NSR Query Results


Output year order : Descending
Format : Normal

NSR database version of March 18, 2024.

Search: Author = D.Fang

Found 162 matches.

    Showing 1 to 100.

   [Next]

Back to query form



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
Citations: PlumX Metrics


2024FA02      Chin.Phys.C 48, 034101 (2024)

D.-L.Fang

What can we learn from recent 2νββ experiments?

RADIOACTIVITY 82Se, 100Mo, 136Xe(2β-); calculated nuclear matrix elements with the quasi-particle random phase approximation (QRPA) approach; deduced Gamow-Teller transition strength under a unique quenched axial-vector coupling constant gA, flipping the sign for the decay strength causes the spectra to go beyond the so-called high-lying state dominance hypothesis.

doi: 10.1088/1674-1137/ad181b
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2023FA03      Phys.Rev. C 107, 015501 (2023)

D.-L.Fang, A.Faessler

0νββ decay to the first 2+ state with a two-nucleon mechanism for a L-R symmetric model

RADIOACTIVITY 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 128,130Te, 136Xe(2β-); calculated phase space factors, nuclear matrix elements for 0νββ-decay to the first 2+ state of daughter nuclei. L-R symmetric model.

doi: 10.1103/PhysRevC.107.015501
Citations: PlumX Metrics


2023GU03      Phys.Rev. C 107, 014318 (2023)

L.Guo, W.L.Lv, Y.F.Niu, D.L.Fang, B.S.Gao, K.A.Li, X.D.Tang

Spin-isospin excitations in the direction of β+ decay for 80Zn and 126Ru at finite temperature

RADIOACTIVITY 80Zn, 126Ru(β+); calculated Gamow-Teller (GT+) strength distribution with respect to the ground state of daughter nuclei, spin-dipole (SD) transition strength distributions, sum-rule values of GT and SD transitions. Self consistent finite-temperature proton-neutron relativistic quasiparticle RPA (FT-PNRQRPA) and finite-temperature proton-neutron relativistic RPA (FT-PNRRPA) model.

doi: 10.1103/PhysRevC.107.014318
Citations: PlumX Metrics


2023LV01      Phys.Rev. C 108, L051304 (2023)

W.-L.Lv, Y.-F.Niu, D.-L.Fang, J.-M.Yao, C.-L.Bai, J.Meng

0νββ-decay nuclear matrix elements in self-consistent Skyrme quasiparticle random-phase approximation: Uncertainty from pairing interaction

doi: 10.1103/PhysRevC.108.L051304
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2022BA38      Chin.Phys.C 46, 114104 (2022)

C.L.Bai, D.L.Fang, H.Q.Zhang, C.L.Bai, D.L.Fang, H.Q.Zhang

Roles of tensor and isoscalar pairing interactions in β-Decay calculations for possible r-process waiting point nuclei with N ∼ 82 and 126

RADIOACTIVITY 120,122,124,126,128,130,132Cd(β-); calculated T1/2 with the self-consistent Hartree-Fock-Bogoliubov (HFB) theory with the proton-neutron quasi-particle random phase approximation (pnQRPA) based on the Skyrme force. Comparison with available data.

doi: 10.1088/1674-1137/ac80ee
Citations: PlumX Metrics


2022LV05      Phys.Rev. C 105, 044331 (2022)

W.L.Lv, Y.F.Niu, D.L.Fang, C.L.Bai

Single-state or low-lying-states dominance mechanism of 2νββ-decay nuclear matrix elements

RADIOACTIVITY 48Ca, 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 128,130Te, 136Xe, 150Nd, 238U(2β-); calculated matrix elements, isoscalar pairing strength parameter, Gamow-teller transition amplitudes. Spherical Skyrme HFB + QRPA model. Single-state dominance (SSD) and low-lying-states dominance (LLD) hypothesis. Comparison to experimental values.

doi: 10.1103/PhysRevC.105.044331
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2021FA01      Phys.Lett. B 813, 136067 (2021)

D.-L.Fang, Y.-F.Li, D.Zhang

Ab initio calculations of reactor antineutrino fluxes with exact lepton wave functions

NUCLEAR REACTIONS 235,238U, 239,241Pu(n, F), E thermal; calculated the isotopic reactor antineutrino fluxes with the exact the radial lepton wave functions, assuming all the decay branches are allowed GT transitions within a new ab initio approach.

