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MuonBremsstrahlung.cc
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6 
7 #include <cmath>
8 #include <memory>
9 
10 #include <Math/RotationY.h>
11 #include <Math/RotationZ.h>
12 
17 
18 #include <TMath.h>
19 #include <TF1.h>
20 
22 // Authors: Sandro Fonseca de Souza and Andre Sznajder (UERJ/Brazil)
23 // Date: 23-Nov-2010
24 //
25 // Revision: Class structure modified to match SimplifiedGeometryPropagator
26 // S. Sekmen, 18 May 2017
27 //
28 // Revision: Code very buggy, PetrukhinFunc return negative values, double bremProba wasn't properly defined etc.
29 // Should be all fixed by now
30 // S. Kurz, 23 May 2017
32 
33 namespace fastsim {
35 
40  public:
43 
45  ~MuonBremsstrahlung() override { ; };
46 
48 
54  void interact(Particle &particle,
55  const SimplifiedGeometry &layer,
56  std::vector<std::unique_ptr<Particle> > &secondaries,
57  const RandomEngineAndDistribution &random) override;
58 
59  private:
61 
67  math::XYZTLorentzVector brem(Particle &particle, double xmin, const RandomEngineAndDistribution &random) const;
68 
70 
77  double gbteth(const double ener,
78  const double partm,
79  const double efrac,
80  const RandomEngineAndDistribution &random) const;
81 
83  static double PetrukhinFunc(double *x, double *p);
84 
85  TF1 *Petrfunc;
88  double density_;
89  double radLenInCm_;
90  double A_;
91  double Z_;
92  };
93 } // namespace fastsim
94 
97  // Set the minimal photon energy for a Brem from mu+/-
98  minPhotonEnergy_ = cfg.getParameter<double>("minPhotonEnergy");
99  minPhotonEnergyFraction_ = cfg.getParameter<double>("minPhotonEnergyFraction");
100  // Material properties
101  A_ = cfg.getParameter<double>("A");
102  Z_ = cfg.getParameter<double>("Z");
103  density_ = cfg.getParameter<double>("density");
104  radLenInCm_ = cfg.getParameter<double>("radLen");
105 }
106 
108  const SimplifiedGeometry &layer,
109  std::vector<std::unique_ptr<fastsim::Particle> > &secondaries,
110  const RandomEngineAndDistribution &random) {
111  // only consider muons
112  if (std::abs(particle.pdgId()) != 13) {
113  return;
114  }
115 
116  double radLengths = layer.getThickness(particle.position(), particle.momentum());
117  //
118  // no material
119  //
120  if (radLengths < 1E-10) {
121  return;
122  }
123 
124  // Protection : Just stop the electron if more than 1 radiation lengths.
125  // This case corresponds to an electron entering the layer parallel to
126  // the layer axis - no reliable simulation can be done in that case...
127  if (radLengths > 4.) {
128  particle.momentum().SetXYZT(0., 0., 0., 0.);
129  return;
130  }
131 
132  // muon must have more energy than minimum photon energy
133  if (particle.momentum().E() - particle.momentum().mass() < minPhotonEnergy_) {
134  return;
135  }
136 
137  // Min fraction of muon's energy transferred to the photon
138  double xmin = std::max(minPhotonEnergy_ / particle.momentum().E(), minPhotonEnergyFraction_);
139  // Hard brem probability with a photon Energy above threshold.
140  if (xmin >= 1. || xmin <= 0.) {
141  return;
142  }
143 
144  // Max fraction of muon's energy transferred to the photon
145  double xmax = 1.;
146 
147  // create TF1 using a free C function
148  Petrfunc = new TF1("Petrfunc", PetrukhinFunc, xmin, xmax, 3);
149  // Setting parameters
150  Petrfunc->SetParameters(particle.momentum().E(), A_, Z_);
151  // d = distance for several materials
152  // X0 = radLen
153  // d = radLengths * X0 (for tracker, yoke, ECAL and HCAL)
154  double distance = radLengths * radLenInCm_;
155 
156  // Integration
157  // Fixed previous version which used Petrfunc->Integral(0.,1.) -> does not make sense
158  double bremProba = density_ * distance * (fastsim::Constants::NA / A_) * (Petrfunc->Integral(xmin, xmax));
159  if (bremProba < 1E-10) {
160  return;
161  }
162 
163  // Number of photons to be radiated.
164  unsigned int nPhotons = random.poissonShoot(bremProba);
165  if (nPhotons == 0) {
166  return;
167  }
168 
169  //Rotate to the lab frame
170  double theta = particle.momentum().Theta();
171  double phi = particle.momentum().Phi();
172 
173  // Energy of these photons
174  for (unsigned int i = 0; i < nPhotons; ++i) {
175  // Throw momentum of the photon
176  math::XYZTLorentzVector photonMom = brem(particle, xmin, random);
177 
178  // Check that there is enough energy left.
