#include <bremsstrahlungaction.h>

BremsAction is a special action which takes two incoming particles and performs a perturbative scattering where a Bremsstrahlung photon is produced. The final state particles are not further propagated, only written to the photon output.

Definition at line 26 of file bremsstrahlungaction.h.

Inheritance diagram for smash::BremsstrahlungAction:

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Collaboration diagram for smash::BremsstrahlungAction:

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Public Types
enum	ReactionType { ReactionType::no_reaction, ReactionType::pi_z_pi_m, ReactionType::pi_z_pi_p, ReactionType::pi_p_pi_m, ReactionType::pi_m_pi_m, ReactionType::pi_p_pi_p, ReactionType::pi_z_pi_z }
	Enum for encoding the photon process. More...

Public Member Functions
	BremsstrahlungAction (const ParticleList &in, const double time, const int n_frac_photons, const double hadronic_cross_section_input)
	Construct a ScatterActionBrems object. More...

void	perform_bremsstrahlung (const OutputsList &outputs)
	Create the final state and write to output. More...

void	generate_final_state () override
	Generate the final-state for the Bremsstrahlung process. More...

void	sample_3body_phasespace () override
	Sample the final state anisotropically, considering the differential cross sections with respect to theta and k. More...

double	get_total_weight () const override
	Return the weight of the last created photon. More...

double	hadronic_cross_section () const
	Return the total cross section of the underlying hadronic scattering It is necessary for the weighting procedure. More...

void	add_dummy_hadronic_process (double reaction_cross_section)
	Adds one hadronic process with a given cross-section. More...

void	add_single_process ()
	Add the photonic process. More...

Public Member Functions inherited from smash::ScatterAction
	ScatterAction (const ParticleData &in_part1, const ParticleData &in_part2, double time, bool isotropic=false, double string_formation_time=1.0, double box_length=-1.0)
	Construct a ScatterAction object. More...

void	add_collision (CollisionBranchPtr p)
	Add a new collision channel. More...

void	add_collisions (CollisionBranchList pv)
	Add several new collision channels at once. More...

double	transverse_distance_sqr () const
	Calculate the transverse distance of the two incoming particles in their local rest frame. More...

double	cov_transverse_distance_sqr () const
	Calculate the transverse distance of the two incoming particles in their local rest frame written in a covariant form. More...

double	mandelstam_s () const
	Determine the Mandelstam s variable,. More...

double	relative_velocity () const
	Get the relative velocity of the two incoming particles. More...

void	generate_final_state () override
	Generate the final-state of the scattering process. More...

double	get_total_weight () const override
	Get the total cross section of scattering particles. More...

double	get_partial_weight () const override
	Get the partial cross section of the chosen channel. More...

void	sample_angles (std::pair< double, double > masses, double kinetic_energy_cm) override
	Sample final-state angles in a 2->2 collision (possibly anisotropic). More...

void	add_all_scatterings (double elastic_parameter, bool two_to_one, ReactionsBitSet included_2to2, MultiParticleReactionsBitSet included_multi, double low_snn_cut, bool strings_switch, bool use_AQM, bool strings_with_probability, NNbarTreatment nnbar_treatment, double scale_xs, double additional_el_xs)
	Add all possible scattering subprocesses for this action object. More...

const CollisionBranchList &	collision_channels ()
	Get list of possible collision channels. More...

void	set_string_interface (StringProcess *str_proc)
	Set the StringProcess object to be used. More...

virtual double	cross_section () const
	Get the total cross section of the scattering particles. More...

Public Member Functions inherited from smash::Action
	Action (const ParticleList &in_part, double time)
	Construct an action object with incoming particles and relative time. More...

	Action (const ParticleData &in_part, const ParticleData &out_part, double time, ProcessType type)
	Construct an action object with the incoming particles, relative time, and the already known outgoing particles and type of the process. More...

	Action (const ParticleList &in_part, const ParticleList &out_part, double absolute_execution_time, ProcessType type)
	Construct an action object with the incoming particles, absolute time, and the already known outgoing particles and type of the process. More...

