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NSR database version of May 19, 2024.

Search: Author = D.Ye

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2022LI69      Phys.Rev. C 106, 064611 (2022)

S.Liu, D.Ye, J.Liu

Laser-assisted in-flight muon-catalyzed deuteron-triton fusion

NUCLEAR REACTIONS 3H(d, X), E<100 keV; calculated laser enhanced fusion σ(E) of deuteron and muonic triton atom, penetrability, trajectories of a laser-assisted scattering, distribution of turning points. Explained the shielding effect of muon catalyzing the DT fusion process. Semiclassical method. Wentzel-Kramers-Brillouin formula.

doi: 10.1103/PhysRevC.106.064611
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2021LI59      Phys.Rev. C 104, 044614 (2021)

S.Liu, H.Duan, D.Ye, J.Liu

Deuterium-tritium fusion process in strong laser fields: Semiclassical simulation

NUCLEAR REACTIONS 2H(t, n), E(n)<10 keV; calculated energy distribution of particles for different laser intensities and 12.44-eV laser frequency, typical classical trajectories of d-t collision driven by a laser field at laser frequencies of 0.1 eV, 10 eV and 1000 eV, penetrability versus initial energy, angular dependence of penetrability as functions of laser intensities and frequencies, phase diagram of effective region of laser-field enhanced d-t fusion cross sections as function of initial energies using a model consisting particle scattering in the combined repulsive Coulomb potential and laser field, quantum tunneling process of the Coulomb barrier, nuclear fusion, and penetrability from Wentzel-Kramers-Brillouin (WKB) formula. Comparisons with results from Kramers-Henneberger approximation and Volkov state approximation.

doi: 10.1103/PhysRevC.104.044614
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1995BE31      Phys.Rev. C52, 621 (1995)

L.A.Bernstein, J.A.Cizewski, H.-Q.Jin, W.Younes, R.G.Henry, L.P.Farris, A.Charos, M.P.Carpenter, R.V.F.Janssens, T.L.Khoo, T.Lauritsen, I.G.Bearden, D.Ye, J.A.Becker, E.A.Henry, M.J.Brinkman, J.R.Hughes, A.Kuhnert, T.F.Wang, M.A.Stoyer, R.M.Diamond, F.S.Stephens, M.A.Deleplanque, A.O.Macchiavelli, I.Y.Lee, B.Cederwall, J.R.B.Oliveira, J.Burde, P.Fallon, C.Duyar, J.E.Draper, E.Rubel, D.T.Vo

Onset of Collectivity in Neutron Deficient 196,198Po

NUCLEAR REACTIONS 172Yb(28Si, 4n), E=141, 142, 145 MeV; 174Yb(29Si, 5n), E=141, 146 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, DCO ratios. 196,198Po deduced levels, J, π, γ-multipolarity, B(λ) ratios, γ-ray branching ratios. Single-particle, vibrational phonon models, systematics of the Po isotopes studied.

doi: 10.1103/PhysRevC.52.621
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1995CH05      Phys.Rev. C51, 623 (1995)

A.Charlop, J.Bierman, Z.Drebi, S.Gil, A.Sonzogni, R.Vandenbosch, D.Ye

Fusion-Fission Cross Sections for 32S + 138Ba and 48Ti + 122Sn at Near-Barrier Energies

NUCLEAR REACTIONS 138Ba(32S, F), E=150-164.7 MeV; 122Sn(48Ti, F), E=192.8-200 MeV; measured fission σ; deduced fusion σ(E). Other reactions, data analysis included. Coupled-channels model.

doi: 10.1103/PhysRevC.51.623
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1995CH06      Phys.Rev. C51, 628 (1995)

A.Charlop, J.Bierman, Z.Drebi, A.Garcia, S.Gil, D.Prindle, A.Sonzogni, R.Vandenbosch, D.Ye

