NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = B.S.Hu Found 49 matches. 2024HE01 Phys.Rev. C 109, 014327 (2024) J.Heery, J.Henderson, C.R.Hoffman, A.M.Hill, T.Beck, C.Cousins, P.Farris, A.Gade, S.A.Gillespie, J.D.Holt, B.Hu, H.Iwasaki, S.Kisyov, A.N.Kuchera, B.Longfellow, C.Muller-Gatermann, A.Poves, E.Rubino, R.Russell, R.Salinas, A.Sanchez, D.Weisshaar, C.Y.Wu, J.Wu Suppressed electric quadrupole collectivity in 32Si
doi: 10.1103/PhysRevC.109.014327
2024HU02 Phys.Rev. C 109, L021302 (2024) Static quadrupole moment as a criterion to distinguish chiral modes
doi: 10.1103/PhysRevC.109.L021302
2024KO07 Phys.Rev.Lett. 132, 162502 (2024) K.Konig, J.C.Berengut, A.Borschevsky, A.Brinson, B.A.Brown, A.Dockery, S.Elhatisari, E.Eliav, R.F.G.Ruiz, J.D.Holt, B.-Sh.Hu, J.Karthein, D.Lee, Y.-Zh.Ma, U.-G.Meissner, K.Minamisono, A.V.Oleynichenko, S.V.Pineda, S.D.Prosnyak, M.L.Reitsma, L.V.Skripnikov, A.Vernon, A.Zaitsevskii Nuclear Charge Radii of Silicon Isotopes NUCLEAR MOMENTS 28,29,30,32Si; measured frequencies; deduced isotope shifts, nuclear charge radii using collinear laser spectroscopy. Comparison with ab initio nuclear lattice effective field theory, valence-space in-medium similarity renormalization group, and mean field calculations. The BECOLA setup at the Facility for Rare Isotope Beams.
doi: 10.1103/PhysRevLett.132.162502
2024LI18 Phys.Rev. C 109, 034312 (2024) B.D.Linh, A.Corsi, A.Gillibert, A.Obertelli, P.Doornenbal, C.Barbieri, T.Duguet, M.Gomez-Ramos, J.D.Holt, B.S.Hu, T.Miyagi, A.M.Moro, P.Navratil, K.Ogata, S.Peru, N.T.T.Phuc, N.Shimizu, V.Soma, Y.Utsuno, N.L.Achouri, H.Baba, F.Browne, D.Calvet, F.Chateau, S.Chen, N.Chiga, M.L.Cortes, A.Delbart, J.-M.Gheller, A.Giganon, C.Hilaire, T.Isobe, T.Kobayashi, Y.Kubota, V.Lapoux, H.N.Liu, T.Motobayashi, I.Murray, H.Otsu, V.Panin, N.Paul, W.Rodriguez, H.Sakurai, M.Sasano, D.Steppenbeck, L.Stuhl, Y.L.Sun, Y.Togano, T.Uesaka, K.Wimmer, K.Yoneda, O.Aktas, T.Aumann, L.X.Chung, F.Flavigny, S.Franchoo, I.Gasparic, R.B.Gerst, J.Gibelin, K.I.Hahn, N.T.Khai, D.Kim, T.Koiwai, Y.Kondo, P.Koseoglou, J.Lee, C.Lehr, T.Lokotko, M.MacCormick, K.Moschner, T.Nakamura, S.Y.Park, D.Rossi, E.Sahin, D.Sohler, P.-A.Soderstrom, S.Takeuchi, H.Tornqvist, V.Vaquero, V.Wagner, S.T.Wang, V.Werner, X.Xu, Y.Yamada, D.Yan, Z.Yang, M.Yasuda, L.Zanetti Onset of collectivity for argon isotopes close to N=32
doi: 10.1103/PhysRevC.109.034312
2023HE16 Eur.Phys.J. C 83, 1092 (2023) Z.He, M.Li, W.Bu, C.Xiao, X.Wei, Y.Yang, Z.Qin, S.He, T.Qiu, P.Ma, C.Lu, L.Duan, B.Hu, Y.Zhang, H.Yang Development of a semi-cylindrical time projection chamber prototype for (3He, t) charge exchange reaction experiment NUCLEAR REACTIONS 13,17C(3He, t), E ∼ 450 MeV; analyzed available data; deduced rough σ estimate.
doi: 10.1140/epjc/s10052-023-12170-x
2023NI07 Phys.Rev.Lett. 131, 022502 (2023) L.Nies, D.Atanasov, M.Athanasakis-Kaklamanakis, M.Au, K.Blaum, J.Dobaczewski, B.S.Hu, J.D.Holt, J.Karthein, I.Kulikov, Y.A.Litvinov, D.Lunney, V.Manea, T.Miyagi, M.Mougeot, L.Schweikhard, A.Schwenk, K.Sieja, F.Wienholtz Isomeric Excitation Energy for 99Inm from Mass Spectrometry Reveals Constant Trend Next to Doubly Magic 100Sn ATOMIC MASSES 99,100,101In; measured TOF; deduced mass excess, excitation energies. The ISOLTRAP mass spectrometer at ISOLDE/CERN. RADIOACTIVITY 99In(IT); measured decay products; deduced excitation energy with small uncertainty, intriguing constancy of the isomer excitation energies in neutron-deficient indium that persists down to the N=50 shell closure, even when all neutrons are removed from the valence shell. Comparison with large-scale shell model, ab initio, and density functional theory calculations.
