NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = Y.Zhao Found 266 matches. Showing 1 to 100. [Next]2024CH19 Phys.Rev. C 109, 034911 (2024) L.Chen, Y.-Y.Zhao, Y.Cheng, G.Wang, Zh.Li, Y.Wu Impact of limited statistics on the measured hyperorder cumulants of net-proton distributions in heavy-ion collisions
doi: 10.1103/PhysRevC.109.034911
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
2024YI02 Phys.Rev. C 109, 024322 (2024) Alternating-parity doublets of even-even Ba isotopes
doi: 10.1103/PhysRevC.109.024322
2023GU12 Phys.Rev. C 108, 014319 (2023) P.Guo, C.Pan, Y.C.Zhao, X.K.Du, S.Q.Zhang Prolate-shape dominance in atomic nuclei within the deformed relativistic Hartree-Bogoliubov theory in continuum NUCLEAR STRUCTURE 134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,178Te, 136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,178,180Xe, 138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,178,180,182Ba; calculated quadrupole deformation, potential-energy curves, single-neutron energies, pairing correlations. Calculations with deformed relativistic Hartree-Bogoliubov theory in continuum (DRHBc).
doi: 10.1103/PhysRevC.108.014319
2023LI15 Nucl.Instrum.Methods Phys.Res. B537, 147 (2023) C.Liang, X.Zhang, X.Zhou, Y.Zhao, R.Cheng, Gu.Xiao 9642Mo L-shell X-ray production cross sections by 2.0-6.0 MeV 15263Eu ions NUCLEAR REACTIONS Mo(Eu, X), E=2, 3, 4, 5, 6 MeV; measured reaction products, X-rays; deduced Mo L X-ray spectra yields, production σ. Comparison with BEA and PWBA theoretical models. The Institute of Modern Physics, Chinese Academy of Sciences (IMP, CAS) in Lanzhou, China.
doi: 10.1016/j.nimb.2022.10.007
2023MA17 Phys.Rev. C 107, 034316 (2023) β-decay half-lives of the r-process waiting-point isotones of N=8 and 82 nuclei RADIOACTIVITY 131,130In, 130,129Cd, 129,128Ag, 128,127Pd, 127,126Rh, 126,125Ru, 125,124Tc, 124,123Mo, 123,122Nb, 122,121Zr, 121,120Y, 120,119Sr(β-); calculated T1/2, Gamow-Teller decay rates from the ground state. 125mTc, 123mNb, 129mCd, 127mPd, 125mRu, 123mMo, 121mZr, 119mSr(β-); calculated isomers states T1/2. Nucleon-pair approximation (NPA) method assuming S pair condensation in the ground state of parent nuclei. Comparison to available experimental data and other theoretical calculation (shell-model, QRPA, RQRPA+RHB). NUCLEAR STRUCTURE 130Sn, 129,130Cd, 130,131In, 129Ag, 127Rh, 125Tc, 123Nb, 121Y; calculated levels J, π, occupation probability of the proton orbits. Shell-model calculations. NUCLEAR MOMENTS 131,129In, 131Sn, 129,127Ag, 129Cd, 127,125Rh, 127Pd, 125Ru, 125,123Tc, 123,121Nb, 123Mo, 121Zr, 121,119Y, 119Sr; calculated electrical quadrupole moments, magnetic moments. Comparison to experimental data.
doi: 10.1103/PhysRevC.107.034316
2023MA42 Phys.Rev. C 108, 034308 (2023) State-of-the-art nucleon-pair approximation to the nuclear shell model
doi: 10.1103/PhysRevC.108.034308
2023ME12 Phys.Rev. C 108, 034602 (2023) B.Mei, Y.Guan, N.Zeng, Z.Mai, J.Tu, T.Yu, S.Wang, X.Zhang, P.Ma, X.Xu, X.Tu, Y.Sun, Z.Sun, S.Tang, Y.Yu, F.Fang, D.Yan, S.Jin, Y.Zhao, S.Ma, Y.Zhang Isotopic cross sections in fragmentation reactions of 12, 14C, 14, 16N, and 16O projectiles on a carbon target
doi: 10.1103/PhysRevC.108.034602
2023PA19 Chin.Phys.C 47, 064102 (2023) Y.-F.Pan, Y.-Y.Cheng, Y.Lu, H.Jiang, X.-R.Zhou, Y.-M.Zhao Robustness of pair structures for nuclear yrast states NUCLEAR STRUCTURE 28Si, 50Cr, 132Xe; calculated energy levels, J, π, quadrupole moments, yrast states using the nucleon-pair approximation (NPA) and shell-model effective interactions. Comparison with available data.
doi: 10.1088/1674-1137/acc1cc
2023YI02 Chin.Phys.C 47, 064105 (2023) Simple scenario of integrated neutron-proton interaction NUCLEAR STRUCTURE Z=28-82; analyzed available data; deduced the patterns of neutron-proton interactions in a few major shells of the nuclide chart.
doi: 10.1088/1674-1137/acc5dd
2023ZO02 Astrophys.J.Suppl.Ser. 268, 56 (2023) Y.P.Zou, J.S.Zhang, C.Henkel, D.Romano, Y.H.Zheng, Y.T.Yen, J.L.Chen, Y.X.Wang, Y.Zhao A Systematic Observational Study on Galactic Interstellar Ratio 18O/17O. II. C18O and C17O J = 2-1 Data Analysis
doi: 10.3847/1538-4365/acee6b
2022JI03 Chin.Phys.C 46, 014003 (2022) S.-Y.Jin, Y.-Z.Sun, S.-T.Wang, Z.-Y.Sun, X.-H.Zhang, Z.-Q.Chen, B.Mei, Y.-X.Zhao, S.-W.Tang, Y.-H.Yu, D.Yan, F.Fang, Y.-J.Zhang, S.B.Ma, X.-M.Liu, R.Han Fragmentation of stable and neutron-rich 12-16C into boron fragments at approximately 240 MeV/nucleon NUCLEAR REACTIONS C(12C, X), (13C, X), (14C, X), (15C, X), (16C, X)10Be/13B/B, E=240 MeV/nucleon; measured reaction products; deduced σ. Comparison with EPAX3, modified EPAX2, FRACS, NUCFRG2, INCL++, JQMD, and JQMD-2.0 calculations. The ETF of the Institute of Modern Physics, Chinese Academy of Sciences.
doi: 10.1088/1674-1137/ac2ed5
2022LI07 Phys.Rev. C 105, L021305 (2022) Evolution of collectivity and neutron-proton interactions NUCLEAR STRUCTURE Z=28-82, N=50-82; Z=50-82, N=82-126; analyzed energies of first 2+, 4+ states, integrated neutron-proton interactions Vnp; deduced correlation between the evolution of collective motions and Vnp.
doi: 10.1103/PhysRevC.105.L021305
2022ME07 Phys.Rev. C 105, 064604 (2022) B.Mei, J.Tu, X.Zhang, S.Wang, Y.Guan, Z.Mai, N.Zeng, X.Tu, Z.Sun, S.Tang, Y.Yu, F.Fang, D.Yan, S.Jin, Y.Zhao, S.Ma, Y.Zhang New experimental evidence for universal odd-even staggering in fragmentation cross sections NUCLEAR REACTIONS 27Al, 16,17,18O(78Kr, X), E=300 MeV/nucleon; measured reaction products, Bρ, time of flight, ΔE; deduced production yields, odd-even staggering (OES) in fragmentation reaction for Z=5-45 with N-Z from 1–9. Systematics of odd-even staggering magnitudes for 78Kr+Al2O3, 78Kr+Be, 84Kr+112,124Sn and 86Kr+Be/Ta. Fragmentation on Al2O3 target at RIBLL2 separator at the Heavy-Ion Research Facility in Lanzhou (HIRFL).
doi: 10.1103/PhysRevC.105.064604
2022SH45 Phys.Rev. C 106, L061304 (2022) R.Shou, X.Yin, C.Ma, M.Q.Lin, Y.M.Zhao Simple corrections in theoretical models of atomic masses and nuclear charge radii ATOMIC MASSES Z=29-110; N=20-160; A=49-270; analyzed systematic root mean square deviations of mass excesses, S(n), and S(p) between their experimental values from AME2020, and theoretical values from Hartree-Fock-Bogoliubov (HFB31), relativistic mean field (RMF), Duflo-Zuker (DZ), and Weizsaker-Skyrme (WS4+RBF) models using strong and specific correlations of these deviations, and deducing Pearson correlation coefficients for 3258 neutron- and proton-rich nuclei listed in the Supplemental Material of the paper. NUCLEAR STRUCTURE Z=29-59; Z=61-64; Z=66; Z=68-76; Z=78, 79; Z=81-84; Z=86-88; Z=90, 92, 95, 96; analyzed systematic root mean square deviations of charge radii between their experimental values taken from 2021Li25 (Atomic Data and Nuclear Data Tables 140, 101440 (2021)), and theoretical values from Hartree-Fock-Bogoliubov (HFB31), relativistic mean field (RMF), relativistic continuum Hartree-Bogoliubov (RCHB), and Weizsaker-Skyrme (WS*) models using strong and specific correlations of these deviations, and deducing Pearson correlation coefficients for neutron- and proton-rich nuclei listed in the Supplemental Material of the paper.
