NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = Y.B.Sun Found 248 matches. Showing 1 to 100. [Next]2024BA01 Nucl.Instrum.Methods Phys.Res. A1058, 168912 (2024) H.Bai, H.Yi, Y.Sun, Z.Cui, Y.Hu, J.Liu, C.Xia, W.Cao, T.Fan, G.Zhang, R.Fan, Y.Li, W.Jiang, Y.Chen, Y.Lv, W.Jia, Z.Zhang, H.Chen, Z.Chen, M.Zhao, C.Feng, S.Liu Measurement of cross section for the 232Th(n, f) reaction using a time projection chamber NUCLEAR REACTIONS 232Th(n, F), E=5 MeV; measured reaction products; deduced σ. Comparison with JENDL-4, ROSFOND-2010, CENDL-3.2, ENDF/B-VIII.0, and BROND-3.1 libraries.
doi: 10.1016/j.nima.2023.168912
2023GA02 At.Data Nucl.Data Tables 150, 101546 (2023) S.Garg, B.Maheshwari, B.Singh, Y.Sun, A.Goel, A.K.Jain Atlas of nuclear isomers-Second edition COMPILATION Z=4-109; compiled, evaluated nuclear structure data, isomeric T1/2, J, π, decay modes.
doi: 10.1016/j.adt.2022.101546
2023KA05 Phys.Rev.Lett. 130, 052501 (2023) K.Kaneko, Y.Sun, N.Shimizu, T.Mizusaki Quasi-SU(3) Coupling Induced Oblate-Prolate Shape Phase Transition in the Casten Triangle NUCLEAR STRUCTURE 122,124,126,128,130,132Te, 124,126,128,130,132,134Xe, 126,128,130,132,134,136Ba; calculated energy levels, J, π, B(E2), quadrupole moments, potential energy surfaces using HFB+GCM with the PMMU Hamiltonian; deduced hidden symmetries from the vast shell-model configurations, microscopical insights into the empirical symmetry triangle.
doi: 10.1103/PhysRevLett.130.052501
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
2023VE01 Eur.Phys.J. A 59, 139 (2023) S.Velardita, H.Alvarez-Pol, T.Aumann, Y.Ayyad, M.Duer, H.-W.Hammer, L.Ji, A.Obertelli, Y.Sun Method to evidence hypernuclear halos from a two-target interaction cross section measurement RADIOACTIVITY 3H(π-) [from 12C(12C, X)3H, E=1.9 GeV/nucleon]; measured decay products; deduced interaction σ of hypernuclei with a target nucleus via a two-target measurement. R3B (GSI/FAIR).
doi: 10.1140/epja/s10050-023-01050-3
2023WA32 Phys.Rev. C 108, 034309 (2023) J.Wang, S.Dutta, L.-J.Wang, Y.Sun Projected shell model description of nuclear level density: Collective, pair-breaking, and multiquasiparticle regimes in even-even nuclei
doi: 10.1103/PhysRevC.108.034309
2023ZH34 Phys.Rev. C 108, 014614 (2023) J.T.Zhang, P.Ma, Y.Huang, X.L.Tu, P.Sarriguren, Z.P.Li, Y.Kuang, W.Horiuchi, T.Inakura, L.Xayavong, Y.Sun, K.Kaneko, X.Q.Liu, K.Yue, C.J.Shao, Q.Zeng, B.Mei, P.Egelhof, Yu.A.Litvinov, M.Wang, Y.H.Zhang, X.H.Zhou, Z.Y.Sun Matter radius of 78Kr from proton elastic scattering at 153 MeV NUCLEAR REACTIONS 1H(78Kr, p), E=152 MeV/nucleon; measured Ep, Ip; deduced σ(θ). 78Kr; deduced point-matter radius, neutron skin thickness. Glauber model analysis. Comparison of the obtained σ to FRESCO calculations with the phenomenological OMP parameters (KD03). Collision in Cooler Storage Ring of the Heavy Ion Research Facility in Lanzhou (HIRFL-CSR) with molecular hydrogen-gas target. MICRON double-sided Si-strip detector (DSSD) used to measure the recoil protons.
doi: 10.1103/PhysRevC.108.014614
2022BE12 Int.J.Mod.Phys. E31, 2250027 (2022) N.Behera, G.H.Bhat, Z.Naik, R.Palit, Y.Sun, J.A.Sheikh Study of band structure in 76Kr using triaxial projected shell model NUCLEAR STRUCTURE 76Kr; calculated energy levels, bands, staggering parameters using the multi-quasiparticle triaxial projected shell model (TPSM).
doi: 10.1142/S0218301322500276
2022BU22 Phys.Rev. C 106, 054308 (2022) M.J.Burns, R.Chapman, K.M.Spohr, J.Ollier, M.Labiche, X.Liang, Y.Sun, Y.-X.Liu, E.Farnea, M.Axiotis, T.Martinez, D.R.Napoli, C.Ur, Th.Kroll Rotational sequences in N = 98 167Tm populated in the 164Dy(7Li, 4nγ)167Tm fusion-evaporation reaction NUCLEAR REACTIONS 164Dy(7Li, 4nγ), E=5 MeV; measured Eγ, Iγ, γγγ-coin. 167Tm; deduced level, J, π, high-spin states, rotational bands structure, Routhians, quasiparticle alignments, B(M1)/B(E2) ratios. Comparison with the results of the projected shell model calculations and other experimental results. GASP multidetector γ-ray array consisting of 40 escape-suppressed HPGe detectors and 80 element inner BGO ball at XTU Tandem accelerator (INFN Legnaro National Laboratory).
doi: 10.1103/PhysRevC.106.054308
2022KI17 Phys.Rev. C 106, 034311 (2022) S.Kisyov, C.Y.Wu, J.Henderson, A.Gade, K.Kaneko, Y.Sun, N.Shimizu, T.Mizusaki, D.Rhodes, S.Biswas, A.Chester, M.Devlin, P.Farris, A.M.Hill, J.Li, E.Rubino, D.Weisshaar Structure of 126, 128Xe studied in Coulomb excitation measurements NUCLEAR REACTIONS 196Pt, 208Pb(126Xe, 126Xe'), (128Xe, 128Xe'), E(126Xe)=3.74 MeV/nucleon, E(128Xe)=3.81 MeV/nucleon; measured reaction products, Eγ, Iγ, (126Xe)γ-coin, (128Xe)γ-coin using JANUS array consisting of a pair of segmented double-sided Si detectors for particles, and SeGA array with sixteen 32-fold segmented HPGe detector for γ radiation at the NSCL-MSU facility. 126,128Xe; deduced levels, J, π, E2 matrix elements, B(E2), static quadrupole moments. GOSIA + GOSIA2 analyses; calculated Potential-energy surfaces (PES) in (Q0, Q2) plane. Comparison with PMMU shell model calculations, and with previous experimental results.
doi: 10.1103/PhysRevC.106.034311
2022LV06 Phys.Rev. C 105, 054308 (2022) C.-J.Lv, Y.Sun, Y.Fujita, H.Fujita, L.-J.Wang, Z.-C.Gao Effect of nuclear deformation on the observation of a low-energy super-Gamow-Teller state NUCLEAR REACTIONS 42Ca(3He, t), E=140 MeV/nucleon; calculated Gamow-Teller strength distribution. Reproduced experimentally observed so-called low-energy super-GT (LeSGT) state population. Projected shell model (PSM) calculations. NUCLEAR STRUCTURE 82Nb; calculated Gamow-Teller strength in charge exchange reactions populating excited states in 82Nb from ground state of 82Zr. Results point on absence of low-energy super-GT (LeSGT) state in 82Nb.
doi: 10.1103/PhysRevC.105.054308
2022LV08 Phys.Rev.Lett. 129, 042502 (2022) C.-J.Lv, F.-Q.Chen, Y.Sun, M.Guidry ΔI=2 Bifurcation as a Characteristic Feature of Scissors Rotational Bands NUCLEAR STRUCTURE 156Gd; calculated energy levels, B(E2), B(M1), staggering features for the scissors-mode rotational band, moments of inertia. Microscopic many-body. Comparison with available data.
doi: 10.1103/PhysRevLett.129.042502
2022SU08 Phys.Rev. C 105, 034911 (2022) Y.Sun, Z.Zhang, C.M.Ko, W.Zhao Evolution of Λ polarization in the hadronic phase of heavy-ion collisions
doi: 10.1103/PhysRevC.105.034911
2022WA42 Phys.Rev. C 106, 054320 (2022) B.-L.Wang, F.Gao, L.-J.Wang, Y.Sun Effective and efficient algorithm for the Wigner rotation matrix at high angular momenta NUCLEAR STRUCTURE 156Dy; calculated levels, energies of the yrast band, high-spin states. Method for evaluation of the Wigner d function based on the Jacobi polynomials. Comparison to other theoretical methods.
