Search results for "Ground"

showing 10 items of 2432 documents

First spatial separation of a heavy ion isomeric beam with a multiple-reflection time-of-flight mass spectrometer

2015

Physics letters / B 744, 137 - 141 (2015). doi:10.1016/j.physletb.2015.03.047

Nuclear reactionNuclear and High Energy PhysicsISOBAR SEPARATIONPROJECTILESpatial isomer separationMass spectrometry530Ion211Po ionsPo-211 ionsCRYOGENIC STOPPING CELLPhysics::Atomic and Molecular ClustersIsomeric ratioFACILITYddc:530Physics::Chemical PhysicsSpectroscopyNuclear ExperimentFRAGMENTSPhysicsExcitation energyta114Multiple-reflection time-of-flight mass spectrometerPERFORMANCEIsotope separation in flightlcsh:QC1-999IsomerFRS-ESRTime of flightSTATESEXOTIC NUCLEIMass spectrumIsomeric beamAtomic physicsGround stateSYSTEMExcitationlcsh:Physics
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α-decay of the new isotopePo187: Probing prolate structures beyond the neutron mid-shell at N = 104

2006

The new neutron-deficient isotope $^{187}\mathrm{Po}$ has been identified in the complete fusion reaction $^{46}\mathrm{Ti}$+$^{144}\mathrm{Sm}$\ensuremath{\rightarrow}$^{187}\mathrm{Po}$+$3n$ at the velocity filter SHIP. Striking features of the $^{187}\mathrm{Po}$ \ensuremath{\alpha} decay are the strongly-hindered decay to the spherical ground state and unhindered decay to a surprisingly low-lying deformed excited state at 286 keV in the daughter nucleus $^{183}\mathrm{Pb}$. Based on the potential energy surface calculations, the $^{187}\mathrm{Po}$ ground state and the 286 keV excited state in $^{183}\mathrm{Pb}$ were interpreted as being of prolate origin. The systematic deviation of t…

Nuclear reactionPhysicsNuclear and High Energy Physics010308 nuclear & particles physics01 natural sciencesExcited state0103 physical sciencesPotential energy surfaceNeutronAlpha decayAtomic physics010306 general physicsGround stateEnergy (signal processing)Radioactive decayPhysical Review C
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New isomer and decay half-life ofRu115

2010

Exotic, neutron-rich nuclei of mass $A=115$ produced in proton-induced fission of $^{238}\mathrm{U}$ were extracted using the IGISOL mass separator. The beam of isobars was transferred to the JYFLTRAP Penning trap system for further separation to the isotopic level. Monoisotopic samples of $^{115}\mathrm{Ru}$ nuclei were used for $\ensuremath{\gamma}$and $\ensuremath{\beta}$ coincidence spectroscopy. In $^{115}\mathrm{Ru}$ we have observed excited levels, including an isomer with a half-life of 76(6) ms and ($7/{2}^{\ensuremath{-}}$) spin and parity. The first excited 61.7-keV level in $^{115}\mathrm{Ru}$ with spins and parity ($3/{2}^{+}$) may correspond to an $\mathit{oblate}$ $3/{2}^{+}$…

Nuclear reactionPhysicsNuclear and High Energy Physics010308 nuclear & particles physicsHadron01 natural sciencesDouble beta decayExcited state0103 physical sciencesIsobarAtomic physicsNuclear Experiment010306 general physicsNucleonGround stateRadioactive decayPhysical Review C
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Overlappingβdecay and resonance neutron spectroscopy of levels inKr87

1983

Energy levels in $^{87}\mathrm{Kr}$ have been studied, with special emphasis on the unbound region, using two different methods. The first method comprises neutron capture and transmission measurements on an enriched gas target of $^{86}\mathrm{Kr}$ using neutron time-of-flight techniques. In this way, neutron widths were determined for 39 resonances below 400 keV and capture areas for 14 resonances below 90 keV. The second method is a decay study of 56-s $^{87}\mathrm{Br}$ in which a level scheme for $^{87}\mathrm{Kr}$ has been established that shows 126 levels in the bound and 12 levels in the unbound region. A detailed comparison amongst the neutron resonance, the $\ensuremath{\gamma}$-r…

Nuclear reactionPhysicsNuclear and High Energy PhysicsAstrophysics::High Energy Astrophysical PhenomenaIsotopes of bromineNeutron cross sectionResonanceNeutronAtomic physicsGround stateDelayed neutronEnergy (signal processing)Physical Review C
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g factors of $^{31,32,33}$Al: Indication for intruder configurations in the $^{33}$Al ground state

2006

Abstract The g factors of 31,32,33 Al have been measured using the β -nuclear magnetic resonance ( β -NMR) technique on spin-polarized beams produced in the fragmentation of a 36 S (77.5 MeV/u) beam on a 9 Be target. Nearly pure beams of Al ( Z = 13 ) isotopes were selected with the high-resolution fragment separator LISE at GANIL. An asymmetry as high as 6% has been observed in the β -NMR curve for 32 Al implanted in a Si single crystal. The magnetic moment of the N = 20 nucleus 33 Al is obtained for the first time: μ ( Al 33 , I π = 5 / 2 + ) = 4.088 ( 5 ) μ N , while those of 31,32 Al are obtained with improved accuracy: μ ( Al 31 , I π = 5 / 2 + ) = 3.830 ( 5 ) μ N and μ ( Al 32 , I π =…