	Action (const Action &)=delete
	Copying is disabled. Use pointers or create a new Action. More...

virtual	~Action ()
	Virtual Destructor. More...

bool	operator< (const Action &rhs) const
	Determine whether one action takes place before another in time. More...

virtual ProcessType	get_type () const
	Get the process type. More...

template<typename Branch >
void	add_process (ProcessBranchPtr< Branch > &p, ProcessBranchList< Branch > &subprocesses, double &total_weight)
	Add a new subprocess. More...

template<typename Branch >
void	add_processes (ProcessBranchList< Branch > pv, ProcessBranchList< Branch > &subprocesses, double &total_weight)
	Add several new subprocesses at once. More...

virtual void	perform (Particles *particles, uint32_t id_process)
	Actually perform the action, e.g. More...

bool	is_valid (const Particles &particles) const
	Check whether the action still applies. More...

bool	is_pauli_blocked (const Particles &particles, const PauliBlocker &p_bl) const
	Check if the action is Pauli-blocked. More...

const ParticleList &	incoming_particles () const
	Get the list of particles that go into the action. More...

void	update_incoming (const Particles &particles)
	Update the incoming particles that are stored in this action to the state they have in the global particle list. More...

const ParticleList &	outgoing_particles () const
	Get the list of particles that resulted from the action. More...

double	time_of_execution () const
	Get the time at which the action is supposed to be performed. More...

virtual void	check_conservation (const uint32_t id_process) const
	Check various conservation laws. More...

double	sqrt_s () const
	Determine the total energy in the center-of-mass frame [GeV]. More...

FourVector	total_momentum_of_outgoing_particles () const
	Calculate the total kinetic momentum of the outgoing particles. More...

FourVector	get_interaction_point () const
	Get the interaction point. More...

std::pair< FourVector, FourVector >	get_potential_at_interaction_point () const
	Get the skyrme and asymmetry potential at the interaction point. More...

void	set_stochastic_pos_idx ()
	Setter function that stores a random incoming particle index latter used to determine the interaction point. More...

Static Public Member Functions
static ReactionType	bremsstrahlung_reaction_type (const ParticleList &in)
	Determine photon process from incoming particles. More...

static bool	is_bremsstrahlung_reaction (const ParticleList &in)
	Check if particles can undergo an implemented photon process. More...

Static Public Member Functions inherited from smash::Action
static double	lambda_tilde (double a, double b, double c)
	Little helper function that calculates the lambda function (sometimes written with a tilde to better distinguish it) that appears e.g. More...

Private Member Functions
void	create_interpolations ()
	Create interpolation objects for tabularized cross sections: total cross section, differential dSigma/dk, differential dSigma/dtheta. More...

CollisionBranchList	brems_cross_sections ()
	Computes the total cross section of the bremsstrahlung process. More...

std::pair< double, double >	brems_diff_cross_sections ()
	Computes the differential cross sections dSigma/dk and dSigma/dtheta of the bremsstrahlung process. More...

Private Attributes
CollisionBranchList	collision_processes_bremsstrahlung_
	Holds the bremsstrahlung branch. More...

const ReactionType	reac_
	Reaction process as determined from incoming particles. More...

const int	number_of_fractional_photons_
	Number of photons created for each hadronic scattering, needed for correct weighting. More...

double	weight_ = 0.0
	Weight of the produced photon. More...

double	cross_section_bremsstrahlung_ = 0.0
	Total cross section of bremsstrahlung process. More...

const double	hadronic_cross_section_
	Total hadronic cross section. More...

double	k_
	Sampled value of k (photon momentum) More...

double	theta_
	Sampled value of theta (angle of the photon) More...

Additional Inherited Members
Protected Member Functions inherited from smash::ScatterAction
double	cm_momentum () const
	Get the momentum of the center of mass of the incoming particles in the calculation frame. More...

double	cm_momentum_squared () const
	Get the squared momentum of the center of mass of the incoming particles in the calculation frame. More...

ThreeVector	beta_cm () const
	Get the velocity of the center of mass of the scattering/incoming particles in the calculation frame. More...

double	gamma_cm () const
	Get the gamma factor corresponding to a boost to the center of mass frame of the colliding particles. More...

void	elastic_scattering ()
	Perform an elastic two-body scattering, i.e. just exchange momentum. More...

void	inelastic_scattering ()
	Perform an inelastic two-body scattering, i.e. new particles are formed. More...

void	two_to_three_scattering ()
	Perform a two-to-three-body scattering. More...

void	string_excitation ()
	Todo(ryu): document better - it is not really UrQMD-based, isn't it? Perform the UrQMD-based string excitation and decay. More...

void	format_debug_output (std::ostream &out) const override

Protected Member Functions inherited from smash::Action
FourVector	total_momentum () const
	Sum of 4-momenta of incoming particles. More...

template<typename Branch >
const Branch *	choose_channel (const ProcessBranchList< Branch > &subprocesses, double total_weight)
	Decide for a particular final-state channel via Monte-Carlo and return it as a ProcessBranch. More...

virtual std::pair< double, double >	sample_masses (double kinetic_energy_cm) const
	Sample final-state masses in general X->2 processes (thus also fixing the absolute c.o.m. More...

void	sample_2body_phasespace ()
	Sample the full 2-body phase-space (masses, momenta, angles) in the center-of-mass frame for the final state particles. More...

void	assign_formation_time_to_outgoing_particles ()
	Assign the formation time to the outgoing particles. More...

