| 1 | #include <stdio.h>
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| 2 | #include <math.h>
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| 3 | #include "diag.h"
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| 4 | #include "init.h"
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| 5 | #include "lagrange.h"
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| 6 | /* ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ */
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| 7 |
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| 8 | /* random numbers */
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| 9 | #define RandomNumber ranf()
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| 10 |
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| 11 | /* Speed of Light in vacuum, in m/s */
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| 12 | #define Speed_of_Light_vacuum 299792458.0f
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| 13 | #define Speed_of_Light_air (Speed_of_Light_vacuum / 1.000293f)
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| 14 |
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| 15 | /* Speed of Light in vacuum, in cm/ns */
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| 16 | #define Speed_of_Light_vacuum_cmns (Speed_of_Light_vacuum / 1.0e7f)
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| 17 | #define Speed_of_Light_air_cmns (Speed_of_Light_air / 1.0e7f)
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| 18 |
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| 19 | /* Macros */
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| 20 | #define SQR(A) ((A)*(A))
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| 21 | #define NORM(A) ((float) sqrt((SQR(A[0]))+(SQR(A[1]))+(SQR(A[2]))))
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| 22 |
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| 23 | /* Function declarations */
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| 24 | extern float ranf(void);
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| 25 | void rnormal(double *r, int n);
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| 26 |
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| 27 | /* Static definitions */
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| 28 | float OmegaCT[3][3];
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| 29 | float OmegaICT[3][3];
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| 30 | float Omega[3][3];
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| 31 | float OmegaI[3][3];
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| 32 |
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| 33 | static double NormalRandomNumbers[500];
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| 34 | /*
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| 35 | From photons on ground, i.e. observation level,
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| 36 | to photons on focal plane, i.e. chamber !
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| 37 |
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| 38 | Mirror reflectivity
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| 39 | Mirror reflection
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| 40 | Photon position on chamber
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| 41 | Position smearing
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| 42 | Timing
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| 43 |
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| 44 | Returned values:
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| 45 |
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| 46 | 0 OK photon reached the chamber
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| 47 |
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| 48 | 1 Photon lost due to mirror reflectivity
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| 49 | 2 Photon lost because out of mirror
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| 50 | 3 Photon lost due to black spot
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| 51 | 4 Photon lost because reflected out of chamber
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| 52 |
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| 53 | */
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| 54 |
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| 55 | int ph2cph(photon *ph, cphoton *cph)
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| 56 | {
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| 57 |
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| 58 | float u, v, w; /* photon director cosines */
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| 59 |
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| 60 | float r[3]; /* photon trajectory */
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| 61 | float x[3]; /* position of the photon on ground */
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| 62 |
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| 63 | float rCT[3]; /* photon trajectory in the system of the CT */
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| 64 | float xCT[3]; /* photon position on ground (CT) */
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| 65 | float rm[3]; /* photon trajectory in the system of a mirror */
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| 66 | float xmm[3]; /* intermediate values */
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| 67 | float xm[3]; /* photon position on ground */
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| 68 | float xcut[3]; /* location of the cut sphere-trajectory */
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| 69 | float xcutCT[3]; /* location of the cut sphere-trajectory (CT) */
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| 70 |
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| 71 | float rnor[3], rnorm; /* normal in that point */
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| 72 |
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| 73 | float rrefl[3]; /* reflected vector, from the mirror */
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| 74 | float rreflCT[3]; /* reflected vector, from the CT */
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| 75 | float xcam[3]; /* where the photon hits the camera plane */
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| 76 |
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| 77 | float calpha; /* cos(alpha=angle incident/normal) */
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| 78 | float phi; /* angle between photon and camera plane */
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| 79 |
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| 80 | float a, b, c, t; /* intermediate variables */
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| 81 |
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| 82 | float d; /* minimum distance trajectory-mirror center */
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| 83 |
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| 84 | float wl; /* photon wavelength */
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| 85 | float reflec; /* reflectivity for a photon */
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| 86 |
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| 87 | float h; /* photon production height */
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| 88 |
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| 89 | int i, k; /* simple counters */
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| 90 | int i_mirror=-1; /* number of a given mirror */
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| 91 |
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| 92 |
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| 93 | float distmirr, distmirr2; /* distances used in MAGIC reflection routine */
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| 94 | float sx, sy;
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| 95 | float t1, t2;
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| 96 |
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| 97 | void makeOmega(float theta, float phi);
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| 98 | void makeOmegaI(float theta, float phi);
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| 99 | void applyMxV(float M[3][3], float *V, float *Vp);
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| 100 | float Lin2Curv(float x);
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| 101 |
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| 102 | /* begin code */
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| 103 |
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| 104 | /* get photon wawelength */
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| 105 |
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| 106 | wl = ph->w;
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| 107 |
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| 108 | /* get position on ground */
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| 109 |
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| 110 | x[0] = ph->x;
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| 111 | x[1] = ph->y;
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| 112 | x[2] = 0.0; /* ground => obs. level => z=0 */
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| 113 |
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| 114 | /* get director cosines x,y on ground */
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| 115 |
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| 116 | r[0] = ph->u;
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| 117 | r[1] = ph->v;
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| 118 | r[2] = (float) sqrt(1.0 - r[0]*r[0] - r[1]*r[1]);
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| 119 |
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| 120 | /* get photon time and production height */
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| 121 |
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| 122 | h = ph->h;
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| 123 |
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| 124 | /*!@'
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| 125 |
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| 126 | @#### Reflectivity of the mirrors.