doi: 10.1103/PhysRevLett.131.022502
2023YA30 Phys.Rev.Lett. 131, 242501 (2023) Z.H.Yang, Y.L.Ye, B.Zhou, H.Baba, R.J.Chen, Y.C.Ge, B.S.Hu, H.Hua, D.X.Jiang, M.Kimura, C.Li, K.A.Li, J.G.Li, Q.T.Li, X.Q.Li, Z.H.Li, J.L.Lou, M.Nishimura, H.Otsu, D.Y.Pang, W.L.Pu, R.Qiao, S.Sakaguchi, H.Sakurai, Y.Satou, Y.Togano, K.Tshoo, H.Wang, S.Wang, K.Wei, J.Xiao, F.R.Xu, X.F.Yang, K.Yoneda, H.B.You, T.Zheng Observation of the Exotic 0+2 Cluster State in 8He NUCLEAR REACTIONS C, 1H(8He, 8He), E=82.3 MeV/nucleon; measured reaction products, En, In. 6,8He; deduced σ(θ), resonant state J, π, large isoscalar monopole transition strength, and the emission of a strongly correlated neutron pair. Comparison with theoretical calculations. RIPS beam line of RIKEN Nishina Center.
doi: 10.1103/PhysRevLett.131.242501
2023ZH48 Phys.Rev. C 108, 064316 (2023) S.Zhang, F.R.Xu, J.G.Li, B.S.Hu, Z.H.Cheng, N.Michel, Y.Z.Ma, Q.Yuan, Y.H.Zhang Ab initio descriptions of A=16 mirror nuclei with resonance and continuum coupling
doi: 10.1103/PhysRevC.108.064316
2022BA15 Phys.Lett. B 829, 137064 (2022) S.W.Bai, A.Koszorus, B.S.Hu, X.F.Yang, J.Billowes, C.L.Binnersley, M.L.Bissell, K.Blaum, P.Campbell, B.Cheal, T.E.Cocolios, R.P.de Groote, C.S.Devlin, K.T.Flanagan, R.F.Garcia Ruiz, H.Heylen, J.D.Holt, A.Kanellakopoulos, J.Kramer, V.Lagaki, B.Maass, S.Malbrunot-Ettenauer, T.Miyagi, R.Neugart, G.Neyens, W.Nortershauser, L.V.Rodriguez, F.Sommer, A.R.Vernon, S.J.Wang, X.B.Wang, S.G.Wilkins, Z.Y.Xu, C.X.Yuan Electromagnetic moments of scandium isotopes and N=28 isotones in the distinctive 0f7/2 orbit NUCLEAR MOMENTS 41,43,45,46,47,49Sc; measured frequencies; deduced hfs constants, electromagnetic dipole and quadrupole moments. Comparison with theoretical calculations. Two collinear laser spectroscopy (CLS) setups, COLLAPS and CRIS at ISOLDE-CERN.
doi: 10.1016/j.physletb.2022.137064
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
2022HU04 Phys.Rev.Lett. 128, 072502 (2022) B.S.Hu, J.Padua-Arguelles, S.Leutheusser, T.Miyagi, S.R.Stroberg, J.D.Holt Ab Initio Structure Factors for Spin-Dependent Dark Matter Direct Detection
doi: 10.1103/PhysRevLett.128.072502
2022HU13 Nat.Phys. 610, 1196 (2022) B.Hu, W.Jiang, T.Miyagi, Z.Sun, A.Ekstrom, C.Forssen, G.Hagen, J.D.Holt, T.Papenbrock, S.R.Stroberg, I.Vernon Ab initio predictions link the neutron skin of 208Pb to nuclear forces NUCLEAR STRUCTURE 208Pb; analyzed available data; calculated neutron skin using Ab initio, bulk properties.
doi: 10.1038/s41567-022-01715-8
2022KA35 Phys.Rev.Lett. 129, 142502 (2022) S.Kaur, R.Kanungo, W.Horiuchi, G.Hagen, J.D.Holt, B.S.Hu, T.Miyagi, T.Suzuki, F.Ameil, J.Atkinson, Y.Ayyad, S.Bagchi, D.Cortina-Gil, I.Dillmann, A.Estrade, A.Evdokimov, F.Farinon, H.Geissel, G.Guastalla, R.Janik, R.Knobel, J.Kurcewicz, Y.A.Litvinov, M.Marta, M.Mostazo, I.Mukha, C.Nociforo, H.J.Ong, T.Otsuka, S.Pietri, A.Prochazka, C.Scheidenberger, B.Sitar, P.Strmen, M.Takechi, J.Tanaka, I.Tanihata, S.Terashima, J.Vargas, H.Weick, J.S.Winfield Proton Distribution Radii of 16-24O: Signatures of New Shell Closures and Neutron Skin NUCLEAR REACTIONS 12C(16O, X), (18O, X), (19O, X), (20O, X), (21O, X), (22O, X), (23O, X), (24O, X), E<1 GeV/nucleon; measured reaction products. 16,18,20,21,22,23,24O; deduced charge changing σ, root mean square proton and matter radii, neutron skin thickness, shell closure. Comparison with with ab initio calculations employing the chiral NNLO sat interaction, shell model predictions. The fragment separator FRS at GSI.