doi: 10.1016/j.physletb.2021.136067
Citations: PlumX Metrics


2021FA07      Phys.Rev. C 103, 045501 (2021)

D.-L.Fang, A.Faessler

Nuclear matrix elements for the 0νββ(0+ → 2 decay of 76Ge within the two-nucleon mechanism

RADIOACTIVITY 76Ge(2β-); calculated nuclear matrix elements (NMEs) for 0νββ decay to the first 2+ state of 76Se, with estimated uncertainties using various approximations and parameters such as dependence of the NMEs on the model space for different multipoles, NMEs for a Coulomb-type neutrino potential, NME dependence on the short-range correlations, and NME dependence on particle-particle interaction strengths. Nuclear many body calculation using isospin symmetry restored quasiparticle random phase approximation (QRPA) method with the charge-dependent-Bonn realistic force. Comparison with results of previous calculations based on projected Hartree-Fock-Bogolyubov method.

doi: 10.1103/PhysRevC.103.045501
Citations: PlumX Metrics


2020FA05      Chin.Phys.C 44, 084104 (2020)

D.-L.Fang, A.Faessler

2νββ-decay to first 2+states with partial isospin symmetry restoration from spherical QRPA calculations

RADIOACTIVITY 76Ge, 96Zr, 116Cd, 128,130Te, 82Se, 100Mo, 136Xe(2β-); calculated nuclear matrix elements, phase space factors, T1/2.

doi: 10.1088/1674-1137/44/8/084104
Citations: PlumX Metrics


2020GO06      Phys.Rev. C 102, 014323 (2020)

A.Gottardo, G.de Angelis, P.Doornenbal, L.Coraggio, A.Gargano, N.Itaco, K.Kaneko, P.Van Isacker, T.Furumoto, G.Benzoni, J.Lee, H.Liu, M.Matsushita, D.Mengoni, V.Modamio-Hoybjor, S.Momiyama, T.Motobayashi, D.R.Napoli, M.Niikura, E.Sahin, Y.Shiga, H.Sakurai, R.Taniuchi, S.Takeuchi, H.Wang, J.J.Valiente-Dobon, R.Avigo, H.Baba, N.Blasi, F.L.Bello Garrote, F.Browne, F.C.L.Crespi, S.Ceruti, R.Daido, M.-C.Delattre, D.Fang, Zs.Dombradi, T.Isobe, I.Kuti, G.Lorusso, K.Matsui, B.Melon, T.Miyazaki, S.Nishimura, R.Orlandi, Z.Patel, S.Rice, L.Sinclair, P.A.Soderstrom, D.Sohler, T.Sumikama, J.Taprogge, Zs.Vajta, H.Watanabe, O.Wieland, J.Wu, Z.Y.Xu, M.Yalcinkaya, R.Yokoyama

Transition strengths in the neutron-rich 73, 74, 75Ni isotopes

NUCLEAR REACTIONS Pb(73Ni, 73Ni'), (74Ni, 74Ni'), (75Ni, 75Ni'), E=215 MeV/nucleon, [secondary cocktail beam from 9Be(238U, F), E=345 MeV/nucleon, and separated by A/Q using the BigRIPS fragment separator at RIBF-RIKEN facility]; measured reaction products identified by the ZeroDegree spectrometer, Eγ, Iγ, (scattered Ni nuclei)γ-coin using the WAS3Abi-EURICA setup with the DALI2 NaI(Tl) array for γ detection. 73,74,75Ni; deduced levels, J, π, B(E2) from Coulomb excitation cross sections. Comparison with large-scale shell model calculations.

doi: 10.1103/PhysRevC.102.014323
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2020RE12      Phys.Lett. B 809, 135702 (2020), Erratum Phys.Lett. B 820, 136532 (2021)

B.M.Rebeiro, S.Triambak, P.E.Garrett, B.A.Brown, G.C.Ball, R.Lindsay, P.Adsley, V.Bildstein, C.Burbadge, A.Diaz Varela, T.Faestermann, D.L.Fang, R.Hertenberger, M.Horoi, B.Jigmeddorj, M.Kamil, K.G.Leach, P.Z.Mabika, J.C.Nzobadila Ondze, J.N.Orce, H.-F.Wirth

Benchmarking 136Xe neutrinoless ββ decay matrix element calculations with the 138Ba(p, t) reaction

