Wolfram Language Paclet Repository
Community-contributed installable additions to the Wolfram Language
Computes 2-to-2 scattering matrix amplitudes for arbitrary quantum field theories
Contributed by: Andreas Ekstedt
Oliver Gould
Joonas Hirvonen
Benoit Laurent
Lauri Niemi
Philipp Schicho
Jorinde van de Vis
Computes 2-to-2 scattering matrix amplitudes for arbitrary quantum field theories.
To install this paclet in your Wolfram Language environment,
evaluate this code:
PacletInstall["WallGo/WallGoMatrix"]
To load the code after installation, evaluate this code:
Needs["WallGo`WallGoMatrix`"]
Using SU(3) in the representation with Dynkin index {1,1} and representation R= 8.
In[1]:= | ![]() |
No scalars are present in the theory:
In[2]:= | ![]() |
Fermions are implemented as Weyl spinors. Therefore, to create one Dirac fermion, one left-handed and one right-handed fermion is needed:
In[3]:= | ![]() |
For QCD, Nf=6 fermions are needed:
In[4]:= | ![]() |
The input for the gauge interactions to DRalgo are then given by
In[5]:= | ![]() |
To invoke the model, it needs to be imported:
In[6]:= | ![]() |
Representation for top quark:
In[7]:= | ![]() |
Out[7]= | ![]() |
Representation for gluon:
In[8]:= | ![]() |
Out[8]= | ![]() |
Representation for 5 light quarks:
In[9]:= | ![]() |
Out[9]= | ![]() |
Collecting out-of-equilibrium particles:
In[10]:= | ![]() |
Collecting light particles (these are never incoming):
In[11]:= | ![]() |
In[12]:= | ![]() |
Out[8]= | ![]() |
Wolfram Language Version 13
GNU General Public License v3.0 or later