Search for Entrance Channel Effects in Sub-Barrier Fusion Reactions

NUCLEAR REACTIONS 142Ce(28Si, xn), E=110-145.3 MeV; 138Ba(32S, xn), E=121.5-164.9 MeV; 122Sn(48Ti, xn), E=168.9-223.1 MeV; measured γ multiplicity; deduced < l >, no entrance channel mass asymmetry related effects. Coupled-channel model.

doi: 10.1103/PhysRevC.51.628
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1995DR05      Phys.Rev. C52, 578 (1995)

Z.M.Drebi, K.A.Snover, A.W.Charlop, M.S.Kaplan, D.P.Wells, D.Ye, Y.Alhassid

Spin-Induced Shape Changes in Light-Medium Mass Compound Nuclei

NUCLEAR REACTIONS 27Al(32S, X), E=90-215 MeV; 45Sc(18O, X), E=54-149 MeV; measured γ(θ), production σ. 59,63Cu deduced GDR characteristics.

doi: 10.1103/PhysRevC.52.578
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1995KI13      Acta Phys.Pol. B26, 439 (1995)

M.Kicinska-Habior, K.A.Snover, A.Maj, Z.Drebi, D.Ye, M.Kelly

Ultradipole Radiation from Low-Energy Heavy-Ion Reactions

NUCLEAR REACTIONS 26Mg(12C, X), E=6-11 MeV/nucleon; 24Mg(12C, X), E=11 MeV/nucleon; measured Eγ, Iγ(θ); deduced ultradipole radiation related features.


1995SO17      Phys.Lett. 350B, 173 (1995)

F.Soramel, T.L.Khoo, Ph.Benet, K.B.Beard, R.V.F.Janssens, I.Ahmad, I.Bearden, M.P.Carpenter, P.J.Daly, M.W.Drigert, B.Fornal, U.Garg, Z.Grabowski, T.Lauritsen, Y.Liang, R.Meyer, E.F.Moore, W.Reviol, D.Ye

Search for Entrance Channel Dependence in the Population of Superdeformed Bands in 191Hg

NUCLEAR REACTIONS 160Gd(36S, 5n), E=169 MeV; 130Te(64Ni, 3n), E=257 MeV; measured γγ-coin, Eγ, Iγ. 191Hg deduced levels, J, π, superdeformed bands population entrance channel dependence.

doi: 10.1016/0370-2693(95)00342-I
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1994BE27      Nucl.Phys. A576, 441 (1994)

I.G.Bearden, R.V.F.Janssens, M.P.Carpenter, E.F.Moore, I.Ahmad, P.J.Daly, R.Mayer, M.W.Drigert, P.B.Fernandez, B.Fornal, U.Garg, Z.W.Grabowski, T.L.Khoo, T.Lauritsen, W.Reviol, D.Ye

Detailed Band Structures in 189Hg and 190Hg

NUCLEAR REACTIONS 160Gd(34S, 4n), (34S, 5n), E=159, 162, 165 MeV; measured Eγ, Iγ, γγ(θ), DCO ratio. 189,190Hg deduced high-spin levels, J, π, band structures, deformation. Enriched targets, Compton-suppressed Ge-detectors, central array of BGO hexagons. Cranked shell model calculations.

doi: 10.1016/0375-9474(94)90253-4
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1994CH06      Phys.Rev. C49, R1235 (1994)

A.Charlop, J.Bierman, Z.Drebi, A.Garcia, D.Prindle, A.A.Sonzogni, R.Vandenbosch, D.Ye, S.Gil, F.Hasenbalg, J.E.Testoni, D.Abriola, M.di Tada, A.Etchegoyen, M.C.Berisso, J.O.Fernandez-Niello, A.J.Pacheco

Absence of Anomalous Entrance Channel Effects in Sub-Barrier Heavy Ion Fusion

NUCLEAR REACTIONS 142Ce(28Si, X), 138Ba(32S, X), 122Sn(48Ti, X), E not given; measured fusion σ(E), γ multiplicity; deduced mean angular momentum. Coupled channels analysis.

