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NSR database version of April 26, 2024.

Search: Author = Y.Gao

Found 64 matches.

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2024HU03      Eur.Phys.J. A 60, (2024)

Y.Hu, Yu.M.Gledenov, Z.Cui, J.Liu, H.Bai, C.Xia, Zh.Chen, Z.Wu, W.Ren, W.Cao, T.Fan, G.Zhang, E.Sansarbayar, G.Khuukhenkhuu, L.Krupa, I.Chuprakov, Q.Fan, X.Ruan, H.Huang, J.Ren, Y.Gao, X.Yang

Cross section measurement for the ¹⁴N(n, α_{0, 1})¹¹B reactions in the 4.5–11.5 MeV neutron energy region

NUCLEAR REACTIONS ¹⁴N(n, α), E=4.5 -11.5 MeV; measured reaction products, En, In, Eα, Iα; deduced σ and uncertainties. Comparison with EXFOR, ENDF/B-VIII.0, ENDF/B-VII.1, JEFF-3.3, CENDL-3.2, ROSFOND-2010, ADS-2.0, JENDL-5, BROND-3.1, BROND-2.2, FENDL-3.2b, and TENDL-2021 libraries. The 4.5 MV Van de Graaff accelerator at Peking University and the HI-13 tandem accelerator of China Institute of Atomic Energy (CIAE).

doi: 10.1140/epja/s10050-024-01268-9
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2023EK01      Eur.Phys.J. A 59, 103 (2023)

H.Ekawa, W.Dou, Y.Gao, Y.He, A.Kasagi, E.Liu, A.Muneem, M.Nakagawa, C.Rappold, N.Saito, T.R.Saito, M.Taki, Y.K.Tanaka, H.Wang, J.Yoshida

Development of machine learning analyses with graph neural network for the WASA-FRS experiment

doi: 10.1140/epja/s10050-023-01016-5
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2023GA14      Chin.Phys.C 47, 044105 (2023)

Y.Gao, Z.Ren, L.Jin

Systematic study of global optical model potentials in (d, p) transfer reactions

NUCLEAR REACTIONS ¹²C, ⁴⁸Ca, ¹²⁴Sn, ²⁰⁸Pb(d, p), (d, d), E=10-60 MeV; analyzed available data; deduced the optical model potentials (OMPs) parameters, σ(θ).

doi: 10.1088/1674-1137/acb2bc
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2023GA28      Int.J.Mod.Phys. E32, 2350050 (2023)

Y.Gao, Y.Lin, L.Liu

Classification of pairing phase transition in the hot nucleus

NUCLEAR STRUCTURE ¹⁶²Dy; calculated partition function of neutron and proton, partition function with different seniority numbers by the CDFT+SLAP method. Comparison with available data.

doi: 10.1142/S0218301323500507
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2023LI22      J.Phys.(London) G50, 045106 (2023)

J.Liu, Z.Cui, Y.Hu, H.Bai, Y.Yang, X.Ruan, C.Xia, J.Chen, G.Zhang, Y.M.Gledenov, E.Sansarbayar, G.Khuukhenkhuu, L.Krupa, I.Chuprakov, H.Huang, J.Ren, Q.Fan, Y.Gao, X.Yang

⁶³Cu(n, α)⁶⁰Co cross sections in the MeV region

NUCLEAR REACTIONS ⁶³Cu(n, α), ²³⁸U(n, F), E=4.5-10.5 MeV; measured reaction products, Eγ, Iγ; deduced σ using both the direct measurement method and the activation method, preference of ENDF/B-VII.1 over ENDF/B-VIII.0 library. Comparison with TALYS-1.9 calculations. The 4.5 MV Van de Graaff accelerator at Peking University (PKU) and the HI-13 tandem accelerator at the China Institute of Atomic Energy (CIAE).

doi: 10.1088/1361-6471/acb960
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2023WA23      Chin.Phys.C 47, 084101 (2023)

Y.-Z.Wang, F.-Z.Xing, J.-P.Cui, Y.-H.Gao, J.-Z.Gu

Roles of tensor force and pairing correlation in two-proton radioactivity of halo nuclei

RADIOACTIVITY ¹⁸Mg, ²⁰Si(2p); calculated T_1/2 using different Skyrme interactions, Q-values; deduced small effect of tensor force. The framework of spherical Skyrme-Hartree-Fock-Bogoliubov theory.

doi: 10.1088/1674-1137/acd680
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2022CU01      Nucl.Phys. A1017, 122341 (2022)

J.P.Cui, Y.H.Gao, Y.Z.Wang, J.Z.Gu

Improved effective liquid drop model for α-decay half-lives

RADIOACTIVITY ^{255,256,258,259,261,263}Rf, ^{256,257,258,259}Db, ²⁷⁰Db, ^259,260,261Sg, ²⁶³Sg, ^267,269,271Sg, ²⁶³Sg, ^267,269,271Sg, ^260,261Bh, ^265,266,267Bh, ^270,272,274Bh, ^264,265,266Hs, ^268,269,270Hs, ^273,275Hs, ²⁷⁰Mt, ^274,275,276Mt, ²⁷⁸Mt, ²⁶⁷Ds, ^269,270,271Ds, ²⁷³Ds, ^277,279,281Ds, ²⁷²Rg, ^{278,279,280,281,282}Rg, ²⁷⁷Cn, ^281,283Cn, ^284,285Cn, ²⁷⁸Nh, ^{282,283,284,285,286}Nh, ^{285,286,287,288,289}Fl, ²⁸⁷Mc, ^289,290Mc, ^{290,291,292,293}Lv, ^293,294Ts, ²⁹⁴Og(α); calculated T_1/2. Comparison with available data.

doi: 10.1016/j.nuclphysa.2021.122341
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2022CU02      Nucl.Phys. A1017, 122341 (2022)

