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NSR database version of April 11, 2024.

Search: Author = G.Q.Zhang

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2023QI06      Phys.Rev. C 108, 014325 (2023)

L.-J.Qi, D.-M.Zhang, S.Luo, G.-Q.Zhang, P.-C.Chu, X.-J.Wu, X.-H.Li

Cluster radioactivity preformation probability of trans-lead nuclei in the NpNn scheme

RADIOACTIVITY 221Fr, 221,222,223,224,226Ra, 223Ac(14C);228Th(20O);231Pa(23F);230Th, 231Pa, 232,233,234U(24Ne);233U(25Ne);234U(26Ne);234U, 236,238Pu(28Mg), 238Pu(30Mg);238Pu(32Si);242Cm(34Si); calculated cluster preformation probability. Comparison of results obtained with unified fission model (model dependent approach), cluster formation model (microscopic approach) and Wei model (analytical formula).

doi: 10.1103/PhysRevC.108.014325
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2022ZH52      Phys.Rev. C 106, 034604 (2022)

Z.Zhu, J.Xu, G.-Q.Zhang

Simulating fusion reactions from Coulomb explosions within a transport approach

NUCLEAR REACTIONS 2H(d, 3He), E=2-10 keV; calculated fusion σ(E), reaction rate at different temperatures, time evolution of the Coulomb explosion of deuterium clusters induced by high intensity laser beams, neutron production rate in Coulomb explosion. EPOCH model framework - typical particle-in-cell (PIC) transport approach, to simulate the Coulomb explosion of clusters with electrons completely stripped by laser beams, modified to incorporate fusion reactions by introducing nuclear inelastic scattering channels.

doi: 10.1103/PhysRevC.106.034604
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2019CA04      Phys.Rev. C 99, 014606 (2019)

X.G.Cao, E.J.Kim, K.Schmidt, K.Hagel, M.Barbui, J.Gauthier, S.Wuenschel, G.Giuliani, M.R.D.Rodriguez, S.Kowalski, H.Zheng, M.Huang, A.Bonasera, R.Wada, N.Blando, G.Q.Zhang, C.Y.Wong, A.Staszczak, Z.X.Ren, Y.K.Wang, S.Q.Zhang, J.Meng, J.B.Natowitz

Examination of evidence for resonances at high excitation energy in the 7 α disassembly of 28Si

NUCLEAR REACTIONS 12C(28Si, X), (28Si, 7α), E=35 MeV/nucleon; measured Eα, Iα, excitation functions for the α-conjugate exit channels using the 4π NIMROD-ISiS array for charged particle detection at the K500 superconducting cyclotron facility of Texas A and M. 28Si; deduced resonances at high excitation energies, shapes of 7α events in the de-excitation of projectile-like nuclei; calculated energies, J, π, configurations, quadrupole deformation of toroidal high-spin isomers using covariant functional PC-PK1 and DD-ME2.

doi: 10.1103/PhysRevC.99.014606
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2019WA24      Int.J.Mod.Phys. E28, 1950039 (2019)

K.Wang, A.Bonasera, H.Zheng, G.Q.Zhang, Y.G.Ma, W.Q.Shen

The role of the Heisenberg principle in constrained molecular dynamics model

NUCLEAR REACTIONS 12C(p, p), E<250 MeV; 197Au(197Au, X), E=35 MeV/nucleon; 238U(238U, X), E=15 MeV/nucleon; analyzed available data; calculated σ(θ), charge density distributions.

doi: 10.1142/S0218301319500393
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2019ZH22      Chin.Phys.C 43, 064102 (2019)

S.Zhang, J.C.Wang, A.Bonasera, M.R.Huang, H.Zheng, G.Q.Zhang, Z.Kohley, Y.G.Ma, S.J.Yennello

Triple α-particle resonances in the decay of hot nuclear systems

NUCLEAR REACTIONS 70Zn(70Zn, X), 64Zn(64Zn, X)12C, E=35 MeV/nucleon; analyzed available data. 8Be; deduced 3α systems, relative energies, Efimov states.

doi: 10.1088/1674-1137/43/6/064102
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2017LI28      Nucl.Instrum.Methods Phys.Res. B410, 158 (2017)

L.X.Liu, H.W.Wang, Y.G.Ma, X.G.Cao, X.Z.Cai, J.G.Chen, G.L.Zhang, J.L.Han, G.Q.Zhang, J.F.Hu, X.H.Wang, W.J.Li, Z.Yan, H.J.Fu

Measurements of the total cross section of natBe with thermal neutrons from a photo-neutron source

NUCLEAR REACTIONS 9Be(n, X), E=0.007-0.1 eV; measured reaction products, En, In, time-of-flight; deduced σ. Comparison with available data.

doi: 10.1016/j.nimb.2017.08.022
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32767.


