NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = Z.Ma Found 162 matches. Showing 1 to 100. [Next]2023HA08 Phys.Rev. A 107, L020803 (2023) P.Hao, K.Deng, F.F.Wu, Z.Y.Ma, W.Z.Wei, W.H.Yuan, Y.B.Du, H.L.Liu, H.X.Zhang, L.R.Pang, B.Wang, J.Zhang, Z.H.Lu Precision measurement of 25Mg+-ion D1 and D2 transition frequencies ATOMIC PHYSICS 25Mg; measured frequencies; deduced precise values of doublet transition frequencies using the decoherence-assisted spectroscopy method with the full use of spontaneous emission signals to improve the detection sensitivity.
doi: 10.1103/PhysRevA.107.L020803
2021PA03 Appl.Radiat.Isot. 168, 109534 (2021) W.t.Pan, T.Song, H.-y.Lan, Z.-g.Ma, J.-l.Zhang, Z.-c.Zhu, W.Luo Photo-excitation production of medically interesting isomers using intense γ-ray source NUCLEAR REACTIONS 103Rh, 113,115In, 176Lu(γ, γ'), E<30 MeV; calculated isomer production σ, specific activities, yields; deduced suitable decay properties for photo-excitation approach.
doi: 10.1016/j.apradiso.2020.109534
2020SU07 Phys.Rev. C 101, 034302 (2020) X.Sun, R.Xu, Y.Tian, Z.Ma, Z.Zhang, Z.Ge, H.Zhang, E.N.E.van Dalen, H.Muther Relativistic mean-field approach in nuclear systems NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 116,132Sn, 208Pb; calculated binding energy per nucleon, charge radii, charge density distribution, single particle energies, spin-orbit splitting in 16O, scalar and vector potentials for neutrons and protons as a function of isospin asymmetry using both local density approximation (LDA) and improved LDA, based on Dirac-Brueckner-Hartree-Fock (DBHF) approach starting from a realistic nucleon-nucleon interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.101.034302
2019LI22 Chin.Phys.C 43, 064001 (2019) C.-Q.Liu, Z.Wei, C.Han, C.Huang, Z.-W.Huang, Z.-W.Ma, S.-J.Zhang, S.-Hu.Peng, W.-M.Li, X.-H.Bai, J.-R.Wang, X.-L.Lu, Y.Zhang, D.-P.Xu, X.-D.Su, Z.-E.Yao Monte Carlo simulation of fast neutron-induced fission of 237Np NUCLEAR REACTIONS 237Np, 232Th, 235,238U, 239Pu(n, F), E=0.50, 2, 4, 5, 59.9, 5.04, 160, 4.48 MeV; calculated pre-neutron emission fission-fragment mass distribution using GEANT4. Comparison with experimental data.
doi: 10.1088/1674-1137/43/6/064001
2019NA25 Phys.Rev. A 100, 053415 (2019) A.I.Nahlawi, Z.L.Ma, M.S.Conradi, B.Saam High-precision determination of the frequency-shift enhancement factor in Rb- 129Xe ATOMIC PHYSICS Rb, 129Xe; measured frequencies; deduced the dimensionless enhancement factor.
doi: 10.1103/PhysRevA.100.053415
2019PA21 Phys.Rev. C 99, 045807 (2019) S.N.Paneru, C.R.Brune, R.Giri, R.J.Livesay, U.Greife, J.C.Blackmon, D.W.Bardayan, K.A.Chipps, B.Davids, D.S.Connolly, K.Y.Chae, A.E.Champagne, C.Deibel, K.L.Jones, M.S.Johnson, R.L.Kozub, Z.Ma, C.D.Nesaraja, S.D.Pain, F.Sarazin, J.F.Shriner, D.W.Stracener, M.S.Smith, J.S.Thomas, D.W.Visser, C.Wrede s-wave scattering lengths for the 7Be + p system from an R-matrix analysis NUCLEAR REACTIONS 1H(7Be, 7Be), (7Be, 7Be'), E=4-27 MeV; 12C(7Be, 7Be), E=7, 14 meV; measured scattered ions, differential σ(θ) using (CH2)n target and segmented Silicon Detector Array (SIDAR) for scattered ion detection at ORNL-HRIBF; deduced s-wave scattering lengths, R-matrix analysis of elastic and inelastic scattering data; analyzed cross-section data from Louvain-la-Neuve reported in 2003An06 reference. Comparison with previous experimental values, and optical model calculations. Relevance to astrophysical S factor for 7Be(p, γ) reaction. 8B; verified levels at 1.9, 2.21 and 9.0 MeV.
doi: 10.1103/PhysRevC.99.045807
2019WE06 Chin.Phys.C 43, 054001 (2019) Z.Wei, J.-R.Wang, Y.-L.Zhang, Z.-W.Huang, Z.-W.Ma, J.Zhang, Y.-Y.Ding, L.Xia, J.-Y.Li, X.-L.Lu, Y.Zhang, D.-Pe.Xu, L.Yang, Z.-E.Yao Calculation of the wide-angle neutron spectra from the 9Be(d, xn) reaction in a thick beryllium target NUCLEAR REACTIONS 9Be(d, xn), E=10 MeV; calculated σ(θ, E), neutron yields using TALYS-1.8 nuclear model code.
doi: 10.1088/1674-1137/43/5/054001
2019WE13 Eur.Phys.J. A 55, 162 (2019) Z.Wei, C.Han, S.H.Peng, X.H.Bai, C.Q.Liu, Z.W.Ma, Z.W.Huang, S.J.Zhang, W.M.Li, Y.Yang, Z.E.Yao, W.S.Wu, Y.Zhang, X.L.Lu, J.R.Wang, X.D.Su, D.P.Xu Physical design and evaluation of a high-intensity accelerator-based D-D/D-T fusion neutron source
doi: 10.1140/epja/i2019-12848-5
2019ZH39 Nucl.Phys. A990, 1 (2019) Z.Zhang, R.R.Xu, Z.Y.Ma, Z.G.Ge, Y.Tian, D.Y.Pang, X.D.Sun, Y.L.Jin, X.Tao, Y.Zhang, J.M.Wang Global α-nucleus optical model based on an Dirac Brueckner Hartree Fock approach
doi: 10.1016/j.nuclphysa.2019.06.013
2018TI06 Phys.Rev. C 97, 064615 (2018) Effects of nonlocality of nuclear potentials on direct capture reactions NUCLEAR REACTIONS 48Ca(n, γ), E=0.01-0.4 MeV; 7Li(n, γ), E=0.01-2 MeV; 12C(p, γ), E=0-1.2 MeV; calculated local and non-local potential parameters, s-wave phase shifts of target nuclides as function of incident energy, and σ(E) with the Perey-Buck-type nonlocal potentials using a potential model; deduced effects of potential nonlocality in direct radiative capture reactions. Comparison with experimental values.
doi: 10.1103/PhysRevC.97.064615
2017MU07 Int.J.Mod.Phys. E26, 1730001 (2017) Relativistic effects and three-nucleon forces in nuclear matter and nuclei NUCLEAR STRUCTURE 208Pb, 48Ca, 25O, 40Mg; calculated binding energy. NUCLEAR REACTIONS 12C, 40Ca, 27Al, 56Fe, 98Mo, 208Pb(n, n), E<30 MeV; calculated θ(θ). Comparison with available data.
