Search results for "BREAKING"

showing 10 items of 383 documents

Yukawa unified supersymmetricSO(10)model: Cosmology, rare decays, and collider searches

2000

It has recently been pointed out that viable sparticle mass spectra can be generated in Yukawa unified SO(10) supersymmetric grand unified models consistent with radiative breaking of electroweak symmetry. Model solutions are obtained only if $\tan\beta \sim 50$, $\mu <0$ and positive $D$-term contributions to scalar masses from SO(10) gauge symmetry breaking are used. In this paper, we attempt to systematize the parameter space regions where solutions are obtained. We go on to calculate the relic density of neutralinos as a function of parameter space. No regions of the parameter space explored were actually cosmologically excluded, and very reasonable relic densities were found in much of…

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyScalar (mathematics)GauginoYukawa potentialFOS: Physical sciencesSupersymmetryParameter spaceHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)NeutralinoHigh Energy Physics::ExperimentSymmetry breakingSO(10)Physical Review D
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Supersymmetric type-II seesaw mechanism: CERN LHC and leptón flavor violating phenomenology

2008

We study the supersymmetric version of the type-II seesaw mechanism assuming minimal supergravity boundary conditions. We calculate branching ratios for lepton flavor violating (LFV) scalar tau decays, potentially observable at the LHC, as well as LFV decays at low energy, such as l{sub i}{yields}l{sub j}+{gamma}, and compare their sensitivity to the unknown seesaw parameters. In the minimal case of only one triplet coupling to the standard model lepton doublets, ratios of LFV branching ratios can be related unambiguously to neutrino oscillation parameters. We also discuss how measurements of soft SUSY breaking parameters at the LHC can be used to indirectly extract information of the seesa…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderHigh Energy Physics::PhenomenologyFísicaSupersymmetryNuclear physicsSeesaw mechanismSeesaw molecular geometrySoft SUSY breakingHigh Energy Physics::ExperimentNeutrino oscillationPhenomenology (particle physics)Lepton
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Finding the Higgs boson through supersymmetry

2009

6 pages, 7 figures.-- PACS nrs.: 12.60.Jv; 13.85.Ni; 14.60.Pq; 14.80.Cp.-- ArXiv pre-print available at: http://arxiv.org/abs/0809.1637

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderSupergravity[PACS] Non-standard-model Higgs bosonsElectroweak interactionBosón de HiggsHigh Energy Physics::Phenomenology[PACS] Supersymmetric unified modelsFOS: Physical sciencesFísicaSupersymmetry[PACS] Neutrino mass and mixingSupersymmetry breaking[PACS] Hadron-induced inclusive production with identified hadrons (energy > 10 GeV)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)SupersimetríaHiggs bosonHigh Energy Physics::ExperimentNeutrino oscillationMinimal Supersymmetric Standard Model
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Supersymmetric Extension of Technicolor &amp; Fermion Mass Generation

2012

We provide a complete extension of Minimal Walking Technicolor able to account for the standard model fermion masses. The model is supersymmetric at energies greater or equal to the technicolor compositeness scale. We integrate out, at the supersymmetry breaking scale, the elementary Higgses. We use the resulting four-fermion operators to derive the low energy effective theory. We then determine the associated tree-level vacuum and low energy spectrum properties. Furthermore we investigate the phenomenological viability of the model by comparing its predictions with electroweak precision tests and experimental bounds on the mass spectrum. We then turn to the composite Higgs phenomenology at…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderSupersymmetry breaking scaleta114010308 nuclear & particles physicsElectroweak interactionMass generationHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical scienceshep-latTechnicolorhep-ph7. Clean energy01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEffective field theoryHiggs boson010306 general physicsMinimal Supersymmetric Standard Model
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Physics at the Large Hadron Collider

2003

Abstract The experiments at the Large Hadron Collider LHC have a large discovery potential for physics beyond the Standard Model and in the investigation of the nature of electroweak symmetry breaking. The large event rates provided by the high luminosity LHC machine will, however, also allow to perform precision measurements of important Standard Model parameters. Both the discovery potential for new physics and the measurements of Standard Model parameters are summarized in the present paper.