doi: 10.1103/PhysRevLett.129.142502
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
2022ZH57 Phys.Lett. B 827, 136958 (2022) S.Zhang, Y.Z.Ma, J.G.Li, B.S.Hu, Q.Yuan, Z.H.Cheng, F.R.Xu The roles of three-nucleon force and continuum coupling in mirror symmetry breaking of oxygen mass region NUCLEAR STRUCTURE 17,18,19,20,21,22,23,24,25,26,27,28O; calculated g.s. energies, energy levels, J, π, using the complex-energy ab initio Gamow shell model with a core. Comparison with available data.
doi: 10.1016/j.physletb.2022.136958
2021DA11 Phys.Rev. C 103, 064327 (2021) B.Dai, B.S.Hu, Y.Z.Ma, J.G.Li, S.M.Wang, C.W.Johnson, F.R.Xu Tensor force role in β decays analyzed within the Gogny-interaction shell model NUCLEAR STRUCTURE 10,11,12,13,14,15C; calculated levels, J, π, ground-state energies. 10,11,12,13,14,15N; calculated ground-state energies. Shell-model calculations with the effective interaction derived from D1S Gogny interaction with and without the tensor force. 15,17O; calculated spectra using the Single-particle energies (SPEs) and two-body matrix elements (TBMEs) from the D1S interaction. Comparison with theoretical calculations using WBP interaction, and with experimental data. RADIOACTIVITY 10,11C, 12,13N(β+); 14,15C(β-); calculated β spectra, B(GT) using shell model within the p-sd space and the D1S Gogny interaction with different components of tensor force. Comparison with theoretical calculations using WBP interaction, and with experimental data. Relevance to anomalously long half-life of 14C decay, and role of tensor force, cross-shell mixing, and three-body forces in β decay.
doi: 10.1103/PhysRevC.103.064327
2020HU07 Phys.Rev. C 101, 044309 (2020) B.S.Hu, Q.Wu, Q.Yuan, Y.Z.Ma, X.Q.Yan, F.R.Xu Nuclear multipole responses from chiral effective field theory interactions NUCLEAR STRUCTURE 56,68,78Ni; calculated isoscalar monopole (ISGMR), isoscalar quadrupole (ISGQR), isoscalar dipole (ISGDR), and isovector dipole (IVGDR) strength distributions and ground-state energies, excitation energies of isovector pygmy dipole resonances (PDR) and giant dipole resonances (GDR). 4He, 16O, 40,48Ca; calculated isovector dipole (1-) strength distributions and isovector dipole polarizabilities. Hartree-Fock random-phase approximation (HF-RPA), and chiral effective field theory with three-nucleon chiral force. Comparison with experimental values.
doi: 10.1103/PhysRevC.101.044309
2020LI35 Phys.Rev. C 102, 034302 (2020) J.G.Li, B.S.Hu, Q.Wu, Y.Gao, S.J.Dai, F.R.Xu Neutron-rich calcium isotopes within realistic Gamow shell model calculations with continuum coupling NUCLEAR STRUCTURE 49,50,51,52,53,54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72Ca; calculated binding energies, S(n), S(2n), neutron effective single-particle energies (ESPE), energies of the first 2+ states in even-A nuclei. 51,52,53,54,55,56,57,58Ca; calculated levels, J, π. 51,53,55,57Ca; calculated energies and widths of the first 5/2+ and 9/2+ resonance states. Realistic Gamow shell model based on high-precision CD-Bonn potential. Comparison with experimental data. 57Ca; predicted as the heaviest odd-A bound Ca isotope. 70Ca; predicted as the dripline nucleus. Calculations support shell closures at 52Ca, 54Ca, and possibly at 70Ca, and a weakening of shell closure at 60Ca.
doi: 10.1103/PhysRevC.102.034302
2020MA33 Phys.Lett. B 808, 135673 (2020) Y.Z.Ma, F.R.Xu, N.Michel, S.Zhang, J.G.Li, B.S.Hu, L.Coraggio, N.Itaco, A.Gargano Continuum and three-nucleon force in Borromean system: The 17Ne case NUCLEAR STRUCTURE 17Ne; analyzed available data; calculated energy levels, J, π, proton-proton and proton-neutron correlation densities.
doi: 10.1016/j.physletb.2020.135673
2019CH56 J.Phys.(London) G46, 125106 (2019) X.Y.Chen, Z.Zhou, W.G.Jiang, B.S.Hu, F.R.Xu p-shell hypernuclear energy spectra using the Gogny-interaction shell model NUCLEAR STRUCTURE 6,7He, 7,8,9Li, 9,10Be, 9,10,11,12B, 11,12,13C, 14,15N, 15,16O; calculated regular and hypernuclei energy levels, J, π, B(E2) within the shell model based on the nucleon-nucleon (NN)and hyperon-nucleon interactions. Comparison with available data.
