Search results for "Weak"

showing 10 items of 1417 documents

Supersymmetric electroweak baryogenesis

1999

We calculate the baryon asymmetry generated at the electroweak phase transition in the minimal supersymmetric standard model, using a new method to compute the CP-violating asymmetry in the Higgsino flux reflected into the unbroken phase. The method is based on a Higgs insertion expansion. We find that the CP asymmetry at leading order is proportional to the change in $\tan \beta$ in the bubble wall, which is at most of order $10^{-2}$, while at next-to-leading order this suppression factor disappears. This result may enhance the final baryon asymmetry generated during the electroweak phase transition for small $\Delta \beta (< 10^{-3}$).

PhysicsPhase transitionParticle physicsNuclear and High Energy Physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyElectroweak interactionFOS: Physical sciencesFísicaAsymmetryAtomic and Molecular Physics and OpticsBaryogenesisHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Baryon asymmetryHiggs bosonHigh Energy Physics::ExperimentHiggsinoMinimal Supersymmetric Standard Modelmedia_commonNuclear Physics B - Proceedings Supplements
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Lepton asymmetries and primordial hypermagnetic helicity evolution

2012

The hypermagnetic helicity density at the electroweak phase transition (EWPT) exceeds many orders of magnitude the galactic magnetic helicity density. Together with previous magnetic helicity evolution calculations after the EWPT and hypermagnetic helicity conversion to the magnetic one at the EWPT, the present calculation completes the description of the evolution of this important topological feature of cosmological magnetic fields. It suggests that if the magnetic field seeding the galactic dynamo has a primordial origin, it should be substantially helical. This should be taken into account in scenarios of galactic magnetic field evolution with a cosmological seed.

PhysicsPhase transitionParticle physicsQuantitative Biology::BiomoleculesCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsElectroweak interactionFOS: Physical sciencesAstronomy and AstrophysicsAstrophysicsAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesHelicityMagnetic fieldHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Orders of magnitude (time)Magnetic helicity0103 physical sciences010306 general physicsDynamoLeptonAstrophysics - Cosmology and Nongalactic Astrophysics
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Electroweak baryogenesis at high bubble wall velocities

2020

It is widely believed that electroweak baryogenesis should be suppressed in strong phase transitions with fast-moving bubble walls, but this effect has never been quantitatively studied. We rederive fluid equations describing transport of particle asymmetries near the bubble wall without making the small-wall-velocity approximation. We show that the suppression of the baryon asymmetry is a smooth function of the wall speed and that there is no special behavior when crossing the sound speed barrier. Electroweak baryogenesis can thus be efficient also with strong detonations, generically associated with models with observably large gravitational waves. We also make a systematic and critical c…

PhysicsPhase transitionleptogenesis010308 nuclear & particles physicsGravitational waveBubbleastrofysiikkaElectroweak interactionHigh Energy Physics::Phenomenologybaryogenesishiukkasfysiikkakosmologia01 natural sciences114 Physical sciencesBaryogenesisPhysics::Fluid DynamicsBaryon asymmetryQuantum electrodynamicsSpeed of sound0103 physical sciences010306 general physicsVacuum expectation value
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Inversion symmetric vs. asymmetric excitations and the low-temperature universal properties of Ar:N 2 and Ar:N 2 :CO glasses

2015

The bias energies of various two-level systems (TLSs) and their strengths of interactions with the strain are calculated for Ar:N2 glass. Unlike the case in KBr:CN, a distinct class of TLSs having weak interaction with the strain and untypically small bias energies is not found. The addition of CO molecules introduces CO flips which form such a class of weakly interacting TLSs, albeit at much lower coupling than that at which they are typically observed in solids. We conclude that because of the absence of a distinct class of weakly interacting TLSs, Ar:N2 is a non-universal glass, the first such system in three dimensions and in ambient pressure. Our results further suggest that Ar:N2:CO m…

PhysicsPhononAttenuationGeneral Physics and AstronomyMoleculeWeak interactionMolecular physicsUniversality (dynamical systems)Ambient pressureEPL (Europhysics Letters)
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Large Time Behavior for Inhomogeneous Damped Wave Equations with Nonlinear Memory

2020

We investigate the large time behavior for the inhomogeneous damped wave equation with nonlinear memory ϕtt(t,&omega

PhysicsPhysics and Astronomy (miscellaneous)General MathematicsNonlinear memoryWeak solutionlcsh:Mathematics010102 general mathematicsnonexistence resultglobal weak solutionDamped wavenonlinear memorylcsh:QA1-93901 natural sciencesinhomogeneous term010101 applied mathematicsChemistry (miscellaneous)Settore MAT/05 - Analisi MatematicaComputer Science (miscellaneous)damped wave equation0101 mathematicsMathematical physicsSymmetry
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Effective axial-vector strength within proton-neutron deformed quasiparticle random-phase approximation

