Download - New Ideas in Randall-Sundrum Phenomenology
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With M. Carena, E. Pontón and C. Wagner, NPB759 (06) and hep-ph/0612nnn
New Ideas in Randall-Sundrum Phenomenology
José Santiago
Theory Group (FNAL)
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The goods and the bads of the old RS
Higgs
Fermion masses hierarchical with FCNC naturally absent
for light fermions
Solution to the gauge hierarchy
problem
The Goods of RS The Not so Goods of RS
Gauge boson KK modes near IR: large
T
(t,b) near IR: large anomalous Zbb
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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
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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
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New Ideas: custodial symmetry
Custodial protection of Randall-Sundrum:
Bulk Gauge Symmetry:
Agashe, Delgado, May, Sundrum JHEP (03)
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New Ideas: custodial symmetry
Custodial protection of Randall-Sundrum:
Bulk Gauge Symmetry:
Agashe, Contino, Da Rold, Pomarol ph/0605341
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Fermion Quantum Numbers
The simplest option is bidoublets under
The Higgs is also a bidoublet with
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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
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UV singlet localization IR
Quantum corrections to T and Zbb
T negative in most of parameter space: RH top
almost flat
Positive T leads to large deviations in Zbb
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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
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Result of the Global Fit
S can receive corrections from physics above the UV cut-off
IR light localization UV
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Spectrum
First two generation KK modes
Not a necessary prediction
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Typical Spectrum
Third generation KK modes
Solid prediction
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Collider Phenomenology
Tevatron
Searches for new quarks
Interesting possibilities for Higgs physics
LHC
discovery up to 1 TeV
Exciting Higgs physics
Exotic decay channels
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Tevatron searches
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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
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New quarks at the Tevatron
CDF Note 8495