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NSR database version of April 11, 2024.

Search: Author = D.Q.Fang

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2024DI03      Phys.Rev. C 109, 024616 (2024)

M.-Q.Ding, D.-Q.Fang, Y.-G.Ma

Effects of neutron-skin thickness on light-particle production

doi: 10.1103/PhysRevC.109.024616
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2023DI08      Chin.Phys.C 47, 094101 (2023)

M.-Q.Ding, P.Su, D.-Q.Fang, S.-M.Wang

Investigation of the relationship between mirror proton radii and neutron-skin thickness

NUCLEAR STRUCTURE 18O, 18,19,21,22Ne, 19F, 21,23Na, 22,23Mg, 34,35,37,38Ar, 34,36S, 35,37Cl, 36,37,38Ca, 54Fe, 54Ni; analyzed available data; deduced that neutron-skin thickness of a neutron-rich nucleus is proportional to the difference between the proton radii of mirror nuclei using the axially deformed solutions of the Skyrme-Hartree-Fock-Bogoliubov equations with 132 sets of Skyrme interaction parameters.

doi: 10.1088/1674-1137/ace680
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2023WA21      Phys.Rev. C 108, 014609 (2023)

S.S.Wang, Y.G.Ma, W.B.He, D.Q.Fang, X.G.Cao

Influences of α-clustering configurations on the giant dipole resonance in hot compound systems

NUCLEAR REACTIONS 12C(16O, γ)28Si, E=125 MeV;27Al(20Ne, γ)47V, E=160 MeV;12C(20Ne, γ), E=145 MeV; calculated giant dipole resonance (GDR) spectra in hot nucleus, effects of projectile polarization on the GDR spectra. Investigated the sensitivity of GDR lineshape to the α-clustering configurations of projectile, including the linear chain, kite, square, and tetrahedron configurations. Calculations in the framework of an extended quantum molecular dynamics (EQMD) model. Comparison to experimental data.

doi: 10.1103/PhysRevC.108.014609
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2023YA28      Phys.Rev. C 108, 044307 (2023)

Y.H.Yang, Y.G.Ma, S.M.Wang, B.Zhou, D.Q.Fang

Structure and decay mechanism of the low-lying states in 9Be and 9B

doi: 10.1103/PhysRevC.108.044307
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2022WA07      Phys.Rev. C 105, 024620 (2022)

T.T.Wang, Y.G.Ma, D.Q.Fang, H.L.Liu

Temperature and density effects on the two-nucleon momentum correlation function from excited single nuclei

NUCLEAR STRUCTURE A=36, 52, 80, 96, 100, 112, 129; 36P, 129Xe; calculated proton-proton and neutron-neutron momentum correlation functions, gaussian source radius at different source temperatures and densities. Thermal isospin-dependent quantum molecular dynamics (ThIQMD) model.

doi: 10.1103/PhysRevC.105.024620
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2022WA09      Phys.Rev. C 105, 034616 (2022)

S.S.Wang, Y.G.Ma, D.Q.Fang, X.G.Cao

Effects of neutron-skin thickness on direct hard photon emission from reactions induced by the neutron-rich projectile 50Ca

NUCLEAR REACTIONS 12C, 40Ca(50Ca, γX), E=40-150 MeV/nucleon; calculated yield of direct hard photons from central and peripheral collisions, multiplicity of direct hard photons. Studied the effects of neutron skin thickness on direct hard photon emissions. Isospin-dependent quantum molecular dynamics model (IDQMD).

doi: 10.1103/PhysRevC.105.034616
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2020NU01      J.Low Temp.Physics 199, 519 (2020)

I.Nutini, D.Q.Adams, C.Alduino, K.Alfonso, F.T.Avignone, O.Azzolini, G.Bari, F.Bellini, G.Benato, M.Biassoni, A.Branca, C.Brofferio, C.Bucci, A.Caminata, A.Campani, L.Canonica, X.G.Cao, S.Capelli, L.Cappelli, L.Cardani, P.Carniti, N.Casali, D.Chiesa, N.Chott, M.Clemenza, S.Copello, C.Cosmelli, O.Cremonesi, R.J.Creswick, A.D'Addabbo, D.D'Aguanno, I.Dafinei, C.J.Davis, S.Dell'Oro, S.Di Domizio, V.Dompe, D.Q.Fang, G.Fantini, M.Faverzani, E.Ferri, F.Ferroni, E.Fiorini, M.A.Franceschi, S.J.Freedman, B.K.Fujikawa, A.Giachero, L.Gironi, A.Giuliani, P.Gorla, C.Gotti, T.D.Gutierrez, K.Han, K.M.Heeger, R.G.Huang, H.Z.Huang, J.Johnston, G.Keppel, Yu.G.Kolomensky, C.Ligi, Y.G.Ma, L.Ma, L.Marini, R.H.Maruyama, Y.Mei, N.Moggi, S.Morganti, T.Napolitano, M.Nastasi, J.Nikkel, C.Nones, E.B.Norman, V.Novati, A.Nucciotti, T.O'Donnell, J.L.Ouellet, C.E.Pagliarone, L.Pagnanini, M.Pallavicini, L.Pattavina, M.Pavan, G.Pessina, V.Pettinacci, C.Pira, S.Pirro, S.Pozzi, E.Previtali, A.Puiu, C.Rosenfeld, C.Rusconi, M.Sakai, S.Sangiorgio, B.Schmidt, N.D.Scielzo, V.Singh, M.Sisti, D.Speller, L.Taffarello, F.Terranova, C.Tomei, M.Vignati, S.L.Wagaarachchi, B.S.Wang, B.Welliver, J.Wilson, K.Wilson, L.A.Winslow, L.Zanotti, S.Zimmermann, S.Zucchelli

The CUORE Detector and Results

RADIOACTIVITY 130Te(2β-); measured decay products, Eβ, Iβ; deduced two-neutron T1/2 and neutrinoless mode limit. The cryogenic underground observatory for rare events (CUORE).

doi: 10.1007/s10909-020-02402-9
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2020SH15      Phys.Rev. C 102, 014601 (2020)

C.Z.Shi, Y.G.Ma, X.G.Cao, D.Q.Fang, W.B.He, C.Zhong

Direct photon emission and influence of dynamical wave packets in an extended quantum molecular dynamics model

NUCLEAR REACTIONS 12C(14N, X), E=20, 30, 40 MeV/nucleon; C, Zn(α, X), E=53 MeV/nucleon; calculated hard photon production rate, photon energy spectra, angular distributions of photons, double differential σ(Eγ, θ) of direct photon emission from first proton-neutron collision, proton and neutron momentum distributions, invariant photon cross section versus rapidity and transverse energy. Extended quantum molecular dynamics (EQMD) model with embedded hard photon production channel. Comparison with predictions of unmodified extended quantum molecular dynamics model.

doi: 10.1103/PhysRevC.102.014601
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2020WA25      Phys.Rev. C 102, 024620 (2020)

S.S.Wang, Y.G.Ma, X.G.Cao, D.Q.Fang, C.W.Ma

Hard-photon production and its correlation with intermediate-mass fragments in a framework of a quantum molecular dynamics model

NUCLEAR REACTIONS 40Ca(40Ca, X), E=60 MeV/nucleon; calculated differential σ from inclusive events with and without Pauli blocking for hard photons, separation time between direct photons and thermal photons as a function of impact parameter, production probabilities of photons and IMFs and multiplicity correlation as function of time, hard-photon (Eγ=20-130 MeV) energy spectra, temperatures as a function of incident energy. 40Ca(40Ca, X), E=40-120 MeV/nucleon; calculated multiplicities of direct and thermal photons, multiplicity of intermediate-mass fragments (IMFs), and multiplicity correlations between the direct photons or thermal photons and the IMFs as function of incident energy and centrality. 12C(14N, X), E=20, 30, 40 MeV/nucleon; calculated high-energy photon spectra and compared with experimental data. Isospin-dependent quantum molecular dynamics (IQMD) model by embedding incoherent neutron-proton bremsstrahlung photon production channel to investigate high-energy photon production and correlation with fragments.

doi: 10.1103/PhysRevC.102.024620
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2020WA30      Eur.Phys.J. A 56, 254 (2020)

S.S.Wang, Y.G.Ma, X.G.Cao, D.Q.Fang, C.W.Ma

Azimuthal anisotropy and multiplicities of hard photons and free nucleons in intermediate-energy heavy-ion collisions

NUCLEAR REACTIONS 40Ca(40Ca, X), E=60 MeV/nucleon; analyzed available data; calculated average density, hard photon production probability, directed flows, scale-invariant momentum vs scale-invariant rapidity using a framework of isospin-dependent quantum molecular dynamics (IQMD) model.

doi: 10.1140/epja/s10050-020-00264-z
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2019LI24      Phys.Rev. C 99, 054614 (2019)

