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NSR database version of April 26, 2024.

Search: Author = G.Xu

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2013YA06      Phys.Rev. C 87, 044613 (2013), Pub.Note Phys.Rev. C 88, 019901 (2013)

Y.Y.Yang, J.S.Wang, Q.Wang, D.Y.Pang, J.B.Ma, M.R.Huang, J.L.Han, P.Ma, S.L.Jin, Z.Bai, Q.Hu, L.Jin, J.B.Chen, N.Keeley, R.Rusek, R.Wada, S.Mukherjee, Z.Y.Sun, R.F.Chen, X.Y.Zhang, Z.G.Hu, X.H.Yuan, X.G.Cao, Z.G.Xu, S.W.Xu, C.Zhen, Z.Q.Chen, Z.Chen, S.Z.Chen, C.M.Du, L.M.Duan, F.Fu, B.X.Gou, J.Hu, J.J.He, X.G.Lei, S.L.Li, Y.Li, Q.Y.Lin, L.X.Liu, F.D.Shi, S.W.Tang, G.Xu, X.Xu, L.Y.Zhang, X.H.Zhang, W.Zhang, M.H.Zhao, Z.Y.Guo, Y.H.Zhang, H.S.Xu, G.Q.Xiao

Elastic scattering of the proton drip-line nucleus ⁸B off a ^natPb target at 170.3 MeV

NUCLEAR REACTIONS Pb(⁸B, ⁸B), E=170.3 MeV, [secondary ⁸B beam from ⁹Be(¹²C, X), E=54.2 MeV/nucleon primary reaction]; measured reaction products, energy loss, time of flight, magnetic rigidity, σ(θ) at RIBLL-HRIFL facility in Lanzhou. Analysis of σ(θ) data by optical model using a single-folding-type potential, and by continuum discretized coupled-channels (CDCC) method. Effect of breakup-channel couplings. Comparison with previous experimental σ(θ) data for Pb(⁷Be, ⁷Be), E=125 MeV, and ²⁰⁸Pb(⁶Li, ⁶Li), E=99 MeV.

doi: 10.1103/PhysRevC.87.044613
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0085.

2013YA24      Nucl.Instrum.Methods Phys.Res. A 701, 1 (2013)

Y.Y.Yang, J.S.Wang, Q.Wang, J.B.Ma, M.R.Huang, J.L.Han, P.Ma, S.L.Jin, Z.Bai, Q.Hu, L.Jin, J.B.Chen, R.Wada, Z.Y.Sun, R.F.Chen, X.Y.Zhang, Z.G.Hu, X.H.Yuan, X.G.Cao, Z.G.Xu, S.W.Xu, C.Zhen, Z.Q.Chen, Z.Chen, S.Z.Chen, C.M.Du, L.M.Duan, F.Fu, B.X.Gou, J.Hu, J.J.He, X.G.Lei, S.L.Li, Y.Li, Q.Y.Lin, L.X.Liu, F.D.Shi, S.W.Tang, G.Xu, X.Xu, L.Y.Zhang, X.H.Zhang, W.Zhang, M.H.Zhao, Y.H.Zhang, H.S.Xu

A method for the measurement of elastic scattering angular distribution at HIRFL-RIBLL

NUCLEAR REACTIONS Pb(⁷Be, ⁷Be), E=125.3 MeV; measured products, Pb; deduced σ(θ). Data were imported from EXFOR entry S0076.

doi: 10.1016/j.nima.2012.10.088
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0076.

2010FA08      Nucl.Phys. A834, 107c (2010)

P.Fan, D.Yuan, Y.Zheng, Y.Zuo, D.Zhou, X.Wu, Gu.Li, L.Zhu, G.Xu, Q.Fan, X.Zhang, S.Zhu

Experimental and Theoretical Study of Quasi-Particle Alignment in ⁸²Sr

NUCLEAR REACTIONS ⁵⁸Ni(²⁸Si, 4p), E=110 MeV; measured Eγ, Iγ. ⁸²Sr; deduced g factor, rotational bands. Comparison with particle rotor model with Nilsson potential.

doi: 10.1016/j.nuclphysa.2010.01.032
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2010YU03      Chin.Phys.B 19, 062701 (2010)

D.-Q.Yuan, Y.-N.Zheng, Y.Zuo, P.Fan, D.-M.Zhou, X.-G.Wu, L.-H.Zhu, G.-S.Li, G.-J.Xu, Q.-W.Fan, X.-Z.Zhang, S.-Y.Zhu

The g-factors and magnetic rotation in ⁸²Rb

NUCLEAR REACTIONS ⁶⁰Ni(²⁷Al, n4p)⁸²Rb, E=130 MeV; measured Eγ, Iγ, γ-γ-coin.; deduced g factors. Comparison with semiclassical model calculations.

doi: 10.1088/1674-1056/19/6/062701
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2009FA14      Chin.Phys.C 33, Supplement 1, 206 (2009)

