0000000000164827

AUTHOR

Mikhail V. Zhukov

showing 15 related works from this author

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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Exclusive measurements of nuclear breakup reactions of 17Ne

2014

F. Wamers et al.; 4 pags.; 2 figs. Open Access funded by Creative Commons Atribution Licence 2.0

Nuclear reactionPhysicsIsotopePhysicsQC1-999HadronNuclear Theorychemistry.chemical_elementBreakup530Nuclear physicsBaryonchemistryIsotopes of neonPhysics::Accelerator Physicsddc:530Statistical physicsNucleonNuclear ExperimentCarbon
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Invariant mass spectrum and α-n correlation function studied in the fragmentation of 6He on a carbon target

1998

13 pags, 5 figures.-- PACS nrs.: 24.60.−t; 25.70.Ef; 27.20.+n.

PhysicsNuclear and High Energy PhysicsReaction mechanismMomentum distributionsBreakupSpectral lineIon[PACS] Reactions induced by unstable nucleiBreakup reactions6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Fragmentation (mass spectrometry)Halo nucleiFragmentation mechanism[PACS] ResonancesSecondary radioactive beamsInvariant massNeutronHe-5He-6Invariant mass spectra[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Atomic physicsGround stateExotic nucleiNuclear Physics A
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Systematic investigation of the drip-line nuclei 11Li and 14Be and their unbound subsystems 10Li and 13Be

2007

Fragmentation reactions in a carbon target with beams of 11Li and 14Be at relativistic energies have been studied in a kinematically complete experiment at the ALADIN-LAND setup at GSI. Excited states in 11Li and 14Be were obtained from the data in the inelastic channel. The measured cross sections with the core nucleus in the final state show that in the 14Be case core polarization plays an important role. In the one-neutron knockout channels the measured angular correlations between fragment and neutron are asymmetric, which demonstrates the presence of states with different parities in the 11Li and 14Be ground states. For 10Li a low-lying virtual s-state, a p-state and evidence for a d-s…

PhysicsNuclear physicsNuclear and High Energy PhysicsFragmentation (mass spectrometry)Excited stateHalo nucleusNeutronAtomic physicsNuclear ExperimentPolarization (waves)Ground stateNuclear Physics A
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Two- and three-body correlations: breakup of halo nuclei

2004

4 pages, 2 figures.

Nuclear physicsPhysicsNuclear and High Energy PhysicsSpinsCoincidentNuclear TheoryNeutronHaloNuclear ExperimentGround stateBreakup
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Lithium isotopes beyond the drip line

2008

The unbound isotopes 10Li, 12Li and 13Li have been observed after nucleon-knockout reactions at relativistic energies with 11Li and 14Be beams impinging on a liquid hydrogen target. The channels , and were analysed in the ALADIN-LAND setup at GSI. The 10Li data confirm earlier findings, while the 12Li and 13Li nuclei were observed for the first time. The relative-energy spectrum shows that the ground state of 12Li can be described as a virtual s-state with a scattering length of -13.7(1.6) fm. A broad energy spectrum was found for the channel. Based on the assumption that the relative-energy spectrum is dominated by a correlated background presumably stemming from initial correlations in th…

PhysicsNuclear and High Energy PhysicsIsotopeIsotopes of lithiumNuclear TheoryScattering lengthResonance (particle physics)Nuclear physicsEnergy spectrumAtomic physicsNuclear ExperimentGround stateLiquid hydrogenLine (formation)Physics Letters B
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Continuum excitations in6He

1999

T. Aumann et al. ; 11 pags.; 6 figs.; 2 tabs. ; PACS number(s): 27.20.1n, 25.60.Gc, 25.70.De, 29.30.Hs

PhysicsNuclear and High Energy PhysicsAngular distributionContinuum (topology)Giant resonanceExcited stateQuantum mechanicsCoulomb excitationInelastic scatteringAtomic physicsIsotopes of heliumResonance (particle physics)Physical Review C
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Study of the $^{15}$O(2p, γ )$^{17}$Ne cross section by Coulomb dissociation of $^{17}$Ne for the rp process of nucleosynthesis

2014

Acta physica Polonica / B 45(2), 229 - 234 (2014). doi:10.5506/APhysPolB.45.229

PhysicsRadiative captureNuclear structureGeneral Physics and AstronomySigma25.40.Lw 25.70.De 26.30.Ca 27.20.+nrp-process[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]530Dissociation (chemistry)Nuclear physicsNucleosynthesisTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYCoulombddc:530Atomic physicsExcitationComputingMilieux_MISCELLANEOUS
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The electronion scattering experiment ELISe at the International Facility for Antiproton and Ion Research (FAIR) - A conceptual design study

2011

The electronion scattering experiment ELISe is part of the installations envisaged at the new experimental storage ring at the International Facility for Antiproton and Ion Research (FAIR) in Darmstadt, Germany. It offers an unique opportunity to use electrons as probe in investigations of the structure of exotic nuclei. The conceptual design and the scientific challenges of ELISe are presented. © 2011 Elsevier B.V. All rights reserved.

