NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = Y.M.Zhao Found 138 matches. Showing 1 to 100. [Next]2024YI02 Phys.Rev. C 109, 024322 (2024) Alternating-parity doublets of even-even Ba isotopes
doi: 10.1103/PhysRevC.109.024322
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
2014JI01 Phys.Rev. C 89, 014320 (2014) H.Jiang, Y.Lei, C.Qi, R.Liotta, R.Wyss, Y.M.Zhao Magnetic moments of low-lying states in tin isotopes within the nucleon-pair approximation NUCLEAR STRUCTURE 102,104,106,108,110,112,114,116,118,120,122,124,126,128,130Sn; calculated energies, magnetic moments, and B(E2) of first 2+ states. 101,103,105,107,109,123,125,127,129,131Sn; calculated low-lying yrast levels, J, π, magnetic moment. Spin and orbital angular momentum contributions to magnetic moment. Nucleon-pair approximation (NPA) of shell model using standard multipole-multipole interaction. Comparisons with experimental data.
doi: 10.1103/PhysRevC.89.014320
2014JI16 Phys.Rev. C 90, 064303 (2014) H.Jiang, M.Bao, L.-W.Chen, Y.M.Zhao, A.Arima I4 dependence in nuclear symmetry energy
doi: 10.1103/PhysRevC.90.064303
2014LU03 Phys.Rev. C 89, 017301 (2014) Simple correction of nuclear mass models ATOMIC MASSES A=40-260; analyzed deviations of calculated masses by popular theoretical models such as the Skyrme-Hartree-Fock-Bogoliubov approach, the Duflo-Zuker model, the finite range droplet model, and the Weizsacker-Skyrme model from experimental and evaluated values in AME-2012. Odd-even staggering in deviations.
doi: 10.1103/PhysRevC.89.017301
2014LU15 Phys.Rev. C 90, 064313 (2014) Y.Lu, Y.M.Zhao, N.Yoshida, A.Arima Correlations between low-lying yrast states for sd bosons with random interactions
doi: 10.1103/PhysRevC.90.064313
2014SU20 Phys.Rev. C 90, 054318 (2014) B.H.Sun, Y.Lu, J.P.Peng, C.Y.Liu, Y.M.Zhao New charge radius relations for atomic nuclei NUCLEAR STRUCTURE A=20-225; analyzed rms charge radii for 296 stable isotopes; proposed simple relations for charge radii. Comparisons between predictions and experimental data, and with available theoretical calculations. Shape transition shape coexistence.
doi: 10.1103/PhysRevC.90.054318
2013BA14 Phys.Rev. C 87, 044313 (2013) M.Bao, Z.He, Y.M.Zhao, A.Arima Empirical formulas for nucleon separation energies NUCLEAR STRUCTURE N=20-160, Z=10-110; calculated deviations in S(n) and S(p) values with respect to experimental data in AME-2012. 70,71,72,73,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105Zn, 112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142Mo, 151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186,187,188,189,190,191Ba, 229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269Au; calculated Sn using an empirical formula with symmetry energy corrections. Comparison with previous theoretical calculations, and with mass evaluations in AME-2003 and AME-2012.
doi: 10.1103/PhysRevC.87.044313
2013BA60 Phys.Rev. C 88, 064325 (2013) M.Bao, Z.He, Y.Lu, Y.M.Zhao, A.Arima Generalized Garvey-Kelson mass relations ATOMIC MASSES A>16; analyzed Garvey-Kelson mass relations with deviations from experimental data with a different parity of proton and neutron numbers; deduced eight new generalized Garvey-Kelson mass relations; odd-even staggering.