P.Fan, D.-Q.Yuan, Y.Zuo, Y.-N.Zheng, D.-M.Zhou, X.-G.Wu, G.-S.Li, L-H.Zhu, G.-J.Xu, Q.-W.Fan, X.-Z.Zhang, S.-Y.Zhu

Proton alignment in ⁸²Sr investigated by g-factor measurements

NUCLEAR REACTIONS ⁵⁸Ni(²⁸Si, 4p)⁸²Sr, E=110 MeV; measured Eγ, Iγ; deduced rotational bands, g factors, proton alignment.

doi: 10.1088/1674-1137/33/S1/066
Citations: PlumX Metrics

2009YU10      Chin.Phys.C 33, Supplement 1, 188 (2009)

D.-Q.Yuan, Y.-N.Zheng, Y.Zuo, P.Fan, D.-M.Zhou, M.Liu, X.-G.Wu, L.-H.Zhu, G.-S.Li, G.-J.Xu, Q.-W.Fan, X.-Z.Zhang, S.-Y.Zhu

Study of magnetic-rotation in ⁸²Rb by g-factor measurements

NUCLEAR REACTIONS ⁶⁰Ni(²⁷Al, n4p)⁸²Rb, E=130 MeV; measured Eγ, Iγ, γ-γ-coin.; deduced magnetic rotational bands, g factors.

doi: 10.1088/1674-1137/33/S1/060
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2009ZH53      Chin.Phys.C 33, Supplement 1, 218 (2009)

D.-M.Zhou, Y.-N.Zheng, X.-Z.Zhang, D.-Q.Yuan, Y.Zuo, P.Fan, Z.-Q.Wang, H.-L.Luo, G.-J.Xu, S.-Y.Zhu

Structure of β-emitting nuclei ²⁹P

RADIOACTIVITY ²⁹P(β⁺) [from ²⁸Si(d, n)²⁹P, E=3 MeV]; measured decay products, β-NMR spectra; deduced magnetic moment, density distribution of protons, neutrons and matter.

doi: 10.1088/1674-1137/33/S1/070
Citations: PlumX Metrics

2008FA05      Nucl.Instrum.Methods Phys.Res. A590, 96 (2008)

Q.Fan, G.Xu

Preparation of multilayer targets for g-factor measurement of rotational levels

doi: 10.1016/j.nima.2008.02.040
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2008HA10      Chin.Phys.Lett. 24, 1251 (2008)

J.-L.Han, Q.Wang, Z.Bai, Y.-C.Dong, S.-L.Li, L.-M.Duan, H.-S.Xu, H.-G.Xu, R.-F.Chen, H.-Y.Wu, Z.-C.Li, X.-Q.Lu, K.Zhao, P.Zhou, J.-C.Liu, G.-J.Xu, Y.K.Sergey

Cross-Correlation of Excitation Functions for Different Fragments and Different Scattering Angles in ²⁷Al(¹⁹F, x)y Reactions

NUCLEAR REACTIONS ²⁷Al(¹⁹F, X), E=110.25-118.75 MeV; measured energies, intensities, σ(θ), excitation functions of projectile like fragments.

doi: 10.1088/0256-307X/25/4/024
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2008YU04      Chin.Phys.Lett. 25, 3617 (2008)

D.-Q.Yuan, P.Fan, Y.-N.Zheng, Y.Zuo, D.-M.Zhou, X.-G.Wu, G.-S.Li, L.-H.Zhu, G.-J.Xu, Q.-W.Fan, X.-Z.Zhang, S.-Y.Zhu

Measurements of g-Factor of Rotational Band States in ⁸²Sr

NUCLEAR REACTIONS ⁵⁸Ni(²⁸Si, 4p), E=110 MeV; measured Eγ, Iγ, γγ-coin. ⁸²Sr; deduced g-factors for positive parity rotational states. Transient magnetic field ion implantation perturbed angular distribution method.

doi: 10.1088/0256-307X/25/10/026
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Data from this article have been entered in the XUNDL database. For more information, click here.

2007YU03      Hyperfine Interactions 180, 49 (2007)

D.Yuan, Y.Zheng, D.Zhou, Y.Zuo, P.Fan, M.Liu, X.Wu, L.Zhu, G.Li, G.Xu, Q.Fan, X.Zhang, S.Zhu

g-Factors of magnetic-rotational states in ⁸⁵Zr

NUCLEAR REACTIONS ⁶⁰Ni(²⁸Si, n2p), E=98 MeV; measured Eγ, Iγ(θ), g-factors for high spin states.

doi: 10.1007/s10751-008-9684-y
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2007ZH03      J.Phys.(London) G34, 523 (2007)

D.Zhou, Y.Zheng, D.Yuan, X.Zhang, Y.Zuo, T.Minamisono, M.Matsuta, M.Fukuda, M.Mihara, C.Zhang, Z.Wang, E.Du, H.Luo, G.Xu, S.Zhu

Quadrupole moment and a proton halo structure in ¹⁷F (I^π = 5/2⁺)

RADIOACTIVITY ¹⁷F(β⁺), (EC) [from ¹⁶O(d, n)]; measured β-NMR spectra from polarized source. ¹⁷F deduced quadrupole moment, halo features.

