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Search: Author = H.M.Xu

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1998GA02      Phys.Rev.Lett. 80, 421 (1998)

C.A.Gagliardi, A.M.Mukhamedzhanov, R.E.Tribble, H.M.Xu

Comment on ' Angular Distribution for the 7Be(d, n)8B Reaction at E(c.m.) = 5.8 MeV and the S17(0) Factor for the 7Be(p, γ)8B Reaction '

NUCLEAR REACTIONS 7Be(p, γ), E(cm)=5.8 MeV; analyzed previous analysis; deduced uncertanties.

doi: 10.1103/PhysRevLett.80.421
Citations: PlumX Metrics


1998MU09      Nucl.Phys. A631, 788c (1998)

A.M.Mukhamedzhanov, H.L.Clark, H.Dejbakhsh, C.A.Gagliardi, Y.-W.Lui, L.Trache, R.E.Tribble, H.M.Xu, V.Burjan, J.Cejpek, V.Kroha, S.Piskor, J.Vincour, F.Carstoiu, A.Sattarov

Asymptotic Normalization Coefficients and Astrophysical Radiative Capture Reactions

NUCLEAR REACTIONS 9Be(10B, 9Be), E=100 MeV; 16O(3He, d), E=29.75 MeV; measured σ(θ); deduced virtual decays asymptotic normalization coefficients. 16O(p, γ), E < 2.5 MeV; deduced S-factor.

doi: 10.1016/S0375-9474(98)00110-9
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1335.


1997MU19      Phys.Rev. C56, 1302 (1997)

A.M.Mukhamedzhanov, H.L.Clark, C.A.Gagliardi, Y.-W.Lui, L.Trache, R.E.Tribble, H.M.Xu, X.G.Zhou, V.Burjan, J.Cejpek, V.Kroha, F.Carstoiu

Asymptotic Normalization Coefficients for 10B → 9Be + p

NUCLEAR REACTIONS 9Be(10B, 9Be), (10B, 10B), E=100 MeV; measured σ(E, θ); deduced optical model parameters, 9Be(10B, 9Be) reaction σ, asymptotic normalization coefficients for 10B → 9Be+p virtual decays. DWBA approach.

doi: 10.1103/PhysRevC.56.1302
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1996SE01      Phys.Rev. C53, 96 (1996)

D.R.Semon, M.C.Allen, H.Dejbakhsh, C.A.Gagliardi, S.E.Hale, J.Jiang, L.Trache, R.E.Tribble, S.J.Yennello, H.M.Xu, X.G.Zhou, B.A.Brown

l-Forbidden Gamow-Teller β Decay of 57Cu

RADIOACTIVITY 57Cu(β+) [from 1H(58Ni, 57Cu), E=29-31 MeV/nucleon]; measured βγ-coin, Eγ, Iγ, T1/2. 57Ni levels deduced l-forbidden, superallowed Gamow-Teller transition features, absolute branching ratio. Shell model comparison.

NUCLEAR STRUCTURE 29P, 29Si, 57Cu, 57Ni; calculated B(λ), B(GT). Shell model.

doi: 10.1103/PhysRevC.53.96
Citations: PlumX Metrics


1996TS01      Phys.Rev. C53, R1057 (1996)

M.B.Tsang, F.Zhu, W.G.Lynch, A.Aranda, D.R.Bowman, R.T.de Souza, C.K.Gelbke, Y.D.Kim, L.Phair, S.Pratt, C.Williams, H.M.Xu, W.A.Friedman

Cross Comparisons of Nuclear Temperatures Determined from Excited State Populations and Isotope Yields

NUCLEAR REACTIONS 197Au(36Ar, X), E=35 MeV/nucleon; measured 7,8Li, 3,4He isotope yields, other aspects; deduced temperatures.

doi: 10.1103/PhysRevC.53.R1057
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1996XU06      Phys.Rev. C54, 3266 (1996)