2017LV01      Phys.Rev. C 95, 024614 (2017)

M.Lv, Y.G.Ma, J.H.Chen, D.Q.Fang, G.Q.Zhang

Medium effect on the nuclear modification factor of protons and pions in intermediate-energy heavy ion collisions

doi: 10.1103/PhysRevC.95.024614
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2017WA05      Phys.Rev. C 95, 014608 (2017)

K.Wang, Y.G.Ma, G.Q.Zhang, X.G.Cao, W.B.He, W.Q.Shen

Giant dipole resonance in proton capture reactions using an extended quantum molecular dynamics model

NUCLEAR REACTIONS 11B(p, γ)12C, E=30-60 MeV; 27Al(p, γ)28Si, E=30-90 MeV; 39K(p, γ)40Ca, E=25-80 MeV; , 67Co(p, γ)68Ni, E=20-90 MeV; calculated GDR γ spectra, GDR parameters such as peak energies, strengths, and FWHM, dipole moments and temperature of the proton-capture systems as functions of incident energies, GDR width as a function of temperature. Extended quantum molecular dynamics (EQMD) model for giant dipole resonance in proton capture reactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.95.014608
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2016FA10      Phys.Rev. C 94, 044621 (2016)

D.Q.Fang, Y.G.Ma, X.Y.Sun, P.Zhou, Y.Togano, N.Aoi, H.Baba, X.Z.Cai, X.G.Cao, J.G.Chen, Y.Fu, W.Guo, Y.Hara, T.Honda, Z.G.Hu, K.Ieki, Y.Ishibashi, Y.Ito, N.Iwasa, S.Kanno, T.Kawabata, H.Kimura, Y.Kondo, K.Kurita, M.Kurokawa, T.Moriguchi, H.Murakami, H.Ooishi, K.Okada, S.Ota, A.Ozawa, H.Sakurai, S.Shimoura, R.Shioda, E.Takeshita, S.Takeuchi, W.D.Tian, H.W.Wang, J.S.Wang, M.Wang, K.Yamada, Y.Yamada, Y.Yasuda, K.Yoneda, G.Q.Zhang, T.Motobayashi

Proton-proton correlations in distinguishing the two-proton emission mechanism of 23Al and 22Mg

NUCLEAR REACTIONS 12C(23Al, 2pX), (23Al, 2p21Na), (23Al, 2p20Ne), E=57.4 MeV/nucleon; 12C(22Mg, 2pX), (22Mg, 2p20Ne), E=53.5 MeV/nucleon, [secondary 22Mg and 23Al beams from 12C(28Si, X), E=135 MeV/nucleon primary reaction]; measured fragments and protons using ΔE-E detectors at RIBF-RIKEN facility; deduced proton-proton momentum correlation function for decays into p+p+X, p+p+20Na, and p+p+21Na channels, effective source sizes from calculations using the CRAB code with a Gaussian source, mechanism of two-proton emission.

doi: 10.1103/PhysRevC.94.044621
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2016HE07      Phys.Rev. C 94, 014301 (2016)

W.B.He, Y.G.Ma, X.G.Cao, X.Z.Cai, G.Q.Zhang

Dipole oscillation modes in light α-clustering nuclei

NUCLEAR STRUCTURE 8Be, 12C, 16O; calculated centroid energies and spectra of giant dipole resonances (GDR), average binding energy for different α cluster structures, Gaussian wave packets in different clustering states: 8Be as two-α cluster structure, 12C as triangle and chain structures, and 16O as chain, kite and square structures. Extended quantum molecular dynamics (EQMD) model. Comparison with experimental data.

doi: 10.1103/PhysRevC.94.014301
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2016XU03      Phys.Rev. C 93, 044609 (2016)