doi: 10.1103/PhysRevC.106.L061304
2022WA17 Phys.Rev. A 105, 05807 (2022) X.Wang, X.Liu, Z.Xu, J.Ren, Y.Zhao, R.Cheng, Y.Lei, Y.Chen, Y.Liu, X.Zhou, X.Zhang Experimental determination of atomic alignment of 42Mo, 48Cd, and 49In with differential x-ray intensity ratios by 100-250-keV proton impact NUCLEAR REACTIONS Mo, Cd, In(p, X), E=100-250 keV; measured reaction products, X-rays; deduced differential intensity ratios, anisotropy and alignment parameters. Comparison with theoretical calculations. The 320-kV high-voltage platform at IMP-CAS in Lanzhou.
doi: 10.1103/PhysRevA.105.052807
2022XU12 Chin.Phys.C 46, 111001 (2022) Xi.-D.Xu, Y.-Z.Sun, S.-T.Wang, B.Mei, S.-Y.Jin, X.-H.Zhang, Z.-Y.Sun, Y.-X.Zhao, S.-W.Tang, Y.-H.Yu, D.Yan, F.Fang, Y.-J.Zhang, S.-B.Ma Isotopic production cross sections of fragmentation residues produced by 18O ions on a carbon target near 260 MeV/nucleon NUCLEAR REACTIONS C(18O, X)14N/15C/12C/12B/13B/10B, E=260 MeV/nucleon; measured reaction products, TOF; deduced isotopic σ. Comparison with available data. The HIRFL facility in Lanzhou (China).
doi: 10.1088/1674-1137/ac827c
2022YI02 Phys.Rev. C 105, 064304 (2022) Atomic masses of nuclei with neutron numbers N < 126 and proton numbers Z < 82 ATOMIC MASSES 186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209Bi, 186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210Po, 190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211At, 190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212Rn, 196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213Fr, 195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214Ra, 203,204,205,206,207,208,209,210,211,212,213,214,215Ac, 201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216Th, 209,210,211,212,213,214,215,216,217Pa, 207,208,209,210,211,212,213,214,215,216,217,218U; calculated mass excess, S(p), S(2p), α-decay Q-value. Empirical formula with neutron-proton residual interaction extracted from AME2021 data. Comparison to AME2021 values.
doi: 10.1103/PhysRevC.105.064304
2022ZH63 Phys.Rev. C 106, L051901 (2022) Y.-S.Zhao, L.x.Wang, K.Zhou, X.-G.Huang Detecting the chiral magnetic effect via deep learning
doi: 10.1103/PhysRevC.106.L051901
2022ZH77 Sci. Rep. 12, 19264 (2022) X.Zhou, J.Wei, Ru.Cheng, Y.Zhang, Y.Chen, C.Liang, X.Zhang, Y.Zhao Au L-shell x-ray emission induced by 154.3-423.9 MeV/u C6+ ions NUCLEAR REACTIONS 197Au(12C, X), E=154.3-423.9 MeV/nucleon; measured reaction products, X-rays; deduced L-shell X-ray spectra, relative intensity ratios, production σ. Comparison with calculations. The cancer therapy termina l at the national laboratory of Heavy Ion Research Facility in Lanzhou (HIRFL) in the Institute of Modern Physics, Chinese Academic of Science (IMP, CAS).
doi: 10.1038/s41598-022-23830-5
2022ZH78 Sci. Rep. 12, 6253 (2022) X.Zhou, J.Wei, R.Cheng, C.Liang, Y.Chen, X.Zhang, Y.Zhao Multiple ionization of iodine for 2.5-5.0 MeV I22+ ions impacting on Fe target NUCLEAR REACTIONS Fe(I, X), E=2.5-5 MeV; measured reaction products, X-rays; deduced L-shell X-ray spectra, relative intensity ratios, atomic fluorescence yield. Comparison with available data. The Electron Cyclotron Resonance (ECR) ion source, the 320 kV high voltage experimental platform at the Institute of Modern Physics, Chinese Academy of Sciences (IMP, CAS) in Lanzhou, China.
doi: 10.1038/s41598-022-10337-2
2022ZO01 Phys.Rev. C 105, 034321 (2022) Y.Y.Zong, C.Ma, M.Q.Lin, Y.M.Zhao Mass relations of mirror nuclei for both bound and unbound systems ATOMIC MASSES 3He, 6,7Be, 8,9B, 8,9,10,11C, 11,12,13N, 11,12,13,14,15O, 14,15,16,17F, 14,15,16,17,18,19Ne, 17,18,19,20,21Na, 17,18,19,20,21,22,23Mg, 20,21,22,23,24,25Al, 21,22,23,24,25,26,27Si, 23,24,25,26,27,28,29P, 24,25,26,27,28,29,30,31S, 27,28,29,30,31,32,33Cl, 28,29,30,31,32,33,34,35Ar, 31,32,33,34,35,36,37K, 32,33,34,35,36,37,38,39Ca, 35,36,37,38,39,40,41Sc, 36,37,38,39,40,41,42,43Ti, 39,40,41,42,43,44,45V, 40,41,42,43,44,45,46,47Cr, 43,44,45,46,47,48,49Mn, 44,45,46,47,48,49,50,51Fe, 47,48,49,50,51,52,53Co, 48,49,50,51,52,53,54,55Ni, 50,51,52,53,54,55,56,57Cu, 52,53,54,55,56,57,58,59Zn, 54,55,56,57,58,59,60,61Ga, 56,57,58,59,60,61,62,63Ge, 60,61,62,63,64,65As, 62,63,64,65,66,67Se, 65,66,67,68,69Br, 67,68,69,70,71Kr, 70,71,72,73Rb, 71,72,73,74,75Sr, 74,75,76,77Y, 75,76,77,78,79Zr, 78,79,80,81Nb, 79,80,81,82,83Mo, 82,83,84,85Tc, 84,85,86,87Ru, 86,87,88,89Rh, 88,89,90,91Pd, 90,91,92,93Ag, 92,93,94,95Cd, 94,95,96,97In, 96,97,98,99Sn; calculated S(p), S(2p), mass excesses for proton-rich systems, both inside and outside the proton drip line, in terms of mass relations for mirror nuclei, based on Weizsacker mass formula. Comparison with available evaluated experimental data from AME2020, and deduced root-mean-square deviations (RMSD).
doi: 10.1103/PhysRevC.105.034321
2021FA05 Appl.Radiat.Isot. 172, 109669 (2021) Y.Fan, Q.Li, Y.Wang, Y.Zhao, X.Zhang, H.Jia, Y.Chang, S.Liu, X.Ai, S.Wang Assessment of a compton-suppressed spectrometer for measurement of radioactive xenon isotopes RADIOACTIVITY 133Xe(β-), 127Xe(EC); measured decay products, Eγ, Iγ; deduced γ-ray energies and relative intensities.
doi: 10.1016/j.apradiso.2021.109669
2021LI35 Eur.Phys.J. A 57, 232 (2021); Erratum Eur.Phys.J. A 57, 252 (2021) X.Liu, Y.Yang, R.Liu, Z.Wen, J.Wen, Z.Han, Y.Chen, H.Jing, H.Yi, J.Bao, Z.Ren, Q.An, H.Bai, P.Cao, Q.Chen, P.Cheng, Z.Cui, R.Fan, C.Feng, M.Gu, F.Guo, C.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, W.Jiang, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, S.Liu, G.Luan, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, Q.Wu, X.Wu, X.Wu, L.Xie, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurement of the neutron total cross sections of aluminum at the back-n white neutron source of CSNS NUCLEAR REACTIONS 27Al(n, X), E<20 MeV; measured reaction products, En, In; deduced neutron transmission, total σ and uncertainties. Comparison withENDF/B-VIII.0, JEFF-3.3 and CENDL-3.2 library evaluations, EXFOR compilations. Spallation Neutron Source Science Center.
doi: 10.1140/epja/s10050-021-00513-9
2021LI54 J.Radioanal.Nucl.Chem. 330, 325 (2021) Q.Li, S.Wang, Y.Zhao, Y.Fan, X.Zhang, R.Zhang, H.Jia, Z.Zeng Geant4 simulation of detection efficiency and self-attenuation effect of β particles for radioxenon measurement using β-γ coincidence equipment RADIOACTIVITY 131,133Xe(IT), 133,135Xe(β-); calculated β-particles efficiencies, βγ-coin. using Geant4.