H.M.Xu, C.A.Gagliardi, G.K.Ajupova, B.Kokenge, Y.-W.Lui

Gamow-Teller Strength of 26Mg

NUCLEAR REACTIONS 26Mg(d, X), E=125.2 MeV; measured σ(θ(2He)), spectra; deduced (p, n) data may have significant systematic uncertainities. 26Na level deduced Gamow-Teller strength.

doi: 10.1103/PhysRevC.54.3266
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1995GA20      Nucl.Phys. A588, 327c (1995)

C.A.Gagliardi, R.E.Tribble, J.Jiang, A.M.Mukhamedzhanov, L.Trache, H.M.Xu, S.J.Yennello, X.G.Zhou

Determing S17(0) from the 10B(7Be, 8B)9Be Reaction

NUCLEAR REACTIONS 3He, 10B(7Be, 8B), E=100 MeV; calculated σ(θ). DWBA analysis, preliminary investigations for 10B(7Be, 8B) astrophysical S-factor.

doi: 10.1016/0375-9474(95)00157-V
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1995XU02      Phys.Rev. C52, R1161 (1995)

H.M.Xu, G.K.Ajupova, A.C.Betker, C.A.Gagliardi, B.Kokenge, Y.-W.Lui, A.F.Zaruba

(d, 2He) Reactions at E(d) = 125.2 MeV

NUCLEAR REACTIONS 6Li, 12,13C, 24Mg(d, X), E=125.2 MeV; measured spectra of 2He; deduced σ(θ) versus B(GT).

doi: 10.1103/PhysRevC.52.R1161
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0423.


1995ZH17      Phys.Rev. C52, 784 (1995)

F.Zhu, W.G.Lynch, D.R.Bowman, R.T.de SOuza, C.K.Gelbke, Y.D.Kim, L.Phair, M.B.Tsang, C.Williams, H.M.Xu

Impact Parameter Selected Excited State Populations for 36Ar + 197Au Reactions at E/A = 35 MeV

NUCLEAR REACTIONS 197Au(36Ar, X), E=35 MeV/nucleon; measured σ(fragment θ, E) for X=4He, 6Li, 7Be, 10Be; deduced impact parameter selected excited states population related features.

doi: 10.1103/PhysRevC.52.784
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1994LI19      Phys.Rev. C49, 2788 (1994)

M.A.Lisa, W.G.Gong, C.K.Gelbke, N.Carlin, R.T.de Souza, Y.D.Kim, W.G.Lynch, T.Murakami, G.Poggi, M.B.Tsang, H.M.Xu, K.Kwiatkowski, V.E.Viola, Jr., S.J.Yennello

Proton Evaporation Time Scales from Longitudinal and Transverse Two-Proton Correlation Functions

NUCLEAR REACTIONS 27Al(129Xe, X), E=31 MeV/nucleon; analyzed pp-correlations data; deduced evidence for emission from long-lived composite system.

doi: 10.1103/PhysRevC.49.2788
Citations: PlumX Metrics


1994SC15      Phys.Rev. C49, 3316 (1994)

C.Schwarz, W.G.Gong, N.Carlin, C.K.Gelbke, Y.D.Kim, W.G.Lynch, T.Murakami, G.Poggi, R.T.de Souza, M.B.Tsang, H.M.Xu, K.Kwiatkowski, V.E.Viola, S.J.Yennello

Anomalous Populations of Particle-Unbound States in 10B

NUCLEAR REACTIONS 27Al, 197Au(14N, X), E=75 MeV/nucleon; 122Sn, 27Al(129Xe, X), E=31 MeV/nucleon; measured B fragments inclusive yields, (9Be)(p)-correlation functions. 10B deduced particle unstable states relative populations. Statistical calculations.

doi: 10.1103/PhysRevC.49.3316
Citations: PlumX Metrics


1994XU01      Nucl.Phys. A568, 365 (1994)

