NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = Y.S.Chen Found 97 matches. 2023LI33 Chin.Phys.C 47, 074102 (2023) Z.-J.Lian, X.Lu, X.-W.Li, Z.-C.Gao, Y.-S.Chen Weighted variation after projection method for low-lying nonyrast states NUCLEAR STRUCTURE 48Cr, 27Al; calculated level energies; deduced a simple algorithm to further improve the previous variation after projection (VAP) wave functions for low-lying nonyrast states. Comparison with available data.
doi: 10.1088/1674-1137/acccda
2023ZH17 Phys.Rev. C 107, 045809 (2023) S.Zhang, G.Li, W.Jiang, D.X.Wang, J.Ren, M.Huang, E.T.Li, J.Y.Tang, X.C.Ruan, H.W.Wang, Z.H.Li, Y.S.Chen, L.X.Liu, X.X.Li, Q.W.Fan, R.R.Fan, X.R.Hu, J.C.Wang, X.Li, D.D.Niu, N.Song, M.Gu Measurement of the 159Tb (n, γ) cross section at the CSNS Back-n facility NUCLEAR REACTIONS 159Tb(n, γ), E=0.002-1 MeV; measured neutron Time-of-Flight, Eγ, Iγ; deduced σ(E), resonance parameters, Maxwellian-averaged σ (kT=5-100 keV), astrophysical reaction rate. R-matrix analysis (SAMMY code) to obtain resonance parameters and compare to JEFF-3.3 evaluations, recommended data from Mughabghab and ENDF/B-VIII.0. Comparison of cross-section data to other experimental results, TALYS-1.9 calculations, data from KADoNiS-v0.3, KADoNiS-v1.0, JEFF-3.3, ENDF/B-VIII.0. Analyzed impact of the obtained data on the time evolution of nuclear abundances of 159Tb, 160Tb, 160Dy, 161Dy, 162Dy, 163Dy, 164Dy, 163Ho, 165Ho, 164Er, 166Er, 167Er. Four C6D6 detectors. Neutron beam from Back-n Facility of the China spallation neutron source (CSNS).
doi: 10.1103/PhysRevC.107.045809
2021YA18 Phys.Rev. C 104, 014306 (2021) T.Ya, Y.-J.Chen, Y.-S.Chen, Z.-C.Gao, L.Liu Axial shape asymmetry and high-spin states in nuclei with Z=100 suggested by the projected total energy surface approach NUCLEAR STRUCTURE 246,248,250,252,254,256Fm; calculated levels, J, π, yrast bands, moment of inertia of yrast bands as function of rotational frequency, β2 and γ deformation parameters, local triaxial minima, energy surfaces, axial asymmetry shapes; deduced backbending phenomenon at about spin 18+ due to the alignment excitation of two quasi-neutrons of the high-j shell. Projected total-energy surface (PTES), total Routhian surface (TRS), and variation after projection (VAP) calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.104.014306
2019WA07 Phys.Lett. B 790, 498 (2019) X.B.Wang, G.X.Dong, Z.C.Gao, Y.S.Chen, C.W.Shen Tetrahedral symmetry in the ground state of 16O NUCLEAR STRUCTURE 16O; calculated mean-field energies, octupole and quadrupole moments, potential energy surfaces, ground state band using Skyrme functional HF.
doi: 10.1016/j.physletb.2019.02.001
2018WA21 Phys.Rev. C 98, 021301 (2018) J.-Q.Wang, Z.-C.Gao, Y.-J.Ma, Y.S.Chen New algorithm in the variation after projection calculations for non-yrast nuclear states NUCLEAR STRUCTURE 20,22,24,26,28Ne, 24,26,28,30Mg, 28,30,32Si, 32,34S, 36Ar; calculated energies of ten lowest 0+ levels. 24,25,26Mg, 26Al; calculated energies of levels up to 14+. Variation after projection (VAP) approach, and shell model with USDB interaction; deduced differences between the two calculations.
doi: 10.1103/PhysRevC.98.021301
2017YA17 Phys.Rev. C 95, 064307 (2017) T.Ya, Y.He, Z.-C.Gao, J.-Q.Wang, Y.S.Chen Implementation of the variation-after-projection approach in calculations with a time-odd Hartree-Fock mean field NUCLEAR STRUCTURE 24,25,26Mg, 26Al; calculated variation-after-projection (VAP) energies, B(E2), J-scheme shell model dimension; deduced energy differences between the shell model energies and the present VAP energies. 20,22,24,26,28Ne, 24,26,28,30Mg, 28,30,32Si, 32,34S, 36Ar; calculated VAP energies, and compared with previous VAP calculations and shell-model energies for the ground states of even-even nuclei. Time-odd Hartree-Fock (HF) mean field with Slater determinants.
doi: 10.1103/PhysRevC.95.064307
2017YA18 Phys.Rev. C 95, 064316 (2017) T.Ya, Y.-S.Chen, Z.-C.Gao, L.Liu, Y.-J.Chen Beyond-mean-field effects on nuclear triaxiality NUCLEAR STRUCTURE 170,172,174,176,178W; calculated level energies, transition quadrupole moments, and projected total energy surfaces (PTES) in (ϵ2, γ) plane for positive-parity yrast bands up to 20+, level energies of γ bands. Investigated beyond-mean-field effects on nuclear triaxiality by projected total energy surface, based on the triaxial projected shell model and hybridized macroscopic-microscopic method. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.064316
2017YA27 Astrophys.J. 848, 98 (2017) S.Q.Yan, Z.H.Li, Y.B.Wang, K.Nishio, M.Lugaro, A.I.Karakas, H.Makii, P.Mohr, J.Su, Y.J.Li, I.Nishinaka, K.Hirose, Y.L.Han, R.Orlandi, Y.P.Shen, B.Guo, S.Zeng, G.Lian, Y.S.Chen, W.P.Liu The 95Zr(n, γ)96Zr Cross Section from the Surrogate Ratio Method and Its Effect on s-process Nucleosynthesis NUCLEAR REACTIONS 94,90Zr(18O, 16O), E=117 MeV; measured reaction products; deduced σ for surrogate reactions. Comparison with KADONIS and ENDF/B-VII.1 evaluated nuclear library and TALYS nuclear code calculations.
doi: 10.3847/1538-4357/aa8c74
2016CH13 Phys.Rev. C 93, 044310 (2016) Q.M.Chen, X.G.Wu, Y.S.Chen, C.B.Li, Z.C.Gao, G.S.Li, F.Q.Chen, C.Y.He, Y.Zheng, S.P.Hu, J.Zhong, Y.H.Wu, H.W.Li, P.W.Luo Lifetime measurements in 180Pt NUCLEAR REACTIONS 156Gd(28Si, 4n), E=144 MeV; measured Eγ, Iγ, γγ-coin, level half-lives by recoil-distance Doppler shift method using a plunger and differential decay curve analysis at HI-13 tandem accelerator of CIAE-Beijing. 180Pt; deduced levels, J, π, B(E2), transition quadrupole moments for levels in the yrast band. Systematics of B(E2), E(4+)/E(2+) ratios, yrast and γ bands in 176,178,180,182,184,186Pt. Comparison with triaxial projected shell model (TPSM) calculations.