179  if (particle.momentum().E() - particle.momentum().mass() < photonMom.E())
180  break;
181 
182  // Rotate to the lab frame
183  photonMom = ROOT::Math::RotationZ(phi) * (ROOT::Math::RotationY(theta) * photonMom);
184 
185  // Add a photon
186  secondaries.emplace_back(new fastsim::Particle(22, particle.position(), photonMom));
187 
188  // Update the original e+/-
189  particle.momentum() -= photonMom;
190  }
191 }
192 
194  double xmin,
195  const RandomEngineAndDistribution &random) const {
196  // This is a simple version of a Muon Brem using Petrukhin model.
197  // Ref: http://pdg.lbl.gov/2008/AtomicNuclearProperties/adndt.pdf
198  double xp = Petrfunc->GetRandom();
199 
200  // Have photon energy. Now generate angles with respect to the z axis
201  // defined by the incoming particle's momentum.
202 
203  // Isotropic in phi
204  const double phi = random.flatShoot() * 2. * M_PI;
205  // theta from universal distribution
206  const double theta = gbteth(particle.momentum().E(), fastsim::Constants::muMass, xp, random) *
207  fastsim::Constants::muMass / particle.momentum().E();
208 
209  // Make momentum components
210  double stheta = std::sin(theta);
211  double ctheta = std::cos(theta);
212  double sphi = std::sin(phi);
213  double cphi = std::cos(phi);
214 
215  return xp * particle.momentum().E() * math::XYZTLorentzVector(stheta * cphi, stheta * sphi, ctheta, 1.);
216 }
217 
218 double fastsim::MuonBremsstrahlung::gbteth(const double ener,
219  const double partm,
220  const double efrac,
221  const RandomEngineAndDistribution &random) const {
222  // Details on implementation here
223  // http://www.dnp.fmph.uniba.sk/cernlib/asdoc/geant_html3/node299.html#GBTETH
224  // http://svn.cern.ch/guest/AliRoot/tags/v3-07-03/GEANT321/gphys/gbteth.F
225 
226  const double alfa = 0.625;
227 
228  const double d = 0.13 * (0.8 + 1.3 / Z_) * (100.0 + (1.0 / ener)) * (1.0 + efrac);
229  const double w1 = 9.0 / (9.0 + d);
230  const double umax = ener * M_PI / partm;
231  double u;
232 
233  do {
234  double beta = (random.flatShoot() <= w1) ? alfa : 3.0 * alfa;
235  u = -std::log(random.flatShoot() * random.flatShoot()) / beta;
236  } while (u >= umax);
237 
238  return u;
239 }
240 
241 double fastsim::MuonBremsstrahlung::PetrukhinFunc(double *x, double *p) {
242  // Function independent variable
243  double nu = x[0]; // fraction of muon's energy transferred to the photon
244 
245  // Parameters
246  double E = p[0]; // Muon Energy (in GeV)
247  double A = p[1]; // Atomic weight
248  double Z = p[2]; // Atomic number
249 
250  /*
252  // Function of Muom Brem using nuclear screening correction
253  // Ref: http://pdg.lbl.gov/2008/AtomicNuclearProperties/adndt.pdf
254  // http://geant4.cern.ch/G4UsersDocuments/UsersGuides/PhysicsReferenceManual/html/node48.html
255 
256  // Physical constants
257  double B = 182.7;
258  double ee = sqrt(2.7181) ; // sqrt(e)
259  double ZZ= pow( Z,-1./3.); // Z^-1/3
261  double emass = 0.0005109990615; // electron mass (GeV/c^2)
262  double mumass = 0.105658367;//mu mass (GeV/c^2)
263 
264  double re = 2.817940285e-13;// Classical electron radius (Units: cm)
265  double alpha = 1./137.03599976; // fine structure constant
266  double Dn = 1.54* (pow(A,0.27));
267  double constant = pow((2.0 * Z * emass/mumass * re ),2.0);
269 
270  double delta = (mumass * mumass * nu) /(2.* E * (1.- nu));
271 
272  double Delta_n = TMath::Log(Dn / (1.+ delta *( Dn * ee -2.)/ mumass)); //nuclear screening correction
273 
274  double Phi = TMath::Log((B * mumass * ZZ / emass)/ (1.+ delta * ee * B * ZZ / emass)) - Delta_n;//phi(delta)
275 
276  // Diff. Cross Section for Muon Brem from a screened nuclear (Equation 16: REF: LBNL-44742)
277  double f = alpha * constant *(4./3.-4./3.*nu + nu*nu)*Phi/nu;
278  */
279 
281  // Function for Muon Brem Xsec from G4
283 
284  // Physical constants
285  double B = 183.;
286  double Bl = 1429.;
287  double ee = 1.64872; // sqrt(e)
288  double Z13 = pow(Z, -1. / 3.); // Z^-1/3
289  double Z23 = pow(Z, -2. / 3.); // Z^-2/3
290 
291  // Original values of paper
