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NSR database version of May 30, 2024.

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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2695. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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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
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2018TI06      Phys.Rev. C 97, 064615 (2018)

Y.Tian, D.Y.Pang, Z.-y.Ma

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
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2017MU07      Int.J.Mod.Phys. E26, 1730001 (2017)

H.Muther, F.Sammarruca, Z.Ma

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
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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
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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
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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
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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
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2013YA23      Chin.Phys.C 37, 124102 (2013)

D.Yang, L.-G.Cao, Z.-Y.Ma

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1953. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2687. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1881. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1857. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32682.


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


2010MA35      Nucl.Phys. A834, 50c (2010)

Z.-y.Ma, Y.Tian, P.Ring

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
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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
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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
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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
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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
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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
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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
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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
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2009DO20      Chin.Phys.C 33, 532 (2009)

H.-F.Dong, Y.-Q.Ma, Z.-Y.Ma

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
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2009TI03      Phys.Lett. B 676, 44 (2009)

Y.Tian, Z.Y.Ma, P.Ring

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
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2009TI04      Phys.Rev. C 79, 064301 (2009)

Y.Tian, Z.-y.Ma, P.Ring

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
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2009TI07      Phys.Rev. C 80, 024313 (2009)

Y.Tian, Z.-y.Ma, P.Ring

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
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2009YA02      Chin.Phys.Lett. 26, 022101 (2009)

D.Yang, L.-G.Cao, Z.-Yu.Ma

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
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2008CA10      Chin.Phys.Lett. 25, 1625 (2008)

Li.-G.Cao, Z.-Y.Ma

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
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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
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2008ZO03      Phys.Rev. C 78, 064613 (2008)

W.Zou, Y.Tian, Z.-Y.Ma

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
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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
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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
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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)

J.Liang, Li-G.Cao, Z.-Yu.Ma

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
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2007MA02      Chin.Phys.Lett. 24, 69 (2007)

Y.-Q.Ma, Y.Tian, Z.-Y.Ma

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
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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
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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
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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
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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
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2006LI30      Chin.Phys.Lett. 23, 1719 (2006)

J.Liang, Z.-Yu.Ma, B.-Q.Chen

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
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2006MA10      Chin.Phys.Lett. 23, 568 (2006)

Z.-B.Ma, C.-S.Gao

Tetraquarks Production in Quark-Gluon Plasma with Diquarks

doi: 10.1088/0256-307X/23/3/012
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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
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2006RO03      Phys.Rev. C 73, 014614 (2006)

J.Rong, Z.-Y.Ma, N.Van Giai

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
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2006TI10      Chin.Phys.Lett. 23, 3226 (2006)

Y.Tian, Z.-Y.Ma

A Separable Pairing Force in Nuclear Matter

doi: 10.1088/0256-307X/23/12/029
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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
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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
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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
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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
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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
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2005CA15      Phys.Rev. C 71, 034305 (2005)

Li-G.Cao, Z.-Y.Ma

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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2004CA17      Chin.Phys.Lett. 21, 810 (2004)

L.-G.Cao, Z.-Y.Ma

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
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2004CA44      Eur.Phys.J. A 22, 189 (2004)

L.-G.Cao, Z.-Yu.Ma

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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2003CA33      Chin.Phys.Lett. 20, 1459 (2003)

L.-G.Cao, Z.-Y.Ma

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
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2003CH81      Chin.Phys.Lett. 20, 1936 (2003)

B.-Q.Chen, Z.-Y.Ma, Y.-L.Zhao

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
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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
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2003MA26      Chin.Phys.Lett. 20, 1025 (2003)

Z.-Y.Ma, B.-Q.Chen

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
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2003MA53      Chin.Phys.Lett. 20, 1691 (2003)

Z.-B.Ma, H.Miao, C.-S.Gao

Energy Density in Quark-Gluon Plasma

doi: 10.1088/0256-307X/20/10/311
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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
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2003MI15      J.Phys.(London) G29, 2187 (2003)

H.Miao, Z.Ma, C.Gao

Production ratios of strange baryons from QGP with diquarks

doi: 10.1088/0954-3899/29/9/313
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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
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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
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2002CA42      Phys.Rev. C66, 024311 (2002)

L.Cao, Z.Ma

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
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2002DO05      Int.J.Mod.Phys. E11, 155 (2002)

S.-D.Dong, Z.-Q.Ma

Algebraic Approach to the Pseudoharmonic Oscillator in 2D

doi: 10.1142/S0218301302000752
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2002LI09      Chin.Phys.Lett. 19, 190 (2002)

L.Liu, Z.-Y.Ma

A New Decomposition Approach of Dirac Brueckner Hartree-Fock G Matrix for Asymmetric Nuclear Matter

doi: 10.1088/0256-307X/19/2/315
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2002LI36      Phys.Rev. C65, 064305 (2002)

J.Li, Z.Ma, B.Chen, Y.Zhou

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
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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
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2002MA54      Phys.Rev. C66, 024321 (2002)

Z.Y.Ma, L.Liu

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
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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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Note: The following list of authors and aliases matches the search parameter Z.Ma: , Z.B.MA, Z.C.MA, Z.G.MA, Z.L.MA, Z.Q.MA, Z.W.MA, Z.Y.MA