J.Xu, L.-W.Chen, M.Y.B.Tsang, H.Wolter, Y.-X.Zhang, J.Aichelin, M.Colonna, D.Cozma, P.Danielewicz, Z.-Q.Feng, A.Le Fevre, T.Gaitanos, C.Hartnack, K.Kim, Y.Kim, C.-M.Ko, B.-A.Li, Q.-F.Li, Z.-X.Li, P.Napolitani, A.Ono, M.Papa, T.Song, J.Su, J.-L.Tian, N.Wang, Y.-J.Wang, J.Weil, W.-J.Xie, F.-S.Zhang, G.-Q.Zhang

Understanding transport simulations of heavy-ion collisions at 100A and 400A MeV: Comparison of heavy-ion transport codes under controlled conditions

doi: 10.1103/PhysRevC.93.044609
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2015DA04      Phys.Rev. C 91, 034618 (2015)

Z.T.Dai, D.Q.Fang, Y.G.Ma, X.G.Cao, G.Q.Zhang, W.Q.Shen

Effect of neutron skin thickness on projectile fragmentation

NUCLEAR REACTIONS 12C(50Ca, X), (48Ca, X), E=50 MeV/nucleon; calculated neutron and proton density profiles, yields of heavy fragments; analyzed isoscaling by taking the ratio of fragment yields between 50Ca and 48Ca induced reactions. Isospin dependent quantum molecular dynamics (IQMD) model simulation using GEMINI code. Comparison with experimental data.

doi: 10.1103/PhysRevC.91.034618
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2015LI10      Phys.Rev. C 91, 044302 (2015)

Y.D.Liu, H.W.Wang, Y.G.Ma, X.G.Cao, G.Q.Zhang, D.Q.Fang, M.Lyu, W.B.He, Z.T.Dai, C.Li, C.L.Zhou, S.Q.Ye, C.Tao, J.Wang, S.Kumar, J.L.Han, Y.Y.Yang, P.Ma, J.B.Ma, S.L.Jin, Z.Bai, L.Jin, D.Yan, J.S.Wang

New measurement of the excited states in 11B via elastic resonance scattering of 10Be +p

NUCLEAR REACTIONS 1H(10Be, p), E=7.2 MeV/nucleon, [secondary 10Be beam produced in 9Be(16O, X), E=59.62 MeV/nucleon primary reaction]; measured particle spectra using TOF method, angular distribution of scattered particles using ΔE-E telescope, Ep, Ip at HIRFL-Lanzhou facility. 11B; deduced levels, resonances, J, π, l-value, Γp, widths of Wigner limit. R-matrix analysis of proton spectra from elastic resonance scattering. Comparison with previous experimental results, and with evaluated data.

doi: 10.1103/PhysRevC.91.044302
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0194. Data from this article have been entered in the XUNDL database. For more information, click here.


2015MA19      Phys.Lett. B 743, 306 (2015)

Y.G.Ma, D.Q.Fang, X.Y.Sun, P.Zhou, Y.Togano, N.Aoi, H.Baba, X.Z.Cai, X.G.Cao, J.G.Chen, Y.Fu, W.Guo, Y.Hara, T.Honda, Z.G.Hu, K.Ieki, Y.Ishibashi, Y.Ito, N.Iwasa, S.Kanno, T.Kawabata, H.Kimura, Y.Kondo, K.Kurita, M.Kurokawa, T.Moriguchi, H.Murakami, H.Ooishi, K.Okada, S.Ota, A.Ozawa, H.Sakurai, S.Shimoura, R.Shioda, E.Takeshita, S.Takeuchi, W.D.Tian, H.W.Wang, J.S.Wang, M.Wang, K.Yamada, Y.Yamada, Y.Yasuda, K.Yoneda, G.Q.Zhang, T.Motobayashi

Different mechanism of two-proton emission from proton-rich nuclei 23Al and 22Mg

RADIOACTIVITY 23Al, 22Mg(2p) [from 9Be(28Si, X), E=135 MeV/nucleon]; measured decay products, Ep, Ip; deduced two-proton relative momentum and opening angle from the decay. Comparison with available data.

doi: 10.1016/j.physletb.2015.02.066
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Data from this article have been entered in the XUNDL database. For more information, click here.


