NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = B.N.Lu Found 26 matches. 2023RO04 Phys.Lett. B 840, 137896 (2023) Y.-T.Rong, X.-Y.Wu, B.-N.Lu, J.-M.Yao Anatomy of octupole correlations in ^{96}Zr with a symmetry-restored multidimensionally-constrained covariant density functional theory NUCLEAR STRUCTURE ^{96}Zr; calculated potential energy surfaces, deformation parameters and excitation energies, J, π, B(Eλ), single-neutron levels with a unified framework called p-MDCRHB model. Comparison with available data.
doi: 10.1016/j.physletb.2023.137896
2022LU05 Phys.Rev.Lett. 128, 242501 (2022) B.-N.Lu, N.Li, S.Elhatisari, Y.-Z.Ma, D.Lee, U.-G.Meissner Perturbative Quantum Monte Carlo Method for Nuclear Physics NUCLEAR STRUCTURE ^{3}H, ^{4}He, ^{8}Be, ^{12}C, ^{16}O; calculated binding energies using ptQMC. Comparison with experimental data.
doi: 10.1103/PhysRevLett.128.242501
2021LE13 Phys.Rev.Lett. 127, 062501 (2021) D.Lee, S.Bogner, B.A.Brown, S.Elhatisari, E.Epelbaum, H.Hergert, M.Hjorth-Jensen, H.Krebs, N.Li, B.-N.Lu, U.-G.Meissner Hidden Spin-Isospin Exchange Symmetry
doi: 10.1103/PhysRevLett.127.062501
2021SO28 Phys.Rev. C 104, 044304 (2021) Y.-H.Song, Y.Kim, N.Li, B.-N.Lu, R.He, D.Lee Quantum many-body calculations using body-centered cubic lattices
doi: 10.1103/PhysRevC.104.044304
2021SU20 Phys.Rev. C 104, L041901 (2021) N.Summerfield, B.-N.Lu, C.Plumberg, D.Lee, J.Noronha-Hostler, A.Timmins ^{16}O^{16}O collisions at energies available at the BNL Relativistic Heavy Ion Collider and at the CERN Large Hadron Collider comparing α clustering versus substructure NUCLEAR REACTIONS ^{16}O(^{16}O, X), E=200, 6500 GeV; calculated various flow coefficients versus centrality using state-of-the-art iEBE-VISHNU package, tuned using a Bayesian analysis on p+Pb and Pb+Pb systems for proposed experiments using ^{16}O+^{16}O systems at LHC-CERN and at RHIC-BNL to investigate α clustering in ^{16}O; deduced measurable differences between α-clustering, nucleonic, and subnucleonic degrees of freedom in the initial state from ratios of flow harmonics.
doi: 10.1103/PhysRevC.104.L041901
2020LU12 Phys.Rev.Lett. 125, 192502 (2020) B.-N.Lu, N.Li, S.Elhatisari, D.Lee, J.E.Drut, T.A.Lahde, E.Epelbaum, U.G.Meissner Ab Initio Nuclear Thermodynamics
doi: 10.1103/PhysRevLett.125.192502
2018LI53 Phys.Rev. C 98, 044002 (2018) N.Li, S.Elhatisari, E.Epelbaum, D.Lee, B.-N.Lu, U.-G.Meissner Neutron-proton scattering with lattice chiral effective field theory at next-to-next-to-next-to-leading order NUCLEAR STRUCTURE ^{2}H; calculated neutron-proton scattering phase shifts and mixing angles versus relative momenta for different lattice spacings, properties of deuteron wave function and the s-wave effective range parameters, low-energy constants using ab initio lattice formulation of the chiral effective field theory for LO, NLO, N^{2}LO and N^{3}LO NN interactions. Comparison with empirical values.
doi: 10.1103/PhysRevC.98.044002
2017AL18 Eur.Phys.J. A 53, 83 (2017) J.M.Alarcon, D.Du, N.Klein, T.A.Lahde, D.Lee, N.Li, B.-N.Lu, T.Luu, Ulf-G.Meissner Neutron-proton scattering at next-to-next-to-leading order in Nuclear Lattice Effective Field Theory NUCLEAR STRUCTURE ^{4}He, ^{8}Be, ^{12}C, ^{16}O, ^{20}Ne, ^{24}Mg, ^{28}Si;calculated binding energy, mass excess using 2N forces up to NNLO in the NLEFT (Nuclear Lattice Effective Field Theory);deduced parameters using available data.