H.L.Liu, Y.G.Ma, D.Q.Fang

Finite-size scaling phenomenon of nuclear liquid-gas phase transition probes

NUCLEAR STRUCTURE 36P, 52Cr, 80As, 100Rh, 112Sn, 129Xe; calculated total multiplicity, total multiplicity derivative, intermediate mass fragment (IMF), second moment parameter (M2) as a function of temperature of 0-20 MeV for the excited nuclear systems, mass dependence of the phase transition temperatures; deduced finite-size scaling effects on nuclear liquid-gas phase transition probes. Single thermal source version of the isospin-dependent quantum molecular dynamics (ThIQMD) model.

doi: 10.1103/PhysRevC.99.054614
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2018WA05      Int.J.Mod.Phys. E27, 1850014 (2018)

K.Wang, D.Q.Fang, Y.T.Wang, X.X.Xu, L.J.Sun, Z.Bai, M.R.Huang, S.L.Jin, C.Li, H.Li, J.Li, X.F.Li, C.J.Lin, J.B.Ma, P.Ma, W.H.Ma, M.W.Nie, C.Z.Shi, H.W.Wang, J.G.Wang, J.S.Wang, L.Yang, Y.Y.Yang, H.Q.Zhang, Y.J.Zhou, Y.G.Ma, W.Q.Shen

Spectroscopic study of β-delayed particle emission from proton-rich nucleus 23Si

RADIOACTIVITY 23Si(β+), (β+p), (β+2p) [from 9Be(28Si, X)23Si, E=75.8 MeV/nucleon]; measured decay products, Eγ, Iγ, Ep, Ip, p-γ and 2p-γ-coin.; deduced β-delayed charge-particle energy spectrum, decay energies and branching ratios for β-delayed protons, γ-ray energies, J, π, β-delayed proton branch and two proton emissions. Comparison with available data.

doi: 10.1142/S0218301318500143
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2018WA20      Eur.Phys.J. A 54, 107 (2018)

Y.-T.Wang, D.-Q.Fang, K.Wang, X.-X.Xu, L.-J.Sun, Z.Bai, P.-F.Bao, X.-G.Cao, Z.-T.Dai, B.Ding, W.-B.He, M.-R.Huang, S.-L.Jin, Y.Li, C.-J.Lin, L.-X.Liu, M.Lv, J.-B.Ma, P.Ma, H.-W.Wang, J.-G.Wang, J.-S.Wang, S.-T.Wang, Y.-Y.Yang, S.-Q.Ye, H.-Q.Zhang, M.-H.Zhao, C.-L.Zhou, Y.-G.Ma, W.-Q.Shen

β-delayed particle emission from 21Mg

RADIOACTIVITY 21Mg(EC), (β+), (ECp), (ECα), (β+p), (β+α); measured Eg, Ig, E(particle), I(particle), pγ-coin, charged particles using RIBBL1 (Radioactive Ion Beam Line) at Lanzhou, 21Mg decay-time spectrum, γ-ray energy spectrum correlated with β-delayed charged particles; deduced β-delayed charged particles energy spectrum, new partial decay scheme, levels, J, π, T1/2, log ft, branching ratios of individual states.

doi: 10.1140/epja/i2018-12543-1
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2018WA24      Phys.Lett. B 784, 12 (2018)

Y.T.Wang, D.Q.Fang, K.Wang, X.X.Xu, L.J.Sun, P.F.Bao, Z.Bai, X.G.Cao, Z.T.Dai, B.Ding, W.B.He, M.R.Huang, S.L.Jin, C.J.Lin, M.Lv, L.X.Liu, Y.Li, P.Ma, J.B.Ma, J.S.Wang, S.T.Wang, J.G.Wang, H.W.Wang, S.Q.Ye, Y.Y.Yang, C.L.Zhou, M.H.Zhao, H.Q.Zhang, Y.G.Ma, W.Q.Shen

Observation of β-delayed 2He emission from the proton-rich nucleus 22Al

RADIOACTIVITY 22Al(β+2p) [from Be(28Si, X), E=76 MeV/nucleon]; measured decay products, Eγ, Iγ. 22Mg; deduced the momentum and emission angle of the two protons, Ep, Ip. Comparison with Monte Carlo simulations.

doi: 10.1016/j.physletb.2018.07.034
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2017GU14      Phys.Rev. C 95, 054622 (2017)

C.Q.Guo, Y.G.Ma, W.B.He, X.G.Cao, D.Q.Fang, X.G.Deng, C.L.Zhou

Isovector dipole resonance and shear viscosity in low energy heavy-ion collisions

NUCLEAR REACTIONS 100Mo(40Ca, X), E=5, 7.5, 10, 12.5, 15 MeV/nucleon; calculated time evolution of nuclear matter density and kinetic-energy density, temperature, chemical potential, and the entropy density of the compound nucleus, post equilibration time evolution of the stress tensor, ratio of shear viscosity over entropy density as function of temperature, giant dipole moment in coordinate space, isovector giant dipole resonance (IVGDR) photon spectra and centroid energies. Green-Kubo method in the framework of an extended quantum molecular dynamics model (EQMD).

doi: 10.1103/PhysRevC.95.054622
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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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2017SU05      Phys.Rev. C 95, 014314 (2017)

L.J.Sun, X.X.Xu, D.Q.Fang, C.J.Lin, J.S.Wang, Z.H.Li, Y.T.Wang, J.Li, L.Yang, N.R.Ma, K.Wang, H.L.Zang, H.W.Wang, C.Li, C.Z.Shi, M.W.Nie, X.F.Li, H.Li, J.B.Ma, P.Ma, S.L.Jin, M.R.Huang, Z.Bai, J.G.Wang, F.Yang, H.M.Jia, H.Q.Zhang, Z.H.Liu, P.F.Bao, D.X.Wang, Y.Y.Yang, Y.J.Zhou, W.H.Ma, J.Chen, Y.G.Ma, Y.H.Zhang, X.H.Zhou, H.S.Xu, G.Q.Xiao, W.L.Zhan

β-decay study of the Tz = -2 proton-rich nucleus 20Mg

RADIOACTIVITY 20Mg(β+), (β+p)[from 9Be(28Si, X), E=75.8 MeV/nucleon at RIBLL-HIRFL-Lanzhou facility]; measured reaction products, Ep, Ip, Eγ, Iγ, γγ-, γβ- and pβ-coin, (20Mg)γ-coin, half-life of 20Mg decay. 20Na, 19Ne; deduced levels, branching ratios, logft values. Comparison with previous experimental results, and with β transitions in 20O mirror nucleus.

doi: 10.1103/PhysRevC.95.014314
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2017XU01      Phys.Lett. B 766, 312 (2017)

X.X.Xu, C.J.Lin, L.J.Sun, J.S.Wang, Y.H.Lam, J.Lee, D.Q.Fang, Z.H.Li, N.A.Smirnova, C.X.Yuan, L.Yang, Y.T.Wang, J.Li, N.R.Ma, K.Wang, H.L.Zang, H.W.Wang, C.Li, M.L.Liu, J.G.Wang, C.Z.Shi, M.W.Nie, X.F.Li, H.Li, J.B.Ma, P.Ma, S.L.Jin, M.R.Huang, Z.Bai, F.Yang, H.M.Jia, Z.H.Liu, D.X.Wang, Y.Y.Yang, Y.J.Zhou, W.H.Ma, J.Chen, Z.G.Hu, M.Wang, Y.H.Zhang, X.W.Ma, X.H.Zhou, Y.G.Ma, H.S.Xu, G.Q.Xiao, H.Q.Zhang

Observation of β-delayed two-proton emission in the decay of 22Si

RADIOACTIVITY 22Si(β+2p) [from 9Be(28Si, X), E=75.8 MeV/nucleon]; measured decay products, Ep, Ip; deduced Q-value, ground-state mass, two-proton separation energy. Comparison with large-scale shell-model calculations.

doi: 10.1016/j.physletb.2017.01.028
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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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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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2015SU15      Nucl.Instrum.Methods Phys.Res. A804, 1 (2015)

L.J.Sun, X.X.Xu, C.J.Lin, J.S.Wang, D.Q.Fang, Z.H.Li, Y.T.Wang, J.Li, L.Yang, N.R.Ma, K.Wang, H.L.Zang, H.W.Wang, C.Li, C.Z.Shi, M.W.Nie, X.F.Li, H.Li, J.B.Ma, P.Ma, S.L.Jin, M.R.Huang, Z.Bai, J.G.Wang, F.Yang, H.M.Jia, H.Q.Zhang, Z.H.Liu, P.F.Bao, D.X.Wang, Y.Y.Yang, Y.J.Zhou, W.H.Ma, J.Chen

A detection system for charged-particle decay studies with a continuous-implantation method

doi: 10.1016/j.nima.2015.09.039
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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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2014FA07      Phys.Rev. C 89, 047601 (2014)