doi: 10.1088/1361-6471/ab4d94
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
2019LI50 Phys.Rev. C 100, 054313 (2019) J.G.Li, N.Michel, B.S.Hu, W.Zuo, F.R.Xu Ab initio no-core Gamow shell-model calculations of multineutron systems NUCLEAR STRUCTURE 3,4n; calculated resonances, energies and widths using the ab-initio no-core Gamow shell model based on nuclear chiral effective field theory interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.054313
2019WU12 J.Phys.(London) G46, 055104 (2019) Perturbation calculations of nucleon-nucleon effective interactions in the Hartree-Fock basis NUCLEAR STRUCTURE 16,18O, 18F, 18Ne; calculated binding energies, energy levels, J, π. Comparison with experimental data.
doi: 10.1088/1361-6471/ab0ef1
2019ZH41 Yuan.Wul.Ping. 36, 151 (2019); Nucl.Phys.Rev. 36, 151 (2019) Nuclear scattering experiment based on the Polarized Helium-3 Target NUCLEAR REACTIONS 3He(p, p), E not given; analyzed available data; deduced possibility to further verify the 3-body-force part of the chiral effective theory.
doi: 10.11804/NuclPhysRev.36.02.151
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
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
2017HU20 Chin.Phys.C 41, 104101 (2017) Ab initio many-body perturbation theory and no-core shell model NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated binding and ground-state energies, rms radii using no-core shell model (NCSM) and many-body perturbation theory (MBPT).
doi: 10.1088/1674-1137/41/10/104101
2017LA03 Phys.Rev. C 95, 015203 (2017) J.Landay, M.Doring, C.Fernandez-Ramirez, B.Hu, R.Molina Model selection for pion photoproduction NUCLEAR REACTIONS 1H(γ, π0)1H, E=1074-1119 MeV; analyzed experimental data for differential σ(θ), beam asymmetries, and polarized differential σ(θ) using the least absolute shrinkage and selection operator (LASSO) in combination with criteria from information theory and K-fold cross validation.
doi: 10.1103/PhysRevC.95.015203
2017MA58 Eur.Phys.J. A 53, 177 (2017) M.Mai, B.Hu, M.Doring, A.Pilloni, A.Szczepaniak Three-body unitarity with isobars revisited
doi: 10.1140/epja/i2017-12368-4
2017PU05 Phys.Rev. C 96, 055203 (2017); Erratum Phys.Rev. C 98, 019907 (2018) A.J.R.Puckett, E.J.Brash, M.K.Jones, W.Luo, M.Meziane, L.Pentchev, C.F.Perdrisat, V.Punjabi, F.R.Wesselmann, A.Afanasev, A.Ahmidouch, I.Albayrak, K.A.Aniol, J.Arrington, A.Asaturyan, H.Baghdasaryan, F.Benmokhtar, W.Bertozzi, L.Bimbot, P.Bosted, W.Boeglin, C.Butuceanu, P.Carter, S.Chernenko, M.E.Christy, M.Commisso, J.C.Cornejo, S.Covrig, S.Danagoulian, A.Daniel, A.Davidenko, D.Day, S.Dhamija, D.Dutta, R.Ent, S.Frullani, H.Fenker, E.Frlez, F.Garibaldi, D.Gaskell, S.Gilad, R.Gilman, Y.Goncharenko, K.Hafidi, D.Hamilton, D.W.Higinbotham, W.Hinton, T.Horn, B.Hu, J.Huang, G.M.Huber, E.Jensen, C.Keppel, M.Khandaker, P.King, D.Kirillov, M.Kohl, V.Kravtsov, G.Kumbartzki, Y.Li, V.Mamyan, D.J.Margaziotis, A.Marsh, Y.Matulenko, J.Maxwell, G.Mbianda, D.Meekins, Y.Melnik, J.Miller, A.Mkrtchyan, H.Mkrtchyan, B.Moffit, O.Moreno, J.Mulholland, A.Narayan, S.Nedev, Nuruzzaman, E.Piasetzky, W.Pierce, N.M.Piskunov, Y.Prok, R.D.Ransome, D.S.Razin, P.Reimer, J.Reinhold, O.Rondon, M.Shabestari, A.Shahinyan, K.Shestermanov, S.Sirca, I.Sitnik, L.Smykov, G.Smith, L.Solovyev, P.Solvignon, R.Subedi, E.Tomasi-Gustafsson, A.Vasiliev, M.Veilleux, B.B.Wojtsekhowski, S.Wood, Z.Ye, Y.Zanevsky, X.Zhang, Y.Zhang, X.Zheng, L.Zhu Polarization transfer observables in elastic electron-proton scattering at Q2 = 2.5, 5.2, 6.8, and 8.5 GeV2 NUCLEAR REACTIONS 1H(polarized e, e)p, E<5.717 GeV; measured elastically scattered electrons by a large-solid-angle electromagnetic calorimeter (BigCal) in coincidence with the scattered protons, polarization of recoiling protons by focal plane polarimeter (FPP), proton angular distributions and azimuthal asymmetries, focal-plane helicity difference/sum ratio asymmetry, analyzing powers at JLab's Continuous Electron Beam Accelerator Facility (CEBAF); deduced ratio of the proton's electric and magnetic form factors μpGpE/GpM. Comparison with other experimental data, and with theoretical predictions.