2014DA04      Phys.Rev. C 89, 014613 (2014)

Z.T.Dai, D.Q.Fang, Y.G.Ma, X.G.Cao, G.Q.Zhang

Triton/3He ratio as an observable for neutron-skin thickness

NUCLEAR REACTIONS 12C(68Ni, X), (50Ca, X), E=50 MeV/nucleon; calculated yields of triton and 3He; analyzed relation between the ratio of t/3He and neutron skin thickness in 50Ca and 68Ni. Isospin-dependent quantum molecular dynamics (IQMD) model.

doi: 10.1103/PhysRevC.89.014613
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2014HE13      Phys.Rev.Lett. 113, 032506 (2014)

W.B.He, Y.G.Ma, X.Z.Cai, G.Q.Zhang

Giant Dipole Resonance as a Fingerprint of α Clustering Configurations in 12C and 16O

NUCLEAR STRUCTURE 12C, 16O; calculated giant dipole resonance spectra, σ(E); deduced α configurations impact on collective motion. Microscopic dynamical framework.

doi: 10.1103/PhysRevLett.113.032506
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2014WA49      Phys.Rev. C 90, 054601 (2014)

J.Wang, Y.G.Ma, G.Q.Zhang, W.Q.Shen

Effect of initial fluctuations on the collective flow in intermediate-energy heavy ion collisions

doi: 10.1103/PhysRevC.90.054601
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2014ZH42      Phys.Rev. C 90, 057601 (2014)

C.L.Zhou, Y.G.Ma, D.Q.Fang, G.Q.Zhang, J.Xu, X.G.Cao, W.Q.She

Correlation between elliptic flow and shear viscosity in intermediate-energy heavy-ion collisions

doi: 10.1103/PhysRevC.90.057601
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2013PU01      Phys.Rev. C 87, 047603 (2013)

J.Pu, J.H.Chen, S.Kumar, Y.G.Ma, C.W.Ma, G.Q.Zhang

Influence of the symmetry energy on isospin ratios from projectile and target fragmentations in intermediate-energy heavy-ion collisions

NUCLEAR REACTIONS 58,64Ni(40Ca, X), (48Ca, X), E=50, 600 MeV/nucleon; calculated single and double ratios of neutrons to protons as a function of kinetic energy, sensitivity factor of the symmetry energy. Isospin-dependent quantum molecular dynamics (IQMD) model.

doi: 10.1103/PhysRevC.87.047603
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2013TA03      Phys.Rev. C 87, 014621 (2013)

C.Tao, Y.G.Ma, G.Q.Zhang, X.G.Cao, D.Q.Fang, H.W.Wang

Pygmy and giant dipole resonances by Coulomb excitation using a quantum molecular dynamics model

NUCLEAR REACTIONS 197Au(62Ni, 62Ni'), (64Ni, 64Ni'), (66Ni, 66Ni'), (68Ni, 68Ni'), (70Ni, 70Ni'), (72Ni, 72Ni'), (74Ni, 74Ni'), (76Ni, 76Ni'), (78Ni, 78Ni'), E=100-600 MeV; calculated time evolution of binding energies and rms radii, time evolution of dipole moment of pygmy and giant dipole resonance (PDR and GDR), PDR gamma spectrum, EOS and incident energy dependencies of GDR and PDR, EWSR, gamma width and strength, mass number dependence of PDR and GDR. Isospin-dependent quantum molecular dynamics model (IQMD). Comparison with experimental data, and with other model calculations.

doi: 10.1103/PhysRevC.87.014621
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2013TA36      Phys.Rev. C 88, 064615 (2013)

C.Tao, Y.G.Ma, G.Q.Zhang, X.G.Cao, D.Q.Fang, H.W.Wang, J.Xu

Isoscalar giant monopole resonance in Sn isotopes using a quantum molecular dynamics model

NUCLEAR REACTIONS 112,116,120,124Sn(α, α'), E=100-500 MeV; calculated spectra of giant monopole resonances (GMR); analyzed peak energy, FWHM, and strength of isoscalar giant monopole resonances (GMR). 56Ni, 90Zr, 208Pb; analyzed data for GMR; deduced isospin dependence in isotope chains in addition to the mass-number dependence for C, O, Ca, Ni, Zr, Sn, Au and Pb in A=12-210 region. Isospin-dependent quantum molecular dynamics (IQMD) model.

doi: 10.1103/PhysRevC.88.064615
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2013ZH31      Phys.Rev. C 88, 024604 (2013)