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

Shear viscosity of hot nuclear matter by the mean free path method

doi: 10.1103/PhysRevC.89.047601
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2014OZ02      Phys.Rev. C 89, 044602 (2014)

A.Ozawa, T.Moriguchi, T.Ohtsubo, N.Aoi, D.Q.Fang, N.Fukuda, M.Fukuda, H.Geissel, I.Hachiuma, N.Inabe, Y.Ishibashi, S.Ishimoto, Y.Ito, T.Izumikawa, D.Kameda, T.Kubo, T.Kuboki, K.Kusaka, M.Lantz, Y.G.Ma, M.Mihara, Y.Miyashita, S.Momota, D.Nagae, K.Namihira, D.Nishimura, H.Ooishi, Y.Ohkuma, T.Ohnishi, M.Ohtake, K.Ogawa, Y.Shimbara, T.Suda, T.Sumikama, H.Suzuki, S.Suzuki, T.Suzuki, M.Takechi, H.Takeda, K.Tanaka, R.Watanabe, M.Winkler, T.Yamaguchi, Y.Yanagisawa, Y.Yasuda, K.Yoshinaga, A.Yoshida, K.Yoshida

Charge-changing cross sections of 30Ne, 32, 33Na with a proton target

NUCLEAR REACTIONS 1H(30Ne, X), (32Na, X), (33Na, X), [secondary 30Ne, 32,33Na beams from 9Be(48Ca, X)30Ne/31Ne/31Na/32Na/33Na, E=345 MeV/nucleon primary reaction], E≈240 MeV/nucleon; measured particle spectra, charge-changing, partial charge-changing and charge-pickup σ using Big-RIPS and ZDS spectrometers at RIBF-RIKEN facility; deduced rms proton and matter radii, neutron skin thickness. 30Ne, 32Na; deduced neutron skin thickness, rms proton radii. Glauber-model analysis. Comparison with previous experimental results.

doi: 10.1103/PhysRevC.89.044602
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2455.


2014TA32      Phys.Rev. C 90, 061305 (2014)

M.Takechi, S.Suzuki, D.Nishimura, M.Fukuda, T.Ohtsubo, M.Nagashima, T.Suzuki, T.Yamaguchi, A.Ozawa, T.Moriguchi, H.Ohishi, T.Sumikama, H.Geissel, N.Aoi, R.-J.Chen, D.-Q.Fang, N.Fukuda, S.Fukuoka, H.Furuki, N.Inabe, Y.Ishibashi, T.Itoh, T.Izumikawa, D.Kameda, T.Kubo, M.Lantz, C.S.Lee, Y.-G.Ma, K.Matsuta, M.Mihara, S.Momota, D.Nagae, R.Nishikiori, T.Niwa, T.Ohnishi, K.Okumura, M.Ohtake, T.Ogura, H.Sakurai, K.Sato, Y.Shimbara, H.Suzuki, H.Takeda, S.Takeuchi, K.Tanaka, M.Tanaka, H.Uenishi, M.Winkler, Y.Yanagisawa, S.Watanabe, K.Minomo, S.Tagami, M.Shimada, M.Kimura, T.Matsumoto, Y.R.Shimizu, M.Yahiro

Evidence of halo structure in 37Mg observed via reaction cross sections and intruder orbitals beyond the island of inversion

NUCLEAR REACTIONS 12C(24Mg, X), (25Mg, X), (26Mg, X), (27Mg, X), (28Mg, X), (29Mg, X), (30Mg, X), (31Mg, X), (32Mg, X), (33Mg, X), (34Mg, X), (35Mg, X), (36Mg, X), (37Mg, X), (38Mg, X), E=240 MeV/nucleon, [secondary Mg beams from 9Be(48Ca, X), E=345 MeV/nucleon primary reaction]; measured spectra and TOF of outgoing particles, precise reaction σ using BigRIPS spectrometer at RIBF-RIKEN facility. Comparison with theoretical deformation parameter β2 versus mass plot using double-folding model (DFM) calculation combined with antisymmetrized molecular dynamics (AMD) calculation. 37Mg; deduced deformed halo effect from observed enhanced cross section, comparison with DFM calculation based on the deformed Woods-Saxon (DWS) model; collapse of N=28 magic shell for neutrons.

doi: 10.1103/PhysRevC.90.061305
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2471.


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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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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2012MA05      Phys.Rev. C 85, 024618 (2012)

Y.G.Ma, G.H.Liu, X.Z.Cai, D.Q.Fang, W.Guo, W.Q.Shen, W.D.Tian, H.W.Wang

Hard-photon flow and photon-photon correlation in intermediate-energy heavy-ion collisions

NUCLEAR REACTIONS 40Ca(40Ca, X), E=30, 60 MeV/nucleon; calculated time evolution of hard-photon production rate, kinetic energy spectrum and slope parameter of direct and thermal photons, time evolution of elliptic and directed flow of hard photons, average in-plane transverse momentum, azimuthal distribution, directed transverse flow parameter of hard photons and free protons, time evolution of production rate of bremsstrahlung photons, and multiplicity of hard photons, two-photon correlation functions. 40Ca(40Ca, X), E=25-90 MeV/nucleon; calculated excitation function of elliptic flow parameter. 86Kr(58Ni, X), E=60 MeV/nucleon; calculated two-photon correlation functions. Boltzmann-Uehling-Ulenbeck model. Comparison with Experimental data.

doi: 10.1103/PhysRevC.85.024618
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2012TA02      Phys.Lett. B 707, 357 (2012)

M.Takechi, T.Ohtsubo, M.Fukuda, D.Nishimura, T.Kuboki, T.Suzuki, T.Yamaguchi, A.Ozawa, T.Moriguchi, H.Ooishi, D.Nagae, H.Suzuki, S.Suzuki, T.Izumikawa, T.Sumikama, M.Ishihara, H.Geissel, N.Aoi, R.-J.Chen, D.-Q.Fang, N.Fukuda, I.Hachiuma, N.Inabe, Y.Ishibashi, Y.Ito, D.Kameda, T.Kubo, K.Kusaka, M.Lantz, Y.-G.Ma, K.Matsuta, M.Mihara, Y.Miyashita, S.Momota, K.Namihira, M.Nagashima, Y.Ohkuma, T.Ohnishi, M.Ohtake, K.Ogawa, H.Sakurai, Y.Shimbara, T.Suda, H.Takeda, S.Takeuchi, K.Tanaka, R.Watanabe, M.Winkler, Y.Yanagisawa, Y.Yasuda, K.Yoshinaga, A.Yoshida, K.Yoshida

Interaction cross sections for Ne isotopes towards the island of inversion and halo structures of 29Ne and 31Ne

NUCLEAR REACTIONS Be(48Ca, X)29Ne/31Ne, E=345 MeV/nucleon; C(29Ne, X), (31Ne, X), E=260 MeV/nucleon; measured reaction products; deduced σ, Nilsson orbitals, halo structures. Comparison with Glauber-type calculations.

doi: 10.1016/j.physletb.2011.12.028
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2368.


2011FA09      Chin.Phys.Lett. 28, 102102 (2011)

D.-Q.Fang, Y.-G.Ma, X.-Z.Cai, W.-D.Tian, H.-W.Wang

Effects of Neutron Skin Thickness in Peripheral Nuclear Reactions

NUCLEAR REACTIONS 12C(48Ca, n), (48Ca, p), E not given; calculated σ, σ ratios for nuclei with different neutron skin thickness. Statistical Abrasion Ablation (SAA) model.

doi: 10.1088/0256-307X/28/10/102102
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2011FU11      Phys.Rev. C 84, 037603 (2011)

Y.Fu, D.Q.Fang, Y.G.Ma, X.Z.Cai, W.D.Tian, H.W.Wang, W.Guo, G.H.Liu, C.W.Ma, R.R.Fan, F.Fu, H.Gao, Q.Gao, W.T.Guo, J.L.Han, Z.G.Hu, T.H.Huang, F.Jia, B.Li, X.G.Lei, Z.Y.Sun, M.Wang, J.S.Wang, Z.G.Xiao, Z.G.Xu, X.W.Yao, H.B.Zhang, X.H.Zhang, C.Zheng, H.S.Xu, G.Q.Xiao, W.L.Zhan

Measurement of the longitudinal momentum distribution of 30S after one-proton removal from 31Cl

NUCLEAR REACTIONS 12C(31Cl, 30S), E=44 MeV/nucleon; measured particle, spectra, TOF at RIBLL facility. 30S; deduced longitudinal fragment momentum distribution. 31Cl; calculated proton density distributions; deduced configuration of valence proton Few-body Glauber model analysis.

doi: 10.1103/PhysRevC.84.037603
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Data from this article have been entered in the XUNDL database. For more information, click here.


