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Dive into the research topics where B. A. Brown is active.

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Featured researches published by B. A. Brown.


Physical Review C | 1976

Properties of high-spin states inNb91andZr91viaLi6-induced reactions

B. A. Brown; P. M. S. Lesser; D. B. Fossan

The properties of high-spin states in /sup 91/Nb and /sup 91/Zr have been studied with the /sup 88/Sr(/sup 6/Li, 3n)/sup 91/Nb and /sup 88/Sr(/sup 6/Li, p2 n)/sup 91/Zr reactions. In-beam measurements with Ge(Li) and Si(Li) detectors of ..gamma..-ray excitation functions, ..gamma..-..gamma.. coincidences, ..gamma..-ray angular distributions, and pulsed beam-..gamma.. timing spectra were made to establish decay schemes, level energies, spin-parity assignments, ..gamma..-ray multipolarities, and isomeric lifetimes. All of the high-spin states involving the ..pi..1g/sub 9///sub 2/, ..pi..2p/sub 1///sub 2/, and ..nu..2d/sub 5///sub 2/ orbitals as well as other more complicated states were identified. In particular, the theoretically predicted isomeric states in /sup 91/Nb and /sup 91/Zr were found: the vertical-bar (1g/sub 9///sub 2/)/sup 2/2p/sub 1///sub 2/, 17/2/sup -/> state in /sup 91/Nb is at 2035 keV with a tau = 5.42 +- 0.18 ..mu..sec, and vertical-bar (1g/sub 9///sub 2/) /sup 2/2d/sub 5///sub 2/, 21/2/sup +/> state in /sup 91/Zr is at 3167 keV with a tau = 6.28 +- 0.20 ..mu..sec. The experimental energy levels and B (E2) values (E2 effective charges) obtained for these nuclei as well as those of other N = 50 and 51 nuclei are compared with recent theoretical work of Gloeckner et al. (AIP)


Physical Review C | 1976

High-spin states in Zr 92

B. A. Brown; D.B. Fossan; P. M. S. Lesser; A. R. Poletti

High-spin states have been investigated with the /sup 88/Sr(/sup 7/Li, p2n)/sup 92/Zr reaction by ..gamma..-..gamma.. coincidence, ..gamma..-ray angular distribution, and pulsed beam-..gamma.. timing measurements with Ge(Li) detectors. Decay schemes, level energies, and spin-parity information were obtained for /sup 92/Zr from the data. The high-spin states involving the (..pi..1g/sub 9///sub 2/)/sup 2/(..nu..2d/sub 5///sub 2/)/sup 2/ configuration were identified, with the (12/sup +/) member being at 4947 keV. Tentative identification of the members of the (..pi..1g/sub 9///sub 2/..pi..2p/sub 1///sub 2/)(..nu..2d/sub 5///sub 2/)/sup 2/ configuration has also been made. The observed experimental levels in /sup 92/Zr are compared with recent theoretical calculations. (AIP)


Physical Review C | 1976

Properties of high-spin states in Nb 91 and Zr 91 via Li 6 -induced reactions

B. A. Brown; P. M. S. Lesser; D.B. Fossan

The properties of high-spin states in /sup 91/Nb and /sup 91/Zr have been studied with the /sup 88/Sr(/sup 6/Li, 3n)/sup 91/Nb and /sup 88/Sr(/sup 6/Li, p2 n)/sup 91/Zr reactions. In-beam measurements with Ge(Li) and Si(Li) detectors of ..gamma..-ray excitation functions, ..gamma..-..gamma.. coincidences, ..gamma..-ray angular distributions, and pulsed beam-..gamma.. timing spectra were made to establish decay schemes, level energies, spin-parity assignments, ..gamma..-ray multipolarities, and isomeric lifetimes. All of the high-spin states involving the ..pi..1g/sub 9///sub 2/, ..pi..2p/sub 1///sub 2/, and ..nu..2d/sub 5///sub 2/ orbitals as well as other more complicated states were identified. In particular, the theoretically predicted isomeric states in /sup 91/Nb and /sup 91/Zr were found: the vertical-bar (1g/sub 9///sub 2/)/sup 2/2p/sub 1///sub 2/, 17/2/sup -/> state in /sup 91/Nb is at 2035 keV with a tau = 5.42 +- 0.18 ..mu..sec, and vertical-bar (1g/sub 9///sub 2/) /sup 2/2d/sub 5///sub 2/, 21/2/sup +/> state in /sup 91/Zr is at 3167 keV with a tau = 6.28 +- 0.20 ..mu..sec. The experimental energy levels and B (E2) values (E2 effective charges) obtained for these nuclei as well as those of other N = 50 and 51 nuclei are compared with recent theoretical work of Gloeckner et al. (AIP)