doi: 10.1103/PhysRevC.96.055203
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
2015HA09 Nucl.Phys. A936, 17 (2015) R.Han, R.Wada, Z.Chen, Y.Nie, X.Liu, S.Zhang, P.Ren, B.Jia, G.Tian, F.Luo, W.Lin, J.Liu, F.Shi, M.Huang, X.Ruan, J.Ren, Z.Zhou, H.Huang, J.Bao, K.Zhang, B.Hu Fast neutron scattering on Gallium target at 14.8 MeV NUCLEAR REACTIONS 69,71Ga(n, n), (n, n'), E≈14.8 MeV; measured En, In(θ); deduced σ, σ(θ). 69,71Ga(n, n), (n, n'), (n, 2n), (n, np), (n, nα), E=0-15 MeV; calculated σ, σ(θ), using TALYS and MCNP. Compared with experimental data and databases.
doi: 10.1016/j.nuclphysa.2015.01.004
2012BA35 J.Phys.(London) G39, 095103 (2012) X.J.Bao, H.F.Zhang, B.S.Hu, G.Royer, J.Q.Li Half-lives of cluster radioactivity with a generalized liquid-drop model RADIOACTIVITY 221Fr, 221,222,223,224,226Ra, 225Ac, 226Th(14C), 226Th(18O), 228Th(20O), 230Th(24Ne), 232Th(26Ne), 231Pa(24Ne), (23F), 230U(22Ne), (24Ne), 232U(28Mg), (24Ne), 233U(24Ne), (25Ne), (28Mg), 234U(24Ne), (26Ne), (28Mg), 235U(24Ne), (25Ne), (28Mg), 236U, 247Np(30Mg), 236Pu(28Mg), 238Pu(28Mg), (30Mg), (32Si), 220Rn(12C), 221Rn(15N), 222Rn(18O), 223Ra(18O), 226Ra(20O), 225Ac(18O), 224Th(15N), 224Th(24Ne), 226Th(15N), 226,228Th(24Ne), 229Th(21O), (24Ne), 231Pa(27Na), 232Pa(25Ne), (28Mg), 230U(20O), (24Ne), (32Si), 232U(28Mg), 233,234U(27Na), 225Np(12C), (16O), 227Np(16O), (18O), 231Np(20O), 233Np(22Ne), (25Ne), 234Np(28Mg), 235Np(29Mg), 236Np(29Mg), 237Np(32Si), 234Pu(27Na), (29Al), 236Pu(24Ne), (29Al), 237Pu(29Mg), (32Si), 237Am(28Mg), (32Si), 238Am(29Mg), (33Si), 239Am(32Si), (34Si), 240Am(34Si), 241Am(34Si), 238Cm(32Si), 240Cm(30Mg), (34Si), 242Cm(32Si), 243Cm(34Si), 242Cf(32Si), (34Si), 244Cf(34Si), 246Cf(38S), 249Cf(46Ar), (50Ca), 250,252,253,254,255,256,257,258No(48Ca), 258Rf(49Ca), (51Ti), (53Ti); calculated T1/2 for cluster radioactivity. WKB barrier-penetrating probabilities, generalized liquid drop model, comparison with available data.
doi: 10.1088/0954-3899/39/9/095103
2010FU13 Int.J.Mod.Phys. E19, 2480 (2010) Y.Fujii, A.Chiba, D.Doi, T.Gogami, O.Hashimoto, H.Kanda, M.Kaneta, D.Kawama, K.Maeda, T.Maruta, A.Matsumura, S.Nagao, S.N.Nakamura, A.Shichijo, H.Tamura, N.Taniya, T.Yamamoto, K.Yokota, S.Kato, Y.Sato, T.Takahashi, H.Noumi, T.Motoba, E.Hiyama, I.Albayrak, O.Ates, C.Chen, M.Christy, C.Keppel, M.Kohl, Y.Li, A.Liyanage, L.Tang, T.Walton, Z.Ye, L.Yuan, L.Zhu, P.Baturin, W.Boeglin, S.Dhamija, P.Markowitz, B.Raue, J.Reinhold, Ed.V.Hungerford, R.Ent, H.Fenker, D.Gaskell, T.Horn, M.Jones, G.Smith, W.Vulcan, S.A.Wood, C.Johnston, N.Simicevic, S.Wells, C.Samanta, B.Hu, J.Shen, W.Wang, X.Zhang, Y.Zhang, J.Feng, Y.Fu, J.Zhou, S.Zhou, Y.Jiang, H.Lu, X.Yan, Y.Ye, L.Gan, A.Ahmidouch, S.Danagoulian, A.Gasparian, M.Elaasar, F.R.Wesselmann, A.Asaturyan, A.Margaryan, A.Mkrtchyan, H.Mkrtchyan, V.Tadevosyan, D.Androic, M.Furic, T.Petkovic, T.Seva, G.Niculescu, I.Niculescu, V.M.Rodriguez Lopez, E.Cisbani, F.Cusanno, F.Garibaldi, G.M.Uuciuoli, R.De Leo, S.Maronne Hypernuclear spectroscopy with electron beam at JLab HALL C NUCLEAR REACTIONS 7Li, 12C, 28Si(E, EK+)7He/12B/28Al, E=1.2 GeV; measured reaction products; deduced hypernuclear spectroscopy, missing mass spectrum.
