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New Ideas in RandallSundrum Phenomenology

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Randall-Sundrum Phenomenology. Jos Santiago. Theory Group (FNAL) ... Collider Phenomenology. Tevatron. Searches for new quarks ... – PowerPoint PPT presentation

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Title: New Ideas in RandallSundrum Phenomenology


1
New Ideas in Randall-Sundrum Phenomenology
  • José Santiago
  • Theory Group (FNAL)

2
The goods and the bads of the old RS
The Goods of RS
The Not so Goods of RS
Solution to the gauge hierarchy problem
Gauge boson KK modes near IR large T
Higgs
(t,b) near IR large anomalous Zbb
Fermion masses hierarchical with FCNC naturally
absent for light fermions
3
The bads of the old RS T parameter
Gauge KK modes are localized near the IR brane
Large mixing with the Z and W zero modes through
the Higgs
Large T parameter
4
The bads of the old RS Zbb coupling
Top (bottom) zero modes are localized near the IR
brane
Large gauge and Yukawa couplings to GB and
fermion KK modes
Large anomalous Zbb coupling
5
New Ideas custodial symmetry
  • Custodial protection of Randall-Sundrum
  • Bulk Gauge Symmetry

Agashe, Delgado, May, Sundrum JHEP (03)
6
New Ideas custodial symmetry
  • Custodial protection of Randall-Sundrum
  • Bulk Gauge Symmetry

Agashe, Contino, Da Rold, Pomarol ph/0605341
7
Fermion Quantum Numbers
The simplest option is bidoublets under
The Higgs is also a bidoublet with
8
Custodial protection of T and Zbb
  • T and Zbb protected by custodial symmetry broken
    by b.c. only on the UV brane Insensitive to UV
    physics
  • Quantum corrections are calculable
  • T and Zbb do not receive corrections above
  • One loop corrections are typically sizable
  • Triplets contribute negative to T
  • Singlets contribute positive to T
  • Large positive T leads to large positive

9
Quantum corrections to T and Zbb
T negative in most of parameter space RH top
almost flat
UV singlet localization IR
Positive T leads to large deviations in Zbb
10
Global Fit to Electroweak Observables
  • We have performed a global fit to all relevant
    electroweak precision observables including
  • All tree-level effects at leading order in
  • Leading one loop effects S and T parameters and
    Zbb
  • We compute the as a function of the
    localization parameter of the fermion zero modes
  • Zbb coupling and the S parameter are the most
    restrictive observables when the light fermions
    are near the UV brane
  • Loss of universality when light fermions near the
    IR brane

Carena, Ponton, J.S., Wagner hep-ph/0612nnn
11
Result of the Global Fit
IR light localization UV
S can receive corrections from physics above the
UV cut-off
12
Spectrum
First two generation KK modes
Not a necessary prediction
13
Typical Spectrum
Third generation KK modes
Solid prediction
14
Collider Phenomenology
  • Tevatron
  • Searches for new quarks
  • Interesting possibilities for Higgs physics
  • LHC
  • discovery up to 1 TeV
  • Exciting Higgs physics
  • Exotic decay channels

15
Tevatron searches
16
Conclusions
  • Custodial protection T and Zbb in RS Light gauge
    boson KK modes accessible at the LHC
  • T and Zbb are insensitive to UV physics
    calculable and relevant
  • Global fit to EW precision observables taking
    into account all relevant one loop corrections
  • Light quarks 300-600 GeV accessible at Tevatron
    and LHC
  • Interesting collider implications
  • Interesting Higgs physics
  • Exotic decay channels

17
New quarks at the Tevatron
CDF Note 8495
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