J.P.Cui, Y.H.Gao, Y.Z.Wang, J.Z.Gu

Improved effective liquid drop model for α-decay half-lives

RADIOACTIVITY ^{255,256,258,259,261,263}Rf, ^{256,257,258,259,270}Db, ^{259,260,261,263,267,269,271}Sg, ^{260,261,265,266,267,270,272,274}Bh, ^{264,265,266,268,269,270,273,275}Hs, ^{270,274,275,276,278}Mt, ^{267,269,270,271,273,277,279,281}Ds, ^{272,278,279,280,281,282}Rg, ^{277,281,283,284,285}Cn, ^{278,282,284,285,286}Nh, ^{285,286,287,288,289}Fl, ^{287,288,289,290}Mc, ^{290,291,292,293}Lv, ^293,294Ts, ^{278,282,286,290,294,298,302,306}Og, ^{281,285,289,293,297,301,305,309}119, ^{286,290,294,298,302,306,310,289,293,297,301,305,309}120(α); calculated T_1/2. Comparison with available data.

doi: 10.1016/j.nuclphysa.2021.122341
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2022GU21      Astrophys.J. 941, 31 (2022)

D.L.Guo, R.T.Zhang, X.L.Zhu, Y.Gao, K.Z.Lin, T.Cao, D.M.Zhao, X.B.Zhu, C.J.Zhang, S.F.Zhang, X.Ma

Benchmark n ℓ-resolved Cross Sections of Single and Double Charge Exchange Processes in 1.67-20 KeV u^-11 C⁴⁺ Collisions with He

NUCLEAR REACTIONS He(C, X), E=1.67-2 keV/nucleon; analyzed available data; deduced σ for charge exchange processes.

doi: 10.3847/1538-4357/ac9d2e
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2022HA32      Phys.Rev. C 106, 064332 (2022)

S.C.Han, X.L.Shang, W.Zuo, G.C.Yong, Y.Gao

In-medium nucleon-nucleon cross section in nuclear matter

NUCLEAR REACTIONS ¹H(p, X), (n, X), ¹NN(n, X), E=40-420 MeV; calculated σ(E) and medium correction factors in nuclear matter with various densities and isospin asymmetries. ¹²⁴Sn(¹³²Sn, X), E=270 MeV/nucleon; calculated proton and neutron transverse and elliptic flows. Calculations in the framework of the Brueckner-Hartree-Fock approach.

doi: 10.1103/PhysRevC.106.064332
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2022LI59      Phys.Rev. C 106, 054605 (2022)

J.Liu, Y.Wang, Y.Gao, P.Danielewicz, C.Xu, Z.Ren

Exploring the sensitivity of charge-exchange (p, n) reactions to the neutron density distribution

NUCLEAR REACTIONS ⁴⁸Ca(p, p), ⁴⁸Ca, ²⁰⁸Pb(p, n), E=35, 45 MeV;²⁰⁸Pb(n, n), E=30.4, 40 MeV; calculated σ(θ). Distorted-wave Born approximation (DWBA) method with complex folding and the hybrid folding models generated potentials. Calibration of the calculated potentials to PREX-II data. Comparison to experimental data.

NUCLEAR STRUCTURE ⁴⁸Ca, ²⁰⁸Pb; calculated binding energies per nucleon, charge rms radii, neutron skin thickness. ²⁰⁸Pb; calculated ground-state neutron and proton densities. Calculations within Skyrme-Hartree-Fock (SHF) and the relativistic mean-field (RMF) frameworks. Comparison to experimental data.

doi: 10.1103/PhysRevC.106.054605
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2022XI08      Nucl.Phys. A1028, 122528 (2022)

F.Xing, H.Qi, J.Cui, Y.Gao, Y.Wang, J.Gu, G.Yong

An improved Gamow-like formula for α-decay half-lives

RADIOACTIVITY ^{214,215,216,217,218}U, ^{219,220,221,222,223,224}Np, ^{221,222,223,224,225,226,227}Pu, ^{224,225,226,227,228}Am, ^231,232Cm, ^{233,234,235,236,237,238,239,240,241,242}Bk, ^234,235,236Cf, ^237,238,239Es, ^{239,240,241,242,243,244}Fm, ^241,242,243Md, ^{246,247,248,249,250}No, ^249,250,251Lr, ^{251,252,253,254}Rf, ^253,254,255Db, ^256,257,258Sg, ^{258,259,260,261,262,263}Bh, ^261,262Hs, ^263,264,265Mt, ^{261,262,263,264,265,266}Ds, ^{266,267,268,269,270,271,272,273}Rg, ^{270,271,272,273,274,275,276}Cn, ^{272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290}Nh, ^{278,279,280,281,282,283,284,285,286,287,288,289,290,291}Fl, ^{281,282,283,284,285,286,287,288,289,290,291,292}Mc, ^{283,284,285,286,287,288,289}Lv, ^{285,286,287,288,289,290,291,292}Ts, ^{288,289,290,291,292,293}Og, ²⁹⁵Og, ^{290,291,292,293,294,295,296}119, ^{291,292,293,294,295,296,297,298,299,300}120, ^{287,288,289,290,291}Og, ^283,284Lv, ^279,280,281Fl, ^275,276Cn, ^271,272,273Ds, ²⁹⁴120, ^268,269Hs, ^264,265Sg, ²⁸¹Fl(α); calculated T_1/2; deduced an improved Gamow-like (IMGL) formula parameters. Comparison with available data.

doi: 10.1016/j.nuclphysa.2022.122528
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2021GA32      Phys.Rev. C 104, 044607 (2021)

Y.Gao, Y.L.Guo, L.Zhang, G.C.Yong, Z.Y.Liu, W.Zuo

Pion production and absorption in heavy-ion collisions

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E=400 MeV/nucleon; calculated local density distributions and time evolutions of inelastic reactions in central collision, fraction of the different types of free pions, average density and time at which a pion gets produced, π^-/π⁺ ratio versus different types of free pions, average scattering number in the history of the free pions as a function of the kinetic energy and polar angle, dependence of the ratios of the charged pions emitted on kinetic energy in a direction closed to the beam direction. Isospin-dependent Boltzmann-Uehling-Uhlenbeck (IBUU) transport model for pion production and absorption in inelastic collisions.

doi: 10.1103/PhysRevC.104.044607
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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, T_1/2 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
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2021LI36      Nucl.Phys. A1014, 122225 (2021)

T.X.Li, C.B.Li, Y.Zheng, X.G.Wu, J.Zhong, B.J.Zhu, Q.W.Fan, Y.X.Gao, Y.J.Jin, G.S.Li, L.H.Zhu

Lifetime measurements and the structure of some negative-parity states in ¹³⁴Ce

NUCLEAR REACTIONS ¹²²Sn(¹⁶O, 4n), E=76 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, J, π, B(Eλ), lifetimes of negative-parity states. Comparison with cranked Nilsson-Strutinsky Bogoliubov (CNSB) model. Recoil-distance Doppler-shift technique.

doi: 10.1016/j.nuclphysa.2021.122225
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Data from this article have been entered in the XUNDL database. For more information, click here.

