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dc.contributor.authorCMS Collaborationen_US
dc.contributor.authorHayrapetyan, A.en_US
dc.contributor.authorDUBE, SOURABHen_US
dc.contributor.authorHAZARIKA, P.en_US
dc.contributor.authorKANSAL, B.en_US
dc.contributor.authorLAHA, A.en_US
dc.contributor.authorSHARMA, R.en_US
dc.contributor.authorSHARMA, SEEMAen_US
dc.contributor.authorVAISH, K.Y. et al.en_US
dc.date.accessioned2026-07-20T09:49:43Z
dc.date.available2026-07-20T09:49:43Z
dc.date.issued2026-05en_US
dc.identifier.citationPhysical Review D, 113, 092014en_US
dc.identifier.issn2470-0029en_US
dc.identifier.issn2470-0010en_US
dc.identifier.urihttps://doi.org/10.1103/rny9-zby1en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/11380
dc.description.abstractThe Higgs boson (H) decay width is determined from the ratio of off- and on-shell production of 𝐻 β†’π‘Šβ’π‘Š β†’π‘’β’πœˆβ’πœ‡β’πœˆ using proton–proton collision data corresponding to an integrated luminosity of 138 fbβˆ’1 collected at βˆšπ‘  =13 TeV by the CMS experiment at the Large Hadron Collider. The off-shell signal strength is measured as πœ‡offβˆ’shell =1.2+0.8βˆ’0.7. The Higgs boson total decay width is Γ𝐻 =3.9+2.7βˆ’2.2 MeV, in agreement with the standard model prediction. The uncertainty in this result represents a factor of 3 improvement over the previous CMS result in this decay channel.en_US
dc.language.isoenen_US
dc.publisherAmerican Physical Societyen_US
dc.subjectParticle decaysen_US
dc.subjectHiggs bosonsen_US
dc.subjectHadron collidersen_US
dc.subject2026-JUL-WEEK3en_US
dc.subjectTOC-JUL-2026en_US
dc.subject2026en_US
dc.titleMeasurement of the Higgs boson total decay width using the π»β†’π‘Šβ’π‘Šβ†’π‘’β’πœˆβ’πœ‡β’πœˆ decay channel in proton-proton collisions at βˆšπ‘  =13  TeVen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitlePhysical Review Den_US
dc.publication.originofpublisherForeignen_US
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