Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/4841
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dc.contributor.authorBhardwaj, Akankshaen_US
dc.contributor.authorDas, Arindamen_US
dc.contributor.authorKonar, Parthaen_US
dc.contributor.authorTHALAPILLIL, ARUN M.en_US
dc.date.accessioned2020-06-26T05:09:46Z
dc.date.available2020-06-26T05:09:46Z
dc.date.issued2020-07en_US
dc.identifier.citationJournal of Physics G-Nuclear and Particle Physics, 47(7).en_US
dc.identifier.issn0954-3899en_US
dc.identifier.issn1361-6471en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/4841-
dc.identifier.urihttps://doi.org/10.1088/1361-6471/ab7769en_US
dc.description.abstractSimple extensions of the standard model (SM) with additional right handed neutrinos (RHNs) can elegantly explain the existence of small neutrino masses and their flavor mixings. Collider searches for sterile neutrinos are being actively pursued currently. Heavy RHNs may dominantly decay into ${W}^{\pm }{{\ell }}^{\mp }$ after being produced at the LHC. In this paper, we consider collider signatures of heavy pseudo-Dirac neutrinos in the context of the inverse seesaw scenario, with a sizable mixing with the SM neutrinos under two different flavor structures, viz. flavor diagonal and flavor non-diagonal (FND) scenarios. For the latter scenario we use a general parametrization for the model parameters by introducing an arbitrary orthogonal matrix and nonzero Dirac and Majorana phases. We then perform a parameter scan to identify allowed parameter regions which satisfy all experimental constraints. As an alternative channel to the traditional trilepton signature, we propose the opposite-sign di-lepton signature in the final state, in association with a fat jet from the hadronic decay of the boosted ${W}^{\pm }$. We specifically consider a fat jet topology and explore the required enhancements from exploiting the characteristics of the jet substructure techniques. We perform a comprehensive collider analysis to demonstrate the effectiveness of this channel in both of the scenarios, significantly enhancing the bounds on the RHN mass and mixing angles at the 13 TeV LHC. Interestingly the FND scenario can reach up to a 5-σ limit under the presence of the general parametrization at the high luminosity LHC.en_US
dc.language.isoenen_US
dc.publisherIOP Publishingen_US
dc.subjectLarge Hadron Collideren_US
dc.subjectHeavy sterile neutrinosen_US
dc.subjectFat jeten_US
dc.subjectJet substructureen_US
dc.subjectInverse seesaw mechanismen_US
dc.subjectTOC-JUN-2020en_US
dc.subject2020en_US
dc.subject2020-JUN-WEEK4en_US
dc.titleLooking for minimal inverse seesaw scenarios at the LHC with jet substructure techniquesen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitleJournal of Physics G-Nuclear and Particle Physicsen_US
dc.publication.originofpublisherForeignen_US
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