doi: 10.1007/s10967-021-07962-y
2021MA33 Phys.Rev. C 103, 054326 (2021) C.Ma, Y.Y.Zong, S.Q.Zhang, J.Li, K.Wang, Y.M.Zhao, A.Arima Mass relations of mirror nuclei in terms of Coulomb energies based on relativistic continuum Hartree-Bogoliubov calculations ATOMIC MASSES 18,19Ne, 19,20,21Na, 20,21,22,23Mg, 21,22,23,24,25Al, 22,23,24,25,26,27Si, 24,25,26,27,28,29P, 27,28,29,30,31S, 29,30,31,32,33Cl, 32,33,34,35Ar, 33,34,35,36,37K, 35,36,37,38,39Ca, 38,39,40,41Sc, 40,41,42,43Ti, 41,42,43,44,45V, 43,44,45,46,47Cr, 44,45,46,47,48,49Mn, 46,47,48,49,50,51Fe, 49,50,51,52,53Co, 50,51,52,53,54,55Ni, 53,54,55,56,57Cu, 56,57,58,59Zn, 59,60,61Ga, 60,61,62,63Ge, 62,63,64,65As, 65,66,67Se, 67,68,69Br, 69,70,71Kr, 71,72,73Rb, 73,74,75Sr, 75,76,77Y, 78,79Zr, 81Nb, 83Mo, 85Tc, 87Ru; calculated mass excesses, S(p), S(2p) of mirror nuclei, including masses of 61 unknown proton-rich nuclei, in terms of Coulomb energies based on relativistic continuum Hartree-Bogoliubov (RCHB) method. Numerical values listed in Supplemental material of the paper. Comparison with values in AME2016 database.
doi: 10.1103/PhysRevC.103.054326
2021MA43 Phys.Rev. C 104, 014303 (2021) C.Ma, Y.Y.Zong, Y.M.Zhao, A.Arima Evaluation of nuclear charge radii based on nuclear radii changes NUCLEAR STRUCTURE N=8-160; analyzed evaluated experimental data for nuclear charge-radii changes for two isotopes taken from 2013An02 database and later experimental results, and compared with the theoretical calculations based on HFB-31, RCHB, RMF+BCS and WS* models; deduced root-mean-square deviations (RMSD). Z=12, N=21-26, 30; Z=16, N=21-32, 34; Z=17, N=21-34; Z=18, N=20-36; Z=19, N=20-36; Z=20, N=20-38; Z=21, N=20-40; Z=22, N=20-43; Z=23, N=21-26, 27, 29-43; Z=24, N=20-43; Z=25, N=22-45; Z=26, N=21-46; Z=27, N=24-31, 33-46; Z=28, N=22-51; Z=29, N=28-51; Z=30, N=26-55; Z=31, N=30-64; Z=32, N=29-59; Z=33, N=33-41, 43-57; Z=34, N=31-63; Z=35, N=35-61; Z=36, N=33-71; Z=37, N=37-67; Z=38, N=36-72, 75-77; Z=39, N=39-78; Z=40, N=38-77; Z=41, N=41-77; Z=42, N=40-81; Z=44, N=42-75; Z=45, N=45-57, 59-73; Z=46, N=44-79; Z=47, N=47-77; Z=48, N=46-87; Z=49, N=50-93; Z=50, N=49-96; Z=51, N=57-87; Z=52, N=54-99; Z=53, N=59-89; Z=54, N=56-107; Z=55, N=61-106; Z=56, N=58-107; Z=57, N=63-97; Z=58, N=63-105; Z=59, N=67-81, 83-97; Z=60, N=63-105; Z=62, N=67-87, 90-107; Z=63, N=71-87, 90-111; Z=64, N=69-87, 90-111; Z=66, N=90-113; Z=67, N=78-87, 90-113; Z=68, N=76-117; Z=69, N=81-118; Z=70, N=78-122; Z=71, N=84-123; Z=72, N=83-125; Z=73, N=123; Z=74, N=91-127; Z=75, N=95-127; Z=76, N=93-131; Z=78, N=108-135; Z=79, N=108-135; Z=80, N=94-141; Z=81, N=103-142; Z=82, N=98-147; Z=84, N=105-149; Z=86, N=108-151; Z=87, N=115-155; Z=88, N=111-155; Z=90, N=122-155; Z=92, N=126-155; Z=94, N=132-155; Z=95, N=131-155; Z=96, N=131-155; calculated nuclear charge radii by using δRk values based on empirical formula in the present work and the WS* model for 1647 nuclei listed in the Supplemental Material of the paper.
doi: 10.1103/PhysRevC.104.014303
2021RE01 Nucl.Instrum.Methods Phys.Res. A985, 164703 (2021) J.Ren, X.Ruan, W.Jiang, J.Bao, G.Luan, Q.Zhang, H.Huang, Y.Nie, Z.Ge, Q.An, H.Bai, Y.Bao, P.Cao, H.Chen, Q.Chen, Y.Chen, Y.Chen, Z.Chen, Z.Cui, R.Fan, C.Feng, K.Gao, M.Gu, C.Han, Z.Han, G.He, Y.He, Y.Hong, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, Z.Jiang, H.Jing, L.Kang, M.Kang, B.Li, C.Li, J.Li, L.Li, Q.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, Q.Mu, C.Ning, B.Qi, Z.Ren, Y.Song, Z.Song, H.Sun, K.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, X.Tang, B.Tian, L.Wang, P.Wang, Q.Wang, T.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, H.Yi, L.Yu, T.Yu, Y.Yu, G.Zhang, L.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Background study for (n, γ) cross section measurements with C6D6 detectors at CSNS Back-n NUCLEAR REACTIONS 197Au, Pb, C, 181Ta, 59Co(n, γ), E<400 MeV; measured reaction products, Eγ, Iγ; deduced σ.
doi: 10.1016/j.nima.2020.164703
2021SU15 Phys.Rev. C 104, 014310 (2021) Y.Z.Sun, S.T.Wang, Z.Y.Sun, X.H.Zhang, S.Y.Jin, Y.X.Zhao, D.Y.Pang, S.W.Tang, D.Yan, P.Ma, Y.H.Yu, K.Yue, F.Fang, Y.J.Zhang, C.G.Lu, L.M.Duan Single-neutron removal from 14, 15, 16C near 240 MeV/nucleon NUCLEAR REACTIONS C(14C, 13C), E=235 MeV/nucleon; C(15C, 14C), E=237 MeV/nucleon; C(16C, 15C), E=239 MeV/nucleon, [secondary 14,15,16C beams from 9Be(18O, X), E=280 MeV/nucleon primary reactions, followed by separation of fragments using RIBLL2 at the HIRFL-CSR-Lanzhou facility]; measured reaction products, particle identification spectra for neutron-removal products using ionization chambers and plastic scintillators. 13,14,15C; deduced levels, J, π, inclusive single-nucleon removal σ, isospin asymmetry dependence of the reduction factor (σ(exp)/σ(theory)). Comparison with Glauber model predictions using shell-model spectroscopic factors.
doi: 10.1103/PhysRevC.104.014310
2021WE06 Nucl.Instrum.Methods Phys.Res. B496, 78 (2021) J.Wei, X.Zhou, R.Cheng, C.Liang, C.Mei, L.Zeng, Y.Chen, G.Xiao, X.Zhang, Y.Zhao Mg K-shell x-ray emission induced by various ions NUCLEAR REACTIONS Mg(H, X), E=0.0-0.3 MeV; Mg(He, X), E=0.1-0.6 MeV; Mg(Xe, X), E=1.2-6 MeV; (Eu, X), E=2-6 MeV; measured reaction products, X-rays; deduced K X-ray production σ. Comparison with available data.
doi: 10.1016/j.nimb.2021.03.023
2021YA19 Phys.Rev. C 104, 014901 (2021) P.Yang, L.Li, Y.Zhou, Z.Li, M.Xu, Y.Zhao, Y.Wu Measurement methods of radial flow in relativistic heavy-ion collisions
doi: 10.1103/PhysRevC.104.014901
2021ZH27 Nucl.Phys. A1011, 122201 (2021) D.Zhang, Y.Zhao, M.Xu, X.Pan, Y.Wu Rapidity window dependence of ridge correlations in the glasma
doi: 10.1016/j.nuclphysa.2021.122201
2020BA03 Chin.Phys.C 44, 014003 (2020) H.Bai, R.Fan, H.Jiang, Z.Cui, Y.Hu, G.Zhang, Z.Chen, W.Jiang, H.Yi, J.Tang, L.Zhou, Q.An, J.Bao, P.Cao, Q.Chen, Y.Chen, P.Cheng, C.Feng, M.Gu, F.Guo, C.Han, Z.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jing, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, R.Liu, S.Liu, X.Liu, G.Luan, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, J.Zhang, L.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurement of the differential cross sections and angle-integrated cross sections of the 6Li(n, t)4He reaction from 1.0 eV to 3.0 MeV at the CSNS Back-n white neutron source NUCLEAR REACTIONS 6Li(n, t), E=0.000001-3 MeV; measured reaction products; deduced σ. Comparison with ENDF/B-VIII.0 and JEFF-3.3 libraries, experimental data.
