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Hi,
I'd say that either the difference between expressions involving different If you suspect that the problem is on the FeynCalc side, you could do a cross-check with FormCalc or CalcHEP to be safe. Cheers, |
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Hi,
I am encountering a peculiarity with DoPolarizationSums that I do not understand. The problem under consideration is a three body decay of the form
G(p1)->\pi(p2)+\pi(p3)+\gamma(p4),
where all particles are scalar or pseudoscalar and massive, except the photon.
Suppose I have the amplitude
(Id5(Pair[Momentum[p1], Momentum[p2]] - Pair[Momentum[p1], Momentum[p3]])Pair[Momentum[p1], Momentum[Polarization[p4, -I, Transversality -> True]]])/m^2 +
Id5*(Pair[Momentum[p2], Momentum[Polarization[p4, -I, Transversality -> True]]] - Pair[Momentum[p3], Momentum[Polarization[p4, -I, Transversality -> True]]])
When I then compute the squared matrix element via DoPolarizationSums[ComplexConjugate[%] % ,p4 , n] I get different results depending on which auxiliary vector I choose e.g. n= p1, p2 or p3. When the result should of course be independent of that choice.
The scalar product for p4 is set on-shell. The Lagrangian looks like this (or the d5 term in (B5) of 1501.07906):
QuantumField[GaugeField, LorentzIndex[[Nu]1]]*(QuantumField[[CapitalPi]2]*QuantumField[FCPartialD[LorentzIndex[[Mu]1]], [CapitalPi]1] -
QuantumField[[CapitalPi]1]QuantumField[FCPartialD[LorentzIndex[[Mu]1]], [CapitalPi]2])(MT[[Mu]1, [Nu]1]*QuantumField[Gd] -
QuantumField[FCPartialD[LorentzIndex[[Mu]1]], FCPartialD[LorentzIndex[[Nu]1]], Gd]/m1SS^2)
I also encountered the problem in a more complicated decay of a pseudovector into a pseudoscalar + vector + photon. But the problem is probably the same in both cases. So far I had no difficulties with this method for two-body decays even when the interactions are coming from a Chern-Simons term, which is not gauge invariant.
Any help or comment is much appreciated!
Thanks in advance!
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