ThePEG
2.1.4

SimplePhaseSpace defines a set of static functions to be used for distributing momenta evenly in phase space. More...
Functions  
template<typename PType >  
void  CMS (Energy2 s, PType &p1, PType &p2) 
Set two momenta in their center of mass system. More...  
template<typename PType >  
void  CMS (PType &p1, PType &p2, Energy2 s, double cosTheta, double phi) 
Set two momenta in their center of mass system. More...  
template<typename PType >  
void  CMS (PType &p1, PType &p2, Energy2 s, Energy2 t, double phi, const PType &p0) 
Set two momenta in their center of mass system. More...  
template<typename PType >  
void  CMS (PType &p1, PType &p2, Energy2 s) 
Set two momenta in their center of mass system. More...  
template<typename PPairType >  
void  CMS (const PPairType &p, Energy2 s) 
Set two momenta in their center of mass system. More...  
template<typename PType >  
void  CMS (PType &p1, PType &p2, PType &p3, Energy2 s, double x1, double x3) 
Set three momenta in their center of mass system. More...  
template<typename PType >  
void  CMS (PType &p1, PType &p2, PType &p3, Energy2 s, double x1, double x3, double phii=0.0, double theta=0.0, double phi=0.0) 
Set three momenta in their center of mass system. More...  
Energy  getMagnitude (Energy2 s, Energy m1, Energy m2) 
Calculate the absolute magnitude of the momenta of two particles with masses m1 and m2 when put in their CMS of total invariant mass squared s. More...  
Momentum3  polar3Vector (Energy p, double costheta, double phi) 
Return a threevector given the absolute momentum, cos(theta) and phi. More...  
vector< LorentzMomentum >  CMSn (Energy m0, const vector< Energy > &m) 
Get a number of randomly distributed momenta. More...  
template<typename Container >  
void  CMSn (Container &particles, Energy m0) 
Set the momentum of a number of particles. More...  
SimplePhaseSpace defines a set of static functions to be used for distributing momenta evenly in phase space.
In most cases pointers and references to both particle and momentum objects can be used as arguments as long as the ParticleTraits class is specialized properly. When needed, random numbers are generated with the generator given by the static UseRandom class.
void ThePEG::SimplePhaseSpace::CMS  (  Energy2  s, 
PType &  p1,  
PType &  p2  
) 
Set two momenta in their center of mass system.
Their total invariant mass squared is given by s, and their direction is distributed isotropically.
s  the total invariant mass squared. 
p1  pointer or reference to the first momentum. Its invariant mass will be preserved. 
p2  pointer or reference to the second momentum. Its invariant mass will be preserved. 
ImpossibleKinematics  if the sum of the invariant masses was larger than the given invariant mass ( ). 
Referenced by CMS().
void ThePEG::SimplePhaseSpace::CMS  (  PType &  p1, 
PType &  p2,  
Energy2  s,  
double  cosTheta,  
double  phi  
) 
Set two momenta in their center of mass system.
Their total invariant mass squared is given by s, and their direction is given in terms of the polar and azimuth angle of the first momenta.
s  the total invariant mass squared. 
p1  pointer or reference to the first momentum. Its invariant mass will be preserved. 
p2  pointer or reference to the second momentum. Its invariant mass will be preserved. 
cosTheta  cosine of the azimuth angle of the first momentum. 
phi  azimuth angle of the first momentum. 
ImpossibleKinematics  if the sum of the invariant masses was larger than the given invariant mass ( ). 
void ThePEG::SimplePhaseSpace::CMS  (  PType &  p1, 
PType &  p2,  
Energy2  s,  
Energy2  t,  
double  phi,  
const PType &  p0  
) 
Set two momenta in their center of mass system.
Their total invariant mass squared is given by s. The helper momentum p0 is used so that afterwards and p1 has the azimuth angle phi around p0.
p1  pointer or reference to the first momentum. Its invariant mass will be preserved. 
p2  pointer or reference to the second momentum. Its invariant mass will be preserved. 
s  the total invariant mass squared. 
t  . 
phi  azimuth angle of the first momentum around p0. 
p0  pointer or reference to an auxiliary momentum. 
ImpossibleKinematics  if the sum of the invariant masses was larger than the given invariant mass ( ). 
void ThePEG::SimplePhaseSpace::CMS  (  PType &  p1, 
PType &  p2,  
Energy2  s  
) 
Set two momenta in their center of mass system.
Their total invariant mass squared is given by s. p1 will be along the zaxis.
p1  pointer or reference to the first momentum. Its invariant mass will be preserved. 
p2  pointer or reference to the second momentum. Its invariant mass will be preserved. 
s  the total invariant mass squared. 
ImpossibleKinematics  if the sum of the invariant masses was larger than the given invariant mass ( ). 
void ThePEG::SimplePhaseSpace::CMS  (  const PPairType &  p, 
Energy2  s  
) 
Set two momenta in their center of mass system.
Their total invariant mass squared is given by s. The first will be along the zaxis.
p  a pair of pointers or references to the two momenta. Their invariant masses will be preserved. 
s  the total invariant mass squared. 
ImpossibleKinematics  if the sum of the invariant masses was larger than the given invariant mass ( ). 
Definition at line 113 of file SimplePhaseSpace.h.
References CMS(), and getMagnitude().
void ThePEG::SimplePhaseSpace::CMS  (  PType &  p1, 
PType &  p2,  
PType &  p3,  
Energy2  s,  
double  x1,  
double  x3  
) 
Set three momenta in their center of mass system.
Their total invariant mass squared is given by s. The energy fraction of particle p1(3) is x1(3) of the total energy and the angles of the system is distributed isotropically.
p1  pointer or reference to the first momentum. Its invariant mass will be preserved. 
p2  pointer or reference to the second momentum. Its invariant mass will be preserved. 
p3  pointer or reference to the second momentum. Its invariant mass will be preserved. 
s  the total invariant mass squared. 
x1  the energy fraction . 
x3  the energy fraction . 
ImpossibleKinematics  if the sum of the invariant masses was larger than the given invariant mass ( ). 
void ThePEG::SimplePhaseSpace::CMS  (  PType &  p1, 
PType &  p2,  
PType &  p3,  
Energy2  s,  
double  x1,  
double  x3,  
double  phii = 0.0 , 

