Version: SMASH-2.2
spheremodus.cc
Go to the documentation of this file.
1 /*
2  *
3  * Copyright (c) 2013-2021
4  * SMASH Team
5  *
6  * GNU General Public License (GPLv3 or later)
7  *
8  */
9 
10 #include <cmath>
11 #include <cstdio>
12 #include <cstdlib>
13 #include <list>
14 #include <map>
15 #include <utility>
16 #include <vector>
17 
18 #include "smash/angles.h"
20 #include "smash/configuration.h"
21 #include "smash/constants.h"
23 #include "smash/fourvector.h"
24 #include "smash/hadgas_eos.h"
25 #include "smash/logging.h"
26 #include "smash/particles.h"
27 #include "smash/quantumsampling.h"
28 #include "smash/random.h"
29 #include "smash/spheremodus.h"
30 #include "smash/threevector.h"
31 
32 namespace smash {
33 static constexpr int LSphere = LogArea::Sphere::id;
34 
169  const ExperimentParameters &)
170  : radius_(modus_config.take({"Sphere", "Radius"})),
171  sphere_temperature_(modus_config.take({"Sphere", "Temperature"})),
172  start_time_(modus_config.take({"Sphere", "Start_Time"}, 0.)),
173  use_thermal_(
174  modus_config.take({"Sphere", "Use_Thermal_Multiplicities"}, false)),
175  mub_(modus_config.take({"Sphere", "Baryon_Chemical_Potential"}, 0.)),
176  mus_(modus_config.take({"Sphere", "Strange_Chemical_Potential"}, 0.)),
177  muq_(modus_config.take({"Sphere", "Charge_Chemical_Potential"}, 0.)),
178  account_for_resonance_widths_(
179  modus_config.take({"Sphere", "Account_Resonance_Widths"}, true)),
180  init_multipl_(use_thermal_
181  ? std::map<PdgCode, int>()
182  : modus_config.take({"Sphere", "Init_Multiplicities"})
183  .convert_for(init_multipl_)),
184  init_distr_(
185  modus_config.take({"Sphere", "Initial_Condition"},
187  radial_velocity_(
188  modus_config.take({"Sphere", "Add_Radial_Velocity"}, -1.)),
189  insert_jet_(modus_config.has_value({"Sphere", "Jet", "Jet_PDG"})),
190  jet_pdg_(insert_jet_ ? modus_config.take({"Sphere", "Jet", "Jet_PDG"})
191  .convert_for(jet_pdg_)
192  : pdg::p), // dummy default; never used
193  jet_mom_(modus_config.take({"Sphere", "Jet", "Jet_Momentum"}, 20.)) {}
194 
195 /* console output on startup of sphere specific parameters */
196 std::ostream &operator<<(std::ostream &out, const SphereModus &m) {
197  out << "-- Sphere Modus:\nRadius of the sphere: " << m.radius_ << " fm\n";
198  if (m.use_thermal_) {
199  out << "Thermal multiplicities (T = " << m.sphere_temperature_
200  << " GeV, muB = " << m.mub_ << " GeV, muS = " << m.mus_
201  << " GeV, muQ = " << m.muq_ << " GeV)\n";
202  } else {
203  for (const auto &p : m.init_multipl_) {
204  ParticleTypePtr ptype = &ParticleType::find(p.first);
205  out << ptype->name() << " initial multiplicity " << p.second << '\n';
206  }
207  }
208  switch (m.init_distr_) {
210  out << "Boltzmann momentum distribution with T = "
211  << m.sphere_temperature_ << " GeV.\n";
212  break;
214  out << "Fermi/Bose momentum distribution with T = "
215  << m.sphere_temperature_ << " GeV.\n";
216  break;
218  out << "Sphere Initial Condition is IC_ES";
219  break;
221  out << "Sphere Initial Condition is IC_1M";
222  break;
