NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = Y.Jin Found 31 matches. 2022GI04 Phys.Rev. C 105, 044321 (2022) S.A.Gillespie, K.W.Brown, R.J.Charity, L.G.Sobotka, A.K.Anthony, J.Barney, A.Bonaccorso, B.A.Brown, J.Crosby, D.Dell'Aquila, J.Elson, J.Estee, A.Gade, M.Ghazali, G.Jhang, Y.Jin, B.Longfellow, W.G.Lynch, J.Pereira, M.Spieker, S.Sweany, F.C.E.Teh, A.Thomas, M.B.Tsang, C.Y.Tsang, D.Weisshaar, H.Y.Wu, K.Zhu Proton decay spectroscopy of 28S and 30Cl NUCLEAR REACTIONS 9Be(29S, n), (31Ar, p), E=150 MeV/nucleon; measured reaction products, Ep, Ip, Eγ, Iγ, (particle)p-coin, pγ-coin; deduced invariant mass, momentum distribution. Setup consisting of S800 spectrograph, Si-CsI(Tl) DSSD array of 128 concentric rings and 128 annular sectors, CAESAR CsI(Na) photon detection array, BC-400-type scintillation fiber detector at A1900 fragment separator (NSCL). RADIOACTIVITY 28S(p), (2p) [from 9Be(29S, n), E=150 MeV/nucleon]; 30Cl(p), (2p) [from 9Be(29S, n), E=150 MeV/nucleon]; measured Ep, Ip, Eγ, Iγ, pγ-coin; deduced total decay kinetic energy, decay energy spectrum. 30Cl; deduced levels, J, π, S(p). 28S; deduced levels, J, π, spectroscopic factors. Comparison to previous experimental results and shell model calculations.
doi: 10.1103/PhysRevC.105.044321
2022LU01 Phys.Rev. C 105, 024305 (2022) D.W.Luo, C.Xu, Y.K.Wang, Z.H.Li, R.A.Bark, S.Q.Zhang, H.Hua, S.Y.Wang, J.Peng, X.Q.Li, H.Y.Wu, X.Wang, C.G.Wu, Q.T.Li, J.Lin, Y.Jin, W.Z.Xu, L.Mu, J.Meng, F.R.Xu, Y.L.Ye, D.X.Jiang, P.Jones, E.A.Lawrie, P.Papka, M.F.Nkalanga, T.D.Bucher, M.V.Chisapi, L.Msebi, S.Jongile, S.Ntshangase, B.R.Zikhali, S.H.Mthembu, T.Seakamela, M.A.Sithole, O.Shirihda, A.A.Aava, L.Mdletshe, K.L.Malatji, S.Mhlongo, L.Makhathini Collective structures in 62Cu NUCLEAR REACTIONS 54Cr(12C, 3np), E=67 MeV; measured Eγ, Iγ, γ(θ), γγ-coin. 62Cu; deduced levels, J, π, high-spin levels, B(M1)/B(E2), configurations, γγ(linear polarization). Comparison with calculations using the self-consistent tilted axis cranking covariant density functional theory (TAC-C DFT). Comparison with level structures in 60,64Ca. AFRODITE array at the iThemba LABS accelerator facility.
doi: 10.1103/PhysRevC.105.024305
2021JI15 Phys.Rev.Lett. 127, 262502 (2021) Y.Jin, C.Y.Niu, K.W.Brown, Z.H.Li, H.Hua, A.K.Anthony, J.Barney, R.J.Charity, J.Crosby, D.Dell'Aquila, J.M.Elson, J.Estee, M.Ghazali, G.Jhang, J.G.Li, W.G.Lynch, N.Michel, L.G.Sobotka, S.Sweany, F.C.E.Teh, A.Thomas, C.Y.Tsang, M.B.Tsang, S.M.Wang, H.Y.Wu, C.X.Yuan, K.Zhu First Observation of the Four-Proton Unbound Nucleus 18Mg RADIOACTIVITY 18Mg(14O), (2p), (4p) [from 9Be(20Mg, X)18Mg, E=170 MeV/nucleon]; measured decay products, Ep, Ip, 18Mg, 16Ne; deduced decay energy spectra, level scheme, J, π, resonance parameters. Comparison with the Gamow shell model (GSM) calculations.