doi: 10.1103/PhysRevC.106.054320
2021AB12 Phys.Rev. C 104, L061901 (2021) M.S.Abdallah, B.E.Aboona, J.Adam, L.Adamczyk, J.R.Adams, J.K.Adkins, G.Agakishiev, I.Aggarwal, M.M.Aggarwal, Z.Ahammed, I.Alekseev, D.M.Anderson, A.Aparin, E.C.Aschenauer, M.U.Ashraf, F.G.Atetalla, A.Attri, G.S.Averichev, V.Bairathi, W.Baker, J.G.Ball Cap, K.Barish, A.Behera, R.Bellwied, P.Bhagat, A.Bhasin, J.Bielcik, J.Bielcikova, I.G.Bordyuzhin, J.D.Brandenburg, A.V.Brandin, I.Bunzarov, J.Butterworth, X.Z.Cai, H.Caines, M.Calderon de la Barca Sanchez, D.Cebra, I.Chakaberia, P.Chaloupka, B.K.Chan, F.-H.Chang, Z.Chang, N.Chankova-Bunzarova, A.Chatterjee, S.Chattopadhyay, D.Chen, J.Chen, J.H.Chen, X.Chen, Z.Chen, J.Cheng, M.Chevalier, S.Choudhury, W.Christie, X.Chu, H.J.Crawford, M.Csanad, M.Daugherity, T.G.Dedovich, I.M.Deppner, A.A.Derevschikov, A.Dhamija, L.Di Carlo, L.Didenko, P.Dixit, X.Dong, J.L.Drachenberg, E.Duckworth, J.C.Dunlop, N.Elsey, J.Engelage, G.Eppley, S.Esumi, O.Evdokimov, A.Ewigleben, O.Eyser, R.Fatemi, F.M.Fawzi, S.Fazio, P.Federic, J.Fedorisin, C.J.Feng, Y.Feng, P.Filip, E.Finch, Y.Fisyak, A.Francisco, C.Fu, L.Fulek, C.A.Gagliardi, T.Galatyuk, F.Geurts, N.Ghimire, A.Gibson, K.Gopal, X.Gou, D.Grosnick, A.Gupta, W.Guryn, A.I.Hamad, A.Hamed, Y.Han, S.Harabasz, M.D.Harasty, J.W.Harris, H.Harrison, S.He, W.He, X.H.He, Y.He, S.Heppelmann, S.Heppelmann, N.Herrmann, E.Hoffman, L.Holub, Y.Hu, H.Huang, H.Z.Huang, S.L.Huang, T.Huang, X.Huang, Y.Huang, T.J.Humanic, G.Igo, D.Isenhower, W.W.Jacobs, C.Jena, A.Jentsch, Y.Ji, J.Jia, K.Jiang, X.Ju, E.G.Judd, S.Kabana, M.L.Kabir, S.Kagamaster, D.Kalinkin, K.Kang, D.Kapukchyan, K.Kauder, H.W.Ke, D.Keane, A.Kechechyan, M.Kelsey, Y.V.Khyzhniak, D.P.Kikola, C.Kim, B.Kimelman, D.Kincses, I.Kisel, A.Kiselev, A.G.Knospe, H.S.Ko, L.Kochenda, L.K.Kosarzewski, L.Kramarik, P.Kravtsov, L.Kumar, S.Kumar, R.Kunnawalkam Elayavalli, J.H.Kwasizur, R.Lacey, S.Lan, J.M.Landgraf, J.Lauret, A.Lebedev, R.Lednicky, J.H.Lee, Y.H.Leung, C.Li, C.Li, W.Li, X.Li, Y.Li, X.Liang, Y.Liang, R.Licenik, T.Lin, Y.Lin, M.A.Lisa, F.Liu, H.Liu, H.Liu, P.Liu, T.Liu, X.Liu, Y.Liu, Z.Liu, T.Ljubicic, W.J.Llope, R.S.Longacre, E.Loyd, N.S.Lukow, X.F.Luo, L.Ma, R.Ma, Y.G.Ma, N.Magdy, D.Mallick, S.Margetis, C.Markert, H.S.Matis, J.A.Mazer, N.G.Minaev, S.Mioduszewski, B.Mohanty, M.M.Mondal, I.Mooney, D.A.Morozov, A.Mukherjee, M.Nagy, J.D.Nam, Md.Nasim, K.Nayak, D.Neff, J.M.Nelson, D.B.Nemes, M.Nie, G.Nigmatkulov, T.Niida, R.Nishitani, L.V.Nogach, T.Nonaka, A.S.Nunes, G.Odyniec, A.Ogawa, S.Oh, V.A.Okorokov, B.S.Page, R.Pak, J.Pan, A.Pandav, A.K.Pandey, Y.Panebratsev, P.Parfenov, B.Pawlik, D.Pawlowska, H.Pei, C.Perkins, L.Pinsky, R.L.Pinter, J.Pluta, B.R.Pokhrel, G.Ponimatkin, J.Porter, M.Posik, V.Prozorova, N.K.Pruthi, M.Przybycien, J.Putschke, H.Qiu, A.Quintero, C.Racz, S.K.Radhakrishnan, N.Raha, R.L.Ray, R.Reed, H.G.Ritter, M.Robotkova, O.V.Rogachevskiy, J.L.Romero, D.Roy, L.Ruan, J.Rusnak, N.R.Sahoo, H.Sako, S.Salur, J.Sandweiss, S.Sato, W.B.Schmidke, N.Schmitz, B.R.Schweid, F.Seck, J.Seger, M.Sergeeva, R.Seto, P.Seyboth, N.Shah, E.Shahaliev, P.V.Shanmuganathan, M.Shao, T.Shao, A.I.Sheikh, D.Shen, S.S.Shi, Y.Shi, Q.Y.Shou, E.P.Sichtermann, R.Sikora, M.Simko, J.Singh, S.Singha, M.J.Skoby, N.Smirnov, Y.Sohngen, W.Solyst, P.Sorensen, H.M.Spinka, B.Srivastava, T.D.S.Stanislaus, M.Stefaniak, D.J.Stewart, M.Strikhanov, B.Stringfellow, A.A.P.Suaide, M.Sumbera, B.Summa, X.M.Sun, X.Sun, Y.Sun, Y.Sun, B.Surrow, D.N.Svirida, Z.W.Sweger, P.Szymanski, A.H.Tang, Z.Tang, A.Taranenko, T.Tarnowsky, J.H.Thomas, A.R.Timmins, D.Tlusty, T.Todoroki, M.Tokarev, C.A.Tomkiel, S.Trentalange, R.E.Tribble, P.Tribedy, S.K.Tripathy, T.Truhlar, B.A.Trzeciak, O.D.Tsai, Z.Tu, T.Ullrich, D.G.Underwood, I.Upsal, G.Van Buren, J.Vanek, A.N.Vasiliev, I.Vassiliev, V.Verkest, F.Videbaek, S.Vokal, S.A.Voloshin, F.Wang, G.Wang, J.S.Wang, P.Wang, Y.Wang, Y.Wang, Z.Wang, J.C.Webb, P.C.Weidenkaff, L.Wen, G.D.Westfall, H.Wieman, S.W.Wissink, J.Wu, Y.Wu, B.Xi, Z.G.Xiao, G.Xie, W.Xie, H.Xu, N.Xu, Q.H.Xu, Y.Xu, Z.Xu, Z.Xu, C.Yang, Q.Yang, S.Yang, Y.Yang, Z.Ye, Z.Ye, L.Yi, K.Yip, Y.Yu, H.Zbroszczyk, W.Zha, C.Zhang, D.Zhang, J.Zhang, S.Zhang, S.Zhang, X.P.Zhang, Y.Zhang, Y.Zhang, Y.Zhang, Z.J.Zhang, Z.Zhang, Z.Zhang, J.Zhao, C.Zhou, X.Zhu, M.Zurek, M.Zyzak Global Λ-hyperon polarization in Au+Au collisions at √ sNN = 3 GeV
doi: 10.1103/PhysRevC.104.L061901
2021JI16 Symmetry 13, 2278 (2021) H.Jian, Y.Gao, F.Dai, J.Liu, X.Xu, C.Yuan, K.Kaneko, Y.Sun, P.Liang, G.Shi, L.Sun, L.Xayavong, C.Lin, J.Lee, Z.Li, Y.Yang, P.Li, R.Fan, S.Zha, H.Zhu, J.Li, Q.Gao, Z.Zhang, R.Chen, J.Wang, D.Wang, H.Wu, K.Wang, Y.Lam, F.Duan, P.Ma, Z.Gao, Q.Hu, Z.Bai, J.Ma, J.Wang, F.Zhong, C.Wu, D.Luo, Y.Jiang, Y.Liu, D.Hou, R.Li, N.Ma, W.Ma, G.Yu, D.Patel, S.Jin, Y.Wang, Y.Yu, Q.Zhou, P.Wang, L.Hu, X.Wang, H.L.Zang, Q.Zhao, L.Yang, P.Wen, F.Yang, H.Jia, G.Zhang, M.Pan, X.Wang, H.Sun, M.Wang, Z.Hu, X.Zhou, Y.Zhang, H.Xu, M.Liu, H.-J.Ong, W.Yang β-Delayed γ Emissions of 26P and Its Mirror Asymmetry RADIOACTIVITY 26P(β+), (EC) [from 9Be(32S, X), E=80.6 MeV/nucleon, followed by separation using RIBBL1 at HRIBF, Lanzhou facility]; measured Eγ, Iγ, βγ-coin, T1/2 of 26P decay. 26Si; deduced levels, J, π, β++ϵ feedings, logft, mirror asymmetry parameter from comparison with the ϵ decay of mirror nucleus 26Na to 26Mg, mirror-energy differences (MEDs), and halo structure in 26P. Comparison with shell-model calculations. NUCLEAR REACTIONS 9Be(32S, X)22Na/23Mg/24Al/25Si/26P/27S, E=80.6 MeV/nucleon; measured reaction products, particle-identification (PID) plot of ΔE vs TOF for the ions separated using RIBBL1 separator at HRIBF, Lanzhou facility.
doi: 10.3390/sym13122278
2021KA15 Phys.Rev. C 103, L021301 (2021) K.Kaneko, N.Shimizu, T.Mizusaki, Y.Sun Quasi-SU(3) coupling of (1h11/2, 2f7/2) across the N=82 shell gap: Enhanced E2 collectivity and shape evolution in Nd isotopes NUCLEAR STRUCTURE 56Ni; calculated levels, J, π using HFB+gcm and exact shell-model, and compared with experimental data. 102,104,106,108,110,112,114,116,118,120,122,124,126,128,130Sn, 108,110,112,114,116,118,120,122,124,126,128,130,132,134Te, 110,112,114,116,118,120,122,124,126,128,130,132,134,136Xe, 118,120,122,124,126,128,130,132,134,136,138Ba, 126,128,130,132,134,136,138,140Ce, 128,130,132,134,136,138,140,142Nd, 130,132,134,136,138,140,142,144Nd; calculated energies of the first 2+ and 4+ levels, B(E2) for the first 2+ states, and compared with experimental data. 128,130,132,134,136,138,140,142Nd; calculated energies of levels in the g.s. yrast band up to 12+, Qs and B(E2) for the first 2+ states in the gdshf model space, potential energy surfaces for 130,138,142Nd. Comparison with experimental data. Projected Hartree-Fock-Bogolyubov plus generator coordinate method using the PMMU model in the model space of 1g9/2, 1g7/2, 2d5/2, 2d3/2, 3s1/2, and 1h11/2 orbitals.
doi: 10.1103/PhysRevC.103.L021301
2021LI02 Nucl.Phys. A1005, 121895 (2021) Local spin polarizations in relativistic heavy-ion collisions
doi: 10.1016/j.nuclphysa.2020.121895
2021LU08 Int.J.Mod.Phys. E30, 2150037 (2021) Y.X.Luo, J.O.Rasmussen, J.H.Hamilton, A.V.Ramayya, E.H.Wang, S.Frauendorf, W.Y.Liang, C.F.Jiao, Q.Wu, H.L.Liu, F.R.Xu, Y.X.Liu, Y.Sun, J.K.Hwang, S.H.Liu, S.J.Zhu, N.T.Brewer, I.Y.Lee, G.M.Ter-Akopian, Yu.Oganessian, A.V.Daniel, R.Donangelo, W.C.Ma First observation of collective rotational bands in neutron-rich 142La and the study of octupole/triaxial deformations in 142, 143La RADIOACTIVITY 252Cf(SF); measured decay products, Eγ, Iγ, γ-g.-coin. 142,143La; deduced γ-ray energies and intensities, J, π, yrast band, octupole deformation parameter. TRS model calculations.