NUCLEAR REACTIONS 138Ba(p, t), (p, p), E=23 MeV; measured reaction products, Ep, Ip; deduced σ(θ), neutrinoless ββ decay matrix elements.

doi: 10.1016/j.physletb.2020.135702
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2532. Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2019NI10      Chin.Phys.C 43, 113001 (2019)

K.Ni, Y.Lai, A.Abdukerim, W.Chen, X.Chen, Y.Chen, X.Cui, Y.Fan, D.Fang, C.Fu, L.Geng, K.Giboni, F.Giuliani, L.Gu, X.Guo, K.Han, C.He, D.Huang, Y.Huang, Y.Huang, Z.Huang, P.Ji, X.Ji, Y.Ju, K.Liang, H.Liu, J.Liu, W.Ma, Y.Ma, Y.Mao, Y.Meng, P.Namwongsa, J.Ning, X.Ning, X.Ren, C.Shang, L.Si, A.Tan, A.Wang, H.Wang, M.Wang, Q.Wang, S.Wang, X.Wang, Z.Wang, M.Wu, S.Wu, J.Xia, M.Xiao, P.Xie, B.Yan, J.Yang, Y.Yang, C.Yu, J.Yuan, D.Zhang, H.Zhang, T.Zhang, L.Zhao, Q.Zheng, J.Zhou, N.Zhou, X.Zhou

Searching for neutrino-less double beta decay of 136Xe with PandaX-II liquid xenon detector

RADIOACTIVITY 136Xe(2β-); measured decay products, Eβ, Iβ; deduced T1/2 and Majorana neutrino mass limits. Comparison with available data.

doi: 10.1088/1674-1137/43/11/113001
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2018BA38      Phys.Rev. C 98, 044601 (2018)

M.Barbui, K.Hagel, J.Gauthier, S.Wuenschel, R.Wada, V.Z.Goldberg, R.T.deSouza, S.Hudan, D.Fang, X.-G.Cao, J.B.Natowitz

Searching for states analogous to the 12C Hoyle state in heavier nuclei using the thick target inverse kinematics technique

NUCLEAR REACTIONS 4He(20Ne, α), (20Ne, 2α), (20Ne, 3α), (20Ne, 4α), E=13 MeV/nucleon; measured Eα, α(θ), αα-coin, and differential σ(θ) for resonant scattering using ΔE-E telescopes and thick target inverse kinematics (TTIK) technique at K150 cyclotron facility of Texas A and M University. 8Be, 12C, 16O, 24Mg; deduced levels, J, π, multi-α condensed states, widths, evidence for a level in 16O at 15.2 MeV analogous to Hoyle state in 12C. Comparison with PACE4 and HIPSE simulations, and with experimental results.

doi: 10.1103/PhysRevC.98.044601
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2018FA04      Phys.Rev. C 97, 045503 (2018)

D.-L.Fang, A.Faessler, F.Simkovic

0νββ decay nuclear matrix element for light and heavy neutrino mass mechanisms from deformed quasiparticle random-phase approximation calculations for 76Ge, 82Se, 130Te, 136Xe, and 150Nd with isospin restoration

NUCLEAR STRUCTURE 76Ge, 76Se, 82Se, 82Kr, 130Te, 130Xe, 136Xe, 136Ba, 150Nd, 150Sm; calculated quadrupole deformation parameters, pairing strengths, BCS overlap, particle-particle interaction strengths for the corresponding parent/daughter pair in double beta decay using deformed Wood-Saxon potential with Coulomb corrections.

RADIOACTIVITY 76Ge, 82Se, 130Te, 136Xe, 150Nd(2β-); calculated nuclear matrix elements (NME) for 0νββ decay mode for both light and heavy neutrino mechanisms by deformed quasiparticle random-phase approach using AV18 and CD-Bonn potentials with and without short range correlations (SRC). Comparison with other theoretical calculations. 150Nd; detailed decomposition of NMEs for 150Nd decay into various intermediate channels, and for different model spaces.

doi: 10.1103/PhysRevC.97.045503
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2016DO05      Phys.Rev. C 93, 064317 (2016)

A.C.Dombos, D.-L.Fang, A.Spyrou, S.J.Quinn, A.Simon, B.A.Brown, K.Cooper, A.E.Gehring, S.N.Liddick, D.J.Morrissey, F.Naqvi, C.S.Sumithrarachchi, R.G.T.Zegers