doi: 10.1142/S0218301310016983
2010PU02 Phys.Rev.Lett. 104, 242301 (2010) A.J.R.Puckett, E.J.Brash, M.K.Jones, W.Luo, M.Meziane, L.Pentchev, C.F.Perdrisat, V.Punjabi, F.R.Wesselmann, A.Ahmidouch, I.Albayrak, K.A.Aniol, J.Arrington, A.Asaturyan, H.Baghdasaryan, F.Benmokhtar, W.Bertozzi, L.Bimbot, P.Bosted, W.Boeglin, C.Butuceanu, P.Carter, S.Chernenko, E.Christy, M.Commisso, J.C.Cornejo, S.Covrig, S.Danagoulian, A.Daniel, A.Davidenko, D.Day, S.Dhamija, D.Dutta, R.Ent, S.Frullani, H.Fenker, E.Frlez, F.Garibaldi, D.Gaskell, S.Gilad, R.Gilman, Y.Goncharenko, K.Hafidi, D.Hamilton, D.W.Higinbotham, W.Hinton, T.Horn, B.Hu, J.Huang, G.M.Huber, E.Jensen, C.Keppel, M.Khandaker, P.King, D.Kirillov, M.Kohl, V.Kravtsov, G.Kumbartzki, Y.Li, V.Mamyan, D.J.Margaziotis, A.Marsh, Y.Matulenko, J.Maxwell, G.Mbianda, D.Meekins, Y.Melnik, J.Miller, A.Mkrtchyan, H.Mkrtchyan, B.Moffit, O.Moreno, J.Mulholland, A.Narayan, S.Nedev, Nuruzzaman, E.Piasetzky, W.Pierce, N.M.Piskunov, Y.Prok, R.D.Ransome, D.S.Razin, P.Reimer, J.Reinhold, O.Rondon, M.Shabestari, A.Shahinyan, K.Shestermanov, S.Sirca, I.Sitnik, L.Smykov, G.Smith, L.Solovyev, P.Solvignon, R.Subedi, E.Tomasi-Gustafsson, M.Veilleux, B.B.Wojtsekhowski, S.Wood, Z.Ye, Y.Zanevsky, X.Zhang, Y.Zhang, X.Zheng, L.Zhu Recoil Polarization Measurements of the Proton Electromagnetic Form Factor Ratio to Q2=8.5 GeV2
doi: 10.1103/PhysRevLett.104.242301
2008HA14 Nucl.Phys. A804, 125 (2008) O.Hashimoto, S.N.Nakamura, A.Acha, A.Ahmidouch, D.Androic, A.Asaturyan, R.Asaturyan, O.K.Baker, P.Baturin, F.Benmokhtar, P.Bosted, R.Carlini, X.Chen, M.Christy, L.Cole, S.Danagoulian, A.Daniel, V.Dharmawardane, K.Egiyan, M.Elaasar, R.Ent, H.Fenker, Y.Fujii, M.Furic, L.Gan, D.Gaskell, A.Gasparian, E.F.Gibson, P.Gueye, R.Halkyard, D.Honda, T.Horn, B.Hu, S.Hu, Ed.V.Hungerford, M.Ispiryan, K.Johnston, M.Jones, N.Kalantarians, M.Kaneta, F.Kato, S.Kato, D.Kawama, C.Keppel, Y.Li, W.Luo, D.Mack, A.Margaryan, G.Marikyan, N.Maruyama, A.Matsumura, T.Miyoshi, A.Mkrtchyan, H.Mkrtchyan, T.Navasardyan, G.Niculescu, M.-I.Niculescu, H.Nomura, K.Nonaka, A.Ohtani, Y.Okayasu, P.Pamela, N.Perez, T.Petkovic, S.Randeniya, J.Reinhold, R.Rivera, J.Roche, V.M.Rodriguez, Y.Sato, T.Seva, L.Tang, N.Simicevic, G.Smith, M.Sumihama, Y.Song, V.Tadevosyan, T.Takahashi, H.Tamura, V.Tvaskis, W.Vulcan, B.Wang, S.Wells, S.Wood, C.Yan, L.Yuan, S.Zamkochian Hypernuclear spectroscopy program at JLab Hall C2008.01.029 NUCLEAR REACTIONS 1H, 12C, 28Si(e, e'K+), E=1.8 GeV; measured hypernuclei missing mass spectra using the Tilt method.
