#include "forwarddeclarations.h"
#include "isoparticletype.h"
#include "particles.h"
#include "potential_globals.h"
#include "processstring.h"
Go to the source code of this file.
Classes | |
class | smash::CrossSections |
The cross section class assembels everything that is needed to calculate the cross section and returns a list of all possible reactions for the incoming particles at the given energy with the calculated cross sections. More... | |
Namespaces | |
smash | |
smash::transit_high_energy | |
constants related to transition between low and high collision energies | |
Variables | |
const std::array< double, 2 > | smash::transit_high_energy::sqrts_range_Npi = {1.9, 2.2} |
transition range in N-pi collisions More... | |
const std::array< double, 2 > | smash::transit_high_energy::sqrts_range_NN = {3.5, 4.5} |
transition range in N-N collisions: Tuned to reproduce experimental exclusive cross section data, and at the same produce excitation functions that are as smooth as possible. More... | |
const double | smash::transit_high_energy::sqrts_add_lower = 0.9 |
constant for the lower end of transition region in the case of AQM this is added to the sum of masses More... | |
const double | smash::transit_high_energy::sqrts_range = 1.0 |
constant for the range of transition region in the case of AQM this is added to the sum of masses + sqrts_add_lower More... | |
const double | smash::transit_high_energy::pipi_offset = 1.12 |
Constant offset as to where to turn on the strings and elastic processes for pi pi reactions (this is an exception because the normal AQM behavior destroys the cross-section at very low sqrt_s and around the f2 peak) More... | |
const double | smash::transit_high_energy::KN_offset = 15.15 |
Constant offset as to where to shift from 2to2 to string processes (in GeV) in the case of KN reactions. More... | |