doi: 10.1103/PhysRevC.88.064325
2013FU02 Phys.Rev. C 87, 044309 (2013) G.J.Fu, J.J.Shen, Y.M.Zhao, A.Arima Regularities of proton-neutron interactions 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, 58,59,60,61,62,63,64,65Cu, 60,61,62,63,64,65,66Zn, 62,63,64,65,66,67Ga, 64,65,66,67,68Ge, 66,67,68,69As, 68,69,70Se, 210,211,212,213,214,215Bi, 211,212,213,214,215,216Po, 212,213,214,215,216,217At, 213,214,215,216,217,218Rn, 214,215,216,217,218,219Fr, 215,216,217,218,219,220Ra, 216,217,218,219,220,221Ac, 217,218,219,220,221,222Th; calculated isoscalar and isovector valence proton-neutron interactions (Vpn) using the shell model, and comparison with empirical extraction from experimental binding energies. Odd-even staggering, Wigner effect. Discusses possible origin of the anomaly of proton-neutron interactions.
doi: 10.1103/PhysRevC.87.044309
2013FU03 Phys.Rev. C 87, 044310 (2013) G.J.Fu, Y.Lei, Y.M.Zhao, S.Pittel, A.Arima Nucleon-pair approximation of the shell model with isospin symmetry
doi: 10.1103/PhysRevC.87.044310
2013FU04 Phys.Rev. C 87, 044312 (2013) G.J.Fu, J.J.Shen, Y.M.Zhao, A.Arima Spin-aligned isoscalar pair correlation in 96Cd, 94Ag, and 92Pd NUCLEAR STRUCTURE 92Pd, 94Ag, 96Cd; calculated wave functions of T=0 states, levels, J, π, isomers. Nucleon-pair approximation (NPA) of the shell model with JUN45 interaction for the p1/2p3/2f5/2g9/2 shell. Discussed level-inversion isomerism in 94Ag and 96Cd.
doi: 10.1103/PhysRevC.87.044312
2013FU12 Phys.Rev. C 88, 037302 (2013) G.J.Fu, Y.M.Zhao, J.L.Ping, A.Arima Excited states of many-body systems in the fermion dynamical symmetry model with random interactions
doi: 10.1103/PhysRevC.88.037302
2013FU14 Phys.Rev. C 88, 054303 (2013) Spin-J nucleon-pair approximation with a J-pairing interaction for a single-j shell
doi: 10.1103/PhysRevC.88.054303
2013HE12 Phys.Rev. C 87, 057304 (2013) Z.He, M.Bao, Y.M.Zhao, A.Arima New features of the Garvey-Kelson mass relations
doi: 10.1103/PhysRevC.87.057304
2013JI03 Phys.Rev. C 87, 034313 (2013) H.Jiang, F.Pan, Y.M.Zhao, A.Arima Number of spin-I states for three identical particles in a single-j shell
doi: 10.1103/PhysRevC.87.034313
2013JI16 Phys.Rev. C 88, 044332 (2013) H.Jiang, C.Qi, Y.Lei, R.Liotta, R.Wyss, Y.M.Zhao Nucleon pair approximation description of the low-lying structure of 108, 109Te and 109I NUCLEAR STRUCTURE 104,106,108,109Te, 109I; calculated low-lying levels, J, π, ground-state bands of even-even nuclei, ground- and excited bands of odd-A nuclei, B(E2), B(M1), magnetic dipole moments, nucleon-pair wave functions using framework of nucleon pair approximation (NAP) of the nuclear shell model. Weak coupling and residual quadrupole-quadrupole interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.88.044332
2013LE11 Phys.Rev. C 87, 039801 (2013) Comment on "Pair-truncated shell-model analysis of nuclei around mass 130" NUCLEAR STRUCTURE A=130; discussed previous literature on the structure of low-lying levels in A AP 130 nuclei.