doi: 10.1088/1674-1137/44/1/014003
2020BA04 Phys.Rev. C 101, 014316 (2020) M.Bao, H.Jiang, Y.M.Zhao, A.Arima Low-lying states of even-even N=80 isotones within the nucleon-pair approximation NUCLEAR STRUCTURE 130Sn, 132Te, 134Xe, 136Ba, 138Ce; calculated levels, J, π, B(E2), g factors, configurations and wave functions, Matrix elements for nucleon-pair basis states, overlap squared between the proton and neutron excitation configuration, and the NPA wave function using nucleon-pair approximation (NPA) of the shell model. Comparison with experimental data, and with other theoretical predictions.
doi: 10.1103/PhysRevC.101.014316
2020BA34 Phys.Rev. C 102, 014306 (2020) M.Bao, Y.Y.Zong, Y.M.Zhao, A.Arima Local relations of nuclear charge radii NUCLEAR STRUCTURE Z=28-96;N=28-126; calculated nuclear charge radii using three approaches: δRin-jp relations based on the independent particle shell model, δRnn relation from nonpairing interaction δVnn in nuclear binding energies, and linear dependence of nuclear charge radii in terms of valence nucleon numbers. Comparison with experimental data evaluated in CR2013 database of 944 nuclei. Z=28, A=56-81; Z=29, A=57-86; Z=30, A=58-86; Z=31, A=59-88; Z=32, A=60-89; Z=33, A=65-90; Z=34, A=65-91; Z=35, A=69-92; Z=36, A=69-96; Z=37, A=72-98; Z=38, A=72-100; Z=39, A=76-102; Z=40, A=77-102; Z=41, A=80-103; Z=42, A=80-108; Z=44, A=86-126; Z=45, A=93-130; Z=46, A=92-130; Z=47, A=94-133; Z=48, A=95-134; Z=49, A=98-135; Z=50, A=99-136; Z=51, A=111-137; Z=52, A=106-138; Z=53, A=117-139; Z=54, A=109-146; Z=55, A=115-146; Z=56, A=115-148; Z=57, A=125-143; Z=58, A=126-148; Z=59, A=131-145; Z=60, A=128-150; Z=62, A=131-154; Z=63, A=133-159; Z=64, A=135-160; Z=65, A=147-159; Z=66, A=146-173; Z=67, A=151-173; Z=68, A=150-177; Z=69, A=153-184; Z=70, A=152-188; Z=71, A=161-189; Z=72, A=163-196; Z=73, A=171-203; Z=74, A=170-204; Z=75, A=185-207; Z=76, A=175-208; Z=77, A=182-209; Z=78, A=178-210; Z=79, A=183-211; Z=80, A=181-214; Z=81, A=183-209; Z=82, A=182-216; Z=83, A=202-213; Z=84, A=192-220; Z=86, A=195-227; Z=87, A=206-228; Z=88, A=205-232; Z=90, A=226-236; Z=92, A=229-238; Z=94, A=235-244; Z=95, A=241-245; Z=96, A=242-248; calculated unknown nuclear charge radii for 830 nuclei using the same three approaches, and listed in a data file in the Supplementary material of the paper.
doi: 10.1103/PhysRevC.102.014306
2020DE15 J.Radioanal.Nucl.Chem. 324, 705 (2020) J.S.Denton, K.C.Treinen, Y.Chen, E.Baransky, A.M.Gaffney, S.-H.HuangH.T.M.Kayzar-Boggs, K.Samperton, R.E.Steiner, A.M.Wende, R.W.Williams, Y.-G.Zhao International cooperation in age-dating uranium standards for nuclear forensics using the 231Pa/235U radiochronometer RADIOACTIVITY 231Pa, 235U(α); measured decay products using radiochemical methods; deduced that the 231Pa/235U model purification dates calculated for CRMs U010 (October 14, 1957 to June 17, 1959) and U850 (April 8, 1957 to December 4, 1961) are generally concordant between laboratories and agree within analytical uncertainty with the production histories of both CRMs.
doi: 10.1007/s10967-020-07084-x
2020FO11 Phys.Lett. B 811, 135869 (2020) Dark matter capture by atomic nuclei
doi: 10.1016/j.physletb.2020.135869
2020JI06 Nucl.Instrum.Methods Phys.Res. A973, 164126 (2020) W.Jiang, H.Bai, H.Jiang, H.Yi, R.Fan, G.Zhang, J.Tang, Z.Sun, C.Ning, K.Sun, K.Gao, Z.Cui, Q.An, J.Bao, Y.Bao, P.Cao, H.Chen, Q.Chen, Y.Chen, Y.Chen, Z.Chen, C.Feng, M.Gu, F.Guo, C.Han, Z.Han, G.He, Y.He, Y.Hong, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, Z.Jiang, H.Jing, L.Kang, M.Kang, B.Li, C.Li, J.Li, L.Li, Q.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, G.Luan, Q.Mu, B.Qi, J.Ren, Z.Ren, X.Ruan, Y.Song, Z.Song, H.Sun, X.Sun, Z.Tan, H.Tang, X.Tang, B.Tian, L.Wang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, L.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Application of a silicon detector array in (n, lcp) reaction cross-section measurements at the CSNS Back-n white neutron source NUCLEAR REACTIONS 6Li(n, t), 10B(n, α), E<1 MeV; measured reaction products, En, In; deduced σ. Comparison with experimental data, ENDF/B-VIII.0, JEFF-3.3, ROSFOND evaluated libraries.
doi: 10.1016/j.nima.2020.164126
2020LI06 Phys.Rev. C 101, 024305 (2020) P.F.Liang, L.J.Sun, J.Lee, S.Q.Hou, X.X.Xu, C.J.Lin, C.X.Yuan, J.J.He, Z.H.Li, J.S.Wang, D.X.Wang, H.Y.Wu, Y.Y.Yang, Y.H.Lam, P.Ma, F.F.Duan, Z.H.Gao, Q.Hu, Z.Bai, J.B.Ma, J.G.Wang, F.P.Zhong, C.G.Wu, D.W.Luo, Y.Jiang, Y.Liu, D.S.Hou, R.Li, N.R.Ma, W.H.Ma, G.Z.Shi, G.M.Yu, D.Patel, S.Y.Jin, Y.F.Wang, Y.C.Yu, Q.W.Zhou, P.Wang, L.Y.Hu, X.Wang, H.L.Zang, P.J.Li, Q.Q.Zhao, H.M.Jia, L.Yang, P.W.Wen, F.Yang, G.L.Zhang, M.Pan, X.Y.Wang, H.H.Sun, Z.G.Hu, R.F.Chen, M.L.Liu, W.Q.Yang, Y.M.Zhao Simultaneous measurement of β-delayed proton and γ emission of 26P for the 25Al(p, γ)26Si reaction rate RADIOACTIVITY 26P(β+), (β+p)[from 9Be(32S, X), E=806 MeV/nucleon, followed by in-flight separation by the RIBLL1 fragment separator at HIRFL-Lanzhou]; measured E(p), I(p), Eγ, Iγ, βp- and βγ-coin, half-life of the decay of 26P from correlated events of 26P implants and successive decays using three double-sided silicon strip detectors (DSSDs), five Clover-type HPGe detectors, and five quadrant silicon detectors (Q SDs). 26Si; deduced levels, J, π, Γp and Γγ of 5929, 3+ state. Comparison with previous experimental data, and with shell-model calculations. NUCLEAR REACTIONS 9Be(32S, X)22Na/23Mg/24Al/25Si/26P, E=806 MeV/nucleon; measured reaction products and TOF-ΔE spectrum using in-flight separation by the RIBLL1 fragment separator at HIRFL-Lanzhou. 25Al(p, γ)26Si, T=0.03-1.1 GK; deduced energies and strengths of resonances, corresponding astrophysical reaction rates, and compared with data in JINA REACLIB database.