doi: 10.1142/S0218301321500373
2021MI02 Astrophys.J.Suppl.Ser. 252, 2 (2021) G.W.Misch, S.K.Ghorui, P.Banerjee, Y.Sun, M.R.Mumpower Astromers: Nuclear Isomers in Astrophysics RADIOACTIVITY 26Al, 34Cl, 85Kr, 121Sn(IT), 121,123,125,127Sn, 128Sb, 170Ho, 176Lu, 182Hf(IT), 58Mn, 113Cd(β-); calculated thermally mediated transition rates between the ground state and long-lived isomers in nuclei; deduced delimiting a thermalization temperature above which a nucleus may be considered a single species and below which it must be treated as two separate species: a ground-state species and an astrophysical isomer ("astromer") species.
doi: 10.3847/1538-4365/abc41d
2021SU06 Nucl.Phys. A1005, 121913 (2021) Y.Sun, G.Coci, S.K.Das, S.Plumari, M.Ruggieri, V.Greco Impact of Glasma on heavy quark RAA and ν2 in nucleus-nucleus collisions at LHC
doi: 10.1016/j.nuclphysa.2020.121913
2021WA04 Phys.Rev. C 103, 014317 (2021) E.H.Wang, J.M.Eldridge, N.T.Brewer, J.H.Hamilton, J.C.Batchelder, Y.X.Liu, Y.Sun, C.Brown, C.J.Zachary, B.M.Musangu, A.V.Ramayya, K.P.Rykaczewski, C.J.Gross, R.Grzywacz, M.Madurga, D.Miller, D.W.Stracener, C.Jost, E.F.Zganjar, J.A.Winger, M.Karny, S.V.Paulauskas, S.H.Liu, M.Wolinska-Cichocka, S.W.Padgett, A.J.Mendez, K.Miernik, A.Fijalkowska, S.V.Ilyushkin Long-lived isomeric states and quasiparticle band structures in neutron-rich 162, 164Gd nuclei from β decay RADIOACTIVITY 162,164Eu(β-)[from 238U(p, F), E=50 MeV at the at the HRIB facility of ORNL]; measured Eγ, Iγ, γγ- and βγ-coin, half-lives of 162Eu g.s. and isomer and 164Eu g.s. decays, half-lives of isomers in 162,164Gd by γ(t). 162,164Eu; deduced J, π for the ground states, and the isomer in 162Eu. 162,164Gd; deduced levels, J, π, isomers, total conversion coefficients, β feedings and logft for 164Eu to 164Gd decay, configurations, β and γ rotational bands. Comparison with projected shell model calculations, and with systematics of K isomer hindrance factors in neighboring nuclei.
doi: 10.1103/PhysRevC.103.014317
2021WA45 Phys.Rev.Lett. 127, 172702 (2021) L.-J.Wang, L.Tan, Z.Li, G.W.Misch, Y.Sun Urca Cooling in Neutron Star Crusts and Oceans: Effects of Nuclear Excitations RADIOACTIVITY 31Mg, 25Na(EC); analyzed available data; deduced impact of the excited-state structure of atomic nuclei on nuclear processes in stellar environments.
doi: 10.1103/PhysRevLett.127.172702
2021WA51 Phys.Rev. C 104, 064323 (2021) L.-J.Wang, L.Tan, Z.Li, B.Gao, Y.Sun Description of 93Nb stellar electron-capture rates by the projected shell model NUCLEAR STRUCTURE 93Nb, 93Zr; calculated levels, J, π, Nilsson configurations using projected-shell model (PSM) method, and compared with experimental data in ENSDF database and Nuclear Data Sheets. RADIOACTIVITY 93Nb(EC); calculated Gamow Teller (GT) strength distribution B(GT+) and the cumulative sum of the B(GT+) for the transitions from 93Nb to 93Zr as a function of the excitation energy of the daughter nucleus 93Zr, individual GT strength distribution B(GT+) for the transitions from different states of 93Nb parent to states of 93Zr daughter nucleus as a function of its excitation energies, stellar electron-capture rates for 93N to 93Zr as a function of the temperature T=1-15 GK, and at different stellar densities, phase space integral for transitions from the ground state of 93Nb to states of 93Zr at different stellar densities and temperatures, as a function of the excitation energy. Projected shell-model (PSM) calculation for stellar EC rates in medium-heavy odd-mass nuclei. Relevance to electron capture (EC) rates for many astrophysical phenomena such as the core-collapse supernovae, the Urca cooling of neutron star crust, etc.
doi: 10.1103/PhysRevC.104.064323
2021YO08 Phys.Rev. C 104, L021303 (2021) R.Yokoyama, E.Ideguchi, G.S.Simpson, M.Tanaka, Y.Sun, C.-J.Lv, Y.-X.Liu, L.-J.Wang, S.Nishimura, P.Doornenbal, G.Lorusso, P.-A.Soderstrom, T.Sumikama, J.Wu, Z.Y.Xu, N.Aoi, H.Baba, F.L.Bello Garrote, G.Benzoni, F.Browne, R.Daido, Y.Fang, N.Fukuda, A.Gottardo, G.Gey, S.Go, S.Inabe, T.Isobe, D.Kameda, K.Kobayashi, M.Kobayashi, I.Kojouharov, T.Komatsubara, T.Kubo, N.Kurz, I.Kuti, Z.Li, M.Matsushita, S.Michimasa, C.B.Moon, H.Nishibata, I.Nishizuka, A.Odahara, Z.Patel, S.Rice, E.Sahin, H.Sakurai, H.Schaffner, L.Sinclair, H.Suzuki, H.Takeda, J.Taprogge, Zs.Vajta, H.Watanabe, A.Yagi Three-quasiparticle isomers in odd-even 159, 161Pm: Calling for modified spin-orbit interaction for the neutron-rich region RADIOACTIVITY 159,161Pm(IT)[from 9Be(238U, F), E=345 MeV/nucleon, followed by separation of fission fragments using the BigRIPS in-flight separator and implantation of fragments in WAS3ABi setup at RIBF-RIKEN facility]; measured Eγ, Iγ, γγ-coin, half-lives of the isomers by γ(t) using the EURICA array of 12 EUROBALL clusters. 159,161Pm; deduced high-spin levels, J, π, bands, 2-quasiparticle Nilsson configurations for the isomeric states, and 3-quasiparticle configurations from theory, existence of the deformed N=98 subshell gap in odd-mass nuclei. Comparison with projected shell model (PSM) calculations. Discussed modification of strength of spin-orbit interactions in standard Nilsson parameters for neutron-rich rare-earth nuclei around A=165.
doi: 10.1103/PhysRevC.104.L021303
2020FU05 Phys.Rev. C 102, 054311 (2020) C.Y.Fu, Y.H.Zhang, M.Wang, X.H.Zhou, Yu.A.Litvinov, K.Blaum, H.S.Xu, X.Xu, P.Shuai, Y.H.Lam, R.J.Chen, X.L.Yan, X.C.Chen, J.J.He, S.Kubono, M.Z.Sun, X.L.Tu, Y.M.Xing, Q.Zeng, X.Zhou, W.L.Zhan, S.Litvinov, G.Audi, T.Uesaka, T.Yamaguchi, A.Ozawa, B.H.Sun, Y.Sun, F.R.Xu Mass measurements for the Tz= -2 fp-shell nuclei 40Ti, 44Cr, 46Mn, 48Fe, 50Co, and 52Ni ATOMIC MASSES 40Ti, 44Cr, 46Mn, 48Fe, 50Co, 52Ni; measured revolution time spectrum of stored ions by time-of-flight detectors, and mass excesses using isochronous mass spectrometry at CSRe-HIRFL, Lanzhou. Isotopes produced in 9Be(58Ni, X), E=468 MeV/nucleon reaction and separated using RIBLL2. Comparison with AME-2016 evaluation, and with theoretical calculations using four mass-models. A=44, 46, 50, 52; analyzed isospin multiplet mass equation (IMME) and T=2 quintets. 44V; proposed isobaric analog state (IAS). RADIOACTIVITY 44Cr(β+), (β+p); analyzed decay scheme; deduced β feedings, logft values, B(GT) from the branching ratios of β+-delayed protons and Q values.
doi: 10.1103/PhysRevC.102.054311
2020GA29 Eur.Phys.J. Special Topics 229, 2527 (2020) S.Garg, A.K.Jain, Y.Sun, A.Goel Isospin conservation in compound nuclear fusion-fission reactions - empirical evidence NUCLEAR REACTIONS 208Pb(18O, F)Ru/Pd/Mo/Cd/Zr/Sn/Sr/Te/Kr/Xe/Se/Ba, E not given; analyzed available data for A=70-150; deduced relative yields. NUCLEAR STRUCTURE 198Hg, 207,209Bi, 210Po; analyzed available data; deduced the ratio of fission decay width to neutron decay width.
doi: 10.1140/epjst/e2020-000040-8
2020LI23 Phys.Rev.Lett. 125, 062301 (2020) Spin Polarizations in a Covariant Angular-Momentum-Conserved Chiral Transport Model
doi: 10.1103/PhysRevLett.125.062301
2020LI53 J.Phys.(London) G47, 055108 (2020) Y.X.Liu, C.J.Lv, Y.Sun, F.G.Kondev Changes of deformed shell gaps at N ∼ 100 in light rare-earth, neutron-rich nuclei NUCLEAR STRUCTURE 157,158,159,160,161,162Nd, 159,160,161,162,163,164Sm, 161,162,163,164,165,166Gd, 171,173,175,177Yb, 173,175,177,179Hf; calculated energy levels, J, π, ground-state bands, moments of inertia, bandhead energies of isomer state. Comparison with available data.
doi: 10.1088/1361-6471/ab752d
2020TA09 Phys.Lett. B 805, 135432 (2020) L.Tan, Y.-X.Liu, L.-J.Wang, Z.Li, Y.Sun A novel method for stellar electron-capture rates of excited nuclear states RADIOACTIVITY 59Co(EC); calculated stellar electron-capture rates of highly-excited nuclear states using the Projected Shell Model that can incorporate high-order multi-quasiparticle configurations in a large model space.
