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NSR database version of April 11, 2024.

Search: Author = S.W.Huang

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2023EL04      Phys.Lett. B 844, 138072 (2023)

Z.Elekes, V.Panin, T.R.Rodriguez, K.Sieja, D.S.Ahn, A.Al-Adili, H.Baba, A.I.Stefanescu, K.J.Cook, Cs.Dosa, N.Fukuda, J.Gao, J.Gibelin, K.I.Hahn, Z.Halasz, S.W.Huang, T.Isobe, M.M.Juhasz, D.Kim, T.Kobayashi, Y.Kondo, Z.Korkulu, A.Kurihara, I.Kuti, H.Miki, K.Miki, T.Motobayashi, H.Otsu, A.Saastamoinen, M.Sasano, H.Sato, T.Shimada, Y.Shimizu, L.G.Sobotka, I.Stefanescu, L.Stuhl, H.Suzuki, H.Takeda, Y.Togano, T.Tomai, L.Trache, D.Tudor, T.Uesaka, Y.Utsuki, H.Wang, A.Yasuda, K.Yoneda, Y.Yoshitome

Shape coexistence in 66Se

NUCLEAR REACTIONS 12C(67Se, n)66Se, E=170-250 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced γ-ray energies and relative intensities, γ-ray production σ, J, π, partial level scheme, shape coexistence. Comparison with theoretical calculations. The CATANA array, Radioactive Isotope Beam Factory operated by the RIKEN Nishina Center and by the Center for Nuclear Study of the University of Tokyo.

doi: 10.1016/j.physletb.2023.138072
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2022HA10      Phys.Rev. C 105, 044302 (2022)

J.X.Han, Y.Liu, Y.L.Ye, J.L.Lou, X.F.Yang, T.Baba, M.Kimura, B.Yang, Z.H.Li, Q.T.Li, J.Y.Xu, Y.C.Ge, H.Hua, Z.H.Yang, J.S.Wang, Y.Y.Yang, P.Ma, Z.Bai, Q.Hu, W.Liu, K.Ma, L.C.Tao, Y.Jiang, L.Y.Hu, H.L.Zang, J.Feng, H.Y.Wu, S.W.Bai, G.Li, H.Z.Yu, S.W.Huang, Z.Q.Chen, X.H.Sun, J.J.Li, Z.W.Tan, Z.H.Gao, F.F.Duan, J.H.Tan, S.Q.Sun, Y.S.Song

Observation of the π2σ2-bond linear-chain molecular structure in 16C

NUCLEAR REACTIONS 2H(16C, X)16C/2H/1H/2H/3H/3He/4He/5He/6He/6Li/7Li/8Li/9Li/7Be/8Be/9Be/10Be/11Be/12Be, E=23.5 MeV/nucleon; measured reaction products, recoil 2H, 8Be and other outgoing particles; deduced Q-value spectra for breakup of excited states of 16C into 4He+12Be and 6He+10Be channels, angular correlation between 4He and 12Be decay fragments from the 16.5 MeV resonance in 16C, and 6He and 10Be fragments from the 19.4 MeV resonance in 16C. 16C; deduced excitation energy spectra reconstructed from 4He+12Be+2 H and 6He+10Be+2H channels, levels, resonances, total width. Comparison with previous experimental data, and with antisymmetrized molecular dynamics (AMD) theoretical calculations. Secondary 16C beam produced in 9Be(18O, X), E=59.6 MeV/nucleon primary reaction at the HIRFL-RIBLL facility in Lanzhou.

doi: 10.1103/PhysRevC.105.044302
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2022TA09      Chin.Phys.C 46, 054001 (2022)

Z.W.Tan, J.L.Lou, Y.L.Ye, Y.Liu, D.Y.Pang, C.X.Yuan, J.G.Li, W.Liu, Y.Jiang, B.Yang, L.C.Tao, K.Ma, Z.H.Li, Q.T.Li, X.F.Yang, J.Y.Xu, H.Z.Yu, J.X.Han, S.W.Bai, S.W.Huang, G.Li, H.Y.Wu, H.L.Zang, J.Feng, J.S.Wang, Y.Y.Yang, P.Ma, Q.Hu, Z.Bai, Z.H.Gao, F.F.Duan, L.Y.Hu, J.H.Tan, S.Q.Sun, Y.S.Song, H.J.Ong, D.T.Tran, H.Y.Zhu, B.L.Xia

Investigation of negative-parity states in 16C via deuteron inelastic scattering

NUCLEAR REACTIONS 16C(d, d'), E=59.6 MeV/nucleon; measured reaction products; deduced σ(θ), optical model potentials, deformation lengths, energy levels, J, π. Comparison with the distorted-wave Born approximation (DWBA) and shell model calculations. The Radioactive Ion Beam Line in Lanzhou (RIBLL), Institute of Modern Physics (IMP), China.

