Search results for "BREAKING"

showing 10 items of 383 documents

LHC and lepton flavour violation phenomenology of a left-right extension of the MSSM

2010

We study the phenomenology of a supersymmetric left-right model, assuming minimal supergravity boundary conditions. Both left-right and (B-L) symmetries are broken at an energy scale close to, but significantly below the GUT scale. Neutrino data is explained via a seesaw mechanism. We calculate the RGEs for superpotential and soft parameters complete at 2-loop order. At low energies lepton flavour violation (LFV) and small, but potentially measurable mass splittings in the charged scalar lepton sector appear, due to the RGE running. Different from the supersymmetric “pure seesaw” models, both, LFV and slepton mass splittings, occur not only in the left-but also in the right slepton sector. …

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsSuperpotentialHigh Energy Physics::PhenomenologyFOS: Physical sciencesOrder (ring theory)Física01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanismSeesaw molecular geometrySupersymmetry Phenomenology0103 physical sciencesHigh Energy Physics::ExperimentSymmetry breakingNeutrino010306 general physicsPhenomenology (particle physics)Lepton
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Lepton-number violation and right-handed neutrinos in Higgs-less effective theories

2005

Following previous work, we identify a symmetry S_nat that generalizes the concept of custodial symmetry, keeping under control deviations from the Standard Model (SM). To realize S_nat linearly, the space of gauge fields has to be extended. Covariant constraints formulated in terms of spurions reduce S_nat back to SU(2)_L x U(1)_Y. This allows for a covariant introduction of explicit S_nat-breaking parameters. We assume that S_nat is at play in a theory of electroweak symmetry-breaking without a light Higgs particle. We describe some consequences of this assumption, using a non-decoupling effective theory in which the loop expansion procedure is based on both momentum and spurion power cou…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theory010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesLepton numberCustodial symmetryStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]0103 physical sciencesEffective field theoryHiggs bosonSymmetry breaking010306 general physics
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Chiral Perturbation Theory with tensor sources

2007

23 pages, 1 figure.-- ISI Article Identifier: 000249788800051.-- ArXiv pre-print available at: http://arxiv.org/abs/0705.2948

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryCurrent (mathematics)MesonBar (music)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyOrder (ring theory)SigmaFOS: Physical sciencesQCDSpontaneous Symmetry BreakingHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Nonperturbative EffectssymbolsTensorChiral lagrangiansLagrangianMathematical physics
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A non-perturbative chiral approach for meson-meson interactions

2000

A non-perturbative method which combines constraints from chiral symmetry breaking and coupled channel unitarity is used to describe meson-meson interactions up to \sqrt{s}\lesssim 1.2 GeV, extending in this way the range of applicability of the information contained in Chiral Perturbation Theory (\chi PT), since this perturbative series is typically restricted to \sqrt{s}\lesssim 500 MeV. The approach uses the O(p^2) and O(p^4) \chiPT Lagrangians. The seven free parameters resulting from the O(p^4) Lagrangian are fitted to the experimental data. The approach makes use of the expansion of T^{-1} instead of the amplitude itself as done in \chiPT. The former expansion is suggested by analogy …

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryFísica-Modelos matemáticosSeries (mathematics)MesonUnitarityFísicaFOS: Physical sciencesHigh Energy Physics - PhenomenologyAmplitudeHigh Energy Physics - Phenomenology (hep-ph)Física matemáticaNon-perturbativeChiral symmetry breakingFree parameter
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Power counting in baryon chiral perturbation theory including vector mesons

2003

It is demonstrated that using a suitable renormalization condition one obtains a consistent power counting in manifestly Lorentz-invariant baryon chiral perturbation theory including vector mesons as explicit degrees of freedom.