H.M.Xu

Limiting Temperatures and Disappearance of Fusionlike Residues

NUCLEAR REACTIONS 27Al(40Ar, X), E=25-40 MeV/nucleon; calculated residues angular momenta vs impact parameter, mass vs incident energy, other reaction dynamics. Improved Boltzmann-Uehling-Uhlenbeck model.

doi: 10.1016/0375-9474(94)90208-9
Citations: PlumX Metrics


1994XU02      Nucl.Phys. A569, 575 (1994)

H.M.Xu, C.A.Gagliardi, R.E.Tribble, C.Y.Wong

Multifragmentation of Toroidal and Bubble Nuclei within the BUU Approach

NUCLEAR REACTIONS 92Mo(92Mo, X), E=75, 85, 100 MeV/nucleon; calculated compressed state, average density, transverse excitation energy time evolution; deduced multi-fragmentation evidence. Improved Boltzmann-Uehling-Uhlenbeck model.

doi: 10.1016/0375-9474(94)90320-4
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1994XU04      Phys.Rev. C49, R1778 (1994)

H.M.Xu, C.A.Gagliardi, R.E.Tribble, C.Y.Wong

Fragmentation Barriers of Toroidal and Bubble Nuclei

NUCLEAR REACTIONS 92Mo(92Mo, X), E=75 MeV/nucleon; calculated toroidal, bubble nuclei formation deformation energy surfaces; deduced fragmentation barrier time evolution. Improved Boltzmann-Uehling-Uhlenbeck model.

doi: 10.1103/PhysRevC.49.R1778
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1994XU06      Phys.Rev. C50, 1659 (1994)

H.M.Xu, W.G.Lynch, P.Danielewicz

Residue Temperatures in Intermediate Energy Nucleus-Nucleus Collisions

NUCLEAR REACTIONS 124Sn(40Ar, X), E ≈ 35-100 MeV/nucleon; calculated nucleon emission rates, residues excitation energy, temperature, other quantities. Boltzmann-Uehling-Uhlenbeck model.

doi: 10.1103/PhysRevC.50.1659
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1994XU08      Phys.Rev.Lett. 73, 2027 (1994)

H.M.Xu, C.A.Gagliardi, R.E.Tribble, A.M.Mukhamedzhanov, N.K.Timofeyuk

Overall Normalization of the Astrophysical S Factor and the Nuclear Vertex Constant for 7Be(p, γ)8B Reactions

NUCLEAR REACTIONS, ICPND 7Be(p, γ), E(cm) ≤ 2 MeV; calculated astrophysical S-factor S(17) vs E; deduced nuclear vertex constant vs S-factor normalization.

doi: 10.1103/PhysRevLett.73.2027
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1994ZH06      Phys.Lett. 322B, 43 (1994)

F.Zhu, M.J.Huang, W.G.Lynch, T.Murakami, Y.D.Kim, T.K.Nayak, R.Pelak, M.B.Tsang, H.M.Xu, W.G.Gong, K.Kwiatkowski, R.Planeta, S.Rose, V.E.Viola, Jr., L.W.Woo, S.Yennello, J.Zhang

Excited State Populations for Equilibrium and Preequilibrium Emission

NUCLEAR REACTIONS Ag(3He, X), E=200 MeV; measured (particle)(particle)-coin; deduced 5,6Li excited state population ratio temperature dependence; deduced forward, backward fragment emission mechanisms difference.

doi: 10.1016/0370-2693(94)90489-8
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1993BE43      Phys.Rev. C48, 2085 (1993)

A.C.Betker, C.A.Gagliardi, D.R.Semon, R.E.Tribble, H.M.Xu, A.F.Zaruba

Deuteron Elastic Scattering at 110 and 120 MeV

NUCLEAR REACTIONS 12C, 58Ni, 208Pb(d, d), E=110-120 MeV; measured σ(θ); deduced optical model parameters.

doi: 10.1103/PhysRevC.48.2085
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1263.


