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NSR database version of April 11, 2024.

Search: Author = H.Zhang

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2024LI12      Chin.Phys.C 48, 014105 (2024)

J.Liu, Zh.Wang, H.Zhang, Zh.Ren

Theoretical predictions on cluster radioactivity of superheavy nuclei with Z = 119, 120

RADIOACTIVITY 221,222,223,224Ra, 226Ra, 221Fr, 225Ac(14C), 228Th(20O), 230Th(24Ne), 231Pa(24Ne), (23F), 233,234U(24Ne), 236,238Pu(28Mg), 238Pu(32Si), 242Cm(34Si), 293,295,297,299,301,303,305,307,309,311119, 293,294,295,296,297,298,299120(8Be), (12C), (16O), (24Ne), (28Mg), (32Si); calculated T1/2 with two successful theoretical methods with modified parameters: the density-dependent cluster model (DDCM) and unified decay formula (UDF). Comparison with available data.

doi: 10.1088/1674-1137/ad0827
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2024TE03      Phys.Rev. C 109, 034308 (2024)

J.X.Teng, K.Y.Ma, J.B.Lu, H.C.Zhang, H.Wang, S.Y.Liu, D.Zhao, H.Y.Ye, J.Y.Li, X.J.Zhao, Z.H.Zhao, Y.C.Hao, Z.Qiao, Y.J.Ma, D.Yang, X.G.Wu, Y.Zheng, C.B.Li

Possible multiple chiral doublet bands in odd-odd 128La

doi: 10.1103/PhysRevC.109.034308
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2024WA08      Nucl.Phys. A1043, 122834 (2024)

M.Z.Wang, D.Wu, H.Y.Lan, J.Y.Zhang, J.X.Liu, H.G.Lu, J.F.Lv, X.Z.Wu, H.Zhang, J.Cai, Q.Y.Ma, Y.H.Xia, Z.N.Wang, Z.Y.Yang, X.L.Xu, Y.X.Geng, Y.Y.Zhao, H.R.Wang, F.L.Liu, J.Q.Yu, K.J.Luo, W.Luo, X.Q.Yan

Cross section measurements of 27Al(γ, x)24Na reactions as monitors for laser-driven bremsstrahlung γ-ray

NUCLEAR REACTIONS 27Al(γ, X)24Na, E ∼ 78, 103, 135; measured reaction products, Eγ, Iγ; deduced γ-ray energies, σ. Comparison with TALYS 1.9 calculations, experimental data. The 200 TW laser facility in the Compact Laser Plasma Accelerator (CLAPA) Laboratory, Peking University.

doi: 10.1016/j.nuclphysa.2024.122834
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2024ZH15      Nucl.Instrum.Methods Phys.Res. A1059, 168983 (2024)

H.Q.Zhang, P.Kuang, X.T.Yu, P.Zhang, F.Y.Liu, R.S.Yu, X.Z.Cao, B.Y.Wang

Development of novel positron lifetime measurement system for potential liquid material inspection

doi: 10.1016/j.nima.2023.168983
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2024ZH18      Phys.Rev. C 109, 034307 (2024)

H.Zhang, D.Bai, Zh.Wang, Zh.Ren

Microscopic cluster model in harmonic oscillator traps

doi: 10.1103/PhysRevC.109.034307
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2023AK05      Phys.Lett. B 845, 138128 (2023)

T.Akaishi, H.Asano, X.Chen, A.Clozza, C.Curceanu, R.Del Grande, C.Guaraldo, C.Han, T.Hashimoto, M.Iliescu, K.Inoue, S.Ishimoto, K.Itahashi, M.Iwasaki, Y.Ma, M.Miliucci, R.Murayama, H.Noumi, H.Ohnishi, S.Okada, H.Outa, K.Piscicchia, A.Sakaguchi, F.Sakuma, M.Sato, A.Scordo, K.Shirotori, D.Sirghi, F.Sirghi, S.Suzuki, K.Tanida, T.Toda, M.Tokuda, T.Yamaga, X.Yuan, P.Zhang, Y.Zhang, H.Zhang

Precise lifetime measurement of 4ΛH hypernucleus using in-flight 4He(K-, π0)4ΛH reaction

RADIOACTIVITY 4H(π-) [from 4He(K-, π0), E not given]; measured decay products, Eγ, Iγ; deduced hypernucleus T1/2. Comparison with available data. Experiment (J-PARC E73).

doi: 10.1016/j.physletb.2023.138128
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2023FA05      Appl.Radiat.Isot. 197, 110791 (2023)

Z.Fan, H.Liu, J.Liang, Y.Xiao, D.Yuan, C.Sun, Z.Yang, J.Yang, H.Zhang

Activity determination of 56Mn using extended TDCR-Cerenkov method

RADIOACTIVITY 56Mn(β-) [from 55Mn(n, γ), E thermal]; measured decay products, Eγ, Iγ, Eβ, Iβ; deduced branch ratio of cascades and discrete point of beta emission spectra, anisotropy parameters. Comparison with calculations.

doi: 10.1016/j.apradiso.2023.110791
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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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2023HU10      Phys.Rev. C 107, 044309 (2023)

Z.Huang, G.X.Zhang, C.X.Yuan, G.L.Zhang, D.Mengoni, B.S.Cai, S.P.Hu, H.Q.Zhang, H.B.Sun, J.J.Valiente-Dobon, D.Testov, A.Goasduff, D.Bazzacco, D.R.Napoli, F.Galtarossa, F.Recchia, G.de Angelis, M.Siciliano, R.Menegazzo, S.M.Lenzi

Level scheme study of 91Mo: Weak-coupling approximation in the N=50 region

NUCLEAR REACTIONS 89Y(6Li, X)91Mo, E=34 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ). 91Mo; deduced levels, J, π, transition intensities, angular distribution from oriented nuclei (ADO) ratios, δ, T1/2 for two isomeric states, high-spin states, B(E2), configurations. Comparison with shell-model calculation employing the JUN45 interaction (KSHELL code). GALILEO ψ-ray spectrometer consisting of 25 Compton-suppressed HPGe tapered detectors at Tandem-XTU accelerator (INFN-LNL, Italy).

doi: 10.1103/PhysRevC.107.044309
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2023LI49      Phys.Rev. C 108, L041602 (2023)

T.Li, H.Zhang, X.Wang

Theory of Coulomb excitation of the 229Th nucleus by protons

doi: 10.1103/PhysRevC.108.L041602
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2023LI51      Phys.Rev. C 108, 044604 (2023)

J.-X.Li, H.-F.Zhang

Possibility to synthesize Z > 118 superheavy nuclei with 54Cr projectiles

doi: 10.1103/PhysRevC.108.044604
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2023LI62      Chin.Phys.C 47, 124105 (2023)

J.-X.Li, H.-F.Zhang

Evaporation residue cross sections of superheavy nuclei based on optimized nuclear data

NUCLEAR REACTIONS 238U(48Ca, X), E not given; analyzed available data; deduced the evaporation residue σ in 3n and 4n channels using an optimized method for estimating atomic nucleus masses by combining the finite-range droplet model (FRDM) with the support vector machine algorithm.

doi: 10.1088/1674-1137/ad021f
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2023MA04      Phys.Rev. C 107, 014310 (2023)

N.-N.Ma, Ti.-L.Zhao, W.-Xi.Wang, H.-F.Zhang

Simple deep-learning approach for α-decay half-life studies

RADIOACTIVITY N=90-180(α); A=160-320(α); Z=80-120(α); calculated T1/2. The deep learning algorithm trained directly with sets of experimental α-decay half-lives.

doi: 10.1103/PhysRevC.107.014310
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2023NI11      Nucl.Instrum.Methods Phys.Res. A1057, 168703 (2023)

M.Niu, Z.Long, R.Fan, W.Jiang, J.Liu, Q.Xiu, R.Xu, H.Wang, Zh.Zhou, K.Sun, Zh.Zhang, H.Zhang, H.Yi, Y.Chen, D.Wang, X.Xia, H.Liang

Research on the performance of a diamond detector for the cross-section measurements at CSNS Back-n

NUCLEAR REACTIONS 12C, 6Li(n, α), 12C(n, n'), E=0.00001-100 MeV; measured reaction products, En, In, TOF; deduced the bi-parametric contour plot facilitated the identification of event bands in a bi-parameter experiment (neutron time of flight and deposited energy). Comparison with MATLAB simulations. The Back-n white neutron facility located within the China Spallation Neutron Source (CSNS).

doi: 10.1016/j.nima.2023.168703
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2023QI04      Phys.Rev.Lett. 130, 112501 (2023)

J.Qi, H.Zhang, X.Wang

Isomeric Excitation of 229Th in Laser-Heated Clusters

NUCLEAR REACTIONS 229Th(γ, X)229mTh, E<1 keV; calculated total (E2 + M1) isomeric-excitation σ, production yields. Nuclear excitation by electron capture (NEEC) and nuclear excitation by inelastic electron scattering (NEIES).

doi: 10.1103/PhysRevLett.130.112501
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2023RE11      Phys.Rev. C 108, 044301 (2023)

Z.Ren, J.-B.Lu, G.-X.Dong, Y.Zheng, Y.-H.Wu, T.-J.Gao, P.-Y.Yang, Y.Hao, K.-Y.Ma, X.-G.Wu, C.-B.Li, Z.Huang, G.-X.Zhang, S.-P.Hu, H.-B.Sun, H.-Q.Zhang, D.Testov, J.J.Valiente-Dobon, A.Goasduff, M.Siciliano, F.Galtarossa, D.Mengoni, D.Bazzacco, G.-L.Zhang

Level scheme of 92Nb and observation of an oblate collective rotational band

doi: 10.1103/PhysRevC.108.044301
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2023SH06      Astrophys.J. 945, 41 (2023)

Y.Shen, B.Guo, R.J.deBoer, E.Li, Z.Li, Y.Li, X.Tang, D.Pang, S.Adhikari, C.Basu, J.Su, S.Yan, Q.Fan, J.Liu, C.Chen, Z.Han, X.Li, G.Lian, T.Ma, W.Nan, W.Nan, Y.Wang, S.Zeng, H.Zhang, W.Liu

New Determination of the 12C(α, γ)16O Reaction Rate and Its Impact on the Black-hole Mass Gap

NUCLEAR REACTIONS 12C(11B, 7Li), (11B, 11B), E=50 MeV; measured reaction products. 16O; deduced σ(θ), the asymptotic normalization coefficient (ANC) for the 16O ground state (GS), astrophysical S-factor and the stellar rate. The HI-13 tandem accelerator of China Institute of Atomic Energy (CIAE) in Beijing, China.

doi: 10.3847/1538-4357/acb7de
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2023WA05      Phys.Rev.Lett. 130, 092701 (2023)

L.H.Wang, J.Su, Y.P.Shen, J.J.He, M.Lugaro, B.Szanyi, A.I.Karakas, L.Y.Zhang, X.Y.Li, B.Guo, G.Lian, Z.H.Li, Y.B.Wang, L.H.Chen, B.Q.Cui, X.D.Tang, B.S.Gao, Q.Wu, L.T.Sun, S.Wang, Y.D.Sheng, Y.J.Chen, H.Zhang, Z.M.Li, L.Y.Song, X.Z.Jiang, W.Nan, W.K.Nan, L.Zhang, F.Q.Cao, T.Y.Jiao, L.H.Ru, J.P.Cheng, M.Wiescher, W.P.Liu

Measurement of the 18O(α, γ)22Ne Reaction Rate at JUNA and Its Impact on Probing the Origin of SiC Grains

NUCLEAR REACTIONS 18O(α, γ), E=470-787 keV; measured reaction products, Eγ, Iγ; deduced thick target yields, resonance energies and resonance strengths, total reaction rates. Comparison with available data. The Jinping Underground Nuclear Astrophysics experimental facility (JUNA).

doi: 10.1103/PhysRevLett.130.092701
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2023XI07      Phys.Rev. C 108, L011901 (2023)

M.Xie, W.Ke, H.Zhang, X.-N.Wang

Information-field-based global Bayesian inference of the jet transport coefficient

doi: 10.1103/PhysRevC.108.L011901
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2023XU01      Phys.Lett. B 839, 137789 (2023)

W.Z.Xu, S.Y.Wang, X.G.Wu, H.Jia, C.Liu, H.F.Bai, Y.J.Li, B.Qi, H.Y.Zhang, G.S.Li, Y.Zheng, C.B.Li, L.Mu, A.Rohilla, S.Wang, D.P.Sun, Z.Q.Li, N.B.Zhang, R.J.Guo, X.C.Han, X.Xiao

First observation of high-spin states in 116In and possible new region of chirality

NUCLEAR REACTIONS 116Cd(7Li, X)116In, E=42 MeV; measured reaction products, Eγ, Iγ, γ-γ-coin.; deduced γ-ray energies and relative intensities, partial level scheme, J, π, angular distributions from the oriented states (ADO) ratios, high-spin states, negative-parity band, positive-parity doublet bands. Comparison with the adiabatic and configuration-fixed constrained triaxial relativistic-mean-field and multiparticle plus rotor model calculations. The HI-13 Tandem Accelerator at the China Institute of Atomic Energy in Beijing (CIAE).

doi: 10.1016/j.physletb.2023.137789
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Data from this article have been entered in the XUNDL database. For more information, click here.