2021ZH66      Nucl. Sci. Tech. 32, 107 (2021)

J.Zhong, X.-G.Wu, S.-P.Hu, Y.-J.Ma, Y.Zheng, C.-B.Li, G.-S.Li, B.-J.Zhu, T.-X.Li, Y.-J.Jin, Y.-X.Gao, Q.-W.Fan, K.-Y.Ma, D.Yang, H.-B.Sun, H.-G.Zhao, L.Gan, Q.Luo, Z.X.Wu

Lifetime measurements in ¹³⁸Nd

NUCLEAR REACTIONS ¹²³Sb(¹⁹F, 4n), E=87 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and relative intensities, J, π, partial level scheme, level T_1/2, B(E2). Comparison with Grodzins systematics and available data. The recoil distance Doppler shift technique in combination with the differential decay curve method. The HI-13 tandem accelerator of the China Institute of Atomic Energy (CIAE) in Beijing.

doi: 10.1007/s41365-021-00953-4
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Data from this article have been entered in the XUNDL database. For more information, click here.

2020CU01      Phys.Rev. C 101, 014301 (2020), Erratum Phys.Rev. C 104, 029902 (2021)

J.P.Cui, Y.H.Gao, Y.Z.Wang, J.Z.Gu

Two-proton radioactivity within a generalized liquid drop model

RADIOACTIVITY ⁶Be, ¹²O, ¹⁶Ne, ¹⁹Mg, ⁴⁵Fe, ⁴⁸Ni, ⁵⁴Zn, ⁶⁷Kr(2p); calculated half-lives for 2p decay mode using generalized liquid drop model (GLDM) and compared with experimental half-lives, and other theoretical calculations. ²²Si, ²⁶S, ³⁴Ca, ^38,39Ti, ⁴²Cr, ⁴⁹Ni, ⁵⁵Zn, ^58,59,60Ge, ⁶⁴Se(2p); predicted half-lives using GLDM for 2p radioactivity.

doi: 10.1103/PhysRevC.101.014301
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2020LI35      Phys.Rev. C 102, 034302 (2020)

J.G.Li, B.S.Hu, Q.Wu, Y.Gao, S.J.Dai, F.R.Xu

Neutron-rich calcium isotopes within realistic Gamow shell model calculations with continuum coupling

NUCLEAR STRUCTURE ^{49,50,51,52,53,54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72}Ca; calculated binding energies, S(n), S(2n), neutron effective single-particle energies (ESPE), energies of the first 2+ states in even-A nuclei. ^{51,52,53,54,55,56,57,58}Ca; calculated levels, J, π. ^51,53,55,57Ca; calculated energies and widths of the first 5/2+ and 9/2+ resonance states. Realistic Gamow shell model based on high-precision CD-Bonn potential. Comparison with experimental data. ⁵⁷Ca; predicted as the heaviest odd-A bound Ca isotope. ⁷⁰Ca; predicted as the dripline nucleus. Calculations support shell closures at ⁵²Ca, ⁵⁴Ca, and possibly at ⁷⁰Ca, and a weakening of shell closure at ⁶⁰Ca.

doi: 10.1103/PhysRevC.102.034302
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2020MA02      Phys.Rev. C 101, 014304 (2020)

Y.Ma, C.Su, J.Liu, Z.Ren, C.Xu, Y.Gao

Predictions of nuclear charge radii and physical interpretations based on the naive Bayesian probability classifier

NUCLEAR STRUCTURE A>3; calculated nuclear charge radii for 896 nuclei using naive Bayesian probability (NBP) method and the Skyrme-Hartree-Fock-Bogoliubov model. Comparison with experimental data.

doi: 10.1103/PhysRevC.101.014304
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2019CH04      Phys.Rev. A 99, 012710 (2019)

L.Chen, X.Shan, X.Zhao, X.Zhu, X.Hu, Y.Wu, W.Feng, D.Guo, R.Zhang, Y.Gao, Z.Huang, J.Wang, X.Ma, X.Chen

Two-body fragmentation dynamics of N₂O^q+(q=2, 3) induced by electron-capture collisions with 5.7 - keV/u Xe¹⁵⁺

NUCLEAR REACTIONS N, O(Xe, Xe'), E=5.7 keV/nucleon; measured reaction products; deduced kinetic energy release (KER) distributions for the ion-pair products. Comparison with calculations.

doi: 10.1103/PhysRevA.99.012710
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2019CU01      Nucl.Phys. A987, 99 (2019)

J.P.Cui, Y.Xiao, Y.H.Gao, Y.Z.Wang

α-decay half-lives of neutron-deficient nuclei

RADIOACTIVITY Z=80-118(α); calculated α-decay T_1/2 of neutron-deficient nuclei using Effective Liquid Drop Model (ELDM), generalized Liquid Drop Model (GLDM) within fission-like and cluster-like modes and using Royer and Denisov formulae; T_1/2 compared to data; deduced that GLDM gives higher values than calculations using other approaches; calculated, predicted T_1/2 n-deficient nuclei not measured using GLDM with WS4 Q_α values.

doi: 10.1016/j.nuclphysa.2019.04.008
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2019YA23      Phys.Rev. C 100, 054325 (2019)

Z.X.Yang, X.L.Shang, G.C.Yong, W.Zuo, Y.Gao

Nucleon momentum distributions in asymmetric nuclear matter

doi: 10.1103/PhysRevC.100.054325
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2018GA03      Phys.Rev. C 97, 014609 (2018)

Y.Gao, G.-C.Yong, L.Zhang, W.Zuo

Influence of the nuclear symmetry energy on the collective flows of charged pions

doi: 10.1103/PhysRevC.97.014609
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2018LI14      Phys.Rev. C 97, 034331 (2018)