doi: 10.1088/0954-3899/34/3/010
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2006HA40      Chin.Phys.Lett. 23, 2706 (2006)

J.-L.Han, Q.Wang, Yu.C.Dong, S.-L.Li, L.-M.Duan, H.-S.Xu, H.-G.Xu, R.-F.Chen, Z.Bai, H.-Yu.Wu, Z.-C.Li, X.-Q.Lu, K.Zhao, P.Zhou, J.-C.Liu, G.-J.Xu, Yu.-K.Sergey

Largely Deformed Dinuclear System Formed in ¹⁹F + ²⁷Al Dissipative Collision

NUCLEAR REACTIONS ²⁷Al(¹⁹F, X), E=110.25-118.75; measured fragments charge and angular distributions, excitation functions; deduced dinuclear system features.

doi: 10.1088/0256-307X/23/10/023
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0528.

2005YU04      Chin.Phys.Lett. 22, 1628 (2005)

D.-Q.Yuan, Y.-N.Zheng, D.-M.Zhou, Y.Zuo, E.-P.Du, X.Duan, C.-H.Wang, Q.Luo, X.-G.Wu, G.-S.Li, S.-X.Wen, G.-J.Xu, Z.-C.Gao, Y.-S.Chen, S.-Y.Zhu

Measurements of g-Factor of Rotational Levels in ⁸³Y

NUCLEAR REACTIONS ⁵⁸Ni(²⁸Si, 3p), E=98 MeV; measured Eγ, Iγ(θ, H, t), γγ-coin. ⁸³Y deduced g-factors for rotational band levels. Transient field technique, comparison with cranking model predictions.

doi: 10.1088/0256-307X/22/7/019
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2002BA98      Phys.Rev. C 66, 054901 (2002)

B.B.Back, R.R.Betts, J.Chang, W.C.Chang, C.Y.Chi, Y.Y.Chu, J.B.Cumming, J.C.Dunlop, W.Eldredge, S.Y.Fung, R.Ganz, E.Garcia, A.Gillitzer, G.Heintzelman, W.F.Henning, D.J.Hofman, B.Holzman, J.H.Kang, E.J.Kim, S.Y.Kim, Y.Kwon, D.M.McLeod, A.C.Mignerey, M.Moulson, V.Nanal, C.A.Ogilvie, R.Pak, A.Ruangma, D.E.Russ, R.K.Seto, R.K.Seto, P.J.Stanskas, G.S.F.Stephans, H.Q.Wang, F.L.H.Wolfs, A.H.Wuosmaa, H.Xiang, G.H.Xu, H.B.Yao, C.M.Zou, and the E917 Collaboration

Proton emission in Au+Au collisions at 6, 8, and 10.8 GeV/nucleon

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E=6, 8, 10.8 GeV/nucleon; measured proton yields, transverse mass spectra, rapidity; deduced source features. Thermal source plus longitudinal expansion model.

doi: 10.1103/PhysRevC.66.054901
Citations: PlumX Metrics

2001BA22      J.Phys.(London) G27, 301 (2001)

B.B.Back, R.R.Betts, J.Chang, W.C.Chang, C.Y.Chi, Y.Y.Chu, J.B.Cumming, J.C.Dunlop, W.Eldredge, S.Y.Fung, R.Ganz, E.Garcia, A.Gillitzer, G.Heintzelman, W.Henning, D.J.Hofman, B.Holzman, J.H.Kang, E.J.Kim, S.Y.Kim, Y.Kwon, D.McLeod, A.Mignerey, M.Moulson, V.Nanal, C.A.Ogilvie, R.Pak, A.Ruangma, D.Russ, R.Seto, J.Stanskas, G.S.F.Stephans, H.Wang, F.Wolfs, A.H.Wuosmaa, H.Xiang, G.Xu, H.Yao, C.Zou, for the E917 Collaboration

Strangeness Production in Au + Au Collisions at AGS Energies

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E=6, 8, 10.8 GeV/nucleon; measured proton spectra, rapidity, pion and kaon spectra; deduced strangeness production enhancement relative to pp-collisions.

doi: 10.1088/0954-3899/27/3/307
Citations: PlumX Metrics

2001ZH44      Hyperfine Interactions 136/137, 205 (2001)

S.Y.Zhu, Q.Luo, Y.G.Wang, Z.G.Fan, Y.J.Xu, R.Wang, J.Z.Zhu, G.S.Li, X.A.Liu, X.G.Wu, S.X.Wen, G.J.Xu, Z.C.Gao, X.Z.Zhang, Y.S.Chen, K.Matsuta, M.Fukuda, M.Mihara, T.Minamisono

g-Factor Measurements of Rotational States in ^{84, 86}Zr

NUCLEAR REACTIONS ⁵⁸Ni(²⁸Si, 2p), E=98 MeV; ⁵⁸Ni(³²S, 4p), E=110 MeV; measured Eγ, Iγ(θ, H, t). ^84,86Zr deduced g factors for rotational band states. Transient-field technique.

