source: branches/MarsISDCBranchBasedOn17887/msim/MSimAtmosphere.cc@ 19094

Last change on this file since 19094 was 9429, checked in by tbretz, 16 years ago
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1/* ======================================================================== *\
2!
3! *
4! * This file is part of CheObs, the Modular Analysis and Reconstruction
5! * Software. It is distributed to you in the hope that it can be a useful
6! * and timesaving tool in analysing Data of imaging Cerenkov telescopes.
7! * It is distributed WITHOUT ANY WARRANTY.
8! *
9! * Permission to use, copy, modify and distribute this software and its
10! * documentation for any purpose is hereby granted without fee,
11! * provided that the above copyright notice appears in all copies and
12! * that both that copyright notice and this permission notice appear
13! * in supporting documentation. It is provided "as is" without express
14! * or implied warranty.
15! *
16!
17!
18! Author(s): Thomas Bretz, 1/2009 <mailto:tbretz@astro.uni-wuerzburg.de>
19!
20! Copyright: CheObs Software Development, 2000-2009
21!
22!
23\* ======================================================================== */
24
25//////////////////////////////////////////////////////////////////////////////
26//
27// MSimAtmosphere
28//
29// Task to calculate wavelength or incident angle dependent absorption
30//
31// Input Containers:
32// MPhotonEvent
33// MCorsikaRunHeader
34//
35// Output Containers:
36// MPhotonEvent
37//
38//////////////////////////////////////////////////////////////////////////////
39#include "MSimAtmosphere.h"
40
41#include <fstream>
42
43#include <TGraph.h>
44#include <TRandom.h>
45
46#include "MLog.h"
47#include "MLogManip.h"
48
49#include "MParList.h"
50
51#include "MCorsikaRunHeader.h"
52#include "MPhotonEvent.h"
53#include "MPhotonData.h"
54
55ClassImp(MSimAtmosphere);
56
57using namespace std;
58
59// ==========================================================================
60//
61// January 2002, A. Moralejo: We now precalculate the slant paths for the
62// aerosol and Ozone vertical profiles, and then do an interpolation in
63// wavelength for every photon to get the optical depths. The parameters
64// used, defined below, have been taken from "Atmospheric Optics", by
65// L. Elterman and R.B. Toolin, chapter 7 of the "Handbook of geophysics
66// and Space environments". (S.L. Valley, editor). McGraw-Hill, NY 1965.
67//
68// WARNING: the Mie scattering and the Ozone absorption are implemented
69// to work only with photons produced at a height a.s.l larger than the
70// observation level. So this is not expected to work well for simulating
71// the telescope pointing at theta > 90 deg (for instance for neutrino
72// studies. Rayleigh scattering works even for light coming from below.
73//
74// Fixed bugs (of small influence) in Mie absorption implementation: there
75// were errors in the optical depths table, as well as a confusion:
76// height a.s.l. was used as if it was height above the telescope level.
77// The latter error was also present in the Ozone aborption implementation.
78//
79// On the other hand, now we have the tables AE_ABI and OZ_ABI with optical
80// depths between sea level and a height h (before it was between 2km a.s.l
81// and a height h). So that we can simulate also in the future a different
82// observation level.
83//
84// AM: WARNING: IF VERY LARGE zenith angle simulations are to be done (say
85// above 85 degrees, for neutrino primaries or any other purpose) this code
86// will have to be adapted accordingly and checked, since in principle it has
87// been written and tested to simulate the absorption of Cherenkov photons
88// arriving at the telescope from above.
89//
90// AM: WARNING 2: not to be used for wavelengths outside the range 250-700 nm
91//
92// January 2003, Abelardo Moralejo: found error in Ozone absorption treatment.
93// At large zenith angles, the air mass used was the one calculated for
94// Rayleigh scattering, but since the Ozone distribution is rather different
95// from the global distribution of air molecules, this is not a good
96// approximation. Now I have left in this code only the Rayleigh scattering,
97// and moved to atm.c the Mie scattering and Ozone absorption calculated in
98// a better way.
99//
100// A. Moralejo, January 2003: added some parameters for Mie scattering
101// and Ozone absorption derived from the clear standard atmosphere model
102// in "Atmospheric Optics", by L. Elterman and R.B. Toolin, chapter 7 of
103// the "Handbook of geophysics and Space environments". S.L. Valley,
104// editor. McGraw-Hill, NY 1965.
105//
106// AM, Jan 2003: Changed the meaning of the argument height: now it is the
107// true height above sea level at which a photon has been emitted, before
108// it was the height given by Corsika, measured in the vertical of the
109// observer and not in the vertical of the emitting particle.