1993GO01      Phys.Rev. C47, R429 (1993)

W.G.Gong, P.Danielewicz, C.K.Gelbke, N.Carlin, R.T.de Souza, Y.D.Kim, W.G.Lynch, T.Murakami, G.Poggi, M.B.Tsang, H.M.Xu, S.Pratt, K.Kwiatkowski, V.E.Viola, Jr., S.J.Yennello, J.C.Shillcock

Two-Deuteron Correlation Functions in 14N + 27Al Collisions at E/A = 75 MeV

NUCLEAR REACTIONS 27Al(14N, X), E=75 MeV/nucleon; measured dd-, pp-correlation functions; deduced ejectile time span differences. Microscopic transport model.

doi: 10.1103/PhysRevC.47.R429
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1993SC21      Phys.Rev. C48, 676 (1993)

C.Schwarz, W.G.Gong, N.Carlin, C.K.Gelbke, Y.D.Kim, W.G.Lynch, T.Murakami, G.Poggi, R.T.de Souza, M.B.Tsang, H.M.Xu, D.E.Fields, K.Kwiatkowski, V.E.Viola, Jr., S.J.Yennello

Emission Temperatures from Widely Separated States in 14N- and 129Xe-Induced Reactions

NUCLEAR REACTIONS 27Al, 197Au(14N, X), E=75 MeV/nucleon; 27Al, 122Sn(129Xe, X), E=31 MeV/nucleon; measured light charged particle relative momentum correlation functions, inclusive σ(fragment θ, E) for α, 6Li, 7Be; deduced nuclear temperatures of 4He, 5Li, and 8Be.

doi: 10.1103/PhysRevC.48.676
Citations: PlumX Metrics


1993XU01      Phys.Rev. C47, 891 (1993)

H.M.Xu

Disappearance of Rotation in Heavy-Ion Collisions

NUCLEAR REACTIONS 51V(40Ar, X), E=35-125 MeV/nucleon; calculated nucleon azimuthal distributions; deduced multi-fragmentation role in rotation disappearance. Boltzmann equation approach.

doi: 10.1103/PhysRevC.47.891
Citations: PlumX Metrics


1993XU02      Phys.Lett. 299B, 199 (1993)

H.M.Xu, P.Danielewicz, W.G.Lynch

Residue Temperatures and the Nuclear Equation of State

NUCLEAR REACTIONS 124Sn(40Ar, X), E=65 MeV/nucleon; calculated excitation energy/nucleon, nucleon emission rate vs time for heavy residues; deduced impact parameter dependence. Central collisions, Boltzmann-Uehling-Uhlenbeck model.

doi: 10.1016/0370-2693(93)90247-F
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1993XU03      Phys.Rev. C48, 933 (1993)

H.M.Xu, J.B.Natowitz, C.A.Gagliardi, R.E.Tribble, C.Y.Wong, W.G.Lynch

Formation and Decay of Toroidal and Bubble Nuclei and the Nuclear Equation of State

NUCLEAR REACTIONS 92Mo(92Mo, X), E=75-100 MeV/nucleon; calculated multi-fragment decay multiplicity. Stiff, soft equations of state, toroidal, bubble nuclei formation.

doi: 10.1103/PhysRevC.48.933
Citations: PlumX Metrics


1992NA01      Phys.Rev. C45, 132 (1992)

T.K.Nayak, T.Murakami, W.G.Lynch, K.Swartz, D.J.Fields, C.K.Gelbke, Y.D.Kim, J.Pochodzalla, M.B.Tsang, H.M.Xu, F.Zhu, K.Kwiatkowski

Emission Temperatures from the Decay of Particle Unstable Complex Nuclei

NUCLEAR REACTIONS Ag(14N, X), E=35 MeV/nucleon; measured σ(fragment θ, E) for X=Li, Be, B, C, N, O isotopes; deduced emission temperatures. Statistical model.