doi: 10.1023/A:1020532332334
Citations: PlumX Metrics

2000XU06      Nucl.Phys. A675, 337c (2000)

G.Xu, on behalf of the BES Collaboration

The Analysis of Decay Channel J/ψ → γγV(ρ, φ)

doi: 10.1016/S0375-9474(00)00278-5
Citations: PlumX Metrics

2000ZH28      Chin.Phys.Lett. 17, 560 (2000)

S.-Y.Zhu, Q.Luo, G.-S.Li, Z.-G.Fan, Y.-J.Xu, Z.-C.Gao, S.-X.Wen, X.-G.Wu, X.-A.Liu, G.-J.Xu, J.-Z.Zhu, Y.-S.Chen, K.Matsuta, M.Fukuda, M.Mihara, T.Minamisono

Rotational State g-Factors in ⁸⁴Zr

NUCLEAR REACTIONS ⁵⁸Ni(²⁸Si, 2p), E=98 MeV; measured Eγ, Iγ(θ, H, t) in polarized Fe. ⁸⁴Zr deduced rotational band levels g-factors, configurations. Transient field technique.

1999BE73      Nucl.Phys. A661, 661c (1999)

M.J.Bennett, M.Bobrek, J.G.Boissevain, C.L.Britton, J.Chang, R.Conway, R.Cunningham, M.S.Emery, M.N.Ericson, S.-Y.Fung, S.Hahn, H.W.van Hecke, D.Jaffe, J.H.Kang, S.Y.Kim, Y.G.Kim, L.J.Marek, J.A.Moore, J.H.Park, G.Richardson, S.S.Ryu, B.R.Schlei, T.Shiina, J.Simon-Gillo, G.Smith, C.Y.Soon, J.P.Sullivan, Y.Takahashi, G.Xu

The PHENIX Multiplicity and Vertex Detector

doi: 10.1016/S0375-9474(99)85112-4
Citations: PlumX Metrics

1997AH01      Phys.Rev.Lett. 78, 618 (1997)

I.Ahmad, S.M.Austin, B.B.Back, R.R.Betts, F.P.Calaprice, K.C.Chan, A.Chishti, C.Conner, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, S.B.Gazes, A.L.Hallin, T.Happ, D.Henderson, N.I.Kaloskamis, E.Kashy, W.Kutschera, J.Last, C.J.Lister, M.Liu, M.R.Maier, D.J.Mercer, D.Mikolas, P.A.A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.A.Trainor, P.Wilt, J.S.Winfield, M.R.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, G.Xu, A.Young, J.E.Yurkon, and the APEX Collaboration

Search for Monoenergetic Positron Emission from Heavy-Ion Collisions at Coulomb-Barrier Energies

NUCLEAR REACTIONS ¹⁸¹Ta(²³⁸U, X), E=5.95-6.3 MeV/nucleon; ²³²Th(²³⁸U, X), E=5.95 MeV/nucleon; measured positron energy spectra; deduced no structure.

doi: 10.1103/PhysRevLett.78.618
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1997AH04      Phys.Rev. C55, R2755 (1997)

I.Ahmad, S.M.Austin, B.B.Back, R.R.Betts, F.P.Calaprice, K.C.Chan, A.A.Chishti, C.Conner, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, J.S.Greenberg, S.B.Gazes, A.L.Hallin, T.Happ, D.Henderson, N.I.Kaloskamis, E.Kashy, W.Kutschera, J.Last, C.J.Lister, M.Liu, M.R.Maier, D.J.Mercer, D.Mikolas, P.A.A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.A.Trainor, P.Wilt, J.S.Winfield, M.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, G.Xu, A.Young, J.E.Yurkon, and the APEX Collaboration

Internal Pair Conversion in Heavy Nuclei

NUCLEAR REACTIONS ²⁰⁶Pb(²⁰⁶Pb, X), E=5.90 MeV/nucleon; measured e⁺e^--sum energy spectra, Doppler corrected Eγ; deduced internal pair conversion to gamma branching ratio. ²³²Th(²⁰⁸Pb, X), E=5.80 MeV/nucleon; ²³⁸U(²⁰⁸Pb, X), E=5.80 MeV/nucleon; ¹⁸¹Ta(²³⁸U, X), E=5.95 MeV/nucleon; ²³²Th(²³⁸U, X), E=5.90 MeV/nucleon; measured e⁺e^--sum energy, Doppler corrected Eγ; deduced no discrete lines evidence in e⁺e^- spectra. ²³⁸U deduced new levels evidence.

doi: 10.1103/PhysRevC.55.R2755
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1997RE07      Z.Phys. A357, 137 (1997)

Z.Ren, B.Chen, Z.Ma, G.Xu

Level Inversion of N = 9 Isotones in the Relativistic Mean-Field Theory

NUCLEAR STRUCTURE ^16,17O, ^15,16N, ^14,15C, ^13,14B, ^12,13Be; calculated binding energy, nucleon, charge radii, single particle level energies, density distributions in some cases. Relativistic mean-field theory.

doi: 10.1007/s002180050228
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1997RE11      Chin.Phys.Lett. 14, 259 (1997)

Z.-Z.Ren, Z.-Y.Zhu, Y.-H.Cai, Y.-S.Shen, W.-L.Zhan, G.-O.Xu

Ground State Properties of Z = 114 Isotopes in the Relativistic Mean-Field Theory

NUCLEAR STRUCTURE ^{298,296,294,292,290,288,286,284,282,280,278,276,274,272,270}Fl; calculated binding energies, nucleon, matter radii, βp, βn ground-state deformations, two-neutron separation energies. ²⁹⁸Fl; calculated single-particle energies; deduced spherical shell at N=184. Shell model, relativistic mean-field theory.

