Radius
(double, required):
Radius of the Sphere, in fm.
Temperature
(double, required):
Temperature to sample momenta in the sphere, in GeV.
Start_Time
(double, required):
Starting time of sphere calculation.
Init_Multiplicities
(int int, required if Use_Thermal_Multiplicities is false):
Initial multiplicities per particle species. Map of PDG number and quantity of this PDG number. Controls how many particles of each species will be initialized.
Use_Thermal_Multiplicities
(bool, optional, default = false):
If this option is set to true then Init_Multiplicities are ignored and the box is initialized with all particle species of the particle table that belong to the hadron gas equation of state (see HadronGasEos::is_eos_particle()). The multiplicities are sampled from Poisson distributions \( Poi(n_i V) \), where \( n_i \) are the grand-canonical thermal densities of the corresponding species and \( V \) is the box volume. This option simulates the grand-canonical ensemble, where the number of particles is not fixed from event to event.
Baryon_Chemical_Potential
(double, optional, default = 0.0):
Baryon chemical potential \( \mu_B \) only used if Use_Thermal_Multiplicities is true to compute thermal densities \( n_i \).
Strange_Chemical_Potential
(double, optional, default = 0.0):
Strangeness chemical potential \( \mu_S \) only used if Use_Thermal_Multiplicities is true to compute thermal densities \( n_i \).
Charge_Chemical_Potential
(double, optional, default = 0.0):
Charge chemical potential \( \mu_Q \) only used if Use_Thermal_Multiplicities is true to compute thermal densities \( n_i \).
Account_Resonance_Widths
(bool, optional, default = true):
In case of thermal initialization: true – account for resonance spectral functions, while computing multiplicities and sampling masses, false – simply use pole masses.
Initial_Condition
(string, optional, default = "thermal momenta")
Initial distribution to use for momenta of particles. Mainly used in the expanding universe scenario, options are:
thermal
momenta - equilibrium Boltzmann distribution IC_ES
- off-equilibrium distribution IC_1M
- off-equilibrium distribution IC_2M
- off-equilibrium distribution IC_Massive
- off-equilibrium distributionSee Bazow:2016oky [2] and Tindall:2016try [11] for further explanations about the different distribution functions.
Jet:
This subset of config values is used to put a single high energy particle (a "jet") in the center of the sphere, on an outbound trajectory along the x axis; if no pdg is specified no jet is produced.
Jet_PDG
(int, optional): The type of particle to be used as a jet, as given by its PDG code; if none is provided no jet is initialized.Jet_Momentum
(double, optional, default = 20.): The initial momentum to give to the jet particle (in GeV)
The following example configures an expanding sphere with a radius of 5 fm at a temperature of 200 MeV. The particles are initialized with thermal momenta at a start time of 0 fm. The particle numbers at initialization are 100 \( \pi^+ \), 100 \( \pi^0 \), 100 \( \pi^- \), 50 protons and 50 neutrons.
Modi: Sphere: Radius: 5.0 Temperature: 0.2 Initial_Condition: "thermal momenta" Start_Time: 0.0 Init_Multiplicities: 211: 100 111: 100 -211: 100 2212: 50 2112: 50
It is also possible to initialize a sphere based on thermal multiplicities. This is done via
Modi: Sphere: Radius: 10.0 Temperature: 0.2 Use_Thermal_Multiplicities: True
If one wants to simulate a jet in the hadronic medium, this can be done by using the following configuration setup:
Modi: Sphere: Radius: 10.0 Temperature: 0.2 Use_Thermal_Multiplicities: True Jet: Jet_PDG: 211 Jet_Momentum: 100.0
./smash -i INPUT_DIR/sphere/config.yaml