Protected Attributes inherited from smash::ScatterAction
CollisionBranchList	collision_channels_
	List of possible collisions. More...

double	total_cross_section_
	Total hadronic cross section. More...

double	partial_cross_section_
	Partial cross-section to the chosen outgoing channel. More...

bool	isotropic_ = false
	Do this collision isotropically? More...

double	string_formation_time_ = 1.0
	Time fragments take to be fully formed in hard string excitation. More...

Protected Attributes inherited from smash::Action
ParticleList	incoming_particles_
	List with data of incoming particles. More...

ParticleList	outgoing_particles_
	Initially this stores only the PDG codes of final-state particles. More...

const double	time_of_execution_
	Time at which the action is supposed to be performed (absolute time in the lab frame in fm/c). More...

ProcessType	process_type_
	type of process More...

double	box_length_ = -1.0
	Box length: needed to determine coordinates of collision correctly in case of collision through the wall. More...

int	stochastic_position_idx_ = -1
	This stores a randomly-chosen index to an incoming particle. More...

Member Enumeration Documentation

◆ ReactionType

enum smash::BremsstrahlungAction::ReactionType

strong

Enum for encoding the photon process.

It is uniquely determined by the incoming particles. The naming scheme is : Incoming_1_Incoming_2_.

Enumerator
no_reaction
pi_z_pi_m
pi_z_pi_p
pi_p_pi_m
pi_m_pi_m
pi_p_pi_p
pi_z_pi_z

Definition at line 105 of file bremsstrahlungaction.h.

                           {
     no_reaction,
     pi_z_pi_m,
     pi_z_pi_p,
     pi_p_pi_m,
     pi_m_pi_m,
     pi_p_pi_p,
     pi_z_pi_z
   };

Constructor & Destructor Documentation

◆ BremsstrahlungAction()

smash::BremsstrahlungAction::BremsstrahlungAction	(	const ParticleList &	in,
		const double	time,
		const int	n_frac_photons,
		const double	hadronic_cross_section_input
	)

Construct a ScatterActionBrems object.

Parameters

[in]	in	ParticleList of incoming particles.
[in]	time	Time relative to underlying hadronic action.
[in]	n_frac_photons	Number of photons to produce for each hadronic scattering.
[in]	hadronic_cross_section_input	Cross-section of underlying hadronic cross-section.

Returns: The constructed object.

Definition at line 18 of file bremsstrahlungaction.cc.

     : ScatterAction(in[0], in[1], time),
       reac_(bremsstrahlung_reaction_type(in)),
       number_of_fractional_photons_(n_frac_photons),
       hadronic_cross_section_(hadronic_cross_section_input) {}

Member Function Documentation

◆ perform_bremsstrahlung()

void smash::BremsstrahlungAction::perform_bremsstrahlung ( const OutputsList & outputs )

Create the final state and write to output.

Parameters

[in] outputs List of all outputs. Does not have to be a specific photon output, the function will take care of this.

Definition at line 62 of file bremsstrahlungaction.cc.

                                                                             {
   for (int i = 0; i < number_of_fractional_photons_; i++) {
     generate_final_state();
     for (const auto &output : outputs) {
       if (output->is_photon_output()) {
         // we do not care about the local density
         output->at_interaction(*this, 0.0);
       }
     }
   }
 }

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◆ generate_final_state()

void smash::BremsstrahlungAction::generate_final_state ( )

overridevirtual

Generate the final-state for the Bremsstrahlung process.

Generates only 3-body final state.

Implements smash::Action.

Definition at line 74 of file bremsstrahlungaction.cc.

                                                 {
   // we have only one reaction per incoming particle pair
   if (collision_processes_bremsstrahlung_.size() != 1) {
     logg[LScatterAction].fatal()
         << "Problem in BremsstrahlungAction::generate_final_state().\nThe "
            "brocess branch has "
         << collision_processes_bremsstrahlung_.size()
         << " entries. It should however have 1.";
     throw std::runtime_error("");
   }
  
   auto *proc = collision_processes_bremsstrahlung_[0].get();
  
   outgoing_particles_ = proc->particle_list();
   process_type_ = proc->get_type();
   FourVector interaction_point = get_interaction_point();
  
   // Sample k and theta:
   // minimum cutoff for k to be in accordance with cross section calculations
   double delta_k;  // k-range
   double k_min = 0.001;
   double k_max =
       (sqrt_s() * sqrt_s() - 2 * outgoing_particles_[0].type().mass() * 2 *
                                  outgoing_particles_[1].type().mass()) /
       (2 * sqrt_s());
  
   if ((k_max - k_min) < 0.0) {
     // Make sure it is kinematically even possible to create a photon that is
     // in accordance with the cross section cutoff
     k_ = 0.0;
     delta_k = 0.0;
   } else {
     k_ = random::uniform(k_min, k_max);
     delta_k = (k_max - k_min);
   }
   theta_ = random::uniform(0.0, M_PI);
  