doi: 10.1103/PhysRevC.101.024305
2020LI33 Nucl.Instrum.Methods Phys.Res. A980, 164506 (2020) Q.Li, H.Jing, B.Zhou, C.Ning, J.Tang, J.Ren, H.Yi, X.Zhu, L.Zhang, W.Jiang, R.Fan, J.Bao, C.Feng, X.Ruan, Y.Chen, L.Zhou, Y.Li, Z.Tan, Y.Chen, Q.An, H.Bai, P.Cao, Q.Chen, P.Cheng, Z.Cui, M.Gu, F.Guo, C.Han, Z.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, L.Kang, M.Kang, B.Li, L.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, G.Luan, Y.Ma, B.Qi, Z.Song, H.Sun, X.Sun, Z.Sun, H.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Neutron and γ background measurements of the experimental halls at the CSNS back-streaming white neutron source
doi: 10.1016/j.nima.2020.164506
2020MA19 Phys.Rev. C 101, 045204 (2020) C.Ma, M.Bao, Z.M.Niu, Y.M.Zhao, A.Arima New extrapolation method for predicting nuclear masses ATOMIC MASSES 121Rh, 123Pd, 129,131Cd, 138Sb, 141I, 149Ba, 150,151La, 137Eu, 190Tl, 215Pb, 194Bi, 198At, 197,198,202,232,233Fr, 201Ra, 205,206Ac, 215,216,221,222U, 219Np, 229Am, 259No; A=20-260; Z=36-106, N=56-160; calculated mass excesses using method based on the Garvey-Kelson mass relations and the Jannecke mass formulas. Comparison with evaluated data in AME2016, and other theoretical predictions over the entire chart of nuclides. Z=43-106, A=120-273; predicted masses in Supplemental material for about 600 nuclei for which no experimental data exist. Z=8-106, N=10-157; deduced parameters for each prediction of masses based on AME2016, listed in Supplemental material.
doi: 10.1103/PhysRevC.101.045204
2020MA35 Phys.Rev. C 102, 024330 (2020) C.Ma, Y.Y.Zong, Y.M.Zhao, A.Arima Mass relations of mirror nuclei with local correlations ATOMIC MASSES 41Ti, 43,44V, 45Cr, 47,48Mn, 49Fe, 51,52Co, 53Ni, 55,56Cu; calculated extrapolated mass excesses by analyzing correlations between deviations between theoretical results and experimental data, the latter from AME1995 and AME2016. 34Ca, 38,39Ti, 42Cr, 59Ge, 66Kr, 70,71Sr; calculated Q(2p) and Q(p) for proton-rich nuclei. Z=12-38, N=6-38; predicted proton and diproton drip lines based on predicted masses in the present work. 34Ca, 38,39Ti, 42Cr, 59Ge, 66Kr, 70,71Sr; predicted 2p emitters. 19Mg, 45Fe, 48Ni, 54Zn, 67Kr; experimentally suggested to be 2p emitters, consistent with predictions in the present work. Z=10-44, N=8-37, A=18-81; calculated mass excesses of 292 proton-rich nuclei and compared with available mass excesses in AME2016. Examined mass relations of mirror nuclei with local correlations, with odd-even staggering of Coulomb energy.
doi: 10.1103/PhysRevC.102.024330
2020RE11 Phys.Rev. C 102, 034604 (2020) Z.Ren, Y.Yang, J.Wen, H.Guo, Z.Wen, R.Liu, Z.Han, W.Sun, X.Liu, Q.Chen, T.Ye, Q.An, H.Bai, J.Bao, P.Cao, Y.Chen, P.Cheng, Z.Cui, R.Fan, C.Feng, M.Gu, F.Guo, C.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, W.Jiang, H.Jing, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, S.Liu, G.Luan, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, Q.Wu, X.Wu, X.Wu, L.Xie, H.Yi, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurement of the 236U(n, f) cross section for neutron energies from 0.4 MeV to 40 MeV from the back-streaming white neutron beam at the China Spallation Neutron Source NUCLEAR REACTIONS 235,236U(n, F), E AP 0.4-40 MeV beam from the China Spallation Neutron Source (CSNS)-Back-streaming white neutron source (WNS); measured fission fragments, energy spectra, time-of-flight using Fast Ionization Chamber Spectrometer; deduced 236U(n, F)/235U(n, F) cross section ratios. Comparison with theoretical calculation using the UNF code, and with evaluated data in JENDL-4.0, CENDL-3.1, and ENDF/B-VIII.0 libraries.
doi: 10.1103/PhysRevC.102.034604
2020WE04 Ann.Nucl.Energy 140, 107301 (2020) J.Wen, Y.Yang, Z.Wen, R.Liu, X.Liu, Z.Han, Q.Chen, Z.Ren, Q.An, H.Bai, J.Bao, P.Cao, Y.Chen, P.Cheng, Z.Cui, R.Fan, C.Feng, M.Gu, F.Guo, C.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, W.Jiang, H.Jing, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, S.Liu, G.Luan, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, Q.Wu, X.Wu, X.Wu, L.Xie, H.Yi, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurement of the U-238/U-235 fission cross section ratio at CSNS - Back-in WNS NUCLEAR REACTIONS 235,238U(n, F), E=1-20 MeV; measured reaction products, fission fragments, Eγ, Iγ; deduced neutron resonances, σ. Comparison with ENDF/B-VIII.0 library evaluations.
doi: 10.1016/j.anucene.2019.107301
2020ZH07 Eur.Phys.J. A 56, 57 (2020) The effect of gluon condensate on imaginary potential and thermal width from holography
doi: 10.1140/epja/s10050-020-00072-5
2020ZO03 Phys.Rev. C 102, 024302 (2020) Y.Y.Zong, C.Ma, Y.M.Zhao, A.Arima Mass relations of mirror nuclei ATOMIC MASSES Z=11-47, N=10-43, A=21-90; analyzed mass relations of mirror nuclei by comparing theoretical values and AME2016 evaluated data through root-mean squared deviations (RMSD); predicted mass excesses of experimentally inaccessible proton-rich nuclei.
doi: 10.1103/PhysRevC.102.024302
2019CH32 Phys.Rev. C 100, 014318 (2019) Y.-Y.Cheng, J.-Ji.Shen, G.-J.Fu, X.-R.Zhou, Y.-M.Zhao, A.Arima Nucleon-pair wave functions in a single-J shell
doi: 10.1103/PhysRevC.100.014318
2019CH35 Phys.Rev. C 100, 024321 (2019) Y.-Y.Cheng, H.Wang, J.-J.Shen, X.-R.Zhou, Y.-M.Zhao, A.Arima Nucleon-pair picture of low-lying states in semi-magic and open-shell nuclei NUCLEAR STRUCTURE 43,44,45,46,47,48Ca, 130Pd, 131Ag, 132Cd; calculated level energies vs spin for negative-parity yrast states of odd-mass Ca and positive-parity yrast states for even mass Ca isotopes, overlaps between one-dimensional nucleon-pair wave functions and corresponding shell-model wave functions, nucleon-pair wave functions using the framework of nucleon-pair approximation (NPA) of the shell model. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.024321
2019CH37 Eur.Phys.J. A 55, 115 (2019), Erratum Eur.Phys.J. A 55, 145 (2019) Y.Chen, G.Luan, J.Bao, H.Jing, L.Zhang, Q.An, H.Bai, P.Cao, Q.Chen, P.Cheng, Z.Cui, R.Fan, C.Feng, M.Gu, F.Guo, Ch.Han, Z.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, W.Jiang, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, R.Liu, S.Liu, X.Liu, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, H.Yi, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Neutron energy spectrum measurement of the Back-n white neutron source at CSNS
doi: 10.1140/epja/i2019-12808-1
2019CH53 J.Radioanal.Nucl.Chem. 322, 1605 (2019) Y.Chen, S.-H.Huang, R.i-X.Hu, Y.-G.Zhao, L.-L.Li, J.-J.Zhou, C.Li, J.-L.Zhang, Z.-H.Wu Age determination for uranium standard samples by 231Pa/235U radiochronometer
doi: 10.1007/s10967-019-06922-x
2019JI07 Chin.Phys.C 43, 124002 (2019) H.Jiang, W.Jiang, H.Bai, Z.Cui, G.Zhang, R.Fan, H.Yi, C.Ning, L.Zhou, J.Tang, Q.An, J.Bao, Y.Bao, P.Cao, H.Chen, Q.Chen, Y.Chen, Y.Chen, Z.Chen, C.Feng, K.Gao, M.Gu, C.Han, Z.Han, G.He, Y.He, Y.Hong, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, Z.Jiang, H.Jing, L.Kang, M.Kang, B.Li, C.Li, J.Li, L.Li, Q.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, G.Luan, Q.Mu, B.Qi, J.Ren, Z.Ren, X.Ruan, Z.Song, Y.Song, H.Sun, K.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, X.Tang, B.Tian, L.Wang, P.Wang, Q.Wang, T.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, L.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurements of differential and angle-integrated cross sections for the 10B(n, α)7Li reaction in the neutron energy range from 1.0 eV to 2.5 MeV NUCLEAR REACTIONS 10B(n, α), E=0.000001-2.5 MeV; measured reaction products, Eα, Iα; deduced σ(θ), σ and uncertainties. Comparison with ENDF/B-VIII.0, JEFF-3.3, CENDL-3.1 and JENDL 4.0 libraries.