doi: 10.1142/S0218301317300016
2016MA88 Sci. Rep. 5, 17712 (2016) Z.-C.Ma, Q.-D.Chen, B.Han, X.-Q.Liu, J.-F.Song, H.-B.Sun Measurement of Two-Photon Absorption Cross Section of Metal Ions by a Mass Sedimentation Approach
doi: 10.1038/srep17712
2016XU07 Phys.Rev. C 94, 034606 (2016) R.Xu, Z.Ma, Y.Zhang, Y.Tian, E.N.E.van Dalen, H.Muther Global analysis of isospin dependent microscopic nucleon-nucleus optical potentials in a Dirac-Brueckner-Hartree-Fock approach NUCLEAR REACTIONS 40Ca(n, n), E=2.06-185.0 MeV; 208Pb(n, n), E=1.8-155.0 MeV; 12C(n, n), E=1.04-225.0 MeV; 56Fe(n, n), E=1.8-75.0 MeV; 98Mo(n, n), E=1.5-26.0 MeV; 103Rh(n, n), E=4.51-10.0 MeV; 28Si, 90Zr, 120Sn(n, n), E=65 MeV; 27Al(n, n), E=3.2-26.0 MeV; 40Ca, 56Fe(p, p), E=61.5, 65 MeV; 28Si(p, p), E=14.26-250.0 MeV; 58Ni(p, p), E=7.0-250.0 MeV; 90Zr(p, p), E=9.7-185.0 MeV; 208Pb(p, p), E=16.0-201.0 MeV; calculated σ(θ, E). 12C, 40Ca(polarized n, n), E=10.9 MeV; 58Ni(polarized n, n), E=9.92 MeV; 208Pb(polarized n, n), E=9.97 MeV; 56Fe(polarized p, p), E=16.0-65.0 MeV; 58Ni(polarized p, p), E=16.0-250.0 MeV; 208Pb(polarized p, p), E=80, 200 MeV; calculated analyzing powers Ay(θ, E). 12C, 56Fe, 208Pb(n, X), 40Ca, 120Sn, 208Pb(p, X), E<200 MeV; calculated reaction σ(E). Global analysis of the isospin dependent nucleon-nucleus microscopic optical potential (MOP) based on the DBHF calculation in symmetric and asymmetric nuclear matter; deduced relativistic MOP for nucleon-nucleus scattering. Comparisons with experimental data, and with results from phenomenological Koning-Delaroche global potential. Compiled bibliographic information for experimental (n, n) data for 12C, 14N, 16O, 23Na, 24Mg, 27Al, 28Si, 31P, 32S, 39K, 40Ca, 48Ti, 52Cr, 55Mn, 56Fe, 59Co, 58Ni, 63Cu, 80Se, 88Sr, 89Y, 90Zr, 93Nb, 98Mo, 103Rh, 115In, 120Sn, 197Au, 208Pb, 209Bi targets, and experimental (p, p) data for 12C, 27Al, 28Si, 40Ca, 56Fe, 58Ni, 90Zr, 120Sn, 208Pb targets.
doi: 10.1103/PhysRevC.94.034606
2015ZH31 Nucl.Phys. A942, 54 (2015) J.-Q.Zhu, Z.-L.Ma, C.-Y.Shi, Y.-D.Li Thermal single-gluon exchange potential for heavy quarkonium in the static limit
doi: 10.1016/j.nuclphysa.2015.07.017
2015ZH43 Phys.Rev. C 92, 054907 (2015) J.-Q.Zhu, Z.-L.Ma, C.-Y.Shi, Y.-D.Li Inelastic heavy quark and quarkonium ultra-incoherent photoproduction in ultra-peripheral collisions
doi: 10.1103/PhysRevC.92.054907
2013YA23 Chin.Phys.C 37, 124102 (2013) Collective multipole excitations of exotic nuclei in relativistic continuum random phase approximation NUCLEAR STRUCTURE 34,40,48,60Ca, 16,28O, 100,132Sn; calculated isoscalar and isovector collective multipole excitations, strength functions. Comparison with available data.
doi: 10.1088/1674-1137/37/12/124102
2012KO36 Phys.Rev.Lett. 109, 172501 (2012) R.L.Kozub, G.Arbanas, A.S.Adekola, D.W.Bardayan, J.C.Blackmon, K.Y.Chae, K.A.Chipps, J.A.Cizewski, L.Erikson, R.Hatarik, W.R.Hix, K.L.Jones, W.Krolas, J.F.Liang, Z.Ma, C.Matei, B.H.Moazen, C.D.Nesaraja, S.D.Pain, D.Shapira, J.F.Shriner, Jr., M.S.Smith, T.P.Swan Neutron Single Particle Structure in 131Sn and Direct Neutron Capture Cross Sections NUCLEAR REACTIONS 2H(130Sn, p), E=630 MeV; 130Sn(n, γ), E<5 MeV;measured reaction products, Ep, Ip; deduced σ(θ), energy levels, J, π, properties of single-particle states, direct-semidirect σ. Comparison with available data.
doi: 10.1103/PhysRevLett.109.172501
2012XU03 Phys.Rev. C 85, 034613 (2012) R.Xu, Z.Ma, E.N.E.van Dalen, H.Muther Relativistic nucleon optical potentials with isospin dependence in a Dirac-Brueckner-Hartree-Fock approach NUCLEAR REACTIONS 27Al(n, n), (p, p), E=0.1-250 MeV; calculated Schrodinger equivalent central potential, spin-orbit, and Darwin potentials as function of incident energy and deformation parameter, σ(θ, E), vector analyzing powers. Relativistic microscopical optical potential (RMOP) method in the framework of Dirac-Brueckner-Hartree-Fock (DBHF). Comparison with experimental data.
doi: 10.1103/PhysRevC.85.034613
2011AD05 Phys.Rev. C 83, 052801 (2011) A.S.Adekola, D.W.Bardayan, J.C.Blackmon, C.R.Brune, K.Y.Chae, C.Domizioli, U.Greife, Z.Heinen, M.J.Hornish, K.L.Jones, R.L.Kozub, R.J.Livesay, Z.Ma, T.N.Massey, B.Moazen, C.D.Nesaraja, S.D.Pain, J.F.Shriner Jr, N.D.Smith, M.S.Smith, J.S.Thomas, D.W.Visser, A.V.Voinov First proton-transfer study of 18F + p resonances relevant for novae NUCLEAR REACTIONS 2H(18F, n), E=150 MeV; measured α- and 15O-particle spectra. α(15O)-coin, σ(θ), DWBA analysis. 19Ne; deduced levels, J, π, L-transfers, resonances, proton and α-widths. 19Ne-19F mirror symmetry. 18F(p, α)15O; deduced reaction rates. Relevance to nova nucleosynthesis of 18F.
doi: 10.1103/PhysRevC.83.052801
2011AD24 Phys.Rev. C 84, 054611 (2011) A.S.Adekola, C.R.Brune, D.W.Bardayan, J.C.Blackmon, K.Y.Chae, C.Domizioli, U.Greife, Z.Heinen, M.J.Hornish, K.L.Jones, R.L.Kozub, R.J.Livesay, Z.Ma, T.N.Massey, B.Moazen, C.D.Nesaraja, S.D.Pain, J.F.Shriner, Jr., N.D.Smith, M.S.Smith, J.S.Thomas, D.W.Visser, A.V.Voinov Single-nucleon transfer reactions on 18F NUCLEAR REACTIONS 2H(18F, n)19Ne, (18F, p)19F, [secondary 18F beam from 16O(α, np)18F, E=85 MeV primary reaction], E=150 MeV; measured particle spectra, (15O)α-, (15N)α-coin, σ(θ), proton. 19F, 19Ne; deduced levels, J, π, l-values, spectroscopic factors, proton widths, asymptotic normalization coefficients, isospin mirror levels. DWBA analysis of σ(θ) data. Monte-Carlo simulations. Comparison with previous studies.
