Electrons annihilation to photons in QED
Code: "redberry2.groovy". Programming language: Groovy
DMelt Version 1.8. Last modified: 04/22/2014. License: Pro
https://datamelt.org/code/cache/redberry2_5786.groovy
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import cc.redberry.groovy.Redberry
import static cc.redberry.core.indices.IndexType.*
import static cc.redberry.groovy.RedberryPhysics.*
import static cc.redberry.groovy.RedberryStatic.*
//******************************************************//
//******** Electrons annihilation in two photons *******//
//******************************************************//
use(Redberry) {
//setting up matrix quantities
defineMatrices 'G_a', 'V_i', 'D[x_m]', Matrix1.matrix,
'v[p_a]', 'u[p_a]', Matrix1.vector,
'cv[p_a]', 'cu[p_a]', Matrix1.covector
//vertex
def V = 'V_m = -I*e*G_m'.t,
//electron propagator
D = 'D[p_m] = -I*(m + p_m*G^m)/(m**2 - p_m*p^m)'.t,
//diagramm a)
Ma = 'cv[p2_m]*V_m*e^m[k2_m]*D[p1_m-k1_m]*V_n*e^n[k1_m]*u[p1_m]'.t,
//diagramm b)
Mb = 'cv[p2_m]*V_m*e^m[k1_m]*D[p1_m-k2_m]*V_n*e^n[k2_m]*u[p1_m]'.t,
//matrix element
M = Ma + Mb
//substitute vertex and propagator in matrix element
M = (V & D) >> M
//mandelstam and mass shell substitutions
def mandelstam = setMandelstam(
['p1_m': 'm', 'p2_m': 'm', 'k1_m': '0', 'k2_m': '0'])
//expand and apply substitutions
M = (ExpandAll & mandelstam) >> M
//complex conjugation
//exchange spinor momentums
def MC = 'u[p1_m]*cv[p2_m] = v[p2_m]*cu[p1_m]'.t >> M
//complex conjugate and reorder gamma matrices
MC = (Conjugate & Reverse[Matrix1]) >> MC
//squared matrix element
def M2 = ExpandAll >> (M * MC / 4)
//photon polarizations
M2 = 'e_m[k1_a]*e_n[k1_a] = -g_mn'.t >> M2
M2 = 'e_m[k2_a]*e_n[k2_a] = -g_mn'.t >> M2
//electron polarizations
M2 = 'u[p1_m]*cu[p1_m] = m + p1^m*G_m'.t >> M2
M2 = 'v[p2_m]*cv[p2_m] = -m + p2^m*G_m'.t >> M2
//trace of gamma matrices
M2 = DiracTrace['G_a'] >> M2
//final simplifications
M2 = (ExpandAndEliminate & 'd^m_m = 4'.t & mandelstam) >> M2
M2 = 'u = 2*m**2 -s-t'.t >> M2
M2 = Factor >> M2
println M2
}
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