2011LI36      Phys.Rev. C 84, 024607 (2011)

S.X.Li, D.Q.Fang, Y.G.Ma, C.L.Zhou

Shear viscosity to entropy density ratio in the Boltzmann-Uehling-Uhlenbeck model

doi: 10.1103/PhysRevC.84.024607
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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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2011ZH20      Chin.Phys.Lett. 28, 062101 (2011)

P.Zhou, W.-D.Tian, Y.-G.Ma, X.-Z.Cai, D.-Q.Fang, H.-W.Wang

The influence of Multi-Step Sequential Decay on Isoscaling and Fragment Isospin Distribution in GEMINI Simulation

doi: 10.1088/0256-307X/28/6/062101
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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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2011ZH33      Phys.Rev. C 84, 037605 (2011)

P.Zhou, W.D.Tian, Y.G.Ma, X.Z.Cai, D.Q.Fang, H.W.Wang

Influence of statistical sequential decay on isoscaling and symmetry energy coefficient in a GEMINI simulation

doi: 10.1103/PhysRevC.84.037605
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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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2010FA05      Phys.Rev. C 81, 047603 (2010)

D.Q.Fang, Y.G.Ma, X.Z.Cai, W.D.Tian, H.W.Wang

Neutron removal cross section as a measure of neutron skin

NUCLEAR REACTIONS 12C(23Na, X), (25Na, X), (27Na, X), (29Na, X), (31Na, X), (33Na, X), (31P, X), (33P, X), (35P, X), (37P, X), (39P, X), (41P, X), (42Ca, X), (44Ca, X), (46Ca, X), (48Ca, X), (50Ca, X), (52Ca, X), (58Ni, X), (60Ni, X), (62Ni, X), (64Ni, X), (66Ni, X), (68Ni, X), E=1 GeV/nucleon; calculated neutron removal σ using statistical abrasion ablation (SAA) model.

doi: 10.1103/PhysRevC.81.047603
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2010FU09      Nucl.Phys. A834, 584c (2010)

Y.Fu, D.Q.Fang, Y.G.Ma, X.Z.Cai, X.Y.Sun, W.D.Tian

Isoscaling in projectile fragmentation reaction induced by 40, 48Ca and 58, 64Ni

NUCLEAR REACTIONS 9Be(40Ca, X), (48Ca, X), (58Ni, X), (64Ni, X), E=140 MeV/nucleon; calculated fragment yields using HIPSE (Heavy-Ion Phase Space Exploration) model; deduced isoscaling behaviour.

doi: 10.1016/j.nuclphysa.2010.01.098
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2010SU07      Phys.Lett. B 682, 396 (2010)

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

Neutron/proton ratio of nucleon emissions as a probe of neutron skin

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/proton yield ratio and dependence on neutron skin thickness using isospin-dependent quantum molecular model.

doi: 10.1016/j.physletb.2009.11.031
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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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2010SU19      Nucl.Phys. A834, 502c (2010)

X.Y.Sun, D.Q.Fang, Y.G.Ma, X.Z.Cai, X.G.Cao, Y.Fu, W.D.Tian

Dependence of n/p with neutron skin thickness for neutron-rich nuclei

NUCLEAR REACTIONS 12C(50Ca, n), (50Ca, p), (52Ca, n), (52Ca, p), (54Ca, n), (54Ca, p), (56Ca, n), (56Ca, p), (60Ni, n), (60Ni, p), (62Ni, n), (62Ni, p), (64Ni, n), (64Ni, p), (66Ni, n), (66Ni, p), (68Ni, n), (68Ni, p), (70Ni, n), (70Ni, p), E=50 MeV/nucleon; calculated neutron-, proton-yields dependence on neutron skin, reduced impact and diffuseness parameters, rapidity using isospin-dependent quantum molecular dynamics model.

doi: 10.1016/j.nuclphysa.2010.01.077
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2010TI03      Int.J.Mod.Phys. E19, 1076 (2010)

W.D.Tian, H.W.Wang, Y.G.Ma, G.H.Liu, C.W.Ma, Q.M.Su, T.Z.Yan, Y.Shi, X.Z.Cai, D.Q.Fang, J.G.Chen, W.Guo, K.Wang, H.S.Xu, Z.G.Hu, Z.G.Xiao, Z.Y.Sun, Z.Y.Guo, G.Q.Xiao, X.G.Lei, B.Li, X.H.Yuan, H.B.Zhang, X.W.Yao, W.T.Guo, X.H.Zhang, Q.Gao, C.Zheng, H.Gao, Z.G.Xu, F.Fu, J.L.Han, R.R.Fan

Projectile fragmentation of 36, 40Ar induced reactions

NUCLEAR REACTIONS 64Ni(36Ar, X), (40Ar, X), E=50 MeV/nucleon; measured reaction products; deduced fragment yields, σ(θ), isoscaling parameters. Comparison with empirical models.

doi: 10.1142/S0218301310015515
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2010TI05      Int.J.Mod.Phys. E19, 1815 (2010)

W.D.Tian, Y.G.Ma, H.W.Wang, G.H.Liu, C.W.Ma, Q.M.Su, T.Z.Yan, X.Z.Cai, D.Q.Fang, J.G.Chen, W.Guo, Y.Shi, K.Wang, H.S.Xu, Z.G.Hu, Z.G.Xiao, Z.Y.Sun, Z.Y.Guo, G.Q.Xiao, X.G.Lei, B.Li, X.H.Yuan, H.B.Zhang, X.W.Yao, W.T.Guo, X.H.Zhang, Q.Gao, C.Zheng, H.Gao, Z.G.Xu, F.Fu, J.L.Han, R.R.Fan

Projectile fragmentation of 36-40Ar induced reactions

NUCLEAR REACTIONS 64Ni(36Ar, X), (40Ar, X), E=50 MeV/nucleon; measured reaction products; deduced fragment yields, σ. Comparison with EPAX and SAA models.

doi: 10.1142/S0218301310016247
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0182.


2010WU02      Phys.Rev. C 81, 047602 (2010)

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

Dynamical dipole γ radiation in heavy-ion collisions on the basis of a quantum molecular dynamics model

NUCLEAR REACTIONS 48Ca(40Ca, X), E=10, 15, 20 MeV/nucleon; 116Sn(16O, X), E=15.6 MeV/nucleon; calculated γ-ray yields, giant dipole moment, dipole dynamical emission spectra, maximum γ-emission probability, and symmetry energy coefficients using isospin-dependent quantum molecular dynamics (IDQMD) model for GDR. Comparison with experimental data.

doi: 10.1103/PhysRevC.81.047602
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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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2009CA35      Chin.Phys.C 33, Supplement 1, 49 (2009)

X.-G.Cao, J.-G.Chen, Y.-G.Ma, D.-Q.Fang, W.-D.Tian, T.-Z.Yan, X.-Z.Cai

Density effect of the neutron halo nucleus induced reactions in intermediate energy heavy ion collisions

NUCLEAR REACTIONS 12C(15C, X), E=30, 60, 90, 120 MeV/nucleon; 15C; calculated fragmentation multiplicities, spectrum of emitted neutrons. Isospin-dependent quantum molecular dynamics (IQMD) model.

doi: 10.1088/1674-1137/33/S1/016
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2009FA12      Chin.Phys.C 33, 197 (2009)

D.-Q.Fang, Y.Fu, X.-Y.Sun, X.-Z.Cai, W.Guo, W.-D.Tian, H.-W.Wang, Y.-G.Ma

Scaling property in one-nucleon removal reactions induced by exotic nuclei

NUCLEAR REACTIONS 12C(19C, X), E=70 MeV/nucleon; calculated reaction fragment parallel momentum distributions; deduced scaling properties, halo nuclei identification.

doi: 10.1088/1674-1137/33/3/007
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2009FU06      Chin.Phys.Lett. 26, 082503 (2009)

Y.Fu, D.-Q.Fang, Y.-G.Ma, X.-Z.Cai, W.-D.Tian, H.-W.Wang, W.Guo

Isoscaling Behavior in 48, 40Ca+9Be Collisions at Intermediate Energy Investigated by the HIPSE Model

NUCLEAR REACTIONS 9Be(48Ca, X), (40Ca, X), E=140 MeV/nucleon; calculated fragment production σ, isoscaling parameters α and β; deduced impact of excitation energy and evaporation on isoscaling behavior. Heavy-ion phase space exploration (HIPSE) model.

doi: 10.1088/0256-307X/26/8/082503
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2009FU19      Chin.Phys.C 33, Supplement 1, 126 (2009)

Y.Fu, D.-Q.Fang, Y.-G.Ma, X.-Z.Cai, W.Guo, C.-W.Ma, W.-D.Tian, H.-W.Wang, K.Wang

Isoscaling behavior studied by HIPSE model

NUCLEAR REACTIONS 9Be(58Ni, X), (64Ni, X), E=140 MeV/nucleon; calculated isotopic distribution, yield ratios; deduced HIPSE parameters dependence of isoscaling parameters. Heavy-ion phase-space exploration (HIPSE) model.