doi: 10.1103/PhysRevC.45.132
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1992WI04      Phys.Rev. C45, 2300 (1992)

J.L.Wile, D.E.Fields, K.Kwiatkowski, S.J.Yennello, K.B.Morley, E.Renshaw, V.E.Viola, C.K.Gelbke, W.G.Lynch, N.Carlin, H.M.Xu, W.G.Gong, M.B.Tsang, J.Pochodzalla, R.T.deSouza, D.J.Fields, S.M.Austin

Excitation Functions for Complex Fragment Emission in the E/A = 20-100 MeV 14N + (nag)Ag, 197Au Reactions

NUCLEAR REACTIONS Ag, 197Au(14N, X), E=20-100 MeV/nucleon; measured σ(fragment θ, E); deduced fragment emission mechanism. Three-source model.

doi: 10.1103/PhysRevC.45.2300
Citations: PlumX Metrics


1992XU03      Phys.Rev. C46, R389 (1992)

H.M.Xu

Disappearance of Flow and the In-Medium Nucleon-Nucleon Cross Section

NUCLEAR REACTIONS 51V(40Ar, X), E=50-120 MeV/nucleon; calculated fragment transverse momentum vs longitudinal rapidity, flow parameter vs E; deduced energy balance role in determining σ(n-n). Boltzmann equation.

doi: 10.1103/PhysRevC.46.R389
Citations: PlumX Metrics


1992XU05      Phys.Rev. C46, R2144 (1992)

H.M.Xu

Mass Asymmetry, Equation of State, and Nuclear Multifragmentation

NUCLEAR REACTIONS 92Mo(92Mo, X), E=75 MeV/nucleon; 51V(40Ar, X), E=35-75 MeV/nucleon; 51V(12C, X), E=75-200 MeV/nucleon; calculated density vs time, collective, expansion thermal energies vs time; deduced multifragmentation evidence, mechanism. Boltzmann-Uehling-Uhlenbeck model.

doi: 10.1103/PhysRevC.46.R2144
Citations: PlumX Metrics


1992ZH08      Phys.Lett. 282B, 299 (1992)

F.Zhu, W.G.Lynch, D.R.Bowman, R.T.de Souza, C.K.Gelbke, Y.D.Kim, L.Phair, M.B.Tsang, C.Williams, H.M.Xu, J.Dinius

Thermalization in Nucleus-Nucleus Collisions

NUCLEAR REACTIONS 197Au(36Ar, X), E=35 MeV/nucleon; measured σ(fragment θ, E) for X=10B, yields for 10B breakup into 6Li+α, 9Be+p; deduced thermalization population inversion features.

doi: 10.1016/0370-2693(92)90642-H
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1991DE33      Phys.Lett. 268B, 6 (1991)

R.T.de Souza, L.Phair, D.R.Bowman, N.Carlin, C.K.Gelbke, W.G.Gong, Y.D.Kim, M.A.Lisa, W.G.Lynch, G.F.Peaslee, M.B.Tsang, H.M.Xu, F.Zhu, W.A.Friedman

Multifragment Emission in the Reaction 36Ar + 197Au at E/A = 35, 50, 80, and 110 MeV

NUCLEAR REACTIONS 197Au(36Ar, X), E=35-110 MeV/nucleon; measured fragment multiplicity distributions, first, second moments. Statistical decay model.

doi: 10.1016/0370-2693(91)90913-B
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1991GO05      Phys.Rev. C43, 1804 (1991)

W.G.Gong, C.K.Gelbke, W.Bauer, N.Carlin, R.T.de Souza, Y.D.Kim, W.G.Lynch, T.Murakami, G.Poggi, D.P.Sanderson, M.B.Tsang, H.M.Xu, D.E.Fields, K.Kwiatkowski, R.Planeta, V.E.Viola, Jr., S.J.Yennello, S.Pratt