2023YA02      Phys.Rev. C 107, 014325 (2023)

M.J.Yang, H.Sagawa, C.L.Bai, H.Q.Zhang

Effects of two-particle--two-hole configurations and tensor force on β decay of magic nuclei

RADIOACTIVITY 34Si, 68,78Ni, 132Sn(β-); calculated T1/2, Gamow-Teller strength distribution with respect to daughter nucleus. Self-consistent Hartree-Fock plus subtracted second random-phase approximation (HF+SSRPA) model with Skyrme EDFs (SGII, SAMi, SAMi-T).Comparison to experimental data.

doi: 10.1103/PhysRevC.107.014325
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2023ZH08      Phys.Rev. C 107, 024305 (2023)

J.Zhang, X.-T.He, Y.-C.Li, H.-Q.Zhang

Parity-doublet bands in the odd-A isotones 237U and 239Pu investigated by a particle-number-conserving method based on the cranked shell model

NUCLEAR STRUCTURE 237U, 239Pu; calculated cranked Nilsson levels near the Fermi surface for neutrons and protons, kinematic moments of inertia and alignments of the parity-doublet rotational bands, neutron and proton orbitals occupation probabilities, contributions of protons to the angular momentum alignments, contributions of neutrons to the moments of inertia. Particle-number-con serving method in the framework of the cranked shell model (PNC-CSM) calculations. Comparison to experimental data.

doi: 10.1103/PhysRevC.107.024305
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2023ZH14      Phys.Rev. C 107, 044310 (2023)

Z.H.Zhao, C.B.Li, K.Y.Ma, X.G.Wu, Y.Zheng, Y.K.Pan, J.L.Wang, H.C.Zhang, Y.C.Hao, X.F.Li, G.S.Li, S.H.Yao, C.Y.He, B.B.Yu, X.P.Cao, S.P.Hu, J.B.Lu, Y.J.Ma, D.Yang, H.D.Wang, G.Y.Liu, L.Li, C.Xu, Y.Y.Cheng

Possible antimagnetic rotational band in 114In

NUCLEAR REACTIONS 110Pd(7Li, 3n)114In, E=26 MeV; analyzed Eγ, Iγ, γγ-coin, γγ(θ)(DCO) data from an experiment reported by 2011Li43 in Eur. Phys. Jour. A 47, 191 (2011) at the HI-13 tandem accelerator of CIAE, Beijing. 114In; deduced high-spin levels, Jπ, multipolarities, bands, possible anti-magnetic rotational band, spherical configurations; predicted B(E2) and I2/B(E2) from classical particle-rotor model calculations. Systematics of yrast states in 102,104,106,108,110Ag and 104,106,108,110,112,114In.

doi: 10.1103/PhysRevC.107.044310
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Data from this article have been entered in the XUNDL database. For more information, click here.

2023ZH22      J.Phys.(London) G50, 045101 (2023)

T.L.Zhao, X.J.Bao, H.F.Zhang

Effect of deformation dependence and mirror nucleus corrections energy on multinucleon transfer reaction cross sections

NUCLEAR REACTIONS 208Pb(136Xe, X), E(cm)=450 MeV; 238U(64Ni, X), E(cm)=307.40 MeV; calculated σ using the dinuclear system (DNS) model, three macroscopic microscopic mass models. Comparison with available data.

doi: 10.1088/1361-6471/acb4b2
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2023ZH23      Phys.Rev. C 107, 064304 (2023)

H.Zhang, D.Bai, Z.Wang, Z.Ren

Complex scaled nonlocalized cluster model with continuum level density

NUCLEAR STRUCTURE 8Be; calculated low-lying resonances state energies, decay widths of the resonant states, phase shifts for α-α scattering. Calculations using complex scaled nonlocalized cluster model (CSNLCM), complex scaled nonlocalized cluster model with the continuum level density (CSNLCM-CLD) and R-matrix method. Comparison to experimental data.

doi: 10.1103/PhysRevC.107.064304
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2023ZH26      Phys.Rev. C 107, 065801 (2023)

H.Zhang, J.Su, Z.H.Li, Y.J.Li, E.T.Li, C.Chen, J.J.He, Y.P.Shen, G.Lian, B.Guo, X.Y.Li, L.Y.Zhang, Y.D.Sheng, Y.J.Chen, L.H.Wang, L.Zhang, F.Q.Cao, W.Nan, W.K.Nan, G.X.Li, N.Song, B.Q.Cui, L.H.Chen, R.G.Ma, Z.C.Zhang, T.Y.Jiao, B.S.Gao, X.D.Tang, Q.Wu, J.Q.Li, L.T.Sun, S.Wang, S.Q.Yan, J.H.Liao, Y.B.Wang, S.Zeng, D.Nan, Q.W.Fan, W.P.Liu

Updated reaction rate of 25Mg(p, γ)26Al and its astrophysical implication

NUCLEAR REACTIONS 25Mg(p, γ), E=117-350 keV; measured Eγ, Iγ, sum of γ energies; deduced γ-ray branching ratios, resonances, resonance strengths, astrophysical reaction rate (T=0.01-2.0 GK), contribution of individual resonances to the reaction rate, ground-state and isomeric state contribution. Comaprison to other experimental data and NACRE compilation. Evaluated the impact of the obtained data on the 26Al yield in stellar environment (code MESA). BGO detector array in nearby 4π geometry composed of 8 identical segments at high-current 400 kV JUNA accelerator (China JinPing underground Laboratory).

doi: 10.1103/PhysRevC.107.065801
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Data from this article have been entered in the XUNDL database. For more information, click here.

2023ZH38      Phys.Rev. C 108, 024314 (2023)

H.C.Zhang, K.Y.Ma, J.X.Teng, Z.H.Zhao, H.Wang, S.Y.Liu, Y.C.Hao, J.B.Lu, Y.J.Ma, D.Yang, X.G.Wu, Y.Zheng, C.B.Li

New positive-parity bands in 110Ag and systematic studies in silver isotopes

NUCLEAR REACTIONS 110Pd(7Li, X)110Ag, E=65 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ). 110Ag; deduced levels, J, π, high-spin states, δ, DCO ratios, positive-parity rotational bands structure, B(M1)/B(E2) ratios for inside band transitions, configurations. Systematics of alignment for the bands, B(M1)/B(E2) ratios and energy staggering parameters in 105Ag, 106Ag, 107Ag, 108Ag, 109Ag, 110Ag. Comparison to particle-rotor model and geometrical model based calculations. Investigated signature inversion in odd-odd and odd-A silver isotopes. Array consisting of 9 Compton-suppressed HPGe detectors, 2 planar-type HPGe detectors, and 1 clover detector at HI-13 tandem accelerator of China Institute of Atomic Energy (CIAE).

doi: 10.1103/PhysRevC.108.024314
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Data from this article have been entered in the XUNDL database. For more information, click here.

2023ZH41      Phys.Rev. C 108, 024602 (2023)

T.L.Zhao, X.J.Bao, H.F.Zhang

Exploring the optimal way to produce Z=100-106 neutron-rich nuclei

NUCLEAR REACTIONS 238U(16O, X), E(cm)=70-160 MeV; calculated capture σ(E). 248Cm(18O, 4n), E*=28-60 MeV;248Cm(18O, 5n), E*=40-60 MeV;248Cm(18O, 6n), E*=46-60 MeV;244Pu(22Ne, 5n), E*=40-56 MeV; calculated evaporation residue σ(E). 248Cm(238U, X)239Bk/240Bk/241Bk/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/255Bk/256Bk/257Bk/258Bk/259Bk/260Bk/240Cf/241Cf/242Cf/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf/257Cf/258Cf/259Cf/260Cf/261Cf/262Cf/263Cf/241Es/242Es/243Es/244Es/245Es/246Es/247Es/248Es/249Es/250Es/251Es/252Es/253Es/254Es/255Es/256Es/257Es/258Es/259Es/260Es/261Es/262Es/263Es/264Es/248Fm/249Fm/250Fm/251Fm/252Fm/253Fm/254Fm/255Fm/256Fm/257Fm/258Fm/259Fm/260Fm/261Fm/262Fm/263Fm/264Fm/265Fm/266Fm/267Fm/250Md/251Md/252Md/253Md/254Md/255Md/256Md/257Md/258Md/259Md/260Md/261Md/262Md/263Md/264Md/265Md/266Md, E(cm)=898.71 MeV; calculated primary and final fragments σ(E). 238U, 244Pu, 248Cm, 249Cf(22O, 2n), (22O, 3n), (22O, 4n), (22O, 5n), (22O, 6n), E*=24-60 MeV; calculated evaporation residue σ(E). 248Cm(238U, X)246Fm/247Fm/248Fm/249Fm/250Fm/251Fm/252Fm/253Fm/254Fm/255Fm/256Fm/257Fm/258Fm/259Fm/260Fm/261Fm/262Fm/263Fm/264Fm/265Fm/253No/254No/255No/256No/257No/258No/259No/260No/261No/262No/263No/264No/265No/266No/267No/258Rf/259Rf/260Rf/261Rf/262Rf/263Rf/264Rf/265Rf/266Rf/267Rf/268Rf/269Rf/265Sg/266Sg/267Sg/268Sg, E(cm)=898.71 MeV; calculated σ(E) of the multinucleon transfer reaction, fusion σ(E). Dinuclear system model (DNS) combined with GEMINI++ for calculating the evaporation residue cross section. Comparison to experimental data.

doi: 10.1103/PhysRevC.108.024602
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2022BA38      Chin.Phys.C 46, 114104 (2022)

C.L.Bai, D.L.Fang, H.Q.Zhang, C.L.Bai, D.L.Fang, H.Q.Zhang

Roles of tensor and isoscalar pairing interactions in β-Decay calculations for possible r-process waiting point nuclei with N ∼ 82 and 126

RADIOACTIVITY 120,122,124,126,128,130,132Cd(β-); calculated T1/2 with the self-consistent Hartree-Fock-Bogoliubov (HFB) theory with the proton-neutron quasi-particle random phase approximation (pnQRPA) based on the Skyrme force. Comparison with available data.

doi: 10.1088/1674-1137/ac80ee
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2022DE15      Chin.Phys.C 46, 061001 (2022)