Physical Review C | 1976

Properties of high-spin states in Nb91 and Zr91 via Li6-induced reactions

B. A. Brown; P. M. S. Lesser; D. B. Fossan

The properties of high-spin states in /sup 91/Nb and /sup 91/Zr have been studied with the /sup 88/Sr(/sup 6/Li, 3n)/sup 91/Nb and /sup 88/Sr(/sup 6/Li, p2 n)/sup 91/Zr reactions. In-beam measurements with Ge(Li) and Si(Li) detectors of ..gamma..-ray excitation functions, ..gamma..-..gamma.. coincidences, ..gamma..-ray angular distributions, and pulsed beam-..gamma.. timing spectra were made to establish decay schemes, level energies, spin-parity assignments, ..gamma..-ray multipolarities, and isomeric lifetimes. All of the high-spin states involving the ..pi..1g/sub 9///sub 2/, ..pi..2p/sub 1///sub 2/, and ..nu..2d/sub 5///sub 2/ orbitals as well as other more complicated states were identified. In particular, the theoretically predicted isomeric states in /sup 91/Nb and /sup 91/Zr were found: the vertical-bar (1g/sub 9///sub 2/)/sup 2/2p/sub 1///sub 2/, 17/2/sup -/> state in /sup 91/Nb is at 2035 keV with a tau = 5.42 +- 0.18 ..mu..sec, and vertical-bar (1g/sub 9///sub 2/) /sup 2/2d/sub 5///sub 2/, 21/2/sup +/> state in /sup 91/Zr is at 3167 keV with a tau = 6.28 +- 0.20 ..mu..sec. The experimental energy levels and B (E2) values (E2 effective charges) obtained for these nuclei as well as those of other N = 50 and 51 nuclei are compared with recent theoretical work of Gloeckner et al. (AIP)


Physical Review C | 1976

Properties of high-spin states in /sup 91/Nb and /sup 91/Zr via /sup 6/Li-induced reactions. [J,. pi. , multipolarities, isomeric lifetimes]

B. A. Brown; P. M. S. Lesser; D. B. Fossan

The properties of high-spin states in /sup 91/Nb and /sup 91/Zr have been studied with the /sup 88/Sr(/sup 6/Li, 3n)/sup 91/Nb and /sup 88/Sr(/sup 6/Li, p2 n)/sup 91/Zr reactions. In-beam measurements with Ge(Li) and Si(Li) detectors of ..gamma..-ray excitation functions, ..gamma..-..gamma.. coincidences, ..gamma..-ray angular distributions, and pulsed beam-..gamma.. timing spectra were made to establish decay schemes, level energies, spin-parity assignments, ..gamma..-ray multipolarities, and isomeric lifetimes. All of the high-spin states involving the ..pi..1g/sub 9///sub 2/, ..pi..2p/sub 1///sub 2/, and ..nu..2d/sub 5///sub 2/ orbitals as well as other more complicated states were identified. In particular, the theoretically predicted isomeric states in /sup 91/Nb and /sup 91/Zr were found: the vertical-bar (1g/sub 9///sub 2/)/sup 2/2p/sub 1///sub 2/, 17/2/sup -/> state in /sup 91/Nb is at 2035 keV with a tau = 5.42 +- 0.18 ..mu..sec, and vertical-bar (1g/sub 9///sub 2/) /sup 2/2d/sub 5///sub 2/, 21/2/sup +/> state in /sup 91/Zr is at 3167 keV with a tau = 6.28 +- 0.20 ..mu..sec. The experimental energy levels and B (E2) values (E2 effective charges) obtained for these nuclei as well as those of other N = 50 and 51 nuclei are compared with recent theoretical work of Gloeckner et al. (AIP)


