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Third family quasi-yukawa unification: Higgsino dark matter, nlsp gluino, and all that

dc.contributor.authorShafi, Qaisar
dc.contributor.authorTiwari, Amit
dc.contributor.buuauthorÜN, CEM SALİH
dc.contributor.buuauthorÜn, Cem Salih
dc.contributor.departmentFen Edebiyat Fakültesi
dc.contributor.departmentFizik Bölümü
dc.contributor.orcid0000-0002-0595-8803
dc.contributor.researcheridN-3421-2014
dc.date.accessioned2024-11-20T12:18:30Z
dc.date.available2024-11-20T12:18:30Z
dc.date.issued2023-08-18
dc.description.abstractWe explore the implications of third family (t - b - z) quasi-Yukawa unification (QYU) for collider and dark matter (DM) searches within the framework of a supersymmetric SU(4)c x SU(2)L x SU(2)R model. The deviation from exact Yukawa unification is quantified through the relation yt:yb:yz = (1 + C):(1 - C):(1 + 3C), with C being a real parameter (ICI & LE; 0.2). We allow for the breaking of left-right symmetry both by the soft scalar and gaugino mass parameters and obtain a variety of viable solutions that predict the sparticle mass spectrum including the lightest supersymmetric particle (LSP) DM (whose stability is guaranteed by a Z2 gauge symmetry). We highlight solutions that include a next to LSP (NLSP) gluino with mass & SIM;1.3-2.5 TeV, which should be accessible at LHC Run 3. There also exist NSLP stop solutions with masses heavier than about 1.8 TeV, which are consistent with the LSP neutralino dark matter relic density through stop-neutralino coannihilation. We identify A-resonance solutions, which arise when the CP-odd Higgs boson is in resonance with a pair of LSP neutralinos (mA = 2m & chi;& SIM;01) with DM mass & SIM;0.8-2 TeV, as well as bino-chargino, bino-slepton and bino-stau coannihilation scenarios. Finally, we also identify Wino-like (& SIM;99%) and Higgsino-like (& SIM;99%) solutions whose masses are heavier than about 1.5 and 1 TeV, respectively. These solutions are compatible with the desired dark matter relic density and testable in ongoing and future direct detection experiments.
dc.description.sponsorshipBartol Research Institute, University of Delaware
dc.description.sponsorshipMinistry of Science and Innovation, Spain (MICINN) Spanish Government PID2019 - 107844GB-C22
dc.description.sponsorshipCEAFMC
dc.description.sponsorshipUniversidad de Huelva High Performance Computer (HPC@UHU) in the Campus Universitario el Carmen
dc.description.sponsorshipSpanish Government UNHU-15CE-2848
dc.identifier.doi10.1103/PhysRevD.108.035027
dc.identifier.issn2470-0010
dc.identifier.issue3
dc.identifier.scopus2-s2.0-85168832442
dc.identifier.urihttps://doi.org/10.1103/PhysRevD.108.035027
dc.identifier.urihttps://hdl.handle.net/11452/48231
dc.identifier.volume108
dc.identifier.wos001058588900005
dc.indexed.wosWOS.SCI
dc.language.isoen
dc.publisherAmer Physical Soc
dc.relation.journalPhysical Review D
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi
dc.rightsinfo:eu-repo/semantics/openAccess
dc.subjectTop-quark
dc.subjectElectroweak
dc.subjectPredictions
dc.subjectSupersymmetry
dc.subjectParticle
dc.subjectSpheno
dc.subjectScience & technology
dc.subjectPhysical sciences
dc.subjectAstronomy & astrophysics
dc.subjectPhysics, particles & fields
dc.subjectPhysics
dc.titleThird family quasi-yukawa unification: Higgsino dark matter, nlsp gluino, and all that
dc.typeArticle
dspace.entity.typePublication
local.contributor.departmentFen Edebiyat Fakültesi/Fizik Bölümü
local.indexed.atWOS
local.indexed.atScopus
relation.isAuthorOfPublication0c6ad07c-f6f6-4949-a2f0-e288af6b9411

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