doi: 10.1088/1674-1137/ac488b
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2021HU28      Few-Body Systems 62, 102 (2021)

S.W.Huang, Z.H.Yang, F.M.Marques, N.L.Achouri, D.S.Ahn, T.Aumann, H.Baba, D.Beaumel, M.Bohmer, K.Boretzky, M.Caamano, S.Chen, N.Chiga, M.L.Cortes, D.Cortina, P.Doornenbal, C.A.Douma, F.Dufter, J.Feng, B.Fernandez-Dominguez, Z.Elekes, U.Forsberg, T.Fujino, N.Fukuda, I.Gasparic, Z.Ge, R.Gernhauser, J.M.Gheller, J.Gibelin, A.Gillibert, Z.Halasz, T.Harada, M.N.Harakeh, A.Hirayama, N.Inabe, T.Isobe, J.Kahlbow, N.Kalantar-Nayestanaki, D.Kim, S.Kim, S.Kiyotake, T.Kobayashi, Y.Kondo, P.Koseoglou, Y.Kubota, I.Kuti, C.Lehr, C.Lenain, P.J.Li, Y.Liu, Y.Maeda, S.Masuoka, M.Matsumoto, A.Matta, J.Mayer, H.Miki, M.Miwa, B.Monteagudo, I.Murray, T.Nakamura, A.Obertelli, N.A.Orr, H.Otsu, V.Panin, S.Park, M.Parlog, S.Paschalis, M.Potlog, S.Reichert, A.Revel, D.Rossi, A.Saito, M.Sasano, H.Sato, H.Scheit, F.Schindler, T.Shimada, Y.Shimizu, S.Shimoura, H.Simon, I.Stefan, S.Storck, L.Stuhl, H.Suzuki, D.Symochko, H.Takeda, S.Takeuchi, J.Tanaka, Y.Togano, T.Tomai, H.T.Tornqvist, E.Tronchin, J.Tscheuschner, T.Uesaka, V.Wagner, K.Wimmer, H.Yamada, B.Yang, L.Yang, Y.Yasuda, K.Yoneda, L.Zanetti, J.Zenihiro

Experimental Study of 4n by Directly Detecting the Decay Neutrons

RADIOACTIVITY 7H(t), 6He(2n) [from 1H(8He, 2p), E=150 MeV/nucleon]; measured decay products, En, In. 4NN; deduced relative-energy spectrum, neutron multiplicity distribution. The radioactive isotope beam factory (RIBF).

doi: 10.1007/s00601-021-01691-4
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2020LI14      Phys.Rev.Lett. 124, 192501 (2020)

Y.Liu, Y.L.Ye, J.L.Lou, X.F.Yang, T.Baba, M.Kimura, B.Yang, Z.H.Li, Q.T.Li, J.Y.Xu, Y.C.Ge, H.Hua, J.S.Wang, Y.Y.Yang, P.Ma, Z.Bai, Q.Hu, W.Liu, K.Ma, L.C.Tao, Y.Jiang, L.Y.Hu, H.L.Zang, J.Feng, H.Y.Wu, J.X.Han, S.W.Bai, G.Li, H.Z.Yu, S.W.Huang, Z.Q.Chen, X.H.Sun, J.J.Li, Z.W.Tan, Z.H.Gao, F.F.Duan, J.H.Tan, S.Q.Sun, Y.S.Song

Positive-Parity Linear-Chain Molecular Band in 16C

NUCLEAR REACTIONS 2H(16C, X)2H, E=23.5 MeV/nucleon; measured reaction products, Eα, Iα. 16C; deduced excitation energies, spin parities, total decay widths of the resonances in 16C. Comparison with AMD calculations.

doi: 10.1103/PhysRevLett.124.192501
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1997TS08      Aust.J.Phys. 50, 35 (1997)

K.Tsushima, S.W.Huang, A.Faessler

A Study of the πB → YK Reactions for Kaon Production in Heavy Ion Collisions

NUCLEAR REACTIONS 1H(π+, K+X), (π-, K+X), (π-, K0X), E=high; 1n(π+, K+X), (π0, K+X), E=high; analyzed Λ, Σ production associated σ; deduced parameters. Microscopic transport models.

doi: 10.1071/P96052
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1997ZI01      J.Phys.(London) G23, L1 (1997)

J.Zipprich, C.Fuchs, E.Lehmann, L.Sehn, S.W.Huang, A.Faessler

Influence of the Pion-Nucleon Interaction on the Collective Pion Flow in Heavy Ion Reactions

