0000000000007534

AUTHOR

V. I. Mishin

showing 16 related works from this author

Frequency tripling for resonance ionization spectroscopy (RIS) of Cd

1998

To explore the nucleosynthesis of heavy elements in the rapid neutron-capture process, investigations on short- lived, very neutron-rich Cd isotopes are planned that require pure samples. These will be produced at the CERN-ISOLDE on-line mass separator in combination with a chemically se- lective laser ion source. The excitation scheme for resonance ionization of Cd was tested in Mainz with a copper-vapor- pumped dye laser system. Due to the high ionization potential of Cd, frequency tripling was required for the first excita- tion step.1D 228: 8n m/. Laser light with an average power of 2m Wwas obtained after frequency tripling and was suc- cessfully used for RIS test measurements on cadmi…

Materials scienceDye laserPhysics and Astronomy (miscellaneous)IsotopeGeneral EngineeringAnalytical chemistryGeneral Physics and AstronomyMass spectrometryLaserIon sourcelaw.inventionNuclear magnetic resonancelawIonization energyNuclear ExperimentSpectroscopyExcitationApplied Physics B: Lasers and Optics
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On-line yields obtained with the ISOLDE RILIS

2003

The ISOLDE resonance ionization laser ion source (RILIS) allows to ionize efficiently and selectively many metallic elements. In recent yield surveys and on-line experiments with the ISOLDE RILIS we observed 23–34 Mg, 26–34 Al, 98–132 Cd, 149 Tb, 155–177 Yb, 179–200 Tl, 183–215 Pb and 188–218 Bi. The obtained yields are presented together with measured release parameters which allow to extrapolate the release efficiency towards more exotic (short-lived) nuclides of the same elements. 2002 Elsevier Science B.V. All rights reserved.

Nuclear and High Energy PhysicsIsotopeChemistryRadiochemistryLaserAccelerators and Storage RingsIon sourcelaw.inventionNuclear physicslawIonizationIsotopes of cadmiumYield (chemistry)NuclideInstrumentationIsotopes of magnesiumParticle Physics - Experiment
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New information on β-delayed neutron emission from Be-12, Be-14

1999

17 pages, 3 tables, 5 figures, 1 appendix.-- PACS nrs.: 23.40.Hc; 27.20.+n.

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderRadioactivity: Be-12 Be-14 (from 1 GeV p on UC target selective mass separation)Astrophysics::High Energy Astrophysical PhenomenaConfidence intervalNuclear physics6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Neutron long countersBe-12 Be-14 deduced P(n) values Be-14 deduced P(xn) valuesHigh Energy Physics::ExperimentNeutronMeasured βn nn time correlations[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Nuclear ExperimentDelayed neutronRadioactive beam[PACS] Relation with nuclear matrix elements and nuclear structureBe-12 Be-14 (from 1 GeV p on UC target selective mass separation) [Radioactivity]
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Atomic spectroscopy studies of short-lived isotopes and nuclear isomer separation with the ISOLDE RILIS

2002

The Resonance Ionization Laser Ion Source (RILIS) at the ISOLDE on-line isotope separator is based on the selective excitation of atomic transitions by tunable laser radiation. Ion beams of isotopes of 20 elements have been produced using the RILIS setup. Together with the mass separator and a particle detection system it represents a tool for high-sensitive laser spectroscopy of short-lived isotopes. By applying narrow-bandwidth lasers for the RILIS one can study isotope shifts (IS) and hyperfine structure (HFS) of atomic optical transitions. Such measurements are capable of providing data on nuclear charge radii, spins and magnetic moments of exotic nuclides far from stability. Although t…

Nuclear and High Energy PhysicsIsotopeChemistryAtomic spectroscopyNuclear isomerAccelerators and Storage RingsIon sourceNuclidePhysics::Atomic PhysicsAtomic physicsSpectroscopyNuclear ExperimentInstrumentationHyperfine structureDoppler broadening
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Light exotic isotopes: recent beam developments and physics applications at ISOLDE

2002

This paper is divided in three parts: (i) the measurement of yields and decay losses of Li and Be isotopes released from a thin foil tantalum target at the CERN/ISOLDE PS-Booster; (ii) results from beta-decay experiments on Be-12 and Be-14, an improved half-life of 21.49(3) ms has been obtained for Be-12; (iii) the beta-decay of C-9. An outline of the analysis procedure to determine the branching at high excitation energies is given. The ground-state branch has been determined to 54.1(15)%.

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderC-9Isotope[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]Tantalumchemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Beta-decayNuclear physicschemistryNuclear Physics - ExperimentAtomic physicsFOIL methodExcitation
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Study of short-lived tin isotopes with a laser ion source

1995

A chemically selective laser ion source based on resonance ionization of atoms in a hot cavity has been applied for the study of short-lived silver isotopes at CERN/ ISOLDE. Silver atoms were ionized by two resonant excitations and final laser ionization into the continuum. Decay properties of the neutron-rich isotopes121–127Ag were studied with a neutron long-counter and aβ-detector.