doi: 10.1016/j.nuclphysa.2008.01.029
2006HU09 Phys.Rev. C 73, 064004 (2006) B.Hu, M.K.Jones, P.E.Ulmer, H.Arenhovel, O.K.Baker, W.Bertozzi, E.J.Brash, J.Calarco, J.-P.Chen, E.Chudakov, A.Cochran, S.Dumalski, R.Ent, J.M.Finn, F.Garibaldi, S.Gilad, R.Gilman, C.Glashausser, J.Gomez, V.Gorbenko, J.-O.Hansen, J.Hovdebo, C.W.de Jager, S.Jeschonnek, X.Jiang, C.Keppel, A.Klein, A.Kozlov, S.Kuhn, G.Kumbartzki, M.Kuss, J.J.LeRose, M.Liang, N.Liyanage, G.J.Lolos, P.E.C.Markowitz, D.Meekins, R.Michaels, J.Mitchell, Z.Papandreou, C.F.Perdrisat, V.Punjabi, R.Roche, D.Rowntree, A.Saha, S.Strauch, L.Todor, G.Urciuoli, L.B.Weinstein, K.Wijesooriya, B.B.Wojtsekhowski, R.Woo Polarization transfer in the 2H(e(pol), e'p(pol))n reaction up to Q2 = 1.61 (GeV/c)2 NUCLEAR REACTIONS 1,2H(polarized e, e'p), E=1.669 GeV; measured recoil proton polarization vs momentum transfer, missing momentum; deduced form factor ratios. Comparison with model predictions.
doi: 10.1103/PhysRevC.73.064004
2006MA08 Nucl.Phys. A764, 261 (2006) G.MacLachlan, A.Aghalaryan, A.Ahmidouch, B.D.Anderson, R.Asaturyan, O.Baker, A.R.Baldwin, D.Barkhuff, H.Breuer, R.Carlini, E.Christy, S.Churchwell, L.Cole, E.Crouse, S.Danagoulian, D.Day, T.Eden, M.Elaasar, R.Ent, M.Farkhondeh, H.Fenker, J.M.Finn, L.Gan, K.Garrow, P.Gueye, C.R.Howell, B.Hu, M.K.Jones, J.J.Kelly, C.Keppel, M.Khandaker, W.-Y.Kim, S.Kowalski, A.Lai, A.Lung, D.Mack, R.Madey, D.M.Manley, P.Markowitz, J.Mitchell, H.Mkrtchyan, A.K.Opper, B.Plaster, C.Perdrisat, V.Punjabi, B.Raue, T.Reichelt, J.Reinhold, J.Roche, Y.Sato, N.Savvinov, A.Yu.Semenov, I.A.Semenova, W.Seo, N.Simicevic, G.Smith, S.Taylor, S.Stepanyan, V.Tadevosyan, S.Tajima, L.Tang, W.Tireman, P.E.Ulmer, W.Vulcan, J.W.Watson, S.P.Wells, F.Wesselmann, S.Wood, C.Yan, C.Yan, S.Yang, L.Yuan, W.-M.Zhang, H.Zhu, X.Zhu The ratio of proton electromagnetic form factors via recoil polarimetry at Q2=1.13 (GeV/c)2 NUCLEAR REACTIONS 1H(polarized e, e'p), E=2329 MeV; measured recoil proton spectra, polarization. 1H deduced ratio of electromagnetic form factors.
doi: 10.1016/j.nuclphysa.2005.09.012
2003MA36 Eur.Phys.J. A 17, 323 (2003) R.Madey, A.Yu.Semenov, S.Taylor, A.Aghalaryan, E.Crouse, G.MacLachlan, B.Plaster, S.Tajima, W.Tireman, C.Yan, A.Ahmidouch, B.D.Anderson, H.Arenhovel, R.Asaturyan, O.Baker, A.R.Baldwin, H.Breuer, R.Carlini, E.Christy, S.Churchwell, L.Cole, S.Danagoulian, D.Day, M.Elaasar, R.Ent, M.Farkhondeh, H.Fenker, J.M.Finn, L.Gan, K.Garrow, P.Gueye, C.Howell, B.Hu, M.K.Jones, J.J.Kelly, C.Keppel, M.Khandaker, W.-Y.Kim, S.Kowalski, A.Lung, D.Mack, D.M.Manley, P.Markowitz, J.Mitchell, H.Mkrtchyan, A.Opper, C.Perdrisat, V.Punjabi, B.Raue, T.Reichelt, J.Reinhold, J.Roche, Y.Sato, I.A.Semenova, W.Seo, N.Simicevic, G.Smith, S.Stepanyan, V.Tadevosyan, L.Tang, P.Ulmer, W.Vulcan, J.W.Watson, S.Wells, F.Wesselmann, S.Wood, C.Yan, S.Yang, L.Yuan, W.-M.Zhang, H.Zhu, X.Zhu Neutron electric form factor up to Q2 = 1.47 (GeV/c)2 NUCLEAR REACTIONS 2H(polarized e, e'n), E=0.844-3.395 GeV; measured neutron spectra, polarization. 1n deduced form factors.