doi: 10.1088/1674-1137/33/S1/040
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2009LI63      Chin.Phys.C 33, Supplement 1, 89 (2009)

G.-H.Liu, Y.-G.Ma, X.-Z.Cai, D.-Q.Fang, W.-Q.Shen, W.-D.Tian, K.Wang

Impact parameter and beam energy dependence for azimuthal asymmetry of direct photons and free protons in intermediate energy heavy-ion collisions

doi: 10.1088/1674-1137/33/S1/029
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2009MA13      Phys.Rev. C 79, 034606 (2009)

C.-W.Ma, H.-L.Wei, J.-Y.Wang, G.-J.Liu, D.-Q.Fang, W.-D.Tian, X.-Z.Cai, H.-W.Wang, Y.-G.Ma

Isospin dependence of projectile-like fragment production at intermediate energies

NUCLEAR REACTIONS 9Be(40Ca, X), (48Ca, X), (58Ni, X), (64Ni, X), E=140 MeV/nucleon; calculated σ. Discussed isospin dependence of projectile fragmentation, shapes of fragment isotopic and isotonic distributions of different asymmetric projectiles. Statistical abration-ablation model. Comparison with experimental data.

doi: 10.1103/PhysRevC.79.034606
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2009WA30      Chin.Phys.C 33, Supplement 1, 119 (2009)

K.Wang, Y.-G.Ma, Q.-S.Zheng, X.-Z.Cai, D.-Q.Fang, Y.Fu, G.-Ch.Lu, W.-D.Tian

Temperature dependent fission fragment distribution in the Langevin equation

NUCLEAR REACTIONS 209Bi(α, X), (20Ne, X), E=40-240 MeV; 232Th(11B, X), (19F, X), (20Ne, X), E=40-240 MeV; 238U(16O, X), (18O, X), E=40-240 MeV; 181Ta(20Ne, X), E=40-240 MeV; 197Au(18O, X), E=40-240 MeV;calculated σ, fission time, mass distribution. Combined dynamical and statistical model (CDSM).

doi: 10.1088/1674-1137/33/S1/038
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2008CH34      Int.J.Mod.Phys. E17, Supplement 1, 50 (2008)

J.G.Chen, X.Z.Cai, Y.Shi, Y.G.Ma, Z.Z.Ren, D.Q.Fang, W.Guo, H.W.Wang, W.D.Tian, W.Q.Shen

Nuclear halo and its scaling laws in the excited states of nuclei near the β-stability line

NUCLEAR STRUCTURE 13,15N, 13C, 15O, 21Na; calculated binding energies, radii, excited states; deduced proton halo and proton skin. Nonlinear RMF model.

doi: 10.1142/S0218301308011756
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2008MA13      Chinese Physics B 17, 1216 (2008)

C.-W.Ma, Y.Fu, D.-Q.Fang, Y.-G.Ma, X.-Z.Cai, W.Guo, W.-D.Tian, H.-W.Wang

A possible experimental observable for the determination of neutron skin thickness

doi: 10.1088/1674-1056/17/4/011
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2008MA47      Int.J.Mod.Phys. E17, 1669 (2008)

C.W.Ma, Y.Fu, D.Q.Fang, Y.G.Ma, X.Z.Cai, W.D.Tian, K.Wang, C.Zhong

Isospin effect and isoscaling phenomenon in projectile fragmentation

doi: 10.1142/S0218301308010684
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2008OZ01      Phys.Rev. C 78, 054313 (2008)

A.Ozawa, D.Q.Fang, M.Fukuda, N.Iwasa, T.Izumikawa, H.Jeppesen, R.Kanungo, R.Koyama, T.Ohnishi, T.Ohtsubo, W.Shinozaki, T.Suda, T.Suzuki, M.Takahashi, I.Tanihata, C.Wu, Y.Yamaguchi

Measurement of the reaction cross section of 18C and observations of fragments from 17C and 18C at 80A MeV

NUCLEAR REACTIONS C(17C, n), (17C, 2n), (18C, n), (18C, 2n), E=80 MeV/nucleon; measured momentum distributions, σ. Comparison with Glauber model calculations.

doi: 10.1103/PhysRevC.78.054313
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2008TI10      Int.J.Mod.Phys. E17, 1705 (2008)

W.D.Tian, Y.G.Ma, X.Z.Cai, D.Q.Fang, W.Guo, C.W.Ma, G.H.Liu, W.Q.Shen, Y.Shi, H.W.Wang, K.Wang, T.Z.Yan

Dynamical and sequential decay effects on isoscaling and density dependence of the symmetry energy

doi: 10.1142/S0218301308010714
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2007FA14      J.Phys.(London) G34, 2173 (2007)

D.Q.Fang, Y.G.Ma, C.Zhong, C.W.Ma, X.Z.Cai, J.G.Chen, W.Guo, Q.M.Su, W.D.Tian, K.Wang, T.Z.Yan, W.Q.Shen

Systematic study of isoscaling behavior in projectile fragmentation by the statistical abrasion-ablation model

NUCLEAR REACTIONS 27Al(86Kr, X), E=44 MeV/nucleon; 27Al(129Xe, X), E=790 MeV/nucleon; 112Sn(112Sn, X), (124Sn, X), E=60 MeV/nucleon; calculated calculated fragment yields and isotopic distributions using a modified statistical abrasion-ablation model. Compared results to available data.

doi: 10.1088/0954-3899/34/10/007
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2007FA16      Phys.Rev. C 76, 031601 (2007)

D.Q.Fang, W.Guo, C.W.Ma, K.Wang, T.Z.Yan, Y.G.Ma, X.Z.Cai, W.Q.Shen, Z.Z.Ren, Z.Y.Sun, J.G.Chen, W.D.Tian, C.Zhong, M.Hosoi, T.Izumikawa, R.Kanungo, S.Nakajima, T.Ohnishi, T.Ohtsubo, A.Ozawa, T.Suda, K.Sugawara, T.Suzuki, A.Takisawa, K.Tanaka, T.Yamaguchi, I.Tanihata

Examining the exotic structure of the proton-rich nucleus 23Al

NUCLEAR REACTIONS 12C(23Al, p), E=74 MeV/nucleon; measured fragment longitudinal momentum distributions. 12C(23Al, X), (24Al, X), (24Al, X), E=74 MeV/nucleon; measured reaction cross sections. Compared results to model calculations.

doi: 10.1103/PhysRevC.76.031601
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2007MA53      Nucl.Phys. A790, 299c (2007)

Y.G.Ma, X.Z.Cai, J.G.Chen, D.Q.Fang, W.Guo, G.H.Liu, C.W.Ma, E.J.Ma, W.Q.Shen, Y.Shi, Q.M.Su, W.D.Tian, H.W.Wang, K.Wang, Y.B.Wei, T.Z.Yan

Nucleon-nucleon momentum correlation function for light nuclei

NUCLEAR STRUCTURE 11Li; calculated binding energies, neutron-neutron correlation functions. 6,7,8,9,11Li, 13,14,15,16,17,18,19C, 14,15,16,17N; calculated binding energies, proton-neutron correlation functions. 27,28,29,30S; calculated binding energies, proton-proton correlation functions. Isospin-dependent quantum molecular dynamics.

doi: 10.1016/j.nuclphysa.2007.03.146
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2007MA56      Nucl.Phys. A787, 611c (2007)

Y.G.Ma, T.Z.Yan, X.Z.Cai, J.G.Chen, D.Q.Fang, W.Guo, G.H.Liu, C.W.Ma, E.J.Ma, W.Q.Shen, Y.Shi, Q.M.Su, W.D.Tian, H.W.Wang, K.Wang

Scaling of anisotropy flows in intermediate energy heavy ion collisions

NUCLEAR REACTIONS 40Ca(40Ca, X), 58Ni, 124Sn(86Kr, X), E=25 MeV/nucleon; calculated directed flow vs rapidity, elliptic flow and 4th momentum anisotropy vs transverse momentum. Quantum molecular dynamics model. Nucleonic coalescence and reaction mechanism features discussed.

doi: 10.1016/j.nuclphysa.2006.12.091
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2007TI01      Chin.Phys.Lett. 24, 385 (2007)

W.-D.Tian, Yu.-G.Ma, X.-Z.Cai, D.-Q.Fang, W.Guo, C.-W.Ma, G.-H.Liu, W.-Q.Shen, Yu.Shi, Q.-M.Su, H.-W.Wang, K.Wang, T.-Z.Yan

Isoscaling in Statistical Sequential Decay Model

NUCLEAR STRUCTURE 150,168Re; calculated isotope yield ratios, isoscaling parameters from decay of excited nuclides. Sequential decay model.

