Please use this identifier to cite or link to this item: http://hdl.handle.net/123456789/4447
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dc.contributor.authorBhattacharya, Arunima-
dc.contributor.authorMahakhud, Maguni-
dc.contributor.authorMathews, Prakash-
dc.contributor.authorRavindran, V.-
dc.date.accessioned2023-08-10T09:33:13Z-
dc.date.available2023-08-10T09:33:13Z-
dc.date.issued2022-
dc.identifier.urihttps://doi.org/10.1007/978-981-19-2354-8_9-
dc.identifier.urihttp://hdl.handle.net/123456789/4447-
dc.descriptionOnly IISER Mohali authors are available in the record.en_US
dc.description.abstractWe compute the radiative corrections to the four-point amplitude g+g→A+A in massless quantum chromodynamics (QCD) up to order a4s 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.isoen_USen_US
dc.publisherSpringer Linken_US
dc.subjectTwo-Loopen_US
dc.subjectAmplitudesen_US
dc.subjectDi-pseudoen_US
dc.subjectGluon Fusionen_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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