1996AH07      Nucl.Instrum.Methods Phys.Res. A370, 539 (1996)

I.Ahmad, S.M.Austin, B.B.Back, R.R.Betts, F.P.Calaprice, K.C.Chan, A.Chishti, P.Chowdhury, C.Conner, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, S.B.Gazes, J.S.Greenberg, J.P.Greene, A.L.Hallin, Th.Happ, D.Henderson, N.I.Kaloskamis, E.Kashy, W.Kutschera, J.Last, C.J.Lister, M.Liu, M.R.Maier, D.M.Mercer, D.Mikolas, P.A.A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.A.Trainor, P.Wilt, J.S.Winfield, M.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, G.Xu, A.R.Young, J.E.Yurkon

A Solenoidal Spectrometer for Positron-Electron Pairs Produced in Heavy-Ion Collisions

RADIOACTIVITY ⁸⁵Sr(EC); ¹¹³Sn(EC); ²⁰³Hg(β^-); measured electron spectra; deduced apparatus response, efficiency. New solenoidal spectrometer.

NUCLEAR REACTIONS ¹⁸¹Ta(²³⁸U, X), E=6.1 MeV/nucleon; measured γ-, positron energy spectra. New solenoidal spectrometer.

doi: 10.1016/0168-9002(95)00829-2
Citations: PlumX Metrics

1996RE02      Phys.Rev. C53, R572 (1996)

Z.Ren, B.Chen, Z.Ma, G.Xu

One-Proton Halo in ²⁶P and Two-Proton Halo in ²⁷S

NUCLEAR STRUCTURE ²⁶P, ²⁵Si, ²⁷S; calculated binding energy, neutron, proton, single particle orbitals radii, nucleon, matter density distributions; deduced halo characteristics. Nonlinear relativistic mean field theory.

doi: 10.1103/PhysRevC.53.R572
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1996RE04      J.Phys.(London) G22, L1 (1996); Erratum J.Phys.(London) G22, 1115 (1996)

Z.Ren, B.Chen, Z.Ma, G.Xu

Relativistic Mean-Field Study of Odd-A N and F Isotopes

NUCLEAR STRUCTURE ^{15,17,19,21,23}N, ^{17,19,21,23,25,27,29}F; calculated binding energy, nucleon rms radii. ^15,21,23N, ^27,29,23,25F; calculated nucleon, matter, halo neutron density distribution. Non-linear relativistic mean field theory, effective interactions.

doi: 10.1088/0954-3899/22/1/001
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1996RE10      Phys.Lett. 380B, 241 (1996)

Z.Ren, Z.Y.Zhu, Y.H.Cai, G.Xu

Relativistic Mean-Field Study of Mg Isotopes

NUCLEAR STRUCTURE ^{20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40}Mg; calculated binding energy, nucleon matter radii, deformation, quadrupole moments.

doi: 10.1016/0370-2693(96)00462-5
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1996RE13      J.Phys.(London) G22, 523 (1996)

Z.Ren, B.Chen, Z.Ma, Z.Zhu, G.Xu

One-Neutron Halos in ²²N, ²³O and ²⁴F and Three-Neutron Halo in ²⁶F

NUCLEAR STRUCTURE ²²N, ²³O, ^24,26F; calculated binding energy, neutron, proton, matter radii, density distributions, single particle energies. ²²Ne, ²³O, ^26,24F deduced neutron halo characteristics. Nonlinear relativistic mean-field theory.

doi: 10.1088/0954-3899/22/4/013
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1996RE19      Nucl.Phys. A605, 75 (1996)

Z.Ren, Z.Y.Zhu, Y.H.Cai, G.Xu

Relativistic Mean-Field Study of Exotic Carbon Nuclei

NUCLEAR STRUCTURE ^{9,10,11,12,13,14,15,16,17,18,19,20,21,22}C; calculated levels, J, π, binding energy, nucleon, charge, matter radii, nucleon deformation, isotope shifts, nucleon, matter density distributions in some cases. Relativistic mean-field approach.

doi: 10.1016/0375-9474(96)00186-8
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1996RE24      J.Phys.(London) G22, 1793 (1996)

Z.Ren, Z.Y.Zhu, Y.H.Cai, G.Xu

Relativistic Mean-Field Study of Even-Even Nuclei Near Z = 108 and N = 162

RADIOACTIVITY Z=108-114; N=162-170; calculated α-decay energies. Z=106; Z=108; Z=110; Z=112; Z=114; calculated binding energy, nucleon radii, β₂. Relativistic mean-field theory.