doi: 10.1103/PhysRevC.84.054611
2011JO08 Phys.Rev. C 84, 034601 (2011) K.L.Jones, F.M.Nunes, A.S.Adekola, D.W.Bardayan, J.C.Blackmon, K.Y.Chae, K.A.Chipps, J.A.Cizewski, L.Erikson, C.Harlin, R.Hatarik, R.Kapler, R.L.Kozub, J.F.Liang, R.Livesay, Z.Ma, B.Moazen, C.D.Nesaraja, S.D.Pain, N.P.Patterson, D.Shapira, J.F.Shriner Jr, M.S.Smith, T.P.Swan, J.S.Thomas Direct reaction measurements with a 132Sn radioactive ion beam NUCLEAR REACTIONS 2H(132Sn, p), (132Sn, d), E=630 MeV; measured Ep, Ip, Ed, Id, elastic σ, σ(θ), DWBA analysis. 133Sn; deduced levels, J, π, l values, spectroscopic factors, configurations, asymptotic normalization coefficients. 132Sn; deduced ground-state configuration and structure. Level systematics of N=83 nuclei 133Sn, 135Te, 137Xe, 139Ba, 141Ce, 143Nd and 145Sm.
doi: 10.1103/PhysRevC.84.034601
2011RU13 J.Korean Phys.Soc. 59, 1729s (2011) X.C.Ruan, G.C.Chen, H.X.Huang, X.Li, Y.B.Nie, B.Zhou, Z.Y.Ma, J.Bao, Q.P.Zhong, Z.Y.Zhou, H.Q.Tang, J.S.Zhang, C.L.Lan, Y.L.Zhang, Y.M.Li Measurement of the Secondary Neutron Emission Differential and Double-Differential Cross Sections between 20 and 30 MeV NUCLEAR REACTIONS 9Be(n, n), (n, xn), E=21.65 MeV; measured In, En using TOF and BC501A; deduced σ, σ(θ), σ(E, θ); calculated TOF neutron spectra using Monte Carlo code STREUER, σ by LUNF code. Compared with other data.
doi: 10.3938/jkps.59.1729
2010JO03 Nature(London) 465, 454 (2010) K.L.Jones, A.S.Adekola, D.W.Bardayan, J.C.Blackmon, K.Y.Chae, K.A.Chipps, J.A.Cizewski, L.Erikson, C.Harlin, R.Hatarik, R.Kapler, R.L.Kozub, J.F.Liang, R.Livesay, Z.Ma, B.H.Moazen, C.D.Nesaraja, F.M.Nunes, S.D.Pain, N.P.Patterson, D.Shapira, J.F.Shriner Jr, M.S.Smith, T.P.Swan, J.S.Thomas The magic nature of 132Sn explored through the single-particle states of 133Sn NUCLEAR REACTIONS 2H(132Sn, p)133Sn, E=630 MeV; measured Ep, Ip;132Sn; deduced proton σ(θ), Q-value spectrum, properties of single-particle states in 133Sn, magic nature of 132Sn, spectroscopic factors and configurations . DWBA and FRESCO calculations, U(p, F) fission secondary beams.
doi: 10.1038/nature09048
2010MA35 Nucl.Phys. A834, 50c (2010) Density functional theory with a separable pairing force in finite nuclei NUCLEAR STRUCTURE 102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136Sn; calculated E2, B(E2), pairing gap using separable and Gogny D1S forces. 128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188Sm; calculated deformation using RMF+BCS, HFB, RHB (relativistic Hartree-Bogoliubov). Comparison with data.
doi: 10.1016/j.nuclphysa.2010.01.015
2010NI06 Phys.Rev. C 81, 054318 (2010) T.Niksic, P.Ring, D.Vretenar, Y.Tian, Z.-y.Ma 3D relativistic Hartree-Bogoliubov model with a separable pairing interaction: Triaxial ground-state shapes NUCLEAR STRUCTURE 134,136,138,140,142,144,146,148,150,152,154,156Sm, 190,192,194,196,198,200Pt; calculated triaxial quadrupole binding-energy contour maps, neutron and proton pairing energy maps in β-γ plane, quadrupole deformations. 192Pt; calculated proton and neutron canonical single-particle energy levels. Relativistic Hartree-Bogoliubov (RHB) model.
doi: 10.1103/PhysRevC.81.054318
2010NI11 Ann.Nucl.Energy 37, 1456 (2010) Y.Nie, J.Bao, X.Ruan, H.Huang, X.Li, Q.Zhong, B.Zhou, Z.Ma, Y.Zhang, Z.Zhou Benchmarking of evaluated nuclear data for uranium by a 14.8 MeV neutron leakage spectra experiment with slab sample
doi: 10.1016/j.anucene.2010.06.018
2010YA20 Phys.Rev. C 82, 054305 (2010) D.Yang, L.-G.Cao, Y.Tian, Z.-Y.Ma Importance of self-consistency in relativistic continuum random-phase approximation calculations NUCLEAR STRUCTURE 40Ca, 132Sn, 208Pb; calculated inverse energy-weighted moments and strength distributions of isoscalar giant-monopole resonances (ISGMR), isovector giant-monopole resonances (IVGMR), isoscalar giant-quadrupole resonances (ISGQR), isovector giant-quadrupole resonances (IVGQR) using relativistic continuum random phase approximation (RCRPA) method.
doi: 10.1103/PhysRevC.82.054305
2010ZH11 Phys.Rev. C 81, 044319 (2010) D.-D.Zhang, Z.-Y.Ma, B.-Q.Chen, S.-F.Shen α-decay half-lives of superheavy elements with the Dirac-Brueckner-Hartree-Fock (DBHF) nucleon effective interaction RADIOACTIVITY 261,263Sg, 264,267,272Bh, 264,265,275Hs, 268Mt, 270,279,281Ds, 272Rg, 283,285Cn, 283,284Nh, 286,287,288,289Fl, 287,288Mc, 290,291,292,293Lv, 294Og; calculated half-lives using microscopic NN effective interaction based on the Dirac-Brueckner-Hartree-Fock (DBHF) approach and the M3Y effective interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.044319
2010ZH19 Chin.Phys.C 34, 334 (2010) D.-D.Zhang, B.-Q.Chen, Z.-Y.Ma Systematic studies on α-decay half-lives for super heavy nuclei NUCLEAR STRUCTURE Z=102-120; calculated T1/2; deduced nucleus-nucleus potential. Performed cluster model (PCM).
doi: 10.1088/1674-1137/34/3/006
2010ZO02 Chin.Phys.C 34, 56 (2010) W.-H.Zou, Y.Tian, S.-F.Shen, J.-Z.Gu, B.-B.Peng, D.-D.Zhang, Z.-Y.Ma Nuclear structure around 80Zr NUCLEAR STRUCTURE 80,82,84Zr; calculated potential energy surfaces, ground state bands. Projected shell model (PSM) and relativistic Hartee-Bogoliubov (RHB) theory.
doi: 10.1088/1674-1137/34/1/010
2010ZO03 Phys.Rev. C 82, 024309 (2010) W.-h.Zou, Y.Tian, J.-z.Gu, S.-f.Shen, J.-m.Yao, B.-b.Peng, Z.-y.Ma Microscopic description of nuclear structure around 80Zr NUCLEAR STRUCTURE 80,82,84Zr; calculated ground-state total binding energies and angular momentum projected potential energy surfaces (AMPPES) using projected shell model with a quadrupole constrained relativistic Hartree-Bogoliubov (RHB) theory and NL3 effective interaction and Gogny D1S interaction for the pairing force. Shape coexistence and shape transitions, and decay out of superdeformed rotational bands.