292  double emass = 0.0005109990615; // electron mass (GeV/c^2)
293  double mumass = 0.105658367; // muon mass (GeV/c^2)
294  // double re = 2.817940285e-13; // Classical electron radius (Units: cm)
295  double alpha = 0.00729735; // 1./137.03599976; // fine structure constant
296  double constant = 1.85736e-30; // pow( ( emass / mumass * re ) , 2.0);
297 
298  // Use nomenclature from reference -> Follow those formula step by step
299  if (nu * E >= E - mumass)
300  return 0;
301 
302  double Dn = 1.54 * (pow(A, 0.27));
303  double Dnl = pow(Dn, (1. - 1. / Z));
304 
305  double delta = (mumass * mumass * nu) / (2. * E * (1. - nu));
306 
307  double Phi_n = TMath::Log(B * Z13 * (mumass + delta * (Dnl * ee - 2)) / (Dnl * (emass + delta * ee * B * Z13)));
308  if (Phi_n < 0)
309  Phi_n = 0;
310 
311  double Phi_e =
312  TMath::Log((Bl * Z23 * mumass) / (1. + delta * mumass / (emass * emass * ee)) / (emass + delta * ee * Bl * Z23));
313  if (Phi_e < 0 || nu * E >= E / (1. + (mumass * mumass / (2. * emass * E))))
314  Phi_e = 0;
315 
316  // Diff. Cross Section for Muon Brem from G4 (without NA/A factor)
317  double f = 16. / 3. * alpha * constant * Z * (Z * Phi_n + Phi_e) * (1. / nu) * (1. - nu + 0.75 * nu * nu);
318 
319  return f;
320 }
321 
static double constexpr NA
Avogadro&#39;s number.
Definition: Constants.h:16
Implementation of a generic detector layer (base class for forward/barrel layers).
Definition: APVGainStruct.h:7
double PetrukhinFunc(double *x, double *p)
Sin< T >::type sin(const T &t)
Definition: Sin.h:22
const math::XYZTLorentzVector & position() const
Return position of the particle.
Definition: Particle.h:140
double minPhotonEnergyFraction_
Cut on minimum fraction of particle&#39;s energy which has to be carried by photon.
static double constexpr muMass
Muon mass [GeV].
Definition: Constants.h:14
double radLenInCm_
Radiation length of material (usually silicon X0=9.360)
XYZTLorentzVectorD XYZTLorentzVector
Lorentz vector with cylindrical internal representation using pseudorapidity.
Definition: LorentzVector.h:29
Base class for any interaction model between a particle and a tracker layer.
math::XYZTLorentzVector brem(Particle &particle, double xmin, const RandomEngineAndDistribution &random) const
Compute Brem photon energy and angles, if any.
double gbteth(const double ener, const double partm, const double efrac, const RandomEngineAndDistribution &random) const
A universal angular distribution.
double density_
Density of material (usually silicon rho=2.329)
Cos< T >::type cos(const T &t)
Definition: Cos.h:22
double minPhotonEnergy_
Cut on minimum energy of bremsstrahlung photons.
Implementation of Bremsstrahlung from mu+/mu- in the tracker layers based on a Petrukhin Model (nucle...
Abs< T >::type abs(const T &t)
Definition: Abs.h:22
double f[11][100]
~MuonBremsstrahlung() override
Default destructor.
TF1 * Petrfunc
The Petrukhin Function.
d
Definition: ztail.py:151
#define M_PI
int pdgId() const
Return pdgId of the particle.
Definition: Particle.h:134
static double PetrukhinFunc(double *x, double *p)
Petrukhin Function: Returns cross section using nuclear-electron screening correction from G4 style...
const math::XYZTLorentzVector & momentum() const
Return momentum of the particle.
Definition: Particle.h:143
MuonBremsstrahlung(const std::string &name, const edm::ParameterSet &cfg)
Constructor.
unsigned int poissonShoot(double mean) const
float x
void interact(Particle &particle, const SimplifiedGeometry &layer, std::vector< std::unique_ptr< Particle > > &secondaries, const RandomEngineAndDistribution &random) override
Perform the interaction.
#define DEFINE_EDM_PLUGIN(factory, type, name)
double A_
Atomic weight of material (usually silicon A=28.0855)
Definition: APVGainStruct.h:7
double Z_
Atomic number of material (usually silicon Z=14)
double flatShoot(double xmin=0.0, double xmax=1.0) const
Definition of a generic FastSim Particle which can be propagated through the detector (formerly Parti...
Definition: Particle.h:16
Geom::Theta< T > theta() const
Power< A, B >::type pow(const A &a, const B &b)
Definition: Power.h:29