J.-G.Deng, H.-F.Zhang, X.-D.Sun

New behaviors of α-particle preformation factors near doubly magic 100Sn

RADIOACTIVITY 104,106,108,110Te, 108,110,112Xe, 114Ba, 212,214,216,218Po, 212,214,216,218,220,222Rn, 214,216,218,220,222,224,226Ra(α); calculated T1/2 within the generalized liquid drop model. Comparison with available data.

doi: 10.1088/1674-1137/ac5a9f
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2022DE22      Eur.Phys.J. A 58, 165 (2022)

J.-G.Deng, H.-F.Zhang

Probing the robustness of N = 126 shell closure via the α decay systematics

RADIOACTIVITY 186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 194,196,198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 202,204,206,208,210,212,214,216,218,220,222,224,226Ra, 208,210,212,214,216,218,220,222,224,226,228,230,232Th, 214,216,218,220,222,224,226,228,230,232,234,236,238U(α); calculated T1/2 within the generalized liquid drop model (GLDM); deduced α-particle preformation factors. Comparison with experimental data.

doi: 10.1140/epja/s10050-022-00813-8
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2022GA07      Nucl.Instrum.Methods Phys.Res. B514, 15 (2022)

Z.Gao, X.Zhang, Y.Ju, L.Chen, H.L.Ge, Y.Zhang, F.Ma, H.Zhang, G.Shi, Z.Chen, R.Han, G.Tian, F.Shi, B.Liu, X.Zhang

Nuclear reaction measurements of 80.5 MeV/u 12C beam bombarding on C, Cu, W, Au, Pb targets

NUCLEAR REACTIONS C, Cu, W, 197Au, Pb(12C, X), E=80.5 MeV/nucleon; measured reaction products; deduced σ(θ, E). Institute of Modern Physics, Chinese Academy of Sciences.

doi: 10.1016/j.nimb.2022.01.003
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2022HU12      Phys.Lett. B 834, 137484 (2022)

M.H.Huang, Z.G.Gan, Z.Y.Zhang, L.Ma, J.G.Wang, M.M.Zhang, H.B.Yang, C.L.Yang, X.Y.Huang, Z.Zhao, S.Y.Xu, L.X.Chen, X.J.Wen, Y.F.Niu, C.X.Yuan, Y.L.Tian, Y.S.Wang, J.Y.Wang, M.L.Liu, Y.H.Qiang, W.Q.Yang, H.B.Zhang, Z.W.Lu, S.Guo, W.X.Huang, Y.He, Z.Z.Ren, S.G.Zhou, X.H.Zhou, H.S.Xu, V.K.Utyonkov, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov

α decay of the new isotope 204Ac

RADIOACTIVITY 204,205Ac(α) [from 169Tm(40Ca, xn), E=202, 210, 212, 214 MeV using SHANS2 separator at CAFE2 and SHANS separator at HRIFL, Lanzhou accelerator facility]; 200Fr, 196At(α) [from 204Ac α-decay chain]; measured evaporation residues (ERs), Eα, (ER)α-α-α correlated events, production cross sections, T1/2 of decays using two multiwire proportional counters for implanted events, double-sided silicon strip detectors (DSSSDs) for α particles, and a segmented clover Ge detector for γ radiation. 204,205Ac, 200Fr, 196At; deduced T1/2 of decays of ground-state decays, and Eα values, reduced α-width in Rasmussen formalism, favored α decay for 204Ac decay. 204Ac(p); no proton decay events observed. 201,201m,202,202m,203,204,205Fr, 204,205,206Ra(α); observed α spectra, (ERs)-α-α-correlated events. Comparison with previous available experimental results. Systematics of experimental and theoretical T1/2 and Q(α) values for 196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211At, 198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213Fr, 203,204,205,206,207,208,209,210,211,212,213,214,215Ac, 211,212,213,214,215,216,217Pa, using Hartree-Fock-BCS (HFBSC) method, and macroscopic-microscopic (MM) mass formula for theory.

doi: 10.1016/j.physletb.2022.137484
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2022HU22      Phys.Rev. C 106, 064331 (2022)

Z.Huang, G.X.Zhang, G.L.Zhang, S.P.Hu, S.M.Lenzi, D.Mengoni, J.L.Ferreira, Y.F.Lv, J.B.Lu, B.Paes, E.N.Cardozo, H.Q.Zhang, H.B.Sun, J.J.Valiente-Dobon, D.Testov, A.Goasduff, D.Bazzacco, P.R.John, D.R.Napoli, F.Galtarossa, F.Recchia, G.de.Angelis, M.Siciliano, R.Menegazzo, J.Lubian

Level scheme study of 92Mo: Searching for evidence of core excitation

NUCLEAR REACTIONS 89Y(6Li, 3n), E=34 MeV; measured Eγ, Iγ; γγ-coin, γγ(θ). 92Mo; deduced levels, J, π, δ, B(E1), T1/2 of excited states, high-spin states, angular distribution from the oriented nuclei (ADO) ratio, configurations. Comparison to JUN45 and JJGLEM shell-model calculation. GALILEO γ-array consisting of 25 Compton suppressed HPGe and 8 BGO crystals served as the anti-Compton shield of each HPGe at XTU Tandem accelerator (INFN Legnaro National Laboratory).

doi: 10.1103/PhysRevC.106.064331
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2022LI27      Phys.Rev. C 105, 054606 (2022)

J.-X.Li, H.-F.Zhang

Predictions for the synthesis of the Z=119 superheavy element

NUCLEAR REACTIONS 238U, 237Np, 242,244Pu, 243Am, 245,248Cm, 249Bk, 249Cf(48Ca, X), (48Ca, 2n), (48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E*=20-60 MeV; calculated evaporation residue σ(E). 250Cf(45Sc, X), 244Cm(51V, X), 240Pu(55Mn, X), E*=30-60; calculated potential energy surface, evaporation residue σ(E). 248,249,250,251,252Cf(45Sc, 3n); calculated survival probability. 252,253,254Es(48Ca, 3n), E*=34 MeV;248,249,250,251,252Cf(45Sc, 3n), E*=38-40 MeV; 247,248,249Bk(50Ti, 3n), E*=35 MeV;242,244,243,244,245,246,247,248,249(51V, 3n), E*=35-38 MeV;241,242,243Am, E*=38 MeV;(54Cr, 3n), 236,238,239,240,241,242,243,244Pu(55Mn, 3n), E*=37-41 MeV; calculated evaporation residue σ(E) at maximum production energy. Calculations in the framework of dinuclear system (DNS) model. Comparison to available experimental data.

doi: 10.1103/PhysRevC.105.054606
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2022LI28      Few-Body Systems 63, 43 (2022)

W.P.Liu, Z.H.Li, J.J.He, X.D.Tang, G.Lian, J.Su, Y.P.Shen, Z.An, F.Q.Chao, J.J.Chang, L.H.Chen, H.Chen, X.J.Chen, Y.H.Chen, Z.J.Chen, B.Q.Cui, X.C.Du, X.Fang, C.B.Fu, L.Gan, B.Guo, Z.Y.Han, X.Y.Guo, G.Z.He, J.R.He, A.Heger, S.Q.Hou, H.X.Huang, N.Huang, B.L.Jia, L.Y.Jiang, S.Kubono, J.M.Li, M.C.Li, K.A.Li, E.T.Li, T.Li, Y.J.Li, M.Lugaro, X.B.Luo, H.Y.Ma, S.B.Ma, D.M.Mei, W.Nan, W.K.Nan, N.C.Qi, Y.Z.Qian, J.C.Qin, J.Ren, C.S.Shang, L.T.Sun, W.L.Sun, W.P.Tan, I.Tanihata, S.Wang, P.Wang, Y.B.Wang, Q.Wu, S.W.Xu, S.Q.Yan, L.T.Yang, Y.Yang, X.Q.Yu, Q.Yue, S.Zeng, L.Zhang, H.Zhang, H.Y.Zhang, L.Y.Zhang, N.T.Zhang, P.Zhang, Q.W.Zhang, T.Zhang, X.P.Zhang, X.Z.Zhang, W.Zhao, J.F.Zhou, Y.Zho

Progress of Underground Nuclear Astrophysics Experiment JUNA in China

NUCLEAR REACTIONS 12C(α, γ), 13C(α, n), 25Mg(p, γ), 19F(p, α), E(cm)<600 keV; measured reaction products; deduced yields near the Gamow window. Comparison with available data.

doi: 10.1007/s00601-022-01735-3
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2022LI51      Phys.Rev. C 106, 034613 (2022)

J.-X.Li, H.-F.Zhang

Predictions for the synthesis of the Z=120 superheavy element

NUCLEAR REACTIONS 252Es(45Sc, X), (45Sc, 3n), (45Sc, 4n), E*=25-60 MeV; calculated evaporation residue σ(E), capture σ(Ε), survival probability, complete fusion probability, potential energy surface. 257Fm(50Ca, 3n), (50Ca, 4n), (50Ca, 5n), (51Ca, 3n), (51Ca, 4n), (51Ca, 5n), (52Ca, 3n), (52Ca, 4n), (52Ca, 5n), E*=34-54 MeV; 252Es(55Sc, 3n), (55Sc, 4n), (55Sc, 5n), (56Sc, 3n), (56Sc, 4n), (56Sc, 5n), (57Sc, 3n), (57Sc, 4n), (57Sc, 5n), E*=36-57 MeV; 251Cf(56Ti, 3n), (56Ti, 4n), (56Ti, 5n), (57Ti, 3n), (57Ti, 4n), (57Ti, 5n), (58Ti, 3n), (58Ti, 4n), (58Ti, 5n), E*=36-60 MeV; 249Bk(58V, 3n), (58V, 4n), (58V, 5n), (59V, 3n), (59V, 4n), (59V, 5n), (60V, 3n), (60V, 4n), (60V, 5n), E*=37-59 MeV; 248Cm(59Cr, 3n), (59Cr, 4n), (59Cr, 5n), (60Cr, 3n), (60Cr, 4n), (60Cr, 5n), (61Cr, 3n), (61Cr, 4n), (61Cr, 5n), E*=36-57 MeV; 243Am(64Mn, 3n), (64Mn, 4n), (64Mn, 5n), (65Mn, 3n), (65Mn, 4n), (65Mn, 5n), (66Mn, 3n), (66Mn, 4n), (66Mn, 5n), E*=37-58 MeV;E*=34-60; calculated evaporation residue σ(E) at maximum production energy. Calculations in the framework of dinuclear system (DNS) model. Comparison to available experimental data.

doi: 10.1103/PhysRevC.106.034613
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2022LI57      Phys.Rev. C 106, 044601 (2022)

J.-X.Li, W.-X.Wang, H.-F.Zhang

Properties and synthesis of the superheavy nucleus 298114Fl

NUCLEAR REACTIONS 238U(64Ti, X), E*=32-60 MeV;242Pu(48Ca, X), E*=25-60 MeV; calculated capture σ(E), fusion probabilities, fusion barrier, potential-energy surfaces, survival probabilities in the 4n channels. 238U(64Ti, 4n)298Fl, E*=33-60 MeV; 242Pu, 244Pu(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E*=30-60 MeV; calculated evaporation residue σ(E). Dinuclear system model. Suggested 238U(64Ti, 4n) at 43 MeV excitation energy as preferred way for the synthesis of 298Fl. Comparison with available experimental data.

NUCLEAR STRUCTURE 284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304Fl, 292HS, 293Mt, 294Ds, 295Rg, 296Cn, 297Nh, 299Mc, 300Lv, 301Ts, 302Og, 303119, 304120; calculated S(n), S(2n). Finite-range droplet model (FRDM2012). Discuss the evidence that 298Fl could be spherical double-magic nucleus and also the center of the stability island of superheavy nuclei.