doi: 10.1103/PhysRevC.93.044310
2016YA09 Phys.Rev. C 94, 015804 (2016) S.Q.Yan, Z.H.Li, Y.B.Wang, K.Nishio, H.Makii, J.Su, Y.J.Li, I.Nishinaka, K.Hirose, Y.L.Han, R.Orlandi, Y.P.Shen, B.Guo, S.Zeng, G.Lian, Y.S.Chen, X.X.Bai, L.H.Qiao, W.P.Liu Examination of the surrogate ratio method for the determination of the 93Zr (n, γ)94Zr cross section with 90, 92Zr(18O, 16O) 92, 94Zr reactions NUCLEAR REACTIONS 90,92Zr(18O, 16O), E=117 MeV; measured Eγ, Iγ, (16O)γ-coin at the Tandem accelerator of JAEA facility. 92,94Zr; measured γ-decay probability ratios. 93Zr(n, γ), E>3 MeV; deduced σ(E) by surrogate ratio method, using reference cross sections of the 91Zr(n, γ)92Zr reaction from ENDF/B-VII.1, and the measured γ-decay probability ratios.
doi: 10.1103/PhysRevC.94.015804
2015CH04 Phys.Rev. C 91, 014317 (2015) Y.-J.Chen, Z.-C.Gao, Y.-S.Chen, Y.Tu Octupole bands and simplex inversion in the neutron-rich nucleus 145Ba NUCLEAR STRUCTURE 145Ba; calculated levels, J, π, rotational bands, single-proton and single-neutron levels as a function of quadrupole and octupole deformation, configuration mixing, simplex inversion; evidence for reflection asymmetric shape in the ground state and low-lying states. Reflection asymmetric shell model. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.014317
2015CH59 Int.J.Mod.Phys. E24, 1550081 (2015) Y.-J.Chen, Y.-S.Chen, Z.-C.Gao, Y.Tu The octupole deformation of 143Ba NUCLEAR STRUCTURE 143Ba; calculated energy levels, J. π, rotational bands, B(E1)/B(E2) values. The reflection asymmetric shell model (RASM), comparison with available data.
doi: 10.1142/S0218301315500810
2015GA42 Phys.Rev. C 92, 064310 (2015) Variation after projection with a triaxially deformed nuclear mean field NUCLEAR STRUCTURE 20,22,24,26,28Ne, 24,26,28,30Mg, 28,30,32Si, 32,34S, 36Ar; calculated converged energies and associated shape parameters for even-even sd-shell nuclei with the USDB Hamiltonian. Variation after projection (VAP) calculations on spin, isospin, and mass number of a triaxially deformed Hartree-Fock-Bogoliubov vacuum state.
doi: 10.1103/PhysRevC.92.064310
2015HO05 Phys.Rev. C 91, 055802 (2015) S.Q.Hou, J.J.He, S.Kubono, Y.S.Chen Revised thermonuclear rate of 7Be (n, α)4He relevant to Big-Bang nucleosynthesis NUCLEAR REACTIONS 7Be(n, α)4He, E=38-50 MeV; 4He(α, p)7Li, E(cm)=0.0113-5.754 MeV; analyzed σ(E); deduced thermonuclear reaction rates for 7Be(n, α) reaction for T=0.1-5 GK. Comparison with previous calculations and with TENDL-2014 evaluation. Big-Bang nucleosynthesis (BBN) simulations. Discussed cosmological 7Li abundance problem.
doi: 10.1103/PhysRevC.91.055802
2013GU04 Phys.Rev. C 87, 015803 (2013) B.Guo, J.Su, Z.H.Li, Y.B.Wang, S.Q.Yan, Y.J.Li, N.C.Shu, Y.L.Han, X.X.Bai, Y.S.Chen, W.P.Liu, H.Yamaguchi, D.N.Binh, T.Hashimoto, S.Hayakawa, D.Kahl, S.Kubono, J.J.He, J.Hu, S.W.Xu, N.Iwasa, N.Kume, Z.H.Li Determination of the astrophysical 12N(p, γ)13O reaction rate from the 2H(12N, 13O)n reaction and its astrophysical implications NUCLEAR REACTIONS 2H(12N, 13O)1n, E=59 MeV; measured reaction products, energy loss, time-of-flight, differential σ(θ); deduced ANC, astrophysical S factors. 12N(p, γ)13O, at T9=0.3-3.0; deduced stellar reaction rate. Astrophysical implications discussed.
doi: 10.1103/PhysRevC.87.015803
2013SU07 Phys.Rev. C 87, 024312 (2013) J.Su, W.P.Liu, N.C.Shu, S.Q.Yan, Z.H.Li, B.Guo, W.Z.Huang, S.Zeng, E.T.Li, S.J.Jin, X.Liu, Y.B.Wang, G.Lian, Y.J.Li, Y.S.Chen, X.X.Bai, J.S.Wang, Y.Y.Yang, R.F.Chen, S.W.Xu, J.Hu, S.Z.Chen, S.B.Ma, J.L.Han, P.Ma, Q.Hu, J.B.Ma, X.G.Cao, S.L.Jin, Z.Bai, K.Yang, F.D.Shi, W.Zhang, Z.Chen, L.X.Liu, Q.Y.Lin, X.S.Yan, X.H.Zhang, F.Fu, J.J.He, X.Q.Li, C.He, M.S.Smith Reexamining the β decay of 53, 54Ni, 52, 53Co, 51Fe, and 50Mn RADIOACTIVITY 50Mn, 50Cr, 51Fe, 52,53Co, 53,54Ni(β+), (EC), (β+p)[from (58Ni, X), E=68.6 MeV/nucleon]; measured β-delayed protons, (proton)γ-coin, Eγ, Iγ, T1/2 at HIRFL facility in Lanzhou. Implications for r process. Comparison with previous experimental studies.
doi: 10.1103/PhysRevC.87.024312
2012GU18 Astrophys.J. 756, 193 (2012) B.Guo, Z.H.Li, M.Lugaro, J.Buntain, D.Y.Pang, Y.J.Li, J.Su, S.Q.Yan, X.X.Bai, Y.S.Chen, Q.W.Fan, S.J.Jin, A.I.Karakas, E.T.Li, Z.C.Li, G.Lian, J.C.Liu, X.Liu, J.R.Shi, N.C.Shu, B.X.Wang, Y.B.Wang, S.Zeng, W.P.Liu New Determination of the 13C(α, n)16O Reaction Rate and its Influence on the s-process Nucleosynthesis in AGB Stars NUCLEAR REACTIONS 12,13C(11B, 7Li), E=50 MeV; measured reaction products; deduced σ(θ), S-factors, stellar rates. Comparison with available data.
doi: 10.1088/0004-637X/756/2/193
2012ZH30 Phys.Rev. C 86, 014320 (2012) Y.Zheng, L.H.Zhu, X.G.Wu, Z.C.Gao, C.Y.He, G.S.Li, L.L.Wang, Y.S.Chen, Y.Sun, X.Hao, Y.Liu, X.Q.Li, B.Pan, Y.J.Ma, Z.Y.Li, H.B.Ding Abnormal signature inversion and multiple alignments in doubly odd 126I NUCLEAR REACTIONS 124Sn(7Li, 5n)126I, E=48 MeV; measured Eγ, Iγ, γγ-coin, DCO ratios. 126I; deduced levels, J, π, multipolarity, rotational bands, alignments, configurations, signature inversion, Routhians. Comparison with triaxial projected shell-model (TPSM) and cranked-shell-model (CSM) calculations. Evidence for 4-quasiparticle chiral structures.