Physical Review C | 1976

High-spin states in Zr92

B. A. Brown; D. B. Fossan; P. M. S. Lesser; A. R. Poletti

High-spin states have been investigated with the /sup 88/Sr(/sup 7/Li, p2n)/sup 92/Zr reaction by ..gamma..-..gamma.. coincidence, ..gamma..-ray angular distribution, and pulsed beam-..gamma.. timing measurements with Ge(Li) detectors. Decay schemes, level energies, and spin-parity information were obtained for /sup 92/Zr from the data. The high-spin states involving the (..pi..1g/sub 9///sub 2/)/sup 2/(..nu..2d/sub 5///sub 2/)/sup 2/ configuration were identified, with the (12/sup +/) member being at 4947 keV. Tentative identification of the members of the (..pi..1g/sub 9///sub 2/..pi..2p/sub 1///sub 2/)(..nu..2d/sub 5///sub 2/)/sup 2/ configuration has also been made. The observed experimental levels in /sup 92/Zr are compared with recent theoretical calculations. (AIP)


Physical Review C | 1976

High-spin states inZr92

B. A. Brown; D. B. Fossan; P. M. S. Lesser; A. R. Poletti

High-spin states have been investigated with the /sup 88/Sr(/sup 7/Li, p2n)/sup 92/Zr reaction by ..gamma..-..gamma.. coincidence, ..gamma..-ray angular distribution, and pulsed beam-..gamma.. timing measurements with Ge(Li) detectors. Decay schemes, level energies, and spin-parity information were obtained for /sup 92/Zr from the data. The high-spin states involving the (..pi..1g/sub 9///sub 2/)/sup 2/(..nu..2d/sub 5///sub 2/)/sup 2/ configuration were identified, with the (12/sup +/) member being at 4947 keV. Tentative identification of the members of the (..pi..1g/sub 9///sub 2/..pi..2p/sub 1///sub 2/)(..nu..2d/sub 5///sub 2/)/sup 2/ configuration has also been made. The observed experimental levels in /sup 92/Zr are compared with recent theoretical calculations. (AIP)


Physical Review C | 1976

High-spin states in /sup 92/Zr

B. A. Brown; D. B. Fossan; P. M. S. Lesser; A. R. Poletti

High-spin states have been investigated with the /sup 88/Sr(/sup 7/Li, p2n)/sup 92/Zr reaction by ..gamma..-..gamma.. coincidence, ..gamma..-ray angular distribution, and pulsed beam-..gamma.. timing measurements with Ge(Li) detectors. Decay schemes, level energies, and spin-parity information were obtained for /sup 92/Zr from the data. The high-spin states involving the (..pi..1g/sub 9///sub 2/)/sup 2/(..nu..2d/sub 5///sub 2/)/sup 2/ configuration were identified, with the (12/sup +/) member being at 4947 keV. Tentative identification of the members of the (..pi..1g/sub 9///sub 2/..pi..2p/sub 1///sub 2/)(..nu..2d/sub 5///sub 2/)/sup 2/ configuration has also been made. The observed experimental levels in /sup 92/Zr are compared with recent theoretical calculations. (AIP)


Physical Review C | 1974

Lifetimes of the(f72)3152−states inV51andCa43and(f72)24+states inTi50andCa42via heavy-ion recoil-distance-method measurements

A. R. Poletti; B. A. Brown; D. B. Fossan; Ph. Gorodetzky; J. J. Kolata; J. Olness; E. K. Warburton


Physical Review C | 1974

Nuclear spectroscopy with lithium beams. I. High-spin states in Fe 55 , Mn 55 , and Cr 53

A. R. Poletti; B. A. Brown; D.B. Fossan; E.K. Warburton

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A. R. Poletti

Brookhaven National Laboratory

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P. M. S. Lesser

City University of New York

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E.K. Warburton

Brookhaven National Laboratory

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D.B. Fossan

State University of New York System

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E. K. Warburton

Brookhaven National Laboratory

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J. Olness

Brookhaven National Laboratory

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J. J. Kolata

University of Notre Dame

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A. R. Poletti

Brookhaven National Laboratory

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