C.L.Zhou, Y.G.Ma, D.Q.Fang, G.Q.Zhang

Thermodynamic properties and shear viscosity over entropy-density ratio of the nuclear fireball in a quantum-molecular dynamics model

doi: 10.1103/PhysRevC.88.024604
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2012CA35      Phys.Rev. C 86, 044620 (2012)

X.G.Cao, X.Z.Cai, Y.G.Ma, D.Q.Fang, G.Q.Zhang, W.Guo, J.G.Chen, J.S.Wang

Nucleon-nucleon momentum-correlation function as a probe of the density distribution of valence neutrons in neutron-rich nuclei

NUCLEAR STRUCTURE 15C; calculated rms radii, proton, neutron, valence neutron, and total density distribution using RMF theory.

NUCLEAR REACTIONS 12C(12C, X), (13C, X), (14C, X), (15C, X), (16C, X), E=800 MeV/nucleon; calculated proton-neutron, neutron-neutron, and proton-proton momentum-correlation functions, root mean square of the coordinate and momentum space distributions. Relativistic mean-field (RMF) model, isospin-dependent quantum-molecular-dynamics (IDQMD) model. Comparison with experimental data.

doi: 10.1103/PhysRevC.86.044620
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2012KU09      Phys.Rev. C 85, 024620 (2012)

S.Kumar, Y.G.Ma, G.Q.Zhang, C.L.Zhou

Sensitivity of neutron to proton ratio toward the high density behavior of the symmetry energy in heavy-ion collisions

NUCLEAR REACTIONS 132Sn(132Sn, X), E=50-600 MeV/nucleon; calculated time evolution of average density, free nucleons, light charged particles (LCP) and intermediate mass fragments (IMF) at semicentral geometry, n/p ratios, power law. 112Sn(112Sn, X), 124Sn(124Sn, X), 132Sn(132Sn, X), E=50-600 MeV/nucleon; calculated excitation function of single and double neutron to proton ratio for free nucleons and light-charged particles (LCP), isospin asymmetry dependence of double neutron-to-proton ratio. Isospin quantum molecular dynamics (IQMD) model.

doi: 10.1103/PhysRevC.85.024620
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2012KU30      Phys.Rev. C 86, 044616 (2012)

S.Kumar, Y.G.Ma, G.Q.Zhang

Correlation and isospin dynamics of participant-spectator matter in neutron-rich colliding nuclei at 50 MeV/nucleon

NUCLEAR REACTIONS 112Sn(112SN, X), 124Sn(124SN, X), E=50 MeV/nucleon; calculated kinetic energy spectra, and fragment multiplicities. Isospin quantum molecular dynamical model.

doi: 10.1103/PhysRevC.86.044616
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2011KU18      Phys.Rev. C 84, 044620 (2011)

S.Kumar, Y.G.Ma, G.Q.Zhang, C.L.Zhou

Probing the density dependence of the symmetry energy via multifragmentation at subsaturation densities

NUCLEAR REACTIONS 112Sn(112Sn, X), 124Sn(124Sn, X), 132Sn(132Sn, X), E=50 MeV/nucleon; calculated kinetic energy spectra of nucleons and other fragments, proton-neutron ratios. Isospin-dependent quantum molecular dynamics model. Comparison with experimental data.

doi: 10.1103/PhysRevC.84.044620
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2011SU12      Chin.Phys.C 35, 555 (2011)

X.-Y.Sun, D.-Q.Fang, Y.-G.Ma, X.-Z.Cai, J.-G.Chen, W.Guo, W.-D.Tian, H.-W.Wang, G.-Q.Zhang, P.Zhou

A new probe of neutron skin thickness

NUCLEAR REACTIONS 12C(50Ca, X), (52Ca, X), (54Ca, X), (56Ca, X), (60Ni, X), (62Ni, X), (64Ni, X), (66Ni, X), (68Ni, X), (70Ni, X), E = 50 MeV/nucleon; calculated neutron skin thickness vs. impact parameter. Isospin-Dependent Quantum Molecular Dynamics (IQMD) model.

doi: 10.1088/1674-1137/35/6/009
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2011ZH21      Phys.Rev. C 83, 064607 (2011)