doi: 10.1103/PhysRevLett.127.262502
2021LI36 Nucl.Phys. A1014, 122225 (2021) T.X.Li, C.B.Li, Y.Zheng, X.G.Wu, J.Zhong, B.J.Zhu, Q.W.Fan, Y.X.Gao, Y.J.Jin, G.S.Li, L.H.Zhu Lifetime measurements and the structure of some negative-parity states in 134Ce NUCLEAR REACTIONS 122Sn(16O, 4n), E=76 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, J, π, B(Eλ), lifetimes of negative-parity states. Comparison with cranked Nilsson-Strutinsky Bogoliubov (CNSB) model. Recoil-distance Doppler-shift technique.
doi: 10.1016/j.nuclphysa.2021.122225
2021ZH66 Nucl. Sci. Tech. 32, 107 (2021) J.Zhong, X.-G.Wu, S.-P.Hu, Y.-J.Ma, Y.Zheng, C.-B.Li, G.-S.Li, B.-J.Zhu, T.-X.Li, Y.-J.Jin, Y.-X.Gao, Q.-W.Fan, K.-Y.Ma, D.Yang, H.-B.Sun, H.-G.Zhao, L.Gan, Q.Luo, Z.X.Wu Lifetime measurements in 138Nd NUCLEAR REACTIONS 123Sb(19F, 4n), E=87 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and relative intensities, J, π, partial level scheme, level T1/2, B(E2). Comparison with Grodzins systematics and available data. The recoil distance Doppler shift technique in combination with the differential decay curve method. The HI-13 tandem accelerator of the China Institute of Atomic Energy (CIAE) in Beijing.
doi: 10.1007/s41365-021-00953-4
2020JI05 Eur.Phys.J. A 56, 135 (2020) Y.Jin, X.R.Zhou, Y.-Y.Cheng, H.-J.Schulze Study of Ξ- hypernuclei in the Skyrme-Hartree-Fock approach
doi: 10.1140/epja/s10050-020-00143-7
2020JI08 Phys.Rev. C 102, 015201 (2020) Y.Jin, S.-Y.Li, Y.-R.Liu, Z.-X.Meng, Z.-G.Si, T.Yao Exclusive production ratio of neutral to charged kaon pair in e+e- annihilation continuum via a relativistic quark model
doi: 10.1103/PhysRevC.102.015201
2020KA09 Nucl.Data Sheets 163, 109 (2020) T.Kawano, Y.S.Cho, P.Dimitriou, D.Filipescu, N.Iwamoto, V.Plujko, X.Tao, H.Utsunomiya, V.Varlamov, R.Xu, R.Capote, I.Gheorghe, O.Gorbachenko, Y.L.Jin, T.Renstrom, M.Sin, K.Stopani, Y.Tian, G.M.Tveten, J.M.Wang, T.Belgya, R.Firestone, S.Goriely, J.Kopecky, M.Krticka, R.Schwengner, S.Siem, M.Wiedeking IAEA Photonuclear Data Library 2019
doi: 10.1016/j.nds.2019.12.002
2020WA16 Nucl.Instrum.Methods Phys.Res. A971, 164068 (2020) X.Wang, Z.H.Li, Z.Liu, J.Li, H.Hua, H.Y.Lu, W.Q.Zhang, T.H.Huang, M.D.Sun, J.G.Wang, X.Y.Liu, B.Ding, Z.G.Gan, L.Ma, H.B.Yang, Z.Y.Zhang, L.Yu, J.Jiang, K.L.Wang, Y.S.Wang, M.L.Liu, C.J.Lin, L.J.Sun, N.R.Ma, H.S.Xu, X.H.Zhou, G.Q.Xiao, H.Y.Wu, C.Xu, S.Q.Zhang, X.Q.Li, R.Han, Z.Q.Chen, C.G.Wu, D.W.Luo, Y.Jin, J.Lin, D.X.Jiang, Y.L.Ye, F.S.Zhang An effective digital pulse processing method for pile-up pulses in decay studies of short-lived nuclei RADIOACTIVITY 219Th(α), 210,211Ra(IT) [from 175Lu, 186W, 187Re(40Ar, X), E=188 MeV]; measured decay products, Eα, Iα; deduced α spectra, proper baseline correction, standard pulse construction and plateau-region fitting, spectroscopic information of overlapping signals.