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| 127 |
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| 128 | We make a 3rd. order interpolation using Lagrange
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| 129 | polynomials, in order to calculate the reflectivity of the
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| 130 | mirror for that wavelength. Further developments will
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| 131 | include also a incidence-angle dependence (which is not very
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| 132 | important).
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| 133 |
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| 134 | */
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| 135 |
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| 136 | /* ++
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| 137 | FILTER: REFLECTIVITY R(lambda)
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| 138 | -- */
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| 139 |
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| 140 | /* find data point to be used in Lagrange interpolation (-> k) */
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| 141 |
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| 142 | FindLagrange(Reflectivity,k,wl);
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| 143 |
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| 144 | /* if random > reflectivity then goes to the TOP of the loop again */
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| 145 |
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| 146 | reflec = Lagrange(Reflectivity,k,wl);
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| 147 |
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| 148 | if ( RandomNumber > reflec ) return 1;
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| 149 |
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| 150 |
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| 151 | /*!@'
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| 152 |
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| 153 | @#### Reflection on mirrors.
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| 154 | We calculate reflected photon direction
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| 155 |
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| 156 | */
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| 157 |
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| 158 | /* ++
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| 159 | REFLECTION
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| 160 | -- */
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| 161 |
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| 162 | Debug("@1 %f %f %f %f %f %f\n", x[0], x[1], x[2], r[0], r[1], r[2]);
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| 163 |
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| 164 | /* change to the system of the CT */
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| 165 |
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| 166 | applyMxV( OmegaCT, x, xCT );
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| 167 | applyMxV( OmegaCT, r, rCT );
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| 168 |
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| 169 | /*
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| 170 | before moving to the system of the mirror
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| 171 | we look whether the photon hits a mirror or not
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| 172 |
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| 173 | calculate the intersection of the trajectory of the photon
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| 174 | with the GLOBAL DISH !!!
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| 175 | we reproduce the calculation of the coefficients of the
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| 176 | second order polynomial in z (=xCT[2]), made with
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| 177 | Mathematica
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| 178 | */
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| 179 |
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| 180 | /*
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| 181 | * In[1]:= parab:=z-(x^2+y^2)/(4F)
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| 182 | * par1=parab /. {x->x0+u/w(z-z0),y->y0+v/w(z-z0)}
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| 183 | *
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| 184 | * Out[1]=
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| 185 | * u (z - z0) 2 v (z - z0) 2
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| 186 | * (x0 + ----------) + (y0 + ----------)
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| 187 | * w w
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| 188 | * z - ---------------------------------------
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| 189 | * 4 F
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| 190 | *
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| 191 | * In[2]:= CoefficientList[ExpandAll[par1*4F*w^2],z]
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| 192 | *
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| 193 | * Out[2]=
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| 194 | * 2 2 2 2
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| 195 | * {-(w x0 ) - w y0 + 2 u w x0 z0 +
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| 196 | *
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| 197 | * 2 2 2 2
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| 198 | * 2 v w y0 z0 - u z0 - v z0 ,
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| 199 | *
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| 200 | * 2 2
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| 201 | * 4 F w - 2 u w x0 - 2 v w y0 + 2 u z0 +
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| 202 | *
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| 203 | * 2 2 2
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| 204 | * 2 v z0, -u - v }
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| 205 | */
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| 206 |
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| 207 | /* the z coordinate is calculated */
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| 208 |
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| 209 | a = - SQR(rCT[0]) - SQR(rCT[1]);
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| 210 |
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| 211 | b = (float) (4.0*ct_Focal_mean*SQR(rCT[2])
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| 212 | - 2.0*rCT[0]*rCT[2]*xCT[0] - 2.0*rCT[1]*rCT[2]*xCT[1]
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| 213 | + 2.0*SQR(rCT[0])*xCT[2] + 2.0*SQR(rCT[1])*xCT[2]);
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| 214 |
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| 215 | c = 2*rCT[0]*rCT[2]*x[0]*x[2] + 2*rCT[1]*rCT[2]*x[1]*x[2]
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| 216 | - SQR(rCT[2])*SQR(x[0]) - SQR(rCT[2])*SQR(x[1])
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| 217 | - SQR(rCT[0])*SQR(x[2]) - SQR(rCT[1])*SQR(x[2]);
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| 218 |
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| 219 | if ( fabs(a) < 1.e-6 ) {
