Sr87(d, p)Sr88 reaction

Kamal K Seth; Kurt A. Buzard; J. Picard; G. Bassani

doi:10.1103/PhysRevC.10.1928

Sr87(d, p)Sr88 reaction

Kamal K Seth^*, Kurt A. Buzard, J. Picard, G. Bassani

^*Corresponding author for this work

Physics and Astronomy

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Abstract

Neutron particle-hole states in Sr88 have been studied by means of the reaction Sr87(d,p)Sr88 at Ed=12 MeV. It has been determined that the earlier reported transitions to presumed states at 4744 and 5780 keV in Sr88 arise mainly from transition to the ground state and the first excited state in Sr89. Spectroscopic strengths for states of the multiplets [g92-1d52] and [g92-1s12] have been determined by detailed distorted-wave Born-approximation analysis. Jπ assignments are suggested on the basis of sum rules and comparison with other experiments. Matrix elements for two-particle effective interactions are derived. NUCLEAR REACTIONS Sr87(d,p), E=12 MeV; measured σ(θ) deduced level energies, Jπ; deduced two body matrix elements; enriched targets.

Original language	English (US)
Pages (from-to)	1928-1938
Number of pages	11
Journal	Physical Review C
Volume	10
Issue number	5
DOIs	https://doi.org/10.1103/PhysRevC.10.1928
State	Published - Jan 1 1974

ASJC Scopus subject areas

Physics and Astronomy(all)
Nuclear and High Energy Physics

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title = "Sr87(d, p)Sr88 reaction",

abstract = "Neutron particle-hole states in Sr88 have been studied by means of the reaction Sr87(d,p)Sr88 at Ed=12 MeV. It has been determined that the earlier reported transitions to presumed states at 4744 and 5780 keV in Sr88 arise mainly from transition to the ground state and the first excited state in Sr89. Spectroscopic strengths for states of the multiplets [g92-1d52] and [g92-1s12] have been determined by detailed distorted-wave Born-approximation analysis. Jπ assignments are suggested on the basis of sum rules and comparison with other experiments. Matrix elements for two-particle effective interactions are derived. NUCLEAR REACTIONS Sr87(d,p), E=12 MeV; measured σ(θ) deduced level energies, Jπ; deduced two body matrix elements; enriched targets.",

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doi = "10.1103/PhysRevC.10.1928",

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T1 - Sr87(d, p)Sr88 reaction

AU - Seth, Kamal K

AU - Buzard, Kurt A.

AU - Picard, J.

AU - Bassani, G.

PY - 1974/1/1

Y1 - 1974/1/1

N2 - Neutron particle-hole states in Sr88 have been studied by means of the reaction Sr87(d,p)Sr88 at Ed=12 MeV. It has been determined that the earlier reported transitions to presumed states at 4744 and 5780 keV in Sr88 arise mainly from transition to the ground state and the first excited state in Sr89. Spectroscopic strengths for states of the multiplets [g92-1d52] and [g92-1s12] have been determined by detailed distorted-wave Born-approximation analysis. Jπ assignments are suggested on the basis of sum rules and comparison with other experiments. Matrix elements for two-particle effective interactions are derived. NUCLEAR REACTIONS Sr87(d,p), E=12 MeV; measured σ(θ) deduced level energies, Jπ; deduced two body matrix elements; enriched targets.

AB - Neutron particle-hole states in Sr88 have been studied by means of the reaction Sr87(d,p)Sr88 at Ed=12 MeV. It has been determined that the earlier reported transitions to presumed states at 4744 and 5780 keV in Sr88 arise mainly from transition to the ground state and the first excited state in Sr89. Spectroscopic strengths for states of the multiplets [g92-1d52] and [g92-1s12] have been determined by detailed distorted-wave Born-approximation analysis. Jπ assignments are suggested on the basis of sum rules and comparison with other experiments. Matrix elements for two-particle effective interactions are derived. NUCLEAR REACTIONS Sr87(d,p), E=12 MeV; measured σ(θ) deduced level energies, Jπ; deduced two body matrix elements; enriched targets.

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Sr87(d, p)Sr88 reaction

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