Search results for "Symmetry Breaking"

showing 10 items of 319 documents

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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Configuration mixing and total muon capture rates

1973

Abstract We modify the Primakoff closure approximation to get independence on the mean neutrino energy and energy weighted sum rules are used for the corrective terms. A near model - independent discussion is then possible, and the total rates are shown to be a very sensitive tool to investigate configuration mixing of the target. Wild discrepancies with experiment would arise if the limit of pure jj or LS couplings are used for 12 C, whereas the Cohen-Kurath wave function gives a very good result.

PhysicsNuclear and High Energy PhysicsParticle physicsFísicaMuon captureNuclear physicsClosure (computer programming)Limit (mathematics)Symmetry breakingNeutrinoWave functionMixing (physics)Independence (probability theory)Nuclear Physics
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SU(4) breaking, allowed transitions and total muon capture rates in nuclei

1973

The authors study muon capture rates in light nuclei and show that one can evaluate them in a model-independent way by correcting the Primakoff closure approximation to the first order in the neutrino energy dependence. In this framework the interplay between the existence of allowed transitions and SU(4) breaking is analyzed. In the correction to the first order in the neutrino energy dependence by a sum rule, Majorana and SU(4) breaking potentials are taken into account. The method is also applied to single multipolar transitions, in particular for the dipole transitions. General considerations are illustrated for /sup 6/Li and /sup 12/C by explicit calculations. The stability of the resu…

PhysicsNuclear and High Energy PhysicsParticle physicsFísicaMuon captureNuclear physicsMAJORANADipoleMatrix (mathematics)Symmetry breakingSum rule in quantum mechanicsNeutrinoMixing (physics)Nuclear Physics
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Meson-meson interactions in a nonperturbative chiral approach

1999

A non-perturbative method which combines constraints from chiral symmetry breaking and coupled channel unitarity is used to describe the meson-meson interaction up to about 1.2 GeV. The approach uses the O(p^2) and O(p^4) chiral Lagrangians. The seven free parameters of the O(p^4) Lagrangian are fitted to the data. The results are in good agreement with a vast amount of experimental analyses. The amplitudes develop poles in the complex plane corresponding to the f0, a0, rho, K*, phi, sigma and kappa resonances; the latter two, very broad. The total and partial decay widths of the resonances are also well reproduced. Further extensions and applications of this chiral non-perturbative scheme …

PhysicsNuclear and High Energy PhysicsParticle physicsFísica-Modelos matemáticosNuclear TheoryUnitarityMesonHigh Energy Physics::LatticePartial wave analysisHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesNuclear Theory (nucl-th)RenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)BibliographyFísica matemáticaHigh Energy Physics::ExperimentPi interactionChiral symmetry breakingComplex plane
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Dynamical Symmetry Breaking in Warped Compactifications

2001

We study dynamical electroweak symmetry breaking in the Randall-Sundrum scenario. We show that one extra dimension is enough to give the correct pattern of electroweak symmetry breaking in a simple model with gauge bosons and the right-handed top quark in the bulk. The top quark mass is also in agreement with experiment. Furthermore, we propose an extended scenario with all Standard Model gauge bosons and fermions propagating in the bulk, which naturally accommodates the fermion mass hierarchies. No new fields or interactions beyond the observed in the Standard Model are required.

PhysicsNuclear and High Energy PhysicsParticle physicsGauge bosonSpontaneous symmetry breakingHigh Energy Physics::LatticeElectroweak interactionHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesTechnicolorTop quark condensateExplicit symmetry breakingHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Symmetry breakingChiral symmetry breaking
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Dynamical left-right symmetry breaking.

1995

We study a left--right symmetric model which contains only elementary gauge boson and fermion fields and no scalars. The phenomenologically required symmetry breaking emerges dynamically leading to a composite Higgs sector with a renormalizable effective Lagrangian. We discuss the pattern of symmetry breaking and phenomenological consequences of this scenario. It is shown that a viable top quark mass can be achieved for the ratio of the VEVs of the bi--doublet $\tan\beta\equiv\kappa/\kappa'$ =~ 1.3--4. For a theoretically plausible choice of the parameters the right--handed scale can be as low as $\sim 20 TeV$; in this case one expects several intermediate and low--scale scalars in addition…

PhysicsNuclear and High Energy PhysicsParticle physicsGauge bosonSpontaneous symmetry breakingHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesHiggs sectorStandard ModelHiggs fieldExplicit symmetry breakingHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentSymmetry breakingPhysical review. D, Particles and fields
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Search for supersymmetry in pp collisions at s=7 TeV in final states with missing transverse momentum and b-jets

2011

Results are presented of a search for supersymmetric particles in events with large missing transverse momentum and at least one heavy flavour jet candidate in sqrt{s} = 7 TeV proton-proton collisions. In a data sample corresponding to an integrated luminosity of 35 pb-1 recorded by the ATLAS experiment at the Large Hadron Collider, no significant excess is observed with respect to the prediction for Standard Model processes. For R-parity conserving models in which sbottoms (stops) are the only squarks to appear in the gluino decay cascade, gluino masses below 590 GeV (520 GeV) are excluded at the 95% C.L. The results are also interpreted in an MSUGRA/CMSSM supersymmetry breaking scenario w…

PhysicsNuclear and High Energy PhysicsParticle physicsGluinoLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyATLAS experimentSupersymmetry01 natural sciencesSupersymmetry breakingStandard ModelNuclear physicsR-parity0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsMinimal Supersymmetric Standard ModelPhysics Letters B
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