Search results for "Tonian"

showing 10 items of 802 documents

Minimal technicolor on the lattice

2009

Abstract We present results from a lattice study of SU(2) gauge theory with 2 flavors of Dirac fermions in adjoint representation. This is a candidate for a minimal (simplest) walking technicolor theory, and has been predicted to possess either an IR fixed point (where the physics becomes conformal) or a coupling which evolves very slowly, so-called walking coupling. In this initial part of the study we investigate the lattice phase diagram and the excitation spectrum of the theory.

PhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeLattice field theoryTechnicolorFixed pointsymbols.namesakeHamiltonian lattice gauge theoryDirac fermionQuantum mechanicsLattice gauge theorysymbolsGauge theoryLattice model (physics)Mathematical physicsNuclear Physics A
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Non-abelian gauge dynamics of slowly moving fermions

1987

We study the dynamics generated by local gauge invariance under a non-abelianSU(N) group for two nonrelativistic particles interacting through the effect of the group charges. We describe the local gauge invariant potential which contains the exchange of infinitely many gluons. We discuss the possible implications of our result.

PhysicsNuclear and High Energy PhysicsIntroduction to gauge theoryGauge bosonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyBRST quantizationHamiltonian lattice gauge theorySupersymmetric gauge theoryLattice gauge theoryQuantum mechanicsGauge anomalyMathematical physicsGauge fixingZeitschrift f�r Physik A Atomic Nuclei
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GAUGE-HIGGS UNIFICATION MODELS WITH COSET SPACE DIMENSIONAL REDUCTION SCHEME

2009

We investigate the gauge-Higgs unification models within the scheme of the coset space dimensional reduction, beginning with two types of set up; fourteen-dimensional gauge theory with simple gauge groups and ten-dimensional gauge theory with direct product gauge groups. We found some phenomenologically acceptable models through an exhaustive search for the candidates of the coset spaces, the gauge group in higher dimension, and fermion representation.

PhysicsNuclear and High Energy PhysicsIntroduction to gauge theoryQuantum gauge theoryHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyAstronomy and AstrophysicsAtomic and Molecular Physics and OpticsBRST quantizationHigh Energy Physics::TheoryTheoretical physicsHamiltonian lattice gauge theorySupersymmetric gauge theoryLattice gauge theoryQuantum electrodynamicsGauge anomalyGauge symmetryInternational Journal of Modern Physics A
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Microscopic description of even-even nuclei in the mass A = 130 region

1986

Abstract We present a systematic study of even-even nuclei in the mass A = 130 region using a microscopic nuclear structure model, in which the nuclear wave functions are approximated by linear combinations of number- and spin-projected zero-quasiparticle and two-quasipartile determinants obtained from a self-consistent Hartree-Fock-Bogoliubov mean field. With a fixed hamiltonian, being a slightly renormalized Brueckner G-matrix based on the Bonn potential the model is able to reproduce the main trends of empirical energy and electromagnetic properties of the transitional, soft nuclei in the region. The empirical nature of the crossing ( πh 11 2 ) 2 and ( vh 11 2 ) 2 superbands in Ce and Ba…

PhysicsNuclear and High Energy PhysicsIsotopeNuclear TheoryNuclear structureParity (physics)symbols.namesakeMean field theoryExcited stateQuadrupolesymbolsAtomic physicsHamiltonian (quantum mechanics)Wave functionNuclear Physics A
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Microscopic quasiparticle-phonon description of odd-mass127−133Xeisotopes and their β decay

1998

Quasiparticle-phonon equations of motion are solved starting from a microscopic realistic many-body Hamiltonian. In this microscopic quasiparticle-phonon model (MQPM) the relevant part of the three-quasiparticle Hilbert space may possibly be taken into account even in calculations using large single-particle bases. As an example, the MQPM is applied to the calculation of energy levels and Fermi and Gamow-Teller beta-decay transition amplitudes for transitions between odd-mass ${}^{127\ensuremath{-}133}\mathrm{Xe}$, ${}^{127\ensuremath{-}133}\mathrm{I}$, and ${}^{127\ensuremath{-}133}\mathrm{Cs}$ isotopes. Considering the fully microscopic nature of the MQPM, comparison of its results and da…

PhysicsNuclear and High Energy PhysicsIsotopePhononHilbert spaceEquations of motionsymbols.namesakeAmplitudeQuantum mechanicsQuasiparticlesymbolsCondensed Matter::Strongly Correlated ElectronsAtomic physicsHamiltonian (quantum mechanics)Fermi Gamma-ray Space TelescopePhysical Review C
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An extended Lipkin-type model with residual proton-neutron interaction