doi: 10.1016/j.nima.2020.164068
2019CH24 Phys.Rev.Lett. 122, 212502 (2019) Z.Q.Chen, Z.H.Li, H.Hua, H.Watanabe, C.X.Yuan, S.Q.Zhang, G.Lorusso, S.Nishimura, H.Baba, F.Browne, G.Benzoni, K.Y.Chae, F.C.L.Crespi, P.Doornenbal, N.Fukuda, G.Gey, R.Gernhauser, N.Inabe, T.Isobe, D.X.Jiang, A.Jungclaus, H.S.Jung, Y.Jin, D.Kameda, G.D.Kim, Y.K.Kim, I.Kojouharov, F.G.Kondev, T.Kubo, N.Kurz, Y.K.Kwon, X.Q.Li, J.L.Lou, G.J.Lane, C.G.Li, D.W.Luo, A.Montaner-Piza, K.Moschner, C.Y.Niu, F.Naqvi, M.Niikura, H.Nishibata, A.Odahara, R.Orlandi, Z.Patel, Z.Podolyak, T.Sumikama, P.-A.Soderstrom, H.Sakurai, H.Schaffner, G.S.Simpson, K.Steiger, H.Suzuki, J.Taprogge, H.Takeda, Zs.Vajta, H.K.Wang, J.Wu, A.Wendt, C.G.Wang, H.Y.Wu, X.Wang, C.G.Wu, C.Xu, Z.Y.Xu, A.Yagi, Y.L.Ye, K.Yoshinaga Proton Shell Evolution below 132Sn : First Measurement of Low-Lying β-Emitting Isomers in 123, 125Ag RADIOACTIVITY 123,125Pd(β-) [from Be(238U, X), E=345 MeV/nucleon]; measured decay products, Eγ, Iγ; deduced energy levels, J, π. Comparison with shell-model calculations.
doi: 10.1103/PhysRevLett.122.212502
2019JI10 Prog.Theor.Exp.Phys. 2019, 123D03 (2019) Y.Jin, C.F.Chen, X.-R.Zhou, Y.-Y.Cheng, H.-J.Schulze Deformed K- nuclei in the Skyrme-Hartree-Fock approach NUCLEAR STRUCTURE 8Be, 16O, 20Ne, 40Ca, 208Pb; calculated hypernuclei central kaon potential, kaon removal energies using a two-dimensional Skyrme–Hartree–Fock model with a KN Skyrme force.
doi: 10.1093/ptep/ptz141
2019ZH39 Nucl.Phys. A990, 1 (2019) Z.Zhang, R.R.Xu, Z.Y.Ma, Z.G.Ge, Y.Tian, D.Y.Pang, X.D.Sun, Y.L.Jin, X.Tao, Y.Zhang, J.M.Wang Global α-nucleus optical model based on an Dirac Brueckner Hartree Fock approach
doi: 10.1016/j.nuclphysa.2019.06.013
2018BE05 Phys.Rev. C 97, 032501 (2018) L.Berge, M.Chapellier, M.de Combarieu, L.Dumoulin, A.Giuliani, M.Gros, P.de Marcillac, S.Marnieros, C.Nones, V.Novati, E.Olivieri, B.Paul, D.V.Poda, T.Redon, B.Siebenborn, A.S.Zolotarova, E.Armengaud, C.Augier, A.Benoit, J.Billard, A.Broniatowski, P.Camus, A.Cazes, F.Charlieux, M.De Jesus, K.Eitel, N.Foerster, J.Gascon, Y.Jin, A.Juillard, M.Kleifges, V.Kozlov, H.Kraus, V.A.Kudryavtsev, H.Le Sueur, R.Maisonobe, X.-F.Navick, P.Pari, E.Queguiner, S.Rozov, V.Sanglard, L.Vagneron, M.Weber, E.Yakushev Complete event-by-event α/γ(β) separation in a full-size Teo2 CUORE bolometer by Neganov-Luke-magnified light detection RADIOACTIVITY 130Te(2β-); measured Eγ, Iγ, Eα, Iα, Eβ, heat versus light signals, event-by-event α, β and γ signals using full-size TeO2 CUORE bolometer and Neganov-Luke-magnified light detector at Gran Sasso (LNGS); achieved event-by-event active particle identification capability for requirements of the CUORE Upgrade with Particle IDentification (CUPID) 0νββ project in terms of α background rejection.
