نتایج جستجو برای: symmetry breaking

تعداد نتایج: 114821  

1998
T. Asaka Masahiro Yamaguchi

A simple hadronic axion model is proposed in the framework of gaugemediated supersymmetry breaking. Dynamics of Peccei-Quinn symmetry breaking is governed by supersymmetry breaking effects and the Peccei-Quinn breaking scale fPQ is inversely proportional to the gravitino mass. The gravitino mass range which corresponds to the axion window fPQ ≃ 109 GeV – 1013 GeV lies in the region predicted by...

1995
James F. Amundson

I calculate heavy-light decay constants in a nonrelativistic potential model. The resulting estimate of heavy quark symmetry breaking connicts with similar estimates from lattice QCD. I show that a semirelativistic potential model eliminates the connict. Using the results of heavy quark eeective theory allows me to identify and compensate for shortcomings in the model calculations in addition t...

2007
Romuald A. Janik Niels A. Obers Peter B. Rønne

We present an explicit construction of the factorization of Seiberg-Witten curves for N = 2 theory with fundamental flavors. We first rederive the exact results for the case of complete factorization, and subsequently derive new results for the case with breaking of gauge symmetry U(Nc) → U(N1)×U(N2). We also show that integrality of periods is necessary and sufficient for factorization in the ...

2004
John McGreevy

We study soft supersymmetry breaking in local models of type II string theory compactifications with branes and fluxes. In such models, magnetic fluxes can be treated as auxiliary fields in N = 2 SUSY multiplets. These multiplets appear as “spurion superfields” in the low-energy effective action for the local model. We discuss the pattern of SUSY breaking from N = 2 to N = 1 to N = 0 in these m...

2008
PETRE BIRTEA RĂZVAN TUDORAN

For simple mechanical systems, bifurcating branches of relative equilibria with trivial symmetry from a given set of relative equilibria with toral symmetry are found. Lyapunov stability conditions along these branches are given.

2009
JOSEPH I. KAPUSTA

We incorporate chiral symmetry breaking in a soft-wall version of the AdS/QCD model by using a modified dilaton profile and a quartic term in the bulk scalar potential. This allows one to separate the dependence on spontaneous and explicit chiral symmetry breaking. The resulting mass spectra in the scalar, vector and axial-vector sectors compares favorably with the respective QCD resonances.

2008
S. Yasui A. Hosaka

We discuss the stability of strangelets by considering dynamical chiral symmetry breaking and confinement. We use a U(3)L×U(3)R symmetric Nambu–Jona-Lasinio model for chiral symmetry breaking supplemented by a boundary condition for confinement. It is shown that strangelets with baryon number A<2×10 can stably exist. For the observables, we obtain the masses and the charge-to-baryon number rati...

2008
Rouven Essig Jean-François Fortin

The regions in the Minimal Supersymmetric Standard Model with the minimal amount of fine-tuning of electroweak symmetry breaking are presented for general messenger scale. No a priori relations among the soft supersymmetry breaking parameters are assumed and fine-tuning is minimized with respect to all the important parameters which affect electroweak symmetry breaking. The superpartner spectra...

2002
T. Biswas C. N. Yang

In this paper, I explain how gauge symmetry can be broken in a geometric way, à la Kaluza-Klein. In higher dimensional gravitational theories, one usually considers the extra dimensions to be “frozen” in time. However, the internal manifold is actually a dynamic entity. For example, its metric can change even if one expects its topological properties to be invariant. It is conceivable then, tha...

2008
MARTA CALANCHI ELIDE TERRANEO

For the equation −∆u = ||x| − 2| α u p−1 , 1 < |x| < 3, we prove the existence of two solutions for α large, and of two additional solutions when p is close to the critical Sobolev exponent 2 * = 2N/(N − 2). A symmetry– breaking phenomenon appears, showing that the least–energy solutions cannot be radial functions.

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