Total absorption spectroscopy of the β decay of 76Ga

RADIOACTIVITY 76Ga(β-)[from 9Be(76Ge32+, X), E=130 MeV/nucleon and separated by A1900 fragment separator at NSCL-MSU]; measured Eγ, Iγ, total absorption gamma-ray (TAS) spectrum using a segmented NaI(Tl)(SuN) detector, Eβ, Iβ by a silicon surface barrier, βγ-coin, half-life of 76Ga decay; deduced Iβ feedings and compared to the evaluated data in the ENSDF database, β strength functions and B(GT). Comparison with shell-model calculations using jj44b and JUN45 interactions. Relevance to studies of neutrinoless double β-decay of 76Ge.

doi: 10.1103/PhysRevC.93.064317
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2016FA03      Phys.Rev. C 93, 034306 (2016)

D.-L.Fang

Effect of the Pauli principle on the deformed quasiparticle random-phase approximation calculations and its consequence for β-decay calculations of deformed even-even nuclei

RADIOACTIVITY 98,100Kr, 98,100,102,104,106Sr, 102,104,106,108,110,112Zr, 108,110,112,114,116Mo, 150,152,154,156,158,160,162,164,166,168,170,172,174Ce, 152,154,156,158,160,162,164,166,168,170,172,174,176Nd, 158,160,162,164,166,168,170,172,174,176,178Sm, 164,166,168,170,172,174,176,178,180Gd(β-); calculated half-lives, B(GT) for 100,102Sr, 110Zr using Pauli exclusion principle (PEP) in quasiparticle random phase approximation (QRPA) and renormalized quasiparticle random phase approximation (nQRPA)calculations by replacing traditional quasiboson approximation (QBA) for the deformed systems. Comparison with available experimental results.

doi: 10.1103/PhysRevC.93.034306
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2016NI07      Phys.Lett. B 756, 273 (2016)

N.Nishimura, Z.Podolyak, D.-L.Fang, T.Suzuki

Impact of the first-forbidden β decay on the production of A ∼ 195 r-process peak

NUCLEAR STRUCTURE A=175-210; calculated isotopic abundances, β-decay rates; deduced effects of first-forbidden transitions in β-decays on the production of the r-process A ∼ 195 peak. Comparison with available data.

doi: 10.1016/j.physletb.2016.03.025
Citations: PlumX Metrics


2016SU22      Yuan.Wul.Ping. 33, 230 (2016); Nucl.Phys.Rev. 33, 230 (2016)

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

An implantation and detection system for spectroscopy of 22, 24Si

RADIOACTIVITY 22,24Si(β+p); measured decay products, Ep, Ip; deduced energy levels, J, π, T1/2, branchning ratios.

doi: 10.11804/NuclPhysRev.33.02.230
Citations: PlumX Metrics


2015BR15      Phys.Rev. C 92, 041301 (2015)

B.A.Brown, D.L.Fang, M.Horoi

Evaluation of the theoretical nuclear matrix elements for ββ decay of 76Ge

RADIOACTIVITY 76Ge(2β-); calculated nuclear matrix elements (NMEs) for 2νββ and 0νββ decay modes using configuration-interaction (CI), quasiparticle random-phase approximation (QRPA), and interacting boson model methods. Comparison with experimental values.

doi: 10.1103/PhysRevC.92.041301
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2015FA05      Phys.Rev. C 91, 025503 (2015)

D.-L.Fang, B.A.Brown

Effect of first-forbidden decays on the shape of neutrino spectra

RADIOACTIVITY 136Te, 140Xe(β-); calculated levels, J, π in 136I and 140Cs, logft, neutrino spectra of low-lying first-forbidden (FF) β decay branches by shell-model (SM) and pn-QRPA (QRPA). Comparison with available experimental values.

doi: 10.1103/PhysRevC.91.025503
Citations: PlumX Metrics


2015FA11      Phys.Rev. C 92, 044301 (2015)

D.-L.Fang, A.Faessler, F.Simkovic

Partial restoration of isospin symmetry for neutrinoless double β decay in the deformed nuclear system of 150Nd

RADIOACTIVITY 150Nd(2β-); calculated nuclear matrix elements (NME), Fermi and Gamow-Teller matrix elements for the 0νββ decay mode, decomposition of the matrix elements for different values of Kπ using the deformed quasiparticle random-phase approximation (pn-QRPA) method. Isospin symmetry restoration.

