QED manual (development version)

Load FeynCalc and the necessary add-ons or other packages

description = "El El -> El El, QED, matrix element squared, tree";
If[ $FrontEnd === Null, 
    $FeynCalcStartupMessages = False; 
    Print[description]; 
  ];
If[ $Notebooks === False, 
    $FeynCalcStartupMessages = False 
  ];
$LoadAddOns = {"FeynArts"};
<< FeynCalc`
$FAVerbose = 0; 
 
FCCheckVersion[9, 3, 1];

\text{FeynCalc }\;\text{10.0.0 (dev version, 2023-12-20 22:40:59 +01:00, dff3b835). For help, use the }\underline{\text{online} \;\text{documentation}}\;\text{, check out the }\underline{\text{wiki}}\;\text{ or visit the }\underline{\text{forum}.}

\text{Please check our }\underline{\text{FAQ}}\;\text{ for answers to some common FeynCalc questions and have a look at the supplied }\underline{\text{examples}.}

\text{If you use FeynCalc in your research, please evaluate FeynCalcHowToCite[] to learn how to cite this software.}

\text{Please keep in mind that the proper academic attribution of our work is crucial to ensure the future development of this package!}

\text{FeynArts }\;\text{3.11 (3 Aug 2020) patched for use with FeynCalc, for documentation see the }\underline{\text{manual}}\;\text{ or visit }\underline{\text{www}.\text{feynarts}.\text{de}.}

\text{If you use FeynArts in your research, please cite}

\text{ $\bullet $ T. Hahn, Comput. Phys. Commun., 140, 418-431, 2001, arXiv:hep-ph/0012260}

Generate Feynman diagrams

Nicer typesetting

MakeBoxes[p1, TraditionalForm] := "\!\(\*SubscriptBox[\(p\), \(1\)]\)";
MakeBoxes[p2, TraditionalForm] := "\!\(\*SubscriptBox[\(p\), \(2\)]\)";
MakeBoxes[k1, TraditionalForm] := "\!\(\*SubscriptBox[\(k\), \(1\)]\)";
MakeBoxes[k2, TraditionalForm] := "\!\(\*SubscriptBox[\(k\), \(2\)]\)";

diags = InsertFields[CreateTopologies[0, 2 -> 2], {F[2, {1}], F[2, {1}]} -> 
            {F[2, {1}], F[2, {1}]}, InsertionLevel -> {Classes}, 
            Restrictions -> QEDOnly]; 
 
Paint[diags, ColumnsXRows -> {2, 1}, Numbering -> Simple, 
    SheetHeader -> None, ImageSize -> {512, 256}];

Obtain the amplitude

amp[0] = FCFAConvert[CreateFeynAmp[diags], IncomingMomenta -> {p1, p2}, 
    OutgoingMomenta -> {k1, k2}, UndoChiralSplittings -> True, ChangeDimension -> 4, 
    List -> False, SMP -> True, Contract -> True]

\frac{\text{e}^2 \left(\varphi (\overline{k_1},m_e)\right).\bar{\gamma }^{\text{Lor1}}.\left(\varphi (\overline{p_2},m_e)\right) \left(\varphi (\overline{k_2},m_e)\right).\bar{\gamma }^{\text{Lor1}}.\left(\varphi (\overline{p_1},m_e)\right)}{(\overline{k_1}-\overline{p_2}){}^2}-\frac{\text{e}^2 \left(\varphi (\overline{k_1},m_e)\right).\bar{\gamma }^{\text{Lor2}}.\left(\varphi (\overline{p_1},m_e)\right) \left(\varphi (\overline{k_2},m_e)\right).\bar{\gamma }^{\text{Lor2}}.\left(\varphi (\overline{p_2},m_e)\right)}{(\overline{k_2}-\overline{p_2}){}^2}

Fix the kinematics

FCClearScalarProducts[];
SetMandelstam[s, t, u, p1, p2, -k1, -k2, 
    SMP["m_e"], SMP["m_e"], SMP["m_e"], SMP["m_e"]];

Square the amplitude

ampSquared[0] = (amp[0] (ComplexConjugate[amp[0]])) // 
        FeynAmpDenominatorExplicit // 
        FermionSpinSum[#, ExtraFactor -> 1/2^2] & // 
    DiracSimplify // Simplify

\frac{2 \;\text{e}^4 \left(-4 m_e^2 \left(s \left(t^2+3 t u+u^2\right)+t^3-2 t^2 u-2 t u^2+u^3\right)+8 m_e^4 \left(t^2+t u+u^2\right)+s^2 (t+u)^2+t^4+u^4\right)}{t^2 u^2}

ampSquaredMassless[0] = ampSquared[0] // ReplaceAll[#, {SMP["m_e"] -> 0}] & // 
    Simplify

\frac{2 \;\text{e}^4 \left(s^2 (t+u)^2+t^4+u^4\right)}{t^2 u^2}

Check the final results

knownResult = 2 SMP["e"]^4 (s^2/t^2 + u^2/t^2 + s^2/u^2 + t^2/u^2) + 
    4 SMP["e"]^4 s^2/(t u);
FCCompareResults[ampSquaredMassless[0], knownResult, 
   Text -> {"\tCheck the final result:", 
     "CORRECT.", "WRONG!"}, Interrupt -> {Hold[Quit[1]], Automatic}];
Print["\tCPU Time used: ", Round[N[TimeUsed[], 4], 0.001], " s."];

\text{$\backslash $tCheck the final result:} \;\text{CORRECT.}

\text{$\backslash $tCPU Time used: }22.019\text{ s.}