C.B.Li, X.G.Wu, Y.Zheng, Y.J.Jin, H.L.Ma, G.S.Li, J.Zhong, B.J.Zhu, T.X.Li, Y.X.Gao, X.Guan, J.Q.Liu

Level structure in the transitional nucleus ¹⁹⁹Tl

NUCLEAR REACTIONS ¹⁹⁶Pt(⁷Li, 4n), E=40 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) using eight Compton-suppressed HPGe detectors and two planar HPGe detectors at HI-13 tandem accelerator of China Institute of Atomic Energy (CIAE). ¹⁹⁹Tl; deduced high-spin levels, J, π, bands, multipolarities, configurations, alignments, oblate shapes, potential energy surfaces for 17/2- state. Comparison with cranked Nilsson-Strutinsky-Bogoliubov (CNSB) model calculations. Systematics of 13/2+ states in N=104-122 Tl and Bi nuclei. Systematics of negative-parity yrast states and positive-parity 3-qp yrast states in ^195,197,199Tl.

doi: 10.1103/PhysRevC.97.034331
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Data from this article have been entered in the XUNDL database. For more information, click here.

2018LI51      Chin.Phys.C 42, 114101 (2018)

M.Liu, Y.Gao, N.Wang

Statistical errors in Weizsacker-Skyrme mass model

NUCLEAR STRUCTURE ¹³²Sn, ²⁰⁸Pb, Ca, Zr, Sb, Rn; calculated atomic masses; deduced statistical uncertainties of 13 model parameters. Comparison with AME2016.

doi: 10.1088/1674-1137/41/11/114101
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2017GA30      Eur.Phys.J. A 53, 197 (2017)

Y.Gao, H.Zheng, L.L.Zhu, A.Bonasera

Description of charged particle pseudorapidity distributions in Pb+Pb collisions with Tsallis thermodynamics

doi: 10.1140/epja/i2017-12397-y
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2017GU01      Phys.Rev. A 95, 012707 (2017)

D.L.Guo, X.Ma, R.T.Zhang, S.F.Zhang, X.L.Zhu, W.T.Feng, Y.Gao, B.Hai, M.Zhang, H.B.Wang, Z.K.Huang

State-selective electron capture in 30- and 100-keV He⁺ + He collisions

NUCLEAR REACTIONS He(α, E), E=30, 100 keV; measured reaction products, Eβ, Iβ; deduced σ, σ(θ). Comparison with theoretical calculations.

doi: 10.1103/PhysRevA.95.012707
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2017GU03      Phys.Rev. A 95, 022705 (2017)

D.L.Guo, X.Ma, S.F.Zhang, X.L.Zhu, W.T.Feng, R.T.Zhang, Y.Gao, B.Hai, M.Zhang, D.B.Qian, S.Yan, and P.Zhang

Dynamics of transfer ionization in p-He collisions at intermediate energies

NUCLEAR REACTIONS He(p, X), E=50-100 keV; measured reaction products, Eβ, Iβ; deduced that electron momentum distribution projected onto the scattering plane is consistent with the prediction of an independent two-step mechanism involving a binary encounter. Comparison with theoretical calculations.

doi: 10.1103/PhysRevA.95.022705
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2017GU30      Phys.Rev. C 96, 044622 (2017)

S.Q.Guo, Y.Gao, J.Q.Li, H.F.Zhang

Dynamical deformation in heavy ion reactions and the characteristics of quasifission products

NUCLEAR REACTIONS ²⁴⁸Cm(⁴⁸Ca, X), E(cm)=205 MeV; calculated potential energy surface for the reaction as a function of quadrupole deformations in the entrance channel, evolution of the distribution function and the mass yield as a function of fragment deformations, relative quasifission yield distribution, TKE, and relative mass yield of quasi fission (QF) products. Dinuclear system (DNS), including the deformation variables of fragments in addition to mass numbers of the fragments. Comparison with available experimental data.

doi: 10.1103/PhysRevC.96.044622
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2017LI42      Chin.Phys.C 41, 114101 (2017)

M.Liu, Y.Gao, N.Wang

Statistical errors in Weizsacker-Skyrme mass model

NUCLEAR STRUCTURE ¹³²Sn, ²⁰⁸Pb, Ca, Zr, Sb, Rn; calculated masses. Comparison with AME2003 and AME2016 evaluations.

doi: 10.1088/1674-1137/41/11/114101
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2017ZH45      Nucl.Instrum.Methods Phys.Res. B412, 81 (2017)

J.P.Zhu, X.Xiao, S.Yan, Y.Gao, J.M.Xue, Y.G.Wang

Measurement of differential cross section of D(3He, p)4He from 0.8 MeV to 3.6 MeV

NUCLEAR REACTIONS ²H(³He, p), E=0.8-3.6 MeV; measured reaction products; deduced σ(θ). Comparison with available data.

doi: 10.1016/j.nimb.2017.07.020
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0089.

2016BA20      Phys.Rev. C 93, 044615 (2016)

X.J.Bao, Y.Gao, J.Q.Li, H.F.Zhang

Possibilities for synthesis of new isotopes of superheavy nuclei in cold fusion reactions