doi: 10.1088/0256-307X/24/2/023
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2007TI08      Phys.Rev. C 76, 024607 (2007)

W.D.Tian, Y.G.Ma, X.Z.Cai, D.Q.Fang, W.Guo, W.Q.Shen, K.Wang, H.W.Wang, M.Veselsky

Isospin effect in statistical sequential decay

doi: 10.1103/PhysRevC.76.024607
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2007YA16      Chin.Phys.Lett. 24, 3388 (2007)

T.-Z.Yan, Y.-G.Ma, X.-Z.Cai, D.-Q.Fang, G.-C.Lu, W.-Q.Shen, W.-D.Tian, H.-W.Wang, K.Wang

Phenomenological Scaling of Rapidity Dependence for Anisotropic Flows in 25 MeV/nucleon Ca+Ca by Quantum Molecular Dynamics Model

NUCLEAR REACTIONS 40Ca(40Ca, X), E=25 MeV/nucleon; calculated anisotropic flows of light fragments up to A=4, transverse momentum per nucleon as a function of the normalized rapidity, phenomenological scaling model.

doi: 10.1088/0256-307X/24/12/028
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2006GU28      Int.J.Mod.Phys. E15, 1523 (2006)

W.Guo, D.Q.Fang, Y.G.Ma, C.W.Ma, K.Wang, T.Z.Yan, X.Z.Cai, W.Q.Shen, Z.Y.Sun, Z.Z.Ren, J.G.Chen, J.H.Chen, G.H.Liu, E.J.Ma, G.L.Ma, Y.Shi, Q.M.Su, W.D.Tian, H.W.Wang, C.Zhong, J.X.Zuo, M.Hosoi, T.Izumikawa, R.Kanungo, S.Nakajima, T.Ohnishi, T.Ohtsubo, A.Ozawa, T.Suda, K.Sugawara, T.Suzuki, A.Takisawa, K.Tanaka, T.Yamaguchi, I.Tanihata

Measurements of reaction cross section and fragment momentum distribution for N=10 proton-rich isotones

NUCLEAR REACTIONS 12C(23Al, 22MgX), (24Al, 23MgX), (22Mg, 21NaX), (21Na, 20NeX), E not given; measured fragment parallel momentum distribution following one-proton removal. 12C(23Al, X), (24Al, X), E not given; measured reaction σ.

doi: 10.1142/S0218301306005101
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2006MA05      Phys.Rev. C 73, 014604 (2006)

Y.G.Ma, Y.B.Wei, W.Q.Shen, X.Z.Cai, J.G.Chen, J.H.Chen, D.Q.Fang, W.Guo, C.W.Ma, G.L.Ma, Q.M.Su, W.D.Tian, K.Wang, T.Z.Yan, C.Zhong, J.X.Zuo

Surveying the nucleon-nucleon momentum correlation function in the framework of quantum molecular dynamics model

NUCLEAR REACTIONS 12C(13C, X), (14C, X), (15C, X), (16C, X), (17C, X), (18C, X), (19C, X), E=800 MeV/nucleon; 12C(18C, X), E=100 MeV/nucleon; calculated two-nucleon momentum correlation functions. Isospin-dependent quantum molecular dynamics model.

doi: 10.1103/PhysRevC.73.014604
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2006MA62      Chin.Phys.Lett. 23, 2695 (2006)

E.-J.Ma, Yu.-G.Ma, J.-G.Chen, X.-Z.Cai, D.-Q.Fang, W.Guo, G.-H.Liu, C.-W.Ma, W.-Q.Shen, Yu.Shi, Q.-M.Su, W.-D.Tian, H.W.Wang, K.Wang, T.-Z.Yan

Cross Sections of Elastic Electron and Positron Scattering from Proton-Rich Nuclei

NUCLEAR REACTIONS 12C, 208Pb(e, e), (e+, e+), E=450 MeV; 12C, 16O(e, e), (e+, e+), E=374.5, 750 MeV; 28,32S(e, e), (e+, e+), E=250, 500 MeV; calculated σ(θ). Relativistic partial-wave expansion method, comparison with data.

doi: 10.1088/0256-307X/23/10/020
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2006MA96      High Energy Phys. and Nucl.Phys. (China), Supplement 2, 30, 186 (2006)

C.-W.Ma, D.-Q.Fang, W.Guo, K.Wang, T.-Z.Yan, Y.-G.Ma, X.-Z.Cai, W.-Q.Shen, Z.-Y.Sun, Z.-Z.Ren, J.-G.Chen, W.-D.Tian, H.-W.Wang, E.-J.Ma, G.-H.Liu, Y.Shi, Q.-M.Su, C.Zhong, M.Hosoi, T.Izumikawa, R.Kanungo, S.Nakajima, T.Ohnishi, T.Ohtsubo, T.Suda, K.Sugawara, T.Suzuki, A.Ozawa, A.Takisawa, K.Tanaka, T.Yamaguchi, I.Tanihata

Study of Exoticness of Proton-Rich Nuclei 23Al and it's Neighboring Nuclei


2006OZ02      Nucl.Instrum.Methods Phys.Res. B247, 155 (2006)

A.Ozawa, Y.Z.Cai, Z.Q.Chen, M.Chiba, D.Q.Fang, Z.G.Guo, T.Izumikawa, J.X.Li, R.S.Mao, T.Ohnishi, W.Q.Shen, T.Suda, Z.Y.Sun, T.Suzuki, I.Tanihata, W.D.Tian, J.S.Wang, M.Wang, Y.B.Wei, G.Q.Xiao, Z.G.Xiao, T.Yamaguchi, Y.Yamaguchi, A.Yoshida, W.L.Zhan, H.Y.Zhang, T.Zheng, C.Zhong

Measurements of the interaction cross-sections for 14Be and 14, 15B as projectiles with a new scheme at RIBLL

NUCLEAR REACTIONS C(14Be, X), (14B, X), (15B, X), E ≈ 50 MeV/nucleon; measured interaction σ.

doi: 10.1016/j.nimb.2006.01.054
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2006SU22      Int.J.Mod.Phys. E15, 1803 (2006)

Q.M.Su, D.Q.Fang, Y.G.Ma, C.Zhong, C.W.Ma, K.Wang, T.Z.Yan, X.Z.Cai, W.Q.Shen

Study of isoscaling phenomena for projectile-like fragments

NUCLEAR REACTIONS 112Sn(40Ca, X), (48Ca, X), (58Ni, X), (64Ni, X), (78Kr, X), (86Kr, X), (112Sn, X), (124Sn, X), (129Xe, X), (136Xe, X), E=60 MeV/nucleon; calculated fragment yields; deduced isoscaling parameters. Statistical abrasion-ablation model.

doi: 10.1142/S021830130600537X
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2006YA09      Phys.Lett. B 638, 50 (2006)

T.Z.Yan, Y.G.Ma, X.Z.Cai, J.G.Chen, D.Q.Fang, W.Guo, C.W.Ma, E.J.Ma, W.Q.Shen, W.D.Tian, K.Wang

Scaling of anisotropic flow and momentum-space densities for light particles in intermediate energy heavy ion collisions

NUCLEAR REACTIONS 124Sn(86Kr, X), E=25 MeV/nucleon; calculated elliptic and higher order flows vs transverse momentum, related quantities. Isospin dependent quantum molecular dynamics model.

doi: 10.1016/j.physletb.2006.05.018
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2005CH71      Chinese Physics 14, 2444 (2005)

J.-G.Chen, X.-Z.Cai, T.-T.Wang, Yu.-G.Ma, Z.-Z.Ren, D.-Q.Fang, C.Zhong, Yi.-B.Wei, W.Guo, X.-F.Zhou, K.Wang, G.-L.Ma, W.-D.Tian, J.-H.Chen, T.-Z.Yan, J.-X.Zuo, C.-W.Ma, W.-Q.Shen

Investigation on the deformation of Ne and Mg isotope chains within relativistic mean-field model

NUCLEAR STRUCTURE 18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36Ne, 20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44Mg; calculated deformations, binding energies, shape coexistence features. Relativistic mean-field model, comparison with data.

doi: 10.1088/1009-1963/14/12/013
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2005FA05      Chin.Phys.Lett. 22, 572 (2005)

D.-Q.Fang, C-W.Ma, Y.-G.Ma, X.-Z.Cai, J.-G.Chen, J.-H.Chen, W.Guo, W.-D.Tian, K.Wang, Y.-B.Wei, T.-Z.Yan, C.Zhong, J.-X.Zuo, W.-Q.Shen

One-Proton Halo Structure in 23Al

NUCLEAR REACTIONS 12C(23Al, X), E ≈ 36 MeV/nucleon; analyzed reaction σ. 23Al deduced s-wave spectroscopic factor, halo features. Glauber model.