doi: 10.1103/PhysRevC.49.R1235
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1994PL02      Phys.Rev. C49, 2851 (1994)

A.J.M.Plompen, M.N.Harakeh, W.H.A.Hesselink, G.van't Hof, N.Kalantar-Nayestanaki, J.P.S.van Schagen, R.V.F.Janssens, I.Ahmad, I.G.Bearden, M.P.Carpenter, T.L.Khoo, T.Lauritsen, Y.Liang, U.Garg, W.Reviol, D.Ye

Reply to ' Comment on ' Lack of Evidence for a Superdeformed Band in 192Pb ' '

NUCLEAR STRUCTURE 192Pb; analyzed, reviewed existing data; deduced need for more definitive experiments to determine superdeformed band evidence.

doi: 10.1103/PhysRevC.49.2851
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1993BI12      Phys.Rev. C48, 319 (1993)

J.D.Bierman, A.W.Charlop, D.J.Prindle, R.Vandenbosch, D.Ye

Rotational State Populations in 16O + 154Sm Near-Barrier Fusion

NUCLEAR REACTIONS 154Sm(16O, X), E=63-68 MeV; 166Er(α, X), E=43, 47.6 MeV; measured Eγ, Iγ, γγ-coin; deduced mean compound nuclear angular momenta, 4n evaporation channel.

doi: 10.1103/PhysRevC.48.319
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1993CI01      Phys.Rev. C47, 1294 (1993)

J.A.Cizewski, M.A.C.Hotchkis, J.L.Durell, J.Copnell, A.S.Mowbray, J.Fitzgerald, W.R.Phillips, I.Ahmad, M.P.Carpenter, R.V.F.Janssens, T.L.Khoo, E.F.Moore, L.R.Morss, Ph.Benet, D.Ye

New N = 84 Isotone: 136Te

RADIOACTIVITY 248Cm(SF); measured γγ-coin. 252Cf(SF); measured Eγ, Iγ. 136Te deduced levels, J, π, transitions.

doi: 10.1103/PhysRevC.47.1294
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1993KH06      Nucl.Phys. A557, 83c (1993)

T.L.Khoo, T.Lauritsen, I.Ahmad, M.P.Carpenter, P.B.Fernandez, R.V.F.Janssens, E.F.Moore, F.L.H.Wolfs, Ph.Benet, P.J.Daly, K.B.Beard, U.Garg, D.Ye, M.W.Drigert

Feeding and Decay of Superdeformed States

NUCLEAR STRUCTURE 192Hg; analyzed superdeformed band feeding, decay data; deduced mechanisms.

doi: 10.1016/0375-9474(93)90533-4
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1993PL01      Phys.Rev. C47, 2378 (1993)

A.J.M.Plompen, M.N.Harakeh, W.H.A.Hesselink, G.van't Hof, N.Kalantar-Nayestanaki, J.P.S.van Schagen, R.V.F.Janssens, I.Ahmad, I.G.Bearden, M.P.Carpenter, T.L.Khoo, T.Lauritsen, Y.Liang, U.Garg, W.Reviol, D.Ye

Lack of Evidence for a Superdeformed Band in 192Pb

NUCLEAR REACTIONS 173Yb(24Mg, 5n), E=132 MeV; measured γγ-coin, DSA. 192Pb deduced no superdeformed band.

doi: 10.1103/PhysRevC.47.2378
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1993PL02      Nucl.Phys. A562, 61 (1993)

A.J.M.Plompen, M.N.Harakeh, W.H.A.Hesselink, G.van't Hof, N.Kalantar-Nayestanaki, J.P.S.van Schagen, M.P.Carpenter, I.Ahmad, I.G.Bearden, R.V.F.Janssens, T.L.Khoo, T.Lauritsen, Y.Liang, U.Garg, W.Reviol, D.Ye