   // Sample the phase space anisotropically in the local rest frame
   sample_3body_phasespace();
  
   // Get differential cross sections
   std::pair<double, double> diff_xs_pair = brems_diff_cross_sections();
   double diff_xs_k = diff_xs_pair.first;
   double diff_xs_theta = diff_xs_pair.second;
  
   // Assign weighting factor
   const double W_theta = diff_xs_theta * (M_PI - 0.0);
   const double W_k = diff_xs_k * delta_k;
   weight_ = std::sqrt(W_theta * W_k) /
             (number_of_fractional_photons_ * hadronic_cross_section());
  
   // Scale weight by cross section scaling factor of incoming particles
   weight_ *= incoming_particles_[0].xsec_scaling_factor() *
              incoming_particles_[1].xsec_scaling_factor();
  
   // Set position and formation time and boost back to computational frame
   for (auto &new_particle : outgoing_particles_) {
     // assuming decaying particles are always fully formed
     new_particle.set_formation_time(time_of_execution_);
     new_particle.set_4position(interaction_point);
     new_particle.boost_momentum(
         -total_momentum_of_outgoing_particles().velocity());
   }
  
   // Photons are not really part of the normal processes, so we have to set a
   // constant arbitrary number.
   const auto id_process = ID_PROCESS_PHOTON;
   Action::check_conservation(id_process);
 }

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◆ sample_3body_phasespace()

void smash::BremsstrahlungAction::sample_3body_phasespace ( )

overridevirtual

Sample the final state anisotropically, considering the differential cross sections with respect to theta and k.

Reimplemented from smash::Action.

Definition at line 144 of file bremsstrahlungaction.cc.

                                                    {
   assert(outgoing_particles_.size() == 3);
   const double m_a = outgoing_particles_[0].type().mass(),
                m_b = outgoing_particles_[1].type().mass(),
                m_c = outgoing_particles_[2].type().mass();
   const double sqrts = sqrt_s();
   const double E_ab = sqrts - m_c - k_;  // Ekin of the pion pair in cm frame
   const double pcm = pCM(sqrts, E_ab, m_c);  // cm momentum of (π pair - photon)
   const double pcm_pions = pCM(E_ab, m_a, m_b);  // cm momentum within pion pair
  
   // Photon angle: Phi random, theta from theta_ sampled above
   const Angles phitheta_photon(random::uniform(0.0, twopi), std::cos(theta_));
   outgoing_particles_[2].set_4momentum(m_c, pcm * phitheta_photon.threevec());
   // Boost velocity to cm frame of the two pions
   const ThreeVector beta_cm_pion_pair_photon =
       pcm * phitheta_photon.threevec() / std::sqrt(pcm * pcm + E_ab * E_ab);
  
   // Sample pion pair isotropically
   Angles phitheta;
   phitheta.distribute_isotropically();
   outgoing_particles_[0].set_4momentum(m_a, pcm_pions * phitheta.threevec());
   outgoing_particles_[1].set_4momentum(m_b, -pcm_pions * phitheta.threevec());
   outgoing_particles_[0].boost_momentum(beta_cm_pion_pair_photon);
   outgoing_particles_[1].boost_momentum(beta_cm_pion_pair_photon);
 }

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◆ get_total_weight()

double smash::BremsstrahlungAction::get_total_weight ( ) const

inlineoverridevirtual

Return the weight of the last created photon.

Returns: The total weight.

Implements smash::Action.

Definition at line 68 of file bremsstrahlungaction.h.

68 { return weight_; }

◆ hadronic_cross_section()

double smash::BremsstrahlungAction::hadronic_cross_section ( ) const

inline

Return the total cross section of the underlying hadronic scattering It is necessary for the weighting procedure.

Returns: total cross-section [mb]

Definition at line 76 of file bremsstrahlungaction.h.

76 { return hadronic_cross_section_; }

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◆ add_dummy_hadronic_process()

void smash::BremsstrahlungAction::add_dummy_hadronic_process ( double reaction_cross_section )

Adds one hadronic process with a given cross-section.

The intended use is to add the hadronic cross-section from the already performed hadronic action without recomputing it.

Parameters

[in] reaction_cross_section Total cross-section of underlying hadronic process [mb]

Definition at line 170 of file bremsstrahlungaction.cc.

                                    {
   CollisionBranchPtr dummy_process = make_unique<CollisionBranch>(
       incoming_particles_[0].type(), incoming_particles_[1].type(),
       reaction_cross_section, ProcessType::Bremsstrahlung);
   add_collision(std::move(dummy_process));
 }

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◆ add_single_process()

void smash::BremsstrahlungAction::add_single_process ( )

inline

Add the photonic process.