1997

Abstract The Lipkin-Meshkov-Glick (LMG) model is extended to explicitly take into account the proton and neutron degrees of freedom. The proton and neutron Hamiltonians are taken to be of the LMG form, and, in addition, a residual proton-neutron interaction is include. Exact solutions in an SU (2) ⊗ SU (2) basis as well as the RPA solutions for the energy spectrum of the model Hamiltonian are obtained. The spectrum of the exact solutions is degenerate in the limit of no proton-neutron residual interaction, but this degeneracy is totally removed when this type of residual interaction is turned on. The spectrum obtained with RPA is compressed or expanded, as compared to the LMG model with the…

PhysicsNuclear and High Energy PhysicsNuclear TheoryDegenerate energy levelsResidualsymbols.namesakeQuantum mechanicsExcited stateEnergy spectrumsymbolsNeutronRandom phase approximationNucleonHamiltonian (quantum mechanics)Nuclear Physics A
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Charge-changing transitions in an extended Lipkin-type model

1998

Charge-changing transitions are considered in an extended Lipkin-Meshkov-Glick (LMG) model taking into account explicitly the proton and neutron degrees of freedom. The proton and neutron Hamiltonians are taken to be of the LMG form and, in addition, a residual proton-neutron interaction is included. Model charge-changing operators and their action on eigenfunctions of the model Hamiltonian are defined. Transition amplitudes of these operators are calculated using exact eigenfunctions and then the RPA approximation. The best agreement between the two kinds of calculation is obtained when the correlated RPA ground state, instead of the uncorrelated HF ground state, is employed and when the p…

PhysicsNuclear and High Energy PhysicsNuclear TheoryHadronEigenfunctionResidualsymbols.namesakeAmplitudeQuantum mechanicsQuantum electrodynamicssymbolsNuclear fusionNeutronNuclear ExperimentHamiltonian (quantum mechanics)Ground stateThe European Physical Journal A
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Complex-energy approach to sum rules within nuclear density functional theory

2015

The linear response of the nucleus to an external field contains unique information about the effective interaction, correlations, and properties of its excited states. To characterize the response, it is useful to use its energy-weighted moments, or sum rules. By comparing computed sum rules with experimental values, the information content of the response can be utilized in the optimization process of the nuclear Hamiltonian or EDF. But the additional information comes at a price: compared to the ground state, computation of excited states is more demanding. To establish an efficient framework to compute sum rules of the response that is adaptable to the optimization of the nuclear EDF an…

PhysicsNuclear and High Energy PhysicsNuclear Theoryta114nuclear density functional theoryComplex energyComputationFOS: Physical sciencesNuclear Theory (nucl-th)symbols.namesakeQuantum mechanicsExcited statesymbolsQuasiparticleStatistical physicsGround stateHamiltonian (quantum mechanics)Functional theoryNuclear densityPhysical review C
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Energy-independent new physics in the flavour ratios of high-energy astrophysical neutrinos

2010

We have studied the consequences of breaking the CPT symmetry in the neutrino sector, using the expected high-energy neutrino flux from distant cosmological sources such as active galaxies. For this purpose we have assumed three different hypotheses for the neutrino production model, characterised by the flavour fluxes at production phi(0)(e) : phi(0)(mu) : phi(0)(tau) = 1 : 2 : 0, 0 : 1 : 0, and 1 : 0 : 0, and studied the theoretical and experimental expectations for the muon-neutrino flux at Earth, phi(mu), and for the flavour ratios at Earth, R = phi(mu)/phi(e) and S = phi(tau)/phi(mu). CPT violation (CPTV) has been implemented by adding an energy-independent term to the standard neutrin…

PhysicsNuclear and High Energy PhysicsParticle physicsActive galactic nucleusCPT symmetryPhysics beyond the Standard ModelFísicaFOS: Physical sciencesSeparable spacesymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Astrophysical neutrinossymbolsLarge deviations theoryCPT violationNeutrinoHamiltonian (quantum mechanics)Neutrino oscillation
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Global fit to b → cτν transitions

2019

Abstract We perform a general model-independent analysis of $$ b\to c\tau {\overline{\nu}}_{\tau } $$ b → cτ ν ¯ τ transitions, including measurements of ℛ D , ℛ D∗, their q 2 differential distributions, the recently measured longitudinal D* polarization $$ {F}_L^{D\ast } $$ F L D ∗ , and constraints from the $$ {B}_c\to \tau {\overline{\nu}}_{\tau } $$ B c → τ ν ¯ τ lifetime, each of which has significant impact on the fit. A global fit to a general set of Wilson coefficients of an effective low-energy Hamiltonian is presented, the solutions of which are interpreted in terms of hypothetical new-physics mediators. From the obtained results we predict selected $$ b\to c\tau {\overline{\nu}}_…

PhysicsNuclear and High Energy PhysicsParticle physicsBeyond Standard Model; Effective Field TheoriesEffective Field TheoriesLambdaBaryonsymbols.namesakePotential changeBeyond Standard Modelsymbolslcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. RadioactivityHamiltonian (quantum mechanics)Bar (unit)Journal of High Energy Physics
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