NUCLEAR STRUCTURE 22Mg, 23Al; calculated matter density distributions.

doi: 10.1088/0256-307X/22/3/015
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2005KA49      Eur.Phys.J. A 25, Supplement 1, 261 (2005)

R.Kanungo, M.Chiba, B.Abu-Ibrahim, S.Adhikari, D.Q.Fang, N.Iwasa, K.Kimura, K.Maeda, S.Nishimura, T.Ohnishi, A.Ozawa, C.Samanta, T.Suda, T.Suzuki, Q.Wang, C.Wu, Y.Yamaguchi, K.Yamada, A.Yoshida, T.Zheng, I.Tanihata

A new view to the structure of 19C

NUCLEAR REACTIONS Be(19C, 18CX), (19C, 17CX), E not given; measured longitudinal momentum distributions; deduced role of neutron evaporation. Comparison with Glauber model calculations.

doi: 10.1140/epjad/i2005-06-183-0
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2005KA51      Eur.Phys.J. A 25, Supplement 1, 327 (2005)

R.Kanungo, M.Chiba, B.Abu-Ibrahim, S.Adhikari, D.Q.Fang, N.Iwasa, K.Kimura, K.Maeda, S.Nishimura, T.Ohnishi, A.Ozawa, C.Samanta, T.Suda, T.Suzuki, Q.Wang, C.Wu, Y.Yamaguchi, K.Yamada, A.Yoshida, T.Zheng, I.Tanihata

Observation of a two-proton halo in 17Ne

NUCLEAR REACTIONS Be(17Ne, 15OX), E=64 MeV/nucleon; measured fragments longitudinal momentum distributions, interaction σ. 17Ne deduced two-proton halo features. Few-body Glauber model analysis.

doi: 10.1140/epjad/i2005-06-184-y
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2005MA37      J.Phys.(London) G31, S1179 (2005)

Y.G.Ma, G.L.Ma, X.Z.Cai, J.G.Chen, J.H.Chen, D.Q.Fang, W.Guo, Z.J.He, H.Z.Huang, J.L.Long, C.W.Ma, B.H.Sa, W.Q.Shen, Q.M.Su, K.Wang, Y.B.Wei, T.Z.Yan, C.Zhong, J.X .Zuo

Δ-scaling and heat capacity in relativistic ion collisions

NUCLEAR REACTIONS 1H(p, X), C(C, X), Pb(Pb, X), E=20-200 GeV/nucleon; calculated particle multiplicities, heat capacity, Δ-scaling features.

doi: 10.1088/0954-3899/31/6/082
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2005MB06      Phys.Rev. C 72, 064603 (2005)

Y.G.Ma, K.Wang, X.Z.Cai, J.G.Chen, J.H.Chen, D.Q.Fang, W.Guo, C.W.Ma, G.L.Ma, W.Q.Shen, Q.M.Su, W.D.Tian, Y.B.Wei, T.Z.Yan, C.Zhong, X.F.Zhou, J.X.Zuo

Isoscaling behavior in fission dynamics

NUCLEAR REACTIONS 112Sn(112Sn, X), 116Sn(116Sn, X), E ≈ 7-10 MeV/nucleon; calculated fission fragment isotopic yields, mean temperature; deduced isoscaling behavior. Langevin model.

doi: 10.1103/PhysRevC.72.064603
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2005TI01      Chin.Phys.Lett. 22, 306 (2005)

W.-D.Tian, Yu.-G.Ma, X.-Z.Cai, J.G.Chen, J.-H.Chen, D.-Q.Fang, W.Guo, C.-W.Ma, G.-L.Ma, W.-Q.Shen, K.Wang, Y.-B.Wei, T.-Z.Yan, C.Zhong, J.-X.Zuo

Isoscaling Behaviour in the Isospin-Dependent Quantum Molecular Dynamics Model

NUCLEAR REACTIONS 40Ca(40Ca, X), 48Ca(48Ca, X), E=25-70 MeV/nucleon; calculated fragment yield ratios, isoscaling parameters. Isospin-dependent quantum molecular dynamics.

doi: 10.1088/0256-307X/22/2/011
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2005WA04      Chin.Phys.Lett. 22, 53 (2005)

K.Wang, Y.-G.Ma, Y.-B.Wei, X.-Z.Cai, J.-G.Chen, D.-Q.Fang, W.Guo, G.-L.Ma, W.-Q.Shen, W.-D.Tian, C.Zhong, X.-F.Zhou

Isoscaling of the Fission Fragments with Langevin Equation

NUCLEAR REACTIONS 112Sn(112Sn, X), 116Sn(116Sn, X), E=8.4 MeV/nucleon; calculated fission fragment yield ratios, isoscaling features. Langevin equation.

doi: 10.1088/0256-307X/22/1/016
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2005WE01      Chin.Phys.Lett. 22, 61 (2005)

Y.-B.Wei, Y.-G.Ma, X.-Z.Cai, C.Zhong, J.-G.Chen, H.-Y.Zhang, D.-Q.Fang, K.Wang, G.-L.Ma, W.Guo, W.-D.Tian, W.-Q.Shen, W.-L.Zhan, G.-Q.Xiao, H.-S.Xu, Z.-Y.Sun, J.-X.Li, Z.-Y.Guo, M.Wang, Z.-Q.Chen, Z.-G.Hu, L.-X.Chen, C.Li, R.-S.Mao, J.Bai

Parallel Momentum Distribution of 28Si Fragments from 29P

NUCLEAR REACTIONS 12C(29P, 28SiX), E=30.7 MeV/nucleon; measured fragments parallel momentum distribution. 28Si, 29P deduced particle density distributions, related features. Glauber model and Skyrme-Hartree-Fock calculations.

doi: 10.1088/0256-307X/22/1/018
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2005YE05      J.Phys.(London) G31, S1647 (2005)

Y.L.Ye, D.Y.Pang, G.L.Zhang, D.X.Jiang, T.Zheng, Z.H.Li, X.Q.Li, Q.J.Wang, Y.C.Ge, C.E.Wu, J.Wang, Z.Q.Chen, Y.Ai, A.Ozawa, Y.Yamaguchi, D.Q.Fang, I.Tanihata

Study of the halo nucleus 6He through the direct nuclear reactions

NUCLEAR REACTIONS 9Be(6He, 6He), (6He, 5He), (6He, α), (6He, αX), (6He, tX), E=25 MeV/nucleon; measured quasielastic, breakup, and transfer σ(θ). 6He deduced two-triton configuration.

doi: 10.1088/0954-3899/31/10/048
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2004CH43      Nucl.Phys. A741, 29 (2004)

M.Chiba, R.Kanungo, B.Abu-Ibrahim, S.Adhikari, D.Q.Fang, N.Iwasa, K.Kimura, K.Maeda, S.Nishimura, T.Ohnishi, A.Ozawa, C.Samanta, T.Suda, T.Suzuki, I.Tanihata, Q.Wang, C.Wu, Y.Yamaguchi, K.Yamada, A.Yoshida, T.Zheng

Neutron removal studies on 19C

NUCLEAR REACTIONS Be(19C, 18CX), (19C, 17CX), E=64 MeV/nucleon; measured one- and two-neutron removal σ, longitudinal momentum distributions. Comparison with previous results.

doi: 10.1016/j.nuclphysa.2004.06.009
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2004CH60      Chin.Phys.Lett. 21, 2140 (2004)

J.-G.Chen, X.-Z.Cai, T.-T.Wang, Y.-G.Ma, Z.-Z.Ren, D.-Q.Fang, C.Zhong, Y.-B.Wei, W.Guo, X.-F.Zhou, K.Wang, G.-L.Ma, W.-D.Tian, J.-X.Zuo, C.-W.Ma, J.-H.Chen, T.-Z.Yan, W.-Q.Shen

Investigation of Exotic Structure of the Largely Deformed Nucleus 23Al in the Relativistic-Mean-Field Model

NUCLEAR STRUCTURE 23Al; calculated ground-state binding energy, quadrupole deformation, radii, one- and two-proton separation energies, excited states energies, J, π, configurations. 20Ne, 21Na, 22Mg; calculated ground-state quadrupole deformations. Deformed relativistic mean field model.

doi: 10.1088/0256-307X/21/11/018
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2004FA06      Phys.Rev. C 69, 034613 (2004)

D.Q.Fang, T.Yamaguchi, T.Zheng, A.Ozawa, M.Chiba, R.Kanungo, T.Kato, K.Morimoto, T.Ohnishi, T.Suda, Y.Yamaguchi, A.Yoshida, K.Yoshida, I.Tanihata

One-neutron halo structure 15C

NUCLEAR REACTIONS C(14C, X), E=83 MeV/nucleon; C(15C, X), E=51, 83 MeV/nucleon; measured reaction σ. C(15C, 14CX), (15C, 13CX), (14C, 13CX), E=83 MeV/nucleon; measured fragment longitudinal momentum distributions. 15C deduced matter density distribution, halo structure.