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| 220 |
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| 221 | /* only one value */
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| 222 |
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| 223 | xcut[2] = -c / b;
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| 224 |
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| 225 | } else {
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| 226 |
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| 227 | d = (float) sqrt( b*b - 4.0*a*c );
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| 228 |
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| 229 | /* two possible values for z */
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| 230 |
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| 231 | t1 = (float) ((-b+d) / (2.0*a));
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| 232 | t2 = (float) ((-b-d) / (2.0*a));
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| 233 |
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| 234 | /* z must be the minimum of t1 and t2 */
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| 235 |
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| 236 | xcut[2] = (t1 < t2) ? t1 : t2;
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| 237 |
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| 238 | }
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| 239 |
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| 240 | /*
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| 241 | xcut[] is NOW the cut between the GLOBAL dish of MAGIC and
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| 242 | the trajectory of the photon
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| 243 | */
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| 244 |
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| 245 | xcut[0] = xCT[0] + rCT[0]/rCT[2]*(xcut[2]-xCT[2]);
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| 246 | xcut[1] = xCT[1] + rCT[1]/rCT[2]*(xcut[2]-xCT[2]);
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| 247 |
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| 248 | /* convert to Curvilinear distance over the parabolic dish */
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| 249 |
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| 250 | sx = Lin2Curv( xcut[0] );
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| 251 | sy = Lin2Curv( xcut[1] );
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| 252 |
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| 253 | /* is it outside the dish? */
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| 254 |
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| 255 | if ((fabs(sx) > 850.0) || (fabs(sy) > 850.0)) {
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| 256 | /*
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| 257 | cout << "CONDITION 1 !" << endl << flush;
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| 258 | cout << '1';
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| 259 | */
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| 260 | return 2;
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| 261 | }
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| 262 |
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| 263 | /* calculate the mirror to be used */
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| 264 |
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| 265 | distmirr = 1000000.0f;
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| 266 |
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| 267 | for (i=0; i<ct_NMirrors && distmirr>=ct_RMirror; ++i) {
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| 268 | distmirr2 = (float) sqrt(SQR(ct_data[i].x - xcut[0]) +
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| 269 | SQR(ct_data[i].y - xcut[1]) +
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| 270 | SQR(ct_data[i].z - xcut[2]));
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| 271 | if (distmirr2 < distmirr) {
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| 272 | i_mirror = i;
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| 273 | distmirr = distmirr2;
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| 274 | }
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| 275 | }
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| 276 |
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| 277 | /*
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| 278 | the mirror to use is i_mirror (calculated several lines above)
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| 279 | check whether the photon is outside the nearest (this) mirror
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| 280 | */
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| 281 |
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| 282 | if ((fabs(ct_data[i_mirror].sx - sx) > ct_RMirror) ||
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| 283 | (fabs(ct_data[i_mirror].sy - sy) > ct_RMirror)) {
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| 284 | /*
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| 285 | cout << "CONDITION 2 !" << endl << flush;
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| 286 | cout << '2';
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| 287 | */
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| 288 | return 2;
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| 289 | }
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| 290 |
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| 291 | /* calculate matrices for the mirror */
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| 292 |
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| 293 | makeOmega (-ct_data[i_mirror].theta,
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| 294 | ct_data[i_mirror].phi);
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| 295 | makeOmegaI(-ct_data[i_mirror].theta,
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| 296 | ct_data[i_mirror].phi);
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| 297 |
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| 298 | /* change to the system of the mirror */
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| 299 |
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| 300 | /* first translation... */
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| 301 |
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| 302 | xmm[0] = xCT[0] - ct_data[i_mirror].x;
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| 303 | xmm[1] = xCT[1] - ct_data[i_mirror].y;
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| 304 | xmm[2] = xCT[2] - ct_data[i_mirror].z;
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| 305 |
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| 306 | /* ...then rotation */
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| 307 |
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| 308 | applyMxV( Omega, xmm, xm );
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| 309 | applyMxV( Omega, rCT, rm );
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| 310 |
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| 311 | /*
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| 312 | the vector rCT should be normalized, and
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| 313 | so the vector rm remains normalized as well, but, anyhow...