doi: 10.1088/0954-3899/22/12/010
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1995AH01      Nucl.Phys. A583, 247c (1995)

I.Ahmad, S.M.Austin, B.B.Back, D.Bazin, R.R.Betts, F.P.Calaprice, K.C.Chan, A.Chishti, P.Chowdhury, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, S.B.Gazes, J.S.Greenberg, A.L.Hallin, T.Happ, J.Last, N.Kaloskamis, E.Kashy, W.Kutschera, C.J.Lister, M.Liu, M.R.Maier, D.Mercer, A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.Trainor, P.Wilt, J.S.Winfield, M.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, G.Xu, A.Young, J.E.Yurkon

Positron Production in Heavy Ion Collisions: Current status of the problem

NUCLEAR REACTIONS ¹⁸¹Ta(²³⁸U, X), E=5.9-6.3 MeV/nucleon; compiled, analyzed, reviewed electron, positron production data.

doi: 10.1016/0375-9474(94)00667-C
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1995AH06      Phys.Rev.Lett. 75, 2658 (1995)

I.Ahmad, S.M.Austin, B.B.Back, R.R.Betts, F.P.Calaprice, K.C.Chan, A.Chishti, P.Chowdhury, C.Conner, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, S.B.Gazes, A.L.Hallin, T.Happ, D.Henderson, N.I.Kaloskamis, E.Kashy, W.Kutschera, J.Last, C.J.Lister, M.Liu, M.R.Maier, D.J.Mercer, D.Mikolas, P.A.A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.A.Trainor, P.Wilt, J.S.Winfield, M.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, G.Xu, A.Young, J.E.Yurkon, and the APEX Collaboration

Search for Narrow Sum-Energy Lines in Electron-Positron Pair Emission from Heavy-Ion Collisions Near the Coulomb Barrier

NUCLEAR REACTIONS ¹⁸¹Ta(²³⁸U, X), E=5.95-6.3 MeV/nucleon; ²³²Th(²³⁸U, X), E=5.95 MeV/nucleon; measured pair emission sum spectra; deduced no sharp lines evidence, neutral particle isolated decay related features.

doi: 10.1103/PhysRevLett.75.2658
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1995RE10      J.Phys.(London) G21, 691 (1995)

Z.Ren, G.-O.Xu, B.Chen, Z.Ma

Ground-State Properties of the Nucleus ¹⁰⁰Sn in Relativistic and Non-Relativistic Mean-Field Approaches

NUCLEAR STRUCTURE ^100,114,132Sn; calculated binding energy per nucleon, n-, p- radii, differences. Mean field approach, Skyrme interactions.

doi: 10.1088/0954-3899/21/5/013
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1995RE13      Phys.Lett. 351B, 11 (1995)

Z.Ren, G.Xu, B.Chen, Z.Ma, W.Mittig

Structure of Halo Nuclei ¹⁴Be and ³²Ne

NUCLEAR STRUCTURE ^12,14Be, ^30,32Ne; calculated proton, neutron, matter density distribution, rms radii, binding energy, single particle levels energy; deduced halo neutron occupation related features. Density-dependent relativistic mean-field theory.

doi: 10.1016/0370-2693(95)00364-Q
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1995RE16      Phys.Rev. C52, R1764 (1995)

Z.Ren, W.Mittig, B.Chen, Z.Ma, G.Auger, G.Xu

Neutron Halo and Spin-Orbit Splitting in Some Neutron-Rich Nuclei

NUCLEAR STRUCTURE ^12,14Be, ^30,32Ne, ^60,62Ca, ^122,124Zr; calculated ground state energy. ¹⁴Be, ³²Ne; calculated neutron, proton, halo radii, single particle energies. ^40,48,60Ca; calculated spin-orbit splitting variation. Density-dependent relativistic mean-field theory.

doi: 10.1103/PhysRevC.52.R1764
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1995RE23      J.Phys.(London) G21, L83 (1995)

Z.Ren, B.Chen, Z.Ma, W.Mittig, G.Xu

Spin-Orbit Splittings in the Relativistic Mean-Field Theory

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ⁹⁰Zr, ²⁰⁸Pb; calculated binding energy per nucleon, nucleon rms radii. ^40,48,60Ca; calculated spin-orbit splittings vs tensor coupling strength. Relativistic mean-field theory.

doi: 10.1088/0954-3899/21/11/001
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1995XU03      Phys.Rev. C52, 2859 (1995)

G.Xu, S.F.Pate, C.Bloch, S.E.Vigdor, S.M.Bowyer, T.W.Bowyer, W.W.Jacobs, H.O.Meyer, E.Pierce, J.Sowinski, C.Whiddon, S.W.Wissink, P.L.Jolivette, M.A.Pickar

Radiative Capture of Polarized Neutrons by Polarized Protons at T(n) = 183 MeV

NUCLEAR REACTIONS ¹H(polarized n, γ), E=183 MeV; measured σ(θ), proton-, neutron analyzing powers, normal-component spin correlation coefficent. Polarized target.

doi: 10.1103/PhysRevC.52.2859
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13608.

