meta-stable supersymmetry breaking in an n=1 perturbed seiberg-witten theory
DESCRIPTION
Meta-stable Supersymmetry Breaking in an N=1 Perturbed Seiberg-Witten Theory. Shin Sasaki (Univ. of Helsinki, Helsinki Inst. of Physics) Phys. Rev. D76 (2007) 125009, arXiv:0708.0668 [hep-th] JHEP 03 (2008) 004, arXiv:0712.4252 [hep-th] (M.Arai, C.Montonen, N.Okada and S.S). SQCD. - PowerPoint PPT PresentationTRANSCRIPT
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Meta-stable Supersymmetry Breaking in an N=1 Perturbed Seiberg-Witten Theory
Shin Sasaki(Univ. of Helsinki, Helsinki Inst. of Physics)
Phys. Rev. D76 (2007) 125009, arXiv:0708.0668 [hep-th]JHEP 03 (2008) 004, arXiv:0712.4252 [hep-th]
(M.Arai, C.Montonen, N.Okada and S.S)
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• Dynamical SUSY breakinghierarchy problem can be solved [Witten (1981)]
• Witten index – # of SUSY vacua in a model [Witten (1982)]
very restricted models have been considered before the discovery of the ISS model
meta-stable SUSY breaking vacua
IntroductionMeta-stable SUSY breaking?
[Intriligator-Seiberg-Shih (2006)]
N=2 SQCD non-perturbative analysis is possible
SQCD
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Four-dimensional N=2 SQCD with FI term perturbation
Massless fundamental hypermultiplets, preserves N=2 SUSY
Gauge group is
Simple case
Quantum Theory – Seiberg-Witten analysis [Seiberg-Witten (1994)]
There is a meta-stable SUSY breaking vacuumat the dyon singular point in the moduli space
Exact effective potential can be obtained andstational point was analyzed
[Arai-Montonen-Okada-S.S, arXiv:0708.0668 [hep-th]]
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The model[Arai-Montonen-Okada-S.S, arXiv:0712.4252 [hep-th]]
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N=1 preserving adjoint scalar mass deformation to N=2 SQCD
Classical SUSY vacua on the Coulomb branch
Classical SUSY vacua on the Higgs branch
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Quantum theory
Modulus
Coulomb branch in vanishing FI term
U(1) gauge theory cutoff theory, Landau pole
[Arai-Okada (2001)]U(1) part is always weak
Moduli space is constrained
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Vector multiplet part
Hypermultiplets
Light BPS states around singular points in moduli space
M corresponds to dyons, monopoles, quarks
SUSY preserving part
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Stational points in Hypermultiplet directions
Energies corresponding to these solutions are
Energetically favored at singular points in the moduli space
This solution is stable in M directions
Let us find out stational point in the directionsExplicit form of the metric on the moduli space is needed
The potential is a function
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Moduli space
Monodoromy transf. subgroup of
Same structure with SU(2) massive SQCD (common quark hypermultiplet mass)
Prepotential Metric of the moduli space is determined
C is a free parameter which defines the Landau pole scale [Arai-Okada (2001)]
The structure of the potential is completely determined
can be regarded as the mass
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Now, the potential is a function of which has been minimized in thedirections due to the non-zero condensation of monopoles, dyons, quarks.
In the moduli space, the singular points are completely determined by the cubic polynomial [Seiberg-Witten (1994)] There is a relation between and at each singular points
At the singular points, the potential is a function of only!
There are three singularities in our model (dyons, monople, quark)
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Degenerate dyon and monopole
Left and right dyonsand quark
Flow of singularities (real part of )
Flow of singularities for complex is essentially the same with
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First, consider case
Numerical analysis
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Potential behavior around the monopole singular point
Potential plotComplex
SUSY vacuum at
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Potential around dyon singular points
SUSY vacuum at
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Global structure of the potential, case
monopole
Left, right dyons right dyon
quark
SUSY vacua
SUSY vacua atat dyons and monopole points
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Turn on
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Izawa-Yanagida-Intriligator-Thomas (IYIT) mechanism
If we turn on which produce a vacuum at a point different from as SUSY vacua, the full effective action would contain SUSY breaking vacua
This is similar to the Izawa-Yanagida-Intriligator-Thomas (IYIT) model
U(1) part is essential in our model
[Izawa-Yanagida (1996), Intriligator-Thomas (1996)]
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Potential behavior at monopole singular point, case
Two SUSY breaking local minima at the degenerated dyon and monopole singular points
The behavior of the degenerate dyon singular point is the same withthe monopole one symmetry
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Global structure of the full potential
Meta-stable SUSY breakingminima
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Decay rate estimation
Higgs branch no quantum corrections Classical SUSY vacua remains intact
The bounce action can be estimated from the classical potential
can be taken to be large meta-stable vacua
Coulomb branch
Higgs branch
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• gauge theory with hypermultiplets perturbed by adjoint
mass and FI-terms• We have found meta-stable SUSY breaking
vacua in the non-perturbative effective potential via the Seiberg-Witten analysis
• Long-lived local minimum• The SUSY breaking mechanism presented
here is similar to the one in the IYIT model• Generalization to arbitrary by the help
of brane configurations
Summary and perspective