= "Qi Qibar -> Qi Qibar, QCD, matrix element squared, tree";
description If[ $FrontEnd === Null,
= False;
$FeynCalcStartupMessages Print[description];
];
If[ $Notebooks === False,
= False
$FeynCalcStartupMessages ];
= {"FeynArts"};
$LoadAddOns
<< FeynCalc`= 0;
$FAVerbose
[9, 3, 1]; FCCheckVersion
\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}
Nicer typesetting
MakeBoxes[p1, TraditionalForm] := "\!\(\*SubscriptBox[\(p\), \(1\)]\)";
MakeBoxes[p2, TraditionalForm] := "\!\(\*SubscriptBox[\(p\), \(2\)]\)";
MakeBoxes[k1, TraditionalForm] := "\!\(\*SubscriptBox[\(k\), \(1\)]\)";
MakeBoxes[k2, TraditionalForm] := "\!\(\*SubscriptBox[\(k\), \(2\)]\)";
= InsertFields[CreateTopologies[0, 2 -> 2], {F[3, {1}], -F[3, {1}]} ->
diags {F[3, {1}], -F[3, {1}]}, InsertionLevel -> {Classes}, Model -> "SMQCD",
-> {S[_], V[1 | 2]}];
ExcludeParticles
[diags, ColumnsXRows -> {2, 1}, Numbering -> Simple,
Paint-> None, ImageSize -> {512, 256}]; SheetHeader
[0] = FCFAConvert[CreateFeynAmp[diags], IncomingMomenta -> {p1, p2},
amp-> {k1, k2}, UndoChiralSplittings -> True, ChangeDimension -> 4,
OutgoingMomenta List -> False, SMP -> True, Contract -> True, DropSumOver -> True]
\frac{g_s^2 T_{\text{Col3}\;\text{Col1}}^{\text{Glu5}} T_{\text{Col2}\;\text{Col4}}^{\text{Glu5}} \left(\varphi (\overline{k_1},m_u)\right).\bar{\gamma }^{\text{Lor2}}.\left(\varphi (\overline{p_1},m_u)\right) \left(\varphi (-\overline{p_2},m_u)\right).\bar{\gamma }^{\text{Lor2}}.\left(\varphi (-\overline{k_2},m_u)\right)}{(\overline{k_2}-\overline{p_2}){}^2}-\frac{g_s^2 T_{\text{Col2}\;\text{Col1}}^{\text{Glu5}} T_{\text{Col3}\;\text{Col4}}^{\text{Glu5}} \left(\varphi (\overline{k_1},m_u)\right).\bar{\gamma }^{\text{Lor1}}.\left(\varphi (-\overline{k_2},m_u)\right) \left(\varphi (-\overline{p_2},m_u)\right).\bar{\gamma }^{\text{Lor1}}.\left(\varphi (\overline{p_1},m_u)\right)}{(\overline{k_1}+\overline{k_2}){}^2}
[];
FCClearScalarProducts[s, t, u, p1, p2, -k1, -k2, SMP["m_u"], SMP["m_u"],
SetMandelstam["m_u"], SMP["m_u"]]; SMP
[0] = 1/(SUNN^2) (amp[0] (ComplexConjugate[amp[0]])) //
ampSquared// SUNSimplify[#, Explicit -> True,
FeynAmpDenominatorExplicit -> False] & // FermionSpinSum[#, ExtraFactor -> 1/2^2] & //
SUNNToCACF // TrickMandelstam[#, {s, t, u, 4 SMP["m_u"]^2}] & // Simplify DiracSimplify
\frac{\left(N^2-1\right) g_s^4 \left(-4 m_u^2 \left(N s^3+N t^3-2 s t u\right)+4 m_u^4 \left(N s^2+N t^2-3 s t\right)+N s^4+N s^3 t+N s^2 t^2+N s t^3+N t^4-s t u^2\right)}{N^3 s^2 t^2}
[0] = ampSquared[0] // ReplaceAll[#, {SMP["m_u"] -> 0}] & //
ampSquaredMassless[#, {s, t, u, 0}] & TrickMandelstam
-\frac{\left(1-N^2\right) g_s^4 \left(N t^4+2 N t^3 u+4 N t^2 u^2+3 N t u^3+N u^4-s t u^2\right)}{N^3 s^2 t^2}
[0] = ampSquaredMassless[0] /. SUNN -> 3 ampSquaredMasslessSUNN3
\frac{8 g_s^4 \left(-s t u^2+3 t^4+6 t^3 u+12 t^2 u^2+9 t u^3+3 u^4\right)}{27 s^2 t^2}
= {
knownResults 4/9) SMP["g_s"]^4 ((s^2 + u^2)/t^2 + (t^2 + u^2)/s^2) - (8/27) SMP["g_s"]^4 u^2/(s t))
((};
[{ampSquaredMasslessSUNN3[0]}, {knownResults},
FCCompareResultsText -> {"\tCompare to Ellis, Stirling and Weber, QCD and Collider Physics, Table 7.1:",
"CORRECT.", "WRONG!"}, Interrupt -> {Hold[Quit[1]], Automatic}, Factoring ->
Function[x, Simplify[TrickMandelstam[x, {s, t, u, 0}]]]]
Print["\tCPU Time used: ", Round[N[TimeUsed[], 3], 0.001], " s."];
\text{$\backslash $tCompare to Ellis, Stirling and Weber, QCD and Collider Physics, Table 7.1:} \;\text{CORRECT.}
\text{True}
\text{$\backslash $tCPU Time used: }18.467\text{ s.}