doi: 10.1140/epja/i2017-12273-x
2017EL05 Phys.Rev.Lett. 119, 222505 (2017) S.Elhatisari, E.Epelbaum, H.Krebs, T.A.Lahde, D.Lee, N.Li, B.-n.Lu, U.-G.Meissner, G.Rupak Ab initio Calculations of the Isotopic Dependence of Nuclear Clustering NUCLEAR STRUCTURE ^{12,14,16}C; calculated proton and neutron densities for the ground states, spin-up proton probability distributions.
doi: 10.1103/PhysRevLett.119.222505
2017ZH05 Phys.Rev. C 95, 014320 (2017) J.Zhao, B.-N.Lu, E.-G.Zhao, S.-G.Zhou Tetrahedral shapes of neutron-rich Zr isotopes from a multidimensionally constrained relativistic Hartree-Bogoliubov model NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114}Zr; calculated potential energy curves as function of β_{20}, binding energy and β_{32} deformation, ground state binding energies, quadrupole deformation β_{20}, axial octupole deformation β_{30}, nonaxial octupole deformation β_{32}, and hexadecapole deformation β_{40}, binding energies for various energy minima for oblate, pear-like, tetrahedral and prolate shapes, neutron and proton single-particle levels near the Fermi surface and pairing energies for ^{110}Zr, potential energy surfaces for A=106-114 Zr isotopes in (β_{30}, β_{32}) plane. Multidimensionally constrained relativistic Hartree-Bogoliubov (MDC-RHB) model with relativistic functionals DD-PC1 and PC-PK1. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.014320
2016EL03 Phys.Rev.Lett. 117, 132501 (2016) S.Elhatisari, N.Li, A.Rokash, J.M.Alarcon, D.Du, N.Klein, B.-n.Lu, U.-G.Meissner, E.Epelbaum, H.Krebs, Ti.A.Lahde, De.Lee, G.Rupak Nuclear Binding Near a Quantum Phase Transition NUCLEAR STRUCTURE ^{3}H, ^{3,4}He, ^{8}Be, ^{12}C, ^{16}O, ^{20}Ne; calculated ground state energies; deduced a first-order transition at zero temperature from a Bose-condensed gas of alpha particles to a nuclear liquid. Leading order (LO) nuclear interactions.
doi: 10.1103/PhysRevLett.117.132501
2016ZH14 Phys.Rev. C 93, 044315 (2016) J.Zhao, B.-N.Lu, T.Niksic, D.Vretenar, S.-G.Zhou Multidimensionally-constrained relativistic mean-field study of spontaneous fission: Coupling between shape and pairing degrees of freedom RADIOACTIVITY ^{250,264}Fm(SF); calculated effective collective potentials in (β_{20}, β_{22}), (β_{20}, λ_{2}) and (β_{20}, β_{30}) planes, 3D dynamic fission paths, action integrals, SF half-lives, particle-number fluctuation degrees of freedom on symmetric and asymmetric spontaneous fission (SF) dynamics. Multidimensionally-constrained relativistic-mean-field (MDC-RMF) model with pairing correlations in the BCS approximation. Comparison with Hartree-Fock-Bogoliubov (HFB) model calculations.
doi: 10.1103/PhysRevC.93.044315
2015PR04 Phys.Rev. C 91, 034324 (2015) V.Prassa, B.-N.Lu, T.Niksic, D.Ackermann, D.Vretenar High-K isomers in transactinide nuclei close to N=162 NUCLEAR STRUCTURE ^{264,266,268,270}Rf, ^{266,268,270,272}Sg, ^{268,270,272,274}Hs, ^{270,272,274,276}Ds; calculated lowest two-quasiparticle states, and lowest calculated two-quasiparticle K isomers, self-consistent RHB triaxial energy contours in (β, γ) plane for even-even Hs isotopes shape evolutions. Relevance to occurrence of deformed shell gaps in very heavy nuclei. Self-consistent mean-field framework based on relativistic energy density functionals.
doi: 10.1103/PhysRevC.91.034324
2015ZH03 Phys.Rev. C 91, 014321 (2015) J.Zhao, B.-N.Lu, D.Vretenar, E.-G.Zhao, S.-G.Zhou Multidimensionally constrained relativistic mean-field study of triple-humped barriers in actinides NUCLEAR STRUCTURE ^{226,228,230,232}Th, ^{232,234,236,238}U; calculated energy curves as function of deformation parameter β_{20}, two dimensional potential energy surfaces (PES) in (β_{20}, β_{30}) plane, odd-even differences of binding energies, excitation energies of the second saddle point, third (hyperdeformed) minimum, and third saddle point, depth of third potential well. Covariant density functional theory (CDFT) with relativistic mean field (MDCRMF) model and nonlinear point-coupling functional PC-PK1 and density-dependent functional DD-ME2, with pairing correlations in BCS approximation.
