Single production of composite electrons at future sppc-based lepton–hadron colliders

MakaleAçık Erişim

Özet

We consider the production of excited electrons with spin-1/2 at future SPPC-based electron–proton colliders with center-of-mass energies of 8.4, 11.6, 26.6, and 36.8 TeV. These exotic particles are predicted in the composite models. We calculate the production cross sections and concentrate on the photon decay channel of the excited electrons with the process of ep → e*X → eγX. The pseudo rapidity and transverse momentum distributions of the electrons and photons in the final state have been plotted to determine the kinematical cutoffs best suited for discovery of the excited electrons. By applying these cutoffs we compute 2σ, 3σ, and 5σ contour plots of the statistical significance of the expected signal in the parameter space (L, m*), where L denotes the integrated luminosity of the collider and m* is the mass of the composite electrons.

Anahtar Kelimeler

RDL Kalıcı Bağlantı (PID)
https://rdlopen.rawdatalibrary.net/r/gumushane/14860Resmi atıflarda kullanılan kalıcı adres
DOI
https://doi.org/10.1139/cjp-2019-0216Yayıncı resmi DOI adresi
Tam Kayıt
AlanDeğerDil
dc.contributor.authorCaliskan, A.
dc.date.accessioned2026-10-22T10:23:14.742844353Z
dc.date.available2026-10-22T10:23:14.742844353Z
dc.date.issued2020
dc.description.abstractWe consider the production of excited electrons with spin-1/2 at future SPPC-based electron–proton colliders with center-of-mass energies of 8.4, 11.6, 26.6, and 36.8 TeV. These exotic particles are predicted in the composite models. We calculate the production cross sections and concentrate on the photon decay channel of the excited electrons with the process of ep → e*X → eγX. The pseudo rapidity and transverse momentum distributions of the electrons and photons in the final state have been plotted to determine the kinematical cutoffs best suited for discovery of the excited electrons. By applying these cutoffs we compute 2σ, 3σ, and 5σ contour plots of the statistical significance of the expected signal in the parameter space (L, m*), where L denotes the integrated luminosity of the collider and m* is the mass of the composite electrons.
dc.description.sponsorshipTürkiye Bilimsel ve Teknolojik Araştirma Kurumu, TÜBITAK, (114F337)
dc.identifier.doi10.1139/cjp-2019-0216
dc.identifier.eissn1208-6045
dc.identifier.endpage356
dc.identifier.issn0008-4204
dc.identifier.issue4
dc.identifier.scopus2-s2.0-85082858636
dc.identifier.startpage349
dc.identifier.urihttps://rdlopen.rawdatalibrary.net/r/gumushane/14860
dc.identifier.volume98
dc.identifier.wosWOS:000522811700004
dc.language.isoen
dc.publisherCanadian Science Publishing
dc.relation.ispartofCanadian Journal of Physics
dc.rightsinfo:eu-repo/semantics/openAccess
dc.subjectCross sections
dc.subjectExcited electrons
dc.subjectExcited leptons
dc.subjectFuture colliders
dc.subjectSPPC
dc.subject.classificationPhysics, Multidisciplinary
dc.subject.classificationPhysics
dc.subject.otherDynamic mechanical analysis
dc.subject.otherExcited states
dc.subject.otherPhotons
dc.subject.otherCenter-of-mass energies
dc.subject.otherCross sections
dc.subject.otherExcited electrons
dc.subject.otherExcited leptons
dc.subject.otherIntegrated luminosity
dc.subject.otherProduction cross section
dc.subject.otherSPPC
dc.subject.otherStatistical significance
dc.subject.otherElectrons
dc.titleSingle production of composite electrons at future sppc-based lepton–hadron colliders
dc.typeArticle
dspace.entity.typePublication
rdl.citation.openalex3
rdl.citation.scopus2
rdl.citation.wos2
rdl.oa.statusgreen
rdl.oa.urlhttps://utoronto.scholaris.ca/bitstreams/b6a3150d-8208-4b3b-92a3-a4e65a652f69/download
rdl.source.indexSCOPUS
rdl.source.indexWOS
rdl.wos.indexScience Citation Index Expanded (SCI-EXPANDED)