Also compute the total cross section as a side effect.

Definition at line 94 of file bremsstrahlungaction.h.

                             {
     add_processes<CollisionBranch>(brems_cross_sections(),
                                    collision_processes_bremsstrahlung_,
                                    cross_section_bremsstrahlung_);
   }

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◆ bremsstrahlung_reaction_type()

BremsstrahlungAction::ReactionType smash::BremsstrahlungAction::bremsstrahlung_reaction_type ( const ParticleList & in )

static

Determine photon process from incoming particles.

If incoming particles are not part of any implemented photonic process, return no_reaction.

Parameters

[in] in ParticleList of incoming particles.

Returns: ReactionType enum-member

Definition at line 27 of file bremsstrahlungaction.cc.

                                                                          {
   if (in.size() != 2) {
     return ReactionType::no_reaction;
   }
  
   PdgCode a = in[0].pdgcode();
   PdgCode b = in[1].pdgcode();
  
   switch (pack(a.code(), b.code())) {
     case (pack(pdg::pi_z, pdg::pi_m)):
     case (pack(pdg::pi_m, pdg::pi_z)):
       return ReactionType::pi_z_pi_m;
  
     case (pack(pdg::pi_z, pdg::pi_p)):
     case (pack(pdg::pi_p, pdg::pi_z)):
       return ReactionType::pi_z_pi_p;
  
     case (pack(pdg::pi_m, pdg::pi_p)):
     case (pack(pdg::pi_p, pdg::pi_m)):
       return ReactionType::pi_p_pi_m;
  
     case (pack(pdg::pi_m, pdg::pi_m)):
       return ReactionType::pi_m_pi_m;
  
     case (pack(pdg::pi_p, pdg::pi_p)):
       return ReactionType::pi_p_pi_p;
  
     case (pack(pdg::pi_z, pdg::pi_z)):
       return ReactionType::pi_z_pi_z;
  
     default:
       return ReactionType::no_reaction;
   }
 }

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◆ is_bremsstrahlung_reaction()

static bool smash::BremsstrahlungAction::is_bremsstrahlung_reaction ( const ParticleList & in )

inlinestatic

Check if particles can undergo an implemented photon process.

This function does not check the involved kinematics.

Parameters

[in] in ParticleList of incoming particles.

Returns: bool if photon reaction implemented.

Definition at line 134 of file bremsstrahlungaction.h.

                                                                  {
     return bremsstrahlung_reaction_type(in) != ReactionType::no_reaction;
   }

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◆ create_interpolations()

void smash::BremsstrahlungAction::create_interpolations ( )

private

Create interpolation objects for tabularized cross sections: total cross section, differential dSigma/dk, differential dSigma/dtheta.

Definition at line 319 of file bremsstrahlungaction.cc.

                                                  {
   // Read in tabularized values for sqrt(s), k and theta
   std::vector<double> sqrts = BREMS_SQRTS;
   std::vector<double> photon_momentum = BREMS_K;
   std::vector<double> photon_angle = BREMS_THETA;
  
   // Read in tabularized total cross sections
   std::vector<double> sigma_pipi_pipi_opp = BREMS_PIPI_PIPI_OPP_SIG;
   std::vector<double> sigma_pipi_pipi_same = BREMS_PIPI_PIPI_SAME_SIG;
   std::vector<double> sigma_pipi0_pipi0 = BREMS_PIPI0_PIPI0_SIG;
   std::vector<double> sigma_pipi_pi0pi0 = BREMS_PIPI_PI0PI0_SIG;
   std::vector<double> sigma_pi0pi0_pipi = BREMS_PI0PI0_PIPI_SIG;
  
   // Read in tabularized differential cross sections dSigma/dk
   std::vector<double> dsigma_dk_pipi_pipi_opp = BREMS_PIPI_PIPI_OPP_DIFF_SIG_K;
   std::vector<double> dsigma_dk_pipi_pipi_same =
       BREMS_PIPI_PIPI_SAME_DIFF_SIG_K;
   std::vector<double> dsigma_dk_pipi0_pipi0 = BREMS_PIPI0_PIPI0_DIFF_SIG_K;
   std::vector<double> dsigma_dk_pipi_pi0pi0 = BREMS_PIPI_PI0PI0_DIFF_SIG_K;
   std::vector<double> dsigma_dk_pi0pi0_pipi = BREMS_PI0PI0_PIPI_DIFF_SIG_K;
  
