Search results for "Homogeneous space"

showing 10 items of 142 documents

Clusters and the quasi-dynamical symmetry

2008

The possible role of the quasi-dynamical symmetry in nuclear clusterization is discussed. Two particular examples are considered: i) the phases and phase-transitions of some algebraic cluster models, and ii) the clusterization in heavy nuclei. The interrelation of exotic (superdeformed, hyperdeformed) nuclear shapes and cluster-configurations are also investigated both for light, and for heavy nuclei, based on the dynamical and quasi-dynamical SU(3) symmetries, respectively.

PhysicsHistoryParticle physicsNuclear TheoryFizikai tudományokDynamical symmetrySymmetry (physics)Computer Science ApplicationsEducationTheoretical physicsTermészettudományokHomogeneous spaceCluster (physics)Algebraic numberNuclear Experiment
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Unrestricted Shapes of Jellium Clusters

1995

A jellium model with a completely relaxable background charge density is used to study metal clusters containing 2 to 22 electrons. The resulting shapes of the clusters exhibit breaking of axial and inversion symmetries, as well as molecular formation. The clusters without inversion symmetry are soft against deformation. The strongly deformed 14-electron cluster is found to be semi-magic. Stable-shape isomers are predicted.

PhysicsHomogeneous spaceJelliumPoint reflectionPhysics::Atomic and Molecular ClustersCluster (physics)General Physics and AstronomyElectronAtomic physicsDeformation (engineering)Inversion (discrete mathematics)Metal clustersEurophysics Letters (EPL)
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Symmetries and Effective Vertices

2015

When facing the computation of more realistic processes, the calculations can become lengthy very fast as the number of Feynman diagrams grows. Before starting the calculation process the problem should be reduced to its minimal form. Here we will present an example of how to reduce the number of calculated diagrams for a given process (which in this case will be a Higgs-like scalar decay to two photons through a charged scalar loop) using gauge symmetry.

PhysicsLoop (graph theory)symbols.namesakeTheoretical physicsPhotonComputationScalar (mathematics)Homogeneous spacesymbolsProcess (computing)Feynman diagramGauge symmetry
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Spatial symmetries of the local densities

2010

Spatial symmetries of the densities appearing in the nuclear Density Functional Theory are discussed. General forms of the local densities are derived by using methods of construction of isotropic tensor fields. The spherical and axial cases are considered.

PhysicsNuclear Theory (nucl-th)Nuclear and High Energy PhysicsNuclear TheoryHomogeneous spaceGeneral Physics and AstronomyFOS: Physical sciencesFunctional theoryNuclear densityIsotropic tensorMathematical physics
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Scotogenic dark symmetry as a residual subgroup of Standard Model symmetries

2019

We show that the scotogenic dark symmetry can be obtained as a residual subgroup of the global $U(1)_{B-L}$ symmetry already present in Standard Model. We propose a general framework where the $U(1)_{B-L}$ symmetry is spontaneously broken to an even $\mathcal{Z}_{2n}$ subgroup, setting the general conditions for neutrinos to be Majorana and the dark matter stability in terms of the residual $\mathcal{Z}_{2n}$. Under this general framework, as examples, we build a class of simple models where, in the scotogenic spirit, the dark matter candidate is the lightest particle running inside the neutrino mass loop. The global $U(1)_{B-L}$ symmetry in our framework being anomaly free can also be gaug…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsDark matterFOS: Physical sciencesAstronomy and AstrophysicsResidual01 natural sciencesHigh Energy Physics - PhenomenologyMAJORANAHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHomogeneous spaceNeutrino010306 general physicsInstrumentationPhenomenology (particle physics)Mathematical physics
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Shape evolution in116,118Ru: Triaxiality and transition between the O(6) and U(5) dynamical symmetries

