/* ======================================================================== *\ ! ! * ! * This file is part of CheObs, the Modular Analysis and Reconstruction ! * Software. It is distributed to you in the hope that it can be a useful ! * and timesaving tool in analysing Data of imaging Cerenkov telescopes. ! * It is distributed WITHOUT ANY WARRANTY. ! * ! * Permission to use, copy, modify and distribute this software and its ! * documentation for any purpose is hereby granted without fee, ! * provided that the above copyright notice appears in all copies and ! * that both that copyright notice and this permission notice appear ! * in supporting documentation. It is provided "as is" without express ! * or implied warranty. ! * ! ! ! Author(s): Thomas Bretz, 1/2009 ! ! Copyright: CheObs Software Development, 2000-2009 ! ! \* ======================================================================== */ ////////////////////////////////////////////////////////////////////////////// // // MSimAtmosphere // // Task to calculate wavelength or incident angle dependent absorption // // Input Containers: // MPhotonEvent // MCorsikaRunHeader // // Output Containers: // MPhotonEvent // ////////////////////////////////////////////////////////////////////////////// #include "MSimAtmosphere.h" #include #include #include #include "MLog.h" #include "MLogManip.h" #include "MParList.h" #include "MCorsikaRunHeader.h" #include "MPhotonEvent.h" #include "MPhotonData.h" ClassImp(MSimAtmosphere); using namespace std; // ========================================================================== // // January 2002, A. Moralejo: We now precalculate the slant paths for the // aerosol and Ozone vertical profiles, and then do an interpolation in // wavelength for every photon to get the optical depths. The parameters // used, defined below, have been taken from "Atmospheric Optics", by // L. Elterman and R.B. Toolin, chapter 7 of the "Handbook of geophysics // and Space environments". (S.L. Valley, editor). McGraw-Hill, NY 1965. // // WARNING: the Mie scattering and the Ozone absorption are implemented // to work only with photons produced at a height a.s.l larger than the // observation level. So this is not expected to work well for simulating // the telescope pointing at theta > 90 deg (for instance for neutrino // studies. Rayleigh scattering works even for light coming from below. // // Fixed bugs (of small influence) in Mie absorption implementation: there // were errors in the optical depths table, as well as a confusion: // height a.s.l. was used as if it was height above the telescope level. // The latter error was also present in the Ozone aborption implementation. // // On the other hand, now we have the tables AE_ABI and OZ_ABI with optical // depths between sea level and a height h (before it was between 2km a.s.l // and a height h). So that we can simulate also in the future a different // observation level. // // AM: WARNING: IF VERY LARGE zenith angle simulations are to be done (say // above 85 degrees, for neutrino primaries or any other purpose) this code // will have to be adapted accordingly and checked, since in principle it has // been written and tested to simulate the absorption of Cherenkov photons // arriving at the telescope from above. // // AM: WARNING 2: not to be used for wavelengths outside the range 250-700 nm // // January 2003, Abelardo Moralejo: found error in Ozone absorption treatment. // At large zenith angles, the air mass used was the one calculated for // Rayleigh scattering, but since the Ozone distribution is rather different // from the global distribution of air molecules, this is not a good // approximation. Now I have left in this code only the Rayleigh scattering, // and moved to atm.c the Mie scattering and Ozone absorption calculated in // a better way. // // A. Moralejo, January 2003: added some parameters for Mie scattering // and Ozone absorption derived from the clear standard atmosphere model // in "Atmospheric Optics", by L. Elterman and R.B. Toolin, chapter 7 of // the "Handbook of geophysics and Space environments". S.L. Valley, // editor. McGraw-Hill, NY 