Space-Time Evolution of the Reactions 14N + 27Al, 197Au at E/A = 75 MeV and 129Xe + 27Al, 122Sn at E/A = 31 MeV Probed by Two-Proton Intensity Interferometry

NUCLEAR REACTIONS 27Al, 197Au(14N, 2p), E=75 MeV/nucleon; 27Al, 122Sn(129Xe, 2p), E=31 MeV/nucleon; measured two-proton correlation function; deduced reaction mechanism.

doi: 10.1103/PhysRevC.43.1804
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1991WI16      Phys.Lett. 264B, 26 (1991)

J.L.Wile, D.E.Fields, K.Kwiatkowski, K.B.Morley, E.Renshaw, S.J.Yennello, V.E.Viola, N.Carlin, C.K.Gelbke, W.G.Gong, W.G.Lynch, R.T.de Souza, M.B.Tsang, H.M.Xu

Complex Fragment Emission in the E/A = 60-100 MeV 14N + (nat)Ag, 197Au Reactions

NUCLEAR REACTIONS Ag, 197Au(14N, X), E=60-100 MeV/nucleon; measured fragment production σ(E) for fragment Z=3-15. Three-source model.

doi: 10.1016/0370-2693(91)90697-O
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1991XU03      Phys.Lett. 261B, 240 (1991)

H.M.Xu, W.G.Lynch, P.Danielewicz, G.F.Bertsch

Entrance Channel Effects and the Formation of Hot Nuclei

NUCLEAR REACTIONS 27Al(40Ar, X), E ≥ 25 MeV/nucleon; calculated heavy composite residue excitation, angular momenta. Hot nuclei, entrance channel effects, Boltzmann-Uehling-Uhlenbeck equation.

doi: 10.1016/0370-2693(91)90321-G
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1991XU04      Phys.Rev.Lett. 67, 2769 (1991)

H.M.Xu

Disappearance of Flow in Intermediate-Energy Nucleus-Nucleus Collisions

NUCLEAR REACTIONS 27Al(40Ar, X), E=40-120 MeV/nucleon; calculated flow parameter, transverse momentum distribution vs rapidity. Improved Boltzmann-Uehling-Uhlenbeck equation.

doi: 10.1103/PhysRevLett.67.2769
Citations: PlumX Metrics


1991ZH14      Phys.Rev. C44, R582 (1991)

F.Zhu, W.G.Lynch, T.Murakami, C.K.Gelbke, Y.D.Kim, T.K.Nayak, R.Pelak, M.B.Tsang, H.M.Xu, W.G.Gong, W.Bauer, K.Kwiatkowski, R.Planeta, S.Rose, V.E.Viola, Jr., L.W.Woo, S.Yennello, J.Zhang

Light Particle Correlations for the 3He + Ag Reaction at 200 MeV

NUCLEAR REACTIONS Ag(3He, 2pX), E=200 MeV; measured σ(Ep, θp), proton-proton correlation; deduced nuclear reaction source size, energy dependence.

doi: 10.1103/PhysRevC.44.R582
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1442.


1990DE46      Nucl.Instrum.Methods Phys.Res. A295, 109 (1990)

R.T.De Souza, N.Carlin, Y.D.Kim, J.Ottarson, L.Phair, D.R.Bowman, C.K.Gelbke, W.G.Gong, W.G.Lynch, R.A.Pelak, T.Peterson, G.Poggi, M.B.Tsang, H.M.Xu

The MSU Miniball 4π Fragment Detection Array

NUCLEAR REACTIONS 197Au(40Ar, X), E=35 MeV/nucleon; measured fragment spectra. Fast-plastic CSI(Tl) phoswich detectors.

doi: 10.1016/0168-9002(90)90429-A
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1990GO16      Phys.Lett. 246B, 21 (1990)