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| 314 | */
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| 315 |
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| 316 | rnorm = NORM( rm );
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| 317 | rm[0] /= rnorm;
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| 318 | rm[1] /= rnorm;
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| 319 | rm[2] /= rnorm;
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| 320 |
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| 321 | /*
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| 322 | calculate the intersection of the trajectory of the photon
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| 323 | with the mirror
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| 324 | we reproduce the calculation of the coefficients of the
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| 325 | second order polynomial in z (=xm[2]), made with
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| 326 | Mathematica
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| 327 | */
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| 328 |
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| 329 | /*
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| 330 | * In[1]:= esfera:=x^2+y^2+(z-R)^2-R^2;
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| 331 | * recta:={x->x0+u/w(z-z0),y->y0+v/w(z-z0)}
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| 332 | *
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| 333 | * In[2]:= esfera
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| 334 | *
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| 335 | * 2 2 2 2
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| 336 | * Out[2]= -R + x + y + (-R + z)
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| 337 | *
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| 338 | * In[3]:= recta
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| 339 | *
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| 340 | * u (z - z0) v (z - z0)
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| 341 | * Out[3]= {x -> x0 + ----------, y -> y0 + ----------}
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| 342 | * w w
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| 343 | *
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| 344 | * In[4]:= esf=esfera /. recta
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| 345 | *
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| 346 | * 2 2 u (z - z0) 2 v (z - z0) 2
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| 347 | * Out[4]= -R + (-R + z) + (x0 + ----------) + (y0 + ----------)
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| 348 | * w w
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| 349 | *
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| 350 | * In[5]:= coefs=CoefficientList[ExpandAll[esf],z]
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| 351 | *
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| 352 | * 2 2 2 2
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| 353 | * 2 2 2 u x0 z0 2 v y0 z0 u z0 v z0
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| 354 | * Out[5]= {x0 + y0 - --------- - --------- + ------ + ------,
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| 355 | * w w 2 2
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| 356 | * w w
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| 357 | *
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| 358 | * 2 2 2 2
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| 359 | * 2 u x0 2 v y0 2 u z0 2 v z0 u v
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| 360 | * > -2 R + ------ + ------ - ------- - -------, 1 + -- + --}
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| 361 | * w w 2 2 2 2
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| 362 | * w w w w
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| 363 | * In[6]:= Simplify[ExpandAll[coefs*w^2]]
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| 364 | *
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| 365 | * 2 2 2 2 2 2
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| 366 | * Out[6]= {w (x0 + y0 ) - 2 w (u x0 + v y0) z0 + (u + v ) z0 ,
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| 367 | *
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| 368 | * 2 2 2 2 2
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| 369 | * > -2 (R w - u w x0 + u z0 + v (-(w y0) + v z0)), u + v + w }
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| 370 | *
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| 371 | */
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| 372 |
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| 373 | /*
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| 374 | the z coordinate is calculated, using the coefficient
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| 375 | shown above
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| 376 | */
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| 377 |
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| 378 | a = SQR(rm[0]) + SQR(rm[1]) + SQR(rm[2]);