doi: 10.1103/PhysRevC.82.024309
2009DO20 Chin.Phys.C 33, 532 (2009) Elastic scattering of 6He from 12C at 38.3 MeV/nucleon NUCLEAR REACTIONS 12C(6He, 6He), E=38.3 MeV/nucleon; analyzed elastic scattering data within standard optical model; calculated σ(θ). Comparison with theoretical models and experimental data.
doi: 10.1088/1674-1137/33/7/006
2009TI03 Phys.Lett. B 676, 44 (2009) A finite range pairing force for density functional theory in superfluid nuclei NUCLEAR STRUCTURE Sn, Pb; calculated pairing energy and associated matrix elements using the relativistic Hartree?Bogoliubov approach.
doi: 10.1016/j.physletb.2009.04.067
2009TI04 Phys.Rev. C 79, 064301 (2009) Separable pairing force for relativistic quasiparticle random-phase approximation NUCLEAR STRUCTURE 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136Sn, 122Zr, 124Mo, 126Ru, 128Pd, 130Cd, 132Sn, 134Te, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm, 146Gd, 148Dy, 150Er, 152Yb; calculated energies of first 2+, first and second 3-, B(E2), proton average gap, and isoscalar giant monopole resonance (ISGMR) using Relativistic Hartree-Bogoliubov (RHB) and relativistic quasiparticle random phase approximation (RQRPA). Comparison with experimental data.
doi: 10.1103/PhysRevC.79.064301
2009TI07 Phys.Rev. C 80, 024313 (2009) Axially deformed relativistic Hartree Bogoliubov theory with a separable pairing force NUCLEAR STRUCTURE 164Er, 128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188Sm, 240Pu; calculated binding energies, neutron and proton pairing energies using axially symmetric relativistic Hartree-Bogoliubov calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.024313
2009YA02 Chin.Phys.Lett. 26, 022101 (2009) Isoscalar Giant Monopole Resonance in Relativistic Continuum Random Phase Approximation NUCLEAR STRUCTURE 120Sn, 208Pb; calculated Isoscalar Giant Monopole resonance strength in the framework of relativistic continuum random phase approximation.
doi: 10.1088/0256-307X/26/2/022101
2008CA10 Chin.Phys.Lett. 25, 1625 (2008) Symmetry Energy and Isovector Giant Dipole Resonance in Finite Nuclei NUCLEAR STRUCTURE 90Zr, 132Sn, 144Sm, 208Pb; calculated IVGDR energies as a function of symmetry energy using relativistic mean field theory.
doi: 10.1088/0256-307X/25/5/028
2008ZO01 Phys.Rev. C 77, 014314 (2008) W.Zou, G.Colo, Z.Ma, H.Sagawa, P.F.Bortignon Tensor correlations and evolution of single-particle energies in medium-mass nuclei NUCLEAR STRUCTURE 40,42,44,46,48Ca; calculated energy differences between states. 46Ar, 48Ca; calculated spin-orbit splittings, single particle energies using Skyrme model with tensor forces. Compared with experiment and with Skyrme model without tensor force.
doi: 10.1103/PhysRevC.77.014314
2008ZO03 Phys.Rev. C 78, 064613 (2008) Microscopic optical potential for α-nucleus elastic scattering in a Dirac-Brueckner-Hartree-Fock approach NUCLEAR REACTIONS 12C(α, α), E=104, 120, 145, 166, 172.5 MeV; 16O(α, α), E=48.7, 54.1, 69.5, 80.7, 104 MeV; 28Si(α, α), E=104, 166, 240 MeV; 40Ca(α, α), E=40.05, 47, 53.9, 80, 104, 141.7 MeV; calculated density dependence of optical model potentials, normalization factors, σ(θ). DBHF calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.78.064613
2007BA69 Phys.Rev. C 76, 045803 (2007) D.W.Bardayan, J.C.Blackmon, R.P.Fitzgerald, W.R.Hix, K.L.Jones, R.L.Kozub, J.F.Liang, R.J.Livesay, Z.Ma, L.F.Roberts, M.S.Smith, J.S.Thomas, D.W.Visser 30S studied with the 32S(p, t)30S reaction and the 29P(p, γ)30S reaction rate NUCLEAR REACTIONS 32S(p, t), E=37 MeV; measured triton energies, angular distributions. 30S deduced levels, J, π. 29P(p, γ)30S; deduced reaction rates of astrophysical significance.
doi: 10.1103/PhysRevC.76.045803
2007GR21 Phys.Rev. C 76, 044319 (2007) M.Grasso, Z.Y.Ma, E.Khan, J.Margueron, N.Van Giai Evolution of the proton sd states in neutron-rich Ca isotopes NUCLEAR STRUCTURE 48,52,70,78Ca; calculated excitation energies. Skyrme-Hartree-Fock equations used.
doi: 10.1103/PhysRevC.76.044319
2007JO09 Acta Phys.Pol. B38, 1205 (2007) K.L.Jones, A.S.Adekola, D.W.Bardayan, J.C.Blackmon, K.Y.Chae, K.Chipps, J.A.Cizewski, D.J.Dean, L.Erikson, R.P.Fitzgerald, A.L.Gaddis, U.Greife, C.Harlin, R.Hatarik, J.A.Howard, M.S.Johnson, R.L.Kozub, J.F.Liang, R.J.Livesay, Z.Ma, B.H.Moazen, P.D.O'Malley, C.D.Nesaraja, S.D.Pain, N.P.Patterson, S.V.Paulauskas, D.Shapira, J.F.Shriner Jr, D.J.Sissom, M.S.Smith, T.P.Swan, J.S.Thomas Single Neutron Transfer Experiments Close to the r-Process Path NUCLEAR REACTIONS 2H(82Ge, p), E=4 MeV/nucleon; 2H(84Se, p), E=4.5 MeV/nucleon; 2H(132Sn, p), E=4.77 MeV/nucleon; measured Ep and angular distributions. 83Ge, 85Se, 133Sn deduced levels, J, π and spectroscopic factors. Compared results to model calculations.
2007LI26 Phys.Rev. C 75, 054320 (2007) Pygmy and giant dipole resonances in Ni isotopes NUCLEAR STRUCTURE Ni; calculated properties of the isovector giant and pigmy dipole resonances for even-even Ni isotopes within the framework of a relativistic random phase approximation built on a relativistic mean field ground state.
doi: 10.1103/PhysRevC.75.054320
2007MA02 Chin.Phys.Lett. 24, 69 (2007) Influence of D-state in 4He on S Factor for the 2H(d, γ)4He Reaction NUCLEAR REACTIONS 2H(d, γ), E(cm)=10-1000 keV; calculated astrophysical S-factors; deduced sensitivity to 4He D-state.
doi: 10.1088/0256-307X/24/1/019
2007MA48 Phys.Rev. C 76, 015803 (2007); Erratum Phys.Rev. C 76, 039901 (2007) Z.Ma, D.W.Bardayan, J.C.Blackmon, R.P.Fitzgerald, M.W.Guidry, W.R.Hix, K.L.Jones, R.L.Kozub, R.J.Livesay, M.S.Smith, J.S.Thomas, D.W.Visser Astrophysically important 31S states studied with the 32S(p, d)31S reaction NUCLEAR REACTIONS 32S(p, d), E=32 MeV; measured Ed, σ and angular distributions. 31S deduced level energies and spectroscopic factors.
