Please use this identifier to cite or link to this item: http://hdl.handle.net/123456789/3412
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dc.contributor.authorBhattacharya, A.-
dc.contributor.authorMahakhud, M.-
dc.contributor.authorMathews, P.-
dc.contributor.authorRavindran, V.-
dc.date.accessioned2020-12-28T06:39:03Z-
dc.date.available2020-12-28T06:39:03Z-
dc.date.issued2020-
dc.identifier.citationJournal of High Energy Physics 2020(2),121en_US
dc.identifier.other10.1007/JHEP02(2020)121-
dc.identifier.urihttps://link.springer.com/article/10.1007%2FJHEP02%282020%29121-
dc.identifier.urihttp://hdl.handle.net/123456789/3412-
dc.description.abstractWe compute the radiative corrections to the four-point amplitude g+g → A+A in massless Quantum Chromodynamics (QCD) up to order α4s in perturbation theory. We used the effective field theory that describes the coupling of pseudo-scalars to gluons and quarks directly, in the large top quark mass limit. Due to the CP odd nature of the pseudo-scalar Higgs boson, the computation involves careful treatment of chiral quantities in dimensional regularisation. The ultraviolet finite results are shown to be consistent with the universal infrared structure of QCD amplitudes. The infrared finite part of these amplitudes constitutes the important component of any next to next to leading order corrections to observables involving pair of pseudo-scalars at the Large Hadron Collider.en_US
dc.language.isoenen_US
dc.publisherSpringer Linken_US
dc.subjectQuantum Chromodynamics (QCD)en_US
dc.subjectField theoryen_US
dc.subjectPseudo-scalarsen_US
dc.titleTwo loop QCD amplitudes for di-pseudo scalar production in gluon fusionen_US
dc.typeArticleen_US
Appears in Collections:Research Articles

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