1965. // // AM, Jan 2003: Changed the meaning of the argument height: now it is the // true height above sea level at which a photon has been emitted, before // it was the height given by Corsika, measured in the vertical of the // observer and not in the vertical of the emitting particle. // // // MAGIC-Winter and MAGIC-Summer by M. Haffke, // parametrizing profiles obtained with MSIS: // http://uap-www.nrl.navy.mil/models_web/msis/msis_home.htm // // // The MAGIC-Winter and MAGIC-Summer parametrisations reproduce the MSIS // profiles for the 3 atmospheric layers from 0 up to 40 km height. Beyond // that height, it was not possible to achieve a good fit, but the amount // of residual atmosphere is so small that light absorption would be // negligible anyway. Showers develop well below 40 km. // // // The mass overburden is given by T = AATM + BATM * exp(-h/CATM) // The last layer of the US standard atmosphere (in which T varies // linearly with h) is above 100 km and has not been included here // because it should not matter. // class MAtmRayleigh { private: static const Double_t fgMeanFreePath; // [g/cm^2] Mean free path for scattering Rayleigh XR Double_t fR; // [cm] Earth radius to be used Double_t fHeight[5]; // Layer boundaries (atmospheric layer) // Parameters of the different atmospheres. We use the same parametrization // shape as in Corsika atmospheric models (see Corsika manual, appendix D). // The values here can be/are obtained from the Corsika output //Float_t fAtmA[4]; // The index refers to the atmospheric layer (starting from sea level and going upwards) Float_t fAtmB[4]; // The index refers to the atmospheric layer (starting from sea level and going upwards) Float_t fAtmC[4]; // The index refers to the atmospheric layer (starting from sea level and going upwards) Double_t fRho[5]; // Precalculated integrals for rayleigh scatterning // -------------------------------------------------------------------------- // // Precalcalculate the integrals from the observer level to the next // atmpsheric layer below including the lower boundary. Thus a // correct calculation is reduced to the calculation of the upper // boundary. // // fRho[0] = B0; // fRho[1] = B0-A0 + B1; // fRho[2] = B0-A0 + B1-A1 + B2; // fRho[3] = B0-A0 + B1-A1 + B2+A2 + B3; // fRho[4] = B0-A0 + B1-A1 + B2+A2 + B3 - A3; // void PreCalcRho() { // Limits (height in cm) of the four layers in which // atmosphere is parametrized. // This is a stupid trick giving 0 for the integrals below // the observer // FIXME: Could be replaced by 0, AtmLay[0]-fAtmLay[3] const Double_t h[5] = { fObsLevel, // fObsLevel, // 0km TMath::Max(fObsLevel, 7.75e5), // TMath::Max(fObsLevel, 4e5), // 4km 16.5e5, // 10e5, // 10km 50.0e5, // 40e5, // 40km 105.0e5, // 100e5 // 100km }; memcpy(fHeight, h, sizeof(Double_t)*5); fRho[0] = 0; for (int i=0; i<4; i++) { const Double_t b = fAtmB[i]; const Double_t c = fAtmC[i]; const Double_t h1 = h[i+1]; const Double_t h0 = h[i]; const Double_t B = b*TMath::Exp(-h0/c); const Double_t A = b*TMath::Exp(-h1/c); // Calculate rho for the i-th layer from the lower // to the higher layer boundary. // If height is within the layer only calculate up to height. fRho[i] += B; fRho[i+1] = fRho[i] - A; } } protected: Double_t fObsLevel; // [cm] observation level a.s.l. public: // Init an atmosphere from the data stored in MCorsikaRunHeader MAtmRayleigh(const MCorsikaRunHeader &h) { Init(h); } // Defualt constructor MAtmRayleigh() : fObsLevel(-1) { } // Check if the ovservation level has been correctly initialized // Used as a marker for correct initialization Bool_t IsValid() const { return fObsLevel>=0; } // Get the Earth radius to be used Double_t R() const { return fR; } // Init an atmosphere from the data stored in MCorsikaRunHeader // This initialized fObsLevel, fR, fAtmB and fAtmC and // PreCalcRho void Init(const MCorsikaRunHeader &h) { // Observation level above earth radius fObsLevel = h.GetObsLevel(); // Use earth radius as defined in Corsika fR = h.EarthRadius(); //memcpy(fAtmA, (Float_t*)h.GetAtmosphericCoeffA(), sizeof(Float_t)*4); memcpy(fAtmB, (Float_t*)h.GetAtmosphericCoeffB(), sizeof(Float_t)*4); memcpy(fAtmC, (Float_t*)h.GetAtmosphericCoeffC(), sizeof(Float_t)*4); PreCalcRho(); } // Return