Levels in <sup>115</sup>Sn

Madueme, G.Ch.; Westerberg, L.; Edvardson, L.O.; Migahed, M. D.

doi:10.1088/0031-8949/12/4/003

Cited by 20 publications

(2 citation statements)

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“…The experimental procedure follows closely that described in ref. [6]. The targets for the y-spectroscopy were self-supporting with thicknesses that ranged between 1-3 mg/cm* for cadmium and 2.5-3.5 mg/cm2 for the tin isotopes.…”

Section: Experimental Methodsmentioning

confidence: 84%

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Excited States in Odd Sn Nuclei, A = 109-125

1976

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Gamma-ray and internal conversion studies of the odd Sn isotopes investigated through (α,n) and (d,p) reactions are reported. A level scheme is proposed for each nucleus. An odd parity state at moderate excitation energy above the 1h 11/2 single quasiparticle state is identified or proposed in each nucleus, some of which are observed for the first time. Individual level structure and the level systematics in the odd tin isotopes are discussed.

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Section: Experimental Methodsmentioning

confidence: 84%

“…In a recent paper [6] an investigation of the states in W n through (p,n) and (cq) reactions was reported. In this paper the results from an extension of the studies to the other odd tin isotopes are presented.…”

Section: Introductionmentioning

confidence: 99%

Excited States in Odd Sn Nuclei, A = 109-125

1976

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Number-projected three-quasiparticle description of the odd Sn isotopes

1978

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An account is given of the description of the low-energy properties of the odd Sn nuclei in terms of number projected one-(1 q.p.) and three-quasiparticle (3 q.p.) states. The shell model space for the neutrons consists of one major shell. A simple Gaussian force is used as an effective interaction. Its strength and the single-particle energies, which are the only parameters, are derived in a consistent way from spectroscopic data on the onequasiparticle states. We find that the spectra can be well interpreted in terms of l q.p. and 3q.p. states. Branching ratios of gamma decay, one-nucleon transfer spectroscopic factors, electric and magnetic moments show generally good agreement with the experimental data. For halflives and mixing ratios, which are most sensitive to details of the 3 q.p. components, the agreement is less, but all have the correct order of magnitude.

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