doi: 10.1103/PhysRevC.76.015803
2007TH15 Phys.Rev. C 76, 044302 (2007) J.S.Thomas, G.Arbanas, D.W.Bardayan, J.C.Blackmon, J.A.Cizewski, D.J.Dean, R.P.Fitzgerald, U.Greife, C.J.Gross, M.S.Johnson, K.L.Jones, R.L.Kozub, J.F.Liang, R.J.Livesay, Z.Ma, B.H.Moazen, C.D.Nesaraja, D.Shapira, M.S.Smith, D.W.Visser Single-neutron excitations in neutron-rich 83Ge and 85Se NUCLEAR REACTIONS 2H(82Ge, p), (84Se, p), E=330, 380 MeV; measured Ep, Ip, recoil-proton-coin, angular distributions; deduced asymptotic normalization coefficients, spectroscopic factors. 83Ge, 85Se; deduced levels, J, π, angular momentum using DWBA analysis. 82Ge, 84Se(n, γ), E=0-1 MeV; calculated cross sections.
doi: 10.1103/PhysRevC.76.044302
2006CH30 Phys.Rev. C 74, 012801 (2006) K.Y.Chae, D.W.Bardayan, J.C.Blackmon, D.Gregory, M.W.Guidry, M.S.Johnson, R.L.Kozub, R.J.Livesay, Z.Ma, C.D.Nesaraja, S.D.Pain, S.Paulauskas, M.Porter-Peden, J.F.Shriner, Jr., N.Smith, M.S.Smith, J.S.Thomas First experimental constraints on the interference of (3/2)+ resonances in the 18F(p, α)15O reaction NUCLEAR REACTIONS 1H(18F, α), E(cm) ≈ 663-877 keV; measured particle spectra, excitation functions; deduced resonance interference effects. 19Ne deduced upper limits on resonance widths. R-matrix calculations.
doi: 10.1103/PhysRevC.74.012801
2006KO13 Phys.Rev. C 73, 044307 (2006) R.L.Kozub, D.W.Bardayan, J.C.Batchelder, J.C.Blackmon, C.R.Brune, A.E.Champagne, J.A.Cizewski, U.Greife, C.J.Gross, C.C.Jewett, R.J.Livesay, Z.Ma, B.H.Moazen, C.D.Nesaraja, L.Sahin, J.P.Scott, D.Shapira, M.S.Smith, J.S.Thomas Neutron single particle strengths from the (d, p) reaction on 18F NUCLEAR REACTIONS 2H(18F, p), E=108.5 MeV; measured Ep, σ(E, θ). 19F deduced levels, J, π, neutron spectroscopic factors. Finite-range DWBA analysis. Comparison with shell model predictions. Daresbury recoil separator.
doi: 10.1103/PhysRevC.73.044307
2006LI30 Chin.Phys.Lett. 23, 1719 (2006) Ground-State Properties of Ca Isotopes and the Density Dependence of the Symmetry Energy NUCLEAR STRUCTURE 52,54,60,70Ca; calculated neutron and proton density distributions, radii, single-particle energies. Relativistic mean field approach.
doi: 10.1088/0256-307X/23/7/018
2006MA10 Chin.Phys.Lett. 23, 568 (2006) Tetraquarks Production in Quark-Gluon Plasma with Diquarks
doi: 10.1088/0256-307X/23/3/012
2006MA82 Int.J.Mod.Phys. E15, 1347 (2006) Z.-Yu.Ma, B.-Q.Chen, J.Liang, L.-G.Cao Giant resonances and asymmetry energy NUCLEAR STRUCTURE 70,72,74,76,78,80,82,84,86,88,90,92,94,96Ni; calculated GDR energies. 132Sn, 208Pb; calculated asymmetry energy, giant resonance strength. Relativistic quasiparticle RPA.
doi: 10.1142/S0218301306004934
2006RO03 Phys.Rev. C 73, 014614 (2006) Isospin-dependent optical potentials in Dirac-Brueckner-Hartree-Fock approach NUCLEAR REACTIONS 40Ca, 208Pb(p, p), E=10-200 MeV; calculated σ(θ), Ay(θ), spin-rotation functions. Relativistic microscopic optical model, comparison with data.
doi: 10.1103/PhysRevC.73.014614
2006TI10 Chin.Phys.Lett. 23, 3226 (2006) A Separable Pairing Force in Nuclear Matter
doi: 10.1088/0256-307X/23/12/029
2006ZH15 Chin.Phys.Lett. 23, 1723 (2006) H.-F.Zhang, W.Zuo, J.-Q.Li, S.Im, Z.-Yu.Ma, B.-Q.Chen Anomaly in the Charge Radii and Nuclear Structure NUCLEAR STRUCTURE A=118-150; calculated isotope shifts, radii, quadrupole deformations for Pr isotopes. 139,140,141,142Pr; calculated single-particle energy levels, proton and neutron density distributions. Relativistic mean field approach.
doi: 10.1088/0256-307X/23/7/019
2006ZH16 Chin.Phys.Lett. 23, 1734 (2006) H.-F.Zhang, J.-Q.Li, W.Zuo, B.-Q.Chen, Z.-Yu.Ma, S.Im, G.Royer Alpha Decay Half-Lives of New Superheavy Elements through Quasimolecular Shapes RADIOACTIVITY 294Og, 290,291,292,293Lv, 286,287,288,289Fl, 283,285Cn, 279Ds, 275Hs, 271Sg(α); calculated T1/2. WKB approximation, comparison with data and other models.
doi: 10.1088/0256-307X/23/7/022
2006ZH41 Eur.Phys.J. A 30, 519 (2006) H.Zhang, S.Im, J.Li, W.Zuo, Z.Ma, B.Chen, W.Scheid Improved BCS-type pairing for the relativistic mean-field theory NUCLEAR STRUCTURE 74,76,78,80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136Sr; calculated neutron and proton shell gaps, total energy per nucleon, quadrupole deformation, isotope shifts, shape coexistence, two-neutron separation energies. Relativistic mean-field theory, density-dependent δ interaction.
doi: 10.1140/epja/i2006-10147-0
2005BA82 Nucl.Phys. A758, 737c (2005) D.W.Bardayan, J.C.Blackmon, J.Gomez del Campo, R.L.Kozub, J.F.Liang, Z.Ma, L.Sahin, D.Shapira, M.S.Smith New 19Ne Level Observed with a Thick Target 18F(p, p)18F Measurement NUCLEAR REACTIONS 1H(18F, p), E(cm) ≈ 0.3-1.3 MeV; measured proton spectra, σ(θ), excitation functions. 19Ne deduced resonance parameters, excited state energy, J, π. 18F(p, α), (p, γ), E=low; calculated astrophysical reaction rates.
doi: 10.1016/j.nuclphysa.2005.05.133
2005BB05 Eur.Phys.J. A 25, Supplement 1, 643 (2005) D.W.Bardayan, J.C.Blackmon, J.Gomez del Campo, R.L.Kozub, J.F.Liang, Z.Ma, D.Shapira, L.Sahin, M.S.Smith New 19Ne resonance observed using an exotic 18F beam NUCLEAR REACTIONS 1H(18F, p), E(cm) ≈ 0.3-1.3 MeV; measured Ep, σ(θ); deduced excitation functions. 19Ne deduced resonance energies, J, π, analog states. 18F(p, α), (p, γ), E=low; calculated astrophysical reaction rates.
doi: 10.1140/epjad/i2005-06-007-3
2005CA15 Phys.Rev. C 71, 034305 (2005) Low-lying dipole modes in 26, 28Ne in the quasiparticle relativistic random phase approximation NUCLEAR STRUCTURE 26,28Ne; calculated isovector dipole strength distributions, resonance features. Quasiparticle relativistic RPA.
doi: 10.1103/PhysRevC.71.034305
2005CH09 Chin.Phys.Lett. 22, 302 (2005) B.-Q.Chen, Z.Yu.Ma, Z.-Y.Zhu, H.-Q.Song, Y.-L.Zhao Deformed Potential Energy of Super Heavy Element Z = 120 in a Generalized Liquid Drop Model NUCLEAR REACTIONS 244Pu(58Fe, X), 208Pb(88Sr, X), (94Sr, X), 166Dy(136Xe, X), 252Fm(50Ca, X), E not given; calculated deformed potential energies for fusion reactions. Generalized liquid drop model.