   // Read in tabularized differential cross sections dSigma/dtheta
   std::vector<double> dsigma_dtheta_pipi_pipi_opp =
       BREMS_PIPI_PIPI_OPP_DIFF_SIG_THETA;
   std::vector<double> dsigma_dtheta_pipi_pipi_same =
       BREMS_PIPI_PIPI_SAME_DIFF_SIG_THETA;
   std::vector<double> dsigma_dtheta_pipi0_pipi0 =
       BREMS_PIPI0_PIPI0_DIFF_SIG_THETA;
   std::vector<double> dsigma_dtheta_pipi_pi0pi0 =
       BREMS_PIPI_PI0PI0_DIFF_SIG_THETA;
   std::vector<double> dsigma_dtheta_pi0pi0_pipi =
       BREMS_PI0PI0_PIPI_DIFF_SIG_THETA;
  
   // Create interpolation objects containing linear interpolations for
   // total cross sections
   pipi_pipi_opp_interpolation =
       make_unique<InterpolateDataLinear<double>>(sqrts, sigma_pipi_pipi_opp);
   pipi_pipi_same_interpolation =
       make_unique<InterpolateDataLinear<double>>(sqrts, sigma_pipi_pipi_same);
   pipi0_pipi0_interpolation =
       make_unique<InterpolateDataLinear<double>>(sqrts, sigma_pipi0_pipi0);
   pipi_pi0pi0_interpolation =
       make_unique<InterpolateDataLinear<double>>(sqrts, sigma_pipi_pi0pi0);
   pi0pi0_pipi_interpolation =
       make_unique<InterpolateDataLinear<double>>(sqrts, sigma_pi0pi0_pipi);
  
   // Create interpolation objects containing bicubic interpolations for
   // differential dSigma/dk
   pipi_pipi_opp_dsigma_dk_interpolation = make_unique<InterpolateData2DSpline>(
       photon_momentum, sqrts, dsigma_dk_pipi_pipi_opp);
   pipi_pipi_same_dsigma_dk_interpolation = make_unique<InterpolateData2DSpline>(
       photon_momentum, sqrts, dsigma_dk_pipi_pipi_same);
   pipi0_pipi0_dsigma_dk_interpolation = make_unique<InterpolateData2DSpline>(
       photon_momentum, sqrts, dsigma_dk_pipi0_pipi0);
   pipi_pi0pi0_dsigma_dk_interpolation = make_unique<InterpolateData2DSpline>(
       photon_momentum, sqrts, dsigma_dk_pipi_pi0pi0);
   pi0pi0_pipi_dsigma_dk_interpolation = make_unique<InterpolateData2DSpline>(
       photon_momentum, sqrts, dsigma_dk_pi0pi0_pipi);
  
   // Create interpolation objects containing bicubic interpolations for
   // differential dSigma/dtheta
   pipi_pipi_opp_dsigma_dtheta_interpolation =
       make_unique<InterpolateData2DSpline>(photon_angle, sqrts,
                                            dsigma_dtheta_pipi_pipi_opp);
   pipi_pipi_same_dsigma_dtheta_interpolation =
       make_unique<InterpolateData2DSpline>(photon_angle, sqrts,
                                            dsigma_dtheta_pipi_pipi_same);
   pipi0_pipi0_dsigma_dtheta_interpolation =
       make_unique<InterpolateData2DSpline>(photon_angle, sqrts,
                                            dsigma_dtheta_pipi0_pipi0);
   pipi_pi0pi0_dsigma_dtheta_interpolation =
       make_unique<InterpolateData2DSpline>(photon_angle, sqrts,
                                            dsigma_dtheta_pipi_pi0pi0);
   pi0pi0_pipi_dsigma_dtheta_interpolation =
       make_unique<InterpolateData2DSpline>(photon_angle, sqrts,
                                            dsigma_dtheta_pi0pi0_pipi);
 }

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◆ brems_cross_sections()

CollisionBranchList smash::BremsstrahlungAction::brems_cross_sections ( )

private

Computes the total cross section of the bremsstrahlung process.

Returns: List of photon reaction branches.

Definition at line 178 of file bremsstrahlungaction.cc.

                                                                {
   CollisionBranchList process_list;
   // ParticleList final_state_particles;
   static const ParticleTypePtr photon_particle =
       &ParticleType::find(pdg::photon);
   static const ParticleTypePtr pi_z_particle = &ParticleType::find(pdg::pi_z);
   static const ParticleTypePtr pi_p_particle = &ParticleType::find(pdg::pi_p);
   static const ParticleTypePtr pi_m_particle = &ParticleType::find(pdg::pi_m);
  
   // Create interpolation objects, if not yet existent; only trigger for one
   // of them as either all or none is created
   if (pi0pi0_pipi_dsigma_dtheta_interpolation == nullptr) {
     create_interpolations();
   }
  