NUCLEAR REACTIONS ²⁰⁹Bi(⁵⁴Cr, n)²⁶²Bh, ²⁰⁸Pb(⁵⁶Fe, n)²⁶³Hs, ²⁰⁸Pb(⁵⁸Fe, n)²⁶⁵Hs, ²⁰⁹Bi(⁵⁸Fe, n)²⁶⁶Mt, ²⁰⁸Pb(⁶²Ni, n)²⁶⁹Ds, ²⁰⁷Pb(⁶⁴Ni, n)²⁷⁰Ds, ²⁰⁸Pb(⁶⁴Ni, n)²⁷¹Ds, ²⁰⁹Bi(⁶⁴Ni, n)²⁷²Rg, ²⁰⁸Pb(⁶⁸Zn, n)²⁷⁵Cn, ²⁰⁸Pb(⁷⁰Zn, n)²⁷⁷Cn, ²⁰⁹Bi(⁷⁰Zn, n)²⁷⁸Nh, E not given; calculated evaporation residue cross section (ERCS) for cold fusion reactions and compared with experimental data. ²⁰⁷Pb(⁵⁸Fe, n), (⁶⁴Ni, n), (⁷⁰Zn, n), ²⁰⁸Pb, ²⁰⁹Bi(⁵⁶Fe, n), (⁵⁸Fe, n), (⁵⁹Fe, n), (⁶⁰Fe, n), (⁶¹Fe, n), (⁵⁸Ni, n), (⁵⁹Ni, n), (⁶⁰Ni, n), (⁶¹Ni, n), (⁶²Ni, n), (⁶⁴Ni, n), (⁶⁵Ni, n), ²⁰⁸Pb(⁶⁶Zn, n), (⁶⁷Zn, n), (⁶⁸Zn, n), (⁷⁰Zn, n), (⁷¹Zn, n), E not given; calculated evaporation residue cross section (ERCS) for cold fusion reactions for production A=262-278, Z=108-112 superheavy nuclides (SHN), isospin dependence. ²⁰⁸Pb(⁵⁸Mn, n), (⁶¹Fe, n), (⁵⁸Co, n), (⁶⁵Ni, n), (⁶⁶Cu, n), (⁷⁴Ga, n), (⁷⁸As, n), (⁸⁵Se, n), (⁸⁹Br, n), (⁹¹Kr, n), ²⁰⁹Bi(⁶⁶Cu, n), (⁸⁰Ga, n), E not given; calculated evaporation residue cross section (ERCS) for cold fusion reactions for production of Z=107-118, A=265-298 and compared with other theoretical calculations. ¹³⁶Xe(¹³⁶Xe, n)²⁷¹Hs, E not given; calculated cross section. Dinuclear system (DNS) model via cold fusion reactions.

doi: 10.1103/PhysRevC.93.044615
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2016BA43      Chin.Phys.C 40, 094102 (2016)

Z.-J.Bai, C.-F.Jiao, Y.Gao, F.-R.Xu

Searching for high-K isomers in the proton-rich A ∼ 80 mass region

NUCLEAR STRUCTURE ^70,72Se, ^{70,72,74,76,78}Kr, ^{72,74,76,78,80}Sr, ^76,78,80,82Zr, ^78,80,82Mo; calculated ground-state deformation parameters, high-K states.

doi: 10.1088/1674-1137/40/9/094102
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2016HO20      Chin.Phys.C 40, 114102 (2016)

S.Hong, Y.-W.Yang, H.-S.Xu, H.-Y.Meng, L.Zhang, Z.-Q.Liu, Y.-C.Gao, K.Chen

Application of Origen2.1 in the decay photon spectrum calculation of spallation products

doi: 10.1088/1674-1137/40/11/114102
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2016ZH08      Phys.Rev. A 93, 032709 (2016)

R.T.Zhang, W.T.Feng, X.L.Zhu, S.F.Zhang, D.L.Guo, Y.Gao, D.B.Qian, S.Xu, S.C.Yan, P.Zhang, Z.K.Huang, H.B.Wang, B.Hai, D.M.Zhao, X.Ma

Two-electron transfer and ionization mechanism in 80-keV/u Ne⁸⁺ on He collisions

NUCLEAR REACTIONS He(Ne, X), E=80 keV/nucleon; measured reaction products, Eβ, Iβ; deduced autoionization decay from doubly excited states with symmetric and asymmetric configurations.

doi: 10.1103/PhysRevA.93.032709
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2015BA03      Phys.Rev. C 91, 011603 (2015)

X.J.Bao, Y.Gao, J.Q.Li, H.F.Zhang

Influence of the nuclear dynamical deformation on production cross sections of superheavy nuclei

NUCLEAR REACTIONS ²³⁸U, ²³⁷Np, ^242,244Pu, ^245,248Cm, ²⁴⁹Bk, ^249,251Cf, ^252,254Es(⁴⁸Ca, 3n), (⁴⁸Ca, 4n), (⁴⁸Ca, 5n), at E(compound nucleus)=20-60 MeV; calculated evaporation residue cross sections as function of the excitation energy of the compound nucleus. Z=119, 120; predicted production σ. Calculations based on Dinuclear system with deformations of the two nuclei described by a Fokker-Planck equation. Comparison with experimental data.

doi: 10.1103/PhysRevC.91.011603
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2015BA19      Phys.Rev. C 91, 064612 (2015)

X.J.Bao, Y.Gao, J.Q.Li, H.F.Zhang

Theoretical study of the synthesis of superheavy nuclei using radioactive beams

NUCLEAR REACTIONS ²⁴⁴Pu(³⁴S, X), (⁴⁸Ca, X), E not given; calculated contour plot of driving potential as function of neutron and proton numbers of fragment. ¹⁵⁴Sm(⁴⁰Ca, X)¹⁹⁴Pb*, E(*)=56-75 MeV; ¹⁵⁴Sm(⁴⁸Ca, X)²⁰²Pb*, E(*)=49-95 MeV; ¹⁸²W(³²S, X)²¹⁴Th*, E(*)=56-136 MeV; ²⁰⁸Pb(¹⁹F, X)²²⁷Pa*, E(*)=51-124 MeV; ²⁰⁸Pb(²⁴Mg, X)²³²Pu*, E(*)=52-114 MeV; ¹⁵⁴Sm(⁴⁰Ca, X)¹⁹⁴Pb*, E(*)=56-75 MeV; ²⁰⁸Pb(²⁸Si, X)²³⁶Cm*, E(*)=50-138 MeV; ²⁰⁸Pb(³²S, X)²⁴⁰Cf*, E(*)=66-111 MeV; ²³⁸U(³⁶S, X)²⁷⁴Hs*, E(*)=36-56 MeV; ²⁴⁸Cm(²⁶Mg, X)²⁷⁴Hs*, E(*)=37-64 MeV; calculated fusion probability and compared with experimental values. ²⁴⁹Bk, ²⁵²Cf(¹⁴N, 3n), (¹⁴N, 4n), (¹⁴N, 5n), ²⁴⁹Bk(¹⁹F, 3n), (¹⁹F, 4n), (¹⁹F, 5n), ²⁴⁶Cm, ²⁴⁹Bk, ²⁵⁰Cf(³⁰Si, 3n), (³⁰Si, 4n), (³⁰Si, 5n), ²⁵²Cf, ²⁵³Es(²²Ne, 3n), (²²Ne, 4n), (²²Ne, 5n), ²⁵³Es(¹⁸O, 3n), (¹⁸O, 4n), (¹⁸O, 5n), ²³⁸U, ²³⁷Np, ^242,244Pu, ²⁴³Am, ^245,248Cm, ²⁴⁹Cf, ²⁴⁹Bk(⁴⁸Ca, 3n), (⁴⁸Ca, 4n), (⁴⁸Ca, 5n), ²³⁷Np, ²⁴⁴Pu, ²⁴⁸Cm, ²⁴⁹Bk, ²⁵²Cf, ²⁵³Es(²⁴Na, 4n), (²⁴Na, 5n), ²⁵²Cf(²¹O, 4n), (²¹O, 5n), ²³⁸U, ²⁴⁴Pu(⁴²K, 4n), (⁴²K, 5n), ²³⁷Np, ²⁴⁹Bk(⁴³K, 4n), (⁴³K, 5n), ²⁴⁸Cm(⁴⁶Ar, 4n), (⁴⁶Ar, 5n), ²⁴⁸Cm, ²⁵²Cf, ²⁵³Es(⁴⁶K, 4n), (⁴⁶K, 5n), E not given; calculated formation σ for evaporation residues and compared with available experimental values and previous calculations. Dinuclear system (DNS) model for the formation of Z=108-118 superheavy (SHE) compound nuclei.