doi: 10.1088/0256-307X/22/2/010
2005CI07 Nucl.Instrum.Methods Phys.Res. B241, 200 (2005) J.A.Cizewski, K.L.Jones, S.D.Pain, J.S.Thomas, C.Baktash, D.W.Bardayan, J.C.Blackmon, C.Gross, J.F.Liang, D.Shapira, M.S.Smith, R.L.Kozub, B.H.Moazen, C.D.Nesaraja, H.K.Carter, M.S.Johnson, R.P.Fitzgerald, D.W.Visser, U.Greife, R.J.Livesay, W.Catford, Z.Ma Neutron transfer reactions with neutron-rich radioactive ion beams NUCLEAR REACTIONS 2H(82Ge, p), (84Se, p), E=4 MeV/nucleon; measured Ep, σ(θ). 83Ge, 85Se deduced ground and excited states energies, J, π.
doi: 10.1016/j.nimb.2005.07.025
2005FI01 Nucl.Phys. A748, 351 (2005) R.Fitzgerald, E.Abbotoy, D.W.Bardayan, J.C.Blackmon, A.E.Champagne, A.A.Chen, U.Greife, D.W.Hill, A.N.James, R.L.Kozub, T.A.Lewis, R.Livesay, Z.Ma, S.L.Mahan, J.W.McConnell, W.T.Milner, B.H.Moazen, P.D.Parker, D.E.Pierce, M.E.Roettger, L.Sahin, D.Shapira, M.S.Smith, F.Strieder, K.B.Swartz, J.S.Thomas, D.W.Visser Studies of (p, γ) reactions with the Daresbury Recoil Separator at ORNL'S HRIBF NUCLEAR REACTIONS 1H(17O, γ), E=12.5 MeV; measured particle spectra; deduced resonance strength. Recoil separator, other reactions discussed.
doi: 10.1016/j.nuclphysa.2004.09.155
2005JO23 Eur.Phys.J. A 25, Supplement 1, 283 (2005) K.L.Jones, C.Baktash, D.W.Bardayan, J.C.Blackmon, W.N.Catford, J.A.Cizewski, R.P.Fitzgerald, U.Greife, M.S.Johnson, R.L.Kozub, R.J.Livesay, Z.Ma, C.D.Nesaraja, D.Shapira, M.S.Smith, J.S.Thomas, D.Visser Developing techniques to study A ∼ 132 nuclei with (d, p) reactions in inverse kinematics NUCLEAR REACTIONS 2H(124Sn, p), E=4.5 MeV/nucleon; measured σ(θ). 125Sn levels deduced spectroscopic factors. DWBA analysis.
doi: 10.1140/epjad/i2005-06-112-3
2005KO09 Phys.Rev. C 71, 032801 (2005) R.L.Kozub, D.W.Bardayan, J.C.Batchelder, J.C.Blackmon, C.R.Brune, A.E.Champagne, J.A.Cizewski, T.Davinson, U.Greife, C.J.Gross, C.C.Jewett, R.J.Livesay, Z.Ma, B.H.Moazen, C.D.Nesaraja, L.Sahin, J.P.Scott, D.Shapira, M.S.Smith, J.S.Thomas, P.J.Woods New constraints on the 18F(p, α)15O rate in novae from the (d, p) reaction NUCLEAR REACTIONS 2H(18F, p), E=108.5 MeV; measured Ep, σ(θ). 19F levels deduced spectroscopic factors. 19Ne calculated proton resonance widths. 18F(p, γ), (p, α), E=low; deduced astrophysical reaction rates.
doi: 10.1103/PhysRevC.71.032801
2005KO31 Nucl.Phys. A758, 753c (2005) R.L.Kozub, D.W.Bardayan, J.C.Batchelder, J.C.Blackmon, C.R.Brune, A.E.Champagne, J.A.Cizewski, T.Davinson, U.Greife, C.J.Gross, C.C.Jewet, R.J.Livesay, Z.Ma, B.H.Moazen, C.D.Nesaraja, J.P.Scott, L.Sahin, D.Shapira, M.S.Smith, J.S.Thomas, P.J.Woods New Limits for the 18F(p, α)15O Rate in Novae NUCLEAR REACTIONS 2H(18F, p), E=108.49 MeV; measured particle spectra, σ(θ). 19F levels deduced spectroscopic factors. 18F(p, α), E=low; calculated astrophysical reaction rates.
doi: 10.1016/j.nuclphysa.2005.05.135
2005TH03 Phys.Rev. C 71, 021302 (2005) J.S.Thomas, D.W.Bardayan, J.C.Blackmon, J.A.Cizewski, U.Greife, C.J.Gross, M.S.Johnson, K.L.Jones, R.L.Kozub, J.F.Liang, R.J.Livesay, Z.Ma, B.H.Moazen, C.D.Nesaraja, D.Shapira, M.S.Smith First study of the level structure of the r-process nucleus 83Ge NUCLEAR REACTIONS 2H(82Ge, p), E=330 MeV; measured proton spectra, σ(θ), Q value. 83Ge deduced levels, J, π, spectroscopic factors, mass excess.
doi: 10.1103/PhysRevC.71.021302
2005TH09 Nucl.Phys. A758, 663c (2005) J.S.Thomas, D.W.Bardayan, J.C.Blackmon, J.A.Cizewski, R.P.Fitzgerald, U.Greife, C.J.Gross, M.S.Johnson, K.L.Jones, R.L.Kozub, J.F.Liang, R.J.Livesay, Z.Ma, B.H.Moazen, C.D.Nesaraja, D.Shapira, M.S.Smith, D.W.Visser Neutron Single-Particle States in r-Process Nuclei Near Closed Shells NUCLEAR REACTIONS 2H(84Se, p), (124Sn, p), E=4.5 MeV/nucleon; measured recoil proton spectra, σ(E, θ). 85Se, 125Sn deduced levels, J, π.
doi: 10.1016/j.nuclphysa.2005.05.119
2005TH12 Eur.Phys.J. A 25, Supplement 1, 371 (2005) J.S.Thomas, D.W.Bardayan, J.C.Blackmon, J.A.Cizewski, R.P.Fitzgerald, U.Greife, C.J.Gross, M.S.Johnson, K.L.Jones, R.L.Kozub, J.F.Liang, R.J.Livesay, Z.Ma, B.H.Moazen, C.D.Nesaraja, D.Shapira, M.S.Smith, D.W.Visser Single-neutron excitations in neutron-rich N = 51 nuclei NUCLEAR REACTIONS 2H(82Ge, p), E=4 MeV/nucleon; 2H(84Se, p), E=4.5 MeV/nucleon; measured Ep, recoil particle spectrum, proton angular distribution. 83Ge, 85Se deduced levels J, π, spectroscopic factors. DWBA analysis.
doi: 10.1140/epjad/i2005-06-127-8
2005ZH18 Phys.Rev. C 71, 054312 (2005) H.Zhang, J.Li, W.Zuo, Z.Ma, B.Chen, S.Im Properties of the superheavy element 287115 and its α-decay time NUCLEAR STRUCTURE 287Mc, 283Nh, 279Rg, 275Mt, 271Bh; calculated binding energies, β2, single-particle level energies. RADIOACTIVITY 287Mc, 283Nh, 279Rg, 275Mt, 271Bh(α); calculated Qα, T1/2.