doi: 10.1088/1674-1137/43/12/124002
2019LI11 Appl.Radiat.Isot. 146, 29 (2019) Q.Li, S.Wang, Y.Fan, Y.Zhao, H.Jia, X.Zhang, S.Liu Measurement of the gamma-ray emission probability of 131mXe RADIOACTIVITY 131mXe(IT)[from 131I decay]; measured Eγ, Iγ; deduced γ-ray emission probability. Comparison with ENSDF and DDEP evaluated data.
doi: 10.1016/j.apradiso.2019.01.010
2019SU03 Phys.Rev. C 99, 024605 (2019) Y.Z.Sun, S.T.Wang, Z.Y.Sun, X.H.Zhang, D.Yan, B.H.Sun, J.W.Zhao, Y.P.Xu, D.Y.Pang, Y.H.Yu, K.Yue, S.W.Tang, C.Dong, Y.X.Zhao, F.Fang, Y.Sun, Z.H.Cheng, X.M.Liu, P.Ma, H.R.Yang, C.G.Lu, L.M.Duan Two-neutron removal cross sections from 15, 16C at around 240 MeV/nucleon NUCLEAR REACTIONS 12C(15C, X), (15C, 13C), (16C, X), (16C, 14C)8Li/10Be/11Be/12B/13B/15C/16C/17N, E=237, 239 MeV/nucleon, [secondary 15,16C beams from 9Be(18O, X), E=280 MeV/nucleon primary reaction followed by in-flight fragment separator RIBLL2 at HIRFL-Lanzhou]; measured reaction products, particle identification spectra, time of flight of fragments, and two-neutron removal σ(E) using multiwire drift chambers for particle detection and identification, and plastic scintillators for time of flight measurements. Comparison with previous experimental values, and theoretical calculations for two-neutron removal σ based on eikonal-model and shell-model structure information. Systematics of odd-even staggering in two-neutron removal σ from 15,16,17,18,19,20C projectiles.
doi: 10.1103/PhysRevC.99.024605
2019YU03 Phys.Rev. C 100, 014314 (2019) H.C.Yu, M.Q.Lin, M.Bao, Y.M.Zhao, A.Arima Empirical formulas for nuclear separation energies NUCLEAR STRUCTURE 70,71,72,73,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100Zn, 112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137Mo, 151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186Ba, 204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239W; calculated S(n) and S(p) using empirical formulas. Comparison with AME-2016 evaluation, and with other theoretical model predictions.
doi: 10.1103/PhysRevC.100.014314
2019ZH46 Phys.Rev. C 100, 044609 (2019) Y.X.Zhao, Y.Z.Sun, S.T.Wang, Z.Y.Sun, X.H.Zhang, D.Yan, D.Y.Pang, P.Ma, Y.H.Yu, K.Yue, S.W.Tang, S.M.Wang, F.Fang, Y.Sun, Z.H.Cheng, X.M.Liu, H.R.Yang, C.G.Lu, L.M.Duan One-proton knockout from 16C at around 240 MeV/nucleon NUCLEAR REACTIONS 12C(16C, 15B), E=239 MeV/nucleon, [secondary16O beam from 9Be(18O, X)8Li/10Be/11Be/13B/16C, E=280 MeV/nucleon primary reaction using RIBLL2 at HRIFL-Lanzhou facility]; measured reaction products by magnetic rigidity (Bρ), time of flight (TOF), and energy loss (ΔE), mass yields. 16C, 15B; deduced σ for one-proton knockout, spectroscopic reduction factor. Comparison to predictions based on the eikonal reaction model with shell-model structure inputs, and with previous experimental data for 9Be(16C, 15B), E=75 MeV/nucleon reaction. Discussed energy dependence of the spectroscopic reduction factor, and the role of surface neutrons as spectators.
doi: 10.1103/PhysRevC.100.044609
2019ZO02 Phys.Rev. C 100, 054315 (2019) Y.Y.Zong, M.Q.Lin, M.Bao, Y.M.Zhao, A.Arima Mass relations of corresponding mirror nuclei ATOMIC MASSES 21Na, 22,23Mg, 23,24,25Al, 24,25,26,27Si, 26,27,28,29P, 28,29,30,31S, 30,31,32,33Cl, 32,33,34,35Ar, 34,35,36,37K, 36,37,38,39Ca, 38,39,40,41Sc, 40,41,42,43Ti, 42,43,44,45V, 44,45,46,47Cr, 46,47,48,49Mn, 48,49,50,51Fe, 50,51,52,53Co, 52,53,54,55Ni, 54,55,56,57Cu, 56,57,58,59Zn, 58,59,60,61Ga, 60,61,62,63Ge, 62,63,64,65As, 64,65,66,67Se, 66,67,68,69Br, 68,69,70,71Kr, 70,71,72,73Rb, 72,73,74,75Sr, 74,75,76,77Y, 76,77,78,79Zr, 79,80Nb, 81,83Mo, 83,85Tc, 85,86,87Ru, 87,88Rh, 89Pd; calculated mass excesses, S(n), S(p) using mass relations for corresponding mirror nuclei, and compared with AME2016 values; deduced regularities related to neutron-proton interactions, and to separation energies for mirror nuclei.
doi: 10.1103/PhysRevC.100.054315
2018CH05 Phys.Rev. C 97, 024303 (2018) Nucleon-pair approximation with particle-hole excitations NUCLEAR STRUCTURE 100Sn; calculated energies and B(E2) of the yrast states up to 6+ with both proton and neutron particle-hole excitations up to 4p-4h. Multiple-major-shell nucleon pair approximation (NPA) calculations with particle-hole excitations, where particles and holes are treated simultaneously.
doi: 10.1103/PhysRevC.97.024303
2018FU04 Phys.Rev. C 97, 024337 (2018) Pair correlations in low-lying T=0 states of odd-odd nuclei with six nucleons NUCLEAR STRUCTURE 22Na, 34Cl, 46V, 62Ga, 94Ag; calculated overlaps between the pair-truncated wave functions and the shell-model wave functions, level energies, J, π, electric quadrupole moments of T=0 yrast states for N=Z nuclei, total isovector and isoscalar correlation energies. Shell-model calculations with USDB interaction for 22Na and 34Cl, GXPF1 for 46V, and JUN45 for 62Ga and 94Ag, and S-broken-pair approximation, the isoscalar spin-1 pair condensation, and the isoscalar spin-aligned pair condensation, using schematic interactions.
doi: 10.1103/PhysRevC.97.024337
2018FU06 Phys.Rev. C 97, 024339 (2018) G.J.Fu, Y.Y.Cheng, Y.H.Zhang, P.Zhang, P.Shuai, Y.M.Zhao, M.Wang New local mass relation for isobaric analogue states and isospin-nonconserving forces ATOMIC MASSES A=20-60; A=41-52; derived a new local mass relation for isobaric analog states of four neighboring nuclei, and compared with AME-2012 and IAS-2014 evaluations; discussed empirical Coulomb energy formula and the isobaric multiplet mass equation (IMME), and odd-even staggering of the IMME coefficients.
doi: 10.1103/PhysRevC.97.024339
2018FU13 Phys.Rev. C 98, 034301 (2018) G.J.Fu, Y.Zhang, Y.M.Zhao, A.Arima Collective modes of low-lying states in the interacting boson model with random interactions
doi: 10.1103/PhysRevC.98.034301
2018ZH27 Chin.Phys.C 42, 074103 (2018) Y.-W.Zhao, S.-Q.Guo, H.-F.Zhang α particle preformation and shell effect for heavy and superheavy nuclei NUCLEAR STRUCTURE Z=84-92; calculated α particle preformation factor;deduced another subshell closure after Z = 124 in the superheavy nuclei.
doi: 10.1088/1674-1137/42/7/074103
2017BA11 Phys.Rev. C 95, 044310 (2017) M.Bao, Y.Y.Cheng, Y.M.Zhao, A.Arima Local mass relations and the NpNn scheme NUCLEAR STRUCTURE Z=82-104, N=126-155; analyzed Castens NpNn scheme for nuclear masses, and charge radii of four neighboring nuclei. N=10-160; analyzed energies and B(E2) for the first 2+ states of four neighboring even-even nuclei.
doi: 10.1103/PhysRevC.95.044310
2017CH44 J.Phys.(London) G44, 115102 (2017) Y.Y.Cheng, H.Jiang, Y.M.Zhao, A.Arima Improved mass extrapolations by the Garvey-Kelson relations NUCLEAR STRUCTURE N=1-160; calculated binding energy uncertainties, separation energies. Comparison with AME95, AME03 mass tables.