doi: 10.1103/PhysRevC.86.014320
2011GA22 Phys.Rev. C 83, 057303 (2011) Z.-C.Gao, M.Horoi, Y.S.Chen, Y.J.Chen, Tuya Can one identify the intrinsic structure of the yrast states in 48Cr after the backbending? NUCLEAR STRUCTURE 48Cr; calculated levels, J, π, B(E2), configurations for yrast states using projected configuration interaction (PCI) method. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.057303
2011LI25 Phys.Rev. C 83, 064310 (2011) S.H.Liu, J.H.Hamilton, A.V.Ramayya, Y.S.Chen, Z.C.Gao, S.J.Zhu, L.Gu, E.Y.Yeoh, N.T.Brewer, J.K.Hwang, Y.X.Luo, J.O.Rasmussen, W.C.Ma, J.C.Batchelder, A.V.Daniel, G.M.Ter-Akopian, Yu.Ts.Oganessian, A.Gelberg Signature inversion in odd-odd 114Rh: First identification of high-spin states in very neutron-rich 114Rh and application of the triaxial projected shell model RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin, fission yields ratios using the Gammasphere array. 114Rh; deduced levels, J, π, rotational bands, signature inversion, configurations. Comparison with Triaxial Projected Shell Model calculations. Systematics of negative-parity yrast bands of odd-odd Rh nuclei with A=104-114.
doi: 10.1103/PhysRevC.83.064310
2011WA22 Chin.Phys.C 35, 753 (2011) H.-K.Wang, Z.-C.Gao, Y.-S.Chen, J.-Y.Guo, Y.-J.Chen, Y.Tu The structure of the spherical tensor forces in the USD and GXPF1A shell model Hamiltonians
doi: 10.1088/1674-1137/35/8/010
2010CH35 Nucl.Phys. A834, 378c (2010) Tetrahedral instability in superheavy nuclei NUCLEAR STRUCTURE 228,230Th, 248,250Cf; calculated octupole bands, levels, J, π. 268Sg; calculated rotational bands, levels, J, π; deduced deformation parameters. Reflection asymmetric shell model. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.01.044
2010HO09 Chin.Phys.Lett. 27, 082601 (2010) S.-Q.Hou, K.-S.Wu, Y.-S.Chen, N.-C.Shu, Z.-H.Li The Main Path to C, N, O Elements in Big Bang Nucleosynthesis NUCLEAR REACTIONS 8Li(d, p), E(cm)=7.8 MeV; 8Li(n, γ), 9Li(α, n), E not given; calculated yields; deduced production of C, N, O elements in standard Big Bang nucleosynthesis. RADIOACTIVITY 12B(β-); calculated yields of 12C.
doi: 10.1088/0256-307X/27/8/082601
2010LI38 Nucl.Phys. A834, 661c (2010) Z.H.Li, J.Su, B.Guo, E.T.Li, Z.C.Li, X.X.Bai, Y.J.Li, J.C.Liu, S.Q.Yan, B.X.Wang, Y.B.Wang, G.Lian, S.Zeng, X.Fang, W.P.Liu, Y.S.Chen, N.C.Shu, Q.W.Fan 2H(6He, 7Li)n, 12C(7Li, 6He)13N reactions and 12C(p, γ)13N astrophysical S(E) factors NUCLEAR REACTIONS 2H(6He, 7Li), E not given; 12C(7Li, 6He), E=44.0 MeV; measured σ(θ); deduced 12C(p, γ) S-factor; calculated S-factor using DWBA and asymptotic normalization coefficient. Comparison with other data.
doi: 10.1016/j.nuclphysa.2010.01.117
2010WA37 J.Phys.(London) G37, 125107 (2010) J.G.Wang, S.J.Zhu, L.Gu, Z.G.Xiao, E.Y.Yeoh, M.Zhang, Y.Liu, H.B.Ding, Q.Xu, L.H.Zhu, X.G.Wu, Y.S.Chen, C.Y.He, G.S.Li, L.L.Wang, Y.Zhang, B.Zhang High-spin states and collective band structures in the odd-odd 140Pm nucleus NUCLEAR REACTIONS 126Te(19F, 5n), E=90 MeV; measured Eγ, Iγ, γ-γ-coin.; 140Pm deduced energies, level scheme, yrast bands, J, π, multipolarities. Comparison with TRS calculations.
doi: 10.1088/0954-3899/37/12/125107
2010YA23 Nucl.Phys. A848, 260 (2010) T.Ya, Y.S.Chen, S.Y.Yu, C.W.Shen, Z.C.Gao, Y.J.Chen, L.Liu Triaxial superdeformed bands in odd-odd 160∼168Lu isotopes NUCLEAR STRUCTURE 160,162,164,166,168Lu; calculated triaxial superdeformed band deformation, configurations, related properties with total routhian surface model. Comparison with odd-even systematics and data.
doi: 10.1016/j.nuclphysa.2010.09.004
2009CH70 Chin.Phys.C 33, Supplement 1, 1 (2009) Triaxial rotation in atomic nuclei NUCLEAR STRUCTURE 118,124Cs, 157Ho; calculated signature inversion, projection of the total angular momentum on the intrinsic principal axis; deduced signature inversion impact on rotation of triaxial nucleus. Comparison with experimental data.
doi: 10.1088/1674-1137/33/S1/001
2009GA29 Phys.Rev. C 80, 034325 (2009) Improved basis selection for the projected configuration interaction method applied to medium-heavy nuclei NUCLEAR STRUCTURE 56Ni, 68,70,76Se, 76Ge; calculated level energies using Projection Configuration Interaction (PCI) and full configuration interaction (CI) approaches. 76Ge, 76Se; calculated low-lying 0+ states.
doi: 10.1103/PhysRevC.80.034325
2009WA29 Chin.Phys.C 33, Supplement 1, 79 (2009) M.Wang, Y.-S.Chen, Z.-H.Li, W.-P.Liu, N.-C.Shu Calculation of astrophysical reaction rate of 82Ge(n, γ)83Ge NUCLEAR REACTIONS 82Ge(n, γ), E<1 MeV; 82Ge(d, p), E(cm)=7.9 MeV; analyzed σ(θ); calculated σ(θ), σ; deduced astrophysical reaction rate. DWBA analysis.
doi: 10.1088/1674-1137/33/S1/026
2008CH15 Phys.Rev. C 77, 061305 (2008) Nonaxial-octupole effect in superheavy nuclei NUCLEAR STRUCTURE 220,222,224,226,228,230Ra, 224,226,228,230,232Th, 230,232,234,236,238U, 236,238,240,242Pu, 246,248Cm, 248,250,252Cf, 250Fm, 252No; calculated band head energies, comparison with experimental data. 246Cm, 248Cf, 250Fm, 252No; calculated levels, J, π, B(E3). Reflection Asymmetric Shell Model.