doi: 10.1103/PhysRevC.71.054312
2004BA63 Phys.Rev. C 70, 015804 (2004) D.W.Bardayan, J.C.Blackmon, J.Gomez del Campo, R.L.Kozub, J.F.Liang, Z.Ma, L.Sahin, D.Shapira, M.S.Smith Search for astrophysically important 19Ne levels with a thick-target 18F(p, p)18F measurement NUCLEAR REACTIONS 1H(18F, p), E(cm) ≈ 0.3-1.3 MeV; measured Ep; deduced excitation function. 19Ne deduced levels, J, π, widths. Astrophysical implications discussed.
doi: 10.1103/PhysRevC.70.015804
2004BB08 Nucl.Phys. A746, 557c (2004) D.W.Bardayan, J.C.Blackmon, J.Gomez del Campo, R.L.Kozub, J.F.Liang, Z.Ma, D.Shapira, M.S.Smith Studies of the 18F(p, α)15O reaction rate with a 18F beam at the HRIBF NUCLEAR REACTIONS 1H(18F, p), E=0-24 MeV; measured Ep, σ(θ), excitation function. 19Ne deduced resonance width upper limit.
doi: 10.1016/j.nuclphysa.2004.09.089
2004BB10 Nucl.Phys. A746, 593c (2004) D.W.Bardayan, J.C.Blackmon, J.Gomez del Campo, R.L.Kozub, J.F.Liang, Z.Ma, D.Shapira, M.S.Smith Studies of the 18F(p, α) 15O reaction rate with a 18F beam at the HRIBF NUCLEAR REACTIONS 1H(18F, p), E=0-24 MeV; measured Ep, σ(θ), excitation function. 19Ne deduced resonance width upper limit.
doi: 10.1016/j.nuclphysa.2004.09.095
2004CA17 Chin.Phys.Lett. 21, 810 (2004) Isoscalar Giant Resonances of 120Sn in the Quasiparticle Relativistic Random Phase Approximation NUCLEAR STRUCTURE 120Sn; calculated giant resonance response functions. Quasiparticle relativistic RPA.
doi: 10.1088/0256-307X/21/5/013
2004CA44 Eur.Phys.J. A 22, 189 (2004) Effect of resonant continuum on pairing correlations in the relativistic approach NUCLEAR STRUCTURE 68,70,72,74,76,78,80,82,84,86,88,90,92,94,96,98Ni; calculated pairing energies, binding energies, two-neutron separation energies, radii. Relativistic approach, role of resonant continuum discussed.
doi: 10.1140/epja/i2004-10029-5
2004JO19 Phys.Rev. C 70, 067602 (2004) K.L.Jones, R.L.Kozub, C.Baktash, D.W.Bardayan, J.C.Blackmon, W.N.Catford, J.A.Cizewski, R.P.Fitzgerald, M.S.Johnson, R.J.Livesay, Z.Ma, C.D.Nesaraja, D.Shapira, M.S.Smith, J.S.Thomas, D.W.Visser Study of the 124Sn(d, p) reaction in inverse kinematics close to the Coulomb barrier NUCLEAR REACTIONS 2H(124Sn, p), E=562 MeV; measured Ep, σ(θ). 125Sn deduced levels, spectroscopic factors. DWBA analysis. Comparison with previous results.
doi: 10.1103/PhysRevC.70.067602
2004LI19 Phys.Rev. C 69, 034326 (2004) Z.H.Liu, M.Ruan, Y.L.Zhao, H.Q.Zhang, F.Yang, Z.Y.Ma, C.J.Lin, B.Q.Chen, Y.W.Wu, W.L.Zhan, Z.Y.Guo, G.Q.Xiao, H.S.Xu, Z.Y.Sun, J.X.Li, Z.J.Chen Evidence for enhancement of the total reaction cross sections for 27, 28P with a 28Si target and examination of possibly relevant mechanisms NUCLEAR REACTIONS Si(23Na, X), (24Mg, X), (25Mg, X), (25Al, X), (26Al, X), (26Si, X), (27Si, X), (27P, X), (28P, X), E ≈ 20-40 MeV/nucleon; measured reaction σ; deduced reaction mechanism features. Secondary beams from 36Ar fragmentation. Modified Glauber model analysis.
doi: 10.1103/PhysRevC.69.034326
2004LI57 Chin.Phys.Lett. 21, 1711 (2004) Z.-H.Liu, M.Ruan, Y.-L.Zhao, H.-Q.Zhang, F.Yang, Z.-Y.Ma, C.-J.Lin, B.-Q.Chen, Y.-W.Wu, W.-L.Zhan, Z.-Y.Guo, G.-Q.Xiao, H.-S.Xu, Z.-Y.Sun, J.-X.Li, Z.-Q.Chen Possible Experimental Evidence of a Moderate Proton Halo in 29S NUCLEAR REACTIONS 28Si(29Si, X), (27Si, X), (28P, X), (27P, X), E ≈ 40 MeV/nucleon; measured reaction σ. 29S deduced proton halo features. Modified Glauber theory analysis.
doi: 10.1088/0256-307X/21/9/009
2004MA44 Eur.Phys.J. A 20, 429 (2004) Z.-Y.Ma, B.-Q.Chen, N.Van Giai, T.Suzuki The Gamow-Teller resonance in finite nuclei in the relativistic random phase approximation NUCLEAR STRUCTURE 48Ca, 90Zr, 208Pb; calculated Gamow-Teller response functions, resonance energies. Relativistic RPA.
doi: 10.1140/epja/i2003-10167-2
2004MA90 Phys.Lett. B 604, 170 (2004) Z.-Y.Ma, J.Rong, B.-Q.Chen, Z.-Y.Zhu, H.-Q.Song Isospin dependence of nucleon effective mass in Dirac Brueckner-Hartree-Fock approach
doi: 10.1016/j.physletb.2004.11.004
2004SM08 Nucl.Phys. A746, 565c (2004) M.S.Smith, W.R.Hix, S.Parete-Koon, L.Dessieux, Z.Ma, S.Starrfield, D.W.Bardayan, M.W.Guidry, D.L.Smith, J.C.Blackmon, A.Mezzacappa Element synthesis calculations for stellar explosions: robust uncertainties, sensitivities, and radioactive ion beam measurements
doi: 10.1016/j.nuclphysa.2004.09.091
2004SM09 Nucl.Phys. A746, 569c (2004) M.S.Smith, R.A.Meyer, D.W.Bardayan, J.C.Blackmon, K.Chae, M.W.Guidry, W.R.Hix, R.L.Kozub, E.J.Lingerfelt, Z.Ma, J.P.Scott Nuclear data on unstable nuclei for astrophysics
doi: 10.1016/j.nuclphysa.2004.09.092
2004TH12 Nucl.Phys. A746, 178c (2004) J.S.Thomas, D.W.Bardayan, J.C.Blackmon, J.A.Cizewski, U.Greife, C.J.Gross, M.S.Johnson, K.L.Jones, R.L.Kozub, J.F.Liang, R.J.Livesay, Z.Ma, B.H.Moazen, C.D.Nesaraja, D.Shapira, M.S.Smith Studies of the neutron single-particle structure of exotic nuclei at the HRIBF NUCLEAR REACTIONS 2H(82Ge, p), E=4 MeV/nucleon; measured Ep, σ(θ). 83Ge deduced levels.
doi: 10.1016/j.nuclphysa.2004.09.032
2003BA86 Nucl.Phys. A718, 590c (2003) D.W.Bardayan, J.C.Batchelder, J.C.Blackmon, A.E.Champagne, T.Davinson, R.Fitzgerald, W.R.Hix, C.Iliadis, R.L.Kozub, Z.Ma, S.Parete-Koon, P.D.Parker, N.Shu, M.S.Smith, P.J.Woods Measurement of the 18F(p, α)15O Cross Section at Nova Energies NUCLEAR REACTIONS 1H(18F, α), E(cm) ≈ 0.3-0.8 MeV; measured σ; deduced resonance parameters. 18F(p, α), E(cm) ≈ 0.2-1.0 MeV; deduced σ.