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| 379 |
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| 380 | b = (float) (-2*(2.*ct_data[i_mirror].f*SQR(rm[2])
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| 381 | - rm[0]*rm[2]*xm[0]
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| 382 | + SQR(rm[0])*xm[2]
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| 383 | + rm[1]*(-(rm[2]*xm[1]) + rm[1]*xm[2])));
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| 384 |
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| 385 | c = (SQR(rm[2])*(SQR(xm[0]) + SQR(xm[1]))
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| 386 | - 2*rm[2]*(rm[0]*xm[0] + rm[1]*xm[1])*xm[2]
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| 387 | + (SQR(rm[0]) + SQR(rm[1]))*SQR(xm[2]));
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| 388 |
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| 389 | d = (float) sqrt( b*b - 4.0*a*c );
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| 390 |
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| 391 | /* two possible values for z */
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| 392 |
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| 393 | t1 = (float) ((-b+d) / (2.0*a));
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| 394 | t2 = (float) ((-b-d) / (2.0*a));
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| 395 |
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| 396 | /* z must be the minimum of t1 and t2 */
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| 397 |
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| 398 | xcut[2] = (t1 < t2) ? t1 : t2;
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| 399 | xcut[0] = xm[0] + rm[0]/rm[2]*(xcut[2]-xm[2]);
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| 400 | xcut[1] = xm[1] + rm[1]/rm[2]*(xcut[2]-xm[2]);
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| 401 |
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| 402 | /*
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| 403 | ++
|
|---|
| 404 | BLACK SPOTS: If the photon hits the black spot, it's lost
|
|---|
| 405 | --
|
|---|
| 406 | */
|
|---|
| 407 |
|
|---|
| 408 | if ( sqrt(SQR(xcut[0]) + SQR(xcut[1])) < ct_BlackSpot_rad ) {
|
|---|
| 409 | /*
|
|---|
| 410 | cout << "CONDITION 3!\n" << flush;
|
|---|
| 411 | cout << '3';
|
|---|
| 412 | */
|
|---|
| 413 | return 3;
|
|---|
| 414 | }
|
|---|
| 415 |
|
|---|
| 416 | /*
|
|---|
| 417 | if we still have the photon, we continue with the reflexion;
|
|---|
| 418 | we calculate normal vector in this point
|
|---|
| 419 | (and normalize, with the sign changed)
|
|---|
| 420 | */
|
|---|
| 421 |
|
|---|
| 422 | rnor[0] = 2.0f*xcut[0];
|
|---|
| 423 | rnor[1] = 2.0f*xcut[1];
|
|---|
| 424 | rnor[2] = (float) (2.0*(xcut[2] - 2.0*ct_Focal[i_mirror]));
|
|---|
| 425 |
|
|---|
| 426 | rnorm = -NORM( rnor );
|
|---|
| 427 | rnor[0] /= rnorm;
|
|---|
| 428 | rnor[1] /= rnorm;
|
|---|
| 429 | rnor[2] /= rnorm;
|
|---|
| 430 |
|
|---|
| 431 | /*
|
|---|
| 432 | now, both "normal" vector and original trajectory are
|
|---|
| 433 | normalized
|
|---|
| 434 | just project the original vector in the normal, and
|
|---|
| 435 | take it as the "mean" position of the original and
|
|---|
| 436 | the "reflected" vector
|
|---|
| 437 | from this, we can calculate the "reflected" vector
|
|---|
| 438 | calpha = cos(angle(rnor,rm))
|
|---|
| 439 | */
|
|---|
| 440 |
|
|---|
| 441 | calpha = (float) fabs(rnor[0]*rm[0] + rnor[1]*rm[1] + rnor[2]*rm[2]);
|
|---|
| 442 |
|
|---|
| 443 | /* finally!!! we have the reflected trajectory of the photon */
|
|---|
| 444 |
|
|---|
| 445 | rrefl[0] = (float) (2.0*rnor[0]*calpha - rm[0]);
|
|---|
| 446 | rrefl[1] = (float) (2.0*rnor[1]*calpha - rm[1]);
|
|---|
| 447 | rrefl[2] = (float) (2.0*rnor[2]*calpha - rm[2]);
|
|---|
| 448 |
|
|---|
| 449 | rnorm = NORM( rrefl );
|
|---|
| 450 | rrefl[0] /= rnorm;
|
|---|
| 451 | rrefl[1] /= rnorm;
|
|---|
| 452 | rrefl[2] /= rnorm;
|
|---|
| 453 |
|
|---|
| 454 | /* let's go back to the coordinate system of the CT */
|
|---|
| 455 |
|
|---|
| 456 | /* first rotation... */
|
|---|
| 457 |
|
|---|
| 458 | applyMxV( OmegaI, xcut, xcutCT);
|
|---|
| 459 | applyMxV( OmegaI, rrefl, rreflCT);
|
|---|
| 460 |
|
|---|
| 461 | /* ...then translation */
|
|---|
| 462 |
|
|---|
| 463 | xcutCT[0] += ct_data[i_mirror].x;
|
|---|
| 464 | xcutCT[1] += ct_data[i_mirror].y;
|
|---|
| 465 | xcutCT[2] += ct_data[i_mirror].z;
|
|---|
| 466 |
|
|---|
| 467 | /*
|
|---|
| 468 | calculate intersection of this trajectory and the camera plane
|
|---|
| 469 | in the system of the CT, this plane is z = ct_Focal
|
|---|
| 470 | */
|
|---|
| 471 |
|
|---|
| 472 | t = (ct_Focal_mean - xcutCT[2]) / rreflCT[2];
|
|---|
| 473 |
|
|---|
| 474 | xcam[0] = xcutCT[0] + rreflCT[0]*t;
|
|---|
| 475 | xcam[1] = xcutCT[1] + rreflCT[1]*t;
|
|---|
| 476 | xcam[2] = xcutCT[2] + rreflCT[2]*t;
|
|---|
| 477 |
|
|---|
| 478 | /*
|
|---|
| 479 | ++
|
|---|
| 480 | AXIS DEVIATION: We introduce it here just as a first order
|
|---|
| 481 | correction, by modifying the position of the reflected photon.