doi: 10.1103/PhysRevC.92.044301
Citations: PlumX Metrics


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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2015MU04      J.Phys.(London) G42, 034027 (2015)

M.Mumpower, R.Surman, D.L.Fang, M.Beard, A.Aprahamian

The impact of uncertain nuclear masses near closed shells on the r-process abundance pattern

doi: 10.1088/0954-3899/42/3/034027
Citations: PlumX Metrics


2015MU12      Phys.Rev. C 92, 035807 (2015)

M.R.Mumpower, R.Surman, D.-L.Fang, M.Beard, P.Moller, T.Kawano, A.Aprahamian

Impact of individual nuclear masses on r-process abundances

NUCLEAR STRUCTURE Z=30-75, N=60-130, A=120-210; calculated relevant Q values, neutron capture rates, photodissociation rates, β-decay rates, and β-delayed neutron emission probabilities using the 2012 version of the Finite-Range Droplet Model (FRDM), and by considering variations of individual nuclear masses; deduced influence of uncertainties in individual masses on the r-process abundance distribution.

doi: 10.1103/PhysRevC.92.035807
Citations: PlumX Metrics


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
Citations: PlumX Metrics

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics


2013FA05      Phys.Rev. C 88, 024314 (2013)

D.-L.Fang, B.A.Brown, T.Suzuki

β-decay properties for neutron-rich Kr-Tc isotopes from deformed pn-quasiparticle random-phase approximation calculations with realistic forces

RADIOACTIVITY 96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,111Kr, 97,98,99,100,101,102,103,104,105,106,107,108,109,110,111,112Rb, 98,99,100,101,102,103,104,105,106,107,108,109,110,111,112,113Sr, 99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114Y, 104,105,106,107,108,109,110,111,112,113,114,115Zr, 105,106,107,108,109,110,111,112,113,114,115,116Nb, 107,108,109,110,111,112,113,114,115,116,117Mo, 108,109,110,111,112,113,114,115,116,117,118Tc(β-), (β-n); calculated half-lives, delayed neutron emission probabilities Pn. 98,100Y, 100Nb, 108Tc; calculated low-spin low-lying levels, J, π; and compared with experimental values. Deformed quasiparticle random-phase approximation (pn-QRPA) method with realistic CD-Bonn forces, including Gamow-Teller and first-forbidden β transitions. Comparison of half-life and Pn values with available data from RIKEN facility. Implications for r-process elemental abundances.

doi: 10.1103/PhysRevC.88.024314
Citations: PlumX Metrics


2013FA08      Phys.Rev. C 88, 034304 (2013)

D.-L.Fang, B.A.Brown, T.Suzuki

Investigating β-decay properties of spherical nuclei along the possible r-process path

RADIOACTIVITY 118,120,122,124,126,128,130,132Cd, 136,138,140Xe, 139Cs, 203,205Au, 207Tl(β-); 124Mo, 125Tc, 126Ru, 127Rh, 128Pd, 129Ag, 130Cd, 131In, 190Gd, 191Tb, 192Dy, 193Ho, 194Er, 195Tm, 196Yb, 197Lu, 198Hf, 199Ta, 113,115,117As, 114,116,118Se, 115,117,119Br, 116,118,120Kr, 117,119,121Rb, 118,120,122Sr, 119,121,123Y, 120,122,124Zr, 121,123,125Nb, 122,124,126Mo, 123,125,127Tc, 124,126,128Ru, 125,127,129Rh, 126,128,130Pd, 127,129,131Ag, 128,130,132Cd, 129,131,133In, 130,132,134Sn, 131,133,135Sb, 174,176Sn, 175,177Sb, 176,178Te, 177,179I, 178,180Xe, 179,181Cs, 180,182,184Ba, 181,183,185La, 182,184,186Ce, 183,185,187Pr, 184,186,188Nd, 185,187,189Pm, 186,188,190Sm, 187,189,191Eu, 188,190,192Gd, 189,191,193Tb, 190,192,194Dy, 191,193,195Ho, 192,194,196Er, 193,195,197Tm, 194,196,198Yb, 195,197,199Lu, 196,198,200Hf, 197,199,201Ta, 198,200,202W, 199,201,203Re, 200,202,204Os, 201,203,205Ir, 202,204,206Pt, 203,205,207Au, 206,208Hg, 207,209Tl(β-), (β-n); calculated Q values, half-life, delayed neutron emission probability Pn, logft, first-forbidden to total ratio. Spherical QRPA + real forces (FRDM+GTF, FRDM+Real, HFB21+Real) using different mass models. Comparison with experimental data. Relevance to r-process path.