doi: 10.1103/PhysRevC.69.034613
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2004MA47      Phys.Rev. C 69, 064610 (2004)

Y.G.Ma, K.Wang, Y.B.Wei, G.L.Ma, X.Z.Cai, J.G.Chen, D.Q.Fang, W.Guo, W.Q.Shen, W.D.Tian, C.Zhong

Isoscaling in the lattice gas model

doi: 10.1103/PhysRevC.69.064610
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2004WE12      J.Phys.(London) G30, 2019 (2004)

Y.B.Wei, Y.G.Ma, W.Q.Shen, G.L.Ma, K.Wang, X.Z.Cai, C.Zhong, W.Guo, J.G.Chen, D.Q.Fang, W.D.Tian, X.F.Zhou

Systematic studies of binding energy dependence of neutron-proton momentum correlation function

NUCLEAR STRUCTURE 11,12,13,14B; calculated binding energies, radii, proton-neutron correlation functions. Isospin-dependent quantum molecular dynamics.

doi: 10.1088/0954-3899/30/12/018
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2004WU03      Nucl.Phys. A739, 3 (2004)

C.Wu, Y.Yamaguchi, A.Ozawa, R.Kanungo, I.Tanihata, T.Suzuki, D.Q.Fang, T.Suda, T.Ohnishi, M.Fukuda, N.Iwasa, T.Ohtsubo, T.Izumikawa, R.Koyama, W.Shinozaki, M.Takahashi

Study of the density distribution of 17C from reaction cross section measurement

NUCLEAR REACTIONS C(17C, X), E=79 MeV/nucleon; measured reaction σ. 17C deduced density distribution. Glauber model analysis.

doi: 10.1016/j.nuclphysa.2004.03.220
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2004YA28      Phys.Rev. C 70, 054320 (2004)

Y.Yamaguchi, C.Wu, T.Suzuki, A.Ozawa, D.Q.Fang, M.Fukuda, N.Iwasa, T.Izumikawa, H.Jeppesen, R.Kanungo, R.Koyama, T.Ohnishi, T.Ohtsubo, W.Shinozaki, T.Suda, M.Takahashi, I.Tanihata

Density distribution of 17B from a reaction cross-section measurement

NUCLEAR REACTIONS C(17B, X), E=77 MeV/nucleon; measured reaction σ. 17B deduced density distribution, halo features.

doi: 10.1103/PhysRevC.70.054320
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2003CA07      Nucl.Phys. A717, 117 (2003)

X.Z.Cai, W.Q.Shen, C.Zhong, Y.G.Ma, D.Q.Fang, H.Y.Zhang, Y.B.Wei, W.Guo, J.G.Chen, K.Wang, G.L.Ma

Study of incident energy and isospin dependencies of total reaction cross section via the BUU model

NUCLEAR REACTIONS 12C(8He, X), (9Be, X), (10Be, X), (11Be, X), (12Be, X), (14Be, X), (8B, X), (12B, X), (13B, X), (14B, X), (15B, X), (9C, X), (10C, X), (11C, X), (12C, X), (13C, X), (14C, X), (15C, X), (16C, X), (17C, X), (18C, X), (19C, X), (12N, X), (13N, X), (13O, X), (14O, X), (15O, X), E=10-1000 MeV/nucleon; calculated reaction σ, isospin dependencies. Boltzmann-Uehling-Uhlenbeck model.

doi: 10.1016/S0375-9474(03)00610-9
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2003ZH12      Chin.Phys.Lett. 20, 629 (2003)

C.Zhong, X.-Z.Cai, W.-Q.Shen, H.-Y.Zhang, Y.-B.Wei, J.-G.Chen, Y.-G.Ma, W.Guo, D.-Q.Fang

Calculation of Total Reaction Cross Section Induced by Intermediate Energy α-Particles with the Boltzmann-Uehling-Uhlenbeck Model

NUCLEAR REACTIONS 9Be, 12C, 16O, 28Si, 40Ca, 58,60Ni, 112,116,120,124Sn, 208Pb(α, X), E ≈ 15-50 MeV; calculated total reaction σ. Boltzmann-Uehling-Uhlenbeck model, comparison with data.

doi: 10.1088/0256-307X/20/5/311
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2003ZH49      Mod.Phys.Lett. A 18, 151 (2003)

H.Y.Zhang, W.Q.Shen, Y.G.Ma, X.Z.Cai, D.Q.Fang, C.Zhong, Y.B.Wei, J.G.Chen, X.F.Zhou, G.L.Ma, K.Wang, Z.Z.Ren, W.L.Zhan, Z.Y.Guo, G.Q.Xiao, H.S.Xu, J.S.Wang, Z.Y.Sun, H.X.Li, M.Wang, Z.Q.Chen, Z.G.Xiao, W.F.Li, J.F.Li, Z.G.Hu, J.Bai, L.X.Chen

Possible exotic structure in light proton-rich nuclei

NUCLEAR REACTIONS C(15N, X), (17N, X), (16O, X), (18O, X), (17F, X), (19F, X), (21F, X), (20Ne, X), (22Ne, X), (21Na, X), (23Na, X), (22Mg, X), (24Mg, X), (23Al, X), (25Al, X), (26Si, X), (27P, X), E ≈ 18-33 MeV; measured reaction σ. 17F, 23Al, 27P deduced radii, halo features. Secondary beams from 36Ar fragmentation. Comparison with model predictions.

doi: 10.1142/S0217732303010156
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2002CA04      Phys.Rev. C65, 024610 (2002)

X.Z.Cai, H.Y.Zhang, W.Q.Shen, Z.Z.Ren, J.Feng, D.Q.Fang, Z.Y.Zhu, W.Z.Jiang, Y.G.Ma, C.Zhong, W.L.Zhan, Z.Y.Guo, G.Q.Xiao, J.S.Wang, Y.T.Zhu, J.C.Wang, J.X.Li, M.Wang, J.F.Wang, Z.J.Ning, Q.J.Wang, Z.Q.Chen

Existence of a Proton Halo in 23Al and Its Significance

NUCLEAR REACTIONS 12C(19F, X), (20Ne, X), (21Na, X), (22Mg, X), (23Al, X), (24Al, X), (25Al, X), (26Al, X), (27Al, X), (28Al, X), E ≈ 20-35 MeV/nucleon; measured reaction σ. 23Al deduced proton halo. Comparison with model prediction.

doi: 10.1103/PhysRevC.65.024610
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0546.


2002CA38      Chin.Phys.Lett. 19, 1068 (2002)

X.-Z.Cai, W.-Q.Shen, Z.-Z.Ren, W.-Z.Jiang, D.-Q.Fang, H.-Y.Zhang, C.Zhong, Y.-B.Wei, W.Guo, Y.-G.Ma, Z.-Y.Zhu

One-Proton Halo in 31Cl with Relativistic Mean-Field Theory

NUCLEAR STRUCTURE 31,32Cl, 30,31S; calculated binding energies, radii, density distributions. 31Cl deduced proton halo. Relativistic mean-field theory.

doi: 10.1088/0256-307X/19/8/312
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2002ZH30      Nucl.Phys. A707, 303 (2002)

H.Y.Zhang, W.Q.Shen, Z.Z.Ren, Y.G.Ma, W.Z.Jiang, Z.Y.Zhu, X.Z.Cai, D.Q.Fang, C.Zhong, L.P.Yu, Y.B.Wei, W.I.Zhan, Z.Y.Guo, G.Q.Xiao, J.S.Wang, J.C.Wang, Q.J.Wang, J.X.Li, M.Wang, Z.Q.Chen

Measurement of Reaction Cross Section for Proton-Rich Nuclei (A < 30) at Intermediate Energies

NUCLEAR REACTIONS C(12C, X), (13C, X), (14C, X), (13N, X), (14N, X), (15N, X), (16N, X), (17N, X), (15O, X), (16O, X), (17O, X), (18O, X), (19O, X), (17F, X), (18F, X), (19F, X), (20F, X), (21F, X), (19Ne, X), (20Ne, X), (21Ne, X), (22Ne, X), (21Na, X), (22Na, X), (23Na, X), (24Na, X), (22Mg, X), (23Mg, X), (24Mg, X), (25Mg, X), (26Mg, X), (23Al, X), (24Al, X), (25Al, X), (26Al, X), (27Al, X), (28Al, X), (26Si, X), (27Si, X), (28Si, X), (29Si, X), (27P, X), (28P, X), (29S, X), E=18-33 MeV; measured reaction σ. 17F, 23Al, 27P deduced radii, halo features. Secondary beams from 36Ar fragmentation. Comparison with model predictions.

doi: 10.1016/S0375-9474(02)01007-2
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0715.


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