   // Find cross section corresponding to given sqrt(s)
   double sqrts = sqrt_s();
   double xsection;
  
   if (reac_ == ReactionType::pi_p_pi_m) {
     // Here the final state is determined by the the final state provided by the
     // sampled process using Monte Carlo techniqus
  
     // In the case of two oppositely charged pions as incoming particles,
     // there are two potential final states: pi+ + pi- and pi0 + pi0
     double xsection_pipi = (*pipi_pipi_opp_interpolation)(sqrts);
     double xsection_pi0pi0 = (*pipi_pi0pi0_interpolation)(sqrts);
  
     // Prevent negative cross sections due to numerics in interpolation
     xsection_pipi = (xsection_pipi <= 0.0) ? really_small : xsection_pipi;
     xsection_pi0pi0 = (xsection_pi0pi0 <= 0.0) ? really_small : xsection_pi0pi0;
  
     // Necessary only to decide for a final state with pi+ and pi- as incoming
     // particles.
     CollisionBranchList process_list_pipi;
  
     // Add both processes to the process_list
     process_list_pipi.push_back(make_unique<CollisionBranch>(
         incoming_particles_[0].type(), incoming_particles_[1].type(),
         *photon_particle, xsection_pipi, ProcessType::Bremsstrahlung));
     process_list_pipi.push_back(make_unique<CollisionBranch>(
         *pi_z_particle, *pi_z_particle, *photon_particle, xsection_pi0pi0,
         ProcessType::Bremsstrahlung));
  
     // Decide for one of the possible final states
     double total_cross_section = xsection_pipi + xsection_pi0pi0;
     const CollisionBranch *proc =
         choose_channel<CollisionBranch>(process_list_pipi, total_cross_section);
  
     xsection = proc->weight();
  
     process_list.push_back(make_unique<CollisionBranch>(
         proc->particle_list()[0].type(), proc->particle_list()[1].type(),
         *photon_particle, xsection, ProcessType::Bremsstrahlung));
  
   } else if (reac_ == ReactionType::pi_m_pi_m ||
              reac_ == ReactionType::pi_p_pi_p ||
              reac_ == ReactionType::pi_z_pi_m ||
              reac_ == ReactionType::pi_z_pi_p) {
     // Here the final state hadrons are identical to the initial state hadrons
     if (reac_ == ReactionType::pi_m_pi_m || reac_ == ReactionType::pi_p_pi_p) {
       xsection = (*pipi_pipi_same_interpolation)(sqrts);
     } else {
       // One pi0 in initial and final state
       xsection = (*pipi0_pipi0_interpolation)(sqrts);
     }
  
     // Prevent negative cross sections due to numerics in interpolation
     xsection = (xsection <= 0.0) ? really_small : xsection;
  
     process_list.push_back(make_unique<CollisionBranch>(
         incoming_particles_[0].type(), incoming_particles_[1].type(),
         *photon_particle, xsection, ProcessType::Bremsstrahlung));
  
   } else if (reac_ == ReactionType::pi_z_pi_z) {
     // Here we have a hard-coded final state that differs from the initial
     // state, namely: pi0 + pi0 -> pi+- + pi-+ + gamma
     xsection = (*pi0pi0_pipi_interpolation)(sqrts);
  
     // Prevent negative cross sections due to numerics in interpolation
     xsection = (xsection <= 0.0) ? really_small : xsection;
  
     process_list.push_back(make_unique<CollisionBranch>(
         *pi_p_particle, *pi_m_particle, *photon_particle, xsection,
         ProcessType::Bremsstrahlung));
   } else {
     throw std::runtime_error("Unknown ReactionType in BremsstrahlungAction.");
   }
  
   return process_list;
 }

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◆ brems_diff_cross_sections()

std::pair< double, double > smash::BremsstrahlungAction::brems_diff_cross_sections ( )

private

Computes the differential cross sections dSigma/dk and dSigma/dtheta of the bremsstrahlung process.

Returns: Pair containing dSigma/dk as a first argument and dSigma/dtheta as a second argument

Definition at line 270 of file bremsstrahlungaction.cc.

                                                                         {
   static const ParticleTypePtr pi_z_particle = &ParticleType::find(pdg::pi_z);
   const double collision_energy = sqrt_s();
   double dsigma_dk;
   double dsigma_dtheta;
  