224  out << "Sphere Initial Condition is IC_2M";
225  break;
227  out << "Sphere Initial Condition is IC_Massive";
228  break;
229  }
230  if (m.insert_jet_) {
232  out << "Adding a " << ptype->name() << " as a jet in the middle "
233  << "of the sphere with " << m.jet_mom_ << " GeV initial momentum.\n";
234  }
235  return out;
236 }
237 
238 /* initial_conditions - sets particle data for @particles */
240  const ExperimentParameters &parameters) {
241  FourVector momentum_total(0, 0, 0, 0);
242  const double T = this->sphere_temperature_;
243  const double V = 4.0 / 3.0 * M_PI * radius_ * radius_ * radius_;
244  /* Create NUMBER OF PARTICLES according to configuration */
245  if (use_thermal_) {
246  if (average_multipl_.empty()) {
247  for (const ParticleType &ptype : ParticleType::list_all()) {
248  if (HadronGasEos::is_eos_particle(ptype)) {
249  const double n = HadronGasEos::partial_density(
251  average_multipl_[ptype.pdgcode()] = n * V * parameters.testparticles;
252  }
253  }
254  }
255  double nb_init = 0.0, ns_init = 0.0, nq_init = 0.0;
256  for (const auto &mult : average_multipl_) {
257  const int thermal_mult_int = random::poisson(mult.second);
258  particles->create(thermal_mult_int, mult.first);
259  nb_init += mult.second * mult.first.baryon_number();
260  ns_init += mult.second * mult.first.strangeness();
261  nq_init += mult.second * mult.first.charge();
262  logg[LSphere].debug(mult.first, " initial multiplicity ",
263  thermal_mult_int);
264  }
265  logg[LSphere].info("Initial hadron gas baryon density ", nb_init);
266  logg[LSphere].info("Initial hadron gas strange density ", ns_init);
267  logg[LSphere].info("Initial hadron gas charge density ", nq_init);
268  } else {
269  for (const auto &p : init_multipl_) {
270  particles->create(p.second * parameters.testparticles, p.first);
271  logg[LSphere].debug("Particle ", p.first, " initial multiplicity ",
272  p.second);
273  }
274  }
275  std::unique_ptr<QuantumSampling> quantum_sampling;
277  quantum_sampling = make_unique<QuantumSampling>(init_multipl_, V, T);
278  }
279  /* loop over particle data to fill in momentum and position information */
280  for (ParticleData &data : *particles) {
281  Angles phitheta;
282  /* thermal momentum according Maxwell-Boltzmann distribution */
283  double momentum_radial = 0.0, mass = data.pole_mass();
284  /* assign momentum_radial according to requested distribution */
285  switch (init_distr_) {
287  momentum_radial = sample_momenta_IC_ES(T);
288  break;
290  momentum_radial = sample_momenta_1M_IC(T, mass);
291  break;
293  momentum_radial = sample_momenta_2M_IC(T, mass);
294  break;
296  momentum_radial = sample_momenta_non_eq_mass(T, mass);
297  break;
299  default:
301  ? data.type().mass()
302  : HadronGasEos::sample_mass_thermal(data.type(), 1.0 / T);
303  momentum_radial = sample_momenta_from_thermal(T, mass);
304  break;
306  /*
307  * **********************************************************************
308  * Sampling the thermal momentum according Bose/Fermi/Boltzmann
309  * distribution.
310  * We take the pole mass as the mass.
