mssm in the bulk of rs spacetime - osaka u
TRANSCRIPT
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MSSM in the Bulk of RS Spacetime
Toshifumi YamadaSokendai, KEK
in collaboration with Nobuchika Okada (Univ. of Alabama)
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Contents
• Introduction
• Setup
• SUSY breaking mass spectrum
• Numerical analysis on mass spectrum
• Summary and outlook
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Introduction
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Basic Structure• Consider 5D Minimal SUSY Standard Model
on Randall-Sundrum background.
• RS Kaluza-Klein scale is at an intermediate scale.
• SUSY solves the gauge hierarchy problem. RS spacetime naturally explains the Yukawa coupling hierarchy.
• SUSY breaking soft mass comes from two origins : Contact terms on IR brane (“Gravity Mediation”) RG effects of gaugino mass (“Gaugino Mediation”)
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Features
• The same extradimensional sequestering controls Yukawa coupling hierarchy and Gravity mediation contribution to matter soft mass.
• It may be possible to reveal the extradimensionalorigin of Yukawa hierarchy by observing Flavor-Violating parts of matter soft mass.
coming from gravity mediation
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Setup
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Setup
• Higgs and SUSY breaking sector : on IR
• Matter and Gauge superfields : in the Bulk
• Zero-modes of 3rd generation : lean towards IR. Zero-modes of 1st generation : lean towards UV.7
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5D Profiles of Superfields
• 5D chiral superfield Lagrangian :
Zero-mode profile :
• 5D gauge superfield
Zero-mode profile :
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Yukawa couplings• For MSSM matter fields, , denote
their overlaps with IR brane, , as
have exponential hierarchy with .
• 4D Yukawa matrices take the form :
Eigenvalues :
CKM matrix takes the form :
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Neutrino Mass
• Neutrino mass may arise from higher dim. operators on IR brane or from seesaw.
• Whichever is the case, neutrino mass arises from the term :
and we have
in the basis of charged lepton mass eigenstate.
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Comparison with Data (Quark)
• From Top Yukawa, .
• From observed CKM matrix, we have
with .
• From observed fermion masses, we have
…….
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Comparison with Data (Lepton)
• Since the neutrino mass matrix has democratic structure, we have
.
• From observed lepton masses, we have
.
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SUSY Breaking Mass Spectrum
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Overview
• At KK scale, no field propagates in the bulk.
SUSY breaking mass arises from contact terms on IR brane.
• Below KK scale, fields propagate in the bulk.
SUSY breaking effects are mediated by radiative corrections in the bulk, especially by renormalization group contributions.
• term arises only from SUSY breaking effects. ( Giudice-Masiero mechanism) 14
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At KK Scale• SUSY breaking terms simply arise from
higher dim. operators on IR brane.
• They are proportional to their resp. overlaps with IR brane.
Gaugino mass :
Matter soft mass : , , …
A-terms :
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At Low Energies
• Low-energy spectrum is calculable by solving MSSM RGE with the initial condition in the previous slide.
• In particular, RG of gauginos generates large diagonal soft mass of matter sparticles,
(hence the name “gaugino mediation”)
which suppresses flavor-violating effects of SUSY breaking terms.
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Gravity Mediation vs. Minimal Flavor Violation
• RG of Yukawa couplings also induces flavor off-diagonal soft mass of SU(2) doublet sparticles. (Minimal flavor violation (MFV))
1. For doublet sparticles, GM effects surpass MFV effects, as is shown below :
It is sufficient to consider only GM effects.
2. For singlet sparticles, only GM effects exist.
Flavor-violating singlet soft mass is unique to our model. 17
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LSP and NLSP
• LSP is gravitino with mass :
• NLSP mostly consists of singlet sleptons. Its flavor composition is characteristic to the model.
(as we will see later)
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Numerical Analysis
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Purpose of Analysis
To numerically check that the model gives realistic mass spectra evading experimental constraints on flavor.
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Calculating Mass Spectrum• With the initial conditions below, we solved
MSSM RGE to derive low energy spectrum.
• As we allow O(1) ambiguity of grav. med. terms, we fixed :
• The free parameters of mass spectrum are :
with the condition . 21
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Low-energy Constraints
• Of all low-energy experiments on flavor,m experiment most severely constrains the model because of flavor-universal s.
• It gives strong limits on Flavor-violating A-term :
Flavor-violating soft mass :
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Samples of Realistic Spectrum• For various values of ,
we calculated mass spectrum and compared it with experimental bounds on and . ( , )
• Table of realistic mass spectra below :
• For smaller / , the bound on unsatisfied.
• For larger / , the bound on unsatisfied.23
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General Consequences1. We have in this model.
The order of the flavor-violating A-term, , is fixed at and it induces event.
Yukawa couplings and A-terms from grav. med. are rooted on the same 5D structure.
2. = “singlet stau localized towards IR” is favored.
Since s are flavor-universal, the bound on severely constrains . (Note that )
(c.f. are resp. suppressed by .)24
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Signatures at LHC
• “General consequence 2” suggests that singlet slepton mass matrix is significantly distorted by gravity mediation.
• Unusual selectron-like NLSP is the case for sample spectra in the table.
• Rate of rare decay of NLSP (e.g. selectron-like NLSP decaying into tau) is predictable in our model.
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Summary and Outlook
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Summary and Outlook
• Studied 5D MSSM on warped background.
• 5D disposition of MSSM superfields provides a natural explanation to Yukawa hierarchy and a viable SUSY breaking mechanism (gaugino mediation + gravity mediation).
• Signatures of the model were discussed.
• Study on rare decay of singlet scharm and smuon at ILC will prove the model.
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