Nuclear reactionPhysicsNuclear and High Energy PhysicsMagnetic momentNUCLEISTABILITY010308 nuclear & particles physicsLandé g-factorMG-32[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesN=20 SHELL CLOSUREMODELMAGNETIC DIPOLEPhysics and AstronomyELECTRIC QUADRUPOLE-MOMENTS0103 physical sciencesSPECTROMETERAtomic physics010306 general physicsGround stateWave functionMagnetic dipoleSingle crystalDimensionless quantity
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Nuclear structure of 131Te studied with (n,γ) and reactions

2003

Abstract The structure of 131 Te has been investigated with the 130 Te( n , γγ ) 131 Te reaction using thermal neutrons and with the 130 Te( d , p ) 131 Te reaction using polarized deuterons with energy E d =18 MeV. About 290 levels were identified in most cases including spin, parity and γ -decay. The γ -decay scheme after neutron capture is essentially complete containing about 100% of the decay of the capture state and about 100% of the population of the 11/2 − isomer and of the ground state. The scheme includes 42 primary transitions with energies between 750 keV and 2500 keV. The experimental level scheme is compared with predictions of the Interacting Boson–Fermion model (IBFM) and of…

Nuclear reactionPhysicsNuclear and High Energy PhysicsNeutron captureDecay schemeDeuteriumAstrophysics::High Energy Astrophysical PhenomenaBinding energyNeutronAtomic physicsNuclear ExperimentGround stateNeutron temperatureNuclear Physics A
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Proton-hole states in theN=30neutron-rich isotopeK49

2010

Excited states in the N=30 neutron-rich isotope {sup 49}K have been studied using multinucleon transfer reactions with thin targets and the PRISMA-CLARA spectrometer combined with thick-target {gamma}-coincidence data from Gammasphere. The d{sub 3/2} proton-hole state is located 92 keV above the s{sub 1/2} ground state, and the proton-particle f{sub 7/2} state is suggested at 2104 keV. Three other levels are established as involving the coupling to 2{sup +} of two neutrons above the N=28 shell. The measured or estimated lifetimes served to reinforce the interpretation of the observed level structure, which is found to be in satisfactory agreement with shell-model calculations.

Nuclear reactionPhysicsNuclear and High Energy PhysicsProtonAstrophysics::High Energy Astrophysical PhenomenaExcited stateGammasphereNeutronAtomic physicsNuclear ExperimentGround stateNucleonCoupling (probability)Physical Review C
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Quasielastic proton knockout from 16O.

1994

The spectral function of the $^{16}\mathrm{O}$(e,e'p${)}^{15}$N reaction has been measured in quasielastic parallel kinematics. Momentum distributions are extracted for transitions to several discrete states, with emphasis on the low-lying positive parity states of $^{15}\mathrm{N}$. Spectroscopic factors and bound state wave functions are deduced from a DWIA analysis employing five different optical potentials. Coupled channels effects are investigated for the first four states of $^{15}\mathrm{N}$ and are found to be minimal. The spectroscopic results of the 1/${2}^{\mathrm{\ensuremath{-}}}$ ground state and the first 3/${2}^{\mathrm{\ensuremath{-}}}$ excited state indicate a 28%\ifmmode\…

Nuclear reactionPhysicsNuclear and High Energy PhysicsProtonExcited stateBound stateHadronSum rule in quantum mechanicsAtomic physicsNucleonGround statePhysical review. C, Nuclear physics
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Decay of the high-spin isomer in 160Re: Changing single-particle structure beyond the proton drip line

2011

WOS: 000286708700015

Nuclear reactionPhysicsNuclear and High Energy PhysicsProtonta114Gas-filled recoil separator Si and Ge strip detectorsNUCLEAR REACTIONS Ni-58+Cd-106 at 290300 MeV beam energy enriched targetsMeasured E gamma t1/2ParticleNeutronNuclear reactionsAtomic physicsProton emissionGround stateMeasuredLine (formation)Spin-½Physics Letters B
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Shape isomerism and spectroscopy ofHg177

2003

High spin states in the $^{177}\mathrm{Hg}$ nucleus were populated by the $^{144}\mathrm{Sm}(^{36}\mathrm{Ar},3\mathrm{n})^{177}\mathrm{Hg}$ reaction at a beam energy of $178\phantom{\rule{0.3em}{0ex}}\text{MeV}$. The emitted prompt $\ensuremath{\gamma}$ rays were detected with the Jurosphere $\ensuremath{\gamma}$-ray spectrometer, while the recoiling nuclei were identified using an active stopper at the focal plane of the gas-filled separator RITU. A quasi-rotational band that decays to an isomeric state with a half-life ${t}_{1∕2}=1.50\ifmmode\pm\else\textpm\fi{}0.15\phantom{\rule{0.3em}{0ex}}\ensuremath{\mu}\mathrm{s}$ and its subsequent $\ensuremath{\gamma}$ decay to the ground state of…

Nuclear reactionPhysicsNuclear and High Energy PhysicsSpin statesExcited stateHadronElementary particleAtomic physicsNuclear ExperimentNucleonGround stateSpectral linePhysical Review C
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