Search results for "Wave function"

showing 10 items of 395 documents

Population of a low-spin positive-parity band from high-spin intruder states in 177Au: The two-state mixing effect

2020

The extremely neutron-deficient isotopes 177,179Au were studied by means of in-beam ?-ray spectroscopy. Specific tagging techniques, ?-decay tagging in 177Au and isomer tagging in 179Au, were used for these studies. Feeding of positive-parity, nearly spherical states, which are associated with 2d3/2 and 3s1/2 proton-hole configurations, from the 1i13/2 proton-intruder configuration was observed in 177Au. Such a decay path has no precedent in odd-Au isotopes and it is explained by the effect of mixing of wave functions of the initial state. © 2020

Nuclear and High Energy Physics? rays179AuPopulation177Au7. Clean energy01 natural scienceskultaIn-beam spectroscopyγ rays0103 physical sciencesMixing effect010306 general physicsWave functioneducationSpectroscopyNuclear Experimenttwo-state mixingPhysicsisotoopiteducation.field_of_studyin-beam spectroscopyIsotope010308 nuclear & particles physicsAu-177Parity (physics)Au-179lcsh:QC1-999gamma raysTwo-state mixingAtomic physicsydinfysiikkalcsh:Physics
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Pinning down the strength function for ordinary muon capture on 100Mo

2019

Ordinary muon capture (OMC) on 100Mo is studied both experimentally and theoretically in order to access the weak responses in wide energy and momentum regions. The OMC populates states in 100Nb up to some 50 MeV in excitation energy. For the first time the associated OMC strength function has been computed and compared with the obtained data. The present computations are performed using the Morita-Fujii formalism of OMC by extending the original formalism beyond the leading order. The participant nuclear wave functions are obtained in extended no-core single-particle model space using the spherical version of proton-neutron quasiparticle random-phase approximation (pnQRPA) with two-nucleon…

Nuclear and High Energy PhysicsIsoscalarmuon-capture giant resonanceNuclear Theorydouble beta decaynuclear matrix elementshiukkasfysiikka01 natural sciencesRenormalization0103 physical sciencesordinary muon capture010306 general physicsWave functionNuclear Experimentvalues of weak axial couplingsPhysicsIsovector010308 nuclear & particles physicslcsh:QC1-999Muon captureGiant resonanceQuantum electrodynamicsIsospinQuasiparticleydinfysiikkacapture-rate distributionlcsh:Physics
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Isospin mixing and the continuum coupling in weakly bound nuclei

2009

The isospin breaking effects due to the Coulomb interaction in weakly-bound nuclei are studied using the Gamow Shell Model, a complex-energy configuration interaction approach which simultaneously takes into account many-body correlations between valence nucleons and continuum effects. We investigate the near-threshold behavior of one-nucleon spectroscopic factors and the structure of wave functions along an isomultiplet. Illustrative calculations are carried out for the T=1 isobaric triplet. By using a shell-model Hamiltonian consisting of an isoscalar nuclear interaction and the Coulomb term, we demonstrate that for weakly bound or unbound systems the structure of isobaric analog states v…

Nuclear and High Energy PhysicsNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]IsoscalarNuclear TheoryFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)symbols.namesakeQuantum mechanics0103 physical sciencesCoulombSymmetry breakingMirror nucleiNuclear Experiment010306 general physicsWave functionPhysics010308 nuclear & particles physics3. Good healthIsospinsymbols21.10.Sf 21.60.Cs 24.10.Cn 21.10.JxAtomic physicsHamiltonian (quantum mechanics)Nucleon
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Detecting the long-distance structure of the X(3872)

2014

We study the X(3872)-->D^0 \bar D^0 \pi^0 decay within a D \bar D^* molecular picture for the X(3872) state. This decay mode is more sensitive to the long-distance structure of the X(3872) resonance than its J/\psi\pi\pi and J/\psi3\pi decays, which are mainly controlled by the details of the X(3872) wave function at short distances. We show that the D^0 \bar D^0 final state interaction can be important, and that a precise measurement of this partial decay width can provide valuable information on the interaction strength between the D^{(*)} \bar D^{(*)} charm mesons.

Nuclear and High Energy PhysicsParticle physicsMeson[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th][SDU.ASTR.CO]Sciences of the Universe [physics]/Astrophysics [astro-ph]/Cosmology and Extra-Galactic Astrophysics [astro-ph.CO]Structure (category theory)FOS: Physical sciencesInteraction strength01 natural sciencesHigh Energy Physics - Experiment[PHYS.ASTR.CO]Physics [physics]/Astrophysics [astro-ph]/Cosmology and Extra-Galactic Astrophysics [astro-ph.CO]High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]0103 physical sciences[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsWave functionComputer Science::DatabasesPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyResonanceFísicaHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentBar (unit)X(3872)
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Long range two-particle rapidity correlations in collisions from high energy QCD evolution

2009

Long range rapidity correlations in A+A collisions are sensitive to strong color field dynamics at early times after the collision. These can be computed in a factorization formalism \cite{GelisLV5} which expresses the $n$-gluon inclusive spectrum at arbitrary rapidity separations in terms of the multi-parton correlations in the nuclear wavefunctions. This formalism includes all radiative and rescattering contributions, to leading accuracy in $\alpha_s\Delta Y$, where $\Delta Y$ is the rapidity separation between either one of the measured gluons and a projectile, or between the measured gluons themselves. In this paper, we use a mean field approximation for the evolution of the nuclear wav…