110//
111//
112// MAGIC-Winter and MAGIC-Summer by M. Haffke,
113// parametrizing profiles obtained with MSIS:
114// http://uap-www.nrl.navy.mil/models_web/msis/msis_home.htm
115//
116//
117// The MAGIC-Winter and MAGIC-Summer parametrisations reproduce the MSIS
118// profiles for the 3 atmospheric layers from 0 up to 40 km height. Beyond
119// that height, it was not possible to achieve a good fit, but the amount
120// of residual atmosphere is so small that light absorption would be
121// negligible anyway. Showers develop well below 40 km.
122//
123//
124// The mass overburden is given by T = AATM + BATM * exp(-h/CATM)
125// The last layer of the US standard atmosphere (in which T varies
126// linearly with h) is above 100 km and has not been included here
127// because it should not matter.
128//
129class MAtmRayleigh
130{
131private:
132 static const Double_t fgMeanFreePath; // [g/cm^2] Mean free path for scattering Rayleigh XR
133
134 Double_t fR; // [cm] Earth radius to be used
135
136 Double_t fHeight[5]; // Layer boundaries (atmospheric layer)
137
138 // Parameters of the different atmospheres. We use the same parametrization
139 // shape as in Corsika atmospheric models (see Corsika manual, appendix D).
140 // The values here can be/are obtained from the Corsika output
141 //Float_t fAtmA[4]; // The index refers to the atmospheric layer (starting from sea level and going upwards)
142 Float_t fAtmB[4]; // The index refers to the atmospheric layer (starting from sea level and going upwards)
143 Float_t fAtmC[4]; // The index refers to the atmospheric layer (starting from sea level and going upwards)
144
145 Double_t fRho[5]; // Precalculated integrals for rayleigh scatterning
146
147 // --------------------------------------------------------------------------
148 //
149 // Precalcalculate the integrals from the observer level to the next
150 // atmpsheric layer below including the lower boundary. Thus a
151 // correct calculation is reduced to the calculation of the upper
152 // boundary.
153 //
154 // fRho[0] = B0;
155 // fRho[1] = B0-A0 + B1;
156 // fRho[2] = B0-A0 + B1-A1 + B2;
157 // fRho[3] = B0-A0 + B1-A1 + B2+A2 + B3;
158 // fRho[4] = B0-A0 + B1-A1 + B2+A2 + B3 - A3;
159 //
160 void PreCalcRho()
161 {
162 // Limits (height in cm) of the four layers in which
163 // atmosphere is parametrized.
164 // This is a stupid trick giving 0 for the integrals below
165 // the observer
166
167 // FIXME: Could be replaced by 0, AtmLay[0]-fAtmLay[3]
168
169 const Double_t h[5] =
170 {
171 fObsLevel, // fObsLevel, // 0km
172 TMath::Max(fObsLevel, 7.75e5), // TMath::Max(fObsLevel, 4e5), // 4km
173 16.5e5, // 10e5, // 10km
174 50.0e5, // 40e5, // 40km
175 105.0e5, // 100e5 // 100km
176 };
177
178 memcpy(fHeight, h, sizeof(Double_t)*5);
179
180 fRho[0] = 0;
181 for (int i=0; i<4; i++)
182 {
183 const Double_t b = fAtmB[i];
184 const Double_t c = fAtmC[i];
185
186 const Double_t h1 = h[i+1];
187 const Double_t h0 = h[i];
188
189 const Double_t B = b*TMath::Exp(-h0/c);
190 const Double_t A = b*TMath::Exp(-h1/c);
191
192 // Calculate rho for the i-th layer from the lower
193 // to the higher layer boundary.
194 // If height is within the layer only calculate up to height.
195 fRho[i] += B;
196 fRho[i+1] = fRho[i] - A;
197 }
198 }
199
200protected:
201 Double_t fObsLevel; // [cm] observation level a.s.l.
202
203public:
204 // Init an atmosphere from the data stored in MCorsikaRunHeader
205 MAtmRayleigh(const MCorsikaRunHeader &h)
206 {
207 Init(h);
208 }
209
210 // Defualt constructor
211 MAtmRayleigh() : fObsLevel(-1) { }
212
213 // Check if the ovservation level has been correctly initialized
214 // Used as a marker for correct initialization
215 Bool_t IsValid() const { return fObsLevel>=0; }
216
217 // Get the Earth radius to be used
218 Double_t R() const { return fR; }
219
220 // Init an atmosphere from the data stored in MCorsikaRunHeader
221 // This initialized fObsLevel, fR, fAtmB and fAtmC and
222 // PreCalcRho
223 void Init(const MCorsikaRunHeader &h)
224 {
225 // Observation level above earth radius
226 fObsLevel = h.GetObsLevel();
227
228 // Use earth radius as defined in Corsika
229 fR = h.EarthRadius();
230
231 //memcpy(fAtmA, (Float_t*)h.GetAtmosphericCoeffA(), sizeof(Float_t)*4);
232 memcpy(fAtmB, (Float_t*)h.GetAtmosphericCoeffB(), sizeof(Float_t)*4);
233 memcpy(fAtmC, (Float_t*)h.GetAtmosphericCoeffC(), sizeof(Float_t)*4);
234
235 PreCalcRho();
236 }
237
238 // Return the vertical thickness between the observer and height.
239 // Therefor the integral of the layers below (including the lower
240 // boudary) Have been precalculated by PreCalcRho
241 Double_t GetVerticalThickness(Double_t height) const
242 {
243 // FIXME: We could store the start point above obs-level
244 // (Does this really gain anything?)
245 Int_t i=0;
246 while (i<4 && height>fHeight[i+1])
247 i++;
248
249 const Double_t b = fAtmB[i];
250 const Double_t c = fAtmC[i];
251
252 return fRho[i] - b*TMath::Exp(-height/c);
253 }
254
255 /*
256 // The "orginal" code for the vertical thickness
257 Double_t GetVerticalThickness(Double_t obslev, Double_t height) const
258 {
259 // This is a C++-version of the original code from attenu.c
260
261 // Limits (height in cm) of the four layers in which atmosphere is parametrized:
262 const double lahg[5] =
263 {
264 obslev,
265 TMath::Max(obslev, 4e5),
266 1.0e6,
267 4.0e6,
268 1.0e7
269 };
270
271 Double_t Rho_Tot = 0.0;
272 for (int i=0; i<4; i++)
273 {
274 const Double_t b = fAtmB[i];
275 const Double_t c = fAtmC[i];
276
277 const Double_t h0 = TMath::Min(height, lahg[i+1]);
278 const Double_t h1 = lahg[i];
279
280 // Calculate rho for the i-th layer from the lower
281 // to the higher layer boundary.
282 // If height is within the layer only calculate up to height.
283 Rho_Tot += b*(exp(-h1/c) - exp(-h0/c));
284
285 if (lahg[i+1] > height)
286 break;
287 }
288
289 return Rho_Tot;
290 }
291 */
292 Double_t CalcTransmission(Double_t height, Double_t wavelength, Double_t sin2) const
293 {
294 // sin2: sin(theta)^2
295 // height is the true height a.s.l.
296
297 // LARGE ZENITH ANGLE FACTOR (AIR MASS FACTOR):
298 // Air mass factor "airmass" calculated using a one-exponential
299 // density profile for the atmosphere,
300 //
301 // rho = rho_0 exp(-height/hscale) with hscale = 7.4 km
302 //
303 // The air mass factor is defined as I(theta)/I(0), the ratio of
304 // the optical paths I (in g/cm2) traversed between two given
305 // heights, at theta and at 0 deg z.a.
306
307 const Double_t H = height-fObsLevel;
308 const Double_t h = 2*H;
309
310 // Scale-height (cm) for Exponential density profile
311 const Double_t hscale = 7.4e5;
312 const Double_t f = 2*hscale;
313
314 // Precalc R*cos(theta)^2 (FIXME: Is ph.GetCosW2 more precise?)
315 const Double_t Rcos2 = fR * (1-sin2); // cos2 = 1 - sin2
316
317 const Double_t x1 = TMath::Sqrt((Rcos2 ) / f);
318 const Double_t x2 = TMath::Sqrt((Rcos2 + 2*h) / f);
319 const Double_t x3 = TMath::Sqrt((fR ) / f);
320 const Double_t x4 = TMath::Sqrt((fR + 2*h) / f);
321
322 // Return a -1 transmittance in the case the photon comes
323 // exactly from the observation level, because in that case the
324 // "air mass factor" would become infinity and the calculation
325 // is not valid!