PhysicsNuclear and High Energy PhysicsParticle physicsLuminosity (scattering theory)Large Hadron ColliderPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyElectroweak interactionTechnicolorAtomic and Molecular Physics and OpticsStandard ModelNuclear physicsLarge extra dimensionHigh Energy Physics::ExperimentSymmetry breakingNuclear Physics B - Proceedings Supplements
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Anomalous tensor magnetic moments and form factors of the proton in the self-consistent chiral quark-soliton model

2010

We investigate the form factors of the chiral-odd nucleon matrix element of the tensor current. In particular, we aim at the anomalous tensor magnetic form factors of the nucleon within the framework of the SU(3) and SU(2) chiral quark-soliton model. We consider $1/N_c$ rotational corrections and linear effects of SU(3) symmetry breaking with the symmetry-conserving quantization employed. We first obtain the results of the anomalous tensor magnetic moments for the up and down quarks: $\kappa_{T}^{u}=3.56$ and $\kappa_{T}^{d}=1.83$, respectively. The strange anomalous tensor magnetic moment is yielded to be $\kappa_{T}^{s}=0.2\sim -0.2$, that is compatible with zero. We also calculate the co…

PhysicsNuclear and High Energy PhysicsParticle physicsMagnetic momentNuclear TheoryQuark modelHadronHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesElementary particleSymmetry groupHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeSymmetry breakingNucleonSpecial unitary group
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Dynamically generated open and hidden charm meson systems

2006

We will study open and hidden charm scalar meson resonances within two different models. The first one is a direct application of a chiral Lagrangian already used to study flavor symmetry breaking in Skyrme models. In another approach to the problem a SU(4) symmetric Lagrangian is built and the symmetry is broken down to SU(3) by identifying currents where heavy mesons are exchanged and suppressing those. Unitarization in couple channels leads to dynamical generation of resonances in both models, in particular a new hidden charm resonance with mass 3.7 GeV is predicted. The small differences between these models and with previous works will be discussed.

PhysicsNuclear and High Energy PhysicsParticle physicsMesonSpontaneous symmetry breakingHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaStability (probability)Symmetry (physics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentSymmetry breakingCharm (quantum number)Quantum field theoryScalar mesonNuclear Experiment
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Majoron emission in muon and tau decays revisited

2009

9 pages, 4 figures.-- ISI article identifier:000264762400078.-- ArXiv pre-print avaible at: http://arxiv.org/abs/0902.0525

PhysicsNuclear and High Energy PhysicsParticle physicsMuonBranching fractionHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaLepton numberHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)NeutralinoGoldstone bosonHigh Energy Physics::ExperimentSymmetry breakingMajoronLepton
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A consistent study of the the low energy baryon spectrum and the nucleon-nucleon interaction within the chiral quark model

1995

By solving the Schr\"{o}dinger equation for the three-quark system in the hyperspherical harmonic approach, we have studied the low energy part of the nucleon and $\Delta$ spectra using a quark-quark interaction which reproduces the nucleon-nucleon phenomenology. The quark-quark hamiltonian considered includes, besides the usual one-gluon exchange, pion and sigma exchanges generated by the chiral symmetry breaking. The baryonic spectrum obtained is reasonable and the resulting wave function gives consistency to the ansatz used in the two baryon system.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryQuark modelFOS: Physical sciencesFísicaNuclear Theory (nucl-th)Baryonsymbols.namesakePionsymbolsHigh Energy Physics::ExperimentNuclear ExperimentHamiltonian (quantum mechanics)Chiral symmetry breakingNucleonWave functionAnsatzPhysics Letters B
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Dynamical generation of hyperon resonances

2003

In this talk we report on how, using a chiral unitary approach for the meson--baryon interactions, two octets of $J^{\pi}=1/2^-$ baryon states and a singlet are generated dynamically, resulting in the case of strangeness $S=-1$ in two poles of the scattering matrix close to the nominal $\Lambda(1405)$ resonance. We suggest experiments which could show evidence for the existence of these states.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryScatteringHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyHyperonResonanceFOS: Physical sciencesFísicaStrangenessNuclear physicsBaryonNuclear Theory (nucl-th)Matrix (mathematics)Symmetry breakingSinglet stateNuclear Experiment
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