NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = Z.H.Sun Found 20 matches. 2024XU04 Chin.Phys.C 48, 024106 (2024) Y.-L.Xu, X.-W.Su, Zh.-H.Sun, Y.-L.Han, X.-J.Sun, D.-H.Zhang, Ch.-H.Cai Description of elastic scattering for 7Li-induced reactions on 1p-shell nuclei NUCLEAR REACTIONS 9Be, 10,11B, 12,13C, 15N, 16O(7Li, 7Li), E=4.5-131.8 MeV; analyzed available data; deduced σ(θ), the global phenomenological optical potentials (GPOPs), the contribution of elastic transfer by the distorted wave Born approximation (DWBA) method.
doi: 10.1088/1674-1137/ad1924
2023GU20 Phys.Rev. C 108, 054309 (2023) C.Gu, Z.H.Sun, G.Hagen, T.Papenbrock Entanglement entropy of nuclear systems
doi: 10.1103/PhysRevC.108.054309
2023KO15 Nature(London) 620, 965 (2023) Y.Kondo, N.L.Achouri, H.Al Falou, L.Atar, T.Aumann, H.Baba, K.Boretzky, C.Caesar, D.Calvet, H.Chae, N.Chiga, A.Corsi, F.Delaunay, A.Delbart, Q.Deshayes, Zs.Dombradi, C.A.Douma, A.Ekstrom, Z.Elekes, C.Forssen, I.Gasparic, J.-M.Gheller, J.Gibelin, A.Gillibert, G.Hagen, M.N.Harakeh, A.Hirayama, C.R.Hoffman, M.Holl, A.Horvat, A.Horvath, J.W.Hwang, T.Isobe, W.G.Jiang, J.Kahlbow, N.Kalantar-Nayestanaki, S.Kawase, S.Kim, K.Kisamori, T.Kobayashi, D.Korper, S.Koyama, I.Kuti, V.Lapoux, S.Lindberg, F.M.Marques, S.Masuoka, J.Mayer, K.Miki, T.Murakami, M.Najafi, T.Nakamura, K.Nakano, N.Nakatsuka, T.Nilsson, A.Obertelli, K.Ogata, F.de Oliveira Santos, N.A.Orr, H.Otsu, T.Otsuka, T.Ozaki, V.Panin, T.Papenbrock, S.Paschalis, A.Revel, D.Rossi, A.T.Saito, T.Y.Saito, M.Sasano, H.Sato, Y.Satou, H.Scheit, F.Schindler, P.Schrock, M.Shikata, N.Shimizu, Y.Shimizu, H.Simon, D.Sohler, O.Sorlin, L.Stuhl, Z.H.Sun, S.Takeuchi, M.Tanaka, M.Thoennessen, H.Tornqvist, Y.Togano, T.Tomai, J.Tscheuschner, J.Tsubota, N.Tsunoda, T.Uesaka, Y.Utsuno, I.Vernon, H.Wang, Z.Yang, M.Yasuda, K.Yoneda, S.Yoshida First observation of 28O NUCLEAR REACTIONS H(29F, X)27O/28O, E=235 MeV/nucleon; measured reaction products; deduced yields. The hydrogen target was surrounded by the MINOS Time Projection Chamber, SAMURAI spectrometer, RIKEN RI Beam Factory. RADIOACTIVITY 28O(4n), 27O(3n); measured decay products, En, In; deduced decay energy spectra and schemes from the measured momenta using the invariant-mass technique, resonance parameters. Comparison with the large-scale shell-model calculations using the new chiral effective field theory (EEdf3) interaction.
doi: 10.1038/s41586-023-06352-6
2023SU07 Phys.Rev. C 108, 014307 (2023) Z.H.Sun, G.Hagen, T.Papenbrock Coupled-cluster theory for strong entanglement in nuclei NUCLEAR STRUCTURE 12C, 28Si, 56Ni; calculated ground-state energy. Single-reference coupled-cluster theory based on spherical and deformed reference states and the tailored coupled-cluster method. Comparison to experimental data.