326 if (fabs(x3-x4) < 1.e-10)
327 return -1.;
328
329 const Double_t e12 = erfc(x1) - erfc(x2);
330 const Double_t e34 = erfc(x3) - erfc(x4);
331
332 const Double_t airmass = TMath::Exp(-fR*sin2 / f) * e12/e34;
333
334 // Calculate the traversed "vertical thickness" of air using the
335 // US Standard atmosphere:
336 const Double_t Rho_tot = GetVerticalThickness(/*fObsLevel,*/ height);
337
338 // We now convert from "vertical thickness" to "slanted thickness"
339 // traversed by the photon on its way to the telescope, simply
340 // multiplying by the air mass factor m:
341 const Double_t Rho_Fi = airmass * Rho_tot;
342
343 // Finally we calculate the transmission coefficient for the Rayleigh
344 // scattering:
345 // AM Dec 2002, introduced ABS below to account (in the future) for
346 // possible photons coming from below the observation level.
347
348 const Double_t wl = 400./wavelength;
349
350 // Mean free path for scattering Rayleigh XR (g/cm^2)
351 return TMath::Exp(-TMath::Abs(Rho_Fi/fgMeanFreePath)*wl*wl*wl*wl);
352 }
353};
354
355// ==========================================================================
356
357class MAtmosphere : public MAtmRayleigh
358{
359private:
360 static const Double_t STEPTHETA; // aprox. 1 degree
361
362 // Aerosol number density for 31 heights a.s.l., from 0 to 30 km,
363 // in 1 km steps (units: cm^-3)
364 static const Double_t aero_n[31];
365
366 // Ozone concentration for 51 heights a.s.l., from 0 to 50 km,
367 // in 1 km steps (units: cm/km)
368 static const Double_t oz_conc[51];
369
370 // aerosol_path contains the path integrals for the aerosol number
371 // density (relative to the number density at sea level) between the
372 // observation level and a height h for different zenith angles. The
373 // first index indicate height above sea level in units of 100m, the
374 // second is the zenith angle in degrees.
375 float aerosol_path[301][90];
376
377 // ozone_path contains the path integrals for the ozone concentration
378 // between the observation level and a height h for different zenith
379 // angles. The first index indicate height above sea level in units
380 // of 100m, the second is the zenith angle in degrees.
381 float ozone_path[501][90];
382
383 // Interpolate the graph at wavelength
384 Double_t GetBeta(Double_t wavelength, const TGraph &g) const
385 {
386 // FIXME: This might not be the fastest because range
387 // checks are done for each call!
388 return g.GetN()==0 ? 0 : g.Eval(wavelength)*1e-5; // from km^-1 to cm^-1
389/*
390 // Linear interpolation
391 // (FIXME: Is it faster to be replaced with a binary search?)
392 // ( This might be faster because we have more photons
393 // with smaller wavelengths)
394 //int index;
395 //for (index = 1; index <g.GetN()-1; index++)
396 // if (wavelength < g.GetX()[index])
397 // break;
398 const Int_t index = TMath::BinarySearch(g.GetN(), g.GetX(), wavelength)+1;
399
400 const Double_t t0 = g.GetY()[index-1];
401 const Double_t t1 = g.GetY()[index];
402
403 const Double_t w0 = g.GetX()[index-1];
404 const Double_t w1 = g.GetX()[index];
405
406 const Double_t beta0 = t0+(t1-t0)*(wavelength-w0)/(w1-w0);
407
408 return beta0 * 1e-5; // from km^-1 to cm^-1
409 */
410 }
411
412
413 //MSpline3 *fAbsCoeffOzone;
414 //MSpline3 *fAbsCoeffAerosols;
415
416 TGraph *fAbsCoeffOzone;
417 TGraph *fAbsCoeffAerosols;
418
419public:
420 MAtmosphere(const MCorsikaRunHeader &h) : fAbsCoeffOzone(0), fAbsCoeffAerosols(0)
421 {
422 Init(h);//, "ozone.txt", "aerosols.txt");
423 }
424
425 MAtmosphere(const char *name1=0, const char *name2=0) : fAbsCoeffOzone(0), fAbsCoeffAerosols(0)
426 {
427 if (name1)
428 InitOzone(name1);
429 if (name2)
430 InitAerosols(name2);
431 }
432