G.Q.Zhang, Y.G.Ma, X.G.Cao, C.L.Zhou

Mach-like emission from nucleon scattering in proton-nucleus reactions

NUCLEAR REACTIONS 208Pb(p, X), E=1 GeV; calculated yield of nucleons at different times, evolution of the kinetic-energy distribution of nucleons with time, correlation between the momentum and polar angular distribution of nucleons, excitation function of the sideward angular peak value of nucleons. Quantum molecular dynamics model.

doi: 10.1103/PhysRevC.83.064607
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2011ZH32      Phys.Rev. C 84, 034612 (2011)

G.Q.Zhang, Y.G.Ma, X.G.Cao, C.L.Zhou, X.Z.Cai, D.Q.Fang, W.D.Tian, H.W.Wang

Unified description of nuclear stopping in central heavy-ion collisions from 10A MeV to 1.2A GeV

NUCLEAR REACTIONS 129Xe(120Sn, X), E=10-1200 MeV/nucleon; analyzed wide-range excitation function of nuclear stopping data from INDRA and FOPI using isospin-dependent quantum molecular dynamics model (IQMD) transport model.

doi: 10.1103/PhysRevC.84.034612
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2010CA18      Phys.Rev. C 81, 061603 (2010)

X.G.Cao, G.Q.Zhang, X.Z.Cai, Y.G.Ma, W.Guo, J.G.Chen, W.D.Tian, D.Q.Fang, H.W.Wang

Roles of deformation and orientation in heavy-ion collisions induced by light deformed nuclei at intermediate energy

NUCLEAR REACTIONS 24Mg(24Mg, X), E=200, 380 MeV; calculated maximal density distributions, fragment multiplicity, excitation functions, charge distributions using isospin-dependent quantum molecular dynamics model (IDQMD).

doi: 10.1103/PhysRevC.81.061603
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2010SU16      Int.J.Mod.Phys. E19, 1823 (2010)

X.Y.Sun, J.G.Chen, D.Q.Fang, Y.G.Ma, X.Z.Cai, W.Guo, W.D.Tian, H.W.Wang, P.Zhou, G.Q.Zhang, X.G.Cao, Y.Fu, Z.G.Hu, J.S.Wang, M.Wang, Y.Togano, N.Aoi, H.Baba, T.Honda, K.Okada, Y.Hara, K.Ieki, Y.Ishibashi, Y.Itou, N.Iwasa, S.Kanno, T.Kawabata, H.Kimura, Y.Kondo, K.Kurita, M.Kurokawa, T.Moriguchi, H.Murakami, H.Oishi, S.Ota, A.Ozawa, H.Sakurai, S.Shimoura, R.Shioda, E.Takeshita, S.Takeuchi, K.Yamada, Y.Yamada, Y.Yasuda, K.Yoneda, T.Motobayashi

Measurement of the proton-proton correlation function from the break-up of 22Mg and 20Ne

NUCLEAR REACTIONS 12C(22Mg, p), (20Ne, p), E=70 MeV/nucleon; measured reaction products, proton spectrum; deduced angular and momentum correlations between two protons, space-time information.

doi: 10.1142/S0218301310016259
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2010ZH15      Int.J.Mod.Phys. E19, 957 (2010)

P.Zhou, D.Q.Fang, Y.G.Ma, X.Z.Cai, J.G.Chen, W.Guo, X.Y.Sun, W.D.Tian, H.W.Wang, G.Q.Zhang, X.G.Cao, Y.Fu, Z.G.Hu, J.S.Wang, M.Wang, Y.Togano, N.Aoi, H.Baba, T.Honda, K.Okada, Y.Hara, K.Ieki, Y.Ishibashi, Y.Itou, N.Iwasa, S.Kanno, T.Kawabata, H.Kimura, Y.Kondo, K.Kurita, M.Kurokawa, T.Moriguchi, H.Murakami, H.Oishi, S.Ota, A.Ozawa, H.Sakurai, S.Shimoura, R.Shioda, E.Takeshita, S.Takeuchi, K.Yamada, Y.Yamada, Y.Yasuda, K.Yoneda, T.Motobayashi

Measurement of two-proton correlation from the break-up of 23Al

RADIOACTIVITY 23Al, 22Mg(2p) [from 12C(23Al, X), (22Mg, X), (21Na, X), (20Ne, X), E=60-70 MeV/nucleon]; measured decay products; deduced trajectories, di-proton emission.

doi: 10.1142/S0218301310015400
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