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear TheoryMesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyDegrees of freedom (statistics)FOS: Physical sciencesPower (physics)Nuclear Theory (nucl-th)RenormalizationBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Chiral symmetry breakingNuclear theoryPhysics Letters B
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Phenomenology of dark matter from A(4) flavor symmetry

2011

We investigate a model in which Dark Matter is stabilized by means of a Z2 parity that results from the same non-abelian discrete flavor symmetry which accounts for the observed pattern of neutrino mixing. In our A4 example the standard model is extended by three extra Higgs doublets and the Z2 parity emerges as a remnant of the spontaneous breaking of A4 after electroweak symmetry breaking. We perform an analysis of the parameter space of the model consistent with electroweak precision tests, collider searches and perturbativity. We determine the regions compatible with the observed relic dark matter density and we present prospects for detection in direct as well as indirect Dark Matter s…

PhysicsNuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsDark matterElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaParity (physics)Parameter space01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHiggs bosonHigh Energy Physics::ExperimentSymmetry breakingNeutrino010306 general physicsPhenomenology (particle physics)Astrophysics - Cosmology and Nongalactic Astrophysics
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Naturality, unification and dark matter

2010

We consider a model where electroweak symmetry breaking is driven by technicolor dynamics with minimal particle content required for walking coupling and saturation of global anomalies. Furthermore, the model features three additional Weyl fermions singlet under technicolor interactions, two of which provide for a one-loop unification of the standard model gauge couplings. Among these extra matter fields exists a possible candidate for weakly interacting dark matter. We evaluate the relic densities and find that they are sufficient to explain the cosmological observations and avoid the experimental limits from earth-based searches. Hence, we establish a nonsupersymmetric framework where hie…

PhysicsNuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsDark matterElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesTechnicolorFermion01 natural sciencesStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesGrand Unified TheorySymmetry breakingQuantum field theory010306 general physicsAstrophysics - Cosmology and Nongalactic Astrophysics
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Collider signals of gravitino dark matter in bilinearly broken R-parity

2005

In models with gauge mediated supersymmetry breaking the gravitino is the lightest supersymmetric particle. If R-parity is violated the gravitino decays, but with a half-live far exceeding the age of the universe and thus is, in principle, a candidate for the dark matter. We consider the decays of the next-to-lightest supersymmetric particle, assumed to be the neutralino. We show that in models where the breaking of R-parity is bilinear, the condition that R-parity violation explains correctly the measured neutrino masses fixes the branching ratio of the decay ${\tilde \chi}^0_1 \to {\tilde G}\gamma$ in the range $10^{-3}-10^{-2}$, if the gravitino mass is in the range required to solve the…

PhysicsNuclear and High Energy PhysicsParticle physicsDark matterHigh Energy Physics::PhenomenologyFísicaOrder (ring theory)FOS: Physical sciencesSupersymmetry breakingLightest Supersymmetric ParticleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)R-parityNeutralinoGravitinoHigh Energy Physics::ExperimentNeutrino
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Self-consistent variational approach to the minimal left-right symmetric model of electroweak interactions

2006

The problem of mass generation is addressed by a Gaussian variational method for the minimal left-right symmetric model of electroweak interactions. Without any scalar bidoublet, the Gaussian effective potential is shown to have a minimum for a broken symmetry vacuum with a finite expectation value for both the scalar Higgs doublets. The symmetry is broken by the fermionic coupling that destabilizes the symmetric vacuum, yielding a self consistent fermionic mass. In this framework a light Higgs is only compatible with the existence of a new high energy mass scale below 2 TeV.

PhysicsNuclear and High Energy PhysicsParticle physicsElectroweak gauge sector quantum field theoryMass generationScalar (mathematics)Electroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesSymmetry (physics)Theoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Variational methodHiggs bosonInvariant massSymmetry breaking
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Sparticle Mass Spectra from SO(10) Grand Unified Models with Yukawa Coupling Unification

1999

We examine the spectrum of superparticles obtained from the minimal SO(10) grand unified model, where it is assumed the gauge symmetry breaking yields the Minimal Supersymmetric Standard Model (MSSM) as the effective theory at $M_{GUT}\sim 2\times 10^{16}$ GeV. In this model, unification of Yukawa couplings implies a value of $\tan\beta\sim 45-55$. At such high values of $\tan\beta$, assuming universality of scalar masses, the usual mechanism of radiative electroweak symmetry breaking breaks down. We show that a set of weak scale sparticle masses consistent with radiative electroweak symmetry breaking can be generated by imposing non-universal GUT scale scalar masses consistent with univers…

PhysicsNuclear and High Energy PhysicsParticle physicsElectroweak interactionHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesSupersymmetryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Effective field theoryHigh Energy Physics::ExperimentSymmetry breakingSO(10)Minimal Supersymmetric Standard ModelGauge symmetry
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