doi: 10.1103/PhysRevC.97.032501
2018LI14 Phys.Rev. C 97, 034331 (2018) C.B.Li, X.G.Wu, Y.Zheng, Y.J.Jin, H.L.Ma, G.S.Li, J.Zhong, B.J.Zhu, T.X.Li, Y.X.Gao, X.Guan, J.Q.Liu Level structure in the transitional nucleus 199Tl NUCLEAR REACTIONS 196Pt(7Li, 4n), E=40 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) using eight Compton-suppressed HPGe detectors and two planar HPGe detectors at HI-13 tandem accelerator of China Institute of Atomic Energy (CIAE). 199Tl; deduced high-spin levels, J, π, bands, multipolarities, configurations, alignments, oblate shapes, potential energy surfaces for 17/2- state. Comparison with cranked Nilsson-Strutinsky-Bogoliubov (CNSB) model calculations. Systematics of 13/2+ states in N=104-122 Tl and Bi nuclei. Systematics of negative-parity yrast states and positive-parity 3-qp yrast states in 195,197,199Tl.
doi: 10.1103/PhysRevC.97.034331
2017AR18 Eur.Phys.J. C 77, 785 (2017) E.Armengaud, C.Augier, A.S.Barabash, J.W.Beeman, T.B.Bekker, F.Bellini, A.Benoit, L.Berge, T.Bergmann, J.Billard, R.S.Boiko, A.Broniatowski, V.Brudanin, P.Camus, S.Capelli, L.Cardani, N.Casali, A.Cazes, M.Chapellier, F.Charlieux, D.M.Chernyak, M.de Combarieu, N.Coron, F.A.Danevich, I.Dafinei, M.De Jesus, L.Devoyon, S.Di Domizio, L.Dumoulin, K.Eitel, C.Enss, F.Ferroni, A.Fleischmann, N.Foerster, J.Gascon, L.Gastaldo, L.Gironi, A.Giuliani, V.D.Grigorieva, M.Gros, L.Hehn, S.Herve, V.Humbert, N.V.Ivannikova, I.M.Ivanov, Y.Jin, A.Juillard, M.Kleifges, V.V.Kobychev, S.I.Konovalov, F.Koskas, V.Kozlov, H.Kraus, V.A.Kudryavtsev, M.Laubenstein, H.Le Sueur, M.Loidl, P.Magnier, E.P.Makarov, M.Mancuso, P.de Marcillac, S.Marnieros, C.Marrache-Kikuchi, S.Nagorny, X-F.Navick, M.O.Nikolaichuk, C.Nones, V.Novati, E.Olivieri, L.Pagnanini, P.Pari, L.Pattavina, M.Pavan, B.Paul, Y.Penichot, G.Pessina, G.Piperno, S.Pirro, O.Plantevin, D.V.Poda, E.Queguiner, T.Redon, M.Rodrigues, S.Rozov, C.Rusconi, V.Sanglard, K.Schaffner, S.Scorza, V.N.Shlegel, B.Siebenborn, O.Strazzer, D.Tcherniakhovski, C.Tomei, V.I.Tretyak, V.I.Umatov, L.Vagneron, Ya.V.Vasiliev, M.Velizquez, M.Vignati, M.Weber, E.Yakushev, A.S.Zolotarova Development of 100Mo-containing scintillating bolometers for a high-sensitivity neutrinoless double-beta decay search RADIOACTIVITY 100Mo(2β-); measured decay products, Eβ, Iβ; deduced T1/2.