Nuclear and High Energy PhysicsParticle physicsNuclear TheoryNuclear TheoryFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Phenomenology (hep-ph)Factorization0103 physical sciencesRadiative transferRapidityNuclear Experiment (nucl-ex)Nuclear Experiment010306 general physicsWave functionNuclear ExperimentQuantum chromodynamicsPhysicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyGluonHigh Energy Physics - PhenomenologyMean field theoryNuclear Physics A
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Evidence for Increased neutron and proton excitations between 51−63 Mn

2015

The hyperfine structures of the odd-even 51−63Mnatoms (N=26 −38) were measured using bunched beam collinear laser spectroscopy at ISOLDE, CERN. The extracted spins and magnetic dipole moments have been compared to large-scale shell-model calculations using different model spaces and effective interactions. In the case of 61,63Mn, the results show the increasing importance of neutron excitations across the N=40subshell closure, and of proton excitations across the Z=28shell gap. These measurements provide the first direct proof that proton and neutron excitations across shell gaps are playing an important role in the ground state wave functions of the neutron-rich Mn isotopes. publisher: Els…

Nuclear and High Energy PhysicsProtonNuclear TheoryMagnetic dipole momentsMagnetic dipole momentNuclear Physics - ExperimentNeutronPhysics::Atomic PhysicsNuclear ExperimentWave functionHyperfine structurePhysicsManganeseta114SpinsMagnetic momentMagnetic dipole moment; Manganese; Spin determination; Nuclear and High Energy Physicsmangaanilcsh:QC1-999Spin determinationPhysics::Accelerator PhysicsPräzisionsexperimente - Abteilung BlaumAtomic physicsGround stateMagnetic dipolelcsh:PhysicsPhysics Letters B
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Azimuthal harmonics of color fields in a high energy nucleus

2015

Recent experimental results have revealed a surprisingly rich structure of multiparticle azimuthal correlations in high energy proton-nucleus collisions. Final state collective effects can be responsible for many of the observed effects, but it has recently been argued that a part of these correlations are present already in the wavefunctions of the colliding particles. We evaluate the momentum space 2-particle cumulant azimuthal anisotropy coefficients v_n{2}, n=2,3,4 from fundamental representation Wilson line distributions describing the high energy nucleus. These would correspond to the flow coefficients in very forward proton nucleus scattering. We find significant differences beteen W…

Nuclear and High Energy PhysicsWilson loopNuclear TheoryGLASMA FLUX TUBESFOS: Physical sciencesPosition and momentum space114 Physical sciences01 natural sciencesColor-glass condensateNuclear Theory (nucl-th)GLUON DISTRIBUTION-FUNCTIONSHigh Energy Physics - Phenomenology (hep-ph)CONDENSATE0103 physical sciencesSIDEproton-nucleus collisionsMultiplicity (chemistry)LONG-RANGE010306 general physicsAnisotropyWave functionNuclear ExperimentPhysicsta114010308 nuclear & particles physicsScatteringPB COLLISIONSTRANSVERSE-MOMENTUMMULTIPLICITYPPB COLLISIONSANGULAR-CORRELATIONSlcsh:QC1-999High Energy Physics - PhenomenologyQuantum electrodynamicsmultiparticle azimuthal correlationsColor chargelcsh:PhysicsPhysics Letters B
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Comparison of full-configuration interaction and coupled-cluster harmonic and fundamental frequencies for BH and HF

2001

The harmonic and fundamental frequencies are calculated for the potential-energy curves of BH and HF using the full-configuration interaction model and two hierarchies of coupled-cluster wavefunction models. The anharmonic contributions are also obtained using second-order vibrational perturbation theory. A consistent and systematic improvement is seen for both the harmonic and anharmonic contributions when increasing the level of the correlation treatment. The changes are largest for the harmonic contributions. This is also the case when including valence or diffuse functions in the basis set. Second-order perturbation theory gives a good approximation to the anharmonic contribution and in…

Nuclear magnetic resonanceCoupled clusterChemistryQuantum mechanicsAnharmonicityHarmonicGeneral Physics and AstronomyPhysical and Theoretical ChemistryConfiguration interactionWave functionFull configuration interactionDiatomic moleculeBasis setChemical Physics Letters
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Pion photoproduction on3He including final-state interaction

1991

Coherent π0 and π+ photoproduction and elastic and charge-exchange pion scattering on3He has ben calculated in a consistent model. Realistic three-body Faddeev wave functions have been used and full nonlocal DWIA results for pion photoproduction are obtained. Furthermore, two-step processes such as3He(γ, π0)3He(π0, π+)3H are included giving rise to unexpected large results. The comparison with experimental data is very good over a wide range of photon energies and nuclear momentum transfers. A long-time discrepancy between previous impulse-approximation calculations and experimental data has been removed.

Nuclear physicsMomentumPhysicsParticle physicsRange (particle radiation)PionPhotonScatteringNuclear TheoryState (functional analysis)Nuclear ExperimentWave functionAtomic and Molecular Physics and OpticsFew-Body Systems
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Relativistic effects and spin observables in deuteron electrodisintegration

1993

The influence of relativistic effects in deuteron electrodisintegration, in particular their manifestation in spin observables, is discussed. We have used a simple phenomenological approach by adding the lowest-order relativistic corrections to the nonrelativistic one-body current and including the kinematic wave-function boost. Furthermore, final-state interaction, meson-exchange currents and isobar configurations are included in order to study kinematic regions off the quasi-free case. Sizeable relativistic effects in many observables are found even at low energies.

Nuclear physicsNuclear reactionPhysicsParticle physicsAngular momentumParticle decayNuclear TheoryIsobarObservableRelativistic quantum chemistrySpin (physics)Wave functionAtomic and Molecular Physics and OpticsFew-Body Systems
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