doi: 10.1088/1361-6471/aa8a25
2017CH56 Chin.Phys.C 41, 104103 (2017) L.-Z.Chen, Y.-Y.Zhao, X.Pan, Z.-M.Li, Y.-F.Wu High cumulants of conserved charges and their statistical uncertainties
doi: 10.1088/1674-1137/41/10/104103
2017FU09 Phys.Rev. C 96, 044306 (2017) G.J.Fu, L.Y.Jia, Y.M.Zhao, A.Arima Monopole pairing correlations with random interactions
doi: 10.1103/PhysRevC.96.044306
2017MA47 Nucl.Phys. A966, 294 (2017) X.B.Ma, Y.F.Zhao, Y.X.Chen, W.L.Zhong, F.P.An Antineutrino flux and spectrum calculation for spent nuclear fuel for the Daya Bay antineutrino experiment
doi: 10.1016/j.nuclphysa.2017.06.009
2017ZH14 Eur.Phys.J. A 53, 55 (2017) Y.X.Zhao, A.Deshpande, J.Huang, K.S.Kumar, S.Riordan Neutral-current weak interactions at an EIC
doi: 10.1140/epja/i2017-12245-2
2017ZH18 Phys.Rev. C 95, 041602 (2017) Y.Zhang, J.Tian, W.Cheng, F.Guan, Y.Huang, H.Li, L.Lu, R.Wang, Y.Wang, Q.Wu, H.Yi, Z.Zhang, Y.Zhao, L.Duan, R.J.Hu, M.Huang, G.Jin, S.Jin, C.G.Lu, J.Ma, P.Ma, J.Wang, H.Yang, Y.Yang, J.Zhang, Ya.Zhang, Y.Zhang, C.Ma, C.Y.Qiao, M.B.Tsang, Z.Xiao Long-time drift of the isospin degree of freedom in heavy ion collisions NUCLEAR REACTIONS Au(40Ar, X), E=30 MeV/nucleon; measured light-charged particles (LCP), α-spectra, coincident fission fragments, (LCP)(fission fragments)-coin using parallel plate avalanche counters (PPAC) and nine ΔE telescopes at RIBLL-Lanzhou facility; deduced inclusive isotopic ratio for Z=1 and 2 isotopes as a function of laboratory angle, angular distribution of the relative neutron richness summed over the LCPs, drift of the isospin degree of freedom (IDOF). Comparison with ImQMD+GEMINI simulations.
doi: 10.1103/PhysRevC.95.041602
2017ZH33 Nucl.Instrum.Methods Phys.Res. B408, 140 (2017) X.Zhou, R.Cheng, Y.Wang, Y.Lei, Y.Chen, X.Chen, Y.Zhao, G.Xiao L x-ray production in ionization of 60Nd by 100-250 keV protons NUCLEAR REACTIONS Nd(p, X), E=100-250 keV; measured reaction products, L X-rays; deduced production cross sections of Li, Lα, Lβ and Lγ x rays. Comparison with theoretical calculations of PWBA, ECPSSR and ECUSAR, along with various atomic parameter databases.
doi: 10.1016/j.nimb.2017.03.102
2016BA03 Phys.Rev. C 93, 014307 (2016) Number of states for identical particles
doi: 10.1103/PhysRevC.93.014307
2016BA54 Phys.Rev. C 94, 044323 (2016) M.Bao, Y.Lu, Y.M.Zhao, A.Arima Simple relations between masses of mirror nuclei ATOMIC MASSES A=3-110; Z=2-56, N=1-54; deduced a relation between difference of neutron and proton separation energies, and difference of Coulomb energies between two mirror nuclei; deduced mass excesses of nuclei and compared with AME-2012 values.
doi: 10.1103/PhysRevC.94.044323
2016BA64 Phys.Rev. C 94, 064315 (2016) M.Bao, Y.Lu, Y.M.Zhao, A.Arima Predictions of nuclear charge radii NUCLEAR STRUCTURE Z=6-95, N=10-150; analyzed charge radii for nuclei using empirical formulas and CR1999, CR2004 and CR2013 databases for charge radii; predicted values for unknown charge radii of ground states of 1085 nuclei.
doi: 10.1103/PhysRevC.94.064315
2016CH31 Phys.Rev. C 94, 024307 (2016) Nucleon-pair states of even-even N=82 isotones NUCLEAR STRUCTURE 134Te, 136Xe, 138Ba, 140Ce, 142Nd; calculated levels, J, π, B(E2), B(E3), magnetic dipole moments, first and second 6+ states. Framework of the nucleon-pair approximation (NPA) of the shell model, with full shell-model (SM) space and truncated NPA space. Comparison with experimental values taken from the ENSDF database.
doi: 10.1103/PhysRevC.94.024307
2016CH32 Phys.Rev. C 94, 024321 (2016) Y.Y.Cheng, C.Qi, Y.M.Zhao, A.Arima Nucleon-pair states of even-even Sn isotopes based on realistic effective interactions NUCLEAR STRUCTURE 104,106,108,128,126,124Sn; calculated levels, yrast states, J, π, B(E2), magnetic dipole moments, neutron-hole occupation number of the pseudo 13/2+ and 17/2- shells. Discussed seniority scheme. Monopole-optimized effective interactions based on the realistic CD-Bonn nucleon-nucleon potential, within the frameworks of the nucleon-pair approximation (NPA) and shell model (SM). Comparison with experimental values taken mainly from the ENSDF database.
doi: 10.1103/PhysRevC.94.024321
2016FU05 Phys.Rev. C 94, 024312 (2016) G.J.Fu, Y.Y.Cheng, H.Jiang, Y.M.Zhao, A.Arima Odd-even staggering of binding energy for nuclei in the sd shell NUCLEAR STRUCTURE 18,19,20,21,22,23,24,25F, 20,21,22,23,24,25,26,27,28Ne, 22,23,24,25,26,27,28,29Na, 24,25,26,27,28,29,30Mg, 26,27,28,29,30,31Al, 28,29,30,31,32,33,34Si, 30,31,32,33,34,35P, 32,33,34,35,36S, 34,35,36,37Cl, 36,37,38Ar, 38,39K; calculated ground-state energies, empirical proton-neutron interactions, Wigner energy coefficients, S(n); deduced odd-even staggering phenomena of nuclear binding energies. Shell model with the USDB interaction.
doi: 10.1103/PhysRevC.94.024312
2016FU06 Phys.Rev. C 94, 024336 (2016) G.J.Fu, Y.Y.Cheng, Y.M.Zhao, A.Arima Shell model study of T=0 states for 96Cd by the nucleon-pair approximation NUCLEAR STRUCTURE 96Cd; calculated low-lying isospin=0, levels, J, π, B(E2), magnetic dipole and electric quadrupole moments using several different approaches: shell model with JUN45 interaction, lowest seniority scheme, spin-aligned pair approximation, Jmax pair approximation, spin-one pair approximation, isovector and isoscalar pair approximations.
doi: 10.1103/PhysRevC.94.024336
2016JI16 Phys.Rev. C 94, 064301 (2016) H.Jiang, Y.Y.Cheng, N.Wang, Li.-W.Chen, Y.M.Zhao, A.Arima Robustness of the I4 symmetry energy coefficient ATOMIC MASSES A=16-300, Z>8, N>8; analyzed I4 symmetry energy coefficient extracted from popular mass models and corresponding databases improved by the radial basis function (RBF) approach and the RBF with odd-even correction; deduced robust linear correlation between present I4 symmetry energy coefficients and the corresponding rms deviations from experimental masses of these theoretical databases.
doi: 10.1103/PhysRevC.94.064301
2016KE01 Nucl.Instrum.Methods Phys.Res. B373, 1 (2016) Reproducibility of (n, γ) gamma ray spectrum in Pb under different ENDF/B releases NUCLEAR REACTIONS Pb(n, γ), E<20 MeV; calculated Eγ, Iγ using MCNP. Comparison with ENDF/B-V, ENDF/B-VI and ENDF/B-VII evaluated nuclear libraries.
doi: 10.1016/j.nimb.2016.02.028
2016LE04 Nucl.Instrum.Methods Phys.Res. B370, 10 (2016) Y.Lei, Y.Zhao, X.Zhou, R.Cheng, X.Wang, Y.Sun, S.Liu, J.Ren, Y.Wang, X.Zhang, Y.Li, C.Liang, G.Xiao K-shell X-ray production in Silicon (Z2 = 14) by (1 ≤ Z1 ≤ 53) slow ions NUCLEAR REACTIONS Si(H, X), (α, X), (Ne, X), (Ar, X), (I, X), E<600 MeV; measured reaction products, X-rays; deduced σ. Comparison with theoretical calculations.
doi: 10.1016/j.nimb.2015.12.045
2016ZH27 Nucl.Phys. A955, 88 (2016) Y.-Y.Zhao, M.-M.Xu, H.-Y.Zhang, Y.-F.Wu Two-gluon rapidity correlations of strong colour field in pp, pA and AA collisions
doi: 10.1016/j.nuclphysa.2016.06.007
2015CH10 Phys.Rev. C 91, 024313 (2015) Y.Y.Cheng, M.Bao, Y.M.Zhao, A.Arima Wigner energy and nuclear mass relations ATOMIC MASSES A=5-80; 58Cu, 98In; calculated Wigner energy, pairing and symmetry energies, binding-energy difference between the lowest T=0 and T=1 states of odd-odd N=Z nuclei by using local mass relations, in the first-order approximation. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.024313
2015CH11 Phys.Rev. C 91, 024314 (2015) Odd-even staggering in the neutron-proton interaction and nuclear mass models ATOMIC MASSES A=60-250; analyzed odd-even staggering of the empirical neutron-proton interaction between the last neutron and the last proton δV1n-1p between even-even, odd-odd, even-odd and odd-even nuclei, and their consequences in Garvey-Kelson (GKs), Duflo-Zuker (DZ) and Weizsacker-Skyrme (WS) mass models. Description of binding energies and S(n), using AME-2012 mass data.