doi: 10.1103/PhysRevC.77.061305
2008CH35 Int.J.Mod.Phys. E17, Supplement 1, 146 (2008) Triaxial reflection asymmetric shell model NUCLEAR STRUCTURE 248,250,252Cf, 226,228Ra; calculated negative parity bands, level energies, J, π; deduced octupole spectra. Reflection Asymmetric Shell Model calculations.
doi: 10.1142/S0218301308011823
2007NE09 Phys.Rev. C 75, 055809 (2007) C.D.Nesaraja, N.Shu, D.W.Bardayan, J.C.Blackmon, Y.S.Chen, R.L.Kozub, M.S.Smith Nuclear structure properties of astrophysical importance for 19Ne above the proton threshold energy NUCLEAR STRUCTURE 19Ne, 19F; analyzed available structure data; deduced level energies, J, π. Discussed astrophysical implications.
doi: 10.1103/PhysRevC.75.055809
2006GA11 Phys.Lett. B 634, 195 (2006) Signature inversion -- manifestation of drift of the rotational axis in triaxial nuclei NUCLEAR STRUCTURE 118,120,122,124,126,128,130Cs; calculated rotational band energies vs spin. 124Cs; calculated B(M1)/B(E2) vs spin. Reflection asymmetric shell model, comparison with data.
doi: 10.1016/j.physletb.2006.01.033
2006GA36 Phys.Rev. C 74, 054303 (2006) Shell model method for Gamow-Teller transitions in heavy, deformed nuclei NUCLEAR STRUCTURE 156Ho, 164Dy; calculated rotational bands level energies, B(E2), B(GT). Projected shell model framework. RADIOACTIVITY 164Ho(EC), (β-); calculated log ft, Gamow-Teller transition rates. Projected shell model framework.
doi: 10.1103/PhysRevC.74.054303
2006GU09 Phys.Rev. C 73, 048801 (2006) B.Guo, Z.H.Li, X.X.Bai, W.P.Liu, N.C.Shu, Y.S.Chen Determination of the astrophysical 26Si(p, γ)27P reaction rate from the asymptotic normalization coefficients of 27Mg → 26Mg + n NUCLEAR REACTIONS 26Mg(d, p), E=12 MeV; analyzed σ(E, θ); deduced asymptotic normalization coefficients. 26Si(p, γ), E=low; deduced astrophysical reaction rate.
doi: 10.1103/PhysRevC.73.048801
2006LI48 Phys.Rev. C 74, 035801 (2006) Z.H.Li, B.Guo, S.Q.Yan, G.Lian, X.X.Bai, Y.B.Wang, S.Zeng, J.Su, B.X.Wang, W.P.Liu, N.C.Shu, Y.S.Chen, H.W.Chang, L.Y.Jiang 13N(d, n)14O reaction and the astrophysical 13N(p, γ)14O reaction rate NUCLEAR REACTIONS 2H(13N, n), E(cm)=8.9 MeV; measured σ(θ); deduced asymptotic normalization coefficient. 13N(p, γ), E(cm)=0-1.0 MeV; deduced astrophysical S-factors, reaction rate.
doi: 10.1103/PhysRevC.74.035801
2006LI62 Int.J.Mod.Phys. E15, 1899 (2006) W.-P.Liu, Z.-H.Li, X.-X.Bai, Y.-B.Wang, G.Lian, B.Guo, S.Zeng, S.-Q.Yan, B.-X.Wang, J.Su, N.-C.Shu, Y.-S.Chen Indirect measurements of nuclear astrophysics reactions using unstable nuclear beams NUCLEAR REACTIONS 2H(7Be, n), (11C, n), (8Li, p), (13N, n), E(cm) ≈ 6-9 MeV; analyzed σ, asymptotic normalization coefficients. 7Be, 11C, 8Li, 13N(p, γ), E=low; deduced astrophysical S-factors, reaction rates.
doi: 10.1142/S0218301306005514
2005CH34 Eur.Phys.J. A 24, 185 (2005) Y.J.Chen, Y.S.Chen, C.W.Shen, Z.C.Gao, S.J.Zhu, Y.Tu Theoretical simulation for identical bands NUCLEAR STRUCTURE 190,192,194Hg, 192,194,196,198Pb, 198Po, 166,168,170,172,174,176Yb, 166,168,170,172,174,176,178Hf; calculated normal-deformed and superdeformed rotational band energies, spins; deduced identical bands frequency, related features. Reflection asymmetric shell model.
doi: 10.1140/epja/i2005-10007-5
2005CH37 Chin.Phys.Lett. 22, 1362 (2005) Y.-J.Chen, Y.-S.Chen, S.-J.Zhu, Z.-C.Gao, Y.Tu Reflection-Asymmetric Shell Model Description of the Neutron-Rich 142, 145Ba Nuclei NUCLEAR STRUCTURE 142,145Ba; calculated octupole-deformed rotational bands levels, J, π, configurations. Reflection-asymmetric shell model, comparison with data.
doi: 10.1088/0256-307X/22/6/018
2005LI19 Phys.Rev. C 71, 052801 (2005) Z.H.Li, W.P.Liu, X.X.Bai, B.Guo, G.Lian, S.Q.Yan, B.X.Wang, S.Zeng, Y.Lu, J.Su, Y.S.Chen, K.S.Wu, N.C.Shu, T.Kajino The 8Li(d, p)9Li reaction and the astrophysical 8Li(n, γ)9Li reaction rate NUCLEAR REACTIONS 2H(8Li, 9Li), E=39 MeV; measured particle spectra, σ(θ). 8Li(n, γ), E=low; deduced astrophysical reaction rates.
doi: 10.1103/PhysRevC.71.052801
2005SH39 Nucl.Phys. A758, 419c (2005) N.-C.Shu, Y.-S.Chen, K.-S.Wu, X.-X.Bai, Z.-H.Li, W.-P.Liu The 11C(p, γ)12N reaction rate and the conversion of 3He into CNO NUCLEAR REACTIONS 11C(p, γ), E=low; analyzed S-factors, related data; deduced astrophysical reaction rates.
doi: 10.1016/j.nuclphysa.2005.05.077
2005TU01 Chin.Phys.Lett. 22, 568 (2005) Y.Tu, S.-Y.Yu, Y.-S.Chen, C.-W.Shen, Y.-J.Chen Triaxial Superdeformed Band and Its Formation Mechanism in Odd-Odd Nucleus 168Lu NUCLEAR STRUCTURE 168Lu; calculated energy vs deformation; deduced triaxial superdeformed band features.
doi: 10.1088/0256-307X/22/3/014
2005XU04 Phys.Rev. C 71, 054318 (2005) S.-W.Xu, Z.-K.Li, Y.-X.Xie, Q.-Y.Pan, W.-X.Huang, X.-D.Wang, Y.Yu, Y.-B.Xing, N.-C.Shu, Y.-S.Chen, F.-R.Xu, K.Wang β-delayed proton decays near the proton drip line RADIOACTIVITY 81Zr, 85Mo, 89Ru, 92Rh, 93Pd, 121Ce, 125Nd, 128Pm, 129Sm, 135,137Gd, 139Dy, 142Ho, 149Yb(β+p); measured β-delayed Eγ, Iγ, proton spectra, pγ-coin, T1/2. Comparison with model predictions. NUCLEAR REACTIONS 92Mo, 106Cd(32S, 3n), E=151 MeV; 92Mo(36Ar, 3n), E=169 MeV; 96Ru(36Ar, 3n), (36Ar, 3np), E=165, 174 MeV; 106Cd(36Ar, 3n), (36Ar, nα), E=176 MeV; 106Cd(40Ca, 4n), E=202 MeV; 112Sn(40Ca, 3n), E=185 MeV; measured σ.