doi: 10.1103/PhysRevC.108.014307
2022GE09 Phys.Rev. C 106, 024304 (2022) Y.F.Geng, J.G.Li, Y.Z.Ma, B.S.Hu, Q.Wu, Z.H.Sun, S.Zhang, F.R.Xu Excitation spectra of the heaviest carbon isotopes investigated within the CD-Bonn Gamow shell model NUCLEAR STRUCTURE 19,20,21,22C; calculated levels, J, π, ground-state energies using Gamow shell model (GSM) based on a realistic nuclear, with a complex GSM effective interaction derived from many-body perturbation theory. Comparison with experimental data.
doi: 10.1103/PhysRevC.106.024304
2022HA19 Phys.Rev. C 105, 064311 (2022) G.Hagen, S.J.Novario, Z.H.Sun, T.Papenbrock, G.R.Jansen, J.G.Lietz, T.Duguet, A.Tichai Angular-momentum projection in coupled-cluster theory: Structure of 34Mg NUCLEAR STRUCTURE 8Be; calculated energies using symmetry-unrestricted Hartree-Fock and HF-RVAP as a function of the mass quadrupole moment q20. 20Ne, 34Mg; calculated the norm kernels and Hamiltonian kernels as function of the rotation angle using Hartree-Fock and CCD theories. 8Be, 20Ne, 34Mg; calculated projected coupled-cluster energies of the ground and excited states as a function of oscillator frequency using CCD, SLD, and SQD approximations. 44,46,48Ti, 48,50Cr; calculated low-lying states of J=0, 2 and 4 using projection-after-variation Hartree-Fock (PAV HF), variation-after-projection Hartree-Fock (VAP-HF), and projected CCD, SLD, and SQD methods, and compared to FCI results. Angular-momentum projection after variation with the disentangled coupled-cluster formalism and a Hermitian approach. Comparison with two-nucleon interaction from chiral effective field theory and for pf-shell nuclei within the traditional shell model, and with experimental data.
doi: 10.1103/PhysRevC.105.064311
2022OH01 Phys.Rev. C 105, L031305 (2022) B.Ohayon, R.F.Garcia Ruiz, Z.H.Sun, G.Hagen, T.Papenbrock, B.K.Sahoo Nuclear charge radii of Na isotopes: Interplay of atomic and nuclear theory NUCLEAR STRUCTURE 18,20,22,24,26,28Ne, 21,23,25,27,28,31Na, 22,24,26,28,30,32Mg; analyzed experimental isotope shifts (from 2012YO01, 1978HU12, 2011MA48, 1975HU04); deduced charge radii using improved atomic calculations and nuclear coupled-cluster theory. Developed analytic response-based RCC (AR-RCC) theory to include full triple electron excitations and perturbatively estimate quadrupole excitations. Comparison to the results obtained with atomic parameters obtained with different calculations and with values returned from the semiempirical neutron-skin for Na isotopes.
doi: 10.1103/PhysRevC.105.L031305
2022SU04 Int.J.Mod.Phys. E31, 2250001 (2022) Z.-H.Sun, Y.-L.Xu, X.-J.Sun, Y.-L.Han, C.-H.Cai Global phenomenological optical model potential for 14N-nucleus elastic scattering NUCLEAR REACTIONS 24Mg, 27Al, 28,29Si, 32S, 40Ca, 56Fe, 59Co, 58,62Ni, 70,74Ge, 90Zr, 92,100Mo, 118Sn, 208Pb(14N, 14N), E<100 MeV; analyzed available data; deduced global optical model potential parameters, σ, σ(θ).
doi: 10.1142/S021830132250001X
2022SU28 Phys.Rev. C 106, L061302 (2022) Z.H.Sun, C.A.Bell, G.Hagen, T.Papenbrock How to renormalize coupled cluster theory ATOMIC MASSES 20,22,24,26,28,30,32,34Na, 16,24O, 40,48Ca, 78Ni, 90Zr, 100Sn; calculated binding energies, energies per nucleon. Coupled cluster theory with included short-range three-body correlations by renormalizing the three-body contact interaction. Comparison to experimental values.