2019

We use the available experimental Gamow-Teller β− and β+/EC (electron-capture) decay rates between 0+ and 1+ ground states in neighboring even-even and odd-odd nuclei, combined with 2νββ half-lives, to analyze the influence of the nuclear environment on the weak axial-vector strength gA. For this purpose, the proton-neutron deformed quasiparticle random-phase approximation (pn-dQRPA), with schematic dipole residual interaction is employed. The Hamiltonian contains particle-hole (ph) and particle-particle (pp) channels with mass-dependent strengths. In deriving the equations of motion we use a self-consistent procedure in terms of a single-particle basis with projected angular momentum provi…

PhysicsProton010308 nuclear & particles physicsNuclear Theorynuclear structure and decays01 natural scienceslifetimes and widthselectroweak interactions in nuclear physics0103 physical sciencesQuasiparticleNeutronbeta decayAtomic physicsydinfysiikka010306 general physicsRandom phase approximationPseudovectorPhysical Review C
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Nonadiabatic quantum search algorithms

2007

7 pages, 4 figures.-- PACS nrs.: 03.67.Lx, 05.45.Mt, 72.15.Rn.-- ISI Article Identifier: 000251326400049.-- ArXiv pre-print available at: http://arxiv.org/abs/0706.1139

PhysicsQuantum PhysicsFOS: Physical sciences[PACS] Semiclassical methods in quantum chaosAdiabatic quantum computationAtomic and Molecular Physics and OpticsQuantum chaosCromodinàmica quànticaAmplitude amplificationSearch algorithm[PACS] Localization effects (metals/alloys) including Anderson or weak localizationGrover's algorithmQuantum algorithmCamps Teoria quàntica deQuantum informationQuantum Physics (quant-ph)AlgorithmQuantum computer[PACS] Quantum computation
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Top quark tensor couplings

2011

We compute the real and imaginary parts of the one-loop electroweak contributions to the left and right tensorial anomalous couplings of the $tbW$ vertex in the Standard Model (SM). For both tensorial couplings we find that the real part of the electroweak SM correction is close to 10$%$ of the leading contribution given by the QCD gluon exchange. We also find that the electroweak real and imaginary parts for the anomalous right coupling are almost of the same order of magnitude. The one loop SM prediction for the real part of the left coupling is close to the 3$\sigma$ discovery limit derived from $b\rightarrow s \gamma$. Besides, taking into account that the predictions of new physics int…

PhysicsQuantum chromodynamicsCouplingNuclear and High Energy PhysicsParticle physicsTop quarkLarge Hadron ColliderPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyElectroweak interactionFOS: Physical sciencesGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Física nuclearHigh Energy Physics::ExperimentOrder of magnitudeJournal of High Energy Physics
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Interpolating between low and high energy QCD via a 5D Yang-Mills model

2005

We describe the Goldstone bosons of massless QCD together with an infinite number of spin-1 mesons. The field content of the model is SU(Nf)xSU(Nf) Yang-Mills in a compact extra-dimension. Electroweak interactions reside on one brane. Breaking of chiral symmetry occurs due to the boundary conditions on the other brane, away from our world, and is therefore spontaneous. Our implementation of the holographic recipe maintains chiral symmetry explicit throughout. For intermediate energies, we extract resonance couplings. These satisfy sum rules due to the 5D nature of the model. These sum rules imply, when taking the high energy limit, that perturbative QCD constraints are satisfied. We also il…

PhysicsQuantum chromodynamicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeElectroweak interactionHigh Energy Physics::PhenomenologyPerturbative QCDFOS: Physical sciencesYang–Mills existence and mass gapMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Goldstone bosonBraneMathematical physics
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Theoretical overview of kaon decays

2014

Kaon decays are an important testing ground of the electroweak flavour theory. They can provide new signals of CP violation and, perhaps, a window into physics beyond the Standard Model. At the same time, they exhibit an interesting interplay of long-distance QCD effects in flavour-changing transitions. A brief overview is presented, focusing on a few selected topics of particular interest. A more detailed and comprehensive review can be found in arXiv:1107.6001.

PhysicsQuantum chromodynamicsHistoryParticle physicsPhysics beyond the Standard ModelHigh Energy Physics::LatticeFlavourElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesWindow (computing)Computer Science ApplicationsEducationHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CP violationHigh Energy Physics::Experiment
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