doi: 10.1103/PhysRevC.71.054318
2005YU04 Chin.Phys.Lett. 22, 1628 (2005) D.-Q.Yuan, Y.-N.Zheng, D.-M.Zhou, Y.Zuo, E.-P.Du, X.Duan, C.-H.Wang, Q.Luo, X.-G.Wu, G.-S.Li, S.-X.Wen, G.-J.Xu, Z.-C.Gao, Y.-S.Chen, S.-Y.Zhu Measurements of g-Factor of Rotational Levels in 83Y NUCLEAR REACTIONS 58Ni(28Si, 3p), E=98 MeV; measured Eγ, Iγ(θ, H, t), γγ-coin. 83Y deduced g-factors for rotational band levels. Transient field technique, comparison with cranking model predictions.
doi: 10.1088/0256-307X/22/7/019
2004CH20 Chin.Phys.Lett. 21, 802 (2004) Y.-J.Chen, Y.-S.Chen, Z.-C.Gao Theoretical Simulation for Identical Bands NUCLEAR STRUCTURE A=142-198; calculated normal-deformed and superdeformed rotational band energies; deduced frequency of occurrence of identical bands.
doi: 10.1088/0256-307X/21/5/011
2004GA23 Chin.Phys.Lett. 21, 806 (2004) Rotational Band Structures of Non-Axial Octupole Deformed Shapes NUCLEAR STRUCTURE 148Sm; analyzed rotational band level energies; deduced possible non-axial deformations.
doi: 10.1088/0256-307X/21/5/012
2003SH25 Chin.Phys.Lett. 20, 1470 (2003) N.-C.Shu, D.W.Bardayan, J.C.Blackmon, Y.-S.Chen, R.L.Kozub, P.D.Parker, M.S.Smith New Astrophysical Reaction Rates for 18F(p, α)15O and 18F(p, γ)19Ne NUCLEAR REACTIONS 18F(p, α), (p, γ), E=low; analyzed data; calculated astrophysical reaction rates.
doi: 10.1088/0256-307X/20/9/317
2003WU01 Chin.Phys.Lett. 20, 49 (2003) K.-S.Wu, Y.-S.Chen, Z.-H.Liu, C.-J.Lin, H.-Q.Zhang Calculation of Cross Section of Radiative Halo-Neutron Capture by 12C at Stellar Energy with the Asymptotic Normalization Coefficient Method NUCLEAR REACTIONS 12C(n, γ), E=0-1 MeV; calculated σ. Asymptotic normalization coefficient method, comparison with data.
doi: 10.1088/0256-307X/20/1/315
2002CH62 Chin.Phys.Lett. 19, 1771 (2002) Pairing Field and Moments of Inertia of Superdeformed Nuclei NUCLEAR STRUCTURE 84Zr, 150Gd, 190Hg; analyzed superdeformed bands dynamic moments of inertia; deduced pairing effects. Harmonic oscillator quadrupole pairing HFB model.
doi: 10.1088/0256-307X/19/12/309
2002GA18 Chin.Phys.Lett. 19, 650 (2002) Band Structures of the Axial and Triaxial Deformed Nuclei in the Reflection Asymmetric Shell Model
doi: 10.1088/0256-307X/19/5/313
2001CH02 Phys.Rev. C63, 014314 (2001) Reflection Asymmetric Shell Model for Octupole-Deformed Nuclei NUCLEAR STRUCTURE 222,224,226,228,230Ra; calculated rotational bands energy vs spin. Reflection-asymmetric shell model, octupole-deformed nuclei. Comparison with data.
doi: 10.1103/PhysRevC.63.014314
2001GA32 Chin.Phys.Lett. 18, 352 (2001) Reflection Asymmetric Shell Model for the Description of Octupole Rotational Bands NUCLEAR STRUCTURE 224Ra; calculated yrast rotational band energy vs spin; deduced octupole deformation features. Reflection asymmetric shell model, comparison with data.
doi: 10.1088/0256-307X/18/3/314
2001GA48 Chin.Phys.Lett. 18, 1186 (2001) Garvey-Kelson Mass Relations and n-p Interaction
doi: 10.1088/0256-307X/18/9/310
2001GA66 Chin.Phys.Lett. 18, 1564 (2001) Reflection Asymmetric Shell Model on the Projected Woods-Saxon + BCS Basis NUCLEAR STRUCTURE 228Th; calculated octupole rotational band energies. Reflection asymmetric shell model, comparison with data.
doi: 10.1088/0256-307X/18/12/307
2001ZH44 Hyperfine Interactions 136/137, 205 (2001) S.Y.Zhu, Q.Luo, Y.G.Wang, Z.G.Fan, Y.J.Xu, R.Wang, J.Z.Zhu, G.S.Li, X.A.Liu, X.G.Wu, S.X.Wen, G.J.Xu, Z.C.Gao, X.Z.Zhang, Y.S.Chen, K.Matsuta, M.Fukuda, M.Mihara, T.Minamisono g-Factor Measurements of Rotational States in 84, 86Zr NUCLEAR REACTIONS 58Ni(28Si, 2p), E=98 MeV; 58Ni(32S, 4p), E=110 MeV; measured Eγ, Iγ(θ, H, t). 84,86Zr deduced g factors for rotational band states. Transient-field technique.
doi: 10.1023/A:1020532332334
2000SH31 Chin.Phys.Lett. 17, 488 (2000) C.-W.Shen, Y.-S.Chen, E.-G.Zhao Prediction of Triaxial Superdeformation in the A ∼ 160, 80 Region NUCLEAR STRUCTURE 155,157,159,161Ho, 157,159,161,163Tm, 159,161,163,165,167,169Lu, 163,165,171Ta, 72,74Ni, 76Zn, 76Ge, 78,80Se, 80Kr, 86Zr, 88,90Mo, 90Ru; calculated total Routhian surfaces; deduced deformation parameters, triaxial superdeformation. Cranked mean-field approach.
2000ZH28 Chin.Phys.Lett. 17, 560 (2000) S.-Y.Zhu, Q.Luo, G.-S.Li, Z.-G.Fan, Y.-J.Xu, Z.-C.Gao, S.-X.Wen, X.-G.Wu, X.-A.Liu, G.-J.Xu, J.-Z.Zhu, Y.-S.Chen, K.Matsuta, M.Fukuda, M.Mihara, T.Minamisono Rotational State g-Factors in 84Zr NUCLEAR REACTIONS 58Ni(28Si, 2p), E=98 MeV; measured Eγ, Iγ(θ, H, t) in polarized Fe. 84Zr deduced rotational band levels g-factors, configurations. Transient field technique.