Materials sciencePhysics::OpticsThermal ionizationLaserIon sourcelaw.inventionAtmospheric-pressure laser ionizationlawIonizationIsotopes of tinPhysics::Atomic and Molecular ClustersNeutronPhysics::Atomic PhysicsAtomic physicsNuclear ExperimentAmbient ionizationAIP Conference Proceedings
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Production of radioactive Ag ion beams with a chemically selective laser ion source

1997

Abstract We have developed a chemically selective laser ion source at the CERN-ISOLDE facility in order to study neutron-rich Ag nuclides. A pulsed laser system with high repetition rate has been used based on high-power coppe-vapour pump lasers and dye lasers. With this source significant reductions of the isobaric background has been achieved.

Nuclear and High Energy PhysicsDye laserIon beamChemistryNuclear TheoryRadiochemistryPhysics::OpticsLaserIon sourceIonlaw.inventionIon beam depositionlawPhysics::Accelerator PhysicsIsobaric processPhysics::Atomic PhysicsNuclideNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Selective laser ionization of very neutron-rich cadmium isotopes: Decay properties of131Cd83and132Cd84

2000

A chemically selective laser ion source has been applied in a decay study of the very neutron-rich isotopes ${}^{131}\mathrm{Cd}$ and ${}^{132}\mathrm{Cd}$ at CERN/ISOLDE. For the ${\ensuremath{\beta}}^{\ensuremath{-}}$ decay of the $N=83$ nuclide ${}^{131}\mathrm{Cd}$ a surprisingly short half-life of $(68\ifmmode\pm\else\textpm\fi{}3)$ ms and a weak delayed-neutron branch of ${P}_{n}=(3.5\ifmmode\pm\else\textpm\fi{}1.0)%$ were observed. For the $N=84$ nuclide ${}^{132}\mathrm{Cd}$ a half-life of $(97\ifmmode\pm\else\textpm\fi{}10)$ ms and a ${P}_{n}$ value of $(60\ifmmode\pm\else\textpm\fi{}15)%$ were obtained. Schematic features of both decay schemes are developed. We find that our new d…

PhysicsNuclear and High Energy PhysicsAb initio quantum chemistry methodsIonizationIsotopes of cadmiumNeutronAtomic physicsPhysical Review C
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$\beta$ - decay of the M$_{T}$=-1 nucleus $^{58}$Zn studied by selective laser ionization

1998

$\beta$ - decay of $^{58}$Zn has been studied for the first time. A new laser ion-source concept has been used to produce mass-separated sources for $\beta$ and $\gamma$ - spectroscopy. The half-life of $^{58}$Zn was determined to be 86(18) ms. Comparisons are made with previous data from charge-exchange reactions. Our Gamow-Teller strength to the 1$^{+}$ state at 1051 keV excitation in $^{58}$Cu agrees well with the value extracted from a recent ($^{3}$He, t) study. Extensive shell-model calculations are presented.

PhysicsNuclear and High Energy Physics[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]Hadron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]LaserBeta decaylaw.inventionlawIonizationNuclear fusionBeta (velocity)Gamma spectroscopyNuclear Physics - ExperimentAtomic physicsExcitation
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Selective laser ionization of radioactive Ni-isotopes

1997

Abstract A chemically selective laser ion source based on resonance ionization of atoms in a hot cavity has been applied in the study of Ni-isotopes at the CERN-ISOLDE on-line isotope separator. Laser ionization enhanced the yields of long-lived Ni-isotopes almost four orders of magnitude when compared to the yields obtained with the surface ionization mode of the source. As a result, high yields of long-lived Ni-isotopes were obtained. Separation efficiencies of 0.3 and 0.8% were obtained for Ni produced in uranium-carbide, produced from uranium-di-pthalocyanine, and Ta-foil targets, respectively. Ni was found to be released very slowly from the present target and ion source combination.

Nuclear and High Energy PhysicsChemical ionizationMatrix-assisted laser desorption electrospray ionizationChemistryRadiochemistryAnalytical chemistryThermal ionizationIon sourceAtmospheric-pressure laser ionizationIonizationPhysics::Atomic PhysicsNuclear ExperimentInstrumentationElectron ionizationAmbient ionizationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Decay of Neutron-Rich Mn Nuclides and Deformation of Heavy Fe Isotopes

1998

The use of chemically selective laser ionization combined with beta-delayed neutron counting at CERN/ISOLDE has permitted identification and half-life measurements for 623-ms Mn-61 up through 14-ms Mn-69. The measured half-lives are found to be significantly longer near N=40 than the values calculated with a QRPA shell model using ground-state deformations from the FRDM and ETFSI models. Gamma-ray singles and coincidence spectroscopy has been performed for Mn-64 and Mn-66 decays to levels of Fe-64 and Fe-66, revealing a significant drop in the energy of the first 2+ state in these nuclides that suggests an unanticipated increase in collectivity near N=40.