doi: 10.1103/PhysRevC.87.039801
2013LE13 Phys.Rev. C 87, 044331 (2013) Kπ=8- isomers of the N=74 isotones with the nucleon-pair approximation NUCLEAR STRUCTURE 128Xe, 130Ba, 132Ce; calculated levels, J, π, B(E1), B(E2), B(E3), B(M1), B(M2), T1/2, magnetic moment, configurations of Kπ=8- isomers. Nucleon-pair approximation (NPA) calculations. Octupole vibration or quadrupole-octupole coupling. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.044331
2013PI08 J.Phys.:Conf.Ser. 445, 012031 (2013) S.Pittel, Y.Lei, G.J.Fu, Y.M.Zhao Spherical to deformed shape transitions in the nucleon pair shell model NUCLEAR STRUCTURE 142,144,146,148Ce; calculated levels, J, π, deformation, deformation energy, binding energy using nucleon-pair approximation of the shell model. Compared with available data.
doi: 10.1088/1742-6596/445/1/012031
2012DI14 Phys.Rev. C 86, 034302 (2012) B.Ding, H.X.Wang, H.Jiang, Y.H.Zhang, X.H.Zhou, Y.M.Zhao, S.T.Wang, M.L.Liu, G.S.Li, Y.Zheng, N.T.Zhang, H.B.Zhou, Y.J.Ma, Y.Sasakiz, K.Yamada, H.Ohshima, S.Yokose, M.Ishizuka, T.Komatsubara, K.Furuno High-spin level scheme of doubly odd 128I NUCLEAR REACTIONS 124Sn(7Li, 3n), E=28, 32 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(ADO). 128I; deduced levels, J, π, bands, multipolarity, configurations. Comparison with nucleon pair approximation, and empirical shell-model calculations. Systematics of levels in doubly odd A=116-128 Iodine isotopes, and 11/2- states in A=117-127 Iodine, A=117-127 Te, and A=119-129 Xe isotopes.
doi: 10.1103/PhysRevC.86.034302
2012FU11 Phys.Rev. C 86, 054303 (2012) G.J.Fu, M.Bao, Z.He, H.Jiang, Y.M.Zhao, A.Arima Pairing interactions and one-nucleon separation energies NUCLEAR STRUCTURE Z=4-104, N=4-160; analyzed empirical proton-neutron, proton-proton, and neutron-neutron pairing and nonpairing interactions using binding energies and separation energies from 2011-AME pre-review database. Discussed Odd-even staggering of one-nucleon separation energies.
doi: 10.1103/PhysRevC.86.054303
2012JI05 Phys.Rev. C 85, 024301 (2012) H.Jiang, G.J.Fu, Y.M.Zhao, A.Arima Volume and surface symmetry energy coefficients NUCLEAR STRUCTURE A=2-290; analyzed double differences in experimental symmetry energies, volume and surface symmetry energy coefficients. Evidence of odd-even staggering.
doi: 10.1103/PhysRevC.85.024301
2012JI07 Phys.Rev. C 85, 054303 (2012) H.Jiang, G.J.Fu, B.Sun, M.Liu, N.Wang, M.Wang, Y.G.Ma, C.J.Lin, Y.M.Zhao, Y.H.Zhang, Z.Ren, A.Arima Predictions of unknown masses and their applications ATOMIC MASSES Z=1-184, N=1-184; analyzed masses for 1566 nuclei using extrapolation approach and shell correction term, S(n), S(2n), S(p), and S(2p); one-neutron and one-proton drip nuclei, R-process nucleosynthesis and astrophysical implications. Comparison with AME-2011 interim mass evaluation, and with Duflo-Zuker model. 85Mo, 87,88,89Tc, 123Ag, 140I, 222Po, 226,227,228Rn, 233,234Ra, 235Ac; compared predicted masses with measured values. RADIOACTIVITY 248,249,250,251,252,253,254,255,256,257No, 251,252,253,254,255,256,257,258,259Lr, 253,254,255,256,257,258,259,260,261Rf, 255,256,257,258,259,260,261,262Db, 256,257,258,259,260,261,262,263Sg(α); calculated Q(α), half-life. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.054303
2012JI09 Phys.Rev. C 86, 014327 (2012) H.Jiang, G.J.Fu, M.Bao, Z.He, Y.M.Zhao, A.Arima Nucleon separation energies in the valence correlation scheme ATOMIC MASSES Z=29-104, N=39-154; analyzed S(n), S(p), S(2n), S(2p) using AME-2011; deduced linear relations between separation energies, odd-even staggering. Discussed predictive power of the simple relations.