doi: 10.1103/PhysRevC.106.L061302
2022YU02 Phys.Rev. C 105, L061303 (2022) Q.Yuan, S.Q.Fan, B.S.Hu, J.G.Li, S.Zhang, S.M.Wang, Z.H.Sun, Y.Z.Ma, F.R.Xu Deformed in-medium similarity renormalization group NUCLEAR STRUCTURE 6,8,10,12,14,16Be, 10,12,14,16,18,20,22C, 14,16,18,20,22,24,26,28O, 16,18,20,22,24,26,28,30,32,34Ne, 20,22,24,26,28,30,32,34,36,38,40Mg; calculated ground-state energies, and charge radii using deformed ab initio in-medium similarity renormalization group (deformed IMSRG), Hartree-Fock, and angular momentum projection methods for open-shell nuclei; results benchmarked with the no-core shell model and valence-space IMSRG calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.105.L061303
2021HO15 Phys.Lett. B 822, 136710 (2021) M.Holl, R.Kanungo, Z.H.Sun, G.Hagen, J.A.Lay, A.M.Moro, P.Navratil, T.Papenbrock, M.Alcorta, D.Connolly, B.Davids, A.Diaz Varela, M.Gennari, G.Hackman, J.Henderson, S.Ishimoto, A.I.Kilic, R.Krucken, A.Lennarz, J.Liang, J.Measures, W.Mittig, O.Paetkau, A.Psaltis, S.Quaglioni, J.S.Randhawa, J.Smallcombe, I.J.Thompson, M.Vorabbi, M.Williams Proton inelastic scattering reveals deformation in 8He NUCLEAR REACTIONS 1H(8He, p), E=8.25 MeV/nucleon; measured reaction products, Ep, Ip. 8He; deduced σ(θ), resonance parameters, first 2+ state, quadrupole deformation parameter. Comparison with no-core shell model predictions. Charged particle spectroscopy station IRIS at TRIUMF in Canada.
doi: 10.1016/j.physletb.2021.136710
2021MO23 Nat.Phys. 17, 1099 (2021) M.Mougeot, D.Atanasov, J.Karthein, R.N.Wolf, P.Ascher, K.Blaum, K.Chrysalidis, G.Hagen, J.D.Holt, W.J.Huang, G.R.Jansen, I.Kulikov, Yu.A.Litvinov, D.Lunney, V.Manea, T.Miyagi, T.Papenbrock, L.Schweikhard, A.Schwenk, T.Steinsberger, S.R.Stroberg, Z.H.Sun, A.Welker, F.Wienholtz, S.G.Wilkins, K.Zuber Mass measurements of 99-101In challenge ab initio nuclear theory of the nuclide 100Sn NUCLEAR REACTIONS La(p, X)99In/100In/101In, E=1.4 GeV; measured reaction products, TOF; deduced atomic masses. Comparison with AME2020, theoretical calculations.
doi: 10.1038/s41567-021-01326-9
2021SU22 Phys.Rev. C 104, 064310 (2021) Z.H.Sun, G.Hagen, G.R.Jansen, T.Papenbrock Effective shell-model interaction for nuclei "southeast" of 100Sn NUCLEAR STRUCTURE 100Sn; calculated single-particle neutron and single-hole proton states from effective shell-model interaction for the valence space and using chiral nucleon-nucleon and three-nucleon forces and single-reference coupled-cluster theory and ΔNNLOGO potentials, with detailed matrix elements given in the Supplemental Material. 98Cd, 100In, 100,102Sn; calculated ground-state energies relative using 1.8/2.0(EM) and ΔNNLOGO potentials and compared to experimental data. 102,104,106,108Sn, 98Cd, 100,101,103,105,107In, 100,102,104,106Cd, ; calculated low-lying positive-parity levels from Jπ=0+ to 8+ for even-A and low-lying positive- and negative-parity levels from Jπ=1/2- to 13/2+ for odd-A using 1.8/2.0(EM) and ΔNNLOGO potentials, and compared to experimental data. Systematic derivation of the particle-hole variant of the shell-model coupled-cluster method to compute nuclei in the vicinity of 100Sn, with the shell-model effective interaction defined in a model space consisting of particles and holes.
