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NSR database version of April 11, 2024.

Search: Author = Q.Gao

Found 17 matches.

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2021JI16      Symmetry 13, 2278 (2021)

H.Jian, Y.Gao, F.Dai, J.Liu, X.Xu, C.Yuan, K.Kaneko, Y.Sun, P.Liang, G.Shi, L.Sun, L.Xayavong, C.Lin, J.Lee, Z.Li, Y.Yang, P.Li, R.Fan, S.Zha, H.Zhu, J.Li, Q.Gao, Z.Zhang, R.Chen, J.Wang, D.Wang, H.Wu, K.Wang, Y.Lam, F.Duan, P.Ma, Z.Gao, Q.Hu, Z.Bai, J.Ma, J.Wang, F.Zhong, C.Wu, D.Luo, Y.Jiang, Y.Liu, D.Hou, R.Li, N.Ma, W.Ma, G.Yu, D.Patel, S.Jin, Y.Wang, Y.Yu, Q.Zhou, P.Wang, L.Hu, X.Wang, H.L.Zang, Q.Zhao, L.Yang, P.Wen, F.Yang, H.Jia, G.Zhang, M.Pan, X.Wang, H.Sun, M.Wang, Z.Hu, X.Zhou, Y.Zhang, H.Xu, M.Liu, H.-J.Ong, W.Yang

β-Delayed γ Emissions of 26P and Its Mirror Asymmetry

RADIOACTIVITY 26P(β+), (EC) [from 9Be(32S, X), E=80.6 MeV/nucleon, followed by separation using RIBBL1 at HRIBF, Lanzhou facility]; measured Eγ, Iγ, βγ-coin, T1/2 of 26P decay. 26Si; deduced levels, J, π, β++ϵ feedings, logft, mirror asymmetry parameter from comparison with the ϵ decay of mirror nucleus 26Na to 26Mg, mirror-energy differences (MEDs), and halo structure in 26P. Comparison with shell-model calculations.

NUCLEAR REACTIONS 9Be(32S, X)22Na/23Mg/24Al/25Si/26P/27S, E=80.6 MeV/nucleon; measured reaction products, particle-identification (PID) plot of ΔE vs TOF for the ions separated using RIBBL1 separator at HRIBF, Lanzhou facility.

doi: 10.3390/sym13122278
Citations: PlumX Metrics


2021SH23      Phys.Rev. C 103, L061301 (2021)

G.Z.Shi, J.J.Liu, Z.Y.Lin, H.F.Zhu, X.X.Xu, L.J.Sun, P.F.Liang, C.J.Lin, J.Lee, C.X.Yuan, S.M.Wang, Z.H.Li, H.S.Xu, Z.G.Hu, Y.Y.Yang, R.F.Chen, J.S.Wang, D.X.Wang, H.Y.Wu, K.Wang, F.F.Duan, Y.H.Lam, P.Ma, Z.H.Gao, Q.Hu, Z.Bai, J.B.Ma, J.G.Wang, F.P.Zhong, C.G.Wu, D.W.Luo, Y.Jiang, Y.Liu, D.S.Hou, R.Li, N.R.Ma, W.H.Ma, G.M.Yu, D.Patel, S.Y.Jin, Y.F.Wang, Y.C.Yu, Q.W.Zhou, P.Wang, L.Y.Hu, X.Wang, H.L.Zang, P.J.Li, Q.R.Gao, H.Jian, S.X.Zha, F.C.Dai, R.Fan, Q.Q.Zhao, L.Yang, P.W.Wen, F.Yang, H.M.Jia, G.L.Zhang, M.Pan, X.Y.Wang, H.H.Sun, X.H.Zhou, Y.H.Zhang, M.Wang, M.L.Liu, H.J.Ong, W.Q.Yang

β-delayed two-proton decay of 27S at the proton-drip line

RADIOACTIVITY 27S(β+2p)[from 9Be(32S, X), E=80.6 MeV/nucleon, followed by separation and purification of fragments using RIBLL1 at HIRFL-Lanzhou facility, and implanted into three W1-type double-sided silicon strip detectors (DSSDs)]; measured reaction products, E(p), I(p), pp-coin, p(θ), half-life of 27S decay using Si detectors surrounded by HPGe detectors; deduced branching ratio of β+2p decay, identified as a two-proton transition, dominantly sequential, via the isobaric-analog state (IAS) in 27P to the ground state of 25Al.

doi: 10.1103/PhysRevC.103.L061301
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Data from this article have been entered in the XUNDL database. For more information, click here.