RADIOACTIVITY 284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304Fl, 292HS, 293Mt, 294Ds, 295Rg, 296Cn, 297Nh, 299Mc, 300Lv, 301Ts, 302Og, 303119, 304120(α), (SF); calculated Q-value, T1/2. Finite-range droplet model (FRDM2012).

doi: 10.1103/PhysRevC.106.044601
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2022RE11      Phys.Rev. C 106, 024323 (2022), Erratum Phys.Rev. C 107, 049902 (2023)

Z.Ren, J.-B.Lu, G.-L.Zhang, Y.-H.Wu, T.-J.Gao, K.-Y.Ma, Z.Huang, G.-X.Zhang, M.-L.Wang, S.-P.Hu, H.-B.Sun, H.-Q.Zhang, D.Testov, P.R.John, J.J.Valiente-Dobon, A.Goasduff, M.Siciliano, F.Galtarossa, D.Mengoni, D.Bazzacco

Reinvestigation of the level structures of the N=49 isotones 89Zr and 91Mo

NUCLEAR REACTIONS 89Y(6Li, 4n2p)89Zr, (6Li, 4n)91Mo, E=34 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(ADO), (particle)γ-coin using GALILEO array with 25 BGO-Compton-suppressed HPGe detectors for γ rays, and EUCLIDES 4π Si-ball array for charged particles at the Tandem-XTU accelerator of INFN-LNL, Legnaro. 89Zr, 91Mo; deduced high-spin levels, J, π, ADO ratios, multipolarities, configurations. 91Nb, 92Mo; deduced ADO ratios for certain γ-transitions. Comparison with spherical-basis shell-model calculations.

NUCLEAR STRUCTURE 89Zr, 91Mo; calculated levels, J, π, components of the wave functions and their partitions for spherical configurations for protons and neutrons. Comparison with experimental data. Systematics of energies in N=49 isotones: 9/2+, 13/2+, 17/2+, 21/2+, 23/2+ and 25/2+ states in 89Zr, 91Mo, 93Ru, 95Pd, and those of 8+, 9+, 10+, 12+, 13+ and 14+ in 88Y, 90Nb, 92Tc, 94Rh.

doi: 10.1103/PhysRevC.106.024323
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2022WA02      Nucl.Instrum.Methods Phys.Res. B512, 49 (2022)

L.H.Wang, Y.P.Shen, J.Su, X.Y.Li, W.Q.Yan, J.J.He, L.Y.Zhang, B.Liao, Y.F.Wu, Y.D.Sheng, Z.M.Li, Y.J.Chen, L.Y.Song, X.Z.Jiang, G.Lian, W.Nan, W.K.Nan, L.Zhang, F.Q.Cao, C.Chen, N.Song, H.Zhang, W.P.Liu

Development of irradiation-resistant enriched 12C targets for astrophysical 12C(α, γ)16O reaction measurements

NUCLEAR REACTIONS 12C(p, γ), E=370 keV; 12C(p, α), E=740 keV; measured reaction products, Eγ, Iγ; deduced yields. The China JinPing underground Laboratory (CJPL).

doi: 10.1016/j.nimb.2021.11.020
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2022XI05      Nucl.Phys. A1023, 122443 (2022)

Y.-Z.Xing, W.-X.Wang, H.-F.Zhang, Y.-M.Zheng

General chaotic behaviors of heavy ion collisions at intermediate energy based on dynamical transport model

NUCLEAR REACTIONS 40Ca(40Ca, X), E=800 MeV/nucleon; analyzed available data; deduced the multifragmentation entropy, information dimension and the dynamical fluctuations of fragment mass distribution in the final state of the reaction.

doi: 10.1016/j.nuclphysa.2022.122443
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2022YA20      Phys.Rev. C 106, 014319 (2022)

M.J.Yang, C.L.Bai, H.Sagawa, H.Q.Zhang

Gamow-Teller transitions in magic nuclei calculated by the charge-exchange subtracted second random-phase approximation

NUCLEAR STRUCTURE 48Ca, 90Zr, 132Sn, 208Pb; calculated Gamow-Teller (GT) strength distributions as function of excitation energy and peak height; evaluated quenching factors of the Ikeda sum rule due to couplings to two-particle two-hole (2p-2h) configurations, effects of tensor interactions on the excitation energies and the quenching factors of GT strength distributions. Self-consistent Hartree-Fock (HF) plus charge-exchange subtracted second random-phase approximation (SSRPA) calculations with several different Skyrme energy density functions (EDFs). Comparison with experimental data.

doi: 10.1103/PhysRevC.106.014319
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2022ZH13      Nucl.Phys. A1021, 122420 (2022)

T.Zhao, H.Zhang

A new method to improve the generalization ability of neural networks: A case study of nuclear mass training

doi: 10.1016/j.nuclphysa.2022.122420
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2022ZH14      Phys.Rev. C 105, 034339 (2022)

H.Zhang, B.Qi, X.D.Wang, H.Jia, S.Y.Wang

Influence of moments of inertia on transverse wobbling mode in odd-mass nuclei

NUCLEAR STRUCTURE 105Pd; calculated yrast and yrare bands energies, reduced transition probabilities B(E2), B(M1), ratios B(E2)out/B(E2)in and B(M1)/B(E2)in, root-mean square values of the core angular momentum components as functions of spin, probability distribution of the angular momentum orientation. Triaxial particle rotor model. Calculations are performed with different sets of Moment of Inertia parameters (e.g. rigid body, hydrodynamical, in between). Comparison to experimental data.

doi: 10.1103/PhysRevC.105.034339
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2022ZH18      Phys.Scr. 97, 025303 (2022)

H.-H.Zhang, H.-L.Wang, H.i-Y.Meng, M.-L.Liu, B.Ding

Impact of the Coriolis interaction on the potential landscape evolution across the nuclide chart: Systematic total-Routhian-surface calculations

NUCLEAR STRUCTURE Z>20; analyzed available data; deduced rotational structure properties along the yrast line for 766 observed even-even nuclei in thenuclide chart by means of the approach of pairing-deformation self-consistent total Routhian surface calculations in three-dimensional deformation space.

doi: 10.1088/1402-4896/ac49ae
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2022ZH27      Phys.Rev. C 105, 054317 (2022)

H.Zhang, D.Bai, Z.Wang, Z.Ren

Complex scaled nonlocalized cluster model for 8Be

NUCLEAR STRUCTURE 8Be; calculated energy surface of the ground state and exited states, energies and widths of resonances. Complex scaling method (CSM) combined with the nonlocalized cluster model. Comparison to experimental data.

doi: 10.1103/PhysRevC.105.054317
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2022ZH38      Chin.Phys.C 46, 044103 (2022)

T.-L.Zhao, H.-F.Zhang

A neural network approach based on more input neurons to predict nuclear mass

NUCLEAR STRUCTURE Z=1-118; calculated atomic masses using the neural network (NN) approach. Comparison with available data.

doi: 10.1088/1674-1137/ac3e5b
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2022ZH45      Phys.Rev. C 106, 024305 (2022)

M.M.Zhang, Y.L.Tian, Y.S.Wang, Z.Y.Zhang, Z.G.Gan, H.B.Yang, M.H.Huang, L.Ma, C.L.Yang, J.G.Wang, C.X.Yuan, C.Qi, A.N.Andreyev, X.Y.Huang, S.Y.Xu, Z.Zhao, L.X.Chen, J.Y.Wang, M.L.Liu, Y.H.Qiang, G.S.Li, W.Q.Yang, R.F.Chen, H.B.Zhang, Z.W.Lu, X.X.Xu, L.M.Duan, H.R.Yang, W.X.Huang, Z.Liu, X.H.Zhou, Y.H.Zhang, H.S.Xu, N.Wang, H.B.Zhou, X.J.Wen, S.Huang, W.Hua, L.Zhu, X.Wang, Y.C.Mao, X.T.He, S.Y.Wang, W.Z.Xu, H.W.Li, Y.F.Niu, L.Guo, Z.Z.Ren, S.G.Zhou

Fine structure in the α decay of the 8+ isomer in 216, 218U

RADIOACTIVITY 216,216m,218,218mU(α)[218U from 182W(40Ar, 4n), E=190 MeV, 184W(40Ca, 2nα), E=206 MeV, 216U from 180W(40Ar, 4n), E=191 MeV]; measured evaporation residues (EVRs), Eα, Iα, (EVR)α12-correlations, T1/2 using position-sensitive strip detectors (PSSDs) for α detection, and SHANS separator at HIRFL-Lanzhou. 216,216m,218,218mU; deduced T1/2, Q-values, α-branching ratio, α-decay hindrance factors. 204Rn, 208,210Ra, 212,214Th(α)[from 216,218U α-decay chains]; measured Eα, T1/2. 212Th; deduced level, J, π, identification of the first 2+ state. 215Ra, 212,213,216Ac, 211,212,213,214,216,216m,217Th, 216,217,217m,218Pa, 217,218,219U; observed Eα from their decays from (EVR)α-correlations. Comparison with previous experimental data.

doi: 10.1103/PhysRevC.106.024305
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2022ZH47      Nucl.Phys. A1027, 122510 (2022)

T.L.Zhao, X.J.Bao, H.F.Zhang

Improvement of evaporation residual cross sections for superheavy nuclei using a neural network method

NUCLEAR REACTIONS 248Cm(18O, X), 242,244Pu(22Ne, X), 238U(26Mg, X), 249Cf(15N, X), 249Bk(16O, X), 248Cm(19F, X), 241Am(22Ne, X), 238U(30Si, X), 249Cf(18O, X), 248Cm(22Ne, X), 249Bk(22Ne, X), 248Cm(26Mg, X), 238U(36S, X), (34S, X), 226Ra(48Ca, X), 232Th(48Ca, X), 238U(48Ca, X), 237Np(48Ca, X), 239,240,242,244Pu(48Ca, X), 243Am(48Ca, X), 245,248Cm(48Ca, X), 249Bk(48Ca, X), 249Cf(48Ca, X)Rf/Db/Sg/Bh/Ds/Hs/Nh/Cn/Fl/Mc/Lv/Ts/Og, E not given; calculated evaporation residual cross section (ERCS) using the neural network method. Comparison with available data.

doi: 10.1016/j.nuclphysa.2022.122510
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2022ZH55      J.Phys.(London) G49, 105104 (2022)

T.L.Zhao, H.F.Zhang

Unified description of α decay and cluster radioactivity using the neural network approach and universal decay law

RADIOACTIVITY 256Fm(46Ar), (48Ar), (48Ca), (50Ca), (52Ca), 252No(44Ar), 254No(44Ar), (46Ar), (48Ca), 256No(44Ar), (46Ar), (48Ar), (48Ca), (50Ca), 240,242Cf(30Si), (32Si), 242Cf(34Si), (36S), 244Cf(32Si), (34Si), (36S), (38Si), 246Cf(34Si), (36S), (38Si), (40Si), 248Cf(38Si), (40S), (42S), (44Ar), 250Cf(40S), (42S), (44Ar), (46Ar), 252Cf(42S), (44Ar), (46Ar), (48Ar), 254Cf(46Ar), (48Ar), 254Cf(46Ar), (48Ar), 246,248Fm(36S), (38S), 248Fm(40S), 250Fm(38S), (40S), (42S), (44Ar), 252Fm(40S), (42S), (44Ar), (46Ar), (48Ca), 254Fm(42S), (44Ar), (46Ar), (48Ca), (50Ca); calculated cluster radioactivity T1/2 using three UDL formulas as well as two neural network methods.

doi: 10.1088/1361-6471/ac8b26
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2022ZH60      Nature(London) 610, 656 (2022)