doi: 10.1103/PhysRevC.86.014327
2012JI13 Phys.Rev. C 86, 054304 (2012) H.Jiang, Y.Lei, G.J.Fu, Y.M.Zhao, A.Arima B(E2;0+1 → 2+1) values of even-even Sn isotopes NUCLEAR STRUCTURE 102,104,106,108,110,112,114,116,118,120,122,124,126,128,130Sn; calculated energies and B(E2) values of first 2+ levels within the framework of the nucleon pair approximation (NPA) of the shell model. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.054304
2012LE21 J.Phys.:Conf.Ser. 381, 012107 (2012) Y.Lei, S.Pittel, N.Sandulescu, A.Poves, B.Thakur, Y.M.Zhao Systematic study of proton-neutron pairing correlations in the nuclear shell model NUCLEAR STRUCTURE 44,46Ti, 48Cr; calculated levels, J, π, rotational ground-state band, mass excess. 48Cr calculated yrast band. Shell model including deformation, spin-orbit effects, isoscalar, isovector pairing. Compared to available data.
doi: 10.1088/1742-6596/381/1/012107
2012LE22 J.Phys.:Conf.Ser. 387, 012018 (2012) Y.Lei, S.Pittel, N.Sandulescu, A.Poves, B.Thakur, Y.M.Zhao Systematic study of isoscalar and isovector pairing in the 2p1f shell NUCLEAR STRUCTURE 44,46Ti, 48Cr; calculated levels, J, π, mass excess, ground band, yrast, yrare bands with isovector, isoscalar and SU(4) pairing. Levels compared with data.
doi: 10.1088/1742-6596/387/1/012018
2012SH19 Phys.Rev. C 85, 064325 (2012) New perturbation method of diagonalizing the nuclear shell model Hamiltonian NUCLEAR STRUCTURE 24Mg, 28Si, 45,46Ti, 48Cr; calculated low-lying levels, J, π, B(E2), magnetic dipole and electric quadrupole moments. New perturbation method for obtaining the lowest eigenvalues of the nuclear-shell-model Hamiltonian.
doi: 10.1103/PhysRevC.85.064325
2011FU09 Phys.Rev. C 84, 034311 (2011) G.J.Fu, Y.Lei, H.Jiang, Y.M.Zhao, B.Sun, A.Arima Description and evaluation of nuclear masses based on residual proton-neutron interactions ATOMIC MASSES A>15; analyzed systematics of residual proton-neutron interactions; evaluated nuclear masses and predicted unknown masses. Comparison of experimental data with AME-2003.
doi: 10.1103/PhysRevC.84.034311
2011FU10 Phys.Rev. C 84, 037305 (2011) G.J.Fu, H.Jiang, Y.M.Zhao, A.Arima Effective valence proton numbers for nuclei with Z ∼ 64 NUCLEAR STRUCTURE 142,144,146,148Ce, 144,146,148,150Nd, 146,148,150,152Sm, 148,150,152,154Gd; analyzed systematics of energies and deformation parameters of first 2+, 4+ and 6+ states, B(E2), g factors of first 2+ states in NpNn scheme; deduced effective valence proton numbers for nuclei relevant for Z=64 subshell closure.
doi: 10.1103/PhysRevC.84.037305
2011JI01 Chin.Phys.Lett. 28, 032101 (2011) Benford's Law in Nuclear Structure Physics
doi: 10.1088/0256-307X/28/3/032101
2011JI02 J.Phys.(London) G38, 045103 (2011) H.Jiang, J.J.Shen, Y.M.Zhao, A.Arima Low-lying states of valence-hole nuclei in the 208Pb region NUCLEAR STRUCTURE 197,198,199,200,201,202Ir, 198,199,200,201,202,203Pt, 199,200,201,202,203,204Au, 200,201,202,203,204,205Hg, 201,202,203,204,205,206Tl; calculated low-lying energy levels, J, π, wavefunctions, quadrupole and magnetic moments. Comparison with experimental data.