1999GA02 Phys.Rev. C59, 735 (1999) Enhancement of the n-p Interaction in Odd-Odd Nuclei NUCLEAR STRUCTURE A=10-220; analyzed binding energies; deduced neutron-proton interaction energies.
doi: 10.1103/PhysRevC.59.735
1998LI06 Eur.Phys.J. A 1, 125 (1998) Z.Liu, X.Sun, X.Zhou, X.Lei, Y.Guo, Y.Zhang, X.Chen, H.Jin, Y.Luo, S.X.Wen, C.X.Yang, G.J.Yuan, G.S.Li, X.A.Liu, W.D.Luo, Y.S.Chen High Spin States and Evidence for Octupole Correlations in 117Xe NUCLEAR REACTIONS 92Mo(28Si, n2p), E=100-120 MeV; measured Eγ, Iγ(θ), γγ-coin, γγ(t). 117Xe deduced high-spin levels, J, π, B(λ), configurations, isomeric states T1/2. Cranked shell-model calculations.
doi: 10.1007/s100500050042
1998SH30 Phys.Rev. C58, 2081 (1998) Identical Bands and Incremental Alignments in Normal Deformed Nuclei NUCLEAR STRUCTURE A=147-186; analyzed rotational bands incremental alignment; deduced unquantized alignment in identical bands in normal-deformed nuclei.
doi: 10.1103/PhysRevC.58.2081
1998YA04 Eur.Phys.J. A 1, 237 (1998) C.X.Yang, X.G.Wu, H.Zheng, X.A.Liu, Y.S.Chen, C.W.Shen, Y.J.Ma, J.B.Lu, S.Wen, G.S.Li, S.G.Li, G.J.Yuan, P.K.Weng, Y.Z.Liu Superdeformed Triaxial Band in 167Lu NUCLEAR REACTIONS 152Sm(19F, 4n), E=85, 87 MeV; measured Eγ, Iγ, γγ-coin. 167Lu deduced high-spin levels, J, π, configurations, superdeformed band. TRS calculation.
doi: 10.1007/s100500050054
1997SH14 Phys.Rev. C55, 1762 (1997) Identical Bands and Quantized Alignments in Superdeformed Nuclei NUCLEAR STRUCTURE A ≈ 130; A ≈ 150; A ≈ 190; 146,147,148,149Gd; 195Pb, 197Bi, 194Tl, 194Hg; analyzed superdeformed bands data; deduced incremental alignments quantization dependence on identical bands criterion tolerance.
doi: 10.1103/PhysRevC.55.1762
1997WE04 Int.J.Mod.Phys. E6, 177 (1997) S.Wen, H.Zheng, L.K.Zhang, S.G.Li, P.K.Weng, P.F.Hua, G.J.Yuan, P.S.Yu, F.X.Jing, C.X.Yang, W.D.Luo, Y.S.Chen, X.F.Sun, J.X.Guo, X.G.Lei Quasiparticle Driving Effect on Shape of 87Nb Soft Nucleus NUCLEAR REACTIONS 58Ni(32S, 3p), E=95-105 MeV; 58Ni(35Cl, 2pα), E=124 MeV; γγ-coin, Iγ(θ), DCO ratios. 87Nb deduced high-spin levels, J, π, band structure.
doi: 10.1142/S0218301397000123
1997WU03 Chin.Phys.Lett. 14, 17 (1997) X.-G.Wu, C.-X.Yang, H.Zheng, X.-A.Liu, C.-W.Shen, Y.-S.Chen, Y.-J.Ma, J.-B.Lu, S.-X.Wen, G.-S.Li, S.-G.Li, G.-J.Yuan, P.-K.Weng, Y.-Z.Liu Superdeformed Bands in 167Lu and 171Ta NUCLEAR REACTIONS 152Sm(19F, 4n), E=87 MeV; measured γγ-coin. 167Lu deduced high-spin levels, J, π, superdeformed bands, dynamic moments of inertia. NUCLEAR STRUCTURE 171Ta; analyzed data; deduced superdeformed bands.
1996CH42 Chin.J.Nucl.Phys. 18, No 1, 33 (1996) Deep Cancellation Between Proton Quantal and Liquid Drop Model Effects in the A = 80 Mass Region NUCLEAR STRUCTURE 82Kr, 78,80,82,84,86,88Sr, 80,82,84,86,88,90Zr, 88Mo; analyzed levels; deduced proton quantal, liquid drop model effects deep cancellation role. Total routhian surface calculations.
1996LI53 Chin.Phys.Lett. 13, 805 (1996) Z.Liu, X.-F.Sun, X.-H.Zhou, X.-G.Lei, Y.-X.Guo, H.-J.Jin, Y.-H.Zhang, X.-F.Chen, Y.-X.Luo, S.-X.Wen, C.-X.Yang, G.-J.Yuan, G.-S.Li, X.-A.Liu, Y.-S.Chen Evidence for Octupole Correlations in 117Xe NUCLEAR REACTIONS 92Mo(28Si, n2p), E=115 MeV; measured γγ-coin. 117Xe deduced high-spin levels, J, π, B(λ), γ-multipolarity, band structure, octupole correlations.
doi: 10.1088/0256-307X/13/11/002
1995LI08 Nucl.Phys. A583, 221c (1995) Z.Liu, X.Sun, X.Zhou, X.Lei, Y.Zhang, H.Jin, Q.Pan, Y.Guo, X.Chen, Y.Luo, S.Wen, G.Yuan, C.Yang, W.Luo, Y.S.Chen, Z.Xing, X.Q.Chen Search for Positive Parity Bands in 117Xe NUCLEAR REACTIONS 92Mo(28Si, n2p), E=115 MeV; measured γγ-coin. 117,119,121,123,125,127Cs level schemes included. 117Xe deduced levels, J, π, band structure, configuration. Model comparison.
doi: 10.1016/0375-9474(94)00662-7
1995LI22 Z.Phys. A351, 363 (1995) Z.Liu, X.Sun, X.Zhou, X.Lei, Y.Zhang, H.Jin, Q.Pan, Y.Guo, X.Chen, Y.Luo, S.Wen, G.J.Yuan, G.S.Li, C.X.Yang, W.D.Luo, Y.S.Chen Observation of High Spin States in 117Xe NUCLEAR REACTIONS 92Mo(28Si, n2p), E=100-120 MeV; measured γγ-coin, DCO ratios. 117Xe deduced high-spin levels, J, π, γ multipolarity, band structure.
doi: 10.1007/BF01291140
1994CH72 Chin.J.Nucl.Phys. 16, No 3, 211 (1994) Anomaly of the Anomalous Delays of the Crossing Frequencies in Odd Proton Nuclei NUCLEAR STRUCTURE 167,169,171,173,175Ta; analyzed crossing frequencies anomalous delays; deduced deformation driving effect, pairing mean fields interplay role. Mean field theory.
