PYTHIA
8.312
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A class containing DGLAP splitting functions for limit checking. More...
#include <VinciaAntennaFunctions.h>
Public Member Functions | |
DGLAP () | |
Constructor. | |
double | Pg2gg (double z, int hA=9, int hB=9, int hC=9) |
DGLAP splitting functions. More... | |
double | Pg2qq (double z, int hA=9, int hB=9, int hC=9, double mu=0.) |
double | Pq2qg (double z, int hA=9, int hB=9, int hC=9, double mu=0.) |
double | Pq2gq (double z, int hA=9, int hB=9, int hC=9, double mu=0.) |
double | Pg2qq (double z, double mu) |
Wrappers to get unpolarized massive Altarelli-Pariis kernels (mu = m/Q). | |
double | Pq2qg (double z, double mu) |
double | Pq2gq (double z, double mu) |
double | Pg2ggLin (double z, int polA=9, int polB=9, int polC=9) |
Pg2ggLin, written without factor 2 normalization convention. More... | |
double | Pg2qqLin (double z, int polA=9, int hB=9, int hC=9, double mu=0.) |
double | Pq2qgLin (double z, int hA=9, int hB=9, int polC=9, double mu=0.) |
double | Pq2gqLin (double z, int hA=9, int polB=9, int hC=9, double mu=0.) |
A class containing DGLAP splitting functions for limit checking.
double Pg2gg | ( | double | z, |
int | hA = 9 , |
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int | hB = 9 , |
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int | hC = 9 |
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) |
DGLAP splitting functions.
Helicity-dependent Altarelli-Parisi kernels (mu = m/Q). Note, Pg2gg is written with standard factor 2 normalization convention.
DGLAP splitting kernels with helicity-dependence (from Larkoski, Peskin, http:///arxiv.org/abs/arXiv:0908.2450). Note, Pg2gg is written with the standard factor 2 normalization convention and gives a factor 2 difference with respect PYTHIA FSR. The difference is related to whether P is interpreted as the probability for gluon A to branch to BC (without factor 2), or as the probability for gluon B to have originated from A (with factor 2). Both quarks and gluons have definite helicities: 9: unpolarized +1: right-handed -1: left-handed where z is momentum fraction taken by B in A -> BC. Pg2gg, written with the standard factor 2 normalization convention.
If A unpolarized, treat as unpolarized.
Expressions coded for hA = 1. Flip helicities if hA = -1.
double Pg2ggLin | ( | double | z, |
int | polA = 9 , |
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int | polB = 9 , |
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int | polC = 9 |
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) |
Pg2ggLin, written without factor 2 normalization convention.
Altarelli-Parisi kernels with linear in/out polarizations for gluons: pol = +1 for in-plane, -1 for out-of-plane.
DGLAP splitting kernels with polarization-dependence (from Ellis, Stirling, Webber) Gluons are plane polarized, quarks have helicities: 9: unpolarized +1: in plane / right-handed -1: out-of-plane / left-handed where z is momentum fraction taken by B in A -> BC.
If A unpolarized, treat as unpolarized.
A in-plane polarized.
A out-of-plane polarized.
double Pg2qq | ( | double | z, |
int | hA = 9 , |
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int | hB = 9 , |
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int | hC = 9 , |
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double | mu2 = 0. |
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) |
Pg2qq, B is quark, C is antiquark. Note, mass corrections not implemented.
If A unpolarized, treat as unpolarized.
Preserve quark helicity.
Expressions coded for hA = 1. Flip helicities if hA = -1.
double Pg2qqLin | ( | double | z, |
int | polA = 9 , |
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int | hB = 9 , |
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int | hC = 9 , |
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double | mu = 0. |
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) |
Pg2qqLin, B is quark, C is antiquark. Note, mass corrections not implemented.
If A unpolarized, treat as unpolarized.
Preserve quark helicity.
A in-plane polarized.
A out-of-plane polarized.
double Pq2gq | ( | double | z, |
int | hA = 9 , |
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int | hB = 9 , |
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int | hC = 9 , |
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double | mu = 0. |
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) |
Pq2qg, B is gluon, C is quark. Note, mass corrections not implemented for polarised.
double Pq2gqLin | ( | double | z, |
int | hA = 9 , |
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int | polB = 9 , |
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int | hC = 9 , |
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double | mu = 0. |
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) |
Pq2qgLin, B is gluon, C is quark. Note, mass corrections not implemented.
double Pq2qg | ( | double | z, |
int | hA = 9 , |
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int | hB = 9 , |
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int | hC = 9 , |
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double | mu2 = 0. |
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) |
Pq2qg, B is quark, C is gluon. Note, mass corrections not implemented for polarised.
If A unpolarized, treat as unpolarized.
Preserve quark helicity
Expressions coded for hA = +1. Flip helicities if hA = -1.
double Pq2qgLin | ( | double | z, |
int | hA = 9 , |
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int | hB = 9 , |
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int | polC = 9 , |
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double | mu = 0. |
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) |
Pq2qgLin, B is quark, C is gluon. Note, mass corrections not implemented.
If A unpolarized, treat as unpolarized.
Preserve quark helicity.
Gluon polarized in plane.
Gluon polarized out of plane.