2011FU11      Phys.Rev. C 84, 037603 (2011)

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

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

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

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


2010TI03      Int.J.Mod.Phys. E19, 1076 (2010)

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

Projectile fragmentation of 36, 40Ar induced reactions

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

doi: 10.1142/S0218301310015515
Citations: PlumX Metrics


2010TI05      Int.J.Mod.Phys. E19, 1815 (2010)

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

Projectile fragmentation of 36-40Ar induced reactions

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

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


2009LI51      Phys.Rev. C 80, 054315 (2009)

Z.H.Li, J.L.Lou, Y.L.Ye, H.Hua, D.X.Jiang, X.Q.Li, S.Q.Zhang, T.Zheng, Y.C.Ge, Z.Kong, L.H.Lv, C.Li, F.Lu, F.Y.Fan, Z.Y.Li, Z.X.Cao, L.Y.Ma, Q.Faisal, H.S.Xu, Z.G.Hu, M.Wang, X.G.Lei, L.M.Duan, Z.G.Xiao, W.L.Zhan, G.Q.Xiao, T.H.Huang, F.Fu, X.H.Zhang, C.Zheng, Y.H.Yu, X.L.Tu, Y.P.Zhang, Y.Y.Yang, H.B.Zhang, B.Thang, Y.L.Tian, Z.Ouang, M.R.Huang, Z.G.Xu, K.Yue, Q.Gao

Experimental study of the β-delayed neutron decay of 21N

RADIOACTIVITY 21N(β-), (β-n) [from 9Be(26Mg, X), E=68.8 MeV]; measured Eγ, Iγ, Eβ, Iβ, En, In, βn-, βγ-, βγn-coin, half-lives and. delayed-neutron emission probabilities. 20,21O; deduced levels, J, π, branching ratios, logft values and B(GT). Comparison with shell model calculations. 20,21F, 20,21O(β-); measured Eγ.

NUCLEAR REACTIONS 9Be(26Mg, X), E=68.8 MeV; measured isotopic yields. 6He, 7,8,9Li, 9,10,11,12Be, 12,13,14,15,17B, 15,16,17,18,19C, 19,20,21N, 22,23O; measured yields.

doi: 10.1103/PhysRevC.80.054315
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Data from this article have been entered in the XUNDL database. For more information, click here.


2009LO07      Chin.Phys.C 33, Supplement 1, 202 (2009)

J.-L.Lou, H.-Z.Li, Y.-L.Ye, D.-X.Jiang, H.Hua, X.-Q.Li, S.-Q.Zhang, T.Zheng, Y.-C.Ge, Z.Kong, L.-H.Lu, C.Li, F.Lu, F.-Y.Fan, Z.-Y.Li, Z.-X.Cao, Y.-L.Ma, J.Q.Faisal, H.-S.Xu, Z.-G.Hu, M.Wang, X.-G.Lei, L.-M.Duan, Z.-H.Xiao, W.-L.Zhan, G.-Q.Xiao, T.-H.Huang, F.Fu, X.H.Zhang, C.Zheng, Y.-H.Yu, X.-L.Tu, Y.-P.Zhang, Y.-Y.Yang, B.-H.Zhang, B.Tang, Y.-L.Tian, Z.Ouyang, M.-R.Huang, Z.-G.Xu, K.Yue, Q.Gao

Characteristics of a 4-fold segmented clover detectore

doi: 10.1088/1674-1137/33/S1/065
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2008LO06      Chin.Phys.Lett. 25, 1992 (2008)

J.-L.Lou, Z.-H.Li, Y.-L.Ye, D.-X.Jiang, H.Hua, X.-Q.Li, S.-Q.Zhang, T.Zheng, Y.-C.Ge, Z.Kong, L.-H.Lv, C.Li, F.Lu, F.-Y.Fan, Z.-Y.Li, Z.-X.Cao, L.-Y.Ma, Faisal, H.-S.Xu, Z.-G.Hu, M.Wang, X.-G.Lei, L.-M.Duan, Z.-G.Xiao, W.-L.Zhan, G.-Q.Xiao, T.-H.Huang, F.Fu, X.-H.Zhang, C.Zheng, Y.-H.Yu, X.-L.Tu, Y.-P.Zhang, Y.-Y.Yang, H.-B.Zhang, B.Tang, Y.-L.Tian, Y.-Z.Ou, M.-R.Huang, Z.-G.Xu, K.Yue, Q.Gao