L.Zhang, J.He, R.J.deBoer, M.Wiescher, A.Heger, D.Kahl, J.Su, D.Odell, Y.Chen, X.Li, J.Wang, L.Zhang, F.Cao, H.Zhang, Z.Zhang, X.Jiang, L.Wang, Z.Li, L.Song, H.Zhao, L.Sun, Q.Wu, J.Li, B.Cui, L.Chen, R.Ma, E.Li, G.Lian, Y.D.Sheng, Z.Li, B.Guo, X.Zhou, Y.Zhang, H.Xu, J.Cheng, W.Liu

Measurement of 19F(p, γ)20Ne reaction suggests CNO breakout in first stars

NUCLEAR REACTIONS 19F(p, γ), E(cm)<400 keV; measured reaction products, Eγ, Iγ; deduced yields, S-factor, resonance strengths, astrophysical reaction rates. Comparison with available data. The Jinping Underground Nuclear Astrophysics Experiment (JUNA).

doi: 10.1038/s41586-022-05230-x
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2022ZH61      Phys.Rev. C 106, 044604 (2022)

H.Zhang, W.Wang, X.Wang

Nuclear excitation cross section of 229Th via inelastic electron scattering

NUCLEAR REACTIONS 229Th(e, e'), E<1 GeV; calculated σ(E) of the isomeric 1+ state excitation, contributions from the E2 or the M1 channels to the σ(E). Dirac distorted wave Born approximation (DWBA) calculations. Calculations show that inelastic scattering at energies below 100 eV is most efficient for the isomer excitation.

doi: 10.1103/PhysRevC.106.044604
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2022ZH67      Phys.Rev. C 106, 055803 (2022)

L.Y.Zhang, J.Su, J.J.He, R.J.deBoer, D.Kahl, M.Wiescher, D.Odell, Y.J.Chen, X.Y.Li, J.G.Wang, L.Zhang, F.Q.Cao, H.Zhang, Z.C.Zhang, T.Y.Jiao, Y.D.Sheng, L.H.Wang, L.Y.Song, X.Z.Jiang, Z.M.Li, E.T.Li, S.Wang, G.Lian, Z.H.Li, B.Guo, X.D.Tang, L.T.Sun, Q.Wu, J.Q.Li, B.Q.Cui, L.H.Chen, R.G.Ma, N.C.Qi, W.L.Sun, X.Y.Guo, P.Zhang, Y.H.Chen, Y.Zhou, J.F.Zhou, J.R.He, C.S.Shang, M.C.Li, J.P.Cheng, W.P.Liu

Direct measurement of the astrophysical 19F(p, αγ)16O reaction in a deep-underground laboratory

NUCLEAR REACTIONS 19F(p, αγ), E(cm)=72.4-344 keV; measured Eγ, Iγ; deduced astrophysical S-factor, thermonuclear astrophysical reaction rates (range 0.05–1 GK), contributions from different channels. R-matrix analysis with AZURE2 together with a MCMC Bayesian uncertainty estimation. Comparison to other experimental data. 4π BGO γ-array with proton beam from JUNA accelerator at China JinPing underground Laboratory (CJPL).

doi: 10.1103/PhysRevC.106.055803
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2021DE07      Chin.Phys.C 45, 024104 (2021)

J.-G.Deng, H.-F.Zhang

Systematic study of α decay half-lives within the Generalized Liquid Drop Model with various versions of proximity energies

RADIOACTIVITY 148Gd, 150,154Dy, 154Er, 154,158Yb, 158,162Hf, 160,164,168W, 162,168,172,186Os, 168,174,178,182,190Pt, 174,178,182,186Hg, 180,186,190Pb, 186,194,198,202,206,212,216Po, 194,200,204,208,212,216,220Rn, 202,208,216,220,224Ra, 208,214,218,222,226,230Th, 218,224,230,234U, 228,232,236,240,244Pu, 236,240,244,248,252Cf, 244,252,256Fm, 256No, 256,260Rf, 264,270Hs, 286Fl, 290Lv, 294Og(α); calculated T1/2.

doi: 10.1088/1674-1137/abcc5a
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2021GU25      Phys.Rev. C 104, L041902 (2021)

Y.Guo, J.Liao, E.Wang, H.Xing, H.Zhang

Hyperon polarization from the vortical fluid in low-energy nuclear collisions

doi: 10.1103/PhysRevC.104.L041902
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2021HE09      Chin.Phys.C 45, 014110 (2021)

Y.He, X.Yu, H.-F.Zhang

Improved empirical formula for α particle preformation factor

RADIOACTIVITY 186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220Po, 191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221At, 194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226Rn, 206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225Ac, 209Th, 224,225,226,227,228,229,230,231,232Th, 217,218,219,220,221,222,223,224,225,226,227,228,229,230,231Pa, 219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238U, 229,230,231,232,233,234,235,236,237,238,239,240,241,242,243Am, 233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250Cm, 245,247Bk, 237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255Cf, 246,247,248,249,250,251,252,253,254,255Es, 244,245,246,247,248,249,250,251,252,253,254,255,256,257Fm, 247,248,249,250,251,252,253,254,255,256,257Md, 251,252,253,254,255,256,257,258No, 253,255,257,259Lr(α); calculated T1/2. Comparison with available data.

doi: 10.1088/1674-1137/abc684
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2021HO04      Nucl.Phys. A1005, 121971 (2021)

D.Hou, A.Huang, J.Liao, S.Shi, H.Zhang

Chirality and Magnetic Field

doi: 10.1016/j.nuclphysa.2020.121971
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2021HU12      Eur.Phys.J. A 57, 137 (2021)

Z.Huang, G.X.Zhang, S.P.Hu, B.Paes, E.N.Cardozo, J.L.Ferreira, M.J.Ermamatov, G.L.Zhang, J.B.Lu, M.Mazzocco, Y.F.Lv, H.Q.Zhang, H.B.Sun, D.Testov, P.R.John, J.J.Valiente-Dobon, A.Goasduff, M.Siciliano, F.Galtarossa, F.Recchia, D.Mengoni, D.Bazzacco, J.Lubian, X.B.Qin, H.M.Zhao

Angular distribution of γ rays emitted by oriented nuclei: the case of 92Mo formed in the reaction 6Li + 89Y

NUCLEAR REACTIONS 89Y(6Li, X)92Mo, E=34 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, J, π, γ-ray angular distributions, E1, M2 transition strengths, mixing ratios and T1/2. Comparison with the NushellX calculation using the jjglem interaction.

doi: 10.1140/epja/s10050-021-00443-6
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2021MA15      Phys.Rev. C 103, 024302 (2021)

K.Y.Ma, H.Wang, H.N.Pan, J.B.Lu, Y.J.Ma, D.Yang, Q.Y.Yang, X.Guan, J.Q.Wang, S.Y.Liu, H.C.Zhang, X.G.Wu, Y.Zheng, C.B.Li

High-spin states and possible chirality in odd-odd 110Ag

NUCLEAR REACTIONS 110Pd(7Li, 3nα)110Ag, E=46 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) using Compton-suppressed HPGe detectors, two planar-type HPGe detectors, and one clover HPGe detector at the HI-13 tandem accelerator of CIAE-Beijing. 110Ag; deduced high-spin levels, J, π, bands, multipolarities, alignments, configurations, moment of inertia plots, staggering parameters, B(M1)/B(E2), chiral doublet bands. Comparison with Cranked shell model calculations.

doi: 10.1103/PhysRevC.103.024302
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2021MA17      Chin.Phys.C 45, 024105 (2021)

N.-N.Ma, X.-J.Bao, H.-F.Zhang

Diffuseness effect and radial basis function network for optimizing α decay calculations

RADIOACTIVITY 256Rf, 258Rf, 263Rf, 257,258,259Db, 263Db, 259,260,261,262Sg, 269Sg, 271Sg, 260Bh, 261Bh, 264Bh, 266,267Bh, 270Bh, 272Bh, 274Bh, 264,265,266,267Hs, 270Hs, 273Hs, 268Mt, 274,275,276Mt, 278Mt, 267Ds, 269,270,271Ds, 273Ds, 277Ds, 281Ds, 272Rg, 274Rg, 278,279,280Rg, 281Cn, 285Cn, 278Nh, 282,283,284,285,286Nh, 286,287,288,289Fl, 287,288,289,290Mc, 290,291,292,293Lv, 293,294Ts, 294Og, 252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288Rf, 272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310Fl, 286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316119, 292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318120(α); calculated T1/2. Comparison with available data.

doi: 10.1088/1674-1137/abcc5c
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2021QI07      J.Phys.(London) G48, 055102 (2021)

B.Qi, H.Zhang, S.Y.Wang, Q.B.Chen

Influence of triaxial deformation on wobbling motion in even-even nuclei

NUCLEAR STRUCTURE 110Ru; analyzed available data; deduced energy levels, J, π, influence of triaxial deformation on the purely collective form of wobbling motion.

doi: 10.1088/1361-6471/abcdf7
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2021ST19      Eur.Phys.J. A 57, 334 (2021)

V.Starastsin, A.Demyanova, A.Danilov, A.Ogloblin, S.Dmitriev, S.Goncharov, Ch.-J.Lin, L.Yang, D.-X.Wang, H.-M.Jia, F.-P.Zhong, F.Yang, Y.-J.Yao, Sh.-H.Zhong, P.-W.Wen, N.R.Ma, H.-Q.Zhang, D.Janseitov, N.Burtebayev, S.Khlebnikov, G.Adamian, N.Antonenko

Structures of the excited states in 9Be studied by scattering of 23 MeV deuterons

NUCLEAR REACTIONS 9Be(d, d), E=23 MeV; measured reaction products; deduced σ(θ), excited state energies, J, π, resonance widths, B(Eλ), form factors. The distorted wave Born approximation (DWBA) and modified diffraction model (MDM).

doi: 10.1140/epja/s10050-021-00643-0
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2021WA56      J.Phys.(London) B54, 244001 (2021)

W.Wang, H.Zhang, X.Wang

Strong-field atomic physics meets 229Th nuclear physics

RADIOACTIVITY 229Th(IT); analyzed available data; calculated electronic excitation σ, flux density of the recolliding electron, ionization probabilities, nuclear isomeric excitation probabilities. Recollision-induced nuclear excitation (RINE).

doi: 10.1088/1361-6455/ac45ce
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2021WE04      Chin.Phys.C 45, 024109 (2021)

K.Wei, H.-F.Zhang, Z.-X.He, X.-Y.Wang, S.-Q.Guo, B.T.Hu

Multi-parameter global calculations of fission fragments using a simplified two-dimensional scission-point model

NUCLEAR REACTIONS 233,235U(n, F), E=6.54 MeV; 239Pu(n, F), E=6.84 MeV; calculated charge and mass distributions, yields. Comparison with available data.

doi: 10.1088/1674-1137/abd083
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2021WU12      Phys.Rev. C 104, 054303 (2021)

D.Wu, C.L.Bai, H.Sagawa, S.Nishimura, H.Q.Zhang

β-delayed one-neutron emission probabilities within a neural network model

RADIOACTIVITY Z=2-57(β-n); calculated β--delayed one-neutron emission probabilities P1n using machine learning (ML) technique and feed-forward neural network (FNN) with root mean squared Prop (RMSProp) method; analyzed correlations between P1n, half-lives, Q-values, neutron shell effects, distance from the first β--delayed neutron emitter, and competitions between β--delayed one- and two- neutron emissions P1n and P2n. 109,110,111,112,113,114,115,116Tc, 116,117,118,119,120,121Ru, 118,119,120,121,122,123,124Rh, 121,122,123,124,125,126,127,128Pd, 124,125,126,127,128,129Ag, 127,128,129,130Cd(β-n); 79Cu, 80Zn, 81Ga, 128Pd, 129Ag, 130Ag(β-n); calculated β--delayed one-neutron emission probabilities P1n using ML-FNN techniques, and compared with experimental and evaluated data in literature, and with theoretical calculations using FRDM12+(Q)RPA+HF and RHB+RQRPA approaches. Relevance to r-process nuclei in nucleosynthesis, and waiting-point nuclei at N=50 and N=82.