doi: 10.1016/j.physletb.2020.135432
2020ZA04 Phys.Rev. C 101, 054312 (2020) C.J.Zachary, N.T.Brewer, J.C.Batchelder, E.Wang, J.H.Hamilton, J.M.Eldridge, B.M.Musangu, A.V.Ramayya, C.J.Gross, K.P.Rykaczewski, R.Grzywacz, A.C.Dai, F.R.Xu, Y.X.Liu, Y.Sun, M.Madurga, D.Miller, D.W.Stracener, C.Jost, E.F.Zganjar, J.A.Winger, M.Karny, S.V.Paulauskas, S.H.Liu, M.Wolinska-Cichocka, S.W.Padgett, A.J.Mendez, K.Miernik, A.Fijalkowska, S.V.Ilyushkin Identification of new transitions and levels in 163Gd from β-decay studies RADIOACTIVITY 163Eu(β-)[from 238U(p, F), E=50 MeV, pure 163Eu beam using high-resolution isobar separator at HRIBF-ORNL]; measured Eγ, Iγ, Eβ-, Iβ-, γγ-, βγγ- and (x ray)γ-coin using the CARDS HPGe clover array for γ detection and plastic scintillators for β detection. 163Gd; deduced levels, J, π, bands, configurations; calculated configuration-constrained potential-energy surface (PES) for ν1/2[521] configuration. Comparison with projected shell-model calculations.
doi: 10.1103/PhysRevC.101.054312
2019DO01 Phys.Rev. C 99, 014319 (2019) J.M.Dong, J.Z.Gu, Y.H.Zhang, W.Zuo, L.J.Wang, Yu.A.Litvinov, Y.Sun Beyond Wigner's isobaric multiplet mass equation: Effect of charge-symmetry-breaking interaction and Coulomb polarization NUCLEAR STRUCTURE A=13, 15, 17, 19, 21, 23, 25, 27, 29, 31, 33, 35, 37, 39, 41, 43, 45, 47, 49, 51, 53, 55, 57, 59, 61; calculated coefficient of the added cubic term to the isobaric multiplet mass equation (IMME) for T=3/2 isobaric quartets, and density differences between neutron and proton for A=37 and 43 isobaric doublets. A=12, 16, 20, 24, 28, 32, 36; calculated coefficients of the added cubic and quartic terms to the isobaric multiplet mass equation (IMME) for T=2 isobaric quintets. Deduced general deviation from the original IMME, and the magnitude of the deviation exhibiting an oscillation-like behavior with mass number, modulated by the shell effect. Comparison with available experimental values.
doi: 10.1103/PhysRevC.99.014319
2019DO03 Nucl.Phys. A983, 133 (2019) J.M.Dong, X.L.Shang, W.Zuo, Y.F.Niu, Y.Sun An effective Coulomb interaction in nuclear energy density functionals
doi: 10.1016/j.nuclphysa.2019.01.003
2019JI11 Phys.Rev. C 100, 064316 (2019) H.Jin, S.Tazaki, K.Kaneko, H.-K.Wang, Y.Sun High-spin states of the N=82 isotones 136Xe, 137Cs, and 138Ba: Monopole-driven competition of neutron core excitations with two-proton excitations to the h11/2 high-j orbit NUCLEAR STRUCTURE 136Xe, 137Cs, 138Ba; calculated high-spin levels, J, π, configurations, B(E2), effective single-particle energies (ESPEs), occupation numbers using large-scale shell-model calculations with the extended paring-plus-quadrupole interaction with monopole corrections (EPQQM); deduced a monopole-driven competition between different excitation modes in the high-lying, high-spin states in nuclei above 132Sn, suggesting the importance of neutron core excitation for nuclei across the N=82 closed shell. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.064316
2019KA19 Nucl.Phys. A986, 107 (2019) K.Kaneko, Y.Sun, T.Mizusaki, D.G.Jenkins, S.K.Ghorui, S.Tazaki Large mirror asymmetry in Gamow-Teller β-decay in the A=26 isobaric multiplet RADIOACTIVITY 26Na, 27Mg, 28Al(β-), 26,27,28P(β+), (EC); compiled experimental mirror asymmetry δ from the ft data for mirror nuclei of A=17-35; deduced large mirror asymmetry between 26P and 26Na; calculated ft, mirror asymmetry in GT β-decay using large-scale shell model including Isospin-NonConserving (INC) forces with introduced T=1, J NOT= 0 INC forces deduced good agreement to the data, whereas usual J=0 INC force does not work. Calculations compared with available data.
doi: 10.1016/j.nuclphysa.2019.03.002
2019SU01 Phys.Rev. C 99, 011903 (2019) Azimuthal angle dependence of the longitudinal spin polarization in relativistic heavy ion collisions
doi: 10.1103/PhysRevC.99.011903
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
2019SU15 Phys.Rev. C 99, 064607 (2019) Effect of internal magnetic field on collective flow in heavy ion collisions at intermediate energies
doi: 10.1103/PhysRevC.99.064607
2019WA14 Phys.Lett. B 792, 263 (2019) H.Watanabe, H.K.Wang, G.Lorusso, S.Nishimura, Z.Y.Xu, T.Sumikama, P.-A.Soderstrom, P.Doornenbal, F.Browne, G.Gey, H.S.Jung, J.Taprogge, Zs.Vajta, J.Wu, A.Yagi, H.Baba, G.Benzoni, K.Y.Chae, F.C.L.Crespi, N.Fukuda, R.Gernhauser, N.Inabe, T.Isobe, A.Jungclaus, D.Kameda, G.D.Kim, Y.K.Kim, I.Kojouharov, F.G.Kondev, T.Kubo, N.Kurz, Y.K.Kwon, G.J.Lane, Z.Li, C.-B.Moon, A.Montaner-Piza, K.Moschner, F.Naqvi, M.Niikura, H.Nishibata, D.Nishimura, A.Odahara, R.Orlandi, Z.Patel, Zs.Podolyak, H.Sakurai, H.Schaffner, G.S.Simpson, K.Steiger, Y.Sun, H.Suzuki, H.Takeda, A.Wendt, K.Yoshinaga New isomers in 125Pd79 and 127Pd81: Competing proton and neutron excitations in neutron-rich palladium nuclides towards the N=82 shell closure RADIOACTIVITY 125,127Pd(IT) [from Be(238U, X)125Pd/127Pd, E=345 MeV/nucleon;] ; measured decay products, Eγ, Iγ; deduced γ-ray energies, intensities, T1/2. Comparison with shell model calculations.
doi: 10.1016/j.physletb.2019.03.053
2019WA35 J.Phys.(London) G46, 105102 (2019) L.-J.Wang, J.Dong, F.-Q.Chen, Y.Sun Projected shell model analysis of structural evolution and chaoticity in fast-rotating nuclei NUCLEAR STRUCTURE 164Yb; calculated d energies and moment of inertia of the yrast band, B(E2), branching number; deduced rotationally-induced evolution from order to chaos infinite quantum many-body systems-nuclei.
doi: 10.1088/1361-6471/ab33be
2019XU09 Phys.Rev. C 99, 064303 (2019) X.Xu, M.Wang, K.Blaum, J.D.Holt, Yu.A.Litvinov, A.Schwenk, J.Simonis, S.R.Stroberg, Y.H.Zhang, H.S.Xu, P.Shuai, X.L.Tu, X.H.Zhou, F.R.Xu, G.Audi, R.J.Chen, X.C.Chen, C.Y.Fu, Z.Ge, W.J.Huang, S.Litvinov, D.W.Liu, Y.H.Lam, X.W.Ma, R.S.Mao, A.Ozawa, B.H.Sun, Y.Sun, T.Uesaka, G.Q.Xiao, Y.M.Xing, T.Yamaguchi, Y.Yamaguchi, X.L.Yan, Q.Zeng, H.W.Zhao, T.C.Zhao, W.Zhang, W.L.Zhan Masses of neutron-rich 52-54Sc and 54, 56Ti nuclides: The N=32 subshell closure in scandium ATOMIC MASSES 52,53,54Sc, 54,56Ti; measured mass excesses using isochronous mass spectrometry at CRSe-HIRFL, Lanzhou. Isotopes produced in 9Be(86Kr, X), E=460.65 MeV/nucleon reaction and separated using RIBLL2. Comparison with AME-2012 evaluation, and results from six previous experiments, and with valence-space in-medium similarity renormalization group (VS-IMSRG) calculations. Systematics of S(2n) values in N=27-34 K, Ca, Sc, Ti isotopic chains, and those of empirical shell gaps in N=24-34 K, Ca, Sc, Ti isotopic chains and Z=19-25 N=32 isotones.
doi: 10.1103/PhysRevC.99.064303
2019XU13 Phys.Rev. C 100, 051303 (2019) X.Xu, J.H.Liu, C.X.Yuan, Y.M.Xing, M.Wang, Y.H.Zhang, X.H.Zhou, Yu.A.Litvinov, K.Blaum, R.J.Chen, X.C.Chen, C.Y.Fu, B.S.Gao, J.J.He, S.Kubono, Y.H.Lam, H.F.Li, M.L.Liu, X.W.Ma, P.Shuai, M.Si, M.Z.Sun, X.L.Tu, Q.Wang, H.S.Xu, X.L.Yan, J.C.Yang, Y.J.Yuan, Q.Zeng, P.Zhang, X.Zhou, W.L.Zhan, S.Litvinov, G.Audi, S.Naimi, T.Uesaka, Y.Yamaguchi, T.Yamaguchi, A.Ozawa, B.H.Sun, K.Kaneko, Y.Sun, F.R.Xu Masses of ground and isomeric states of 101In and configuration-dependent shell evolution in odd-$A$ indium isotopes ATOMIC MASSES 101In, 101mIn; measured mass excesses using storage-ring based isochronous mass spectrometry technique; deduced energy of the isomeric state. Comparison with systematic values in AME-2016 values. Systematics of 1/2- isomeric states in 101,103,105,107,109,111In, data from the present experiment for 101In and from the ENSDF database for others. NUCLEAR STRUCTURE 101,103,105,107,109,111,113In; calculated energies of the 1/2- isomeric levels, neutron occupation numbers for 1/2- and 9/2+ levels, neutron effective single-particle energies of ν1g7/2 with respect to ν2d5/2 for 9/2+ and 1/2- levels using state-of-the-art shell-model calculations. Comparison with available experimental data. NUCLEAR REACTIONS 9Be(112Sn, X)31P/33S/35Cl/37Ar/39K/58Ni/60Cu/62Zn/64Ga/66Ge/68As/70Se/72Br/74Rb/76Rb/78Sr/80Y/89Tc/91Ru/91mRu/93Rh/95Pd/95mPd/97Ag/99Cd/101In/101mIn/103Sn, E=400.88 MeV/nucleon; measured reaction products selected and analyzed by RIBLL2 separator, and revolution time spectrum at the Cooler Storage Ring (CSR) accelerator complex of HIRFL-Lanzhou facility.