W.G.Gong, C.K.Gelbke, N.Carlin, R.T.de Souza, Y.D.Kim, W.G.Lynch, T.Murakami, G.Poggi, D.Sanderson, M.B.Tsang, H.M.Xu, D.E.Fields, K.Kwiatkowski, R.Planeta, V.E.Viola, Jr., S.J.Yennello, S.Pratt

Two-Proton Correlation Functions for Equilibrium and Non-Equilibrium Emission

NUCLEAR REACTIONS 122Sn, 197Au, 27Al(129Xe, 2p), E=31 MeV/nucleon; measured 2p-correlation functions; deduced emission process time scale differences.

doi: 10.1016/0370-2693(90)91301-Q
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1990GO32      Phys.Rev.Lett. 65, 2114 (1990)

W.G.Gong, W.Bauer, C.K.Gelbke, N.Carlin, R.T.de Souza, Y.D.Kim, W.G.Lynch, T.Murakami, G.Poggi, D.P.Sanderson, M.B.Tsang, H.M.Xu, S.Pratt, D.E.Fields, K.Kwiatkowski, R.Planeta, V.E.Viola, Jr., S.J.Yennello

Intensity-Interferometric Test of Nuclear Collision Geometries Obtained from the Boltzmann-Uehling-Uhlenbeck Equation

NUCLEAR REACTIONS 27Al(14N, X), E=75 MeV/nucleon; measured pp-correlation. Boltzmann-Uehling-Uhlenbeck equation based analysis.

doi: 10.1103/PhysRevLett.65.2114
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1990TS02      Phys.Rev. C42, R15 (1990)

M.B.Tsang, Y.D.Kim, N.Carlin, Z.Chen, C.K.Gelbke, W.G.Gong, W.G.Lynch, T.Murakami, T.Nayak, R.M.Ronningen, H.M.Xu, F.Zhu, L.G.Sobotka, D.W.Stracener, D.G.Sarantites, Z.Majka, V.Abenante

Azimuthal Distributions of Fission Fragments and α Particles Emitted in the Reactions 36Ar + 238U at E/A = 20 and 35 MeV and 14N + 238U at E/A = 50 MeV

NUCLEAR REACTIONS 238U(36Ar, F), E=20, 35 MeV/nucleon; 238U(14N, F), E=50 MeV/nucleon; measured fission (fragment)α(θ, φ); deduced in-plane, out of plane anisotropies.

doi: 10.1103/PhysRevC.42.R15
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1990XU03      Phys.Rev.Lett. 65, 843 (1990)

H.M.Xu, W.G.Lynch, P.Danielewicz, G.F.Bertsch

Disappearance of Fusionlike Residues and the Nuclear Equation of State

NUCLEAR REACTIONS, ICPND 40Ca(40Ca, X), E=20-60 MeV/nucleon; 27Al(40Ar, X), E=20-60 MeV/nucleon; calculated residue production σ(E).

doi: 10.1103/PhysRevLett.65.843
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1989KI12      Phys.Rev.Lett. 63, 494 (1989)

Y.D.Kim, M.B.Tsang, C.K.Gelbke, W.G.Lynch, N.Carlin, Z.Chen, R.Fox, W.G.Gong, T.Murakami, T.K.Nayak, R.M.Ronningen, H.M.Xu, F.Zhu, W.Bauer, L.G.Sobotka, D.Stracener, D.G.Sarantites, Z.Majka, V.Abenante, H.Griffin

Multifragment Emission Observed for the Reaction 36Ar + 238U at E/A = 35 MeV

NUCLEAR REACTIONS 238U(36Ar, X), E=35 MeV/nucleon; measured charged particle multiplicities; deduced reaction mechanism.

doi: 10.1103/PhysRevLett.63.494
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1989MU03      Nucl.Instrum.Methods Phys.Res. A275, 112 (1989)

T.Murakami, T.K.Nayak, W.G.Lynch, K.Swartz, Z.Chen, D.J.Fields, C.K.Gelbke, Y.D.Kim, M.R.Maier, J.Pochodzalla, M.B.Tsang, H.M.Xu, F.Zhu