Collective and Quasiparticle Structure in 192Pb

NUCLEAR REACTIONS 173Yb(24Mg, 5n), E=132 MeV; measured Eγ, Iγ, γγ(θ), γγ(t), γγ-coin. 192Pb deduced levels, J, π. Enriched target, Compton-suppressed Ge-detectors, central array of BGO detectors. Cranked shell model calculations.

doi: 10.1016/0375-9474(93)90032-S
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1993RE09      Nucl.Phys. A557, 391c (1993)

W.Reviol, U.Garg, I.Ahmad, A.Aprahamian, M.P.Carpenter, B.F.Davis, R.V.F.Janssens, T.L.Khoo, T.Lauritsen, Y.Liang, S.Naguleswaran, J.C.Walpe, D.Ye

Spectroscopy of 96,97,98Ru: Possible emergence of collectivity at N ≥ 52

NUCLEAR REACTIONS 65Cu(36S, xnp), E=135, 142 MeV; measured γγ-coin. 96,97,98Ru deduced levels, J, possible π, γ multipolarity.

doi: 10.1016/0375-9474(93)90556-D
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1992BE18      Z.Phys. A341, 491 (1992)

I.G.Bearden, R.V.F.Janssens, M.P.Carpenter, E.F.Moore, I.Ahmad, A.M.Baxter, Ph.Benet, P.J.Daly, M.W.Drigert, P.B.Fernandez, U.Garg, Z.W.Grabowski, T.L.Khoo, T.Lauritsen, W.Reviol, D.Ye

Characterization of the Superdeformed Band in 189Hg

NUCLEAR REACTIONS 160Gd(34S, 5n), E=165 MeV; measured γγ-coin. 189Hg deduced superdeformed band, levels, J, π.

doi: 10.1007/BF01301395
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1992LA07      Phys.Lett. 279B, 239 (1992)

T.Lauritsen, R.V.F.Janssens, M.P.Carpenter, E.F.Moore, I.Ahmad, P.B.Fernandez, T.L.Khoo, J.A.Kuehner, D.Prevost, J.C.Waddington, U.Garg, W.Reviol, D.Ye, M.W.Drigert

Dynamic Moment of Inertia of the 192Hg Superdeformed Band at High Rotational Frequencies

NUCLEAR REACTIONS 160Gd(36S, 4n), E=154-167 MeV; measured γγγ-coin. 192Hg deduced superdeformed states, relative Iγ, increasing dynamic moment of inertia.

doi: 10.1016/0370-2693(92)90386-I
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1992LA19      Phys.Rev.Lett. 69, 2479 (1992)

T.Lauritsen, Ph.Benet, T.L.Khoo, K.B.Beard, I.Ahmad, M.P.Carpenter, P.J.Daly, M.W.Drigert, U.Garg, P.B.Fernandez, R.V.F.Janssens, E.F.Moore, F.L.H.Wolfs, D.Ye

Feeding of Superdeformed Bands: The mechanism and constraints on band energies and the well depth

NUCLEAR REACTIONS 160Gd(36S, 4n), E=159 MeV; measured γγ-coin. 192Hg deduced superdeformed band feeding, entry distribution features.

doi: 10.1103/PhysRevLett.69.2479
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1992RE08      Nucl.Phys. A548, 331 (1992)

W.Reviol, M.P.Carpenter, U.Garg, R.V.F.Janssens, I.Ahmad, I.G.Bearden, Ph.Benet, P.J.Daly, M.W.Drigert, P.B.Fernandez, T.L.Khoo, E.F.Moore, S.Pilotte, D.Ye

Shape-Driving Effects in 193Tl from the Spectroscopy of Yrast and Near-Yrast States

NUCLEAR REACTIONS 160Gd(37Cl, 4n), E=167 MeV; measured Eγ, Iγ, γγ-coin, DCO ratios. 193Tl deduced levels, J, π, band structures, deformation. Enriched targets, Compton-suppressed Ge detectors, 4π BGO array. Total Routhian surface, cranked shell model calculations.