NUCLEAR STRUCTURE 118,120,122,124,126,128,130,132Cd, 136,138,140Xe, 139Cs, 203,205Au, 207Tl; calculated levels, J, π. Spherical QRPA + real forces. Comparison with experimental data.

doi: 10.1103/PhysRevC.88.034304
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2013XU01      Phys.Rev. C 87, 014335 (2013)

R.Xu, C.Wu, G.Ma, D.Fang, Z.Ren

Properties of deformed even-even nuclei near Z=20 in an improved quark mass density-dependent model

NUCLEAR STRUCTURE 24,26,28,30,32,34,36,38,40,42Si, 28,30,32,34,36,38,40,42,44,46S, 32,34,36,38,40,42,44,46,48,50Ar, 36,38,40,42,44,46,48,50,52,54,56Ca, 40,42,44,46,48,50,52,54,56,58,60Ti, 42,44,46,48,50,52,54,56,58,60,62,64,66Cr, 50,52,54,56,58,60,62,64,66,68,70,72Fe; calculated binding energy/nucleon, S(2n), S(2p), β2 prolate and oblate, rms charge, neutron and proton radii, hexadecapole moment, prolate-oblate energy difference, neutron skin thickness. Improved quark mass density-dependent (IQMDD) model. Comparison with experimental data.

doi: 10.1103/PhysRevC.87.014335
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2012FA02      Phys.Rev. C 85, 035503 (2012)

D.-L.Fang, K.Blaum, S.Eliseev, A.Faessler, M.I.Krivoruchenko, V.Rodin, F.Simkovic

Evaluation of the resonance enhancement effect in neutrinoless double-electron capture in 152Gd, 164Er, and 180W atoms

RADIOACTIVITY 152Gd, 164Er, 180W(2EC); calculated matrix elements and half-lives for neutrinoless double-electron capture. Deformed quasiparticle random-phase approximation using the realistic charge-dependent Bonn (CD-Bonn) nucleon-nucleon interaction. Comparison of half-life with that for neutrinoless 2β decay of 76Ge.

doi: 10.1103/PhysRevC.85.035503
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2368.


2012TO06      Phys.Rev.Lett. 108, 222501 (2012)

Y.Togano, Y.Yamada, N.Iwasa, K.Yamada, T.Motobayashi, N.Aoi, H.Baba, S.Bishop, X.Cai, P.Doornenbal, D.Fang, T.Furukawa, K.Ieki, T.Kawabata, S.Kanno, N.Kobayashi, Y.Kondo, T.Kuboki, N.Kume, K.Kurita, M.Kurokawa, Y.G.Ma, Y.Matsuo, H.Murakami, M.Matsushita, T.Nakamura, K.Okada, S.Ota, Y.Satou, S.Shimoura, R.Shioda, K.N.Tanaka, S.Takeuchi, W.Tian, H.Wang, J.Wang, K.Yoneda

Hindered Proton Collectivity in 2816S12: Possible Magic Number at Z=16

NUCLEAR REACTIONS Pb(28S, 28S'), (28Mg, 28Mg') E=53 MeV/nucleon; measured reaction products, Eγ, Iγ. 28S, 28Mg; deduced level energy, σ(θ), B(E2), deformation parameters. Comparison with available data, 36Ar secondary beams.

doi: 10.1103/PhysRevLett.108.222501
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2378. Data from this article have been entered in the XUNDL database. For more information, click here.