doi: 10.1103/PhysRevC.91.014321
2015ZH45 Phys.Rev. C 92, 064315 (2015) J.Zhao, B.-N.Lu, Ta.Niksic, D.Vretenar Multidimensionally constrained relativistic Hartree-Bogoliubov study of spontaneous nuclear fission RADIOACTIVITY ^{250,264}Fm(SF); calculated triaxial quadrupole constrained energy surfaces, binding energy, deformation parameter β_{40}, perturbative- and non-perturbative cranking inertia tensors, dynamic paths, action integral and SF half-lives in (β_{20}, β_{22}) and (β_{20}, β_{30}) planes. Symmetric and asymmetric fissions. Inclusion of nonaxial quadrupole and octupole shape degrees of freedom in fission dynamics. Multidimensionally-constrained relativistic Hartree-Bogoliubov (MDC-RHB) model, with the energy density functionals PC-PK1 and DD-PC1, and pairing correlations in the Bogoliubov approximation. The least-action principle used to determine dynamic spontaneous fission paths.
doi: 10.1103/PhysRevC.92.064315
2014LU01 Phys.Rev. C 89, 014323 (2014) B.-N.Lu, J.Zhao, E.-G.Zhao, S.-G.Zhou Multidimensionally-constrained relativistic mean-field models and potential-energy surfaces of actinide nuclei NUCLEAR STRUCTURE ^{240}Pu; calculated potential energy curves as function of deformation and truncations, three-dimensional potential energy surface contours as function of deformation around the ground state, the inner barrier, and fission isomer. ^{230,232}Th, ^{232,234,236,238,240}U, ^{238,240,242,244,246}Pu, ^{242,244,246,248,250}Cm, ^{250,252}Cf; calculated potential energy curves around the ground states and the first and second fission barriers, heights of the first second fission barriers. Multidimensionally-constrained relativistic mean-field (MDC-RMF) models, with the solution of Dirac equation in an axially deformed harmonic oscillator (ADHO) basis. Importance of nonaxial and spatial reflection asymmetric shapes in the study of potential energy surfaces and fission barriers of actinides and Superheavy nuclei. Comparison with available experimental data.
doi: 10.1103/PhysRevC.89.014323
2014LU06 Phys.Rev. C 89, 044307 (2014) B.-N.Lu, E.Hiyama, H.Sagawa, S.-G.Zhou Superdeformed Λ hypernuclei within relativistic mean field models NUCLEAR STRUCTURE ^{33}S, ^{37,39,41}Ar, ^{41}Ca, ^{57}Ni, ^{61}Zn; calculated energies as function of deformation parameter, β_{2}, β_{p}, β_{n}, β_{Λ}, I_{overlap}, binding energy, rms radii, Λ separation energies, density distribution contours in (r, z) plane, Nilsson wave function for ground state and superdeformed states of hypernuclei. ^{36,38,40,41}Ar, ^{40}Ca; calculated energies as function of deformation parameter, β_{2}, β_{p}, β_{n} deformation parameters, rms radii, binding energies, density distribution contours in (r, z) plane. Multidimensionally constrained relativistic mean field (MDC-RMF) models for superdeformed states of nuclei and hypernuclei. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.044307
2014LU17 Phys.Scr. 89, 054028 (2014) B.-N.Lu, J.Zhao, E.-G.Zhao, S.-G.Zhou Multidimensionally constrained relativistic mean field model and applications in actinide and transfermium nuclei NUCLEAR STRUCTURE ^{240}Pu; calculated potential energy vs deformation for various selfconsistent symmetries using covariant density functional.