doi: 10.1103/PhysRevC.100.051303
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
2018BA23 Phys.Rev. C 97, 065807 (2018) P.Banerjee, G.W.Misch, S.K.Ghorui, Y.Sun Effective stellar β-decay rates of nuclei with long-lived isomers: 26Al and 34Cl RADIOACTIVITY 26Al, 34Cl(β+), (IT); calculated effective β-decay, and electromagnetic transition rates for ground states, isomeric states, and several low-spin excited states up to about 2.5 MeV at temperatures suitable for stellar environments; deduced time evolution of 26Al abundance. Calculations used NUSHELLX and OXBASH shell model codes with USDB interaction. Comparison with available experimental values from the ENSDF database, and with other theoretical calculations.
doi: 10.1103/PhysRevC.97.065807
2018DO02 Phys.Rev. C 97, 021301 (2018) J.M.Dong, Y.H.Zhang, W.Zuo, J.Z.Gu, L.J.Wang, Y.Sun Generalized isobaric multiplet mass equation and its application to the Nolen-Schiffer anomaly ATOMIC MASSES 20O, 53Ni, 208Pb; calculated first-order symmetry energy coefficient for charge symmetry breaking (CSB) and second-order charge-independent breaking (CIB) components using SLy4, SLy5 and KBD interactions. Derived a generalized isobaric mass multiplet equation (GIMME), and applied to the study of Nolen-Schiffer anomaly (NSA) in the Coulomb displacement energy of mirror nuclei. A=10-60; calculated contributions of the CSB and CIB effects to coefficients of Tz and Tz2 using SLy4 interaction. 15O, 15N; 17F, 17O; 39Ca, 39K; 41Sc, 41Ca; calculated ΔNSA for T=1/2 mirror pairs due to CSB effects using SLy4, SLy5 and KBD interactions. A=18-42; calculated Coulomb displacement energy (CDE) of the T=1 mirror pairs using SLy4 interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.97.021301
2018FU11 Phys.Rev. C 98, 014315 (2018) C.Y.Fu, Y.H.Zhang, X.H.Zhou, M.Wang, Yu.A.Litvinov, K.Blaum, H.S.Xu, X.Xu, P.Shuai, Y.H.Lam, R.J.Chen, X.L.Yan, T.Bao, X.C.Chen, H.Chen, J.J.He, S.Kubono, D.W.Liu, R.S.Mao, X.W.Ma, M.Z.Sun, X.L.Tu, Y.M.Xing, P.Zhang, Q.Zeng, X.Zhou, W.L.Zhan, S.Litvinov, G.Audi, T.Uesaka, Y.Yamaguchi, T.Yamaguchi, A.Ozawa, B.H.Sun, Y.Sun, F.R.Xu Masses of the Tz = -3/2 nuclei 27P and 29S ATOMIC MASSES 27P, 29S; measured revolution time spectrum, and mass excesses using isochronous mass spectrometry (IMS) technique at Cooler Storage Ring (CSR) of HIRFL-Lanzhou facility. 29S, 29P, 29Si, 29Al; analyzed linear and quadratic coefficients of the isobaric multiplet mass equation (IMME). Comparison with AME-2016 values. 27P, 29S; isotopes produced in 9Be(58Ni, X), E=468 MeV/nucleon reaction, and using RIBLL2 fragment separator.
doi: 10.1103/PhysRevC.98.014315
2018HU01 Phys.Rev. A 97, 013424 (2018) Q.-Q.Hu, C.Freier, Y.Sun, B.Leykauf, V.Schkolnik, J.Yang, M.Krutzik, A.Peters Observation of vector and tensor light shifts in 87Rb using near-resonant, stimulated Raman spectroscopy ATOMIC PHYSICS 87Rb; measured relative frequency; deduced the differential vector and tensor light shifts, Raman spectra, implications for higher fidelities for applications of neutral atoms in quantum information and precision measurements.
doi: 10.1103/PhysRevA.97.013424
2018KA24 Phys.Rev. C 97, 054326 (2018) Isoscalar neutron-proton pairing and SU(4)-symmetry breaking in Gamow-Teller transitions NUCLEAR STRUCTURE 42Sc, 46V, 50Mn, 54Co; calculated cumulative sums of Gamow-Teller transition strengths B(GT) of lowest 1+ states, with separate contributions from each interaction, level energies, B(GT) and overlap between wave functions for the first 0+ and 1+ states. Large-scale shell-model calculations with realistic PMMU Hamiltonian; deduced role of isoscalar T=0, Jπ=1+ np-pairing interaction and SU(4)-symmetry breaking in GT transitions. Comparison with experimental values.
doi: 10.1103/PhysRevC.97.054326
2018MI01 Astrophys.J. 852, 43 (2018) Neutrino Spectra from Nuclear Weak Interactions in sd-Shell Nuclei under Astrophysical Conditions NUCLEAR STRUCTURE A=21-35; calculated electron- and positron-capture spectra, isospin-raising reaction neutrino spectra at a temperature and density typical of early core collapse.
doi: 10.3847/1538-4357/aa9c41
2018SU03 Phys.Rev. C 97, 044904 (2018) Elliptic flow from Coulomb interaction and low density elastic scattering
doi: 10.1103/PhysRevC.97.044904
2018SU13 Phys.Rev. C 98, 014911 (2018) Chiral kinetic approach to the chiral magnetic effect in isobaric collisions
doi: 10.1103/PhysRevC.98.014911
2018VA08 Phys.Lett. B 782, 99 (2018) Zs.Vajta, D.Sohler, Y.Shiga, K.Yoneda, K.Sieja, D.Steppenbeck, Zs.Dombradi, N.Aoi, P.Doornenbal, J.Lee, H.Liu, M.Matsushita, S.Takeuchi, H.Wang, H.Baba, P.Bednarczyk, Zs.Fulop, S.Go, T.Hashimoto, E.Ideguchi, K.Ieki, K.Kobayashi, Y.Kondo, R.Minakata, T.Motobayashi, D.Nishimura, H.Otsu, H.Sakurai, Y.Sun, A.Tamaii, R.Tanaka, Z.Tian, T.Yamamoto, X.Yang, Z.Yang, Y.Ye, R.Yokoyama, J.Zenihiro Proton single particle energies next to 78Ni: Spectroscopy of 77Cu via single proton knock-out reaction NUCLEAR REACTIONS 9Be(78Zn, p)77Cu, E=240 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, level scheme. Comparison with shell model calculations.
doi: 10.1016/j.physletb.2018.05.023
2018WA09 Phys.Rev. C 97, 044302 (2018) Shell-model method for Gamow-Teller transitions in heavy deformed odd-mass nuclei RADIOACTIVITY 83Zr(β-), (β+); calculated Gamow-Teller (GT) transition rates from the first 1/2- state to all the 1/2- and 3/2- states of 83Nb and 83Y. 153Nd(β-); calculated Gamow-Teller (GT) transition rates from 3/2- states and 5/2+ isomeric state of 153Nd to excited states of 153Pm. 153Pm; calculated levels, J, π, logft, configurations. Projected shell model (PSM) for calculating GT strength, with Pfaffian formula for multi-quasiparticle configurations. Comparison with experimental results. NUCLEAR STRUCTURE 153Nd, 153Pm; calculated levels, J, π, yrast band, transition energies based on 5/2+ isomer in 153Nd, configurations. Projected shell model (PSM). Comparison with experimental data.
doi: 10.1103/PhysRevC.97.044302
2018XI04 Phys.Lett. B 781, 358 (2018) Y.M.Xing, K.A.Li, Y.H.Zhang, X.H.Zhou, M.Wang, Yu.A.Litvinov, K.Blaum, S.Wanajo, S.Kubono, G.Martinez-Pinedo, A.Sieverding, R.J.Chen, P.Shuai, C.Y.Fu, X.L.Yan, W.J.Huang, X.Xu, X.D.Tang, H.S.Xu, T.Bao, X.C.Chen, B.S.Gao, J.J.He, Y.H.Lam, H.F.Li, J.H.Liu, X.W.Ma, R.S.Mao, M.Si, M.Z.Sun, X.L.Tu, Q.Wang, J.C.Yang, Y.J.Yuan, Q.Zeng, P.Zhang, X.Zhou, W.L.Zhan, S.Litvinov, G.Audi, T.Uesaka, Y.Yamaguchi, T.Yamaguchi, A.Ozawa, C.Frohlich, T.Rauscher, F.-K.Thielemann, B.H.Sun, Y.Sun, A.C.Dai, F.R.Xu Mass measurements of neutron-deficient Y, Zr, and Nb isotopes and their impact on rp and νp nucleosynthesis processes ATOMIC MASSES 78,79Y, 80,81Zr, 82,83,84Nb, 84Mo; measured revolution time spectrum; deduced mass excess values and proton separation energies. Comparison with available data.
doi: 10.1016/j.physletb.2018.04.009
2018YA24 Eur.Phys.J. A 54, 217 (2018) Y.-C.Yang, Y.-X.Liu, Y.Sun, M.Guidry Superdeformed band in the N = Z + 4 nucleus 40Ar : A projected shell model analysis NUCLEAR STRUCTURE 36,40Ar; calculated rotational band, yrast band levels vs J; compared with published data; deduced kinematical and dynamical moments of inertia vs rotational frequency, g-factor, B(E2) vs spin, neutron and proton pairing gaps using Projected Shell Model (PSM). Compared to data.
doi: 10.1140/epja/i2018-12651-x
2018ZH29 Phys.Rev. C 98, 014319 (2018) Y.H.Zhang, P.Zhang, X.H.Zhou, M.Wang, Yu.A.Litvinov, H.S.Xu, X.Xu, P.Shuai, Y.H.Lam, R.J.Chen, X.L.Yan, T.Bao, X.C.Chen, H.Chen, C.Y.Fu, J.J.He, S.Kubono, D.W.Liu, R.S.Mao, X.W.Ma, M.Z.Sun, X.L.Tu, Y.M.Xing, Q.Zeng, X.Zhou, W.L.Zhan, S.Litvinov, K.Blaum, G.Audi, T.Uesaka, Y.Yamaguchi, T.Yamaguchi, A.Ozawa, B.H.Sun, Y.Sun, F.R.Xu Isochronous mass measurements of Tz = -1 fp-shell nuclei from projectile fragmentation of 58Ni ATOMIC MASSES 43Ti, 44,44m,45V, 46,47Cr, 48,49Mn, 50,51Fe, 52,52mCo, 54Ni, 56Cu; measured time revolution spectra, and mass excesses using isochronous mass spectrometry (IMS) technique using Cooler Storage Ring (CSRm) at HIRFL-Lanzhou. Comparison with AME-2012 evaluation, and with predictions of several mass models. 52,52mCo, 44,44mV; deduced precise energies of the isomeric states from direct mass measurements, and compared with previously known values. 52,52mCo, 52Mn; deduced revised level energies in 52Co from new mass measurements for 52,52mCo and known level energies in 52Mn mirror nucleus. 56Co, 56Cu; deduced revised 56Cu level energies from new mass measurement for 56Cu and using known level energies of 56Co mirror nucleus. 52Co, 52Fe, 52Mn, 52Cr; analyzed quadratic and cubic fit coefficients of the isobaric multiplet mass equation (IMME). Discussed impact of new mass measurements on different aspects in nuclear structure. Isotopes produced in 9Be(58Ni, X), E=467.91 MeV/nucleon reaction, and fragments separated using RIBLL2 separator at Lanzhou.
