Search results for "Coulomb [force]"

showing 10 items of 103 documents

Pygmy dipole resonance in208Pb

2012

Scattering of protons of several hundred MeV is a promising new spectroscopic tool for the study of electric dipole strength in nuclei. A case study of 208Pb shows that at very forward angles J^pi = 1- states are strongly populated via Coulomb excitation. A separation from nuclear excitation of other modes is achieved by a multipole decomposition analysis of the experimental cross sections based on theoretical angular distributions calculated within the quasiparticle-phonon model. The B(E1) transition strength distribution is extracted for excitation energies up to 9 MeV, i.e., in the region of the so-called pygmy dipole resonance (PDR). The Coulomb-nuclear interference shows sensitivity to…

PhysicsNuclear and High Energy PhysicsNuclear TheoryScatteringTransition dipole momentFOS: Physical sciencesCoulomb excitationResonance (particle physics)Nuclear Theory (nucl-th)DipoleNuclear Experiment (nucl-ex)Atomic physicsElectric dipole transitionNuclear ExperimentMultipole expansionNuclear ExperimentExcitationPhysical Review C
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Three-body correlations in electromagnetic dissociation of Borromean nuclei: The 6He case

2005

20 pages, 2 tables, 9 figures, 1 appendix.-- PACS nrs.: 25.60.-t; 27.20.+n; 25.70.De; 25.75.Gz.-- Printed version published Sep 5, 2005.

PhysicsNuclear and High Energy PhysicsParticle correlationsCoulomb excitationCoulomb excitationDissociation (chemistry)Coincidence[PACS] Reactions induced by unstable nucleiAmplitude6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Fragmentation (mass spectrometry)[PACS] Particle correlations and fluctuationsNeutronHe-6[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Atomic physicsSeries expansionGround stateUnstable nucleiNuclear Physics A
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Electromagnetic properties of low-spin states in102, 104Pd

1986

Electromagnetic transitions from low-lying 0+, 2+, 4+ and 3− states in102, 104Pd have been studied using (p, 2n) and (p, p′) reactions and Coulomb excitation. TheE2 transition probabilities from the 0 3 + state in102Pd (13 W.u.) and from the 02/+ state in104Pd (14 W.u.) are somewhat low for two-phonon states. Generally, theE2 transition rates are reasonably well reproduced by the IBA-2 and by the boson-expansion description. The intruding 0 2 + state (t1/2=14.3 ns) in102Pd is connected to the 22/+ and 2 3 + states via strong E2 transitions: B(E2; 0 2 + → 2 2 + )=96±40 W.u.; B(E2; 2 3 + → 0 2 + =17±11 W.u.

PhysicsNuclear and High Energy PhysicsSpin statesNuclear fusionCoulomb excitationState (functional analysis)Atomic physicsZeitschrift f�r Physik A Atomic Nuclei
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Coulomb excitation of Na-29,Na-30: Mapping the borders of the island of inversion

2014

Seidlitz, M., et all ; 10 pags. ; 9 figs. ; 1 tab. ; PACS number(s): 21.60.Cs, 23.20.Js, 25.70.De, 29.38.Gj

PhysicsNuclear and High Energy Physicsregionta114Spectrometer010308 nuclear & particles physicsIsland of inversionshell-modelNuclear TheoryGamma rayCoulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesnuclear-data sheetsExcited state0103 physical sciencesPhysics::Accelerator PhysicsAtomic physics010306 general physicsNucleonWave functionNuclear ExperimentBeam (structure)
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Interweaving of elementary modes of excitation in superfluid nuclei through particle-vibration coupling: Quantitative account of the variety of nucle…

2015

A complete characterization of the structure of nuclei can be obtained by combining information arising from inelastic scattering, Coulomb excitation, and $\ensuremath{\gamma}$-decay, together with one- and two-particle transfer reactions. In this way it is possible to probe both the single-particle and collective components of the nuclear many-body wave function resulting from the coupling of these modes and, as a result, diagonalizing the low-energy Hamiltonian. We address the question of how accurately such a description can account for experimental observations in the case of superfluid nuclei. Our treatment goes beyond the traditional approach, in which these properties are calculated …

PhysicsNuclear and High Energy Physicsta114Nuclear structureObservableCoulomb excitationsuperfluid nucleiInelastic scatteringSuperfluiditysymbols.namesakePairingQuantum mechanicsnuclear structuresymbolsHamiltonian (quantum mechanics)Wave functionPhysical Review C
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Proton-Deuteron Break Up Including Coulomb Effects

1994

The first results of the calculation of proton-deuteron break-up cross sections are presented and compared with experimental data.