doi: 10.1103/PhysRevC.104.054303
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2021XI02      Phys.Rev. C 103, 034911 (2021)

M.Xie, X.-N.Wang, H.-Z.Zhang

γ-hadron spectra in p + Pb collisions at √ sNN = 5.02 TeV

doi: 10.1103/PhysRevC.103.034911
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2021YA14      Phys.Rev. C 103, 054308 (2021)

M.J.Yang, C.L.Bai, H.Sagawa, H.Q.Zhang

Effects of the Skyrme tensor force on 0+, 2+, and 3- states in 16O and 40C nuclei within the second random-phase approximation

NUCLEAR STRUCTURE 16O, 40Ca; calculated isoscalar and isovector strength distributions and energy moments of the monopole (0+), quadrupole (2+) and octupole (3-) transitions B(E0), B(E2) and B(E3), major 1p-1h and 2p-2h configurations; deduced major impact of tensor force in SGII+Te1 on the coupling between 1p-1h and 2p-2h model spaces. Subtracted second random-phase approximation (SSRPA) method with Skyrme energy density functional. Comparison with experimental data.

doi: 10.1103/PhysRevC.103.054308
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2021ZH01      Phys.Rev.Lett. 126, 012301 (2021)

H.Zhang, J.Liao, E.Wang, Q.Wang, H.Xing

Deciphering the Nature of X(3872) in Heavy Ion Collisions

doi: 10.1103/PhysRevLett.126.012301
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2021ZH05      Nucl.Phys. A1005, 121762 (2021)

H.Zhang, D.Hou, J.Liao

Rotation Effects on Mesonic Condensation in Isospin Matter

2021ZH22      Phys.Rev.Lett. 126, 152502 (2021)

Z.Y.Zhang, H.B.Yang, M.H.Huang, Z.G.Gan, C.X.Yuan, C.Qi, A.N.Andreyev, M.L.Liu, L.Ma, M.M.Zhang, Y.L.Tian, Y.S.Wang, J.G.Wang, C.L.Yang, G.S.Li, Y.H.Qiang, W.Q.Yang, R.F.Chen, H.B.Zhang, Z.W.Lu, X.X.Xu, L.M.Duan, H.R.Yang, W.X.Huang, Z.Liu, X.H.Zhou, Y.H.Zhang, H.S.Xu, N.Wang, H.B.Zhou, X.J.Wen, S.Huang, W.Hua, L.Zhu, X.Wang, Y.C.Mao, X.T.He, S.Y.Wang, W.Z.Xu, H.W.Li, Z.Z.Ren, S.G.Zhou

New α-Emitting Isotope 214U and Abnormal Enhancement of α-Particle Clustering in Lightest Uranium Isotopes

RADIOACTIVITY 214,216,218U(α) [from 180,182W(36Ar, 4n), 184W(40Ca, 2nα), E<200 MeV]; measured decay products, Eα, Iα; deduced α-decay Q-values and reduced widths, T1/2, abnormal enhancement by the strong monopole interaction between the valence protons and neutrons. Comparison withavailable data, calculations.

doi: 10.1103/PhysRevLett.126.152502
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2021ZH46      Chin.Phys.C 48, 084108 (2021)

H.Zhang, Z.i-H.Li, J.Su, Y.-J.Li, C.Chen, L.Zhang, F.-Q.Cao, Y.-P.Shen, W.Nan, W.-K.Nan, X.-Y.Li, L.-H.Chen, G.Lian, B.-Q.Cui, B.Guo, W.-P.Liu

Direct measurement of the resonance strengths and branching ratios of low-energy (p, γ) reactions on Mg isotopes

NUCLEAR REACTIONS 24,25,26Mg(p, γ), E=220-400 keV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, yields, resonances, branching ratios, resonance strengths. JUNA experiment, comparison with NACRE data.

doi: 10.1088/1674-1137/ac06aa
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2021ZH53      Phys.Rev.Lett. 127, 152702 (2021)

L.Y.Zhang, J.Su, J.J.He, M.Wiescher, R.J.deBoer, D.Kahl, Y.J.Chen, X.Y.Li, J.G.Wang, L.Zhang, F.Q.Cao, H.Zhang, Z.C.Zhang, T.Y.Jiao, Y.D.Sheng, L.H.Wang, L.Y.Song, X.Z.Jiang, Z.M.Li, E.T.Li, S.Wang, G.Lian, Z.H.Li, X.D.Tang, H.W.Zhao, L.T.Sun, Q.Wu, J.Q.Li, B.Q.Cui, L.H.Chen, R.G.Ma, B.Guo, S.W.Xu, J.Y.Li, N.C.Qi, W.L.Sun, X.Y.Guo, P.Zhang, Y.H.Chen, Y.Zhou, J.F.Zhou, J.R.He, C.S.Shang, M.C.Li, X.H.Zhou, Y.H.Zhang, F.S.Zhang, Z.G.Hu, H.S.Xu, J.P.Chen, W.P.Liu

Direct Measurement of the Astrophysical 19F(p, αγ)16O Reaction in the Deepest Operational Underground Laboratory

NUCLEAR REACTIONS 19F(p, α), E(cm)=72.4-188.8 keV; measured reaction products, Eγ, Iγ; deduced yields, S-factors, reaction rates. The China Jinping Underground Laboratory (CJPL), JUNA accelerator.

doi: 10.1103/physrevlett.127.152702
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2020DE08      Phys.Rev. C 101, 034307 (2020)

J.-G.Deng, H.-F.Zhang, G.Royer

Improved empirical formula for α-decay half-lives

RADIOACTIVITY A=146-294, Z=62-118(α); calculated α-decay half-lives for even-even nuclei; A=147-285, Z=62-112(α); calculated α-decay half-lives of even Z-odd N nuclei; A=145-261, Z=61-107(α); calculated α-decay half-lives of odd Z-even N nuclei; A=148-256, Z=63-101(α); calculated α-decay half-lives for odd-odd nuclei, in all cases isomers included. 279,281,283,285,287,289,291,293,295,297,299,301,303,305,307,309,311,313,315,317Ts, 281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318Og, 285,287,289,291,293,295,297,299,301,303,305,307,309,311,313,315,317,319119, 287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320120(α); calculated Qα, half-lives. Improved Royer formulas and WS3+ mass model. Comparison with available experimental values, and with other theoretical predictions.

doi: 10.1103/PhysRevC.101.034307
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2020DE37      Phys.Rev. C 102, 044314 (2020)

J.-G.Deng, H.-F.Zhang

Analytic formula for estimating the α-particle preformation factor

RADIOACTIVITY 148Eu, 148,150Gd, 149,151Tb, 150,151,152,153,154Dy, 151,151m,152,152m,153m,154Ho, 152,153,154,155,156Er, 153,153m,154,154m,155,156Tm, 154,155,156,157,158Yb, 155,155m,156m,157mLu, 156,157,158,160,162Hf, 157m,158,158m,159,159mTa, 158,159,160,161,162,163,164,166,168,180W, 159m,160,161m,162,162m,163,163m,164m,165,165m,167m,169,169mRe, 161,162,163,165,166,167,168,169,170,172,174,186Os, 164m,165m,166,166m,167,167m,168,168m,169,169m,170,170m,171,171m,172,172m,173m,174,174m,175,177Ir, 166,167,168,171,172,173,174,175,176,177,178,179,180,181,182,183,184,190Pt, 170,170m,171m,173,173m,175,175m,176,177,177m,179,181,183,185,186Au, 171,172,173,174,176,177,178,179,180,181,182,183,184,185,186Hg, 177,177m,179,179m,180,181m,183,183m,186m,187mTl, 178,179,180,183m,184,185m,186,187,187m,188,189,190,191m,192Pb, 186,186m,187,187m,189,190,190m,191,191m,192,192m,193,193m,194,194m,195,195m,196,196m,209,211,212,213,214Bi, 186,187,189,190,194,195,195m,196,197,197m,198,199,199m,200,201,201m,202,203,203m,204,205,206,207,208,209,211m,212,213,214,215,216,218,219Po, 191,191m,192,192m,193,193m,194,194m,195,197,197m,199,199m,200,200m,201,202,202m,203,204,205,206,207,208,209,210,211,212,213,215,217,218,219,220At(α); calculated T1/2 and α-preformation factors using an analytical formula as a bridge between the α-decay energy and α-particle preformation factor for even-even, odd-A and odd-odd α emitters. Comparison with experimental half-lives.

RADIOACTIVITY 193,194,195,195m,196,197,197m,200,202,203,203m,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223Rn, 197,199,199m,200m,201,201m,203,203m,205,207,209,211,212,213,214,215,218,218m,219,220,221,223Fr, 201,201m,202,203,203m,204,207,208,209,213,214,215,216,217,218,219,220,221,222,223,224,226Ra, 205,207,211,215,216,216m,217,217m,218,219,221,222,223,225,226,227Ac, 208,209m,212,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231Th, 213,215,217,220,221,223,224,227,228,229,230Pa, 216,218,219,221,222,224,225,226,227,229,230,231,232,233,234,236U, 227,229,231,235,237,239Np, 228,230,231,232,233,234,235,236,238,239,240,241,242,244Pu, 229,233,235,237,239,241,242m,243Am, 233,234,236,237,238,240,241,242,243,244,245,246,248Cm, 247Bk, 238,240,241,242,243,244,245,246,247,248,250,251,252,254Cf, 245,246,247,248,249,252,253,254m,255Es, 243,244,247,247m,248,252,253,254,256,257Fm, 247,247m,251,256m,258Md, 251,251m,253,254,255,256,258,259No, 253,253m,255,257,259Lr, 255,256,257m,258,259,260,261,263Rf, 259Db, 259,259m,260,261,263Sg, 261Bh, 264,265,268,269,270Hs, 267,269,270,271,271m,273,277Ds, 277,281Cn, 286,288,289Fl, 290,292Lv, 294Og(α); calculated T1/2 and α-preformation factors using an analytical formula as a bridge between the α-decay energy and α-particle preformation factor for even-even, odd-A and odd-odd α emitters. Comparison with experimental half-lives.

doi: 10.1103/PhysRevC.102.044314
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2020GA34      J.Phys.(London) G47, 045108 (2020)

J.Galan, X.Chen, H.Du, C.Fu, K.Giboni, F.Giuliani, K.Han, B.Jiang, X.Ji, H.Lin, Y.Lin, J.Liu, K.Ni, X.Ren, S.Wang, S.Wu, C.Xie, Y.Yang, T.Zhang, L.Zhao, S.Aune, Y.Bedfer, E.Berthoumieux, D.Calvet, N.d'Hose, E.Ferrer-Ribas, F.Kunne, B.Manier, D.Neyret, T.Papaevangelou, L.Chen, S.Hu, P.Li, X.Li, H.Zhang, M.Zhao, J.Zhou, Y.Mao, H.Qiao, S.Wang, Y.Yuan, M.Wang, Y.Chen, A.N.Khan, J.Tang, W.Wang, H.Chen, C.Feng, J.Liu, S.Liu, X.Wang, D.Zhu, J.F.Castel, S.Cebrian, T.Dafni, I.G.Irastorza, G.Luzon, H.Mirallas, X.Sun, A.Tan, W.Haxton, Y.Mei, C.Kobdaj, Y.Yan

Topological background discrimination in the PandaX-III neutrinoless double beta decay experiment

doi: 10.1088/1361-6471/ab4dbe
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2020LI12      Phys.Rev. C 101, 044313 (2020)

C.B.Li, G.L.Zhang, C.X.Yuan, G.X.Zhang, S.P.Hu, W.W.Qu, Y.Zheng, H.Q.Zhang, D.Mengoni, D.Testov, J.J.Valiente-Dobon, H.B.Sun, N.Wang, X.G.Wu, G.S.Li, M.Mazzocco, A.Gozzelino, C.Parascandolo, D.Pierroutsakou, M.La Commara, F.Recchia, A.I.Sison, S.Bakes, I.Zanon, S.Aydin, D.Bazzacco

New level scheme and shell model description of 212Rn

NUCLEAR REACTIONS 209Bi(6Li, 3n)212Rn, E=28, 30, 34 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) using GALILEO array at the Tandem-XTU accelerator of Legnaro National Laboratory. 212Rn; deduced levels, J, π, multipolarities, B(E2), B(E3), configurations. Comparison with large-scale shell-model calculations with multiparticle configurations. Systematics of low-, and medium-spin levels in N=126 isotones: 210Po, 212Rn, 214Ra and 216Th. Systematics of 3- to 0+ and 15/2- to 9/2+ excitation energies in N=126 and 127 isotones of Z=82-91.