doi: 10.1088/0954-3899/38/4/045103
2011JI08 Phys.Rev. C 84, 034302 (2011) H.Jiang, G.J.Fu, Y.M.Zhao, A.Arima Low-lying structure of neutron-rich Zn and Ga isotopes NUCLEAR STRUCTURE 72,74,76,78,80Zn, 73,75,77,79,81Ga; calculated levels, J, π, configurations, magnetic dipole and electric quadrupole moments, B(E2), B(M1) in the framework of SDG-pair approximation of shell model. Monopole and quadrupole pairing plus quadrupole-quadrupole interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.034302
2011LE07 Phys.Rev. C 83, 024302 (2011) Y.Lei, Z.Y.Xu, Y.M.Zhao, S.Pittel, A.Arima Emergence of generalized seniority in low-lying states with random interactions NUCLEAR STRUCTURE 22O, 46Ca; calculated generalized seniority properties of the low-lying spin 0, 2 and 4 states using one and two body random interactions. S-pair correlation structure including two-body random ensemble (TBRE) and random Quasi-particle ensemble (RQE).
doi: 10.1103/PhysRevC.83.024302
2011LE16 Phys.Rev. C 83, 044302 (2011) Y.Lei, Y.M.Zhao, N.Yoshida, A.Arima Correlations of excited states for sd bosons in the presence of random interactions
doi: 10.1103/PhysRevC.83.044302
2011LE26 Phys.Rev. C 84, 044301 (2011) Validity of pair approximations for nuclei in open shells NUCLEAR STRUCTURE 130Te, 131Te, 134Te, 130Sn, 132I; calculated levels, J, π, B(E2). Nucleon pair approximation (NPA), shell-model space configuration (SM), and spin-zero, spin-two (SD) pairs, favored pairs. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.044301
2011LE27 Phys.Rev. C 84, 044318 (2011) Y.Lei, S.Pittel, N.Sandulescu, A.Poves, B.Thakur, Y.M.Zhao Systematic study of proton-neutron pairing correlations in the nuclear shell model NUCLEAR STRUCTURE 42Sc, 44,45,46Ti, 46V, 48Cr; calculated level energies, energy splittings, yrast and yrare bands, E2 transition matrix elements, proton-neutron pairing modes, isoscalar and isovector pairs. Parameterized Hamiltonian, shell-model framework. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.044318
2011SH15 Phys.Rev. C 83, 044322 (2011) J.J.Shen, Y.M.Zhao, A.Arima, N.Yoshinaga New extrapolation method for low-lying states of nuclei in the sd and the pf shells NUCLEAR STRUCTURE 24,26Mg, 28Si, 45,46Ti; calculated levels, J, π, Quadrupole moment, magnetic moment, B(E2) using an extrapolation method for shell-model Hamiltonian.
doi: 10.1103/PhysRevC.83.044322
2010FU03 Phys.Rev. C 82, 014307 (2010) G.J.Fu, H.Jiang, Y.M.Zhao, A.Arima Residual proton-neutron interactions and the NpNn scheme NUCLEAR STRUCTURE Z=28-50, N=50-82; Z=50-82, N=82-126; analyzed correlation between integrated proton-neutron interactions using experimental binding energies and NpNn product of valence nucleons.
doi: 10.1103/PhysRevC.82.014307
2010FU10 Phys.Rev. C 82, 034304 (2010) G.J.Fu, H.Jiang, Y.M.Zhao, S.Pittel, A.Arima Nuclear binding energies and empirical proton-neutron interactions ATOMIC MASSES Z=24-102, N=30-160; calculated binding energies and atomic masses using a local mass formula derived from exponential function to simulate the residual proton-neutron interactions. Comparison with AME-2003 mass evaluation.