433 ~MAtmosphere()
434 {
435 if (fAbsCoeffOzone)
436 delete fAbsCoeffOzone;
437 if (fAbsCoeffAerosols)
438 delete fAbsCoeffAerosols;
439 }
440
441 Float_t GetWavelengthMin() const { return fAbsCoeffOzone && fAbsCoeffAerosols ? TMath::Max(fAbsCoeffOzone->GetX()[0], fAbsCoeffAerosols->GetX()[0]) : -1; }
442 Float_t GetWavelengthMax() const { return fAbsCoeffOzone && fAbsCoeffAerosols ? TMath::Min(fAbsCoeffOzone->GetX()[fAbsCoeffOzone->GetN()-1], fAbsCoeffAerosols->GetX()[fAbsCoeffAerosols->GetN()-1]) : -1; }
443
444 Bool_t HasValidOzone() const { return fAbsCoeffOzone && fAbsCoeffOzone->GetN()>0; }
445 Bool_t HasValidAerosol() const { return fAbsCoeffAerosols && fAbsCoeffAerosols->GetN()>0; }
446
447 Bool_t IsAllValid() const { return IsValid() && HasValidOzone() && HasValidAerosol(); }
448
449 void PreCalcOzone()
450 {
451 // It follows a precalculation of the slant path integrals we need
452 // for the estimate of the Mie scattering and Ozone absorption:
453 Double_t dh = 1.e3;
454 const Double_t STEPTHETA = 1.74533e-2; // aprox. 1 degree
455
456 // Ozone absorption
457 for (Int_t j = 0; j < 90; j++)
458 {
459 const Double_t theta = j * STEPTHETA;
460 const Double_t sin2 = sin(theta)*sin(theta);
461 const Double_t H = R()+fObsLevel;
462
463 Double_t path_slant = 0;
464 for (Double_t h = fObsLevel; h <= 50e5; h += dh)
465 {
466 // h is the true height vertical above ground
467 if (fmod(h,1e4) == 0)
468 ozone_path[(int)(h/1e4)][j] = path_slant;
469
470 const Double_t km = h/1e5;
471 const Int_t i = TMath::FloorNint(km);
472 const Double_t l = R()+h;
473
474 const Double_t L = TMath::Sqrt(l*l - H*H * sin2);
475 const Double_t f = dh * l / L;
476
477 // Linear interpolation at h/1e5
478 Double_t interpol = oz_conc[i] + fmod(km, 1) * (oz_conc[i+1]-oz_conc[i]);
479
480 path_slant += f * interpol;
481 }
482 }
483 }
484
485 void PreCalcAerosol()
486 {
487 // It follows a precalculation of the slant path integrals we need
488 // for the estimate of the Mie scattering and Ozone absorption:
489 Double_t dh = 1.e3;
490 const Double_t STEPTHETA = 1.74533e-2; // aprox. 1 degree
491
492 /* Mie (aerosol): */
493 for (Int_t j = 0; j < 90; j++)
494 {
495 const Double_t theta = j * STEPTHETA;
496 const Double_t sin2 = sin(theta)*sin(theta);
497 const Double_t H = R()+fObsLevel;
498
499 Double_t path_slant = 0;
500 for (Double_t h = fObsLevel; h <= 30e5; h += dh)
501 {
502 // h is the true height vertical above ground
503 if (fmod(h,1e4) == 0)
504 aerosol_path[(int)(h/1e4)][j] = path_slant;
505
506 const Double_t km = h/1e5;
507 const Int_t i = TMath::FloorNint(km);
508 const Double_t l = R()+h;
509
510 const Double_t L = TMath::Sqrt(l*l - H*H * sin2);
511 const Double_t f = dh * l / L;
512
513 // Linear interpolation at h/1e5
514 Double_t interpol = aero_n[i] + fmod(km, 1)*(aero_n[i+1]-aero_n[i]);
515
516 path_slant += f * interpol/aero_n[0]; // aero_n [km^-1]
517 }
518 }
519 }
520
521 Bool_t InitOzone(const TString name="")
522 {
523 if (!name.IsNull())
524 {
525 if (fAbsCoeffOzone)
526 delete fAbsCoeffOzone;
527
528 fAbsCoeffOzone = new TGraph(name);
529 fAbsCoeffOzone->Sort();
530 }
531
532 if (!HasValidAerosol())
533 return kFALSE;
534
535 if (IsValid())
536 PreCalcOzone();
537
538 return kTRUE;
539 }
540
541 Bool_t InitAerosols(const TString name="")
542 {
543 if (!name.IsNull())
544 {
545 if (fAbsCoeffAerosols)
546 delete fAbsCoeffAerosols;
547
548 fAbsCoeffAerosols = new TGraph(name);
549 fAbsCoeffAerosols->Sort();
550 }
551
552 if (!HasValidAerosol())
553 return kFALSE;
554
555 if (IsValid())
556 PreCalcAerosol();
557
558 return kTRUE;
559 }
560
561 void Init(const MCorsikaRunHeader &h, const char *name1=0, const char *name2=0)
562 {
563 MAtmRayleigh::Init(h);
564