doi: 10.1140/epjc/s10052-017-5343-2
1997WI23 Phys.Rev. C56, 3152 (1997) C.F.Williamson, T.C.Yates, W.M.Schmitt, M.Osborn, M.Deady, P.D.Zimmerman, C.C.Blatchley, K.K.Seth, M.Sarmiento, B.Parker, Y.Jin, L.E.Wright, D.S.Onley Quasielastic Electron Scattering from 40Ca NUCLEAR REACTIONS 40Ca(e, e'), E=130-841 MeV; measured σ(θ, E); deduced transverse, longitudinal response functions, agreement with Fermi gas predictions.
doi: 10.1103/PhysRevC.56.3152
1996KI20 Phys.Rev. C54, 2515 (1996) K.S.Kim, L.E.Wright, Y.Jin, D.W.Kosik Approximate Treatment of Electron Coulomb Distortion in Quasielastic (e, e') Reactions NUCLEAR REACTIONS 208Pb(e, e'), E=262-645 MeV; analyzed σ(θ) vs energy transfer. Approximate electron Coulomb distortion treatment.
doi: 10.1103/PhysRevC.54.2515
1994JI03 Phys.Rev. C50, 168 (1994) Effects of Coulomb Distortion and Final State Interaction on the Fourth and Fifth Structure Functions NUCLEAR REACTIONS 16O, 40Ca, 208Pb(e, e'p), E=500 MeV; calculated structure functions W(LT), W(LT'). 16O(e, e'p), E=500 MeV; calculated σ(θ(e'), θ(p), E(e')) vs missing momentum. PWBA, Coulomb distortion.
doi: 10.1103/PhysRevC.50.168
1994JI04 Phys.Rev. C50, 377 (1994) Optical Potential Models used in Quasielastic 40Ca(e, e'p) Calculations NUCLEAR REACTIONS 40Ca(e, e'p), E not given; calculated d5/2, d3/2, 2s1/2 state proton knockout double differential σ vs missing momentum. Relativistic formalism, relativistic, nonrelativistic optical models.
doi: 10.1103/PhysRevC.50.377
1994LI47 Phys.Lett. 341B, 213 (1994) The Nucleon Axial Isoscalar Coupling in Quantum Chromodynamics Sum Rules NUCLEAR STRUCTURE 2,1H, 1n; calculated spin structure functions first moments. Improved Ellis-Jaffe sum rules.
doi: 10.1016/0370-2693(94)90312-3
1993JI01 Phys.Rev. C47, 1697 (1993) Analysis of Total Neutron-Nucleus Cross Sections using Relativistic Impulse Approximation NUCLEAR REACTIONS 208Pb, 90Zr, 40Ca(n, n), E=100-600 MeV; calculated σ(E). Relativistic impulse approximation.
doi: 10.1103/PhysRevC.47.1697
1993JI02 Phys.Rev. C47, 2024 (1993) Y.Jin, J.K.Zhang, D.S.Onley, L.E.Wright Quasielastic 40Ca(e, e'p) Cross Sections in a Many-Particle Self-Consistent Hartree Model NUCLEAR REACTIONS 40Ca(e, e'p), E=460 MeV; analyzed data. Fully distorted partial wave calculation, relativistic self-consistent Hartree wave functions.
doi: 10.1103/PhysRevC.47.2024
1993JI04 Phys.Rev. C48, R964 (1993) e-p Off-Shell Cross Section in Quasielastic (e, e'p) Reaction NUCLEAR REACTIONS 208Pb(e, e'p), E=311-513.7 MeV; calculated reduced σ; deduced effective momentum approximation consequences.