doi: 10.1016/0375-9474(92)90014-B
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1992YE01      Nucl.Phys. A537, 207 (1992)

D.Ye, K.B.Beard, U.Garg, R.V.F.Janssens, M.P.Carpenter, I.Ahmad, T.L.Khoo, E.F.Moore, F.L.H.Wolfs, Ph.Benet, Z.W.Grabowski, M.W.Drigert

Multiple Band Structures in 191Hg

NUCLEAR REACTIONS 160Gd(36S, 5n), E=162, 167, 172 MeV; measured Eγ, Iγ, γγ(θ), Doppler shifts. 191Hg deduced levels, J, π band structures, deformation. Enriched target, Compton-suppressed Ge-detectors, central array of BGO hexagons. Cranked shell model calculations.

doi: 10.1016/0375-9474(92)90165-G
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1991DR04      Nucl.Phys. A530, 452 (1991)

M.W.Drigert, M.P.Carpenter, R.V.F.Janssens, E.F.Moore, I.Ahmad, P.B.Fernandez, T.L.Khoo, F.L.H.Wolfs, I.G.Bearden, Ph.Benet, P.J.Daly, U.Garg, W.Reviol, D.Ye, R.Wyss

Superdeformed Bands in 189,190Hg

NUCLEAR REACTIONS 160Gd(34S, xn), E=159, 162 MeV; measured Eγ, Iγ, γγ-coin, DSA. 189,190Hg deduced levels, J, π, T1/2, superdeformed band characteristics. Enriched targets, Ge detectors, array of anti-Compton spectrometers, 4π bismuth germanate ball. Cranked Woods-Saxon model calculations.

doi: 10.1016/0375-9474(91)90813-L
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1991HO16      Nucl.Phys. A530, 111 (1991)

M.A.C.Hotchkis, J.L.Durell, J.B.Fitzgerald, A.S.Mowbray, W.R.Phillips, I.Ahmad, M.P.Carpenter, R.V.F.Janssens, T.L.Khoo, E.F.Moore, L.R.Morss, Ph.Benet, D.Ye

Rotational Bands in the Mass 100 Region

RADIOACTIVITY 248Cm(SF); measured Eγ, γγ-coin. 98,99,100Sr, 99,101Y, 100,101,102,103,104Zr, 101,103,105Nb, 102,103,104,105,106,107,108Mo deduced levels.

doi: 10.1016/0375-9474(91)90758-X
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1991MO11      Phys.Lett. 258B, 284 (1991)

E.F.Moore, R.V.F.Janssens, I.Ahmad, M.P.Carpenter, A.M.Baxter, M.E.Bleich, P.B.Fernandez, T.Lauritsen, T.L.Khoo, I.G.Bearden, Ph.Benet, P.J.Daly, U.Garg, W.Reviol, D.Ye

K X-Ray Yields Associated with the Superdeformed Band of 192Hg

NUCLEAR REACTIONS 160Gd(36S, 4n), E=159 MeV; measured γ-, X-ray spectra, γ(X-ray)-coin, X-ray yields. 192Hg; deduced no strong superdeformed band E0 decay.

doi: 10.1016/0370-2693(91)91086-B
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1990CA18      Phys.Lett. 240B, 44 (1990)

M.P.Carpenter, R.V.F.Janssens, E.F.Moore, I.Ahmad, P.B.Fernandez, T.L.Khoo, F.L.H.Wolfs, D.Ye, K.B.Beard, U.Garg, M.W.Drigert, Ph.Benet, R.Wyss, W.Satula, W.Nazarewicz, M.A.Riley

Excited Superdeformed Bands in 191Hg

NUCLEAR REACTIONS 160Gd(36S, 5n), E=167, 172 MeV; measured γγ-coin. 191Hg deduced levels, J, π, superdeformed band structure.