NUCLEAR STRUCTURE 212Rn; calculated levels, J, π, amplitudes of shell-model multiparticle configurations for different levels, B(M1), B(E2), B(E3) using large-scale shell-model calculations with multiparticle configurations. Comparison with experimental data.

doi: 10.1103/PhysRevC.101.044313
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2020LI52      J.Phys.(London) G47, 035108 (2020)

P.Li, Y.Wang, Q.Li, J.Wang, H.Zhang

Effects of impact parameter filters on observables in heavy-ion collisions at INDRA energies

NUCLEAR REACTIONS 120Sn(129Xe, X), E<150 MeV/nucleon; analyzed available data; calculated nuclear stopping power, elliptic flow; deduced difference in elliptic flow at mid-rapidity among different centrality filters steadily decreases with increasing beam energy and impact parameter. The ultra-relativistic quantummolecular dynamics (UrQMD) model.

doi: 10.1088/1361-6471/ab6627
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2020SH09      Phys.Rev.Lett. 124, 162701 (2020)

Y.P.Shen, B.Guo, R.J.deBoer, Z.H.Li, Y.J.Li, X.D.Tang, D.Y.Pang, S.Adhikari, C.Basu, J.Su, S.Q.Yan, Q.W.Fan, J.C.Liu, C.Chen, Z.Y.Han, X.Y.Li, G.Lian, T.L.Ma, W.Nan, W.K.Nan, Y.B.Wang, S.Zeng, H.Zhang, W.P.Liu

Constraining the External Capture to the 16O ground State and the E2 S Factor of the 12C(α, γ)16O reaction

NUCLEAR REACTIONS 12C(11B, 7Li)16O, E=50 MeV; measured reaction products; deduced σ(θ), the ground state asymptotic normalization coefficients, S-factors. Comparison with available data.

doi: 10.1103/PhysRevLett.124.162701
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2020SH31      Phys.Rev.Lett. 125, 242301 (2020)

S.Shi, H.Zhang, D.Hou, J.Liao

Signatures of Chiral Magnetic Effect in the Collisions of Isobars

doi: 10.1103/PhysRevLett.125.242301
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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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2020WE11      Phys.Rev. C 102, 034318 (2020)

K.Wei, H.F.Zhang

α decay and cluster radioactivity within the redefined preformed cluster method

RADIOACTIVITY 221,222,223,224,226Ra, 225Ac(α), (14C); 276Ds(α), (68Ni); 228Th(α), (20O); 230U(α), (22Ne); 230Th, 231Pa, 232,234U(α), (24Ne); 231Pa(α), (23F); 233U(α), (25Ne); 234U(α), (26Ne), (28Mg); 238Pu(α), (30Mg), (32Si); 242Cm(α), (34Si); 244Cm(α), (36Si); 246Cf(α), (38S); 248Cf(α), (40S); 250Cf(α), (42S); 252Fm(α), (44Ar); 254Fm(α), (46Ar); 256No(α), (48Ca); 258Md(α), (50K); 259Db(α), (51V); 261Rf(α), (53Ti); 262Rf(α), (54Ti); 264Rf(α), (56Ti); 266Bh(α), (58Mn); 267Bh(α), (59Mn); 269Hs(α), (61Fe); 268Hs(α), (60Fe); 270Hs(α), (62Fe); 271Ds(α), (63Ni); 273Hs(α), (65Fe); 276Mt(α), (68Co); 278Rg(α), (70Cu); 280Rg(α), (72Cu); 273Hs(α), (65Fe); 282Cn(α), (74Ga); 283Cn(α), (75Ga); 284Cn(α), (76Ga); 285Cn(α), (77Ga); 286Cn(α), (78Ga); 287Fl(α), (79Ge); 288Fl(α), (80Ge); 289Fl(α), (81Ge); 290Lv(α), (79Ge); calculated preformation factors, and half-lives of α and cluster decays. Generalized liquid drop model (GLDM) framework, with redefined preformed cluster method, and the preformation factor from WKB approximation. Comparison with available experimental values.

doi: 10.1103/PhysRevC.102.034318
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2020WU09      Phys.Rev. C 102, 054323 (2020)

D.Wu, C.L.Bai, H.Sagawa, H.Q.Zhang

Calculation of nuclear charge radii with a trained feed-forward neural network

NUCLEAR STRUCTURE 40,42,44,46,48,50,52Ca, 108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn, 138,140,142,144,146,148,150,152,154Sm, 182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212Pb; calculated nuclear charge radii, correlation between the symmetry energy and charge radii of Ca isotopes, and confirmed this correlation by Skyrme Hartree-Fock-Bogoliubov calculation. A multilayer feed-forward neural network model (ML-FNN).

doi: 10.1103/PhysRevC.102.054323
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2020XI05      Nucl.Phys. A1004, 122034 (2020)

Y.-Z.Xing, W.-C.Fu, X.-B.Liu, F.-P.Lu, H.-F.Zhang, Y.-M.Zheng

Sensitivity of the mean field dynamics within quantum molecular dynamics

doi: 10.1016/j.nuclphysa.2020.122034
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2020ZH33      Chin.Phys.B 29, 074209 (2020)

B.Zhang, Y.Huang, H.Zhang, Y.Hao, M.Zeng, H.Guan, K.Gao

Progress on the 40Ca+ ion optical clock

ATOMIC PHYSICS 40Ca; analyzed available data; deduced progress on an ion optical clock.

doi: 10.1088/1674-1056/ab9432
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2020ZH36      Phys.Rev. C 102, 044308 (2020)

J.Zhang, H.F.Zhang

Effects of shell correction on α-decay systematics

RADIOACTIVITY 105,106,107,108,109Te, 110,111I, 109,110,111,112,113Xe, 114Cs, 114Ba, 144Nd, 145Pm, 146,147,148Sm, 147,148Eu, 148,149,150,151,152Gd, 151Tb, 150,151,152,153,154Dy, 151,152,153,154Ho, 152,153,154,155,156Er, 153,154,155,156Tm, 154,155,156,157,158Yb, 155,158Lu, 156,157,158,159,160,162,174Hf, 158,159,163Ta, 158,159,160,161,162,163,164,166,167,168,180W, 160,162,163,165,166Re, 161,162,163,164,165,166,167,168,169,170,171,172,173,174,186Os, 166,167,168,169,175,177Ir, 166,167,168,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,186,188,190Pt, 170,173,174,175,176,177,179,181,182,183,185Au, 172,173,174,176,177,178,179,180,181,182,183,184,185,186,188Hg, 177,179Tl, 178,180,182,184,186,188,190,192,194,210Pb, 194Bi, 186,189,190,194,195,196,197,198,199,200,201,202,204,205,206,207,208,210,212,213,214,215,216,218,219Po, 191,192,193,197,199,200,201,202,203,204,205,206,207,208,209,210,211,213,214,215,216,217,218,219,220At(α); calculated T1/2, shell correction energies of the spherical parent and daughter nuclei. Generalized liquid drop model (GLDM), with the effects of the Strutinsky shell correction. Comparison with experimental data.

RADIOACTIVITY 193,194,195,196,197,200,202,203,204,206,207,208,209,210,212,214,215,216,217,218,220,222Rn, 198,199,200,201,203,204,205,206,207,208,209,210,211,213,215,216,217,218,219,220Fr, 201,202,203,204,206,207,208,209,210,212,214,216,217,218,220,222,224,226Ra, 205,206,207,211,215,218,219,221,222,223,227Ac, 208,212,214,215,216,218,219,220,222,224,226,228,230,232Th, 212,213,214,215,217,219,220,221,223,225,226,227,231Pa, 216,218,221,222,224,225,226,229,230,232,233,234,236,238U, 225,226,227,229,231,233Np, 228,230,231,232,233,234,235,236,238,240,242,244Pu, 233,235,236,237Am, 233,234,236,238,240,242,244,246,248Cm, 237,238,240,242,244,245,246,248,250,252,253,254Cf, 243,247,251,253,255Es, 243,246,248,249,250,252,254,256Fm, 251,252,254,256No, 253,259Lr, 256,258,261Rf, 260,263Sg, 264,265,268,269,270,275Hs, 278Mt, 267,270Ds, 285Cn, 285,286,287,288,289Fl, 287,289,290Mc, 290,291,292Lv, 294Og(α); calculated T1/2, shell correction energies of the spherical parent and daughter nuclei. Generalized liquid drop model (GLDM), with the effects of the Strutinsky shell correction. Comparison with experimental data.

doi: 10.1103/PhysRevC.102.044308
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2019CA13      Phys.Rev. C 99, 054615 (2019)

A.Gomez Camacho, A.Diaz-Torres, H.Q.Zhang

Comparative study of the effect of resonances of the weakly bound nuclei 6, 7Li on total fusion with light to heavy mass targets

NUCLEAR REACTIONS 27Al(7Li, X), E(cm)=8-24 MeV; 59Co(7Li, X), E(cm)=10-24 MeV; 144Sm(7Li, X), E(cm)=20-38 MeV; 209Bi(7Li, X), E(cm)=25-50 MeV; 28Si(6Li, X), E(cm)/VB=1-3.6 MeV; 59Co(6Li, X), E(cm)/VB=0.8-2.0 MeV; 96Zr(6Li, X), E(cm)/VB=0.8-1.7 MeV; 198Pt(6Li, X), E(cm)/VB=0.8-1.4 MeV; 209Bi(6Li, X), E(cm)/VB=0.9-1.2 MeV; calculated total fusion σ(E), effects of resonant and non-resonant breakup states in projectile nuclei on total fusion σ. Continuum-discretized coupled-channel (CDCC) calculations. Comparison with available experimental data.

doi: 10.1103/PhysRevC.99.054615
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2019GL02      Phys.Rev. C 99, 065801 (2019)

B.E.Glassman, D.Perez-Loureiro, C.Wrede, J.Allen, D.W.Bardayan, M.B.Bennett, K.A.Chipps, M.Febbraro, M.Friedman, C.Fry, M.R.Hall, O.Hall, S.N.Liddick, P.O'Malley, W.-J.Ong, S.D.Pain, S.B.Schwartz, P.Shidling, H.Sims, L.J.Sun, P.Thompson, H.Zhang

Doppler broadening in 20Mg(βpγ)19Ne decay

RADIOACTIVITY 20Mg(β+p)[20Mg beam from 9Be(24Mg, X), E=170 MeV/nucleon, followed by separation using A1900 separator at NSCL-MSU]; measured Eβ+, Eγ, Iγ, β+γ-coin, γ-decay branching ratios, and E(p) using plastic scintillator for β detection and the SeGA array for γ detection. 19Ne; deduced levels, J, π, half-life of 1507.5 level from Doppler broadening analysis, β+p feedings. Comparison with previous experimental values. Discussed relevance to 15O(α, γ)19Ne thermonuclear reaction rates.