doi: 10.1103/PhysRevC.98.014319
2018ZH50 Eur.Phys.J. A 54, 175 (2018) Light nuclei production in Pb+Pb collisions at √ sNN = 2.76 TeV
doi: 10.1140/epja/i2018-12610-7
2017GA06 Eur.Phys.J. A 53, 61 (2017) L.-N.Gao, F.-H.Liu, Y.Sun, Z.Sun, R.A.Lacey Excitation functions of parameters extracted from three-source (net-)proton rapidity distributions in Au-Au and Pb-Pb collisions over an energy range from AGS to RHIC
doi: 10.1140/epja/i2017-12252-3
2017KA01 Nucl.Phys. A957, 144 (2017) Enhancement of high-spin collectivity in N = Z nuclei by the isoscalar neutron-proton pairing NUCLEAR STRUCTURE 76,78Sr, 80,82Zr, 84,86Mo, 88,90,92Ru; calculated deformation, spin, quadrupole moment, yrast bands, B(E2) using state-of-the-art shell model. Compared with data.
doi: 10.1016/j.nuclphysa.2016.08.007
2017KA55 Phys.Scr. 92, 114008 (2017) Shape coexistence and shape transition in self-conjugate nucleus 72Kr and the tensor force NUCLEAR STRUCTURE 72Kr; calculated energy levels, B(E2), quadrupole moments, occupation numbers. Comparison with available data.
doi: 10.1088/1402-4896/aa8fdc
2017SU08 Phys.Rev. C 95, 034909 (2017) Chiral vortical and magnetic effects in the anomalous transport model
doi: 10.1103/PhysRevC.95.034909
2017SU25 Phys.Rev. C 96, 024906 (2017) Λ hyperon polarization in relativistic heavy ion collisions from a chiral kinetic approach
doi: 10.1103/PhysRevC.96.024906
2017TU01 Phys.Rev. C 95, 014610 (2017) X.L.Tu, A.Kelic-Heil, Yu.A.Litvinov, Zs.Podolyak, Y.H.Zhang, W.J.Huang, H.S.Xu, K.Blaum, F.Bosch, R.J.Chen, X.C.Chen, C.Y.Fu, B.S.Gao, Z.Ge, Z.G.Hu, D.W.Liu, S.A.Litvinov, X.W.Ma, R.S.Mao, B.Mei, P.Shuai, B.H.Sun, Y.Sun, Z.Y.Sun, P.M.Walker, M.Wang, N.Winckler, J.W.Xia, G.Q.Xiao, Y.M.Xing, X.Xu, T.Yamaguchi, X.L.Yan, J.C.Yang, Y.J.Yuan, Q.Zeng, W.Zhang, H.W.Zhao, T.C.Zhao, X.H.Zhou Application of isochronous mass spectrometry for the study of angular momentum population in projectile fragmentation reactions NUCLEAR REACTIONS 9Be(78Kr, X)53Fe/53mFe/53Co/53mCo, E=479.4 MeV/nucleon; measured revolution time spectra of the isomeric and ground states of 53Co and 53Fe using isochronous mass spectrometry (IMS) technique at HIRFL-CSR-Lanzhou facility; deduced isomeric ratios for the 19/2 state, and compared with the predictions of theoretical calculations using ABRABLA07 code. 53Fe; calculated production probability of 53Fe versus spin using ABRABLA07 code for the 58Ni, 78Kr, 84Kr, and 112Sn projectiles.
doi: 10.1103/PhysRevC.95.014610
2017WA03 Phys.Rev. C 95, 011304 (2017) H.-K.Wang, K.Kaneko, Y.Sun, Y.-Q.He, S.-F.Li, J.Li Monopole effects, isomeric states, and cross-shell excitations in the A=129 hole nuclei near 132Sn NUCLEAR STRUCTURE 129Sn, 129In, 129Cd; calculated levels, J, π, predicted cross-shell excited states, monopole effect on the ground-state energies, configurations. Large-scale shell-model calculations for A=129 hole nuclei. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.011304
2017WA19 Phys.Rev. C 95, 064311 (2017); Erratum Phys.Rev. C 109, 019902 (2024) E.H.Wang, J.H.Hamilton, A.V.Ramayya, Y.X.Liu, H.J.Li, A.C.Dai, W.Y.Liang, F.R.Xu, J.K.Hwang, S.H.Liu, N.T.Brewer, Y.X.Luo, J.O.Rasmussen, Y.Sun, S.J.Zhu, G.M.Ter-Akopian, Yu.Ts.Oganessian Oblate deformation in neutron-rich 118, 119Ag RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin using Gammasphere array of 101 Ge detectors at LBNL-Berkeley. 118,119Ag; deduced high-spin levels, J, π, multipolarities, bands, configurations. Total Routhian surface and projected shell model calculation. Systematics of 7/2+ bands in 115,117,119Ag. Systematics of energy levels and staggering in negative-parity bands in A=104-118, odd-odd Ag isotopes.
doi: 110.1103/PhysRevC.95.064311
2017WA45 Phys.Rev. C 96, 054313 (2017) H.-K.Wang, S.K.Ghorui, K.Kaneko, Y.Sun, Z.H.Li Large-scale shell-model study for excitations across the neutron N=82 shell gap in 131-133Sb NUCLEAR STRUCTURE 131,132,133Sb; calculated levels, J, π, cross-shell excitations, configurations, effects of monopole corrections, B(M1), B(E2), B(M2), B(E3), B(M4). Large-scale shell-model calculations with extended paring plus quadrupole-quadrupole force, with additions of monopole corrections (EPQQM model). Comparison with experimental data taken from the ENSDF database.
doi: 10.1103/PhysRevC.96.054313
2017WU01 Nucl.Phys. A957, 208 (2017) X.-Y.Wu, S.K.Ghorui, L.-Ju.Wang, K.Kaneko, Y.Sun Systematical study of high-spin rotational bands in neutron-deficient Kr isotopes by the extended projected shell model NUCLEAR STRUCTURE 72,74,76,78,80Kr; calculated levels, J, π, rotational bands, yrast band, high spin, moments of inertia vs spin for positive and negative parity bands, B(E2) using extended projected shell model. Compared with available data.
doi: 10.1016/j.nuclphysa.2016.09.003
2017WU09 Phys.Rev. C 95, 064314 (2017) X.Y.Wu, S.K.Ghorui, L.-J.Wang, Y.Sun, M.Guidry, P.M.Walker Systematic study of multi-quasiparticle K-isomeric bands in tungsten isotopes by the extended projected shell model NUCLEAR STRUCTURE 174,176,178,180,182,184,186W; calculated levels, J, π, K-isomeric bands, bandhead energies, two- and multi-particle Nilsson configurations, moment of inertia plots, B(E2), B(M1), B(M1)/B(E2), g factors. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.064314
2017YI02 Phys.Rev. C 95, 054913 (2017) Elliptic flow of light nuclei
doi: 10.1103/PhysRevC.95.054913
2017ZH12 Phys.Lett. B 767, 20 (2017) P.Zhang, X.Xu, P.Shuai, R.J.Chen, X.L.Yan, Y.H.Zhang, M.Wang, Yu.A.Litvinov, K.Blaum, H.S.Xu, T.Bao, X.C.Chen, H.Chen, C.Y.Fu, J.J.He, S.Kubono, Y.H.Lam, D.W.Liu, R.S.Mao, X.W.Ma, M.Z.Sun, X.L.Tu, Y.M.Xing, J.C.Yang, Y.J.Yuan, Q.Zeng, X.Zhou, X.H.Zhou, W.L.Zhan, S.Litvinov, G.Audi, T.Uesaka, Y.Yamaguchi, T.Yamaguchi, A.Ozawa, B.H.Sun, Y.Sun, F.R.Xu High-precision QEC values of superallowed 0+ → 0+β-emitters 46Cr, 50Fe and 54Ni ATOMIC MASSES 42Ti, 46Cr, 48Mn, 50Fe, 54Ni; measured the revolution time spectrum; deduced precision mass excesses, corrected log ft values. Comparison with AME12 evaluated data.
doi: 10.1016/j.physletb.2017.01.039
2017ZH48 Phys.Rev. C 96, 055801 (2017) X.Zhang, J.Zhao, D.Yuan, C.Fu, J.Bao, L.Chen, J.He, L.Hou, L.Li, Y.Li, Y.Li, G.Liao, Y.Rhee, Y.Sun, S.Xu, G.Zhao, B.Zhu, J.Zhu, Z.Zhang, J.Zhang Deuteron-deuteron fusion in laser-driven counter-streaming collisionless plasmas NUCLEAR REACTIONS 2H(d, n)3He, E(cm)<45 keV; measured E(n), I(n), time-of-flight spectra using scintillation detectors, and head-on-head collision of plasma streams driven by nanosecond pulse lasers at the National Laboratory on High Power Lasers and Physics, Shanghai; deduced neutron yield. Implications for reactions in plasma environments in astrophysical conditions.
doi: 10.1103/PhysRevC.96.055801
2016BH01 Nucl.Phys. A947, 127 (2016) G.H.Bhat, J.A.Sheikh, Y.Sun, R.Palit Unified description of rotational-, γ-, and quasiparticle-band structures in neutron-rich mass ∼ 110 region NUCLEAR STRUCTURE 102,103,104,105,106,107,108Mo, 108,109,110,111,112Ru; calculated yrast, γ-, γγ-bands, quadrupole moment. 103,105,107Mo, 109,111Ru calculated B(E2) for many transitions. 102,105Mo calculated rotational bands, other bands. TPSM (Tri-axial Projected Shell Model) calculations with multi-quasiparticle configurations; compared to published data.
doi: 10.1016/j.nuclphysa.2015.12.006
2016HU16 Int.J.Mod.Phys. E25, 1650064 (2016) Y.Huang, S.J.Zhu, J.H.Hamilton, A.V.Ramayya, E.H.Wang, Y.X.Liu, Y.Sun, J.K.Hwang, Z.G.Xiao, H.J.Li, Y.X.Luo, J.O.Rasmussen, G.M.Ter-Akopian, Yu.Ts.Oganessian Reinvestigation of two-phonon γ-vibrational band in neutron-rich 114Pd RADIOACTIVITY 252Cf(SF); measured decay products, Eγ.Iγ. 114Pd; deduced energy levels, level scheme, J, π, γ-bands. Comparison with theoretical calculations.