doi: 10.1140/epja/i2002-10169-6
2003ST13 Phys.Rev.Lett. 91, 052301 (2003) S.Strauch, S.Dieterich, K.A.Aniol, J.R.M.Annand, O.K.Baker, W.Bertozzi, M.Boswell, E.J.Brash, Z.Chai, J.-P.Chen, M.E.Christy, E.Chudakov, A.Cochran, R.De Leo, R.Ent, M.B.Epstein, J.M.Finn, K.G.Fissum, T.A.Forest, S.Frullani, F.Garibaldi, A.Gasparian, O.Gayou, S.Gilad, R.Gilman, C.Glashausser, J.Gomez, V.Gorbenko, P.L.J.Gueye, J.O.Hansen, D.W.Higinbotham, B.Hu, C.E.Hyde-Wright, D.G.Ireland, C.Jackson, C.W.de Jager, X.Jiang, C.Jones, M.K.Jones, J.D.Kellie, J.J.Kelly, C.E.Keppel, G.Kumbartzki, M.Kuss, J.J.LeRose, K.Livingston, N.Liyanage, S.Malov, D.J.Margaziotis, D.Meekins, R.Michaels, J.H.Mitchell, S.K.Nanda, J.Nappa, C.F.Perdrisat, V.A.Punjabi, R.D.Ransome, R.Roche, G.Rosner, M.Rvachev, F.Sabatie, A.Saha, A.Sarty, J.M.Udias, P.E.Ulmer, G.M.Urciuoli, J.F.J.van den Brand, J.R.Vignote, D.P.Watts, L.B.Weinstein, K.Wijesooriya, B.Wojtsekhowski Polarization Transfer in the 4He(e(pol), e'p(pol))3H Reaction up to Q2=2.6 (GeV/c)2 NUCLEAR REACTIONS 4He(polarized e, e'p), E=3400, 4237, 4239 MeV; measured polarization transfer; deduced medium modification effects. Comparison with model predictions.
doi: 10.1103/PhysRevLett.91.052301
2002GU27 Phys.Rev. C 66, 054312 (2002) Finite size effect on the strength function in a random matrix analysis
doi: 10.1103/PhysRevC.66.054312
1998HU13 Eur.Phys.J. A 2, 143 (1998) B.Hu, P.P.Zarubin, U.U.Juravlev Isomeric Cross-Section Ratios Resulted from Reaction (p, n) on Targets 100Ru and 104, 106, 110Pd NUCLEAR REACTIONS 100Ru, 104,106,110Pd(p, n), E=6-9 MeV; measured isomer yield ratios. Comparison with statistical model calculations.
doi: 10.1007/s100500050102
1998HU22 J.Phys.(London) G24, 2261 (1998) B.Hu, U.U.Juravlev, P.P.Zarubin Isobaric Analogue Resonance Observed in Isomeric Ratios Resulting from the Reaction (p, n) on Targets 95Mo and 104Ru NUCLEAR REACTIONS 95Mo(p, n), E=5.6-7.3 MeV; 104Ru(p, n), E=6.4-7.0 MeV; measured residuals isomeric ratios; deduced enhancement due to IAR. Activation technique. Comparison with statistical calculations.
doi: 10.1088/0954-3899/24/12/011
1998HU25 Bull.Rus.Acad.Sci.Phys. 62, 823 (1998) B.Hu, P.P.Zarubin, Yu.Yu.Zhuravlev Excitation Function for (pn) and (pp0) Reactions on the 104Ru Nucleus NUCLEAR REACTIONS 104Ru(p, n), (p, p), E=6.4-7.0 MeV; measured total σ, isomeric ratios. Comparisons with optical model, statistical theory. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0839. 1995HU15 Chin.Phys.Lett. 12, 265 (1995) Application of 14N(d, α)12C Nuclear Reaction to the Concentration Analysis of Nitrogen in Iron Meteorites NUCLEAR REACTIONS 14N(d, α), E=2 MeV; measured Eα, Iα; deduced nitrogen content in iron meteorites.
1989HU13 Nucl.Data Sheets 58, 677 (1989) J.Huo, D.Hu, H.Sun, J.You, B.Hu Nuclear Data Sheets for A = 52 COMPILATION 52K, 52Ca, 52Sc, 52Ti, 52V, 52Cr, 52Mn, 52Fe; compiled, evaluated structure data.
1987HU04 Nucl.Data Sheets 51, 1 (1987) Huo Junde, Hu Dailing, Zhou Chunmei, Han Xiaoling, Hu Baohua, Wu Yaodong Nuclear Data Sheets for A = 56 NUCLEAR STRUCTURE 56Cr, 56Mn, 56Fe, 56Co, 56Ni; compiled, evaluated structure data.
1983LI19 Chin.J.Nucl.Phys. 5, 312 (1983) Liu Yunzuo, Zhou Jiewen, Wang Changru, Hu Dailing, Hu Baohua, Huo Junde A Study on the Decay Scheme of 147Nd RADIOACTIVITY 147Nd(β-); measured Eγ, Iγ; deduced log ft. 147Pm deduced levels, Iβ, γ-branching.
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