PhysicsIsotopeSHELL modelFOS: Physical sciencesGeneral Physics and AstronomyIonizationQuasiparticleNuclear Physics - ExperimentNeutronNuclideNuclear Experiment (nucl-ex)Atomic physicsSpectroscopyNuclear ExperimentPhysical Review Letters
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Beta decay of the new isotope101Sn

1995

The very neutron-deficient isotope 101Sn was produced in a 50Cr(58Ni, 2p5n) reaction and its decay properties were determined for the first time. By using chemically selective ion sources of an on-line mass separator, the energy spectrum and the half-life (3 ± 1 s) of beta-delayed protons of 101Sn were measured. These results are compared to theoretical predictions.

PhysicsDecay schemeIsotopeSeparator (oil production)Condensed Matter PhysicsBeta decayAtomic and Molecular Physics and OpticsBeta-decay stable isobarsIonNuclear physicsEnergy spectrumAtomic physicsNuclear ExperimentMathematical PhysicsPhysica Scripta
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Ground-state spin of 59Mn

2001

Beta decay of $^{59}$Mn has been studied at PSB-ISOLDE, CERN. The intense and pure Mn beam was produced using the Resonance Ionization Laser Ion Source (RILIS). Based on the measured $\beta$-decay rates the ground-state spin and parity are proposed to be $J^{\pi}$ = 5/2$^{-}$. This result is consistent with the systematic trend of the odd-A Mn nuclei and extends the systematics one step further towards the neutron drip line.

PhysicsNuclear and High Energy Physics[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]Hadron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Ion sourceSpectral lineExcited stateNuclear fusionNuclear drip lineAtomic physicsNuclear ExperimentGround stateParticle Physics - ExperimentRadioactive decayThe European Physical Journal A
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Charge radius change in the heavy tin isotopes until A = 132 from laser spectroscopy

2001

Laser spectroscopy measurements have been carried out on the very neutron-rich tin isotopes with the COMPLIS experimental setup. Using the 5s 25p 23P 0 → 5s 25p6s 3P 1 optical transition, hyperfine spectra of 126-132Sn and 125m, 127m, 129m-131mSn where recorded for the first time. The variation of the mean-square charge radius ( δ〈r 2〉) between these nuclei and nuclear moments of the isomers and the odd isotopes were thus measured. An odd-even staggering which inverts at A = 130 is clearly observed. This indicates a small appearance of a plateau on the δ〈r 2〉 which has to be confirmed by measuring the isotope shift beyond A = 132.

PhysicsNuclear and High Energy PhysicsIsotopeChemistry010308 nuclear & particles physicsJahn–Teller effect[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Plateau (mathematics)01 natural sciencesSpectral lineCharge radius0103 physical sciencesIsotopes of tinNuclear fusionAtomic physics010306 general physicsSpectroscopyHyperfine structure
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Measurement of the Magnetic Moment of the One-Neutron Halo NucleusB11e

1999

The magnetic moment of ${}^{11}\mathrm{Be}$ ( ${T}_{1/2}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}13.8\phantom{\rule{0ex}{0ex}}\mathrm{s}$) was measured by detecting nuclear magnetic resonance signals in a beryllium crystal lattice. The experimental technique applied to a ${}^{11}{\mathrm{Be}}^{+}$ ion beam from a laser ion source includes in-beam optical polarization, implantation into a metallic single crystal, and observation of rf resonances in the asymmetric angular distribution of the $\ensuremath{\beta}$ decay ( $\ensuremath{\beta}$-NMR). The nuclear magnetic moment $\ensuremath{\mu}{(}^{11}\mathrm{Be})\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}\ensuremath{-}1.6816(8…

PhysicsFermi contact interactionAnomalous magnetic dipole momentMagnetic momentNeutron magnetic momentProton magnetic momentPhysics::Medical PhysicsNuclear magnetic momentGeneral Physics and AstronomyOptical polarizationAtomic physicsSpin magnetic momentPhysical Review Letters
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β-decay studies of135–137Snusing selective resonance laser ionization techniques

2002

The decays of the very neutron rich Sn isotopes Sn135-137 were studied at CERN/ISOLDE using isotopic and isobaric selectivity achieved by the use of a resonance ionization laser ion source and mass spectroscopy, respectively. Neutron decay rates, gamma-ray singles, and gamma-gamma coincidence data were collected as a function of time. The half-life (T-1/2) and delayed neutron emission probability (P-n) values of 135 Sn were measured to be 530(20) ms and 21(3)%, respectively. For Sn-136, a T-1/2 of 250(30) ms was determined along with a P-n value of 30(5)%. For Sn-137, a T-1/2 of 190(60) ms and a P-n value of 58(15)% were deduced. Identification of low-energy transitions in Sb-135 was made p…

PhysicsNuclear and High Energy PhysicsAstrophysics::High Energy Astrophysical PhenomenaIonizationDouble beta decayExcited stateNeutronAtomic physicsMass spectrometryGround stateBeta decayDelayed neutronPhysical Review C
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