1993PA08      Phys.Rev.Lett. 70, 3205 (1993)

S.F.Pate, C.Bloch, G.Xu, S.M.Bowyer, T.W.Bowyer, W.W.Jacobs, H.-O.Meyer, E.Pierce, J.Sowinski, S.E.Vigdor, C.Whiddon, S.W.Wissink, P.L.Jolivette, M.A.Pickar

Spin Correlation and Analyzing Power Measurements for Neutron-Proton Radiative Capture at T(n) = 183 MeV

NUCLEAR REACTIONS ¹H(polarized n, γ), E=183 MeV; measured spin correlation coefficient, analyzing power vs θ; deduced mesonic, isobaric current role. Polarized target.

doi: 10.1103/PhysRevLett.70.3205
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1993XU05      Chin.J.Nucl.Phys. 15, No 3, 209 (1993)

G.Xu, N.Wang

Breaking of Dynamic Symmetry

1990LI01      Phys.Rev. C41, 169 (1990)

G.-Q.Li, G.-O.Xu

Optical Potential and the Fusion Barrier of Two Hot Nuclei

NUCLEAR STRUCTURE ¹²⁰Sn, ²⁰⁸Pb, ⁹⁰Zr; calculated neutron rms radii vs temperature. ¹²⁰Sn; calculated charge distribution vs radius.

NUCLEAR REACTIONS ¹²⁰Sn, ⁴⁰Ca(⁴⁰Ca, ⁴⁰Ca), ⁹⁰Zr(⁹⁰Zr, ⁹⁰Zr), ²⁰⁸Pb(²⁰⁸Pb, ²⁰⁸Pb), E not given; calculated potential, Coulomb interaction vs temperature, internucleus distance; deduced fusion barrier temperature shifts. Finite temperature, self-consistent semi-classical calculation.

doi: 10.1103/PhysRevC.41.169
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1990LI12      Nucl.Phys. A510, 557 (1990)

G.-Q.Li, G.-O.Xu

Finite Temperature Self-Consistent Semiclassical Approach to the Temperature Dependence of Properties of Hot Nuclei

NUCLEAR STRUCTURE ²⁰⁸Pb, ¹²⁰Sn, ⁹⁰Zr, ⁴⁰Ca; calculated rms radii change, giant resonance energy vs temperature. ²⁰⁸Pb; calculated nucleon density vs temperature. ¹²⁰Sn; calculated charge distribution vs temperature. Hot nuclei.

doi: 10.1016/0375-9474(90)90066-U
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1990LI20      Phys.Rev. C42, 290 (1990)

G.-Q.Li, G.-O.Xu

Self-Consistent Semiclassical Sum Rule Approach and the Properties of Giant Resonances

NUCLEAR STRUCTURE ²⁰⁸Pb, ⁴⁰Ca, ⁶⁰Ni, ⁹⁰Zr, ¹²⁰Sn; calculated rms radii, giant resonances. ²⁰⁸Pb; calculated nucleon densities.

doi: 10.1103/PhysRevC.42.290
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1990LI24      Chin.J.Nucl.Phys. 12, No.2, 139 (1990)

G.Li, G.Xu

The Transition Density and Transition Current Density of Giant Resonances

NUCLEAR STRUCTURE ⁴⁰Ca, ⁹⁰Zr, ²⁰⁸Pb, ¹²⁰Sn; calculated giant resonance transition current densities.

1990LI35      Chin.J.Nucl.Phys. 12, No 3, 219 (1990)

G.Li, G.Xu

Temperature Dependence of Nucleus-Nucleus Optical Potentials and Fusion Barrier

NUCLEAR REACTIONS ¹²⁰Sn, ⁴⁰Ca(⁴⁰Ca, ⁴⁰Ca), ⁹⁰Zr(⁹⁰Zr, ⁹⁰Zr), E not given; calculated potential parameters, fusion barriers.

1990LI43      Chin.J.Nucl.Phys. 12, No 4, 325 (1990)

G.Li, G.Xu

Self-Consistent Semiclassical Sum Rule Approach to Nuclear Giant Octupole Resonances

NUCLEAR STRUCTURE ⁴⁰Ca, ⁶⁰Ni, ⁹⁰Zr, ¹²⁰Sn, ²⁰⁸Pb; calculated giant octupole resonances, nucleon rms radii. Self-consistent semi-classical sum rule approach.