the vertical thickness between the observer and height. // Therefor the integral of the layers below (including the lower // boudary) Have been precalculated by PreCalcRho Double_t GetVerticalThickness(Double_t height) const { // FIXME: We could store the start point above obs-level // (Does this really gain anything?) Int_t i=0; while (i<4 && height>fHeight[i+1]) i++; const Double_t b = fAtmB[i]; const Double_t c = fAtmC[i]; return fRho[i] - b*TMath::Exp(-height/c); } /* // The "orginal" code for the vertical thickness Double_t GetVerticalThickness(Double_t obslev, Double_t height) const { // This is a C++-version of the original code from attenu.c // Limits (height in cm) of the four layers in which atmosphere is parametrized: const double lahg[5] = { obslev, TMath::Max(obslev, 4e5), 1.0e6, 4.0e6, 1.0e7 }; Double_t Rho_Tot = 0.0; for (int i=0; i<4; i++) { const Double_t b = fAtmB[i]; const Double_t c = fAtmC[i]; const Double_t h0 = TMath::Min(height, lahg[i+1]); const Double_t h1 = lahg[i]; // Calculate rho for the i-th layer from the lower // to the higher layer boundary. // If height is within the layer only calculate up to height. Rho_Tot += b*(exp(-h1/c) - exp(-h0/c)); if (lahg[i+1] > height) break; } return Rho_Tot; } */ Double_t CalcTransmission(Double_t height, Double_t wavelength, Double_t sin2) const { // sin2: sin(theta)^2 // height is the true height a.s.l. // LARGE ZENITH ANGLE FACTOR (AIR MASS FACTOR): // Air mass factor "airmass" calculated using a one-exponential // density profile for the atmosphere, // // rho = rho_0 exp(-height/hscale) with hscale = 7.4 km // // The air mass factor is defined as I(theta)/I(0), the ratio of // the optical paths I (in g/cm2) traversed between two given // heights, at theta and at 0 deg z.a. const Double_t H = height-fObsLevel; const Double_t h = 2*H; // Scale-height (cm) for Exponential density profile const Double_t hscale = 7.4e5; const Double_t f = 2*hscale; // Precalc R*cos(theta)^2 (FIXME: Is ph.GetCosW2 more precise?) const Double_t Rcos2 = fR * (1-sin2); // cos2 = 1 - sin2 const Double_t x1 = TMath::Sqrt((Rcos2 ) / f); const Double_t x2 = TMath::Sqrt((Rcos2 + 2*h) / f); const Double_t x3 = TMath::Sqrt((fR ) / f); const Double_t x4 = TMath::Sqrt((fR + 2*h) / f); // Return a -1 transmittance in the case the photon comes // exactly from the observation level, because in that case the // "air mass factor" would become infinity and the calculation // is not valid! if (fabs(x3-x4) < 1.e-10) return -1.; const Double_t e12 = erfc(x1) - erfc(x2); const Double_t e34 = erfc(x3) - erfc(x4); const Double_t airmass = TMath::Exp(-fR*sin2 / f) * e12/e34; // Calculate the traversed "vertical thickness" of air using the // US Standard atmosphere: const Double_t Rho_tot = GetVerticalThickness(/*fObsLevel,*/ height); // We now convert from "vertical thickness" to "slanted thickness" // traversed by the photon on its way to the telescope, simply // multiplying by the air mass factor m: const Double_t Rho_Fi = airmass * Rho_tot; // Finally we calculate the transmission coefficient for the Rayleigh // scattering: // AM Dec 2002, introduced ABS below to account (in the future) for // possible photons coming from below the observation level. const Double_t wl = 400./wavelength; // Mean free path for scattering Rayleigh XR (g/cm^2) return TMath::Exp(-TMath::Abs(Rho_Fi/fgMeanFreePath)*wl*wl*wl*wl); } }; // ========================================================================== class MAtmosphere : public MAtmRayleigh { private: static const Double_t STEPTHETA; // aprox. 