The β Decay of 21N

RADIOACTIVITY 21N(β-) [from 9Be(26Mg, X), E=68.8 MeV/nucleon]; measured T1/2, Eβ, Iβ, Eγ, Iγ, En, In, βγ-, (n)β-coin.

doi: 10.1088/0256-307X/25/6/019
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Data from this article have been entered in the XUNDL database. For more information, click here.


2007BA76      Chin.Phys.Lett. 24, 3384 (2007)

Z.Bai, Q.Wang, J.-L.Han, ZG.Xiao, H.-S.Xu, Z.-Y.Sun, Z.-G.Hu, X.-Y.Zhang, H.-W.Wang, R.-S.Mao, X-H.Yuan, Z.-G.Xu, H.-B.Zhang, H.-G.Xu, H.-R.Qi, Y.Wang, F.Jia, L.-J.Wu, X.-L.Ding, Q.Gao, H.Gao, S.-L.Li, J.-Q.Li, Y.-P.Zhang, G.-Q.Xiao, G.-M.Jin, Z.-Z.Ren, S.-G.Zhou, W.Xu, G.-T.Fan, S.-Q.Zhang, D.-Y.Pang, Y.-K.Sergey

Angular Dispersion and Deflection Function for Heavy Ion Elastic Scattering

NUCLEAR REACTIONS 208Pb(17F, 17F), E=141 MeV; 208Pb(17O, 17O), E=128 MeV; measured differential cross sections, angular dispersion plots. 208Pb(16O, 16O), E=170.1 MeV; 208Pb(6He, 6He), E=27, 29.6 MeV; 208Pb(6Li, 6Li), E=73.7, 99 MeV; 208Pb(α, α), E=40 MeV; analyzed differential cross sections, angular dispersion plots.

doi: 10.1088/0256-307X/24/12/027
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0200.


2007LO05      Phys.Rev. C 75, 057302 (2007)

J.L.Lou, Z.H.Li, Y.L.Ye, H.Hua, D.X.Jiang, L.H.Lv, Z.Kong, Y.M.Zhang, F.R.Xu, T.Zheng, X.Q.Li, Y.C.Ge, C.Wu, G.L.Zhang, Z.Q.Chen, C.Li, D.Y.Pang, H.S.Xu, Z.Y.Sun, L.M.Duan, Z.G.Hu, R.J.Hu, H.G.Xu, R.S.Mao, Y.Wang, X.H.Yuan, H.Gao, L.J.Wu, H.R.Qi, T.H.Huang, F.Fu, F.Jia, Q.Gao, X.L.Ding, J.L.Han, X.Y.Zhang

Observation of a new transition in the beta-delayed neutron decay of 18N

RADIOACTIVITY 18N(β-); measured β-delayed neutron spectra. 18O; deduced level energies, J, π. Deduced B(GT), compared to shell model calculations.

doi: 10.1103/PhysRevC.75.057302
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Data from this article have been entered in the XUNDL database. For more information, click here.


2006WA17      Chin.Phys.Lett. 23, 1731 (2006)

Q.Wang, J.-L.Han, Z.-G.Xiao, H.-S.Xu, Z.-Yu.Sun, Z.-G.Hu, X.-Y.Zhang, H.-W.Wang, R.-S.Mao, X.-H.Yuan, Z.-G.Xu, T.-C.Zhao, H.-B.Zhang, H.-G.Xu, H.-R.Qi, Y.Wang, F.Jia, L.-J.Wu, X.-L.Ding, Q.Gao, H.Gao, S.-L.Li, Z.Bai, G.-Q.Xiao, G.-M.Jin, Z.-Z.Ren, S.-G.Zhou, Yu.-K.Sergey

Exotic Behaviour of Angular Dispersion of Weakly Bound Nucleus 17F at Small Angles