doi: 10.1142/S0218301316500646
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
2016SH07 Phys.Rev. C 93, 024320 (2016) Y.Shiga, K.Yoneda, D.Steppenbeck, N.Aoi, P.Doornenbal, J.Lee, H.Liu, M.Matsushita, S.Takeuchi, H.Wang, H.Baba, P.Bednarczyk, Zs.Dombradi, Zs.Fulop, S.Go, T.Hashimoto, M.Honma, E.Ideguchi, K.Ieki, K.Kobayashi, Y.Kondo, R.Minakata, T.Motobayashi, D.Nishimura, T.Otsuka, H.Otsu, H.Sakurai, N.Shimizu, D.Sohler, Y.Sun, A.Tamii, R.Tanaka, Z.Tian, Y.Tsunoda, Zs.Vajta, T.Yamamoto, X.Yang, Z.Yang, Y.Ye, R.Yokoyama, J.Zenihiro Investigating nuclear shell structure in the vicinity of 78Ni: Low-lying excited states in the neutron-rich isotopes 80, 82Zn NUCLEAR REACTIONS 9Be(80Zn, 80Zn'), (81Ga, 80Zn), (80Ga, 78Zn), (83Ge, 82Ge), (83As, 82Ge), E=250 MeV/nucleon, [secondary 80Zn, 80,81Ga, 82,83Ge, 83As and other beams from 9Be(238U, X), E=345 MeV/nucleon primary reaction]; measured yields of reaction products, Eγ, Iγ, Doppler corrected γ rays, γγ-coin, level half-lives by line-shape analysis using BigRIPS separator, ZeroDegree spectrometer for particle identification and detection, and DALI2 array of NaI(Tl) detectors for γ rays at RIBF-RIKEN facility. 76,78,80,82Zn, 82Ge; deduced levels, J, π, B(E2), configurations. Comparison with previous experimental results, and with calculations using Monte Carlo shell-model (MCSM) and shell-model with JUN45 interaction. Systematics of energies of first 2+ and 4+ states and E(4+/2+) ratios in 74,76,78,80,82Zn, 82Ge, 84Se, 86Kr.
doi: 10.1103/PhysRevC.93.024320
2016SU24 Phys.Rev. C 94, 045204 (2016) Anomalous transport model study of chiral magnetic effects in heavy ion collisions
doi: 10.1103/PhysRevC.94.045204
2016TU01 Nucl.Phys. A945, 89 (2016) X.L.Tu, Yu.A.Litvinov, K.Blaum, B.Mei, B.H.Sun, Y.Sun, M.Wang, H.S.Xu, Y.H.Zhang Indirect mass determination for the neutron-deficient nuclides 44V, 48Mn, 52Co and 56Cu RADIOACTIVITY 44V, 48Mn, 52Co, 56Cu(β+), (EC), (β+p); calculated β-delayed proton spectroscopic data; deduced mass excess, Q using mirror symmetry. Compared with other calculations of mass excess and data.
doi: 10.1016/j.nuclphysa.2015.09.016
2016WA07 Phys.Rev. C 93, 034322 (2016) L.-J.Wang, Y.Sun, T.Mizusaki, M.Oi, S.K.Ghorui Reduction of collectivity at very high spins in 134Nd: Expanding the projected-shell-model basis up to 10-quasiparticle states NUCLEAR STRUCTURE 134Nd; calculated levels, J, K, π, bands, B(E2), configurations, moment of inertia of yrast band using projected shell model expanded to include up to 10-qp states. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.034322
2016WA28 Phys.Rev. C 94, 051301 (2016) H.Wang, N.Aoi, S.Takeuchi, M.Matsushita, T.Motobayashi, D.Steppenbeck, K.Yoneda, H.Baba, Zs.Dombradi, K.Kobayashi, Y.Kondo, J.Lee, H.Liu, R.Minakata, D.Nishimura, H.Otsu, H.Sakurai, D.Sohler, Y.Sun, Z.Tian, R.Tanaka, Zs.Vajta, Z.Yang, T.Yamamoto, Y.Ye, R.Yokoyama First spectroscopic information from even-even nuclei in the region "southeast" of 132Sn: Neutron-excitation dominance of the 2+1 state in 132Cd NUCLEAR REACTIONS 9Be(134Sn, 132Cd), E not given, [secondary 134Sn beam from W(238U, F), E=345 MeV/nucleon primary reaction and using BigRIPS fragment separator]; measured reaction residues through identification by TOF, Bρ, ΔE, and total kinetic energy (TKE) using the ZeroDegree spectrometer, Eγ, Iγ, (particle)γ-coin using DALI2 array at RIBF-RIKEN facility; 132Cd; deduced levels, J, π, proton-neutron configuration mixing in the first 2+ state. Comparison with mean-field calculations. Systematics of experimental and theoretical first 2+ energies in N=84, Z=48-66, Z=48, N=50-82, and Z=52, N=54-86 nuclei.
doi: 10.1103/PhysRevC.94.051301
2016XU10 Phys.Rev.Lett. 117, 182503 (2016) X.Xu, P.Zhang, P.Shuai, R.J.Chen, X.L.Yan, Y.H.Zhang, M.Wang, Yu.A.Litvinov, H.S.Xu, T.Bao, X.C.Chen, H.Chen, C.Y.Fu, S.Kubono, Y.H.Lam, D.W.Liu, R.S.Mao, X.W.Ma, M.Z.Sun, X.L.Tu, Y.M.Xing, J.C.Yang, Y.J.Yuan, Q.Zeng, X.Zhou, X.H.Zhou, W.L.Zhan, S.Litvinov, K.Blaum, G.Audi, T.Uesaka, Y.Yamaguchi, T.Yamaguchi, A.Ozawa, B.H.Sun, Y.Sun, A.C.Dai, F.R.Xu Identification of the Lowest T=2, Jπ = 0+ Isobaric Analog State in 52Co and Its Impact on the Understanding of β-Decay Properties of 52Ni NUCLEAR REACTIONS Be(58Ni, X)52Co, E=467.91 MeV/nucleon; measured reaction products, TOF; deduced atomic masses, energy of T=2 isobaric analog state, level scheme. Comparison with shell model calculations using GXPF1J interaction.
doi: 10.1103/PhysRevLett.117.182503
2015KA46 Phys.Rev. C 92, 044331 (2015) K.Kaneko, T.Mizusaki, Y.Sun, S.Tazaki Systematical shell-model calculation in the pairing-plus-multipole Hamiltonian with a monopole interaction for the pf5/2g9/2 shell NUCLEAR STRUCTURE 64,65,66,67,68,69,70,71,72,73,74,75,76Ni, 64,65,66,67,68,69,70,71,72,73,74,75,76,77,78Cu, 65,66,67,68,69,70,71,72,73,74,75,76,77,78,79,80Zn, 66,67,68,69,70,71,72,73,74,75,76,77,78,79,80Ga, 69,70,71,72,73,74,75,76,77,78,79,80Ge, 67,68,69,70,71,72,73,74,75,76,77,78As, 73,74,75,76,77,78,79,80Se; calculated binding energies, effective single-particle energies of proton orbits for Cu isotopes, level energies of low-lying, low spin states and B(E2) values in even- and odd-A isotopes, neutron g9/2 and proton p3/2 occupancies for low lying states in Ge isotopes, magnetic moments and electric quadrupole moments of Cu, Ga, and Ge isotopes. 64,66,68,69,70,71,72,73,74,75,76Ge, 68,69,70,71,72,73,74Se; calculated low- and high-spin levels, J, π, B(E2). Shell-model calculations with a pairing-plus-multipole Hamiltonian and monopole-based universal force interaction (PMMU model) for the pf5/2g9/2 shell nuclei. Comparison with experimental and evaluated data.
doi: 10.1103/PhysRevC.92.044331
2015WA07 Phys.Rev. C 91, 021303 (2015) Quenching of the neutron N=82 shell gap near 120Sr with monopole-driving core excitations NUCLEAR STRUCTURE 118Kr, 120Sr, 122Zr, 124Mo, 126Ru, 128Pd, 130Cd; calculated energies of the first 2+ states with and without neutron core excitation (NCE), and with and without the M2 monopole correction, B(E2) for first 2+ states. 120Sr; calculated energies of excited 2+ states. 130In; calculated negative-, and positive-parity members of the πg9/2νh11/2 multiplet. Large-scale shell-model calculations using extended pairing plus quadrupole-quadrupole forces accompanied by the monopole interaction (EPQQM). Discussed shell-quenching mechanism. Comparison with available experimental data.
doi: 10.1103/PhysRevC.91.021303
2015WA13 Acta Phys.Pol. B46, 497 (2015) L.-J.Wang, F.-Q.Chen, Y.Sun, T.Mizusaki, M.Oi Application of the Pfaffian Algorithm in the Nuclear Structure Study at High Spins NUCLEAR STRUCTURE 166Hf; calculated yrast band at high spin; deduced anomalies. Projected shell model, the Pfaffian algorithm.
doi: 10.5506/APhysPolB.46.497
2015WA28 Phys.Rev. C 92, 034317 (2015); Erratum Phys.Rev. C 109, 029902 (2024) E.H.Wang, A.Lemasson, J.H.Hamilton, A.V.Ramayya, J.K.Hwang, J.M.Eldridge, A.Navin, M.Rejmund, S.Bhattacharyya, S.H.Liu, N.T.Brewer, Y.X.Luo, J.O.Rasmussen, H.L.Liu, H.Zhou, Y.X.Liu, H.J.Li, Y.Sun, F.R.Xu, S.J.Zhu, G.M.Ter-Akopian, Yu.Ts.Oganessian, M.Caamano, E.Clement, O.Delaune, F.Farget, G.de France, B.Jacquot Identification of new transitions and mass assignments of levels in 143-153Pr NUCLEAR REACTIONS 9Be(238U, F), E=6.2 MeV/nucleon; measured Eγ, Iγ, (fission fragment)γ-, γγ-coin using VAMOS++ spectrometer and EXOGAM array at GANIL. 143,144,145,146,147,148,149,150,151,152,153Pr; deduced levels, J, π, bands. Comparison with previous experimental data.
doi: 10.1103/PhysRevC.92.034317
2014BH02 Phys.Rev. C 89, 014328 (2014) G.H.Bhat, W.A.Dar, J.A.Sheikh, Y.Sun Nature of γ deformation in Ge and Se nuclei and the triaxial projected shell model description NUCLEAR STRUCTURE 76Ge; calculated levels, J, π of yrast band, γ band, and 2γ band, level and Eγ versus spin plots for bands, staggering parameter S(I) for γ band, B(E2) values for yrast band. 70,72,74,78,80Ge, 76,78,80,82Se; calculated band energies, staggering parameter, B(E2), Eγ versus spin plots for bands. Multi-quasiparticle triaxial projected shell model (TPSM) calculations. Comparison with spherical shell-model (SSM) calculations, and with experimental data.