1990RE04      Phys.Lett. 237B, 1 (1990)

Z.Ren, G.Xu

Short-Range Correlations in Light Nuclei Near the Neutron Drip Line

NUCLEAR STRUCTURE A=4-32; analyzed neutron separation energies data; deduced stability near N=2Z.

doi: 10.1016/0370-2693(90)90449-G
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1990RE16      Phys.Lett. 252B, 311 (1990)

Z.Ren, G.Xu

A Three-Body Model of ¹¹Li, ¹⁴Be and ¹⁷B

NUCLEAR STRUCTURE ¹¹Li; calculated ground state energy, matter rms radius vs well depth parameter. ¹⁴Be, ¹⁷B; calculated matter rms radius vs well depth parameter. Three-body model.

doi: 10.1016/0370-2693(90)90542-E
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1989LI01      Phys.Rev. C39, 276 (1989)

Li Guo-Qiang, Xu Gong-Ou

Self-Consistent Semiclassical Calculation of the Spin-Orbit Contribution to the Nucleus-Nucleus Optical Potential

NUCLEAR REACTIONS ⁴⁸Ca(⁴⁸Ca, ⁴⁸Ca), ⁶⁰Ni(⁶⁰Ni, ⁶⁰Ni), (⁴⁰Ca, ⁴⁰Ca), ⁴⁸Ca(⁴⁰Ca, ⁴⁰Ca), ⁹⁰Zr(¹⁶O, ¹⁶O), E not given; calculated potential parameter vs internucleus distance. Self-consistent, semi-classical approach.

doi: 10.1103/PhysRevC.39.276
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1989LI02      J.Phys.(London) G15, 79 (1989)

G.-Q.Li, G.-O.Xu

Semiclassical Approach to Centroid Splitting of Giant Resonances on Deformed Nuclei

NUCLEAR STRUCTURE ³⁴S, ³⁶Ar, ^150,152Sm, ¹⁶⁰Gd, ¹⁸⁶W, ²³²Th, ²³⁸U; calculated GDR, GQR energy centroids. Semi-classical approach.

doi: 10.1088/0954-3899/15/1/008
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1989LI07      Nucl.Phys. A492, 340 (1989)

G.-Q.Li, G.-O.Xu

Self-Consistent Semiclassical Calculation of Nucleus-Nucleus Optical Potentials and Fusion Barriers

NUCLEAR STRUCTURE ⁴⁰Ca, ⁴⁰Ar, ^90,92,94Zr, ^120,122,124Sn; calculated rms radii. Self-consistent model.

NUCLEAR REACTIONS ^40,48Ca, ¹²⁰Sn(⁴⁰Ca, ⁴⁰Ca), E not given; calculated potential vs internuclear separation. ⁹⁰Zr(⁴⁰Ca, X), ¹²²Sn(⁴⁰Ar, X), ¹²⁰Sn, ⁹⁰Zr(⁹⁰Zr, X), ¹²⁴Sn(⁹²Zr, X), (⁹⁴Zr, X), E not given; calculated fusion barrier.

doi: 10.1016/0375-9474(89)90091-2
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1989RE03      J.Phys.(London) G15, 465 (1989)

Z.-Z.Ren, G.-O.Xu

Shell and Blocking Effects in α-Transfer Reactions

NUCLEAR REACTIONS ^{116,117,118,119,120}Sn(p, t), (d, ⁶Li), E not given; analyzed relative σ; deduced shell, blocking effects in α-transfer.

doi: 10.1088/0954-3899/15/4/010
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1988LI26      J.Phys.(London) G14, 1387 (1988)

Li Guo-qiang, Xu Gong-ou

Self-Consistent Semiclassical Calculation with Extended Skyrme Forces and the Properties of Giant Resonances

NUCLEAR STRUCTURE ⁴⁸Ca, ⁹⁰Zr, ¹³⁰Sn, ²⁰⁸Pb; calculated GDR splitting, rms radii. ⁴⁰Ca calculated rms radius, nucleon effective mass, charge profile. ²⁰⁸Pb; calculated nucleon effective mass, charge profile. Semi-classical approach.

doi: 10.1088/0305-4616/14/11/010
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1988RE10      Phys.Rev. C38, 1078 (1988)

Ren Zhong-zhou, Xu Gong-ou

Evidence of α Correlation from Binding Energies in Medium and Heavy Nuclei

NUCLEAR STRUCTURE Z=83-92; N=127-142; analyzed binding energies; deduced α clustering role.

doi: 10.1103/PhysRevC.38.1078
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1980XU01      Nucl.Phys. A343, 189 (1980)

G.-O.Xu, J.-Y.Zhang

On Criteria for the Mechanism of Backbending in Even-Even Nuclei

NUCLEAR STRUCTURE ^164,166Yb, ^168,172Hf, ^160,156Er, Ce; analyzed B(E2), g-factor data; deduced criteria for backbending.

doi: 10.1016/0375-9474(80)90648-X
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1979SU15      Chin.J.Nucl.Phys. 1, 93 (1979)

Sun Xiang-Fu, Pan Zong-You, Yuan Shuang-Gui, Xu Guo-Jun

Determination of the Lifetime of Excited Compound Nuclei from ¹²C + ¹⁹⁷Au Reaction by Blocking effect

NUCLEAR REACTIONS, Fission ¹⁹⁷Au(¹²C, F), E=72.5 MeV; measured fragment blocking pattern. ²⁰⁹At deduced T_1/2. Mica track detector.

Note: The following list of authors and aliases matches the search parameter G.Xu: , G.H.XU, G.J.XU, G.O.XU