311  * **********************************************************************
312  */
313  mass = data.type().mass();
314  momentum_radial = quantum_sampling->sample(data.pdgcode());
315  break;
316  }
317  phitheta.distribute_isotropically();
318  logg[LSphere].debug(data.type().name(), "(id ", data.id(),
319  ") radial momentum ", momentum_radial, ", direction",
320  phitheta);
321  data.set_4momentum(mass, phitheta.threevec() * momentum_radial);
322  momentum_total += data.momentum();
323  /* uniform sampling in a sphere with radius r */
324  double position_radial;
325  position_radial = std::cbrt(random::canonical()) * radius_;
326  Angles pos_phitheta;
327  pos_phitheta.distribute_isotropically();
328  data.set_4position(
329  FourVector(start_time_, pos_phitheta.threevec() * position_radial));
330  data.set_formation_time(start_time_);
331  }
332 
333  /* boost in radial direction with an underlying velocity field of the form u_r
334  * = u_0 * r / R */
335  if (radial_velocity_ > 0.0) {
336  if (radial_velocity_ > 1.0) {
337  throw std::invalid_argument(
338  "Additional velocity cannot be greater than 1!");
339  }
340  for (ParticleData &data : *particles) {
341  double particle_radius = std::sqrt(data.position().sqr3());
342  auto e_r = data.position().threevec() / particle_radius;
343  auto radial_velocity = radial_velocity_ * e_r * particle_radius / radius_;
344  data.set_4momentum(data.momentum().lorentz_boost(radial_velocity));
345  momentum_total += data.momentum();
346  }
347  }
348 
349  /* Make total 3-momentum 0 */
350  for (ParticleData &data : *particles) {
351  data.set_4momentum(data.momentum().abs(),
352  data.momentum().threevec() -
353  momentum_total.threevec() / particles->size());
354  }
355 
356  /* Add a single highly energetic particle in the center of the sphere (jet) */
357  if (insert_jet_) {
358  auto &jet_particle = particles->create(jet_pdg_);
359  jet_particle.set_formation_time(start_time_);
360  jet_particle.set_4position(FourVector(start_time_, 0., 0., 0.));
361  jet_particle.set_4momentum(ParticleType::find(jet_pdg_).mass(),
362  ThreeVector(jet_mom_, 0., 0.));
363  }
364 
365  /* Recalculate total momentum */
366  momentum_total = FourVector(0, 0, 0, 0);
367  for (ParticleData &data : *particles) {
368  momentum_total += data.momentum();
369  /* IC: debug checks */
370  logg[LSphere].debug() << data;
371  }
372  /* allows to check energy conservation */
373  logg[LSphere].debug() << "Sphere initial total 4-momentum [GeV]: "
374  << momentum_total;
375  return start_time_;
376 }
377 } // namespace smash
Angles provides a common interface for generating directions: i.e., two angles that should be interpr...
Definition: angles.h:59
ThreeVector threevec() const
Definition: angles.h:268
void distribute_isotropically()
Populate the object with a new direction.
Definition: angles.h:188
Interface to the SMASH configuration files.
The FourVector class holds relevant values in Minkowski spacetime with (+, −, −, −) metric signature.
Definition: fourvector.h:33
ThreeVector threevec() const
Definition: fourvector.h:324
static double partial_density(const ParticleType &ptype, double T, double mub, double mus, double muq, bool account_for_resonance_widths=false)
Compute partial density of one hadron sort.
Definition: hadgas_eos.cc:270
static double sample_mass_thermal(const ParticleType &ptype, double beta)
Sample resonance mass in a thermal medium.
Definition: hadgas_eos.cc:385
static bool is_eos_particle(const ParticleType &ptype)
Check if a particle belongs to the EoS.
Definition: hadgas_eos.h:355
ParticleData contains the dynamic information of a certain particle.
Definition: particledata.h:58
A pointer-like interface to global references to ParticleType objects.
Definition: particletype.h:671
Particle type contains the static properties of a particle species.
Definition: particletype.h:97
static const ParticleType & find(PdgCode pdgcode)
Returns the ParticleType object for the given pdgcode.
Definition: particletype.cc:99
const std::string & name() const
Definition: particletype.h:141
static const ParticleTypeList & list_all()
Definition: particletype.cc:51
The Particles class abstracts the storage and manipulation of particles.
Definition: particles.h:33
size_t size() const
Definition: particles.h:87
void create(size_t n, PdgCode pdg)
Add n particles of the same type (pdg) to the list.
