Search results for "Isovector"

showing 10 items of 82 documents

Fully self-consistent calculations of nuclear Schiff moments

2010

We calculate the Schiff moments of the nuclei 199Hg and 211Ra in completely self-consistent odd-nucleus mean-field theory by modifying the Hartree-Fock-Bogoliubov code HFODD. We allow for arbitrary shape deformation, and include the effects of nucleon dipole moments alongside those of a CP-violating pion-exchange nucleon-nucleon interaction. The results for 199Hg differ significantly from those of previous calculations when the CP-violating interaction is of isovector character.

PhysicsNuclear and High Energy PhysicsIsovectorNuclear TheoryNuclear TheoryFOS: Physical sciencesSelf consistentSymmetry (physics)Nuclear Theory (nucl-th)DipoleMean field theoryCP violationAtomic physicsNucleonRandom phase approximationNuclear Experiment
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Isospin-invariant Skyrme energy-density-functional approach with axial symmetry

2014

We develop the isospin-invariant Skyrme-EDF method by considering local densities in all possible isospin channels and proton-neutron (p-n) mixing terms as mandated by the isospin symmetry. The EDF employed has the most general form that depends quadratically on the isoscalar and isovector densities. We test and benchmark the resulting p-n EDF approach, and study the general properties of the new scheme by means of the cranking in the isospin space. We extend the existing axial DFT solver HFBTHO to the case of isospin-invariant EDF approach with all possible p-n mixing terms. Explicit expressions have been derived for all the densities and potentials that appear in the isospin representatio…

PhysicsNuclear and High Energy PhysicsIsovectorNuclear Theoryta114IsoscalarNuclear TheoryFOS: Physical sciencesSolverNuclear Theory (nucl-th)isospintiheysIsospinPairingQuantum electrodynamicsQuantum mechanicsCoulombSymmetry breakingAxial symmetryNuclear ExperimentPhysical review C
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Neutron-proton pairing in rotating N ∼ Z nuclei: dominance of the isovector component

2004

Theoretical calculations of rotating N ≈ Z nuclei with A = 58 − 80 within the cranked Nilsson+Strutinsky approach, cranked relativistic mean field and cranked relativistic Hartree+Bogoliubov theories show good agreement with experiment. They point on the presence of the isovector t = 1 np -pairing, but do not show any indications of the isoscalar t = 0 np -pairing.

PhysicsNuclear and High Energy PhysicsIsovectorProtonComponent (thermodynamics)IsoscalarNuclear TheoryHartreeMathematics::Numerical AnalysisNuclear physicsMean field theoryPairingNeutronAtomic physicsNuclear Physics A
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Evidence for isovector neutron-proton pairing from high-spin states inN=Z74Rb

2003

High-spin states in the odd-odd N=Z nucleus Rb-74(37)37 were studied using the Ca-40(Ca-40,alphanp) reaction. A previously observed odd-spin T=0 band has been extended to I-pi=(31(+)) and an even-spin T=0 band has been observed for the first time to I-pi=(22(+)); both have a pi(g(9/2))circle timesnu(g(9/2)) structure. A strongly coupled low-spin T=0,K=3 band has been interpreted as being based upon a pi[312]3/2 circle timesnu[312]3/2 configuration. Cranked relativistic Hartree-Bogoliubov calculations, which are corrected for the t=1 np-pair field by restoring isospin symmetry, reproduce the observed spectrum. These new results provide evidence for the existence of an isovector pair field th…

PhysicsNuclear and High Energy PhysicsIsovectorProtonSpin statesField (physics)IsospinPairingNuclear TheoryNeutronAtomic physicsSymmetry (physics)Physical Review C
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The generalized Gerasimov–Drell–Hearn sum rule for deuteron electrodisintegration

2004

The generalized Gerasimov-Drell-Hearn sum rule $I^{GDH}_{\gamma^*d}(Q^2)$ for deuteron electrodisintegration $d(e,e')np$ as function of the squared four-momentum transfer $Q^2$ is evaluated by explicit integration. The calculation is based on a conventional nonrelativistic framework using a realistic $NN$-potential and including contributions from meson exchange currents, isobar configurations and leading order relativistic terms. Good convergence is achieved. The prominent feature is a deep negative minimum, $I_{\gamma^* d}^{GDH}=-9.5$ mb, at low $Q^2\approx 0.2$ fm$^{-2}$ which is almost exclusively driven by the nucleon isovector anomalous magnetic moment contribution to the magnetic dip…