doi: 10.1016/S0375-9474(03)00873-X
2003BL11 Nucl.Phys. A718, 127c (2003) J.C.Blackmon, D.W.Bardayan, W.Bradfield-Smith, R.Brummitt, A.E.Champagne, A.A.Chen, T.Davinson, L.Dessieux, M.W.Guidry, K.I.Hahn, G.M.Hale, W.R.Hix, R.L.Kozub, Z.Ma, P.D.Parker, G.Rajbaidya, R.C.Runkle, C.M.Rowland, A.C.Shotter, M.S.Smith, L.A.Van Wormer, D.W.Visser, P.J.Woods The 14O(α, p)17F Reaction Rate NUCLEAR REACTIONS 1H(17F, 17F), (17F, 17F'), (17F, 14O), E(cm) ≈ 1-4 MeV; measured particle spectra. 17F(p, p'), E(cm)=2-2.5 MeV; deduced σ. 14O(α, p), E=low; deduced astrophysical reaction rate. R-matrix analysis.
doi: 10.1016/S0375-9474(03)00689-4
2003CA33 Chin.Phys.Lett. 20, 1459 (2003) Isovector Giant Dipole Resonance of Stable Nuclei in a Consistent Relativistic Random-phase Approximation NUCLEAR STRUCTURE 40Ca, 90Zr, 116Sn, 208Pb; A=10-250; calculated isovector GDR energies. Relativistic RPA, comparisons with data.
doi: 10.1088/0256-307X/20/9/314
2003CH81 Chin.Phys.Lett. 20, 1936 (2003) Deformed Potential Energy of 236Db in a Generalized Liquid Drop Model NUCLEAR REACTIONS 241Am(22Ne, 4n), E not given; calculated potential barrier, shape evolution in cold fusion reaction. Generalized liquid drop model, quasi-molecular shape. NUCLEAR STRUCTURE 263Db calculated deformed potential energy. Generalized liquid drop model, quasi-molecular shape.
doi: 10.1088/0256-307X/20/11/009
2003DO11 Int.J.Mod.Phys. E12, 555 (2003) S.-H.Dong, X.-Y.Gu, Z.-Q.Ma, J.Yu The Klein-Gordon equation with a Coulomb potential in D dimensions
doi: 10.1142/S0218301303001387
2003MA26 Chin.Phys.Lett. 20, 1025 (2003) Gamow-Teller Resonance of 90Zr in a Relativistic Approach NUCLEAR STRUCTURE 90Zr; calculated Gamow-Teller resonance response function. Relativistic RPA approach.
doi: 10.1088/0256-307X/20/7/315
2003MA53 Chin.Phys.Lett. 20, 1691 (2003) Energy Density in Quark-Gluon Plasma
doi: 10.1088/0256-307X/20/10/311
2003MA71 Nucl.Phys. A722, 491c (2003) Z.Ma, L.-G.Cao, Nguyen Van Giai, P.Ring Giant resonances of stable and exotic nuclei in relativistic RPA NUCLEAR STRUCTURE 208Pb, 32,34,40,48,60,70Ca; calculated giant resonance response functions. A=10-240; calculated isovector GDR energies. Relativistic RPA approach.
doi: 10.1016/S0375-9474(03)01414-3
2003MI15 J.Phys.(London) G29, 2187 (2003) Production ratios of strange baryons from QGP with diquarks
doi: 10.1088/0954-3899/29/9/313
2003ZH03 Chin.Phys.Lett. 20, 53 (2003) Y.-L.Zhao, Z.-Y.Ma, B.-Q.Chen, W.-Q.Shen Halo Structure of Nucleus 23Al NUCLEAR REACTIONS 12C(23Al, X), E ≈ 30 MeV/nucleon; calculated reaction σ vs projectile core radius, diffuseness parameter. Glauber model, comparison with data.
doi: 10.1088/0256-307X/20/1/316
2002BB02 Phys.Rev.Lett. 89, 262501 (2002) D.W.Bardayan, J.C.Batchelder, J.C.Blackmon, A.E.Champagne, T.Davinson, R.Fitzgerald, W.R.Hix, C.Iliadis, R.L.Kozub, Z.Ma, S.Parete-Koon, P.D.Parker, N.Shu, M.S.Smith, P.J.Woods Strength of the 18F(p, α)15O Resonance at Ec.m.=330 keV NUCLEAR REACTIONS 1H(18F, α), E(cm)=330 keV; measured Eα, Iα(θ), σ; deduced resonance parameters. 18F(p, α), E=astrophysical; calculated reaction rates.
doi: 10.1103/PhysRevLett.89.262501
2002CA42 Phys.Rev. C66, 024311 (2002) Exploration of resonant continuum and giant resonance in the relativistic approach NUCLEAR STRUCTURE 120Sn; calculated continuum single-particle resonant states energies, widths, wave functions, giant resonance features. Relativistic mean field theory.
doi: 10.1103/PhysRevC.66.024311
2002DO05 Int.J.Mod.Phys. E11, 155 (2002) Algebraic Approach to the Pseudoharmonic Oscillator in 2D
doi: 10.1142/S0218301302000752
2002LI09 Chin.Phys.Lett. 19, 190 (2002) A New Decomposition Approach of Dirac Brueckner Hartree-Fock G Matrix for Asymmetric Nuclear Matter
doi: 10.1088/0256-307X/19/2/315
2002LI36 Phys.Rev. C65, 064305 (2002) Ground-State and Pairing Properties of Pr Isotopes in Relativistic Mean-Field Theory NUCLEAR STRUCTURE Pr; calculated binding energies, quadrupole deformation, isotope shifts, radii, one-nucleon separation energies.
doi: 10.1103/PhysRevC.65.064305
2002MA27 Nucl.Phys. A703, 222 (2002) Z.-Y.Ma, A.Wandelt, V.G.Nguyen, D.Vretenar, P.Ring, L.-G.Cao Collective Multipole Excitations in a Microscopic Relativistic Approach NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 208Pb; calculated giant resonance strength distributions. 208Pb; calculated transitions B(Eλ). Relativistic RPA, comparisons with data.
doi: 10.1016/S0375-9474(01)01598-6
2002MA54 Phys.Rev. C66, 024321 (2002) Effective Dirac Brueckner-Hartree-Fock method for asymmetric nuclear matter and finite nuclei NUCLEAR STRUCTURE 16O, 40,48Ca, 48,56,68Ni, 90Zr, 100,132Sn, 208Pb; calculated binding energies, radii. 16O, 40,48Ca, 48Ni; calculated spin-orbit splitting. Dirac-Brueckner-Hartree-Fock approach.
doi: 10.1103/PhysRevC.66.024321
2001BL06 Nucl.Phys. A688, 142c (2001) J.C.Blackmon, D.W.Bardayan, W.Bradfield-Smith, A.E.Champagne, A.A.Chen, T.Davinson, K.I.Hahn, R.L.Kozub, Z.Ma, P.D.Parker, G.Rajbaidya, R.C.Runkle, C.M.Rowland, A.C.Shotter, M.S.Smith, K.B.Swartz, D.W.Visser, P.J.Woods Determination of the 14O(α, p)17Fg.s. Reaction Rate bt Measurement of the 1H(17F, α)14O Cross Section NUCLEAR REACTIONS 1H(17F, α), (17F, p), E(cm)=2-4 MeV; measured σ(θ), reaction rates. 18Ne deduced resonance widths and strengths, comparison with calculations and earlier data.
doi: 10.1016/S0375-9474(01)00686-8
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