1993LU10 Nucl.Phys. A564, 413 (1993) The Triaxial Motion in Mo Isotopes NUCLEAR STRUCTURE 86,87,88,89,90Mo; calculated total routhian energy surfaces. Cranking approximation, Strutinsky method.
doi: 10.1016/0375-9474(93)90512-V
1993ZH16 Z.Phys. A346, 183 (1993) L.K.Zhang, S.Wen, H.Zheng, G.S.Li, S.G.Li, P.K.Weng, P.F.Hua, P.S.Yu, G.J.Yuan, C.X.Yang, W.D.Luo, Y.S.Chen First Observation of High Spin States in 90Tc NUCLEAR REACTIONS 58Ni(35Cl, n2p), E=124 MeV; measured Eγ, Iγ, nγ-coin, DCO ratios. 90Tc deduced levels, J, π, band structure, configuration.
doi: 10.1007/BF01306077
1991CH01 Phys.Rev. C43, 173 (1991) Giant Dipole Resonance Built on Superdeformed Rotational States NUCLEAR STRUCTURE 146,148,150,152Dy, 132,134,136Nd, 80Sr, 82Sr, 84Sr; calculated superdeformed states based GDR, γ-anisotropy following decay. Linear response theory, superdeformed mean field, self-consistent approach. NUCLEAR REACTIONS 150Dy, 134Nd, 82Sr(γ, X), E ≤ 20 MeV; calculated total absorption σ(E). Linear response theory, superdeformed mean field, self-consistent approach.
doi: 10.1103/PhysRevC.43.173
1988JA10 Phys.Rev.Lett. 61, 2073 (1988) V.P.Janzen, M.P.Carpenter, L.L.Riedinger, W.Schmitz, S.Pilotte, S.Monaro, D.D.Rajnauth, J.K.Johansson, D.G.Popescu, J.C.Waddington, Y.S.Chen, F.Donau, P.B.Semmes Evidence for a Low-Frequency πh9/2 Band Crossing in 185Pt and 183Ir NUCLEAR REACTIONS 173Yb(16O, 4n), E=90 MeV; 168Er(19F, 4n), E=85 MeV; measured γγ-coin. 185Pt, 183Ir deduced levels, J, π, γ-branching, B(λ) ratio, band crossing. Cranked shell model. NUCLEAR STRUCTURE 185Pt, 183Ir; calculated levels, B(λ). Cranked shell model.
doi: 10.1103/PhysRevLett.61.2073
1988LE13 Phys.Rev. C37, 2744 (1988) Reflection-Asymmetric Rotor Model of Odd A ≈ 219-229 Nuclei NUCLEAR STRUCTURE 219,221,223,225Rn, 221,223,225,227Fr, 219,221,223,225,227Ra, 219,223,225,227,229Ac, 221,223,225,227,229Th, 229Pa; calculated levels, B(λ), relative spectroscopic factors, electromagnetic properties; deduced deformation parameters.
doi: 10.1103/PhysRevC.37.2744
1988SH34 Nucl.Phys. A486, 306 (1988) R.K.Sheline, Y.-S.Chen, G.A.Leander The Nuclear Spectroscopy and Structure of 223Ra NUCLEAR STRUCTURE 223Ra; calculated levels, magnetic moment, quadrupole moment. Reflection asymmetric rotor model.
doi: 10.1016/0375-9474(88)90238-2
1987LE05 Phys.Rev. C35, 1145 (1987) Rigid Reflection-Asymmetric Rotor Description of the Nucleus 227Ac NUCLEAR STRUCTURE 227Ac; calculated levels, structure factor. Particle-rotor model, static octupole deformation.
doi: 10.1103/PhysRevC.35.1145
1987WE06 Phys.Rev. C36, 431 (1987) J.C.Wells, N.R.Johnson, C.Baktash, I.Y.Lee, F.K.McGowan, M.N.Rao, L.L.Riedinger, V.Janzen, W.C.Ma, Shuxian Wen, Ze-Min Chen, P.B.Semmes, G.A.Leander, Y.S.Chen Low-Frequency Anomaly in 172Os Moment of Inertia NUCLEAR STRUCTURE 172Os; calculated dynamical moments of inertia. Cranked shell model, three-band-mixing calculations. NUCLEAR REACTIONS 144Nd(32S, 4n), E=162 MeV; measured Eγ, Iγ, γγ-coin. 172Os deduced levels, yrast sequence moments of inertia, J, π. Cranked shell model, three-band mixing calculations.
doi: 10.1103/PhysRevC.36.431
1986CH12 Phys.Lett. 171B, 7 (1986) Y.S.Chen, S.Frauendorf, L.L.Riedinger Multi-Quasiparticle Induced Prolate-Oblate Transitions in Rapidly Rotating N = 88, 90 Nuclei NUCLEAR STRUCTURE 159Tm, 154Dy; calculated total routhians. 160Yb; calculated transitional quadrupole moment, total routhians; deduced band signature splitting quenching, B(E2) reduction, collective band structure loss. Multi-quasiparticle model.
doi: 10.1016/0370-2693(86)90987-1
1986CH40 Phys.Rev. C34, 1935 (1986) Y.S.Chen, P.B.Semmes, G.A.Leander Calculation of M1 Transition Rates at High Spin in Axial Nuclei NUCLEAR STRUCTURE 165Lu, 81Kr, 166Hf; calculated yrast levels, g factors, B(M1). Cranking, particle-rotor models.
doi: 10.1103/PhysRevC.34.1935
1986RA07 Phys.Rev.Lett. 57, 667 (1986) M.N.Rao, N.R.Johnson, F.K.McGowan, I.Y.Lee, C.Baktash, M.Oshima, J.W.McConnell, J.C.Wells, A.Larabee, L.L.Riedinger, R.Bengtsson, Z.Xing, Y.S.Chen, P.B.Semmes, G.A.Leander Loss of Collectivity at High Spin in 172W and a Three-Band Interpretation of First Yrast Upbends NUCLEAR REACTIONS 124Sn(52Cr, 4n), E=230 MeV; measured γγ-coin, Doppler shift recoil distance. 172W deduced levels, J, π, T1/2, yrast sequence, dynamical moment of inertia, configuration, transition quadrupole moments.
doi: 10.1103/PhysRevLett.57.667
1986SE07 Phys.Rev. C34, 523 (1986) T.M.Semkow, D.G.Sarantites, K.Honkanen, V.Abenante, L.A.Adler, C.Baktash, N.R.Johnson, I.Y.Lee, M.Oshima, Y.Schutz, Y.S.Chen, J.X.Saladin, C.Y.Chen, O.Dietzsch, A.J.Larabee, L.L.Riedinger, H.C.Griffin Spectroscopic Study of the High-Spin States in 135Pr NUCLEAR STRUCTURE 135Pr; calculated levels, alignments, crossing frequencies. Cranked shell model. NUCLEAR REACTIONS 120Sn(19F, 4n), E=91 MeV; measured Eγ, Iγ, γγ(θ). 135Pr deduced levels, J, π, alignments, crossing frequencies, signature splittings, γ-deformation parameter. Cranked shell model comparison.
doi: 10.1103/PhysRevC.34.523
1984CH21 Nucl.Phys. A421, 403c (1984) The Shape Effects of Rotating High-J Orbits in γ-Soft Nuclei NUCLEAR STRUCTURE 159Tm, 155Ho; calculated rotational band signature splitings. 81Kr; calculated rotational band signature splitings, quasiparticle states, energy surfaces. High-j orbit rotation shape effects.