1 degree // Aerosol number density for 31 heights a.s.l., from 0 to 30 km, // in 1 km steps (units: cm^-3) static const Double_t aero_n[31]; // Ozone concentration for 51 heights a.s.l., from 0 to 50 km, // in 1 km steps (units: cm/km) static const Double_t oz_conc[51]; // aerosol_path contains the path integrals for the aerosol number // density (relative to the number density at sea level) between the // observation level and a height h for different zenith angles. The // first index indicate height above sea level in units of 100m, the // second is the zenith angle in degrees. float aerosol_path[301][90]; // ozone_path contains the path integrals for the ozone concentration // between the observation level and a height h for different zenith // angles. The first index indicate height above sea level in units // of 100m, the second is the zenith angle in degrees. float ozone_path[501][90]; // Interpolate the graph at wavelength Double_t GetBeta(Double_t wavelength, const TGraph &g) const { // FIXME: This might not be the fastest because range // checks are done for each call! return g.GetN()==0 ? 0 : g.Eval(wavelength)*1e-5; // from km^-1 to cm^-1 /* // Linear interpolation // (FIXME: Is it faster to be replaced with a binary search?) // ( This might be faster because we have more photons // with smaller wavelengths) //int index; //for (index = 1; index GetX()[0], fAbsCoeffAerosols->GetX()[0]) : -1; } Float_t GetWavelengthMax() const { return fAbsCoeffOzone && fAbsCoeffAerosols ? TMath::Min(fAbsCoeffOzone->GetX()[fAbsCoeffOzone->GetN()-1], fAbsCoeffAerosols->GetX()[fAbsCoeffAerosols->GetN()-1]) : -1; } Bool_t HasValidOzone() const { return fAbsCoeffOzone && fAbsCoeffOzone->GetN()>0; } Bool_t HasValidAerosol() const { return fAbsCoeffAerosols && fAbsCoeffAerosols->GetN()>0; } Bool_t IsAllValid() const { return IsValid() && HasValidOzone() && HasValidAerosol(); } void PreCalcOzone() { // It follows a precalculation of the slant path integrals we need // for the estimate of the Mie scattering and Ozone absorption: Double_t dh = 1.e3; const Double_t STEPTHETA = 1.74533e-2; // aprox. 1 degree // Ozone absorption for (Int_t j = 0; j < 90; j++) { const Double_t theta = j * STEPTHETA; const Double_t sin2 = sin(theta)*sin(theta); const Double_t H = R()+fObsLevel; Double_t path_slant = 0; for (Double_t h = fObsLevel; h <= 50e5; h += dh) { // h is the true height vertical above ground if (fmod(h,1e4) == 0) ozone_path[(int)(h/1e4)][j] = path_slant; const Double_t km = h/1e5; const Int_t i = TMath::FloorNint(km); const Double_t l = R()+h; const Double_t L = TMath::Sqrt(l*l - H*H * sin2); const Double_t f = dh * l / L; // Linear interpolation at h/1e5 Double_t interpol = oz_conc[i] + fmod(km, 1) * (oz_conc[i+1]-oz_conc[i]); path_slant += f * interpol; } } } void PreCalcAerosol() { // It follows a precalculation of the slant path integrals we need // for the estimate of the Mie scattering and Ozone absorption: Double_t dh = 1.e3; const Double_t STEPTHETA = 1.74533e-2; // aprox. 1 degree /* Mie (aerosol): */ for (Int_t j = 0; j < 90; j++) { const Double_t theta = j * STEPTHETA; const Double_t sin2 = sin(theta)*sin(theta); const Double_t H = R()+fObsLevel; Double_t path_slant = 0; for (Double_t h = fObsLevel; h <= 30e5; h += dh) { // h is the true height vertical above ground if (fmod(h,1e4) == 0) aerosol_path[(int)(h/1e4)][j] = path_slant; const Double_t km = h/1e5; const Int_t i = TMath::FloorNint(km); const Double_t l = R()+h; const Double_t L = TMath::Sqrt(l*l - H*H * sin2); const Double_t f = dh * l / L; // Linear interpolation at h/1e5 Double_t interpol = aero_n[i] + fmod(km, 1)*(aero_n[i+1]-aero_n[i]); path_slant += f * interpol/aero_n[0]; // aero_n [km^-1] } } } Bool_t InitOzone(const TString name="") { if (!name.IsNull()) { if (fAbsCoeffOzone) delete fAbsCoeffOzone; fAbsCoeffOzone = new TGraph(name); fAbsCoeffOzone->Sort(); } if (!HasValidAerosol()) return kFALSE; if (IsValid()) PreCalcOzone(); return kTRUE; } Bool_t InitAerosols(const TString name="") { if (!name.IsNull()) { if (fAbsCoeffAerosols) delete fAbsCoeffAerosols; fAbsCoeffAerosols = new TGraph(name); fAbsCoeffAerosols->Sort(); } if (!HasValidAerosol()) return kFALSE; if (IsValid()) PreCalcAerosol(); return kTRUE; } void Init(const MCorsikaRunHeader &h, const char *name1=0, const char *name2=0) { MAtmRayleigh::Init(h); InitOzone(name1); InitAerosols(name2); } /* Double_t GetOz(Double_t height, Double_t theta) const { // Distance between two points D = 1km /cos(theta) // Density along y within this km: f = (x[i+1]-x[i])/1km * dy // Integral of this density