doi: 10.1103/PhysRevC.91.064612
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2015BA30      Phys.Rev. C 92, 014601 (2015)

X.J.Bao, Y.Gao, J.Q.Li, H.F.Zhang

Influence of nuclear basic data on the calculation of production cross sections of superheavy nuclei

NUCLEAR REACTIONS ²³⁷Np, ²³⁸U, ^242,244Pu, ²⁴³Am, ^245,248Cm, ²⁴⁹Cf, ²⁴⁹Bk(⁴⁸Ca, 3n), (⁴⁸Ca, 4n), E not given; calculated survival probabilities of superheavy nuclei (SHN) as function of mass number of compound nucleus, and compared with experimental cross sections. ²⁴³Am(⁴⁸Ca, 3n), (⁴⁸Ca, 4n), (⁴⁸Ca, 5n), E*(CN)=20-60 MeV; calculated capture cross sections, fusion probabilities, and survival probabilities, evaporation residue cross sections as function of excitation energy leading to nuclei with Z=112-118. ²⁴⁹Cf(⁵⁰Ti, 3n), (⁵⁰Ti, 4n), (⁵⁰Ti, 5n), E*=20-60 MeV; ²⁴⁸Cm(⁵⁴Cr, 3n), (⁵⁴Cr, 4n), (⁵⁴Cr, 5n), E*=20-60 MeV; calculated evaporation residue cross sections as function of excitation energy and Z=120 production. Calculations based on the DNS concept, and use of three nuclear data tables (FRDM-1995, KTUY-2005, WS-2010).

doi: 10.1103/PhysRevC.92.014601
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2015BA42      Phys.Rev. C 92, 034612 (2015)

X.J.Bao, Y.Gao, J.Q.Li, H.F.Zhang

Isotopic dependence of superheavy nuclear production in hot fusion reactions

NUCLEAR REACTIONS ²³⁷Np, ²³⁸U, ^242,244Pu, ²⁴³Am, ^245,248Cm, ²⁴⁹Bk, ²⁴⁹Cf(⁴⁸Ca, 2n), (⁴⁸Ca, 3n), (⁴⁸Ca, 4n), (⁴⁸Ca, 5n), E*=20-60 MeV; calculated evaporation residue cross section (ERCSs) for nuclei of SHE of Z=112-118. ^{232,233,234,235,236,237,238}U, ^{236,237,238,239,240,241,242,243,244}Pu, ^{242,243,244,245,246,247,248,249,250}Cm, ^{249,250,251,252}Cf(⁴⁸Ca, 3n), (⁴⁸Ca, 4n), (⁵⁰Ti, 3n), (⁵⁰Ti, 4n), (⁵⁰Ca, 3n), (⁵⁰Ca, 4n), ^235,236,237Np, ^241,242,243Am, ^247,248,249Bk(⁴⁸Ca, 3n), (⁴⁸Ca, 4n), (⁵⁰Ti, 3n), (⁵⁰Ti, 4n), E not given; calculated evaporation residue cross section (ERCSs) for nuclei of SHE region. Dinuclear system (DNS) model. Comparison with available experimental data.

doi: 10.1103/PhysRevC.92.034612
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2015GU02      Nucl.Phys. A934, 110 (2015)

S.Guo, X.Bao, Y.Gao, J.Li, H.Zhang

The nuclear deformation and the preformation factor in the α-decay of heavy and superheavy nuclei

RADIOACTIVITY Z=76-100(α); calculated even-even nuclei T_1/2, α preformation factor using generalized liquid drop model with and without deformation. Compared with values extracted from experimental T_1/2. Paper declares calculations for Z=62-118, but results presented only for its subset.

doi: 10.1016/j.nuclphysa.2014.12.001
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2014LI38      Eur.Phys.J. A 50, 94 (2014)

F.-H.Liu, Y.-Q.Gao, T.Tian, B.-C.Li

Unified description of transverse momentum spectrums contributed by soft and hard processes in high-energy nuclear collisions

doi: 10.1140/epja/i2014-14094-9
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2014LI41      Eur.Phys.J. A 50, 123 (2014)

F.-H.Liu, Y.-Q.Gao, B.-C.Li

Comparing two-Boltzmann distribution and Tsallis statistics of particle transverse momentums in collisions at LHC energies

doi: 10.1140/epja/i2014-14123-9
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2013GA12      Phys.Rev. C 87, 034324 (2013)

Y.Gao, J.Dobaczewski, M.Kortelainen, J.Toivanen, D.Tarpanov

Propagation of uncertainties in the Skyrme energy-density-functional model

NUCLEAR STRUCTURE Z=20, 28, 50, 82, N=20, 28, 50, 82, 126; calculated standard uncertainties in binding energies, S(2n), S(2p), neutron and proton rms radii. Skyrme energy-density-functional (UNEDF0-EDF) model.