PhysicsNuclear physicsBreak-UpProtonDeuteriumNuclear TheoryCoulombNuclear ExperimentCoulomb effect
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Shapes and Collectivity in Neutron Deficient Even-Mass 188–198Pb Isotopes

2015

PhysicsNuclear physicsParticle physicsta114lead isotopesIsotopeCoulomb excitationNeutronProceedings of the Conference on Advances in Radioactive Isotope Science (ARIS2014)
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Thermonuclear reactionS30(p,γ)Cl31studied via Coulomb breakup ofCl31

2014

Coulomb breakup at high energy in inverse kinematics of proton-rich Cl-31 was used to constrain the thermonuclear S-30(p,gamma)Cl-31 capture reaction rate under typical Type I x-ray burst conditions. This reaction is a bottleneck during rapid proton-capture nucleosynthesis (rp process), where its rate depends predominantly on the nuclear structure of Cl-31. Two low-lying states just above the proton-separation threshold of S-p = 296( 50) keV in Cl-31 have been identified experimentally using the (RB)-B-3-LAND setup at the GSI Helmholtzzentrum fur Schwerionenforschung GmbH. Both states are considered to play a key role in the thermonuclear S-30( p,gamma)Cl-31 capture reaction. Excitation ene…

PhysicsNuclear physicsReaction rateNuclear and High Energy PhysicsThermonuclear fusionProtonNucleosynthesisNuclear structureCoulomb excitationAtomic physicsrp-processExcitationPhysical Review C
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Collective 2$^{+1}$ excitations in$^{206}$Po and$^{208,210}$Rn

2016

In the present study, $B(E2; 2^{+}_{1}\rightarrow 0^{+}_{1})$ values have been measured in the 208,210Rn and 206Po nuclei through Coulomb excitation of re-accelerated radioactive beams in inverse kinematics at CERN-ISOLDE. These nuclei have been proposed to lie in, or at the boundary of the region where the seniority scheme should persist. However, contributions from collective excitations are likely to be present when moving away from the N=126 closed shell. Such an effect is confirmed by the observed increased collectivity of the $2^{+}_{1}\rightarrow 0^{+}_{1}$ transitions. Experimental results have been interpreted with the aid of theoretical studies carried out within the BCS-based QRP…

PhysicsNuclear reactionNuclear and High Energy Physics010308 nuclear & particles physicsHadronNuclear TheoryradonCoulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesIsotopes of palladiumcollective excitationExcited state0103 physical sciencesQuasiparticlePhysics::Accelerator PhysicsAtomic physics010306 general physicsNuclear ExperimentOpen shellpoloniumExcitationexcited states
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A new recoil distance technique using low energy coulomb excitation in inverse kinematics

2011

Abstract We report on the first experiment combining the Recoil Distance Doppler Shift technique and multistep Coulomb excitation in inverse kinematics at beam energies of 3–10 A MeV. The setup involves a standard plunger device equipped with a degrader foil instead of the normally used stopper foil. An array of particle detectors is positioned at forward angles to detect target-like recoil nuclei which are used as a trigger to discriminate against excitations in the degrader foil. The method has been successfully applied to measure lifetimes in 128Xe and is suited to be a useful tool for experiments with radioactive ion beams.

PhysicsPlungerNuclear and High Energy PhysicsInverse kinematicsPhysics::Instrumentation and DetectorsDetectorCoulomb excitationsymbols.namesakeRecoilsymbolsPhysics::Accelerator PhysicsAtomic physicsNuclear ExperimentInstrumentationDoppler effectFOIL methodBeam (structure)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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