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NSR database version of May 3, 2024.

Search: Author = J.E.Bush

Found 15 matches.

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2000AU02      Phys.Rev.Lett. 84, 35 (2000)

T.Aumann, A.Navin, D.P.Balamuth, D.Bazin, B.Blank, B.A.Brown, J.E.Bush, J.A.Caggiano, B.Davids, T.Glasmacher, V.Guimaraes, P.G.Hansen, R.W.Ibbotson, D.Karnes, J.J.Kolata, V.Maddalena, B.Pritychenko, H.Scheit, B.M.Sherrill, J.A.Tostevin

One-Neutron Knockout from Individual Single-Particle States of ¹¹Be

NUCLEAR REACTIONS ⁹Be(¹¹Be, ¹⁰BeX), E=60 MeV/nucleon; measured σ(E), Eγ, Iγ, (particle)γ-coin, fragments parallel momentum distributions. ¹¹Be deduced ground-state configuration, halo features.

doi: 10.1103/PhysRevLett.84.35
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1983.

2000GU23      Phys.Rev. C61, 064609 (2000)

V.Guimaraes, J.J.Kolata, D.Bazin, B.Blank, B.A.Brown, T.Glasmacher, P.G.Hansen, R.W.Ibbotson, D.Karnes, V.Maddalena, A.Navin, B.Pritychenko, B.M.Sherrill, D.P.Balamuth, J.E.Bush

Spectroscopy of ^{13, 14}B via the One-Neutron Knockout Reaction

NUCLEAR REACTIONS ⁹Be, ¹⁹⁷Au(¹⁴B, ¹³B), E=830 MeV; measured σ, longitudinal momentum distribution, (particle)γ-coin. ¹³B deduced levels possible J, π. ¹⁴B deduced halo features. Eikonal reaction theory. Comparison with shell model.

doi: 10.1103/PhysRevC.61.064609
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1985.

1998BU11      Phys.Rev.Lett. 81, 61 (1998)

J.E.Bush, P.A.Hausladen, D.P.Balamuth, K.R.Pohl, D.Bazin, J.A.Brown, J.A.Caggiano, L.L.Chen, B.S.Davids, D.J.Morrissey, B.M.Sherrill, M.Thoennessen

Breakup of ¹¹Be: Prompt or delayed ?

NUCLEAR REACTIONS Be, ¹⁹⁷Au(¹¹Be, n¹⁰Be), (¹¹Be, ¹¹Be), E=41.7 MeV/nucleon; measured fragment σ(E, θ), (fragment)γ-coin; deduced no reacceleration effect.

doi: 10.1103/PhysRevLett.81.61
Citations: PlumX Metrics

1996PO07      Phys.Rev. C53, 2682 (1996)

K.R.Pohl, P.H.Regan, J.E.Bush, P.E.Raines, D.P.Balamuth, D.Ward, A.Galindo-Uribarri, V.P.Janzen, S.M.Mullins, S.Pilotte

High-Spin States in ¹⁰⁷Pd, ¹⁰⁸Pd, and ¹⁰⁹Ag

NUCLEAR REACTIONS ⁹⁶Zr(¹⁸O, X), E=72 MeV; measured Eγ, Iγ, (particle)γγ-coin. ¹⁰⁰Mo(¹³C, X), E=65 MeV; measured Eγ, Iγ, γγ-coin. ^107,108Pd, ¹⁰⁹Ag deduced high-spin levels, J, π, δ.

doi: 10.1103/PhysRevC.53.2682
Citations: PlumX Metrics
Data from this article have been entered in the XUNDL database. For more information, click here.

1994BA30      Phys.Rev.Lett. 72, 2355 (1994)

D.P.Balamuth, K.A.Griffioen, J.E.Bush, K.R.Pohl, D.O.Handzy, A.Aguirre, B.M.Sherrill, J.S.Winfield, D.J.Morrissey, M.Thoennessen

Importance of Nuclear Effects in the Dissociation of ⁶He and ⁶Li at E/A = 65 MeV

NUCLEAR REACTIONS ²⁷Al, ¹⁹⁷Au(⁶He, α), (⁶Li, α), E=65 MeV/nucleon; measured αγ-coin, γ-multiplicity distribution, σ(θα, Eα) following projectile dissociation; deduced nuclear, Coulomb processes separation.

doi: 10.1103/PhysRevLett.72.2355
Citations: PlumX Metrics

1994RE06      Phys.Rev. C49, 1885 (1994)

P.H.Regan, J.S.Middleton, K.R.Pohl, J.E.Bush, P.E.Raines, D.P.Balamuth, S.M.Mullins, D.Ward, A.Galindo-Uribarri, V.P.Janzen, S.Pilotte

Rotational Bands and Neutron Alignments in Neutron-Rich Odd-A Cadmium Isotopes

NUCLEAR REACTIONS ⁹⁶Zr(¹⁶O, xn), E=60, 70 MeV; measured γγ-coin, DCO ratios. ¹⁰⁹Cd deduced levels, J, π, Iγ, δ, B(λ). ¹¹¹Cd deduced levels, J, π, δ, B(λ).

doi: 10.1103/PhysRevC.49.1885
Citations: PlumX Metrics

1992FR14      Phys.Rev. C46, 778 (1992)

C.M.Frankle, J.D.Bowman, J.E.Bush, P.P.J.Delheij, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, S.H.Yoo, V.W.Yuan, X.Zhu, and the TRIPLE Collaboration