NUCLEAR REACTIONS La(La, X), E=1.35 GeV/nucleon; analyzed pion spectra. Ca(Ca, X), E=1 GeV/nucleon; analyzed pion flow vs impact parameter; deduced pion-nucleon interaction role.

doi: 10.1088/0954-3899/23/1/001
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1996LE08      Z.Phys. A355, 55 (1996)

E.Lehmann, A.Faessler, J.Zipprich, R.K.Puri, S.W.Huang

Study of In-Medium Effects on the Disappearance of the Sidewards Flow in Heavy-Ion Collisions

NUCLEAR REACTIONS 27Al(20Ne, X), 45Sc(Ar, X), 93Nb(84Kr, X), E ≤ 170 MeV/nucleon; calculated transverse momentum vs E. Quantum molecular dynamics model.

doi: 10.1007/s002180050077
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1996LO24      Nucl.Phys. A611, 568 (1996)

B.Lopez Alvaredo, E.Oset, M.J.Vicente-Vacas, S.W.Huang, P.Fernandez de Cordoba, A.Faessler

Coherent, Semicoherent and Incoherent Pion Production in Heavy-Ion Reactions

NUCLEAR REACTIONS 12C(12C, X), E ≤ 600 MeV/nucleon; calculated coherent, semi-incoherent, incoherent pion production σ(θ).

doi: 10.1016/S0375-9474(96)00299-0
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1995LE05      Phys.Rev. C51, 2113 (1995)

E.Lehmann, R.K.Puri, A.Faessler, G.Batko, S.W.Huang

Consequences of a Convariant Description of Heavy-Ion Reactions at Intermediate Energies

NUCLEAR REACTIONS C(C, X), E=50 MeV/nucleon; Ca(Ca, X), E=1.5, 2 GeV/nucleon; calculated nucleon flow, directed transverse flow; deduced convariant description importance. Relativistic quantum molecular dynamics approach.

doi: 10.1103/PhysRevC.51.2113
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1995PU02      Z.Phys. A351, 59 (1995)

R.K.Puri, E.Lehmann, A.Faessler, S.W.Huang

Relativistic Effects in Heavy-Ion Collisions at SIS Energies

NUCLEAR REACTIONS 12C(12C, X), 16O(16O, X), 20Ne(20Ne, X), 28Si(28Si, X), 40Ca(40Ca, X), E=0.05-2GeV/nucleon; calculated time evolution, average collision rate, rapidity distribution. Convariant, noncovariant quantum molecular dynamics model.

doi: 10.1007/BF01292786
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1995PU03      J.Phys.(London) G21, 583 (1995)

R.K.Puri, E.Lehmann, A.Faessler, S.W.Huang

Sensitivity of the Nuclear Equation of State to Relativistic Effects

NUCLEAR REACTIONS 40Ca(40Ca, X), E ≤ 2000 MeV/nucleon; calculated relativistic effect vs E, scaled impact parameter. Equation of state approach, relativistic quantum molecular dynamics.

doi: 10.1088/0954-3899/21/4/010
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1995TS01      J.Phys.(London) G21, 33 (1995)

K.Tsushima, S.W.Huang, A.Faessler

Resonance Model of πΔ → YK for Kaon Production in Heavy-Ion Collisions

doi: 10.1088/0954-3899/21/1/005
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1995YA13      Phys.Lett. 354B, 24 (1995)

Y.Yan, S.W.Huang, A.Faessler

A Microscopic Quark Model of πN → KΣ Reactions for Heavy-Ion Collisions

NUCLEAR REACTIONS 1n, 1H(π+, X), (π-, X), E=high; calculated K+Σ+, K+Σ-, K+Σ0, K0(lambda) production σ(E). Microscopic quark model.

doi: 10.1016/0370-2693(95)00634-W
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1994BA19      J.Phys.(London) G20, 461 (1994)

G.Batko, A.Faessler, S.W.Huang, E.Lehmann, R.K.Puri

Does the Reduction of the Mass in the Medium Enhance the Production of Antiprotons in High-Energy Nuclear Reactions ( Question )

NUCLEAR REACTIONS Ni(Ni, X), E=1.93 GeV/nucleon; Cu(C, X), E=3.65 GeV/nucleon; calculated antiproton invariant spectra, σ(θ); deduced medium effects role in anti-proton production.

doi: 10.1088/0954-3899/20/3/007
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1994PU03      Nucl.Phys. A575, 733 (1994)

R.K.Puri, N.Ohtsuka, E.Lehmann, A.Faessler, M.A.Matin, D.T.Khoa, G.Batko, S.W.Huang