doi: 10.1016/0370-2693(90)90406-V
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1990CA37      Nucl.Phys. A520, 133c (1990)

M.P.Carpenter, D.Ye, R.V.F.Janssens, T.L.Khoo, I.Ahmad, K.B.Beard, Ph.Benet, J.A.Cizewski, M.W.Drigert, P.Fernandez, U.Garg, E.F.Moore, F.L.H.Wolfs

Evidence of Time Delay in the Decay of the Superdeformed Bands of 191,192Hg

NUCLEAR REACTIONS 160Gd(36S, 4n), (36S, 5n), E=167 MeV; measured γγ-coin. 191,192Hg deduced levels, J, π, superdeformed band decay time delay.

doi: 10.1016/0375-9474(90)91141-D
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1990FE07      Nucl.Phys. A517, 386 (1990)

P.B.Fernandez, M.P.Carpenter, R.V.F.Janssens, I.Ahmad, E.F.Moore, T.L.Khoo, F.Scarlassara, I.G.Bearden, Ph.Benet, P.J.Daly, M.W.Drigert, U.Garg, W.Reviol, D.Ye, S.Pilotte

Proton Excitations in the Superdeformed Well of 193Tl

NUCLEAR REACTIONS 160Gd(37Cl, 4n), E=167 MeV; measured Eγ, Iγ, γγ-coin. 193Tl deduced levels, J, π, rotational, superdeformed bands characteristics. Enriched targets, Ge detectors, array of Compton suppressed spectrometers, 4π bismuth germanate array. Cranked Woods-Saxon calculations.

doi: 10.1016/0375-9474(90)90041-J
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1990GA07      Phys.Rev. C41, 1845 (1990)

U.Garg, K.B.Beard, D.Ye, A.Galonsky, T.Murakami, J.S.Winfield, Y.-W.Lui, D.H.Youngblood

Experimental Test of a Newly Proposed Empirical Relationship between the Centroid and Width of the Giant Quadrupole Resonance and the Neutron Binding Energy of the Nucleus

NUCLEAR REACTIONS 58,64Ni(14N, 14N'), E=700 MeV; measured σ(E(14N)). 58,64Ni deduced GDR parameters.

doi: 10.1103/PhysRevC.41.1845
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1990HO12      Phys.Rev.Lett. 64, 3123 (1990)

M.A.C.Hotchkis, J.L.Durell, J.B.Fitzgerald, A.S.Mowbray, W.R.Phillips, I.Ahmad, M.P.Carpenter, R.V.F.Janssens, T.L.Khoo, E.F.Moore, L.R.Morss, Ph.Benet, D.Ye

New Neutron-Rich Nuclei 103,104Zr and the A ≈ 100 Region of Deformation

RADIOACTIVITY 252Cf(SF); measured prompt Eγ, Iγ. 100,101,102,103,104Zr deduced levels, possible J, π, configuration.

doi: 10.1103/PhysRevLett.64.3123
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1990JA13      Nucl.Phys. A520, 75c (1990)

R.V.F.Janssens, M.P.Carpenter, M.W.Drigert, P.B.Fernandez, E.F.Moore, D.Ye, I.Ahmad, K.B.Beard, I.G.Bearden, Ph.Benet, P.J.Daly, U.Garg, Z.W.Grabowski, T.L.Khoo, W.Reviol, F.L.H.Wolfs

Superdeformation in the Mercury Nuclei

NUCLEAR STRUCTURE 194,196Pb, 193,194Tl, 189,190,191,192,193,194Hg; compiled, analyzed superdeformed band data.

doi: 10.1016/0375-9474(90)91135-E
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1990KH06      Nucl.Phys. A520, 169c (1990)

T.L.Khoo, R.V.F.Janssens, E.F.Moore, K.B.Beard, Ph.Benet, I.Ahmad, M.P.Carpenter, R.R.Chasman, P.J.Daly, M.W.Drigert, U.Garg, Z.W.Grabowski, F.L.H.Wolfs, D.Ye