doi: 10.1088/0031-8949/89/5/054028
2014NO01 Phys.Rev. C 89, 024312 (2014) K.Nomura, D.Vretenar, T.Niksic, B.-N.Lu Microscopic description of octupole shape-phase transitions in light actinide and rare-earth nuclei NUCLEAR STRUCTURE ^{222,224,226,228,230,232}Th, ^{218,220,222,224,226,228}Ra, ^{146,148,150,152,154,156}Sm, ^{140,142,144,146,148,150}Ba; calculated energy surface contours in (β_{2}, β_{3}) plane, mean values of octupole deformation, levels, J, π, E(J)/E(first 2+) ratios, B(E1), B(E2), B(E3), quadrupole and octupole intrinsic moments. Octupole shape transitions. Self-consistent relativistic Hartree-Bogoliubov (RHB), and interacting boson model (IBM) calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.024312
2013LU11 Phys.Rev. C 88, 024323 (2013) Pseudospin symmetry in single-particle resonances in spherical square wells
doi: 10.1103/PhysRevC.88.024323
2013NO07 Phys.Rev. C 88, 021303 (2013) Microscopic analysis of the octupole phase transition in Th isotopes NUCLEAR STRUCTURE ^{220,222,224,228,230,232}Th; calculated levels, J, π, bands, yrast states, energy surface contours in (β_{2}, β_{3}) plane, E(J)/E(2+) ratios, B(E2), B(E1). Shape phase transition between stable octupole deformation and octupole vibrations. Microscopic framework based on nuclear density functional theory using DD-PC1 interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.88.021303
2012LU02 Phys.Rev. C 85, 011301 (2012) Potential energy surfaces of actinide nuclei from a multidimensional constrained covariant density functional theory: Barrier heights and saddle point shapes NUCLEAR STRUCTURE ^{240}Pu, ^{248}Cm; calculated potential energy surfaces. ^{230,232}Th, ^{232,234,236,238}U, ^{238,240,242,244}Pu, ^{242,244,246,248}Cm; calculated inner and outer fission barrier heights. Importance of triaxial and octupole shapes in fission path. Multidimensional constrained covariant density functional theory. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.011301
2012LU17 Phys.Rev.Lett. 109, 072501 (2012) Pseudospin Symmetry in Single Particle Resonant States
doi: 10.1103/PhysRevLett.109.072501
2012ZH45 Phys.Rev. C 86, 057304 (2012) J.Zhao, B.-N.Lu, E.-G.Zhao, S.-G.Zhou Nonaxial-octupole Y_{32} correlations in N=150 isotones from multidimensional constrained covariant density functional theories NUCLEAR STRUCTURE ^{246}Cm, ^{248}Cf, ^{250}Fm, ^{252}No; calculated quadrupole, non-axial octupole and hexadecapole deformations, binding energies, single-particle levels near the Fermi surface for protons and neutrons. Multidimensional constrained covariant density functional theories with DD-PC1 parameter set. Comparison with experimental data. Nonaxial reflection-asymmetric (β_{32} octupole) effects.
doi: 10.1103/PhysRevC.86.057304
2011AD15 Phys.Rev. C 84, 024324 (2011) G.G.Adamian, N.V.Antonenko, S.N.Kuklin, B.N.Lu, L.A.Malov, S.G.Zhou Behavior of one-quasiparticle levels in odd isotonic chains of heavy nuclei NUCLEAR STRUCTURE ^{255}Fm, ^{257}No, ^{259}Rf, ^{261}Sg, ^{263}Hs; calculated ground state deformation parameters β_{2} and β_{4}. ^{239}U, ^{241,243,247}Pu, ^{243,245,247,249}Cm, ^{243,245,247,249,251}Cf, ^{241,243,245,247,249,251,253,255}Fm, ^{245,247,249,251,253,255,257}No, ^{255,257,259}Rf, ^{259,261}Sg, ^{263}Hs; calculated one-quasiparticle states in N=147, 149, 151, 153, 155 nuclei. ^{253}No; calculated collective rotational bands. Discussed isomers in odd-A Fm and No nuclei. Two-center shell model (TCSM), quasiparticle-phonon model (QPM), Skyrme-Hartree-Fock-Bogolyubov (SHFB) approach with SLy4 and SkP parameterization. Comparison with experimental data. RADIOACTIVITY ^{257,257m}Rf, ^{257,257m}No(α); calculated Q(α), decay schemes. ^{253}Fm, ^{253}No; deduced levels.
doi: 10.1103/PhysRevC.84.024324
2010AD17 Physics of Part.and Nuclei 41, 1101 (2010) G.G.Adamian, N.V.Antonenko, L.A.Malov, B.N.Lu, S.G.Zhou, W.Scheid Isomeric states in heavy nuclei NUCLEAR STRUCTURE ^{243}Pu, ^{245}Cm, ^{247}Cf, ^{249}Fm, ^{251}No, ^{270}Ds, ^{266}Hs, ^{262}Sg, ^{258}Rf, ^{254}No; calculated one-, two-quasiparticle states and energies, J, π. HB and shell models.
doi: 10.1134/S1063779610070269
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