NUCLEAR REACTIONS 208Pb(17F, 17F), E=141 MeV; 208Pb(17O, 17O), E=128 MeV; measured σ(θ); deduced possible halo effects.

doi: 10.1088/0256-307X/23/7/021
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2005LI60      Phys.Rev. C 72, 064327 (2005)

Z.H.Li, Y.L.Ye, H.Hua, D.X.Jiang, Y.M.Zhang, F.R.Xu, Q.Y.Hu, G.L.Zhang, Z.Q.Chen, T.Zheng, C.E.Wu, J.L.Lou, X.Q.Li, D.Y.Pang, S.Wang, C.Li, H.S.Xu, Z.Y.Sun, L.M.Duan, Z.G.Hu, R.J.Hu, H.G.Xu, R.S.Mao, Y.Wang, X.H.Yuan, H.Gao, L.J.Wu, H.R.Qi, T.H.Huang, F.Fu, F.Jia, Q.Gao, X.L.Ding, J.L.Han, X.Y.Zhang

β-decay of the neutron-rich nucleus 18N

RADIOACTIVITY 18N(β-), (β-n) [from Be(22Ne, X)]; measured T1/2, β-delayed neutron spectra, Eγ, Iγ; deduced branching ratios, Gamow-Teller strengths. 18O deduced levels, J, π. Comparison with shell model calculations.

doi: 10.1103/PhysRevC.72.064327
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Data from this article have been entered in the XUNDL database. For more information, click here.


1990LI23      Nucl.Phys. A515, 273 (1990)

G.-Q.Li, J.-Q.Shi, Q.Gao

The Thermal Self-Consistent Semiclassical Approach and Microscopic Nucleon-Nucleus Optical Potentials at Finite Temperature

NUCLEAR STRUCTURE 40Ca, 90Zr, 208Pb; calculated nucleon densities, mean free path. Thermal self-consistent, semi-classical calculation.

NUCLEAR REACTIONS 40Ca, 208Pb(n, n), E not given; calculated potential parameters vs nucleon-nucleus distance. Nucleon densities from thermal self-consistent, semi-classical calculation.

doi: 10.1016/0375-9474(90)90369-W
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1987YU02      Chin.J.Nucl.Phys. 9, 316 (1987)

Yuan Haiji, Ye Weilei, Gao Qin, Shen Qingbiao, Zhuo Yizhong

Microscopic Calculations of Single-Particle Spreading Width II. In Finite Nuclei

NUCLEAR STRUCTURE 12C, 16O, 40Ca, 90Zr, 120Sn, 208Pb; calculated single particle spreading widths. Local density approximation.


1986YE01      Chin.J.Nucl.Phys. 8, 15 (1986)

Ye Weilei, Yuan Haiji, Gao Qin, Shen Qingbiao, Zhuo Yizhong

The Calculations of Charge Density Distribution and Charge Radii for Spherical Nuclei using the Hartree-Fock Method with Skyrme Forces

NUCLEAR STRUCTURE 48Ca, 90Zr; calculated levels. 16O, 40,48Ca, 90Zr; calculated charge density distributions. 16O, 28Si, 32S, 40,48Ca, 60Ni, 90Zr, 120Sn; calculated charge rms radii. Hartree-Fock method.


1986YE02      Chin.J.Nucl.Phys. 8, 214 (1986)

Ye Weilei, Yuan Haiji, Gao Qin, Zheng Chunkai, Tian Ye, Shen Qingbiao

Calculations of Neutron Skin for Spherical Nuclei using the Hartree-Fock Method with Skyrme Forces

NUCLEAR STRUCTURE 16O, 28Si, 32S, 40,48Ca, 60Ni, 90Zr, 120Sn; calculated proton, neutron density distributions, rms radii. Hartree-Fock method, Skyrme force.


1985YE02      Chin.J.Nucl.Phys. 7, 166 (1985)

Ye Weilei, Yuan Haiji, Gao Qin, Shen Qingbiao, Zhang Jingshang, Liu Ruizhe, Gu Yingqi

Hartree-Fock Calculations with Extended Skyrme Force for 16O and 40Ca

NUCLEAR STRUCTURE 16O, 40Ca; calculated single particle energies. Hartree-Fock method, extended Skyrme force.


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Note: The following list of authors and aliases matches the search parameter Q.Gao: , Q.R.GAO