doi: 10.1103/PhysRevC.104.064310
2019HU13 Phys.Rev. C 99, 061302 (2019) Ab initio Gamow in-medium similarity renormalization group with resonance and continuum NUCLEAR STRUCTURE 22C, 24O; calculated levels, J, p, resonance and continuum spectra, radial density distributions, and halo structure for 22O using ab initio Gamow in-medium similarity renormalization group (Gamow IMSRG) calculations, effective field theory, and three-body forces. Comparison with experimental level spectra, and with complex coupled-channel (CC) calculation.
doi: 10.1103/PhysRevC.99.061302
2018JI07 Phys.Rev. C 98, 044320 (2018) W.G.Jiang, B.S.Hu, Z.H.Sun, F.R.Xu Gogny-force-derived effective shell-model Hamiltonian NUCLEAR STRUCTURE 10,11B, 18N, 7Li, 10Be, 16,17,18,19,20,21,22,23,24,25,26,27,28O, 18,19,20,21,22,23,24,25,26,27,28,29F, 18,20,21,22,23,24,25,26,27,28,30,32,34Ne; calculated levels, J, π, g.s. energies and binding energies of O, F, Ne isotopes, and first 2+ state energies and B(E2) values in even-even Ne isotopes. Shell model with density-dependent finite-range Gogny force.Comparison with experimental values, and with other theoretical predictions.
doi: 10.1103/PhysRevC.98.044320
2018SU23 Phys.Rev. C 98, 054320 (2018) Z.H.Sun, T.D.Morris, G.Hagen, G.R.Jansen, T.Papenbrock Shell-model coupled-cluster method for open-shell nuclei NUCLEAR STRUCTURE 6,7,8He, 6,7,8Li; calculated low-lying levels, J, π, squared point-proton radii, and isotope shifts using shell-model coupled-cluster method employing 4He core. Comparison with other theoretical predictions.
doi: 10.1103/PhysRevC.98.054320
2018WU03 Phys.Rev. C 97, 054306 (2018) Q.Wu, B.S.Hu, F.R.Xu, Y.Z.Ma, S.J.Dai, Z.H.Sun, G.R.Jansen Chiral NNLOsat descriptions of nuclear multipole resonances within the random-phase approximation NUCLEAR STRUCTURE 4He, 16,22,24O, 40,48Ca; calculated charge radii, strength distributions and centroids of isoscalar monopole, isovector dipole and isoscalar quadrupole resonances, transition densities of protons and neutrons using random-phase approximation (RPA) framework with realistic nuclear forces and chiral potential NNLOsat. 22,24O; deduced low-lying strengths. Comparison with experimental data.
doi: 10.1103/PhysRevC.97.054306
2017HU04 Phys.Rev. C 95, 034321 (2017) B.S.Hu, F.R.Xu, Q.Wu, Y.Z.Ma, Z.H.Sun Brueckner-Hartree-Fock calculations for finite nuclei with renormalized realistic forces NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated ground-state energies, point-nucleon rms radii, single-particle energies, single-proton energies and occupation probabilities. Renormalized Brueckner-Hartree-Fock (RBHF) and BHF calculations with two-step G-matrix approximations. Comparison with available experimental data.
doi: 10.1103/PhysRevC.95.034321
2016HU11 Phys.Rev. C 94, 014303 (2016) B.S.Hu, F.R.Xu, Z.H.Sun, J.P.Vary, T.Li Ab initio nuclear many-body perturbation calculations in the Hartree-Fock basis NUCLEAR STRUCTURE 4He, 16O; calculated binding energies and point-proton rms radii using ab initio many-body perturbation theory (MBPT), with realistic nuclear forces, chiral N3LO and JISP16. Comparison with experimental data.
doi: 10.1103/PhysRevC.94.014303
2014JI06 Phys.Rev. C 90, 024306 (2014) L.F.Jiao, Z.H.Sun, Z.X.Xu, F.R.Xu, C.Qi Correlated-basis method for shell-model calculations NUCLEAR STRUCTURE 28Si; calculated levels, J, π, wave function overlaps and coefficient distributions, convergence properties of low-lying 0+, 2+, 4+ and 6+ states. 106Sn; calculated convergence properties of low-lying 2+ and 4+ states. Correlated-basis Truncated shell-model calculations.
doi: 10.1103/PhysRevC.90.024306
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