f = (x[i+1]-x[i])/1km * (y[i+1]-y[i]) // f(h) = int [ (c1-c0)/1km*(h-h0)*dh + c0 ] dh // = (c-co)*(h-h0) Double_t rc = 0; int i; for (i=0; i<49; i++) if (i>=2 && i+1 km rc += oz_conc[i] * 1e5/cos(theta); rc -= oz_conc[2]*0.2*1e5/cos(theta); rc += oz_conc[i+1]*fmod(height/1e5,1)*1e5/cos(theta); return rc; } */ Double_t CalcOzoneAbsorption(Double_t h, Double_t wavelength, Double_t theta) const { if (!fAbsCoeffOzone) return 1; //******* Ozone absorption ******* if (h > 50.e5) h = 50.e5; // Vigroux Ozone absorption coefficient a.s.l. through interpolation: //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}; //const Double_t beta0 = getbeta(wavelength, oz_vigroux); const Double_t beta0 = GetBeta(wavelength, *fAbsCoeffOzone); // Now use the pre-calculated values of the path integral // for h and theta const UInt_t H = TMath::Nint(h/1e4); const UInt_t T = TMath::Min(89, TMath::Nint(theta/STEPTHETA)); const Double_t path = ozone_path[H][T]; return TMath::Exp(-beta0*path); } Double_t CalcAerosolAbsorption(Double_t h, Double_t wavelength, Double_t theta) const { if (!fAbsCoeffAerosols) return 1; //******* Mie (aerosol) ******* if (h > 30.e5) h = 30.e5; //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}; //const Double_t beta0 = getbeta(wavelength, aero_betap); const Double_t beta0 = GetBeta(wavelength, *fAbsCoeffAerosols); // Now use the pre-calculated values of the path integral // for h and theta const UInt_t H = TMath::Nint(h/1e4); const UInt_t T = TMath::Min(89, TMath::Nint(theta/STEPTHETA)); const Double_t path = aerosol_path[H][T]; return TMath::Exp(-beta0*path); } Double_t GetTransmission(const MPhotonData &ph) const { const Double_t wavelength = ph.GetWavelength(); const Double_t height = ph.GetProductionHeight(); // Reduce the necessary number of floating point operations // by storing the intermediate results const Double_t sin2 = ph.GetSinW2(); const Double_t cost = TMath::Sqrt(1-sin2); const Double_t theta = TMath::ACos(cost); // Path from production height to obslevel const Double_t z = height-fObsLevel; // Distance of emission point to incident point on ground const Double_t d = z/cost; // Avoid problems if photon is very close to telescope: if (TMath::Abs(d)<1) return 1; // Earth radius plus observation height (distance of telescope // from earth center) const Double_t H = R() + fObsLevel; // We calculate h, the true height a.s.l. // of the photon emission point in cm const Double_t h = TMath::Sqrt(H*H + d*d + 2*H*z) - R(); //**** Rayleigh scattering: ***** const Double_t T_Ray = CalcTransmission(h, wavelength, sin2); if (T_Ray<0) return 0; //****** Ozone absorption: ****** const Double_t T_Oz = CalcOzoneAbsorption(h, wavelength, theta); //******** Mie (aerosol) ******** const Double_t T_Mie = CalcAerosolAbsorption(h, wavelength, theta); // FIXME: What if I wanna display these values? // Calculate final transmission coefficient return T_Ray * T_Oz * T_Mie; } }; const Double_t MAtmosphere::STEPTHETA = 1.74533e-2; // aprox. 1 degree const Double_t MAtmRayleigh::fgMeanFreePath = 2970; const 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}; const 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}; // ========================================================================== // -------------------------------------------------------------------------- // // Default Constructor. // MSimAtmosphere::MSimAtmosphere(const char* name, const char *title) : fRunHeader(0), fEvt(0), fAtmosphere(0), fFileAerosols("resmc/atmosphere-aerosols.txt"), fFileOzone("resmc/atmosphere-ozone.txt"), fForce(kFALSE) { fName = name ? name : "MSimAtmosphere"; fTitle = title ? title : "Simulate the wavelength and height-dependant atmpsheric absorption"; fAtmosphere = new MAtmosphere; } // -------------------------------------------------------------------------- // // Calls Clear() // MSimAtmosphere::~MSimAtmosphere() { delete fAtmosphere; } // -------------------------------------------------------------------------- // // Search for the needed parameter containers. Read spline from file // calling ReadFile(); // Int_t MSimAtmosphere::PreProcess(MParList *pList) { fEvt = (MPhotonEvent*)pList->FindObject("MPhotonEvent"); if (!fEvt) { *fLog << err << "MPhotonEvent not found... aborting." << endl; return kFALSE; } return kTRUE; } // -------------------------------------------------------------------------- // Bool_t MSimAtmosphere::ReInit(MParList *pList) { fRunHeader = (MCorsikaRunHeader*)pList->FindObject("MCorsikaRunHeader"); if (!fRunHeader) { *fLog << err << "MCorsikaRunHeader not found... aborting." << endl; return kFALSE; } if (fRunHeader->Has(MCorsikaRunHeader::kCeffic) && !fForce) { *fLog << inf << "CEFFIC enabled... task will be skipped." << endl; return kTRUE; } //if (fRunHeader->Has(MCorsikaRunHeader::kRefraction)) // *fLog << inf << "Atmospheric refraction already applied in Corsika... skipping our own." << endl; // FIXME: Check wavelength range /* if (h->GetWavelengthMin()GetXmin()) *fLog << warn << "WARNING - Lower bound of wavelength bandwidth exceeds lower bound of spline." << endl; if (h->GetWavelengthMax()>fSpline->GetXmax()) *fLog << warn << "WARNING - Upper bound of wavelength bandwidth exceeds upper bound of spline." << endl; */ fAtmosphere->Init(*fRunHeader, fFileOzone, fFileAerosols); if (!fAtmosphere->IsAllValid()) { *fLog << err << "ERROR - Something with the atmoshere's initialization went wrong!" << endl; return kFALSE; } if (fRunHeader->GetWavelengthMin()GetWavelengthMin()) *fLog << warn << "WARNING - Lower bound of wavelength bandwidth exceeds valid range of atmosphere." << endl; if (fRunHeader->GetWavelengthMax()>fAtmosphere->GetWavelengthMax()) *fLog << warn << "WARNING - Lower bound of wavelength bandwidth exceeds valid range of atmosphere." << endl; if (!fRunHeader->Has(MCorsikaRunHeader::kAtmext)) *fLog << warn << "WARNING - ATMEXT option not used for Corsika data." << endl; if (!fRunHeader->Has(MCorsikaRunHeader::kRefraction)) *fLog << warn << "WARNING - Refraction calculation disabled for Corsika data." << endl; return kTRUE; } // -------------------------------------------------------------------------- // Int_t MSimAtmosphere::Process() { // Skip the task if the CEFFIC option has been enabled and // its excution has not been forced by the user if (!fForce && fRunHeader->Has(MCorsikaRunHeader::kCeffic)) return kTRUE; // Get the number of photons in the list const Int_t num = fEvt->GetNumPhotons(); // FIMXE: Add checks for // * upgoing particles // * Can we take the full length until the camera into account? // Counter for number of total and final events Int_t cnt = 0; for (Int_t i=0; iGetTransmission(ph); // Get a random value between 0 and 1 to determine whether the photon will survive // gRandom->Rndm() = [0;1[ if (gRandom->Rndm()>=eff) continue; // Copy the surviving events bakc in the list (*fEvt)[cnt++] = ph; } // Now we shrink the array to the number of new entries. fEvt->Shrink(cnt); return kTRUE; } /* Int_t MSimWavelength::Process() { // Get the number of photons in the list const Int_t num = fEvt->GetNumPhotons(); // FIMXE: Add checks for // * upgoing particles // * wavelength range // * check if corsika atmosphere is switched on // * Can we take the full length until the camera into account? // Counter for number of total and final events Int_t cnt = 0; for (Int_t i=0; iGetWavelengthMin(); // WAVLGL const Double_t max = fRunHeader->GetWavelengthMax(); // WAVLGU const Double_t f = (max-min)/max; // WAVELENGTH = 1. / (1/min - RD(1)/(min*max/(max-min))) ph.SetWavelength(TMath::Nint(min / (1. - gRandom->Rndm()*f))); } return kTRUE; } */ // -------------------------------------------------------------------------- // // FileAerosols: resmc/atmosphere-aerosols.txt // FileOzone: resmc/atmosphere-ozone.txt // Int_t MSimAtmosphere::ReadEnv(const TEnv &env, TString prefix, Bool_t print) { Bool_t rc = kFALSE; if (IsEnvDefined(env, prefix, "FileAerosols", print)) { rc = kTRUE; fFileAerosols = GetEnvValue(env, prefix, "FileAerosols", fFileAerosols); } if (IsEnvDefined(env, prefix, "FileOzone", print)) { rc = kTRUE; fFileOzone = GetEnvValue(env, prefix, "FileOzone", fFileOzone); } if (IsEnvDefined(env, prefix, "Force", print)) { rc = kTRUE; fForce = GetEnvValue(env, prefix, "Force", fForce); } return rc; }