Population of Superdeformed Bands, the Competition with Fission, and the Barrier between Normal and Superdeformed States

NUCLEAR REACTIONS 160Gd(36S, 4n), E=154-172 MeV; 120Sn(36S, 4n), E=170 MeV; measured γγ-coin, γ-multiplicity. 152Dy, 192Hg deduced superdeformed band level entry, feeding spin features.

doi: 10.1016/0375-9474(90)91144-G
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1990MO16      Phys.Rev.Lett. 64, 3127 (1990)

E.F.Moore, R.V.F.Janssens, I.Ahmad, M.P.Carpenter, P.B.Fernandez, T.L.Khoo, S.L.Ridley, F.L.H.Wolfs, D.Ye, K.B.Beard, U.Garg, M.W.Drigert, Ph.Benet, P.J.Daly, R.Wyss, W.Nazarewicz

Lifetime Measurements in the Superdeformed Band of 192Hg

NUCLEAR REACTIONS 160Gd(36S, 4n), E=159 MeV; measured γγ-coin, DSA. 192Hg deduced levels, T1/2, B(E2), transition quadrupole moment, J, π, superdeformed band structure.

doi: 10.1103/PhysRevLett.64.3127
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1990MO18      Phys.Rev. C42, 1126 (1990)

A.S.Mowbray, I.Ahmad, Ph.Benet, R.F.Casten, M.P.Carpenter, J.L.Durell, J.B.Fitzgerald, M.A.C.Hotchkis, R.V.F.Janssens, T.L.Khoo, E.F.Moore, L.R.Morss, W.R.Phillips, W.Walters, D.Ye

New Nucleus 142Xe: Test of the N(p)N(n) scheme

RADIOACTIVITY 248Cm(SF); measured fragment decay γγ-coin. 142Xe deduced levels, J, π. Model NpNn scheme comparison.

doi: 10.1103/PhysRevC.42.1126
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1990YE01      Phys.Rev. C41, R13 (1990)

D.Ye, R.V.F.Janssens, M.P.Carpenter, E.F.Moore, R.R.Chasman, I.Ahmad, K.B.Beard, Ph.Benet, M.W.Drigert, P.B.Fernandez, U.Garg, T.L.Khoo, S.L.Ridley, F.L.H.Wolfs

Superdeformed Band in 192Hg

NUCLEAR REACTIONS 160Gd(36S, 4n), E=162 MeV; measured γγ-coin. 192Hg deduced levels, J, π, superdeformed band structure.

doi: 10.1103/PhysRevC.41.R13
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1990YE03      Phys.Lett. 236B, 7 (1990)

D.Ye, R.V.F.Janssens, M.P.Carpenter, E.F.Moore, I.Ahmad, K.B.Beard, Ph.Benet, M.W.Drigert, U.Garg, Z.W.Grabowski, T.L.Khoo, F.L.H.Wolfs, T.Bengtsson, I.Ragnarsson

Nucleon Alignment in 191Hg. A Competing Mechanism at Moderate Spins

NUCLEAR REACTIONS 160Gd(36S, 5n), E=169 MeV; measured γγ-coin, DCO. 191Hg deduced levels, J, π, configuration, band structure.

doi: 10.1016/0370-2693(90)90585-T
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1989MO08      Phys.Rev.Lett. 63, 360 (1989)

E.F.Moore, R.V.F.Janssens, R.R.Chasman, I.Ahmad, T.L.Khoo, F.L.H.Wolfs, D.Ye, K.B.Beard, U.Garg, M.W.Drigert, Ph.Benet, Z.W.Grabowski, J.A.Cizewski

Observation of Superdeformation in 191Hg

NUCLEAR REACTIONS 160Gd(36S, 5n), E=172 MeV; measured γγ-coin. 191Hg deduced superdeformed band structure, shape characteristics.

doi: 10.1103/PhysRevLett.63.360
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