2011FA02      Phys.Rev. C 83, 034320 (2011)

D.Fang, A.Faessler, V.Rodin, F.Simkovic

Neutrinoless double-β decay of deformed nuclei within quasiparticle random-phase approximation with a realistic interaction

RADIOACTIVITY 76Ge, 150Nd, 160Gd(2β-); calculated nuclear matrix elements for neutrinoless double β decay using quasiparticle random-phase approximation with realistic residual interaction. Analyzed short-range correlations and the quenching of the axial vector coupling constant. 150Nd; probe of the Majorana neutrino mass.

doi: 10.1103/PhysRevC.83.034320
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2011GU14      Phys.Rev. C 83, 064318 (2011)

C.J.Guess, T.Adachi, H.Akimune, A.Algora, S.M.Austin, D.Bazin, B.A.Brown, C.Caesar, J.M.Deaven, H.Ejiri, E.Estevez, D.Fang, A.Faessler, D.Frekers, H.Fujita, Y.Fujita, M.Fujiwara, G.F.Grinyer, M.N.Harakeh, K.Hatanaka, C.Herlitzius, K.Hirota, G.W.Hitt, D.Ishikawa, H.Matsubara, R.Meharchand, F.Molina, H.Okamura, H.J.Ong, G.Perdikakis, V.Rodin, B.Rubio, Y.Shimbara, G.Susoy, T.Suzuki, A.Tamii, J.H.Thies, C.Tur, N.Verhanovitz, M.Yosoi, J.Yurkon, R.G.T.Zegers, J.Zenihiro

The 150Nd(3He, t) and 150Sm(t, 3He) reactions with applications to ββ decay of 150Nd

NUCLEAR REACTIONS 150Nd(3He, t), E=140 MeV/nucleon; 150Sm(t, 3He), E=115 MeV/nucleon; measured triton and 3He spectra, excitation energy spectra, differential cross sections, σ(θ) 150Pm; deduced B(GT) strengths; isovector spin-flip giant monopole resonance (IVSGMR). Grand Raiden Spectrometer for (3He, t) and S-800 spectrometer for (t, 3He). Comparison with Quasi-Particle Random Phase Approximation (QRPA) calculations. Application to double β decay of 150Nd.

RADIOACTIVITY 150Nd(2β-); calculated matrix elements for 0νββ and 2νββ decay modes using QRPA calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.064318
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2347. 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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2011TO15      J.Phys.:Conf.Ser. 312, 042025 (2011)

Y.Togano, T.Motobayashi, N.Aoi, H.Baba, S.Bishop, X.Cai, P.Doornenbal, D.Fang, T.Furukawa, K.Ieki, N.Iwasa, T.Kawabata, S.Kanno, N.Kobayashi, Y.Kondo, T.Kuboki, N.Kume, K.Kurita, M.Kurokawa, Y.G.Ma, Y.Matsuo, H.Murakami, M.Matsushita, T.Nakamura, K.Okada, S.Ota, Y.Satou, S.Shimoura, R.Shioda, K.N.Tanaka, S.Takeuchi, W.Tian, H.Wang, J.Wang, K.Yamada, Y.Yamada, K.Yoneda

Experimental Investigation of the Stellar Reaction 30S(p, γ)31Cl via Coulomb Dissociation

NUCLEAR REACTIONS 208Pb(31Cl, p30S), E=58 MeV/nucleon; measured Coulomb excitation dissociation E(products), I(θ, products), Eγ, Iγ, (Cl)γ-coin; deduced Doppler-corrected γ spectrum, 31Cl dissociation spectrum.

doi: 10.1088/1742-6596/312/4/042025
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2010FA03      Phys.Rev. C 81, 037303 (2010)

D.Fang, A.Faessler, V.Rodin, M.Saleh Yousef, F.Simkovic

Running sums for 2νββ-decay matrix elements within the quasiparticle random-phase approximation with account for deformation

RADIOACTIVITY 76Ge, 150Nd(2β-); calculated matrix elements (running sums) for 2-neutrino double β decay using deformation and p-p strength parameters in quasiparticle random-phase approximation (QRPA) approach.

doi: 10.1103/PhysRevC.81.037303
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2010FA17      Phys.Rev. C 82, 051301 (2010)

D.-L.Fang, A.Faessler, V.Rodin, F.Simkovic

Neutrinoless double-β decay of 150Nd accounting for deformation

NUCLEAR STRUCTURE 150Nd(2β-); calculated neutrinoless double-beta decay matrix elements while accounting for β2 deformation parameter. Microscopic calculation with quasiparticle random phase approximation (QRPA) approach and realistic residual interaction. Relevance for SNO+ collaboration and the best sensitivity for the Majorana neutrino mass measurement.

doi: 10.1103/PhysRevC.82.051301
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2124.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2047.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


Back to query form    [Next]


Note: The following list of authors and aliases matches the search parameter D.Fang: , D.F.FANG, D.L.FANG, D.Q.FANG