Nuclear and High Energy PhysicselectronscatteringFORM-FACTORS[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]Electron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]DATA-ACQUISITION SYSTEMNUCLEAR-STRUCTURE01 natural sciencesBINDING-ENERGIESCHARGE-DENSITY DISTRIBUTIONSIonCROSS-SECTIONSNuclear physicsNuclei far off stabilityConceptual designeA collider0103 physical sciencesCENTRAL DEPRESSIONElectron scattering010306 general physicsInstrumentationPhysics010308 nuclear & particles physicsScattering29.27.-a 25.30.Bf25.30.Dh21.10.Ft29.20.Dh29.30.-hRELATIVISTIC HEAVY-IONSEXOTIC NUCLEIFacility for Antiproton and Ion ResearchGIANT-RESONANCESStorage ring
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Experimental study of the 15O(2p, γ)17Ne cross section by Coulomb Dissociation for the rp process

2016

6th Nuclear Physics in Astrophysics Conference (NPA), Lisbon, Portugal, 19 May 2013 - 24 May 2013; Journal of physics / Conference Series 665, 012046 (2016). doi:10.1088/1742-6596/665/1/012046

HistoryChemistryNuclear structurechemistry.chemical_elementrp-process[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]530Dissociation (chemistry)Computer Science ApplicationsEducationIonSubatomär fysikFragmentation (mass spectrometry)Subatomic PhysicsCoulombNuclear Physics - ExperimentBerylliumAtomic physicsNuclear Experiment[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]Excitation
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Lifetime of 26S and a limit for its 2p decay energy

2010

Unknown isotope 26S, expected to decay by two-proton (2p) emission, was studied theoretically and was searched experimentally. The structure of this nucleus was examined within the relativistic mean field (RMF) approach. A method for taking into account the many-body structure in the three-body decay calculations was developed. The results of the RMF calculations were used as an input for the three-cluster decay model worked out to study a possible 2p decay branch of this nucleus. The experimental search for 26S was performed in fragmentation reactions of a 50.3 A MeV 32S beam. No events of 26S or 25P (a presumably proton-unstable subsystem of 26S) were observed. Based on the obtained produ…

PhysicsNuclear and High Energy PhysicsIsotopeNuclear TheoryGeneral Physics and AstronomyFOS: Physical sciencesMain branchNuclear physicsmedicine.anatomical_structureMean field theoryFragmentation (mass spectrometry)Decay energyPicosecondmedicineNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentNucleus
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Halo excitations in fragmentation of He at 240 MeV/u on carbon and lead targets

2000

Dissociation of a 240 MeV/u beam of He-6, incident on carbon and lead targets, has been studied in kinematically complete experiments to investigate low-lying excitation modes in the halo nucleus He-6. It is shown that alignment effects characterize the inelastic scattering and allow an unambiguous assignment of the spin of a narrow resonance observed in the excitation energy spectrum. The differential cross sections for the He-6 inelastic scattering on carbon and lead targets were deduced from the measured moments of the two neutrons and the a-particle. An analysis of these distributions shows that quadrupole and, possibly, monopole excitations characterize the hadronic interaction, while …

PhysicsNuclear and High Energy PhysicsFragmentation (mass spectrometry)QuadrupoleCoulombHalo nucleusNeutronAtomic physicsInelastic scatteringResonance (particle physics)ExcitationNuclear Physics A
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8He-6He: a comparative study of nuclear fragmentation reactions

2001

19 pages, 3 tables, 6 figures.-- PACS nrs.: 27.20.+n; 24.70.+s; 25.06.-t.-- Available online Dec 4, 2000.

PhysicsNuclear and High Energy Physics[PACS] Polarization phenomena in reactionsResonanceHalo nucleusInelastic scatteringDissociation (chemistry)6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Fragmentation (mass spectrometry)NeutronAtomic physics[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Ground stateExcitation
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First Observation of the Unbound NucleusNe15

2014

We report on the first observation of the unbound proton-rich nucleus Ne-15. Its ground state and first excited state were populated in two-neutron knockout reactions from a beam of 500 MeV/u Ne-17. The Ne-15 ground state is found to be unbound by 2.522(66) MeV. The decay proceeds directly to O-13 with simultaneous two-proton emission. No evidence for sequential decay via the energetically allowed 2(-) and 1(-) states in F-14 is observed. The Ne-15 ground state is shown to have a strong configuration with two protons in the (sd) shell around O-13 with a 63(5)% (1s(1/2))(2) component.

Physicsmedicine.anatomical_structureExcited stateNuclear TheorymedicineShell (structure)Physics::Accelerator PhysicsGeneral Physics and AstronomyAtomic physicsNuclear ExperimentGround stateNucleusBeam (structure)Physical Review Letters
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He-8 - He-6: a comparative study of electromagnetic fragmentation reactions

2002

14 pages, 1 table, 2 figures.-- PACS nrs.:27.20.+n; 24.70.+.-- Available online Oct 8, 2001.

PhysicsNuclear and High Energy PhysicsNuclear Reactions: Pb(He-8xn He-6) E=227 MeV/nucleonNuclear TheoryHalo nucleusElectromagnetic fragmentationB(E1)Dissociation (chemistry)Nuclear physics6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Measured σ σ(Θ) σ(E)He-8 deduced resonance energyPb(He-6xnα) E=240 MeV/nucleonNeutronAtomic physics[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Nuclear ExperimentPb(He-8xn He-6) E=227 MeV/nucleon [Nuclear Reactions]
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