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ATOMIC AND NUCLEAR STRUCTURE
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Excited Nuclear Stat Zoya N. New Book Releases. Contact Us. Monday to Saturday 9. E-Gift Coupon , click here. Insights Insights, Account, Orders. Metastable Zustande der Atomkerne. Naturwissenschaften 24 , — Blatt, J. Bernthal, F.
Connection between backbending and high-spin isomers decay in W. B 74 , — Pedersen, J. Physica Scripta T 5 , — Chowdhury, P. Decay of high-spin isomers in Os nuclei by barrier penetration. Walker, P. High-K barrier penetration in Hf: a challenge to K selection. Resolution of the W isomer anomaly: exposure of a Fermi-aligned s band. Crowell, B. Novel decay modes of high-K isomers: tunneling in a triaxial landscape.
K-forbidden transitions from multi-quasiparticle states. B , 42—46 Bengtsson, T. Competition between pairing-assisted tunneling and single-particle alignment in the decay of high-K isomeric states. Narimatsu, K.
PHY Nuclear Astrophysics: Glossary
A , 69—88 Multi-quasiparticle and rotational structures in W: Fermi alignment, the K-selection rule and blocking. Multi-quasiparticle states in the mass region. A , 61—84 Xu, F. Multi-quasiparticle potential-energy surfaces. Matinyan, S. Lasers as a bridge between atomic and nuclear physics. Baldwin, G. Recoilless gamma-ray lasers. Utter, S.
Reexamination of the optical gamma ray decay in Th. Shaw, R. Collins, C. Accelerated emission of gamma rays from the year isomer of Hf induced by x-ray irradiation.
Glossary of terms used in PHY320
Rowe, D. Download references. Correspondence to Philip Walker.
Reprints and Permissions. Physical Review C The European Physical Journal A Physical Review Letters Chinese Physics C By submitting a comment you agree to abide by our Terms and Community Guidelines. If you find something abusive or that does not comply with our terms or guidelines please flag it as inappropriate.
Advanced search. Skip to main content. Subscribe Search My Account Login. Abstract A small proportion of atomic nuclei can form highly excited metastable states, or isomers. Rent or Buy article Get time limited or full article access on ReadCube. Figure 1: Excitation energy as a function of various nuclear variables. Figure 2: Chart of atomic nucleic, as a function of neutron number N and proton number Z. Figure 3: Some of the possible results of a beam projectile nucleus colliding with a target nucleus.
Figure 4: Illustration of the nuclear velocity fields for a deformed, rotating nucleus. Figure 5: Reduced hindrance as a function of isomer excitation energy, relative to a rotor with the same angular momentum, for selected K -f. Figure 6: Excitation energy of even-mass hafnium isomers relative to a rotor as a function of neutron number.
References 1 Hansen, P. Google Scholar 29 Bardeen, J. Google Scholar 36 Frauendorf, S.
Google Scholar 37 von Weizsacker, C. Google Scholar 39 Bernthal, F. However, in many cases this mode is not particularly favoured over the competing alpha-decay mode. For physicists who study exotic nuclei, these different types of decay are like the loops and lines in a human fingerprint.
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Their presence or absence can prove whether a specific nucleus was present in a particular experiment, as well as providing direct insights into the arrangement of protons and neutrons in the nucleus being studied. But with these exotic nuclei not occurring naturally on Earth, the question is, how can we make them?