptr) |
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441 | A = mxGetPr(tmpmxptr); |
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442 | else |
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443 | mexErrMsgTxt("Required field 'PolynomA' was not found in the element data structure"); |
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444 | |
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445 | tmpmxptr =mxGetField(prhs[0],0,"PolynomB"); |
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446 | if(tmpmxptr) |
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447 | B = mxGetPr(tmpmxptr); |
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448 | else |
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449 | mexErrMsgTxt("Required field 'PolynomB' was not found in the element data structure"); |
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450 | |
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451 | tmpmxptr = mxGetField(prhs[0],0,"MaxOrder"); |
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452 | if(tmpmxptr) |
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453 | max_order = (int)mxGetScalar(tmpmxptr); |
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454 | else |
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455 | mexErrMsgTxt("Required field 'MaxOrder' was not found in the element data structure"); |
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456 | |
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457 | tmpmxptr = mxGetField(prhs[0],0,"NumIntSteps"); |
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458 | if(tmpmxptr) |
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459 | num_int_steps = (int)mxGetScalar(tmpmxptr); |
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460 | else |
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461 | mexErrMsgTxt("Required field 'NumIntSteps' was not found in the element data structure"); |
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462 | |
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463 | tmpmxptr = mxGetField(prhs[0],0,"Length"); |
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464 | if(tmpmxptr) |
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465 | le = mxGetScalar(tmpmxptr); |
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466 | else |
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467 | mexErrMsgTxt("Required field 'Length' was not found in the element data structure"); |
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468 | |
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469 | /* Kicks from multipole elements can be specified as angles. This handles the |
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470 | case where corrector coils are used in sextupoles and used for orbit |
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471 | correction. */ |
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472 | tmpmxptr = mxGetField(prhs[0],0,"KickAngle"); |
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473 | if(tmpmxptr) |
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474 | ka = mxGetPr(tmpmxptr); |
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475 | else |
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476 | ka = NULL; |
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477 | |
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478 | tmpmxptr = mxGetField(prhs[0],0,"Energy"); |
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479 | if(tmpmxptr) |
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480 | E0 = mxGetScalar(tmpmxptr); |
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481 | else |
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482 | mexErrMsgTxt("Required field 'Energy' was not found in the element data structure"); |
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483 | |
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484 | tmpmxptr=mxGetField(prhs[0],0,"R1"); |
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485 | if(tmpmxptr) |
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486 | pr1 = mxGetPr(tmpmxptr); |
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487 | else |
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488 | pr1 = NULL; |
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489 | |
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490 | |
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491 | tmpmxptr=mxGetField(prhs[0],0,"R2"); |
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492 | if(tmpmxptr) |
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493 | pr2 = mxGetPr(tmpmxptr); |
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494 | else |
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495 | pr2 = NULL; |
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496 | |
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497 | tmpmxptr=mxGetField(prhs[0],0,"T1"); |
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498 | if(tmpmxptr) |
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499 | pt1 = mxGetPr(tmpmxptr); |
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500 | else |
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501 | pt1 = NULL; |
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502 | |
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503 | tmpmxptr=mxGetField(prhs[0],0,"T2"); |
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504 | if(tmpmxptr) |
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505 | pt2 = mxGetPr(tmpmxptr); |
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506 | else |
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507 | pt2 = NULL; |
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508 | |
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509 | |
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510 | if(ka!=NULL) |
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511 | { |
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512 | /* Positive angle must correspond to -ve B field since +ve B field corresponds |
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513 | to a bend with the same curvature as the bend magnets. |
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514 | */ |
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515 | B[0] -= sin(ka[0])/le; |
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516 | A[0] += sin(ka[1])/le; |
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517 | } |
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518 | |
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519 | plhs[0] = mxDuplicateArray(prhs[1]); |
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520 | r_in = mxGetPr(plhs[0]); |
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521 | |
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522 | StrMPoleSymplectic4RadPass(r_in, le, A, B, max_order, num_int_steps, |
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523 | pt1, pt2, pr1, pr2, E0, n); |
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524 | |
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525 | if(ka!=NULL) |
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526 | { |
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527 | B[0] -= sin(ka[0])/le; |
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528 | A[0] -= sin(ka[1])/le; |
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529 | } |
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530 | |
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531 | |
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532 | } |
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533 | else |
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534 | { /* return list of required fields */ |
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535 | plhs[0] = mxCreateCellMatrix(6,1); |
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536 | mxSetCell(plhs[0],0,mxCreateString("Length")); |
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537 | mxSetCell(plhs[0],1,mxCreateString("PolynomA")); |
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538 | mxSetCell(plhs[0],2,mxCreateString("PolynomB")); |
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539 | mxSetCell(plhs[0],3,mxCreateString("MaxOrder")); |
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540 | mxSetCell(plhs[0],4,mxCreateString("NumIntSteps")); |
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541 | mxSetCell(plhs[0],5,mxCreateString("Energy")); |
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542 | |
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543 | if(nlhs>1) /* Required and optional fields */ |
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544 | { plhs[1] = mxCreateCellMatrix(4,1); |
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545 | mxSetCell(plhs[1],0,mxCreateString("T1")); |
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546 | mxSetCell(plhs[1],1,mxCreateString("T2")); |
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547 | mxSetCell(plhs[1],2,mxCreateString("R1")); |
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548 | mxSetCell(plhs[1],3,mxCreateString("R2")); |
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549 | mxSetCell(plhs[1],4,mxCreateString("KickAngle")); |
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550 | } |
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551 | } |
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552 | |
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553 | |
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554 | |
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555 | } |
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556 | |
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557 | |
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558 | |
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