A Position Sensitive High Resolution Hodoscope for Particle Unstable Intermediate Mass Fragments

NUCLEAR REACTIONS Ag(14N, p13C), E=35 MeV/nucleon; measured p(13C)-correlation, σ(E(relative)); deduced projectile fragment decay.

doi: 10.1016/0168-9002(89)90341-0
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1989NA03      Phys.Rev.Lett. 62, 1021 (1989)

T.K.Nayak, T.Murakami, W.G.Lynch, K.Swartz, D.J.Fields, C.K.Gelbke, Y.D.Kim, J.Pochodzalla, M.B.Tsang, H.M.Xu, F.Zhu, K.Kwiatkowski

Fragmentation Products with Nonstatistical Excited-State Populations

NUCLEAR REACTIONS Ag(14N, 10B), E=35 MeV/nucleon; measured σ(θ(10B), E(10B)). 10B deduced particle unstable levels, relative population probability.

doi: 10.1103/PhysRevLett.62.1021
Citations: PlumX Metrics


1989TS01      Phys.Lett. 220B, 492 (1989)

M.B.Tsang, Y.D.Kim, N.Carlin, Z.Chen, R.Fox, C.K.Gelbke, W.G.Gong, W.G.Lynch, T.Murakami, T.K.Nayak, R.M.Ronningen, H.M.Xu, F.Zhu, L.Sobotka, D.Stracener, D.G.Sarantites, Z.Majka, V.Abenante, H.Griffin

Reaction Filters. Charged-Particle Multiplicity and Linear Momentum Transfer

NUCLEAR REACTIONS 238U(36Ar, X), E=35 MeV/nucleon; 238U(14N, X), E=50 MeV/nucleon; measured charged particle multiplicity vs θ(ff). 4π charged particle detector.

doi: 10.1016/0370-2693(89)90774-0
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1989XU02      Phys.Rev. C40, 186 (1989)

H.M.Xu, W.G.Lynch, C.K.Gelbke, M.B.Tsang, D.J.Fields, M.R.Maier, D.J.Morrissey, T.K.Nayak, J.Pochodzalla, D.G.Sarantites, L.G.Sobotka, M.L.Halbert, D.C.Hensley

Complex Fragments Emitted in Particle-Stable States for the 32S + (nat)Ag Reaction at E/A = 22.3 MeV

NUCLEAR REACTIONS Ag(32S, X), E=22.3 MeV/nucleon; measured σ(fragment θ, E); deduced reaction mechanism.

doi: 10.1103/PhysRevC.40.186
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1988AW01      Phys.Rev.Lett. 61, 2665 (1988)

T.C.Awes, R.L.Ferguson, F.E.Obenshain, F.Plasil, G.R.Young, S.Pratt, Z.Chen, C.K.Gelbke, W.G.Lynch, J.Pochodzalla, H.M.Xu

Extended Emission Sources Observed via Two-Proton Correlations

NUCLEAR REACTIONS Ag(32S, pX), E=715 MeV; measured pp-correlation; deduced emission mechanism.

doi: 10.1103/PhysRevLett.61.2665
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1986XU02      Phys.Lett. 182B, 155 (1986)

H.M.Xu, D.J.Fields, W.G.Lynch, M.B.Tsang, C.K.Gelbke, M.R.Maier, D.J.Morrissey, J.Pochodzalla, D.G.Sarantites, L.G.Sobotka, M.L.Halbert, D.C.Hensley, D.Hahn, H.Stocker

Nuclear Temperature Measurements and Feeding from Particle Unbound States

NUCLEAR REACTIONS Ag(32S, X), E=715 MeV; measured fragment σ, γ-ray spectra, fractional probabilities, X=8Li, 7Be, 10,12B, 13C. ΔE-ΔE-E detector telescopes, Ge detectors.

doi: 10.1016/0370-2693(86)91568-6
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