doi: 10.1103/PhysRevC.89.014328
2014BI02 Phys.Rev. C 89, 014317 (2014) Projected shell model description for rotational bands in the proton emitter 141Ho NUCLEAR STRUCTURE 141Ho; calculated levels, J, π, rotational band drawings and configurations, B(M1), signature splitting, dynamical moments of inertia, bandhead energies for proton-decaying nucleus. Projected shell model with the deformed Nilsson single-particle states. Discussed role of hexadecapole deformation. Comparisons with experimental data.
doi: 10.1103/PhysRevC.89.014317
2014CU01 Phys.Rev. C 90, 014321 (2014) J.-W.Cui, X.-R.Zhou, F.-Q.Chen, Y.Sun, C.-L.Wu, Z.-C.Gao Description of collective and quasiparticle excitations in deformed actinide nuclei: The first application of the multishell shell model for heavy nuclei NUCLEAR STRUCTURE 230,232Th, 232,234,236U, 240Pu; calculated levels, J, π, ground-, β-, γ-, and K=0 to K=7 bands, 2-quasiparticle configurations, B(E2), staggering parameter. Heavy shell model (HSM), an extension of projected shell model (PSM). Comparison with experimental data.
doi: 10.1103/PhysRevC.90.014321
2014KA03 Phys.Rev. C 89, 011302 (2014) K.Kaneko, T.Mizusaki, Y.Sun, S.Tazaki Toward a unified realistic shell-model Hamiltonian with the monopole-based universal force NUCLEAR STRUCTURE Z=20-28, A=42-64; calculated binding energies and fitted with experimental values for 95 nuclides. 42,44,46,48,50,52,54,56,58Ca, 44,46,48,50,52,54,56,58,60Ti, 48,50,52,54,56,58,60,62Cr, 52,54,56,58,60,62,64Fe, 56,58,60,62,64,66,68,70,72,74Ni, 60,62,64,66,68,70,72,74,76,78,80Zn, 64,66,68,70,72,74,76,78,80,82Ge, 68,70,72,74,76,78,80,82,84Se; calculated energies and B(E2) for first 2+ levels. 55Co, 56Ni, 69,72Ge; calculated levels, J, π. Unified realistic shell-model Hamiltonian employing pairing plus multipole Hamiltonian combined with monopole interaction (PMMU model). Comparison with experimental data.
doi: 10.1103/PhysRevC.89.011302
2014KA08 Phys.Rev. C 89, 031302 (2014) K.Kaneko, Y.Sun, T.Mizusaki, S.Tazaki Isospin nonconserving interaction in the T=1 analogue states of the mass-70 region NUCLEAR STRUCTURE A=66-78; calculated mirror energy differences (MEDs) and triplet energy differences (TEDs) for even-even nuclei in the T=1 analog states; calculated Coulomb energy differences for N=Z nuclei 66As-66Ge, 70Br-70Se, 74Rb-74Kr, and 78Y-78Sr. Large-scale shell-model calculations. Effect of isospin nonconserving (INC) nuclear force for the upper fp-shell region. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.031302
2014LU07 Phys.Rev. C 89, 044326 (2014) Y.X.Luo, J.O.Rasmussen, J.H.Hamilton, A.V.Ramayya, E.Wang, Y.X.Liu, C.F.Jiao, W.Y.Liang, F.R.Xu, Y.Sun, S.Frauendorf, J.K.Hwang, S.H.Liu, S.J.Zhu, N.T.Brewer, I.Y.Lee, G.M.Ter-Akopian, Yu.Oganessian, R.Donangelo, W.C.Ma First observation of a rotational band and the role of the proton intruder orbital π 1/2+[431] in very neutron-rich odd-odd 106Nb RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, 3- and 4-fold γγ-coin, coincidences with γ rays from complementary A=142-144 La isotopes , fission yield ratio using Gammasphere array at LBNL. 104,106Nb; deduced high-spin levels, J, π, rotational bands, alignment and moments of inertia plots, configurations. Comparison with projected shell model calculations. Role of 1/2[431] proton intruder orbital, and shape evolution. NUCLEAR STRUCTURE 104,106Nb; calculated levels, J, π, potential energy surfaces (PES), configurations, alignments, moments of inertia. Projected shell model. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.044326
2014SH14 Phys.Lett. B 735, 327 (2014) P.Shuai, H.S.Xu, X.L.Tu, Y.H.Zhang, B.H.Sun, M.Wang, Yu.A.Litvinov, K.Blaum, X.H.Zhou, J.J.He, Y.Sun, K.Kaneko, Y.J.Yuan, J.W.Xia, J.C.Yang, G.Audi, X.L.Yan, X.C.Chen, G.B.Jia, Z.G.Hu, X.W.Ma, R.S.Mao, B.Mei, Z.Y.Sun, S.T.Wang, G.Q.Xiao, X.Xu, T.Yamaguchi, Y.Yamaguchi, Y.D.Zang, H.W.Zhao, T.C.Zhao, W.Zhang, W.L.Zhan Charge and frequency resolved isochronous mass spectrometry and the mass of 51Co ATOMIC MASSES 51Co, 34Ar; measured revolution frequencies; deduced mass excess values. Comparison with shell model calculations.
doi: 10.1016/j.physletb.2014.06.046
2014SU01 At.Data Nucl.Data Tables 100, 286 (2014) Y.Sun, F.Chen, C.Chen, B.C.Gou Energies, fine structure, and radiative transitions of the high-lying core-excited states 6Se, o(n) and 6pe, o(n) (n=1-5) for the boron isoelectronic sequence ATOMIC PHYSICS Z=6-10; calculated energy levels, fine structure, transition rates, and wavelengths. Rayleigh-Ritz variation method using a multiconfiguration interaction wavefunction. Comparison with available data.
doi: 10.1016/j.adt.2013.06.003
2014TU01 J.Phys.(London) G41, 025104 (2014) X.L.Tu, Y.Sun, Y.H.Zhang, H.S.Xu, K.Kaneko, Y.A.Litvinov, M.Wang A survey of Coulomb displacement energies and questions on the anomalous behavior in the fp-shell NUCLEAR STRUCTURE 69Br, 69Se, 5Li, 5He; calculated Coulomb displacement energy. Shell model, GXPF1A, JUN45 effective interactions, comparison with available data.
doi: 10.1088/0954-3899/41/2/025104
2014WA21 Phys.Rev. C 89, 064311 (2014) Isomerism and persistence of the N=82 shell closure in the neutron-rich 132Sn region NUCLEAR STRUCTURE 124Mo, 126Ru, 126,128Pd, 130Cd; calculated levels, J, π, B(E2) using large-scale shell model calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.064311
2014WA29 Phys.Rev. C 90, 011303 (2014) L.-J.Wang, F.-Q.Chen, T.Mizusaki, M.Oi, Y.Sun Toward extremes of angular momentum: Application of the Pfaffian algorithm in realistic calculations NUCLEAR STRUCTURE 166Hf; calculated back-bending plot, and level-energy versus spin plot for high-spin band structure. 176Hf; calculated levels, J, π for yrast, 2-qp, 4-qp and 6-qp bands with quantum number K=6, 8, 14, 15, 19, 20, 22, B(E2) values using Pfaffian algorithm to calculate matrix elements for Hartree-Fock-Bogoliubov states for high-spin and multi-qp states. Comparison with experimental data.
doi: 10.1103/PhysRevC.90.011303
2013CH02 J.Phys.(London) G40, 015101 (2013) F.-Q.Chen, Y.Sun, P.M.Walker, G.D.Dracoulis, Y.R.Shimizu, J.A.Sheikh Mixing effects on K-forbidden transition rates from the 6+ isomers in the N = 104 isotones RADIOACTIVITY 172Er, 174Yb, 176Hf, 178W(IT); calculated B(E2) values for transitions from 6+ isomers, deformation parameters, transition rates, level energies, J, π, matrix elements. PSM calculations, comparison with experimental data.
doi: 10.1088/0954-3899/40/1/015101
2013CH33 Phys.Rev. C 88, 014315 (2013) Quantum fluctuations in the collective 0+ states of deformed nuclei NUCLEAR STRUCTURE 154,156,158,160,162Gd, 156,158,160,162,164Dy, 158,160,162,164,166Er; calculated energies of 2+, 4+ and 6+ members of ground bands, first excited 0+, probability functions of deformation for ground and first excited 0+ states, E0-matrix elements for 0+ to 0+ and 2+ to 2+ transitions. Extension of the original projected shell model (PSM). Comparison with experimental data.
doi: 10.1103/PhysRevC.88.014315
2013JI04 Phys.Rev. C 87, 044327 (2013) H.Jin, Y.Sun, K.Kaneko, S.Tazaki Shell model description with neutron g9/2 excitation for neutron-rich 57-62Mn isotopes NUCLEAR STRUCTURE 57,58,59,60,61,62Mn; calculated levels, J, π, bands, configurations, B(M1), B(E2), moments of inertia, neutron occupation numbers. Large-scale shell model calculations. Discussed neutron g9/2 excitations. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.044327
2013KA15 Phys.Rev.Lett. 110, 172505 (2013) K.Kaneko, Y.Sun, T.Mizusaki, S.Tazaki Variation in Displacement Energies Due to Isospin-Nonconserving Forces NUCLEAR STRUCTURE A=42-95; calculated Coulomb and triplet displacement energies, one- and two-proton separation energies; deduced importance of isospin-nonconserving forces. Large scale shell model calculation, GXPF1A and JUN45 effective interactions.
doi: 10.1103/PhysRevLett.110.172505
2013LI24 Phys.Rev. C 87, 057303 (2013) H.J.Li, Z.G.Xiao, S.J.Zhu, E.Y.Yeoh, Y.X.Liu, Y.Sun, Z.Zhang, R.S.Wang, H.Yi, W.H.Yan, Q.Xu, X.G.Wu, C.Y.He, Y.Zheng, G.S.Li, C.B.Li, H.W.Li, J.J.Liu, S.P.Hu, J.L.Wang, S.H.Yao Multiphonon γ-vibrational bands in the γ-soft nucleus 138Nd NUCLEAR REACTIONS 124Te(19F, 4np), E=103 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) at CIAE facility. 138Nd; deduced levels, J, π, multipolarity, multiphonon γ-vibrational bands, γ softness; calculated bandhead energies as a function of triaxiality. Comparison with cranked shell-model and, triaxial projected shell-model calculations. Systematics of bandhead energies of one- and two-γ vibrational bands in 104,106Mo, 138Nd, 154Gd, 168Er.
doi: 10.1103/PhysRevC.87.057303
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