Temperature-Dependent Mean Field and Its Effect on Heavy-Ion Reactions

NUCLEAR REACTIONS 40Ca(40Ca, X), 93Nb(93Nb, X), E=400 MeV/nucleon; calculated maximum, average densities, transverse flow time evolution. Temperature dependent mean field nucleon potentials.

doi: 10.1016/0375-9474(94)90164-3
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1994PU05      J.Phys.(London) G20, 1817 (1994)

R.K.Puri, E.Lehmann, A.Faessler, S.W.Huang

Study of Non-Equilibrium Effects and Thermal Properties of Heavy-Ion Collisions using a Covariant Approach

NUCLEAR REACTIONS 40Ca(40Ca, X), 28Si(28Si, X), 20Ne(20Ne, X), 16O(16O, X), 12C(12C, X), E=0.5, 1.5 GeV/nucleon; calculated anisotropy ratio, average temperature, matter density time evolution. Full Lorentz-invariant formalism, nonequilibrium effects.

doi: 10.1088/0954-3899/20/11/010
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1994TS02      Phys.Lett. 337B, 245 (1994)

K.Tsushima, S.W.Huang, A.Faessler

The Role of the Δ(1920) Resonance for Kaon Production in Heavy Ion Collisions

NUCLEAR REACTIONS 1n, 1H(π+, X), (π-, X), (π0, X), E=high; calculated σ(E) for (ΣK) production; deduced Δ(1920) resonance role.

doi: 10.1016/0370-2693(94)90971-7
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1992KH02      Nucl.Phys. A542, 671 (1992)

D.T.Khoa, N.Ohtsuka, A.Faessler, M.A.Matin, S.W.Huang, E.Lehmann, Y.Lofty

Microscopic Study of Thermal Properties of the Nuclear Matter Formed in Heavy-Ion Collisions

NUCLEAR REACTIONS 20Ne(20Ne, X), 40Ca(40Ca, X), 93Nb(93Nb, X), E=100-400 MeV/nucleon; calculated central region nucleon density, temperature, local entropy per nucleon vs evolution time. Generalized hot Thomas-Fermi formalism.

doi: 10.1016/0375-9474(92)90263-J
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1992KH03      Nucl.Phys. A548, 102 (1992)

D.T.Khoa, N.Ohtsuka, M.A.Matin, A.Faessler, S.W.Huang, E.Lehmann, R.K.Puri

In-Medium Effects in the Description of Heavy-Ion Collisions with Realistic NN Interactions

NUCLEAR REACTIONS 40Ca(40Ca, X), 93Nb(93Nb, X), E=400 MeV/nucleon; calculated temperature, nuclear matter density time evolution. Quantum molecular dynamical approach, phenomenological Skyrme forces, Brueckner G-matrix potential.

doi: 10.1016/0375-9474(92)90079-Y
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1992LI03      J.Phys.(London) G18, 291 (1992)

G.Li, Y.Lotfy, S.W.Huang, A.Faessler

Self-Consistent Quantum Molecular Dynamics Description of Photon Production in Nucleus-Nucleus Reactions

NUCLEAR REACTIONS 40Ca(40Ca, X), E=84, 200 MeV/nucleon; Tb(p, X), E=168 MeV; calculated γ-production σ(θ) vs Eγ. Self-consistent quantum molecular dynamics approach.

doi: 10.1088/0954-3899/18/2/011
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1991KH05      Nucl.Phys. A529, 363 (1991)

D.T.Khoa, N.Ohtsuka, S.W.Huang, M.Ismail, A.Faessler, M.El-Shabshiry, J.Aichelin

Photon Production in Heavy-Ion Collisions and Nuclear Equation of State

NUCLEAR REACTIONS 12C(12C, X), 40Ca(40Ca, X), 93Nb(93Nb, X), E=84, 200 MeV/nucleon; calculated γ production σ. Quantum molecular dynamics model.

doi: 10.1016/0375-9474(91)90799-C
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1991LI33      Nucl.Phys. A534, 697 (1991)

G.Li, D.T.Khoa, T.Maruyama, S.W.Huang, N.Ohtsuka, A.Faessler, J.Aichelin

Subthreshold Pion Production in Nucleus-Nucleus Collisions within the Quantum Molecular Dynamics Approach

NUCLEAR REACTIONS 12C(12C, X), Ca(Ca, X), 93Nb(93Nb, X), E=200 MeV/nucleon; 20Ne(20Ne, X), E=183 MeV/nucleon; 64Cu(20Ne, X), E=250 MeV/nucleon; calculated pion production σ(θ, E(π)). Quantum molecular dynamics model.

doi: 10.1016/0375-9474(91)90467-K
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