565 InitOzone(name1);
566 InitAerosols(name2);
567 }
568/*
569 Double_t GetOz(Double_t height, Double_t theta) const
570 {
571 // Distance between two points D = 1km /cos(theta)
572 // Density along y within this km: f = (x[i+1]-x[i])/1km * dy
573 // Integral of this density f = (x[i+1]-x[i])/1km * (y[i+1]-y[i])
574 // f(h) = int [ (c1-c0)/1km*(h-h0)*dh + c0 ] dh
575 // = (c-co)*(h-h0)
576
577 Double_t rc = 0;
578 int i;
579 for (i=0; i<49; i++)
580 if (i>=2 && i+1<height/1e5) // cm -> km
581 rc += oz_conc[i] * 1e5/cos(theta);
582
583 rc -= oz_conc[2]*0.2*1e5/cos(theta);
584 rc += oz_conc[i+1]*fmod(height/1e5,1)*1e5/cos(theta);
585
586 return rc;
587 }
588 */
589
590 Double_t CalcOzoneAbsorption(Double_t h, Double_t wavelength, Double_t theta) const
591 {
592 if (!fAbsCoeffOzone)
593 return 1;
594
595 //******* Ozone absorption *******
596 if (h > 50.e5)
597 h = 50.e5;
598
599 // Vigroux Ozone absorption coefficient a.s.l. through interpolation:
600 //const float oz_vigroux[15]= {1.06e2, 1.01e1, 8.98e-1, 6.40e-2, 1.80e-3, 0, 0, 3.50e-3, 3.45e-2, 9.20e-2, 1.32e-1, 6.20e-2, 2.30e-2, 1.00e-2, 0.00};
601 //const Double_t beta0 = getbeta(wavelength, oz_vigroux);
602 const Double_t beta0 = GetBeta(wavelength, *fAbsCoeffOzone);
603
604 // Now use the pre-calculated values of the path integral
605 // for h and theta
606 const UInt_t H = TMath::Nint(h/1e4);
607 const UInt_t T = TMath::Min(89, TMath::Nint(theta/STEPTHETA));
608
609 const Double_t path = ozone_path[H][T];
610
611 return TMath::Exp(-beta0*path);
612 }
613
614 Double_t CalcAerosolAbsorption(Double_t h, Double_t wavelength, Double_t theta) const
615 {
616 if (!fAbsCoeffAerosols)
617 return 1;
618
619 //******* Mie (aerosol) *******
620 if (h > 30.e5)
621 h = 30.e5;
622
623 //const float aero_betap[15] = {0.27, 0.26, 0.25, 0.24, 0.24, 0.23, 0.20, 0.180, 0.167, 0.158, 0.150, 0.142, 0.135, 0.127, 0.120};
624 //const Double_t beta0 = getbeta(wavelength, aero_betap);
625 const Double_t beta0 = GetBeta(wavelength, *fAbsCoeffAerosols);
626
627 // Now use the pre-calculated values of the path integral
628 // for h and theta
629 const UInt_t H = TMath::Nint(h/1e4);
630 const UInt_t T = TMath::Min(89, TMath::Nint(theta/STEPTHETA));
631
632
633 const Double_t path = aerosol_path[H][T];
634
635 return TMath::Exp(-beta0*path);
636 }
637
638 Double_t GetTransmission(const MPhotonData &ph) const
639 {
640 const Double_t wavelength = ph.GetWavelength();
641 const Double_t height = ph.GetProductionHeight();
642
643 // Reduce the necessary number of floating point operations
644 // by storing the intermediate results
645 const Double_t sin2 = ph.GetSinW2();
646 const Double_t cost = TMath::Sqrt(1-sin2);
647 const Double_t theta = TMath::ACos(cost);
648
649 // Path from production height to obslevel
650 const Double_t z = height-fObsLevel;
651
652 // Distance of emission point to incident point on ground
653 const Double_t d = z/cost;
654
655 // Avoid problems if photon is very close to telescope:
656 if (TMath::Abs(d)<1)
657 return 1;
658
659 // Earth radius plus observation height (distance of telescope
660 // from earth center)
661 const Double_t H = R() + fObsLevel;
662
663 // We calculate h, the true height a.s.l.
664 // of the photon emission point in cm
665 const Double_t h = TMath::Sqrt(H*H + d*d + 2*H*z) - R();
666
667 //**** Rayleigh scattering: *****
668 const Double_t T_Ray = CalcTransmission(h, wavelength, sin2);
669 if (T_Ray<0)
670 return 0;
671
672 //****** Ozone absorption: ******
673 const Double_t T_Oz = CalcOzoneAbsorption(h, wavelength, theta);
674
675 //******** Mie (aerosol) ********
676 const Double_t T_Mie = CalcAerosolAbsorption(h, wavelength, theta);
677
678 // FIXME: What if I wanna display these values?