double  theta = 0.0 , 

double  phi = 0.0 

) 
Set three momenta in their center of mass system.
Their total invariant mass squared is given by s. The energy fraction of particle p1(3) is x1(3) of the total energy. Particle p1 is initially placed along the zaxis and particle p2 is given azimuth angle phii. Then the system is then rotated with theta and phi respectively.
p1  pointer or reference to the first momentum. Its invariant mass will be preserved. 
p2  pointer or reference to the second momentum. Its invariant mass will be preserved. 
p3  pointer or reference to the second momentum. Its invariant mass will be preserved. 
s  the total invariant mass squared. 
x1  the energy fraction . 
x3  the energy fraction . 
phii  the azimuth angle of p2 around p1. 
theta  the polar angle of p1. 
phi  the azimuth angle of p1. 
ImpossibleKinematics  if the sum of the invariant masses was larger than the given invariant mass ( ). 
vector<LorentzMomentum> ThePEG::SimplePhaseSpace::CMSn  (  Energy  m0, 
const vector< Energy > &  m  
) 
Get a number of randomly distributed momenta.
Given a number specified invariant masses and a total invariant mass m0, return corresponding fourmomenta randomly distributed according to phase space.
m0  the total invariant mass of the resulting momenta. 
m  a vector of invariant masses of the resulting momenta. 
ImpossibleKinematics  if the sum of the masses was larger than the given invariant mass ( ). 
Referenced by polar3Vector().
void ThePEG::SimplePhaseSpace::CMSn  (  Container &  particles, 
Energy  m0  
) 
Set the momentum of a number of particles.
Given a number of particles and a total invariant mass m0, distribute their fourmomenta randomly according to phase space.
particles  a container of particles or pointers to particles. The invariant mass of these particles will not be chaned. 
m0  the total invariant mass of the resulting momenta. 
ImpossibleKinematics  if the sum of the masses was larger than the given invariant mass ( ). 
Calculate the absolute magnitude of the momenta of two particles with masses m1 and m2 when put in their CMS of total invariant mass squared s.
s  the total invariant mass squared. 
m1  the mass of particle 1. 
m2  the mass of particle 2. 
ImpossibleKinematics  if the sum of the masses was larger than the given invariant mass ( ). 
Referenced by CMS().
Return a threevector given the absolute momentum, cos(theta) and phi.
p  the magnitude of the momentum. 
costheta  the cosine of the polar angle. 
phi  the azimuth angle. 
Definition at line 185 of file SimplePhaseSpace.h.
References CMSn().