|
|---|
| 482 | --
|
|---|
| 483 | */
|
|---|
| 484 |
|
|---|
| 485 | xcam[0] += AxisDeviation[0][i_mirror];
|
|---|
| 486 | xcam[1] += AxisDeviation[1][i_mirror];
|
|---|
| 487 |
|
|---|
| 488 | /*
|
|---|
| 489 | ++
|
|---|
| 490 | SMEARING: We apply the point spread function for the mirrors
|
|---|
| 491 | --
|
|---|
| 492 | */
|
|---|
| 493 |
|
|---|
| 494 | /* get two N(0;1) random numbers */
|
|---|
| 495 |
|
|---|
| 496 | rnormal( NormalRandomNumbers, 2 );
|
|---|
| 497 |
|
|---|
| 498 | /* modify the Cphoton position in the camera */
|
|---|
| 499 |
|
|---|
| 500 | xcam[0] += (float) (NormalRandomNumbers[0] * ct_PSpread_mean);
|
|---|
| 501 | xcam[1] += (float) (NormalRandomNumbers[1] * ct_PSpread_mean);
|
|---|
| 502 |
|
|---|
| 503 | /* check whether the photon goes out of the camera */
|
|---|
| 504 |
|
|---|
| 505 | if ( (SQR(xcam[0])+SQR(xcam[1])) > SQR(ct_CameraWidth) ) {
|
|---|
| 506 | return 4;
|
|---|
| 507 | }
|
|---|
| 508 |
|
|---|
| 509 | /*
|
|---|
| 510 | ++
|
|---|
| 511 | ANGLE OF INCIDENCE
|
|---|
| 512 | --
|
|---|
| 513 |
|
|---|
| 514 | calculate angle of incidence between tray. and camera plane
|
|---|
| 515 | the camera plane is
|
|---|
| 516 | 0 y + 0 y + z - ct_Focal = 0 => (A,B,C,D) = (0,0,1,-ct_Focal)
|
|---|
| 517 | from Table 3.20 "Tasch. der Math."
|
|---|
| 518 | */
|
|---|
| 519 |
|
|---|
| 520 | phi = (float) asin(rreflCT[2]);
|
|---|
| 521 |
|
|---|
| 522 | /*
|
|---|
| 523 | ++
|
|---|
| 524 | TIMING
|
|---|
| 525 | --
|
|---|
| 526 | */
|
|---|
| 527 |
|
|---|
| 528 | /* calculate the new time of the photon (in the camera) */
|
|---|
| 529 |
|
|---|
| 530 | t = ph->t;
|
|---|
| 531 |
|
|---|
| 532 | /*
|
|---|
| 533 | substract path from the mirror till the ground, 'cos
|
|---|
| 534 | the photon actually hit the mirror!!
|
|---|
| 535 | */
|
|---|
| 536 |
|
|---|
| 537 | t = (float) (t + ((( xm[2] > 0. ) ? -1.0 : +1.0) *
|
|---|
| 538 | sqrt( SQR(xm[0] - xcut[0]) +
|
|---|
| 539 | SQR(xm[1] - xcut[1]) +
|
|---|
| 540 | SQR(xm[2] - xcut[2]) ) / Speed_of_Light_air_cmns));
|
|---|
| 541 |
|
|---|
| 542 | /* add path from the mirror till the camera */
|
|---|
| 543 |
|
|---|
| 544 | t = (float) (t + sqrt( SQR(xcutCT[0] - xcam[0]) +
|
|---|
| 545 | SQR(xcutCT[1] - xcam[1]) +
|
|---|
| 546 | SQR(xcutCT[2] - xcam[2]) ) / Speed_of_Light_air_cmns);
|
|---|
| 547 |
|
|---|
| 548 | /* show it */
|
|---|
| 549 |
|
|---|
| 550 | Debug("@2 %f %f %f %f %f %f %f %f %f\n"
|
|---|
| 551 | "@3 %f %f %d %f %f %f %f\n"
|
|---|
| 552 | "@4 %f %f %f %f\n",
|
|---|
| 553 | xCT[0], xCT[1], xCT[2], rCT[0], rCT[1], rCT[2],
|
|---|
| 554 | xcut[0], xcut[1], xcut[2],
|
|---|
| 555 | sx, sy, i_mirror, ct_data[i_mirror].sx, ct_data[i_mirror].sy,
|
|---|
| 556 | ct_data[i_mirror].sx - sx, ct_data[i_mirror].sy - sy,
|
|---|
| 557 | xcam[0], xcam[1], xcam[2], phi);
|
|---|
| 558 |
|
|---|
| 559 | /* Output */
|
|---|
| 560 |
|
|---|
| 561 | /* cph->w = wl; */
|
|---|
| 562 | cph->x = xcam[0];
|
|---|
| 563 | cph->y = xcam[1];
|
|---|
| 564 | cph->u = r[0];
|
|---|
| 565 | cph->v = r[1];
|
