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Flynn, E.R.; Sherman, J.D.; Stein, N.; Olsen, D.K.; Riley, P. J.

doi:10.1103/physrevc.13.568

Cited by 40 publications

(22 citation statements)

References 25 publications

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“…The remaining 7-rays are listed in Table 1. [17]. The log f~t value for this UFF decay is 10.1, which is close to the average value of 10.3 for UFF population of excited 0 § or 4 § states in aSKr from the decay of 88Br with P = 2-(this is exclusive of the somewhat faster branch to the ground state with a logfz t value of 8.5).…”

Section: Decay Scheme and Level Assignmentsmentioning

confidence: 57%

“…Their possibility to observe this 0 § state was probably severely reduced by the high level density in this region in combination with the energy resolution problems caused by straggling in their gas target cell. The spectrum obtained by Flynn et al [17] shows a hump at 2,379 keV which probably stems from the 2,370 keV level. Spins and parities of 2 § have been assigned to the levels at 2,828 and 2,875 keV based on the branching ratios obtained for their decay to 2 § states and the ground state.…”

Section: Decay Scheme and Level Assignmentsmentioning

confidence: 94%

“…We note that this level may be weakly populated in the (t,p) transfer studies of Flynn et al [17] but obscured by a broad distribution just below the 2,419 keV peak. Their possibility to observe this 0 § state was probably severely reduced by the high level density in this region in combination with the energy resolution problems caused by straggling in their gas target cell.…”

Section: Decay Scheme and Level Assignmentsmentioning

confidence: 95%

“…Our measurements were performed on chemically separated samples, which means that the nuclides 86-89Br were present at the detector site (the amount of bromine isotopes with mass number below 86 was negligible due to longer half-lives). The levels of 88Kr have been studied by several groups earlier, using the/~-decay of 8SBr [7][8][9][10][11][12][13][14][15][16] as well as nuclear reaction spectroscopy [17]. So far, the most detailed investigation was performed by Hoff [16].…”

Section: Introductionmentioning

confidence: 99%

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Subshell closure effects on the collectivity of 36 88 Kr52 and the beta decay of88Br to levels in88Kr

Skarnemark

Bróden

Kaffrell

et al. 1986

Z. Physik A - Atomic Nuclei

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The level structure of 88Kr has been investigated by measurements on chemically separated bromine samples. A total of 146 7-rays have been assigned to the decay of 88Br, and a level scheme with 58 levels is proposed. The collectivity of SaKr has been investigated within the framework of the Interacting Boson Approximation (IBA-2 model). Comparison of our detailed 7-ray data and calculations have led to the establishment of a proton hole boson desciption rather than proton particle nature. This supports recent works establishing Z= 40 as a major subshell closure.

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Section: Decay Scheme and Level Assignmentsmentioning

confidence: 57%

Section: Decay Scheme and Level Assignmentsmentioning

confidence: 94%

Section: Decay Scheme and Level Assignmentsmentioning

confidence: 95%

Section: Introductionmentioning

confidence: 99%

See 2 more Smart Citations

Subshell closure effects on the collectivity of 36 88 Kr52 and the beta decay of88Br to levels in88Kr

Skarnemark

Bróden

Kaffrell

et al. 1986

Z. Physik A - Atomic Nuclei

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“…The existing information on the low-spin structure of 86 Kr is summarized in Ref. [6] and has been obtained mostly from β-decay measurements [7,8], pickup reactions [9,10] and proton scattering reactions [11].…”

mentioning

confidence: 99%

Low-spin states in86Kr from the(n,n′)reaction

et al. 2013

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Theory of the diffusion of hydrogen in metals

Stoneham

1972

Ber Bunsenges Phys Chem

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This paper reviews the various theories of the motion of light interstitials in metals. It discusses the formulation of quantum theories and their relation to each other and to the classical theories. The physical assumptions are summarised, and a comparison of theory and experiment is made.The theory successfully predicts (1) the distinction between bcc and fcc host lattices, (2) the relation between activation energy and volume of solution in bcc hosts, (3) the absolute magnitudes of the activation energies, (4) the temperature dependence of the diffusion rate, (5) the existence of isotope effects in electro‐ and thermomigration, and (6) the Zener relations. Topics which are not yet understood are discussed.

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Kr84(t,p)Kr

Cited by 40 publications

References 25 publications

Subshell closure effects on the collectivity of 36 88 Kr52 and the beta decay of88Br to levels in88Kr

Subshell closure effects on the collectivity of 36 88 Kr52 and the beta decay of88Br to levels in88Kr

Low-spin states in86Kr from the(n,n′)reaction

Theory of the diffusion of hydrogen in metals

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