doi: 10.1103/PhysRevC.87.034324
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2013GA46      Phys.Rev. C 88, 057601 (2013)

Y.Gao, G.C.Yong, Y.Wang, Q.Li, W.Zuo

Influence of the symmetry energy on the cone-azimuthal emission

doi: 10.1103/PhysRevC.88.057601
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2013KO22      Phys.Rev. C 88, 031305 (2013)

M.Kortelainen, J.Erler, W.Nazarewicz, N.Birge, Y.Gao, E.Olsen

Neutron-skin uncertainties of Skyrme energy density functionals

NUCLEAR STRUCTURE Z<120, A<400; analyzed systematic and statistical uncertainties in theoretical neutron-skin thickness predicted by various Skyrme EDF models. Statistical covariance technique.

doi: 10.1103/PhysRevC.88.031305
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2013LI46      Phys.Rev. C 88, 037301 (2013)

C.Liu, S.Y.Wang, B.Qi, D.P.Sun, S.Wang, C.J.Xu, L.Liu, P.Zhang, Z.Q.Li, B.Wang, X.C.Shen, M.R.Qin, H.L.Liu, Y.Gao, L.H.Zhu, X.G.Wu, G.S.Li, C.Y.He, Y.Zheng

Signature splitting, shape evolution, and nearly degenerate bands in ¹⁰⁸Ag

NUCLEAR REACTIONS ¹⁰⁴Ru(⁷Li, 3n), E=33 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) at CIAE, Beijing facility. ¹⁰⁸Ag; deduced high-spin levels, J, π, bands, multipolarities, configurations, signature splitting and signature inversion, staggering parameter. Total Routhian surface (TRS) calculations. Systematics of level energies, staggering parameter, B(M1)/B(E2) ratios, kinematic moments of inertial for bands in ^98,100Tc, ^104,106Rh, ^106,108Ag, and comparison with behavior of chiral partner bands.

doi: 10.1103/PhysRevC.88.037301
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2012GA14      J.Korean Phys.Soc. 60, 1011 (2012)

Y.-Q.Gao, Z.-X.Zhang, Y.-Y.Zhao, F.-H.Liu

Production cross-sections of projectile-like isotopes in ¹¹²Sn + ¹¹²Sn and ¹²⁴Sn + ¹²⁴Sn reactions at 1A GeV

NUCLEAR REACTIONS ¹¹²Sn(¹¹²Sn, X), ¹²⁴Sn(¹²⁴Sn, X), E=1 GeV/nucleon; calculated isotopic σ of fragments. Comparison with experimental data.

doi: 10.3938/jkps.60.1011
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2012GA37      Phys.Rev. C 86, 034611 (2012)

Y.Gao, L.Zhang, W.Zuo, J.-Q.Li

Probing the nuclear symmetry energy using single and double π^-/π⁺ ratios from mirror reaction systems

NUCLEAR REACTIONS ²²O, ²²Si(²²Na, X), E=400 MeV/nucleon; calculated central baryon density, nuclear symmetry energy, π^-/π⁺ ratios, kinetic energy distribution of the double π^-/π⁺ ratio. Isospin and momentum-dependent hadronic transport model IBUU.

doi: 10.1103/PhysRevC.86.034611
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2012ZH02      Phys.Rev. C 85, 014325 (2012)

H.F.Zhang, Y.Gao, N.Wang, J.Q.Li, E.G.Zhao, G.Royer

Double magic nuclei for Z>82 and N>126

NUCLEAR STRUCTURE Z=101-118, N=140-194; calculated binding energies, Q(α). Z=101-129, N=162, 184; calculated S(p), Q(α) using Macroscopic-microscopic model (MMM). ²⁷⁰Hs, ²⁹⁸Fl; calculated potential energy in the constrained relativistic mean-field (CRMF) theory with effective interaction NL3. Comparison with experimental data.

RADIOACTIVITY ²⁶⁹Sg, ²⁷⁴Bh, ²⁷³Hs, ²⁷⁸Mt, ^277,281Ds, ²⁸²Rg, ^281,285Cn, ^285,286Nh, ^285,288,289Fl, ^289,290Mc, ^293,294Ts(α); Z=108, N=148-172(α); Z=114, N=160-190(α); calculated α decay half-lives. Macroscopic-microscopic model (MMM). Comparison with experimental data.

doi: 10.1103/PhysRevC.85.014325
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2012ZH10      Eur.Phys.J. A 48, 30 (2012)

L.Zhang, Y.Gao, Y.Du, G.-H.Zuo, G.-C.Yong

Effect of the momentum dependence of nuclear symmetry potential on the transverse and elliptic flows

NUCLEAR REACTIONS ¹²⁴Sn(¹³²Sn, X), E=400 MeV/nucleon; calculated rapidity distribution of free n/p ratio, transverse flow, elliptic flow using isospin-dependent BUU with two different symmetry potentials.

doi: 10.1140/epja/i2012-12030-9
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2011GA17      Phys.Rev. C 83, 047602 (2011)

Y.Gao, L.Zhang, H.Zhang, X.Chen, G.-C.Yong

Effect of the momentum dependence of the nuclear symmetry potential on the pi-/pi+ ratio in heavy-ion collisions

doi: 10.1103/PhysRevC.83.047602
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2011YO08      Phys.Rev. C 84, 034609 (2011)

G.-C.Yong, Y.Gao, W.Zuo, X.-C.Zhang

Initialization effect in heavy-ion collisions at intermediate energies

NUCLEAR REACTIONS ⁴⁰Ca(⁴⁰Ca, X), ⁴⁸Ca(⁴⁸Ca, X), E=400 MeV/nucleon; ¹⁹⁷Au(¹⁹⁷Au, X), E=200-800 MeV/nucleon; calculated neutron and proton density distributions, neutron to proton, and charged π^-/π⁺ ratios of preequilibrium nucleon emissions, effect of initialization on different ratios. Boltzmann-Uehling-Uhlenbeck transport model plus the Skyrme force parameters.

doi: 10.1103/PhysRevC.84.034609
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2011ZH45      Chin.Phys.Lett. 28, 112102 (2011)