2013

${}^{116}\mathrm{Ru}$ and ${}^{118}\mathrm{Ru}$ have been studied via $\ensuremath{\beta}$-delayed $\ensuremath{\gamma}$-ray spectroscopy of nuclei produced in fragmentation reactions at the Radioactive Ion-Beam Factory (RIBF) facility. Level schemes with positive-parity states up to spin $J=6$ have been constructed. The results have been discussed in terms of the interacting boson model, the algebraic collective model, and total Routhian surfaces. We conclude that the very neutron-rich nuclei still show many features associated with triaxial $\ensuremath{\gamma}$-soft nuclei, represented by the O(6) symmetry, but are approaching a spherical structure, the U(5) symmetry, with increasing neu…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsNuclear Theory01 natural sciencesSymmetry (physics)Classical mechanicsNeutron number0103 physical sciencesHomogeneous spaceInteracting boson modelAtomic physicsAlgebraic numberNuclear Experiment010306 general physicsSpectroscopyGround stateSpin-½Physical Review C
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WEAK INTERACTIONS, SYMMETRIES

1981

Abstract The Standard ideas about the breaking of symmetries, through the mechanism of generation mixing, are discussed. New results and proposals looking for discrete space-time symmetry violation as well as flavour-number violation are reported. The use of weak-interaction processes as a tool for both the study of the structure of the currents and for nuclear-structure problems is emphasized.

PhysicsNuclear and High Energy PhysicsHigh Energy Physics::PhenomenologyStructure (category theory)FísicaFeynman graphWeak interactionSymmetry (physics)Theoretical physicsQuantum mechanicsHomogeneous spaceBibliographySymmetry breakingParticle PhysicsMixing (physics)
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Right–right–left extension of the Standard Model

2016

A right-right-left extension of the standard model is proposed. In this model, the standard model gauge group $SU(2)_L \otimes U(1)_Y $ is extended to $SU(2)_L \otimes SU(2)_R \otimes SU(2)^{\prime}_R \otimes SU(2)^{\prime}_L \otimes U(1)_{Y}$. The gauge symmetries $SU(2)^{\prime}_R$, $SU(2)^{\prime}_L$ are the mirror counter-parts of the $SU(2)_L$ and $SU(2)_R$ respectively. Parity is spontaneously broken when the scalar Higgs fields acquire vacuum-expectation values in a certain pattern. Parity is restored at the scale of $SU(2)^{\prime}_L$. The gauge sector has a unique pattern. The scalar sector of the model is optimum, elegant and unique.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsFOS: Physical sciencesGeneral Physics and AstronomyAstronomy and AstrophysicsParity (physics)01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Gauge group0103 physical sciencesHomogeneous spaceHiggs boson010306 general physicsMathematical physicsModern Physics Letters A
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Phenomenology of fermion dark matter as neutrino mass mediator with gauged B-L

2021

We analyze a model with unbroken B-L gauge symmetry where neutrino masses are generated at one loop, after spontaneous breaking of a global U(1) symmetry. These symmetries ensure dark matter stability and the Diracness of neutrinos. Within this context, we examine fermionic dark matter. Consistency between the required neutrino mass and the observed relic abundance indicates dark matter masses and couplings within the reach of direct detection experiments.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsPhysicsQC1-999High Energy Physics::LatticeDark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesContext (language use)FermionAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesSymmetry (physics)High Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHomogeneous spaceNeutrino010306 general physicsPhenomenology (particle physics)Gauge symmetryPhysics Letters
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Models for neutrino mass with discrete symmetries

2010

Discrete non-abelian flavor symmetries give in a natural way tri-bimaximal (TBM) mixing as showed in a prototype model. However neutrino mass matrix pattern may be very different from the tri-bimaximal one if small deviations of TBM will be observed. We give the result of a model independent analysis for TBM neutrino mass pattern.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsSmall deviationsFOS: Physical sciencesMass matrix01 natural sciencesAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHomogeneous spaceNeutrino10. No inequality010306 general physicsMixing (physics)Nuclear Physics B - Proceedings Supplements
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