Parity Nonconservation for Neutron Resonances in ²³²Th

NUCLEAR REACTIONS ²³²Th(polarized n, X), E=6-400 eV; measured total σ, parity violating asymmetries. ²³³Th deduced resonances, p-wave parity nonconserving matrix element rms values, spreading width.

doi: 10.1103/PhysRevC.46.778
Citations: PlumX Metrics

1992FR15      Phys.Rev. C46, 1542 (1992)

C.M.Frankle, J.D.Bowman, J.E.Bush, P.P.J.Delheij, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, V.W.Yuan, X.Zhu, and the TRIPLE Collaboration

Parity Nonconservation for the 0.88-eV Neutron Resonance in ⁸¹Br

NUCLEAR REACTIONS ⁸¹Br(polarized n, n), E=0.88 eV; measured parity nonconserving longitudinal analyzing power, σ for p-wave resonances.

doi: 10.1103/PhysRevC.46.1542
Citations: PlumX Metrics

1992PO13      Hyperfine Interactions 75, 153 (1992)

H.Postma, J.D.Bowman, C.D.Bowman, J.E.Bush, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.Knudson, G.E.Mitchell, S.Penttila, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, S.H.Yoo, V.W.Yuan, X.Zhu, and the TRIPLE Collaboration

Parity Violation at Neutron p-Wave Resonances of ²³⁸U and ²³²Th and Related Questions

NUCLEAR REACTIONS ²³⁸U, ²³²Th(n, X), E ≈ epithermal; measured transmission. ²³⁹U, ²³³Th deduced p-wave resonances, parity violation matrix element rms value.

doi: 10.1007/BF02398972
Citations: PlumX Metrics

1992ZH12      Phys.Rev. C46, 768 (1992)

X.Zhu, J.D.Bowman, C.D.Bowman, J.E.Bush, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, V.W.Yuan, and the TRIPLE Collaboration

Parity Nonconservation for Neutron Resonances in ²³⁸U

NUCLEAR REACTIONS ²³⁸U(polarized n, X), E=6-300 eV; measured total σ; deduced P-odd, P-even effective nucleon-nucleon interaction. ²³⁹U deduced resonances, l, gΓn, p-wave parity nonconserving matrix element rms value, spreading width.

doi: 10.1103/PhysRevC.46.768
Citations: PlumX Metrics

1991FR08      Phys.Rev.Lett. 67, 564 (1991)

C.M.Frankle, J.D.Bowman, J.E.Bush, P.P.J.Delheij, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, S.H.Yoo, V.W.Yuan, X.Zhu, and the TRIPLE Collaboration

Sign Correlations and Parity Nonconservation for Neutron Resonances in ²³²Th

NUCLEAR REACTIONS ²³²Th(polarized n, n), E ≈ 8.3-392 eV; measured longitudinal analyzing power vs E, transmission yield. ²³²Th resonances deduced parity violation evidence statistical significance. High confidence limit measurement.

doi: 10.1103/PhysRevLett.67.564
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14143.

1991SZ05      Nucl.Phys. A527, 701c (1991)

J.J.Szymanski, C.D.Bowman, J.D.Bowman, J.Knudson, S.Penttila, S.J.Seestrom, V.W.Yuan, J.E.Bush, C.M.Frankle, C.R.Gould, D.G.Haase, G.E.Mitchell, P.P.J.Delheij, H.Postma, N.R.Roberson, X.Zhu

Parity and Time Reversal Symmetry Nonconservation in Neutron-Nucleus Interactions

NUCLEAR REACTIONS ²³⁸U(polarized n, X), E=60-72 eV; measured transmission, resonance σ helicity dependence. ²³⁹U deduced p-, s-wave states mixing parity-violating rms matrix element, parity violating spreading width.

doi: 10.1016/0375-9474(91)90217-T
Citations: PlumX Metrics

1991YU02      Phys.Rev. C44, 2187 (1991)

V.W.Yuan, C.D.Bowman, J.D.Bowman, J.E.Bush, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, X.Zhu

Parity Nonconservation in Polarized-Neutron Transmission Through ¹³⁹La

NUCLEAR REACTIONS ¹³⁹La(polarized n, X), E=0.5-1 eV; measured transmission. ¹⁴⁰La resonance deduced asymmetry. Parity nonconservation, longitudinal beam polarization.

doi: 10.1103/PhysRevC.44.2187
Citations: PlumX Metrics

1990BO26      Phys.Rev.Lett. 65, 1192 (1990)

J.D.Bowman, C.D.Bowman, J.E.Bush, P.P.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, V.W.Yuan, X.Zhu

Parity Nonconservation for Neutron Resonances in ²³⁸U

NUCLEAR REACTIONS ²³⁸U(n, X), E=epithermal; measured transmission, σ(E) vs helicity. ²³⁹U levels deduced parity nonconservation.

doi: 10.1103/PhysRevLett.65.1192
Citations: PlumX Metrics

1990PE19      J.Phys.(Paris), Colloq.C-6, 523 (1990)

S.Penttila, C.D.Bowman, J.D.Bowman, J.E.Bush, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, V.M.Yuan, X.Zhu

Parity Violation in ²³⁹U Neutron Resonances

NUCLEAR REACTIONS ²³⁸U(polarized n, X), E ≤ 250 eV; measured asymmetry in transmission; deduced parity violating matrix element rms value, effective NN-interaction parameter. ²³⁹U resonances deduced parity-violating spreading width.