679
680 // Calculate final transmission coefficient
681 return T_Ray * T_Oz * T_Mie;
682 }
683};
684
685const Double_t MAtmosphere::STEPTHETA = 1.74533e-2; // aprox. 1 degree
686
687const Double_t MAtmRayleigh::fgMeanFreePath = 2970;
688
689const Double_t MAtmosphere::aero_n[31] = {200, 87, 38, 16, 7.2, 3.1, 1.1, 0.4, 0.14, 5.0e-2, 2.6e-2, 2.3e-2, 2.1e-2, 2.3e-2, 2.5e-2, 4.1e-2, 6.7e-2, 7.3e-2, 8.0e-2, 9.0e-2, 8.6e-2, 8.2e-2, 8.0e-2, 7.6e-2, 5.2e-2, 3.6e-2, 2.5e-2, 2.4e-2, 2.2e-2, 2.0e-2, 1.9e-2};
690
691const Double_t MAtmosphere::oz_conc[51]={0.3556603E-02, 0.3264150E-02, 0.2933961E-02, 0.2499999E-02, 0.2264150E-02, 0.2207546E-02, 0.2160377E-02, 0.2226414E-02, 0.2283018E-02, 0.2811320E-02, 0.3499999E-02, 0.4603772E-02, 0.6207545E-02, 0.8452828E-02, 0.9528299E-02, 0.9905657E-02, 0.1028302E-01, 0.1113207E-01, 0.1216981E-01, 0.1424528E-01, 0.1641509E-01, 0.1839622E-01, 0.1971697E-01, 0.1981131E-01, 0.1933962E-01, 0.1801886E-01, 0.1632075E-01, 0.1405660E-01, 0.1226415E-01, 0.1066037E-01, 0.9028300E-02, 0.7933960E-02, 0.6830187E-02, 0.5820753E-02, 0.4830188E-02, 0.4311319E-02, 0.3613206E-02, 0.3018867E-02, 0.2528301E-02, 0.2169811E-02, 0.1858490E-02, 0.1518867E-02, 0.1188679E-02, 0.9301884E-03, 0.7443394E-03, 0.5764149E-03, 0.4462263E-03, 0.3528301E-03, 0.2792452E-03, 0.2226415E-03, 0.1858490E-03};
692
693// ==========================================================================
694
695// --------------------------------------------------------------------------
696//
697// Default Constructor.
698//
699MSimAtmosphere::MSimAtmosphere(const char* name, const char *title)
700 : fEvt(0), fAtmosphere(0),
701 fFileAerosols("resmc/atmosphere-aerosols.txt"),
702 fFileOzone("resmc/atmosphere-ozone.txt")
703{
704 fName = name ? name : "MSimAtmosphere";
705 fTitle = title ? title : "Simulate the wavelength and height-dependant atmpsheric absorption";
706
707 fAtmosphere = new MAtmosphere;
708}
709
710// --------------------------------------------------------------------------
711//
712// Calls Clear()
713//
714MSimAtmosphere::~MSimAtmosphere()
715{
716 delete fAtmosphere;
717}
718
719// --------------------------------------------------------------------------
720//
721// Search for the needed parameter containers. Read spline from file
722// calling ReadFile();
723//
724Int_t MSimAtmosphere::PreProcess(MParList *pList)
725{
726 fEvt = (MPhotonEvent*)pList->FindObject("MPhotonEvent");
727 if (!fEvt)
728 {
729 *fLog << err << "MPhotonEvent not found... aborting." << endl;
730 return kFALSE;
731 }
732
733
734 return kTRUE;
735}
736
737// --------------------------------------------------------------------------
738//
739Bool_t MSimAtmosphere::ReInit(MParList *pList)
740{
741 MCorsikaRunHeader *h = (MCorsikaRunHeader*)pList->FindObject("MCorsikaRunHeader");
742 if (!h)
743 {
744 *fLog << err << "MCorsikaRunHeader not found... aborting." << endl;
745 return kFALSE;
746 }
747
748 //if (fRunHeader->Has(MCorsikaRunHeader::kRefraction))
749 // *fLog << inf << "Atmospheric refraction already applied in Corsika... skipping our own." << endl;
750
751 // FIXME: Check wavelength range
752
753 /*
754 if (h->GetWavelengthMin()<fSpline->GetXmin())
755 *fLog << warn << "WARNING - Lower bound of wavelength bandwidth exceeds lower bound of spline." << endl;
756
757 if (h->GetWavelengthMax()>fSpline->GetXmax())
758 *fLog << warn << "WARNING - Upper bound of wavelength bandwidth exceeds upper bound of spline." << endl;
759 */
760
