Search results for "Excitation"

showing 10 items of 1290 documents

Coulomb excitation of $^{78}$Kr

2006

Expérience à JYFL cyclotron (Jyväskylä, Finlande); The Kr isotopes are considered to be among the best cases for shape coexistence studies in the mass A$\sim$70 region. Our campaign to investigate in detail the development of the shape coexistence in the neutron deficient Kr isotopes was started with the stable nucleus $^{78}$Kr. To obtain the information about the intrinsic shape, Coulomb excitation experiments were performed. A total of 26 matrix elements were determined for $^{78)$Kr. Simple geometrical and algebraic models do not reproduce all details of the electromagnetic structure. A good interpretation of the complex structure of the nucleus with competing oblate and prolate shapes …

PhysicsNuclear and High Energy PhysicsIsotope010308 nuclear & particles physicsNuclear TheoryCoulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesSymmetry (physics)Projection (linear algebra)Matrix (mathematics)Excited state0103 physical sciencesNeutronAlgebraic numberAtomic physics010306 general physics21.10.Ky; 21.60.Jz; 23.20.Js; 25.70.De; 27.50.+e
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Sn108studied with intermediate-energy Coulomb excitation

2005

The unstable neutron-deficient Sn-108 isotope has been studied in inverse kinematics by intermediate-energy Coulomb excitation using the RISING/FRS experimental setup at GSI. This is the highest Z nucleus studied so far with this method. Its reduced transition probability B (E2;0(g.s.)(+)-> 2(1)(+)) has been measured for the first time. The extracted B(E2) value of 0.230(57)e(2) b(2) has been determined relative to the known value in the stable Sn-112 isotope. The result is discussed in the framework of recent large-scale shell model calculations performed with realistic effective interactions. The roles of particle-hole excitations of the Sn-100 core and of the Z=50 shell gap for the E2 po…

PhysicsNuclear and High Energy PhysicsIsotope010308 nuclear & particles physicsNuclear shell modelShell (structure)Coulomb excitationPolarization (waves)01 natural sciencesCore (optical fiber)medicine.anatomical_structure0103 physical sciencesmedicineNeutronAtomic physicsNuclear Experiment010306 general physicsNucleusPhysical Review C
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A thirty second isomer in Hf

1997

An isomer has been detected in Hf-171 with a half-life of T-1/2 = 29.5(9) s. The state was populated in the Yb-170(alpha,3n)Hf-171m reaction at a beam energy of E-alpha = 50 MeV in an on-line ion guide isotope separator. The isomeric Hf-17lm(+) beam was extracted from the ion guide, mass-analysed and implanted in the surface of a microchannel-plate. The half-life of the collected activity was measured from the decay of the microchannel-plate count rate. We associate the isomer with the first excited slate in Hf-171 with spin 1/2(-) at an excitation energy of 22(2) keV.

PhysicsNuclear and High Energy PhysicsIsotopeExcited stateAnalytical chemistryAtomic physicsSpin (physics)Beam energyBeam (structure)ExcitationIonJournal of Physics G: Nuclear and Particle Physics
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Shape coexistence near the double-midshell nucleus 111Rh

1998

The decay of 111Ru obtained from fast on-line chemical and mass separation has been investigated by β-γ-t and γ-γ coincidence techniques. Earlier spin and parity assignments of 111Rh levels based on extrapolations of level systematics are confirmed. In particular, the K=1/2 intruder band is supported by the hindrance of E2 transitions between deformed and spherical states and enhancement of intraband E2 transitions. The excitation energies of intruder band members in Rh isotopes show a minimum at 109Rh64, with two neutrons less than 111Rh at the N=66 midshell. This trend, which differs from the one in the higher-Z neighbouring elements Ag and Cd with minima at N=66, follows the evolution of…

PhysicsNuclear and High Energy PhysicsIsotopeHadronNuclear fusionParity (physics)NeutronAtomic physicsBeta decayCoincidenceExcitationThe European Physical Journal A
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Fine structure in the alpha decays of 226U and 230Pu