NUCLEAR REACTIONS 9Be(24Mg, X)15N/16O/17F/18Ne/20Mg, E=170 MeV/nucleon; measured time of flight, particle identification plot, yields using A1900 fragment separator at the K500 and K1200 coupled cyclotrons of NSCL-MSU.

doi: 10.1103/PhysRevC.99.065801
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2019GU09      Nucl.Phys. A986, 18 (2019)

W.Guo, J.M.Dong, X.Shang, H.F.Zhang, W.Zuo, M.Colonna, U.Lombardo

Proton-proton 1S0 pairing in neutron stars

doi: 10.1016/j.nuclphysa.2019.02.008
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2019GU31      Phys.Rev. C 100, 054616 (2019)

S.Q.Guo, X.J.Bao, H.F.Zhang, J.Q.Li, N.Wang

Effect of dynamical deformation on the production distribution in multinucleon transfer reactions

NUCLEAR REACTIONS 208Pb(136Xe, X), E(cm)=526, 617, 450 MeV; 198Pt(136Xe, X), E(cm)=643; calculated potential energy surfaces (PES), σ for mass distribution of primary products, cross sections of target-like fragments with Z=78-86 and Z=50-58, production cross sections of the N=126 isotones as a function of the atomic number; deduced influences of dynamical deformation on the PES and the mass distribution of the multi-nucleon transfer (MNT) reactions. Calculations based on the framework of the dinuclear system concept. Comparison with experimental data.

doi: 10.1103/PhysRevC.100.054616
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2019LV02      Chin.Phys.C 43, 104102 (2019)

Y.-F.Lv, J.-B.Lu, G.-L.Zhang, Y.-H.Wu, C.-X.Yuan, G.-J.Fu, G.-X.Zhang, Z.Huang, M.-L.Wang, S.-P.Hu, H.-B.Sun, H.-Q.Zhang, C.-Q.Li, K.-Y.Ma, Y.-J.Ma, Yu.-Z.Liu, D.Testov, P.R.John, J.J.Valiente-Dobon, A.Goasduff, M.Siciliano, F.Galtarossa, F.Recchia, D.Mengoni, D.Bazzacco

Low-lying states of 92, 93Nb excited in the reactions induced by the weakly-bound nucleus 6Li near the Coulomb barrier

NUCLEAR REACTIONS 89Y(6Li, X)92Nb/93Nb, E=34 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, level schemes.

doi: 10.1088/1674-1137/43/10/104102
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2019MA25      Chin.Phys.C 43, 044105 (2019)

N.-N.Ma, H.-F.Zhang, X.-Ju.Bao, H.-F.Zhang

Basic characteristics of nuclear landscape by improved Weizsacker-Skyrme-type nuclear mass model

NUCLEAR STRUCTURE Z=8-128; calculated binding energies, quadrupole deformations, One-neutron and one-proton separation energies, α and β decay Q-values, pairing gaps. Comparison with Atomic Mass Evaluation (AME2016).

doi: 10.1088/1674-1137/43/4/044105
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2019MA28      Phys.Rev. C 99, 044312 (2019)

N.Ma, C.J.Halcrow, H.Zhang

Effect of the Coulomb energy on Skyrmions

doi: 10.1103/PhysRevC.99.044312
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2019MA58      Phys.Rev. C 100, 024602 (2019)

M.Mazzocco, N.Keeley, A.Boiano, C.Boiano, M.La Commara, C.Manea, C.Parascandolo, D.Pierroutsakou, C.Signorini, E.Strano, D.Torresi, H.Yamaguchi, D.Kahl, L.Acosta, P.Di Meo, J.P.Fernandez-Garcia, T.Glodariu, J.Grebosz, A.Guglielmetti, Y.Hirayama, N.Imai, H.Ishiyama, N.Iwasa, S.C.Jeong, H.M.Jia, Y.H.Kim, S.Kimura, S.Kubono, G.La Rana, C.J.Lin, P.Lotti, G.Marquinez-Duran, I.Martel, H.Miyatake, M.Mukai, T.Nakao, M.Nicoletto, A.Pakou, K.Rusek, Y.Sakaguchi, A.M.Sanchez-Benitez, T.Sava, O.Sgouros, V.Soukeras, F.Soramel, E.Stiliaris, L.Stroe, T.Teranishi, N.Toniolo, Y.Wakabayashi, Y.X.Watanabe, L.Yang, Y.Y.Yang, H.Q.Zhang

Elastic scattering for the 8B and 7Be + 208Pb systems at near-Coulomb barrier energies

NUCLEAR REACTIONS 208Pb(8B, 8B), E=50 MeV, [8B secondary beam from 3He(6Li, 8B), E=11.2 MeV/nucleon primary reaction at RIKEN]; 208Pb(7Be, 7Be), E=37.4, 40.5, 42.2 MeV, [7Be secondary beam from 1H(7Li, 7Be), E=48.8 MeV primary reaction at LNL-Legnaro]; measured charged particles, σ(θ, E) using the EXPADES detector array, and angular distribution; analyzed by optical model and the continuum discretized coupled channels (CDCC) formalisms. Experiments performed at the CNS Radioactive Ion Beams (CRIB) facility at RIKEN, and EXOTIC facility at the Laboratori Nazionali di Legnaro (LNL).

doi: 10.1103/PhysRevC.100.024602
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2019NI10      Chin.Phys.C 43, 113001 (2019)

K.Ni, Y.Lai, A.Abdukerim, W.Chen, X.Chen, Y.Chen, X.Cui, Y.Fan, D.Fang, C.Fu, L.Geng, K.Giboni, F.Giuliani, L.Gu, X.Guo, K.Han, C.He, D.Huang, Y.Huang, Y.Huang, Z.Huang, P.Ji, X.Ji, Y.Ju, K.Liang, H.Liu, J.Liu, W.Ma, Y.Ma, Y.Mao, Y.Meng, P.Namwongsa, J.Ning, X.Ning, X.Ren, C.Shang, L.Si, A.Tan, A.Wang, H.Wang, M.Wang, Q.Wang, S.Wang, X.Wang, Z.Wang, M.Wu, S.Wu, J.Xia, M.Xiao, P.Xie, B.Yan, J.Yang, Y.Yang, C.Yu, J.Yuan, D.Zhang, H.Zhang, T.Zhang, L.Zhao, Q.Zheng, J.Zhou, N.Zhou, X.Zhou

Searching for neutrino-less double beta decay of 136Xe with PandaX-II liquid xenon detector

RADIOACTIVITY 136Xe(2β-); measured decay products, Eβ, Iβ; deduced T1/2 and Majorana neutrino mass limits. Comparison with available data.

doi: 10.1088/1674-1137/43/11/113001
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2019SH04      Nucl.Phys. A982, 539c (2019)

S.Shi, H.Zhang, D.Hou, J.Liao

Chiral Magnetic Effect in Isobaric Collisions from Anomalous-Viscous Fluid Dynamics (AVFD)

doi: 10.1016/j.nuclphysa.2018.10.007
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2018AL10      Nucl.Phys. A972, 18 (2018)

J.L.Albacete, F.Arleo, G.G.Barnafoldi, G.Biro, D.d'Enterria, B.Ducloue, K.J.Eskola, E.G.Ferreiro, M.Gyulassy, S.M.Harangozo, I.Helenius, Z.-B.Kang, P.Kotko, S.A.Kulagin, K.Kutak, J.P.Lansberg, T.Lappi, P.Levai, Z.-W.Lin, G.Ma, Y.-Q.Ma, H.Mantysaari, H.Paukkunen, G.Papp, R.Petti, A.H.Rezaeian, P.Ru, S.Sapeta, B.Schenke, S.Schlichting, H.-S.Shao, P.Tribedy, R.Venugopalan, I.Vitev, R.Vogt, E.Wang, X.-N.Wang, R.Xing, R.Xu, B.-W.Zhang, H.-F.Zhang, W.-N.Zhang

Predictions for cold nuclear matter effects in p+Pb collisions at √ SNN = 8.16 TeV

doi: 10.1016/j.nuclphysa.2017.11.015
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2018BA09      Phys.Rev. C 97, 024617 (2018)

X.Bao, S.Q.Guo, H.F.Zhang, J.Q.Li

Dynamics of complete and incomplete fusion in heavy ion collisions

NUCLEAR REACTIONS 248Cm(48Ca, X), E(296Lv*)=33 MeV; 238U(48Ca, X), E(286Cn*)=38 MeV; 244Pu(48Ca, X), E(292Fl*)=42 MeV; calculated mass yield of the quasifission products as function of the mass number of the fragment for the hot fusion reaction. 238U(64Ni, X), E(cm)=307.4 MeV; 248Cm(48Ca, X), E(cm)=192-248 MeV; calculated σ(E) for transfer of protons and multinucleons, and compared with available experimental data. 248Cm(48Ca, X), E(cm)=215.93 MeV; calculated production cross sections for light neutron rich nuclei. 238U, 244Pu, 248Cm(48Ca, xn), E(compound nucleus)=25-60 MeV; calculated evaporation residue σ(E) for x=3n, 4n and 5n channels, and compared with experimental data. Dinuclear system (DNS) model with new four-variable master equation (ME). Relevance to formation of superheavy nuclei (SHNs).

doi: 10.1103/PhysRevC.97.024617
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2018GA11      Phys.Rev. C 97, 044903 (2018)

Z.Gao, A.Luo, G.-L.Ma, G.-Y.Qin, H.-Z.Zhang

Overall momentum balance and redistribution of the lost energy in asymmetric dijet events in 2.76A TeV Pb-Pb collisions with a multiphase transport model

doi: 10.1103/PhysRevC.97.044903
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2018GE06      Phys.Rev. C 98, 034312 (2018)

Z.Ge, C.Li, J.Li, G.Zhang, B.Li, X.Xu, C.A.T.Sokhna, X.Bao, H.Zhang, Yu.S.Tsyganov, F.-S.Zhang

Effect of shell corrections on the α-decay properties of 280-305Fl isotopes

RADIOACTIVITY 280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305Fl(α), (SF); calculated Q(α) and half-lives using GLDM, the GLDM with shell correction, the UFM and the Royer's formula, and shell correction energies of the even-even nuclei. 285,286,287,288,289Fl, 281,283,285Cn, 277,279,281Ds, 273,275Hs, 269,271Sg(α); calculated T1/2 using Royer's, UDL, UFM, and GLDM formulas, and by input of experimental Q(α) values. Comparison with experimental values.

doi: 10.1103/PhysRevC.98.034312
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2018GL01      Phys.Lett. B 778, 397 (2018)

B.E.Glassman, D.Perez-Loureiro, C.Wrede, J.Allen, D.W.Bardayan, M.B.Bennett, B.A.Brown, K.A.Chipps, M.Febbraro, M.Friedman, C.Fry, M.R.Hall, O.Hall, S.N.Liddick, P.O'Malley, W.J.Ong, S.D.Pain, C.Prokop, S.B.Schwartz, P.Shidling, H.Sims, P.Thompson, H.Zhang

β-delayed γ decay of 20Mg and the 19Ne(p, γ)20Na breakout reaction in Type I X-ray bursts

RADIOACTIVITY 20Mg(β+) [from 9Be(24Mg, X)20Mg, E=170 MeV/nucleon]; measured decay products, Eβ, Iβ, Eγ, Iγ; deduced γ-ray energies and limits on intensities of β-delayed γ-rays, Gamow-Teller strengths B(GT) and associated log ft values. Comparison with theoretical calculations.

doi: 10.1016/j.physletb.2018.01.041
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