|---|
| 566 | cph->t = t;
|
|---|
| 567 | cph->h = h;
|
|---|
| 568 | cph->phi = phi;
|
|---|
| 569 |
|
|---|
| 570 | return 0;
|
|---|
| 571 |
|
|---|
| 572 | } /* end of ph2cph */
|
|---|
| 573 |
|
|---|
| 574 |
|
|---|
| 575 | /* ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
|
|---|
| 576 |
|
|---|
| 577 | !---------------------------------------------------------------------
|
|---|
| 578 | @name makeOmega
|
|---|
| 579 |
|
|---|
| 580 | @desc function to calculate the matrix Omega(theta,phi)
|
|---|
| 581 |
|
|---|
| 582 | @var theta Angle theta of the transformation
|
|---|
| 583 | @var phi Angle phi of the transformation
|
|---|
| 584 |
|
|---|
| 585 | @date Sat Jun 27 05:58:56 MET DST 1998
|
|---|
| 586 | ----------------------------------------------------------------------
|
|---|
| 587 | @function
|
|---|
| 588 | */
|
|---|
| 589 |
|
|---|
| 590 | void
|
|---|
| 591 | makeOmega (float theta, float phi)
|
|---|
| 592 | {
|
|---|
| 593 | static float ct, st, cp, sp;
|
|---|
| 594 |
|
|---|
| 595 | /* shortcuts for cosine and sine of theta and phi */
|
|---|
| 596 | ct = (float) cos(theta);
|
|---|
| 597 | st = (float) sin(theta);
|
|---|
| 598 | cp = (float) cos(phi);
|
|---|
| 599 | sp = (float) sin(phi);
|
|---|
| 600 |
|
|---|
| 601 | /* save values in the array (see top of file) */
|
|---|
| 602 | Omega[0][0] = cp*ct;
|
|---|
| 603 | Omega[0][1] = sp*ct;
|
|---|
| 604 | Omega[0][2] = -st;
|
|---|
| 605 |
|
|---|
| 606 | Omega[1][0] = -sp;
|
|---|
| 607 | Omega[1][1] = cp;
|
|---|
| 608 | Omega[1][2] = 0;
|
|---|
| 609 |
|
|---|
| 610 | Omega[2][0] = cp*st;
|
|---|
| 611 | Omega[2][1] = sp*st;
|
|---|
| 612 | Omega[2][2] = ct;
|
|---|
| 613 | }
|
|---|
| 614 |
|
|---|
| 615 |
|
|---|
| 616 | /*
|
|---|
| 617 | !---------------------------------------------------------------------
|
|---|
| 618 | @name makeOmegaI
|
|---|
| 619 |
|
|---|
| 620 | @desc function to calculate the matrix Omega-1(theta,phi)
|
|---|
| 621 |
|
|---|
| 622 | @var theta Angle theta of the transformation
|
|---|
| 623 | @var phi Angle phi of the transformation
|
|---|
| 624 |
|
|---|
| 625 | @date Sat Jun 27 05:58:56 MET DST 1998
|
|---|
| 626 | ----------------------------------------------------------------------
|
|---|
| 627 | @function
|
|---|
| 628 | */
|
|---|
| 629 |
|
|---|
| 630 | void
|
|---|
| 631 | makeOmegaI(float theta, float phi)
|
|---|
| 632 | {
|
|---|
| 633 | static float ct, st, cp, sp;
|
|---|
| 634 |
|
|---|
| 635 | /* shortcuts for cosine and sine of theta and phi */
|
|---|
| 636 | ct = (float) cos(theta);
|
|---|
| 637 | st = (float) sin(theta);
|
|---|
| 638 | cp = (float) cos(phi);
|
|---|
| 639 | sp = (float) sin(phi);
|
|---|
| 640 |
|
|---|
| 641 | /* save values in the array (see top of file) */
|
|---|
| 642 | OmegaI[0][0] = cp*ct;
|
|---|
| 643 | OmegaI[0][1] = -sp;
|
|---|
| 644 | OmegaI[0][2] = cp*st;
|
|---|
| 645 |
|
|---|
| 646 | OmegaI[1][0] = sp*ct;
|
|---|
| 647 | OmegaI[1][1] = cp;
|
|---|
| 648 | OmegaI[1][2] = sp*st;
|
|---|
| 649 |
|
|---|
| 650 | OmegaI[2][0] = -st;