1999

The nuclei 226U and 230Pu have been populated via reactions involving 208Pb targets bombarded by 22Ne and 26Mg projectiles. Fusion-evaporation residues were separated in-flight using a gas-filled recoil separator. A position-sensitive Si-strip detector was employed at the focal plane in order to identify correlated α-decay chains. Two fine structure α-decay lines have been observed. The first, with an energy of 7385(5) keV, is assigned as the α decay from 226U to the first excited 2+ state of 222Th. The second line, observed for the first time in this work, has an energy of 6961(30) keV and is assigned as the α decay from 230Pu to the first excited 2+ state of 226U. The excitation energy of…

PhysicsNuclear and High Energy PhysicsIsotopeIsotopes of uranium[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]Excited stateHadronNuclear fusionAlpha decayAtomic physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]ExcitationRadioactive decay
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Multiple coulomb excitation of202Hg and204Hg

1985

Multiple Coulomb excitation measurements on202, 204Hg have been performed with 5 MeV/u208Pb projectiles. The ground bands are excited up to the newly discovered 6+ states and B(E2) values are derived for the 4+→2+ and 6+→4+ transitions. Whereas the 2+ and 4+ levels in the Hg isotopes with 196≦A≦204 have an almost constant energy, the 6+ levels increase in202Hg and204Hg, compared to the lighter isotopes, by approximately 100 and 300 keV, respectively. The relative B(E2) values in both nuclei show that the collectivity in the neutron rich Hg nuclei is of more complex origin than expected from the few proton and neutron holes with respect to the 82 and 126 major shells.

PhysicsNuclear and High Energy PhysicsIsotopeProtonLight isotopeExcited stateNuclear TheoryNuclear fusionElementary particleNeutronCoulomb excitationAtomic physicsNuclear ExperimentZeitschrift für Physik A Atoms and Nuclei
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New μs Isomers in the Neutron-rich 210Hg Nucleus

2013

Neutron-rich nuclei in the lead region, beyond N = 126, have been studied at the FRS-RISING setup at GSI, exploiting the fragmentation of a primary uranium beam. Two isomeric states have been identified in Hg-210: the 8(+) isomer expected from the seniority scheme in the vg(9/2) shell and a second one at low spin and low excitation energy. The decay strength of the 8(+) isomer confirms the need of effective three-body forces in the case of neutron-rich lead isotopes. The other unexpected low-lying isomer has been tentatively assigned as a 3(-) state, although this is in contrast with theoretical expectations. (C) 2013 Elsevier B.V. All rights reserved.

PhysicsNuclear and High Energy PhysicsIsotopechemistry.chemical_elementUraniummedicine.anatomical_structurechemistryFragmentation (mass spectrometry)Subatomic PhysicsmedicineNeutronAtomic physicsNucleusExcitation
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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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Excitation energy dependence of fragment-mass distributions from fission of 180,190 Hg formed in fusion reactions of 36 Ar + 144,154 Sm

2015

Physics letters / B 748, 89 - 94 (2015). doi:10.1016/j.physletb.2015.06.068

PhysicsNuclear and High Energy PhysicsMass asymmetryCluster decayIsotopeFissionNuclear Theory180190HgFusion–fissionActinide530lcsh:QC1-999Mass asymmetric fissionMass spectrumNuclear fusionddc:530Atomic physicsNuclear Experimentlcsh:PhysicsExcitationPhysics Letters B
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Evidence of quasifission in the 180Hg composite system formed in the 68Zn + 112Sn reaction

2021

Abstract For the 68Zn + 112Sn reaction the Coulomb parameter Z 1 Z 2 is equal to 1500 that is close to the threshold value for the appearance of quasifission process. It was found that mass-energy distributions of the reaction fragments differ significantly from those obtained in the 36Ar + 144Sm reaction leading to the formation of the same composite system of 180Hg at similar excitation energies of about 50 MeV. In the case of the reaction with 68Zn ions, the mass distribution of fissionlike fragments has a wide two-humped shape with maximum yields at 70 and 110 u for the light and heavy fragments, respectively, instead of 80 and 100 u observed in the fission of 180Hg formed in the 36Ar +…

PhysicsNuclear and High Energy PhysicsMass distribution010308 nuclear & particles physicsFissionPhysicsQC1-999Composite numberFusion fissionHeavy-ion-induced reactions01 natural sciencesMolecular physicsHeavy and superheavy elementsIonfissioHeavy-ion-induced reactionQuasifission0103 physical sciencesCoulombydinfysiikka010306 general physicsFusion-fissionHeavy and superheavy elementExcitationPhysics Letters B
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