761 fAtmosphere->Init(*h, fFileOzone, fFileAerosols);
762
763 if (!fAtmosphere->IsAllValid())
764 {
765 *fLog << err << "ERROR - Something with the atmoshere's initialization went wrong!" << endl;
766 return kFALSE;
767 }
768
769 if (h->GetWavelengthMin()<fAtmosphere->GetWavelengthMin())
770 *fLog << warn << "WARNING - Lower bound of wavelength bandwidth exceeds valid range of atmosphere." << endl;
771
772 if (h->GetWavelengthMax()>fAtmosphere->GetWavelengthMax())
773 *fLog << warn << "WARNING - Lower bound of wavelength bandwidth exceeds valid range of atmosphere." << endl;
774
775 if (!h->Has(MCorsikaRunHeader::kAtmext))
776 *fLog << warn << "WARNING - ATMEXT option not used for Corsika data." << endl;
777
778 if (!h->Has(MCorsikaRunHeader::kRefraction))
779 *fLog << warn << "WARNING - Refraction calculation disabled for Corsika data." << endl;
780
781 return kTRUE;
782}
783
784// --------------------------------------------------------------------------
785//
786Int_t MSimAtmosphere::Process()
787{
788 // Get the number of photons in the list
789 const Int_t num = fEvt->GetNumPhotons();
790
791 // FIMXE: Add checks for
792 // * upgoing particles
793 // * Can we take the full length until the camera into account?
794
795 // Counter for number of total and final events
796 Int_t cnt = 0;
797 for (Int_t i=0; i<num; i++)
798 {
799 // Get i-th photon from the list
800 const MPhotonData &ph = (*fEvt)[i];
801
802 // Get atmospheric transmission for this photon
803 const Double_t eff = fAtmosphere->GetTransmission(ph);
804
805 // Get a random value between 0 and 1 to determine whether the photon will survive
806 // gRandom->Rndm() = [0;1[
807 if (gRandom->Rndm()>=eff)
808 continue;
809
810 // Copy the surviving events bakc in the list
811 (*fEvt)[cnt++] = ph;
812 }
813
814 // Now we shrink the array to the number of new entries.
815 fEvt->Shrink(cnt);
816
817 return kTRUE;
818}
819
820/*
821 Int_t MSimWavelength::Process()
822 {
823 // Get the number of photons in the list
824 const Int_t num = fEvt->GetNumPhotons();
825
826 // FIMXE: Add checks for
827 // * upgoing particles
828 // * wavelength range
829 // * check if corsika atmosphere is switched on
830 // * Can we take the full length until the camera into account?
831
832 // Counter for number of total and final events
833 Int_t cnt = 0;
834 for (Int_t i=0; i<num; i++)
835 {
836 // Get i-th photon from the list
837 MPhotonData &ph = (*fEvt)[i];
838
839 const Double_t min = fRunHeader->GetWavelengthMin(); // WAVLGL
840 const Double_t max = fRunHeader->GetWavelengthMax(); // WAVLGU
841 const Double_t f = (max-min)/max;
842
843 // WAVELENGTH = 1. / (1/min - RD(1)/(min*max/(max-min)))
844
845
846 ph.SetWavelength(TMath::Nint(min / (1. - gRandom->Rndm()*f)));
847 }
848
849 return kTRUE;
850 }
851 */
852
853// --------------------------------------------------------------------------
854//
855// FileAerosols: resmc/atmosphere-aerosols.txt
856// FileOzone: resmc/atmosphere-ozone.txt
857//
858Int_t MSimAtmosphere::ReadEnv(const TEnv &env, TString prefix, Bool_t print)
859{
860 Bool_t rc = kFALSE;
861
862 if (IsEnvDefined(env, prefix, "FileAerosols", print))
863 {
864 rc = kTRUE;
865 fFileAerosols = GetEnvValue(env, prefix, "FileAerosols", fFileAerosols);
866 }
867
868 if (IsEnvDefined(env, prefix, "FileOzone", print))
869 {
870 rc = kTRUE;
871 fFileOzone = GetEnvValue(env, prefix, "FileOzone", fFileOzone);
872 }
873
874 return rc;
875}
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