   if (reac_ == ReactionType::pi_p_pi_m) {
     if (outgoing_particles_[0].type() != *pi_z_particle) {
       // pi+- + pi+-- -> pi+- + pi+- + gamma
       dsigma_dk =
           (*pipi_pipi_opp_dsigma_dk_interpolation)(k_, collision_energy);
       dsigma_dtheta = (*pipi_pipi_opp_dsigma_dtheta_interpolation)(
           theta_, collision_energy);
     } else {
       // pi+- + pi+-- -> pi0 + pi0 + gamma
       dsigma_dk = (*pipi_pi0pi0_dsigma_dk_interpolation)(k_, collision_energy);
       dsigma_dtheta =
           (*pipi_pi0pi0_dsigma_dtheta_interpolation)(theta_, collision_energy);
     }
   } else if (reac_ == ReactionType::pi_p_pi_p ||
              reac_ == ReactionType::pi_m_pi_m) {
     dsigma_dk = (*pipi_pipi_same_dsigma_dk_interpolation)(k_, collision_energy);
     dsigma_dtheta =
         (*pipi_pipi_same_dsigma_dtheta_interpolation)(theta_, collision_energy);
   } else if (reac_ == ReactionType::pi_z_pi_p ||
              reac_ == ReactionType::pi_z_pi_m) {
     dsigma_dk = (*pipi0_pipi0_dsigma_dk_interpolation)(k_, collision_energy);
     dsigma_dtheta =
         (*pipi0_pipi0_dsigma_dtheta_interpolation)(theta_, collision_energy);
   } else if (reac_ == ReactionType::pi_z_pi_z) {
     dsigma_dk = (*pi0pi0_pipi_dsigma_dk_interpolation)(k_, collision_energy);
     dsigma_dtheta =
         (*pi0pi0_pipi_dsigma_dtheta_interpolation)(theta_, collision_energy);
   } else {
     throw std::runtime_error(
         "Unkown channel when computing differential cross sections for "
         "bremsstrahlung processes.");
   }
  
   // Prevent negative cross sections due to numerics in interpolation
   dsigma_dk = (dsigma_dk < 0.0) ? really_small : dsigma_dk;
   dsigma_dtheta = (dsigma_dtheta < 0.0) ? really_small : dsigma_dtheta;
  
   // Combine differential cross sections to a pair
   std::pair<double, double> diff_x_sections = {dsigma_dk, dsigma_dtheta};
  
   return diff_x_sections;
 }

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Member Data Documentation

◆ collision_processes_bremsstrahlung_

CollisionBranchList smash::BremsstrahlungAction::collision_processes_bremsstrahlung_

private

Holds the bremsstrahlung branch.

As of now, this will always hold only one branch.

Definition at line 143 of file bremsstrahlungaction.h.

◆ reac_

const ReactionType smash::BremsstrahlungAction::reac_

private

Reaction process as determined from incoming particles.

Definition at line 146 of file bremsstrahlungaction.h.

◆ number_of_fractional_photons_

const int smash::BremsstrahlungAction::number_of_fractional_photons_

private

Number of photons created for each hadronic scattering, needed for correct weighting.

Note that in generate_final_state() only one photon + two pions are created.

Definition at line 153 of file bremsstrahlungaction.h.

◆ weight_

double smash::BremsstrahlungAction::weight_ = 0.0

private

Weight of the produced photon.

Definition at line 156 of file bremsstrahlungaction.h.

◆ cross_section_bremsstrahlung_

double smash::BremsstrahlungAction::cross_section_bremsstrahlung_ = 0.0

private

Total cross section of bremsstrahlung process.

Definition at line 159 of file bremsstrahlungaction.h.

◆ hadronic_cross_section_

const double smash::BremsstrahlungAction::hadronic_cross_section_

private

Total hadronic cross section.

Definition at line 162 of file bremsstrahlungaction.h.

◆ k_

double smash::BremsstrahlungAction::k_

private

Sampled value of k (photon momentum)

Definition at line 165 of file bremsstrahlungaction.h.

◆ theta_

double smash::BremsstrahlungAction::theta_

private

Sampled value of theta (angle of the photon)

Definition at line 168 of file bremsstrahlungaction.h.

The documentation for this class was generated from the following files:

src/include/smash/bremsstrahlungaction.h
src/bremsstrahlungaction.cc

Public Types

Public Member Functions

Static Public Member Functions

Private Member Functions

Private Attributes

Additional Inherited Members

Member Enumeration Documentation

◆ ReactionType

Constructor & Destructor Documentation

◆ BremsstrahlungAction()

Member Function Documentation

◆ perform_bremsstrahlung()

◆ generate_final_state()

◆ sample_3body_phasespace()

◆ get_total_weight()

◆ hadronic_cross_section()

◆ add_dummy_hadronic_process()

◆ add_single_process()

◆ bremsstrahlung_reaction_type()

◆ is_bremsstrahlung_reaction()

◆ create_interpolations()

◆ brems_cross_sections()

◆ brems_diff_cross_sections()

Member Data Documentation

◆ collision_processes_bremsstrahlung_

◆ reac_

◆ number_of_fractional_photons_

◆ weight_

◆ cross_section_bremsstrahlung_

◆ hadronic_cross_section_

◆ k_

◆ theta_