doi: 10.1103/PhysRevC.48.R964
1993YA09 Phys.Lett. 312B, 382 (1993) T.C.Yates, C.F.Williamson, W.M.Schmitt, M.Osborn, M.Deady, P.D.Zimmerman, C.C.Blatchley, K.K.Seth, M.Sarmiento, B.Parker, Y.Jin, L.E.Wright, D.S.Onley Longitudinal Response Functions for 40Ca from Quasi-Elastic Electron Scattering NUCLEAR REACTIONS 40Ca(e, e'X), E=130-480 MeV; measured σ(θ) vs energy transfer; deduced longitudinal response functions.
doi: 10.1016/0370-2693(93)90971-J
1993ZH25 Phys.Rev. C48, 2697 (1993) Quantum Hadrodynamics Parametrization: A least-squares fit to nuclear ground-state properties NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 208Pb; analyzed binding energy per nucleon, diffraction radius, surface thickness data; deduced model parameters. A ≈ 25-200; calculated errors in binding energy, charge radius, surface thickness. Hartree-Fock, relativistic Hartree-Fock approaches, quantum hadrodynamics parametrization.
doi: 10.1103/PhysRevC.48.2697
1992JI01 Phys.Rev. C45, 1311 (1992) Electron Coulomb Effects in Quasielastic (e, e'p) Reactions NUCLEAR REACTIONS 208Pb, 40Ca(e, e'p), E not given; calculated reduced σ vs missing momentum; deduced Coulomb distortions role. 208Pb level deduced occupation number. Comparison with other models.
doi: 10.1103/PhysRevC.45.1311
1992JI02 Phys.Rev. C45, 1333 (1992) Single Particle Analysis of (e, e') and the Value of Separated Structure Functions NUCLEAR REACTIONS 40Ca(e, e'), E=250-375 MeV; calculated σ(E(e'), θ), longitudinal structure function. Relativistic Hartree bound state functions.
doi: 10.1103/PhysRevC.45.1333
1988YA08 Phys.Rev. C38, 813 (1988) γ, p(p-bar) as a Probe of the Dirac Negative Energy Bound States NUCLEAR REACTIONS 16O(γ, pp-bar), E ≈ threshold; calculated (p-bar)-nucleus system production σ.
doi: 10.1103/PhysRevC.38.813
1988YA10 Phys.Rev. C38, 923 (1988) Yanhe Jin, L.E.Wright, C.Bennhold, D.S.Onley 14C Beta Decay and the 14N M1 Form Factors NUCLEAR REACTIONS 14N(e, e'), E not given; calculated M1 transition form factors. Relativistic wave functions. NUCLEAR STRUCTURE 14C(β-); calculated β-decay rate. Relativistic wave functions.
doi: 10.1103/PhysRevC.38.923
1986JI02 Nucl.Instrum.Methods Phys.Res. A242, 416 (1986) Y.Jin, R.P.Gardner, K.Verghese A Semi-Empirical Model for the Gamma-Ray Response Function of Germanium Detectors Based on Fundamental Interaction Mechanisms RADIOACTIVITY 28Al(β-); 24Na(β-); 37S(β-); 16N(β-); measured Eγ, Iγ; deduced response function. 49Ca(β-); measured Eγ, Iγ; deduced response function fit.
doi: 10.1016/0168-9002(86)90440-7
1986LA32 Int.J.Appl.Radiat.Isotop. 37, 823 (1986) M.C.Lagunas-Solar, O.F.Carvacho, Bo-Li Liu, Yutai Jin, Zhao Xiang Sun Cyclotron Production of High-Purity 123I I. A Revision of Excitation Functions, Thin-Target and Cumulative Yields for 127I(p, xn) Reactions NUCLEAR REACTIONS, ICPND 127I(p, n), (p, 3n), (p, 5n), (p, 6n), (p, 7n), E=5.3-67.5 MeV; measured σ(E), thin target residual cumulative yields. Hyperpure Ge detector, multichannel analyzer.
doi: 10.1016/0883-2889(86)90278-9
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