doi: 10.1103/PhysRevC.82.034304
2010JI16 Phys.Rev. C 82, 054317 (2010) H.Jiang, G.J.Fu, Y.M.Zhao, A.Arima Nuclear mass relations based on systematics of proton-neutron interactions ATOMIC MASSES A>60; analyzed proton-neutron interaction between the last proton and the last two neutrons, and that between the last two protons and the last neutron; deduced nuclear mass relation between neighboring nuclides. Data from AME-2003 used in the analysis.
doi: 10.1103/PhysRevC.82.054317
2010LE16 Phys.Rev. C 82, 034303 (2010) Y.Lei, Z.Y.Xu, Y.M.Zhao, A.Arima Validity of pair truncations with effective interaction in Ca isotopes NUCLEAR STRUCTURE 43,44,45,46Ca; calculated levels, J, π, B(E2), wave function overlaps using Shell Model with GXPF1A interaction for the pf shell nuclei. Pair approximations.
doi: 10.1103/PhysRevC.82.034303
2010SH13 Phys.Rev. C 82, 014309 (2010) Lowest eigenvalue of the nuclear shell model Hamiltonian NUCLEAR STRUCTURE 24Mg, 28Si; calculated matrix elements of the nuclear shell model Hamiltonian, levels, J, π. Exact diagonalization procedures.
doi: 10.1103/PhysRevC.82.014308
2009LE33 Phys.Rev. C 80, 064316 (2009) Y.Lei, Z.Y.Xu, Y.M.Zhao, A.Arima Validity of pair truncation of the nuclear shell model in 46Ca NUCLEAR STRUCTURE 46Ca; calculated energy levels and E2 transition rates using shell-model. Comparison with nucleon pair approximation (NPA) and broken-pair calculations, and with experimental data.
doi: 10.1103/PhysRevC.80.064316
2009XU05 Phys.Rev. C 79, 054315 (2009) Z.Y.Xu, Y.Lei, Y.M.Zhao, S.W.Xu, Y.X.Xie, A.Arima Low-lying states of heavy nuclei within the nucleon pair approximation NUCLEAR STRUCTURE 202,203,204,205,206Pb, 203,205,207Bi, 204,205,206,207,208,209,210Po, 206,207,208,209,210,211,212Rn, 205,207,209,211At, 208,210,211,212,213,214Ra, 209,211,213Fr; calculated levels, J, π, binding energies, electric quadrupole and magnetic dipole moments, B(E2) using phenomenological shell-model Hamiltonian calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.054315
2009YO02 Phys.Rev. C 79, 017301 (2009) N.Yoshinaga, A.Arima, J.J.Shen, Y.M.Zhao Correlation between eigenvalues and sorted diagonal elements of a large dimensional matrix NUCLEAR STRUCTURE 24Mg, 28Si; calculated eigenvalues and diagonal matrix elements of a large dimensional matrix using nuclear shell model.
doi: 10.1103/PhysRevC.79.017301
2009YO10 Phys.Rev. C 80, 064324 (2009) Proton-neutron interacting boson model under random two-body interactions
doi: 10.1103/PhysRevC.80.064324
2009ZH48 Chin.Phys.C 33, Supplement 1, 137 (2009) Number of spin I states for bosons
doi: 10.1088/1674-1137/33/S1/043
2008SH14 Phys.Rev. C 77, 054312 (2008) J.J.Shen, Y.M.Zhao, A.Arima, N.Yoshinaga Lowest eigenvalues of random Hamiltonians
doi: 10.1103/PhysRevC.77.054312
2008SH22 Phys.Rev. C 78, 044305 (2008) J.J.Shen, A.Arima, Y.M.Zhao, N.Yoshinaga Strong correlation between eigenvalues and diagonal matrix elements NUCLEAR STRUCTURE 24,26Mg, 28Si; calculated levels, J, π using eigenvalues of many-body systems using USD interactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.78.044305
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