doi: 10.1103/PhysRevC.91.024314
2015CH63 Phys.Rev. C 92, 064320 (2015) Y.Y.Cheng, Y.Lei, Y.M.Zhao, A.Arima Low-lying states of the 132Ba nucleus within the nucleon-pair approximation NUCLEAR STRUCTURE 132Ba; calculated levels, J, π, bands, B(E2), g factors, configurations, band crossings and backbends. Nucleon-pair approximation of the shell model with five neutron configuration spaces. Comparison with experimental data.
doi: 10.1103/PhysRevC.92.064320
2015FU05 Phys.Rev. C 91, 054318 (2015) Quartet structure in atomic nuclei NUCLEAR STRUCTURE 92Pd; calculated quartet correlation in the ground state in the p1/2p3/2f5/2g9/2 shell using JUN45 effective interaction; deduced validity of the stretch scheme, tightly bound cluster character of quartet, and weak interaction between the two quartets.
doi: 10.1103/PhysRevC.91.054318
2015FU06 Phys.Rev. C 91, 054319 (2015) G.J.Fu, J.J.Shen, Y.M.Zhao, A.Arima Regularities in low-lying states of atomic nuclei with random interactions
doi: 10.1103/PhysRevC.91.054319
2015FU07 Phys.Rev. C 91, 054322 (2015) Nucleon-pair approximations for low-lying states of even-even N=Z nuclei NUCLEAR STRUCTURE 20Ne, 24Mg, 32S, 36Ar, 44Ti, 48Cr, 60Zn, 64Ge, 92Pd, 96Cd; calculated ground-state energies, overlaps between the pair-condensation wave function and the shell-model wave function for N=Z nuclei. Isovector and isoscalar pair approximation calculations for low-lying T=0 states of an eight-nucleon system, with both schematic and realistic interactions. Effect of spin-orbit coupling potential on the isovector and isoscalar pair condensations.
doi: 10.1103/PhysRevC.91.054322
2015JI06 Phys.Rev. C 91, 054302 (2015) H.Jiang, N.Wang, L.-W.Chen, Y.M.Zhao, A.Arima Model dependence of the I4 term in the symmetry energy for finite nuclei
doi: 10.1103/PhysRevC.91.054302
2015LU01 Phys.Rev. C 91, 027301 (2015) Spin I ground state probabilities of integrable systems under random interactions
doi: 10.1103/PhysRevC.91.027301
2015MO14 Nucl.Instrum.Methods Phys.Res. B358, 32 (2015) J.Monari Kebwaro, Y.Zhao, C.He Investigation of photoneutron and capture gamma-ray production in Pb and W under irradiation from 16N decay radiation NUCLEAR REACTIONS Pb, W(γ, n), E<1 MeV; calculated photoneutron and capture gamma-ray spectra in the two materials when irradiated by 16N decay radiation with MCNP. Comparison with ENDF/B-VII.1 evaluated library.
doi: 10.1016/j.nimb.2015.05.012
2015WA14 Phys.Rev. C 91, 044308 (2015) N.Wang, M.Liu, H.Jiang, J.L.Tian, Y.M.Zhao Mass dependence of symmetry energy coefficients in the Skyrme force ATOMIC MASSES A=160; A=20-300; A=20-106; analyzed properties of nuclear symmetry energy as function of mass using the extended Thomas-Fermi (ETF2) approximation and 36 different Skyrme forces. Comparison with other theoretical calculations.
doi: 10.1103/PhysRevC.91.044308
2015YD01 Phys.Rev. C 91, 014307 (2015) E.Ydrefors, J.Suhonen, Y.M.Zhao Neutrino-nucleus scattering off 136Xe NUCLEAR REACTIONS 136Xe(ν, X), (ν-bar, X), E=5.0-100.0 MeV; calculated σ(E) for the neutral-, and charge-current neutrino and antineutrino scatterings. 136Xe(ν, ν)136Xe; 136Xe(ν, e-)136Cs; 136Xe(ν-bar, e+)136I; E not given; calculated σ(J) from the dominant multipole channels to the averaged cross section. Quasiparticle random-phase approximation (QRPA), and the pnQRPA to construct the initial and final nuclear states. Relevance to experiments on search for neutrinoless double β decay of 136Xe, and studies of supernova or solar neutrinos.
doi: 10.1103/PhysRevC.91.014307
2015ZH01 Nucl.Phys. A933, 143 (2015) Kinetics analysis and quantitative calculations for the successive radioactive decay process
doi: 10.1016/j.nuclphysa.2014.11.001
2015ZH22 Phys.Rev. C 92, 015207 (2015) Y.X.Zhao, for the Jefferson Lab Hall A Collaboration Double spin asymmetries of inclusive hadron electroproduction from a transversely polarized 3He target
doi: 10.1103/PhysRevC.92.015207
2015ZH39 Chin.Phys.Lett. 32, 113301 (2015) Y.-T.Zhao, J.-P.Yuan, Z.-H.Li, Z.-H.Ji, L.-T.Xiao, S.-T.Jia Production and Detection of Ultracold Ground State 85Rb133Cs Molecules in the Lowest Vibrational Level by Short-Range Photoassociation ATOMIC PHYSICS 85Rb, 133Cs; measured ultracold RbCs molecules, time-of-flight ion signals; deduced photoionization spectrum of ground state, yields.
doi: 10.1088/0256-307X/32/11/113301
2014BA36 Phys.Rev. C 90, 024314 (2014) M.Bao, Z.He, Y.M.Zhao, A.Arima Simple relations for α-decay energies of neighboring nuclei RADIOACTIVITY N=110-180, A>200(α); deduced simple relationships of α-decay energies for four neighboring nuclei based on the longitudinal Garvey-Kelson relation, and its odd-even features; deduced deviations of predicted Q(α) values in comparison with experimental data from AME-2012. 275,276,277,278,279,280,281Ds, 276,277,279,280,281,282,283,284,285Rg, 278,279,280,281,282,283,284,285,286,287Cn, 280,282,283,284,285,286,287,288,289Nh, 283,284,285,286,287,288,289,290,291Fl, 285,286,287,288,289,290,291,292Mc, 287,288,289,290,291,292,293Lv, 290,291,292,293,294Ts, 292,293,294,295Og(α); deduced Q(α) using derived formula and half-lives from Viola-Seaborg-Sobiczewski (VSS) formula. Improved predictions for Q(α) values of nuclei in the superheavy element (SHE) region. Comparison with available experimental data.
doi: 10.1103/PhysRevC.90.024314
2014CH25 Phys.Rev. C 89, 061304 (2014) Strong correlations of the Garvey-Kelson mass relations ATOMIC MASSES N=40-160; analyzed odd-even staggering with respect to experimental data from AME-2012; deduced strong correlations in Garvey-Kelson mass relations originating from statistical odd-even feature of the interaction between the last proton and the last neutron in atomic nuclei.
doi: 10.1103/PhysRevC.89.061304
2014CH53 Phys.Rev. C 90, 064304 (2014) Reconstitution of local mass relations NUCLEAR STRUCTURE A>16; analyzed two-neutron separation energies using AME-2003 and AME-2012 evaluations; deduced new local mass relations and compared with Garvey-Kelson relations.
doi: 10.1103/PhysRevC.90.064304
2014FU11 Phys.Rev. C 90, 054333 (2014) Nucleon-pair approximation of low-lying states for N=Z nuclei NUCLEAR STRUCTURE 20Ne, 24Mg; calculated levels, ground-state bands, J, π, B(E2). Shell model calculations with nucleon pair approximation, schematic and effective interactions and isospin symmetry Comparison with experimental results.
doi: 10.1103/PhysRevC.90.054333
2014FU12 Phys.Rev. C 90, 064320 (2014) Regularities of low-lying states with random interactions in the fermion dynamical symmetry model
doi: 10.1103/PhysRevC.90.064320
2014HE31 Phys.Rev. C 90, 054320 (2014) Z.He, M.Bao, Y.M.Zhao, A.Arima Improved Janecke mass formula ATOMIC MASSES Z>5, N>9; analyzed masses for 2275 nuclei with a new version of the Janecke formula. Comparison with predicted results of other mass models.
doi: 10.1103/PhysRevC.90.054320
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