L.Zhang, Y.Gao, H.-F.Zhang, X.-M.Chen, M.-L.Yu.J.-Q.Li

Symmetry Energy Effects in a Statistical Multifragmentation Model

doi: 10.1088/0256-307X/28/11/112102
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2010GA12      Chin.Phys.Lett. 27, 062102 (2010)

Y.Gao, H.-F.Zhang, L.Zhang, X.-M.Chen, J.-Q.Li, W.-J.Guo

Relativistic Mean Field Study of the Z = 117 Isotopic Chain

NUCLEAR STRUCTURE Z=117; calculated binding energies, deformations, α-decay energies, lifetimes. Relativistic mean field theory in the blocked BCS approximation.

doi: 10.1088/0256-307X/27/6/062102
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2009GA43      Chin.Phys.C 33, 848 (2009)

Y.Gao, J.-M.Dong, H.-F.Zhang, W.Zuo, J.-Q.Li

Properties and structure of N = Z nuclei within relativistic mean field theory

NUCLEAR STRUCTURE ⁸⁴Mo; calculated proton and neutron density distributions, single-particle spectra, Fermi energy levels, binding energy, one and two nucleon separation energy, quadrupole deformation, rms radii. Axially deformed RMF.

doi: 10.1088/1674-1137/33/10/006
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2008QI04      Int.J.Mod.Phys. E17, 1955 (2008)

C.Qi, R.Z.Du, Y.Gao, J.C.Pei, J.Y.Zhu, F.R.Xu

Proton resonance properties in light nuclei with mean-field type potentials

NUCLEAR STRUCTURE ¹¹B, ¹¹C, ¹¹N, ¹⁴N, ¹⁴O, ^15,16F, ^18,19Na; calculated energies, J, π, Q-values for proton resonances using a mean-field model.

doi: 10.1142/S0218301308010933
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2006GA23      Eur.Phys.J. A 28, 361 (2006)

Y.-J.Gao, C.Meng, K.-T.Chao

ψ(3770) and B meson exclusive decay B → ψ(3770)K in QCD factorization

doi: 10.1140/epja/i2006-10059-y
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2005FU07      Phys.Rev. C 72, 017901 (2005)

J.Fu, Y.Gao, J.Cheng

Comparison of two types of event-by-event transverse momentum fluctuation measurements

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E(cm)=200 GeV/nucleon; analyzed mean transverse momentum fluctuations.

doi: 10.1103/PhysRevC.72.017901
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2004LI60      Phys.Rev. C 70, 034610 (2004)

J.-Y.Liu, W.-J.Guo, Y.Z.Xing, X.G.Li, Y.Y.Gao

Isospin effect of Coulomb interaction on the dissipation and fragmentation in intermediate energy heavy ion collisions

NUCLEAR REACTIONS ⁶⁴Fe(⁶⁴Fe, X), ⁸⁹Kr(⁸⁹Kr, X), ¹²⁴Sn(¹²⁴Sn, X), E=50 MeV/nucleon; calculated isospin fractionation ratio, momentum dissipation, related features. Isospin-dependent quantum molecular dynamics approach.

doi: 10.1103/PhysRevC.70.034610
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2001LU03      Chin.Phys.Lett. 18, 501 (2001)

Y.-A.Luo, J.-Q.Chen, Y.-C.Gao, P.-Z.Ning, J.P.Draayer

Influence of the Unique-Parity States on the Collectivity of Low-Lying States

NUCLEAR STRUCTURE ¹³⁴Ba; calculated levels, J, π, B(E2), B(M1); deduced role of unique-parity states in collectivity. Nucleon-pair shell model.

doi: 10.1016/S0009-2614(01)00862-4
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1996SA53      Nucl.Instrum.Methods Phys.Res. A383, 245 (1996)

H.F.-W.Sadrozinski, J.DeWitt, D.E.Dorfan, T.Dubbs, A.A.Grillo, S.Kashigin, W.Kroeger, J.Rahn, W.A.Rowe, A.Seiden, E.Spencer, A.Webster, R.Wichmann, M.Wilder, D.Williams, J.Dane, A.Lankford, S.Pier, B.Schmid, R.Bonino, C.Couyoumtzelis, P.Demierre, Y.Iwata, T.Ohsugi, H.Iwasaki, T.Kondo, S.Terada, Y.Unno, W.Dabrowski, M.Idzik, J.Godlewski, R.Takashima, A.Ciocio, T.Collins, C.Haber, I.Kipnis, M.Shapiro, J.Siegrist, H.Spieler, N.Tamura, A.Grewal, R.Nickerson, R.Wastie, Y.Gao, R.Gonzalez, A.M.Walsh, Z.Feng

Monitoring the Performance of Silicon Detectors with Binary Readout in the ATLAS Beam Test

doi: 10.1016/S0168-9002(96)00751-6
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1991GA25      Europhys.Lett. 16, 711 (1991)

Y.Y.Gao, F.Catara, M.Sambataro, A.Vitturi

Study of Negative-Parity States in Near-Closed-Shell Nuclei in the Collective-Pair Approximation Including Particle-Hole Excitations

NUCLEAR STRUCTURE ¹⁸O; calculated levels; deduced (particle-particle)-, (particle-hole)- degrees of freedom role in octupole states. Collective pair approximation.

1990TR03      Phys.Rev. B41, 9570 (1990)

A.Trokiner, R.Mellet, A.-M.Pougnet, D.Morin, Y.M.Gao, J.Primot, J.Schneck

¹⁷O NMR Spectroscopy of Bi₂Sr₂CaCu₂O(8+x) High-T(c) Superconductor

NUCLEAR MOMENTS ¹⁷O; measured NMR. High T(c) superconductor material.

doi: 10.1103/PhysRevB.41.9570
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1980ZH06      Chin.J.Nucl.Phys. 2, 253 (1980)

Zhang Xizhen, He Hanxing, Chen Yongshou, Gao Yuanyi

Backbending Mechanism of ^155,156Er

NUCLEAR STRUCTURE ^155,156Er; calculated B(E2), rotational bands; deduced backbending mechanism, band crossing frequency, interaction matrix element. Two-band crossing model.

Note: The following list of authors and aliases matches the search parameter Y.Gao: , Y.C.GAO, Y.H.GAO, Y.J.GAO, Y.M.GAO, Y.Q.GAO, Y.X.GAO, Y.Y.GAO