|
|---|
| 651 | OmegaI[2][1] = 0;
|
|---|
| 652 | OmegaI[2][2] = ct;
|
|---|
| 653 | }
|
|---|
| 654 |
|
|---|
| 655 |
|
|---|
| 656 | /*
|
|---|
| 657 | !---------------------------------------------------------------------
|
|---|
| 658 | @name applyMxv
|
|---|
| 659 |
|
|---|
| 660 | @desc returns the vector v' such that v' = M x v
|
|---|
| 661 |
|
|---|
| 662 | @var M matrix of the transformation
|
|---|
| 663 | @var v vector to be multiplied
|
|---|
| 664 | @var vi resulting vector
|
|---|
| 665 |
|
|---|
| 666 | @date Sat Jun 27 05:58:56 MET DST 1998
|
|---|
| 667 | ----------------------------------------------------------------------
|
|---|
| 668 | @function
|
|---|
| 669 | */
|
|---|
| 670 |
|
|---|
| 671 | void
|
|---|
| 672 | applyMxV(float M[3][3], float *V, float *Vp)
|
|---|
| 673 | {
|
|---|
| 674 | Vp[0] = (M[0][0] * V[0] +
|
|---|
| 675 | M[0][1] * V[1] +
|
|---|
| 676 | M[0][2] * V[2]);
|
|---|
| 677 | Vp[1] = (M[1][0] * V[0] +
|
|---|
| 678 | M[1][1] * V[1] +
|
|---|
| 679 | M[1][2] * V[2]);
|
|---|
| 680 | Vp[2] = (M[2][0] * V[0] +
|
|---|
| 681 | M[2][1] * V[1] +
|
|---|
| 682 | M[2][2] * V[2]);
|
|---|
| 683 | }
|
|---|
| 684 |
|
|---|
| 685 | /*
|
|---|
| 686 | !---------------------------------------------------------------------
|
|---|
| 687 | @name Lin2Curv
|
|---|
| 688 |
|
|---|
| 689 | @desc Linear (Euclidean) to Curvilinear distance
|
|---|
| 690 |
|
|---|
| 691 | @var x Radial distance from the axis of the paraboloid
|
|---|
| 692 |
|
|---|
| 693 | @return Curvilinear distance over the parabolic shape
|
|---|
| 694 |
|
|---|
| 695 | @date Wed Jul 8 15:25:39 MET DST 1998
|
|---|
| 696 | ----------------------------------------------------------------------
|
|---|
| 697 | @function
|
|---|
| 698 | */
|
|---|
| 699 |
|
|---|
| 700 | float
|
|---|
| 701 | Lin2Curv(float x)
|
|---|
| 702 | {
|
|---|
| 703 | x /= 100.f;
|
|---|
| 704 | return ((x + 0.000144175317185f * x * x * x)*100.f);
|
|---|
| 705 | }
|
|---|
| 706 |
|
|---|
| 707 | /*!---------------------------------------------------------------------
|
|---|
| 708 | // @name rnormal
|
|---|
| 709 | //
|
|---|
| 710 | // @desc returns n(=2k) normaly distributed numbers
|
|---|
| 711 | //
|
|---|
| 712 | // @var *r pointer to a vector where we write the numbers
|
|---|
| 713 | // @var n how many numbers do we generate
|
|---|
| 714 | //
|
|---|
| 715 | // @date Sat Jun 27 05:58:56 MET DST 1998
|
|---|
| 716 | //----------------------------------------------------------------------
|
|---|
| 717 | // @function */
|
|---|
| 718 |
|
|---|
| 719 | void rnormal(double *r, int n)
|
|---|
| 720 | {
|
|---|
| 721 |
|
|---|
| 722 | double z1, z2;
|
|---|
| 723 | int i;
|
|---|
| 724 |
|
|---|
| 725 | for (i=0; i<n; i+=2) {
|
|---|
| 726 |
|
|---|
| 727 | z1 = RandomNumber;
|
|---|
| 728 | z2 = RandomNumber;
|
|---|
| 729 |
|
|---|
| 730 | r[i] = sqrt(-2.0*log(z1)) * cos(2.0*M_PI*z2);
|
|---|
| 731 | r[i+1] = sqrt(-2.0*log(z1)) * sin(2.0*M_PI*z2);
|
|---|
| 732 |
|
|---|
| 733 | }
|
|---|
| 734 |
|
|---|
| 735 | }
|
|---|