doi: 10.1016/0375-9474(84)90356-7
1983AR18 Phys.Scr. T5, 157 (1983) Microscopic Calculations of Nuclear Wobbling Rotation NUCLEAR STRUCTURE 179Hf; calculated high-K configuration moment of inertia. 179W; calculated levels. 158Yb; calculated quasicontinuum level energy vs K. Microscopic model, nuclear wobbling rotation.
doi: 10.1088/0031-8949/1983/T5/029
1983BE30 Nucl.Phys. A405, 221 (1983) R.Bengtsson, Y.-S.Chen, J.-Y.Zhang, S.Aberg Deformation Changes along the Yrast Line in 160Yb NUCLEAR STRUCTURE 160Yb; calculated yrast levels, ground band deformation vs spin, band moments of inertia. Cranked HFB model, particle number projection.
doi: 10.1016/0375-9474(83)90569-9
1983CH05 Nucl.Phys. A393, 135 (1983) Magnetic Moments as a Probe for Rotational Alignment NUCLEAR STRUCTURE 232Th, 156,160Dy, 234,238U; calculated yrast level g, aligned angular momenta; deduced angular momentum alignment effects. Cranking model.
doi: 10.1016/0375-9474(83)90069-6
1983CH46 Phys.Rev. C28, 2437 (1983) Y.S.Chen, S.Frauendorf, G.A.Leander Shape of Rotating Quasiparticle Orbits and Signature Splitting in La, Ce, and Pr Nuclei NUCLEAR STRUCTURE 129,130,131,133,134,135Ce, 129,130,133,134La, 130,131,134,135Pr; calculated yrast, near-yrast band Routhians, (γ) deformation signature splitting. Cranking model.
doi: 10.1103/PhysRevC.28.2437
1982CH12 Phys.Lett. 113B, 124 (1982) Y.S.Chen, L.L.Riedinger, G.Leander Accurate Test of Rotationally Perturbed Wave Functions in 161-167Yb NUCLEAR STRUCTURE 161,163,165,167Yb; calculated B(λ), δ. Quasiparticle plus rotor calculations.
doi: 10.1016/0370-2693(82)90407-5
1982CH30 Phys.Rev. C26, 2607 (1982) Quasicontinuum Properties of M1 Spectra in the Particle-Rotor Model NUCLEAR STRUCTURE 159,161,163,165,167,169,171,173,175,177Yb, 127,129,131,133,135,137,139Ce, 131Pr, 129La, 127Cs, 125I, 123Sb; calculated M1 quasicontinuum γ-spectra; deduced particle, quasiparticle number dependence. Core-quasiparticle coupling models.
doi: 10.1103/PhysRevC.26.2607
1981CH25 Phys.Scr. 24, 763 (1981) Low-energy M1 Gamma-rays Emitted in the Deexcitation process of Highly-Rotating Nuclei. NUCLEAR STRUCTURE 161Yb, 174W; calculated multi-nucleon probability spectra, cooling rates; deduced deexcitation dominant γ-multipolarity.
doi: 10.1088/0031-8949/24/4/015
1981LE17 Phys.Scr. 24, 164 (1981) G.Leander, Y.S.Chen, B.S.Nilsson Nuclear Structure and the Quasi-Continuum Gamma Rays NUCLEAR STRUCTURE 158Er, 166Yb; calculated potential energy, γ-correlation plots, moments of inertia. 152Dy; calculated moments of inertia. 162Er; calculated side feeding to yrast states. 165,166,167,168Yb; calculated γ-cascade correlation plots. Several models, quasicontinuum γ-rays.
doi: 10.1088/0031-8949/24/1B/013
1981WA23 Phys.Scr. 24, 324 (1981) W.Walus, N.Roy, S.Jonsson, L.Carlen, H.Ryde, G.B.Hagemann, B.Herskind, J.D.Garrett, Y.S.Chen, J.Almberger, G.Leander High-Spin Band Structure in 166Yb NUCLEAR REACTIONS 154Sm(16O, 4n), E=80 MeV; measured γγ-coin, Eγ, Iγ, γ(θ), I(ce). 166Yb deduced levels, J, π, γ-branching, rotational bands, B(E2), B(M1) ratios.
doi: 10.1088/0031-8949/24/1B/031
1980CH15 Phys.Lett. B94, 468 (1980) Y.-S.Chen, J.D.Garrett, J.Almberger, G.Leander Gamma Correlation Patterns from the (gSS'S''S''') System NUCLEAR STRUCTURE 166Yb; calculated γγ energy correlation; deduced regions of coherent ridge, bridge, peak formations. Particle-rotor model, Monte-Carlo cascade generation, multiple band crossing.
doi: 10.1016/0370-2693(80)90920-X
1972HA64 Nucl.Phys. A195, 250 (1972) D.M.Hardy, R.J.Spiger, S.D.Baker, Y.S.Chen, T.A.Tombrello Scattering of 3He and 4He from Polarized 3He between 7 and 18 MeV NUCLEAR REACTIONS 3He(α, α)3He, E=7.5-17.9 MeV; measured polarization analyzing power; deduced phase shifts. 3He(3He, 3He)3He, E=9.3-17.5 MeV; measured polarization analyzing power.
doi: 10.1016/0375-9474(72)90733-6
1971JA08 Nucl.Phys. A166, 525 (1971) W.R.Jackson, V.Valkovic, S.T.Emerson, W.D.Simpson, C.Joseph, Y.S.Chen, M.C.Taylor, G.C.Phillips The 2H(p, pn)p Reaction at 9.0 MeV NUCLEAR REACTIONS 2H(p, pn), E=9 MeV; measured σ(Ep, En, θ(p), θ(n)); deduced final state interactions, quasifree scattering contributions.
doi: 10.1016/0375-9474(71)90904-3
1970CH07 Nucl.Phys. A146, 136 (1970) Y.S.Chen, T.A.Tombrello, R.W.Kavanagh Decay Modes of 9Li and States of 9Be RADIOACTIVITY 9Li[from 3H(7Li, p), E=14 MeV; 18O(7Li, 16O), E=20 MeV]; measured T1/2, Eβ, βn-coin, E(delayed n), E(delayed α); deduced log ft, Iβ. 9Be deduced levls, J, π, Γ, Γn.
doi: 10.1016/0375-9474(70)91093-6
1968CH01 Nucl.Phys. A106, 1 (1968) Y.S.Chen, S.T.Emerson, W.R.Jackson, W.D.Simpson, G.C.Phillips The 11B(p, 2α)4He Reaction at 163 keV Resonance NUCLEAR REACTIONS 11B(p, 2α)4He, E = 163 keV; measured σ(Eα1, Eα2, θ(1), θ(2)). Enriched target.
doi: 10.1016/0375-9474(67)90823-8
1967VA11 Nucl.Phys. A96, 241 (1967) V.Valkovic, W.R.Jackson, Y.S.Chen, S.T.Emerson, G.C.Phillips Three-Body Break-Up in 7Li(d, nα)4He and 7Li(d, αα)n Reactions NUCLEAR REACTIONS 7Li(d, αn), 7Li(d, 2α), E=2.6-4.0 MeV; measured σ(En, Eα, θ(n), θ(α)), σ(Eα1, Eα2, θ(α1), θ(α2)). Enriched target.
doi: 10.1016/0375-9474(67)90709-9
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