PhysicsNuclear and High Energy PhysicsNuclear TheoryAnomalous magnetic dipole momentMesonIsovectorMagnetic dipole transitionMomentum transferFOS: Physical sciencesNuclear Theory (nucl-th)Nuclear physicsIsobarSum rule in quantum mechanicsNucleonPhysics Letters B
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Linear response of light deformed nuclei investigated by self-consistent quasiparticle random-phase approximation

2010

We present a calculation of the properties of vibrational states in deformed, axially-symmetric even-even nuclei, within the framework of a fully self-consistent quasiparticle random phase approximation (QRPA). The same Skyrme energy density and density-dependent pairing functionals are used to calculate the mean field and the residual interaction in the particle-hole and particle-particle channels. We have tested our software in the case of spherical nuclei against fully self-consistent calculations published in the literature, finding excellent agreement. We investigate the consequences of neglecting the spin-orbit and Coulomb residual interactions in QRPA. Furthermore we discuss the impr…

PhysicsNuclear and High Energy PhysicsNuclear TheoryIsovectorIsoscalarNuclear TheoryFOS: Physical sciencesNuclear Theory (nucl-th)Mean field theoryQuantum mechanicsPairingQuasiparticleCoulombAtomic physicsSpin (physics)Random phase approximationPhysical Review C
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Dynamical selection rules in p annihilation at rest

1993

Abstract The branching ratios for p p annihilation at rest into two mesons show the existence of dynamical selection rules. The ratios for some annihilation modes are small even though much larger rates should be expected on the basis of statistical models. Dynamical selection rules are observed in annihilations in which strange mesons are produced, and in annihilations into two isovector mesons. The selection rules seem - to first order - not to depend on the spins or orbital angular momenta of the p p atom or of the two mesons produced. This observation suggests an underlying symmetry. It is argued that this symmetry is SU(3).

PhysicsNuclear and High Energy PhysicsParticle physicsAnnihilationMesonIsovectorSpinsBranching fractionNuclear TheoryHigh Energy Physics::ExperimentStatistical modelNuclear ExperimentFirst orderPhysics Letters B
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Gauge fields, hidden local symmetries, and meson exchange currents

1997

Abstract The model dependence of the electromagnetic isovector meson exchange current (MEC) operator at higher momentums transfer is studied. For this purpose, the MEC operator constructed from a Lagrangian of the πϱa 1 system obtained within the framework of the hidden local symmetries (HLS) approach is compared with the analogous operator derived earlier from a minimal Yang-Mills (YM) Lagrangian. Numerical results for the deuteron disintegration near threshold show that the model dependent part of the exchange current modifies the tail of the cross section sensibly and that the presence of the a 1 meson both in the MEC and in the nuclear interaction provides a consistent description of th…

PhysicsNuclear and High Energy PhysicsParticle physicsCross section (physics)Current (mathematics)MesonIsovectorOperator (physics)Quantum electrodynamicsNuclear TheoryHomogeneous spaceCurrent algebraGauge (firearms)Nuclear Physics A
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Description of rotating N=Z nuclei in terms of isovector pairing

2004

A systematic investigation of the rotating $N=Z$ even-even nuclei in the mass $A=58-80$ region has been performed within the frameworks of the Cranked Relativistic Mean field, Cranked Relativistic Hartree Bogoliubov theories and cranked Nilsson-Strutinsky approach. Most of the experimental data is well accounted for in the calculations. The present study suggests that there is strong isovector $np$-pair field at low spin, the strength of which is defined by the isospin symmetry. At high spin, the isovector pair field is destroyed and the data are well described by the calculations assuming zero pairing. No clear evidence for the existence of the isoscalar $t=0$ $np$-pairing has been obtaine…

PhysicsNuclear and High Energy PhysicsParticle physicsField (physics)IsovectorNuclear TheoryIsoscalarNuclear TheoryFOS: Physical sciencesSymmetry (physics)Nuclear Theory (nucl-th)Mean field theoryQuantum electrodynamicsIsospinPairingSpin-½
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The role of electromagnetic form factors in meson exchange currents

1988

The question of electromagnetic form factors, i.e. F1V versus GEV, to be used in isovector meson exchange currents in nonrelativistic calculations is critically reviewed. None of the various arguments given earlier in favour of F1V have been found valid. Furthermore, model dependence of theoretical calculations on deuteron threshold disintegration due to e.m. form factor fits and potential models is found to be substantial. In view of these results, relativistic effects have to be included for a clear understanding of this process in the high momentum transfer region.

PhysicsNuclear and High Energy PhysicsParticle physicsIsovectorMesonQuantum electrodynamicsNuclear TheoryForm factor (quantum field theory)Nuclear fusionRelativistic quantum chemistryHigh momentumZeitschrift f�r Physik A Atomic Nuclei
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