NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = H.Zhang Found 454 matches. Showing 1 to 100. [Next]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
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
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
2024YA10 Nuovo Cim. C 47, 37 (2024) M.J.Yang, C.L.Bai, H.Sagawa, H.Q.Zhang Beyond mean field model for Gamow-Teller giant resonances and β decay NUCLEAR STRUCTURE 48Ca, 90Zr, 132Sn, 208Pb; calculated Gamow-Teller (GT) transitions using self-consistent Hartree-Fock (HF) plus charge-exchange subtracted second random phase approximation (SSRPA) model with several Skyrme energy density functions (EDFs); deduced SRPA improves systematically the description of main GT strength distributions in terms of the excitation energy and the peak height, quenching factors.
doi: 10.1393/ncc/i2024-24037-8
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
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
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
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
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
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
2023LI49 Phys.Rev. C 108, L041602 (2023) Theory of Coulomb excitation of the 229Th nucleus by protons
doi: 10.1103/PhysRevC.108.L041602
2023LI51 Phys.Rev. C 108, 044604 (2023) Possibility to synthesize Z > 118 superheavy nuclei with 54Cr projectiles
doi: 10.1103/PhysRevC.108.044604
2023LI62 Chin.Phys.C 47, 124105 (2023) 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
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
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
2023QI04 Phys.Rev.Lett. 130, 112501 (2023) 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
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
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
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
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
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
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
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
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
2023ZH22 J.Phys.(London) G50, 045101 (2023) 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
2023ZH23 Phys.Rev. C 107, 064304 (2023) 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
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
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
2023ZH41 Phys.Rev. C 108, 024602 (2023) 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
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
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
2022DE22 Eur.Phys.J. A 58, 165 (2022) 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
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
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
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
2022LI27 Phys.Rev. C 105, 054606 (2022) 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
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
2022LI51 Phys.Rev. C 106, 034613 (2022) 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
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
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
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
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
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
2022ZH13 Nucl.Phys. A1021, 122420 (2022) 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
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
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
2022ZH27 Phys.Rev. C 105, 054317 (2022) 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
2022ZH38 Chin.Phys.C 46, 044103 (2022) 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
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)α1-α2-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
2022ZH47 Nucl.Phys. A1027, 122510 (2022) 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
2022ZH55 J.Phys.(London) G49, 105104 (2022) 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
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
2022ZH61 Phys.Rev. C 106, 044604 (2022) 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
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
2021DE07 Chin.Phys.C 45, 024104 (2021) 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
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
2021HE09 Chin.Phys.C 45, 014110 (2021) 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
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
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
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
2021MA17 Chin.Phys.C 45, 024105 (2021) 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
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
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
2021WA56 J.Phys.(London) B54, 244001 (2021) 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
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
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
2021XI02 Phys.Rev. C 103, 034911 (2021) γ-hadron spectra in p + Pb collisions at √ sNN = 5.02 TeV
doi: 10.1103/PhysRevC.103.034911
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
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
2021ZH05 Nucl.Phys. A1005, 121762 (2021) 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
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
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
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
2020DE37 Phys.Rev. C 102, 044314 (2020) 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
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
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
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
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
2020SH31 Phys.Rev.Lett. 125, 242301 (2020) Signatures of Chiral Magnetic Effect in the Collisions of Isobars
doi: 10.1103/PhysRevLett.125.242301
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
2020WE11 Phys.Rev. C 102, 034318 (2020) 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
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
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
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
2020ZH36 Phys.Rev. C 102, 044308 (2020) 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
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
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
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
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
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
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
2019MA28 Phys.Rev. C 99, 044312 (2019) Effect of the Coulomb energy on Skyrmions
doi: 10.1103/PhysRevC.99.044312
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
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
2019SH04 Nucl.Phys. A982, 539c (2019) Chiral Magnetic Effect in Isobaric Collisions from Anomalous-Viscous Fluid Dynamics (AVFD)
doi: 10.1016/j.nuclphysa.2018.10.007
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
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
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
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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