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Phys. Rev. D 76, 115015 (2007) [23 pages]

CERN LHC signals for warped electroweak neutral gauge bosons

Kaustubh Agashe,1,2 Hooman Davoudiasl,3 Shrihari Gopalakrishna,3 Tao Han,4 Gui-Yu Huang,4 Gilad Perez,5,6,7 Zong-Guo Si,8 and Amarjit Soni3
1Department of Physics, Syracuse University, Syracuse, New York 13244, USA
2Maryland Center for Fundamental Physics, Department of Physics, University of Maryland, College Park, Maryland 20742, USA
3Brookhaven National Laboratory, Upton, New York 11973, USA
4Department of Physics, University of Wisconsin, Madison, Wisconsin 53706, USA
5C. N. Yang Institute for Theoretical Physics, State University of New York, Stony Brook, New York 11794-3840, USA
6Jefferson Laboratory of Physics, Harvard University, Cambridge, Massachusetts 02138, USA
7Physics Department, Boston University, Boston, Massachusetts 02215, USA
8Department of Physics, Shandong University, Jinan Shandong 250100, China

Received 14 September 2007; published 27 December 2007

We study signals at the Large Hadron Collider (LHC) for Kaluza-Klein (KK) excitations of the electroweak gauge bosons in the framework with the standard model (SM) gauge and fermion fields propagating in a warped extra dimension. Such a framework addresses both the Planck-weak and flavor hierarchy problems of the SM. Unlike the often studied Z[prime] cases, in this framework, there are three neutral gauge bosons due to the underlying SU(2)L×SU(2)R×U(1)X gauge group in the bulk. Furthermore, couplings of these KK states to light quarks and leptons are suppressed, whereas those to top and bottom quarks are enhanced compared to the SM gauge couplings. Therefore, the production of light quark and lepton states is suppressed relative to other beyond the SM constructions, and the fermionic decays of these states are dominated by the top and bottom quarks, which are, though, overwhelmed by KK gluons dominantly decaying into them. However, as we emphasize in this paper, decays of these states to longitudinal W, Z and Higgs are also enhanced similarly to the case of top and bottom quarks. We show that the W, Z and Higgs final states can give significant sensitivity at the LHC to ~2(3) TeV KK scale with an integrated luminosity of ~100 fb-1 (~1 ab-1). Since current theoretical framework(s) favor KK masses >~3 TeV, a luminosity upgrade of LHC is likely to be crucial in observing these states.

©2007 The American Physical Society

URL: http://link.aps.org/doi/10.1103/PhysRevD.76.115015
DOI: 10.1103/PhysRevD.76.115015
PACS: 12.60.Cn; 11.10.Kk; 12.10.Dm; 12.60.Rc
  • 12.60.Cn
    Extensions of electroweak gauge sector
  • 11.10.Kk
    Field theories in dimensions other than four
  • 12.10.Dm
    Unified theories and models of strong and electroweak interactions
  • 12.60.Rc
    Composite models of unification
  • YEAR: 2007

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