Definition: particles.cc:66
SphereModus: Provides a modus for expanding matter calculations.
Definition: spheremodus.h:47
const bool account_for_resonance_widths_
In case of thermal initialization: true – account for resonance spectral functions,...
Definition: spheremodus.h:113
const bool use_thermal_
Whether to use a thermal initialization for all particles instead of specific numbers.
Definition: spheremodus.h:92
const double muq_
Charge chemical potential for thermal initialization; only used if use_thermal_ is true.
Definition: spheremodus.h:107
double sphere_temperature_
Temperature for momentum distribution (in GeV)
Definition: spheremodus.h:85
const double start_time_
Starting time for the Sphere.
Definition: spheremodus.h:87
const bool insert_jet_
Whether to insert a single high energy particle at the center of the expanding sphere (0,...
Definition: spheremodus.h:140
const PdgCode jet_pdg_
Pdg of the particle to use as a jet; necessary if insert_jet_ is true, unused otherwise.
Definition: spheremodus.h:145
const SphereInitialCondition init_distr_
Initialization scheme for momenta in the sphere; used for expanding metric setup.
Definition: spheremodus.h:128
SphereModus(Configuration modus_config, const ExperimentParameters &parameters)
Constructor.
Definition: spheremodus.cc:168
double initial_conditions(Particles *particles, const ExperimentParameters &parameters)
Generates initial state of the particles in the system according to specified parameters: number of p...
Definition: spheremodus.cc:239
std::map< PdgCode, double > average_multipl_
Average multiplicities in case of thermal initialization.
Definition: spheremodus.h:123
const double mub_
Baryon chemical potential for thermal initialization; only used if use_thermal_ is true.
Definition: spheremodus.h:97
const double jet_mom_
Initial momentum of the jet particle; only used if insert_jet_ is true.
Definition: spheremodus.h:149
const std::map< PdgCode, int > init_multipl_
Particle multiplicities at initialization; required if use_thermal_ is false.
Definition: spheremodus.h:118
const double mus_
Strange chemical potential for thermal initialization; only used if use_thermal_ is true.
Definition: spheremodus.h:102
const double radial_velocity_
Wether to add a constant radial velocity profile to the momenta of the particles in the sphere.
Definition: spheremodus.h:134
double radius_
Sphere radius (in fm/c)
Definition: spheremodus.h:83
The ThreeVector class represents a physical three-vector with the components .
Definition: threevector.h:31
Collection of useful constants that are known at compile time.
std::ostream & operator<<(std::ostream &out, const ActionPtr &action)
Convenience: dereferences the ActionPtr to Action.
Definition: action.h:532
std::array< einhard::Logger<>, std::tuple_size< LogArea::AreaTuple >::value > logg
An array that stores all pre-configured Logger objects.
Definition: logging.cc:39
constexpr int p
Proton.
constexpr int n
Neutron.
int poisson(const T &lam)
Returns a Poisson distributed random number.
Definition: random.h:226
T canonical()
Definition: random.h:113
Definition: action.h:24
static constexpr int LSphere
Definition: spheremodus.cc:33
double sample_momenta_from_thermal(const double temperature, const double mass)
Samples a momentum from the Maxwell-Boltzmann (thermal) distribution in a faster way,...
double sample_momenta_IC_ES(const double temperature)
Sample momenta according to the momentum distribution in Bazow:2016oky .
double sample_momenta_non_eq_mass(const double temperature, const double mass)
Samples a momentum via rejection method from the non-equilibrium distribution.
double sample_momenta_1M_IC(const double temperature, const double mass)
Samples a momentum from the non-equilibrium distribution 1M_IC from Bazow:2016oky .
double sample_momenta_2M_IC(const double temperature, const double mass)
Samples a momentum from the non-equilibrium distribution 2M_IC from Bazow:2016oky .
Helper structure for Experiment.
int testparticles
Number of test-particles.