NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = Yang Jingfu Found 81 matches. 2024CH12 Phys.Rev. C 109, L021604 (2024) X.Chen, J.Yang, Y.Cui, K.Zhao, Zh.Li, Y.Zhang Novel Pauli blocking method in quantum molecular dynamics type models
doi: 10.1103/PhysRevC.109.L021604
2024YA08 Phys.Rev.Lett. 132, 152502 (2024) X.Yan, Zh.Cheng, A.Abdukerim, Z.Bo, W.Chen, X.Chen, Ch.Cheng, X.Cui, Y.Fan, D.Fang, Ch.Fu, M.Fu, L.Geng, K.Giboni, L.Gu, X.Guo, Ch.Han, K.Han, Ch.He, J.He, D.Huang, Y.Huang, J.Huang, Zh.Huang, R.Hou, Y.Hou, X.Ji, Y.Ju, Ch.Li, J.Li, M.Li, Sh.Li, T.Li, Q.Lin, J.Liu, X.Lu, C.Lu, L.Luo, Y.Luo, W.Ma, Y.Ma, Y.Mao, Y.Meng, X.Ning, B.Pang, N.Qi, Zh.Qian, X.Ren, N.Shaheed, X.Shang, X.Shao, G.Shen, L.Si, W.Sun, A.Tan, Y.Tao, A.Wang, M.Wang, Q.Wang, Sh.Wang, S.Wang, W.Wang, X.Wang, Zh.Wang, Y.Wei, M.Wu, W.Wu, J.Xia, M.Xiao, X.Xiao, P.Xie, B.Yan, J.Yang, Y.Yang, Y.Yao, Ch.Yu, Y.Yuan, Zh.Yuan, X.Zeng, D.Zhang, M.Zhang, P.Zhang, Sh.Zhang, Sh.Zhang, T.Zhang, W.Zhang, Y.Zhang, Y.Zhang, Y.Zhang, L.Zhao, Q.Zheng, J.Zhou, N.Zhou, X.Zhou, Y.Zhou, Y.Zhou, for the PandaX Collaboration Searching for Two-Neutrino and Neutrinoless Double Beta Decay of 134Xe with the PandaX-4T Experiment RADIOACTIVITY 134Xe(2β-); measured decay products, Eβ, Iβ; deduced two-neutrino and neutrinoless T1/2 limits. Comparison with available data. The cylindrical active volume PandaX-4T dual-phase TPC.
doi: 10.1103/PhysRevLett.132.152502
2023CH44 Phys.Rev. C 108, 034613 (2023) X.Chen, L.Li, Y.Cui, J.Yang, Z.Li, Y.Zhang Bayesian reconstruction of impact parameter distributions from two observables for intermediate energy heavy ion collisions
doi: 10.1103/PhysRevC.108.034613
2023FA05 Appl.Radiat.Isot. 197, 110791 (2023) Z.Fan, H.Liu, J.Liang, Y.Xiao, D.Yuan, C.Sun, Z.Yang, J.Yang, H.Zhang Activity determination of 56Mn using extended TDCR-Cerenkov method RADIOACTIVITY 56Mn(β-) [from 55Mn(n, γ), E thermal]; measured decay products, Eγ, Iγ, Eβ, Iβ; deduced branch ratio of cascades and discrete point of beta emission spectra, anisotropy parameters. Comparison with calculations.
doi: 10.1016/j.apradiso.2023.110791
2023LI21 Appl.Radiat.Isot. 197, 110824 (2023) C.Li, H.Zhou, H.Liu, T.Sun, H.Fan, J.Yang, W.Xiao Neutron spectrometry of D2O-moderated 252Cf with Bonner sphere spectrometer
doi: 10.1016/j.apradiso.2023.110824
2023YA14 Universe 9, 206 (2023) J.Yang, X.Chen, Y.Cui, Z.Li, Y.Zhang Probing the Neutron Skin of Unstable Nuclei with Heavy-Ion Collisions NUCLEAR REACTIONS 124Sn(124Sn, X), (132Sn, X), E=200 MeV; calculated peripheral collisions; deduced σ of projectile-like residues correlations with the neutron skin of the system.
doi: 10.3390/universe9050206
2023YA15 Phys.Rev. C 107, 054304 (2023) J.Yang, J.Dudek, I.Dedes, A.Baran, D.Curien, A.Gaamouci, A.Gozdz, A.Pedrak, D.Rouvel, H.L.Wang Islands of oblate hyperdeformed and superdeformed superheavy nuclei with D3h point group symmetry in competition with normal-deformed D3h states: "Archipelago" of D3h-symmetry islands NUCLEAR STRUCTURE 302Og, 292124, 318130; calculated contours of projections of the total nuclear energy surfaces on (α22, α20), (α33, α20), ( α33, α22) and (α30, α20) planes, deformation parameters. N=166-206;Z=116-138; calculated single-particle neutron and proton energy levels, shell energies defined as sums of the Strutinsky and pairing correction energies, D3h-symmetric hyperdeformed, superdeformed, and normal-deformed configurations. Found three separate islands of nuclei with D3h symmetry ("archipelago of three islands") differing by their average α20 < 0 deformations. Macroscopic-microscopic method with a realistic phenomenological Woods-Saxon potential.
doi: 10.1103/PhysRevC.107.054304
2023ZH01 At.Data Nucl.Data Tables 149, 101547 (2023) G.Zhang, B.Deng, J.Yang, K.Tang, B.Meng, X.Zhang Wavelengths, transition rates, weight oscillator strengths and line strengths for He-like to Ne-like cobalt ions ATOMIC PHYSICS Co; calculated wavelengths, transition rates, absorption oscillator strengths, and line strengths for the 2s-3p, 2p-3s, and 2p-3d electric dipole (E1) transitions in He-like to Ne-like cobalt ions using the multi-configuration Dirac–Hartree–Fock (MCDHF) and Relativistic Configuration Interaction (RCI) methods. Comparison with available data.
doi: 10.1016/j.adt.2022.101547
2022LI02 At.Data Nucl.Data Tables 143, 101476 (2022) Z.Li, D.Li, J.Yang, X.Jiang, W.Jiang, D.Chen Non-dissociative ionization cross section of the electronically excited H2 and D2 with atomic-limit principal quantum number n=3 and 4 NUCLEAR REACTIONS 1,2H(e-, X), E<10 keV; calculated electron-impact σ for non-dissociative ionization via the ground vibrational level of the electronically excited H2 and D2.
doi: 10.1016/j.adt.2021.101476
2022PO02 Phys.Rev. C 105, L041301 (2022) W.S.Porter, B.Ashrafkhani, J.Bergmann, C.Brown, T.Brunner, J.D.Cardona, D.Curien, I.Dedes, T.Dickel, J.Dudek, E.Dunling, G.Gwinner, Z.Hockenbery, J.D.Holt, C.Hornung, C.Izzo, A.Jacobs, A.Javaji, B.Kootte, G.Kripko-Koncz, E.M.Lykiardopoulou, T.Miyagi, I.Mukul, T.Murbock, W.R.Plass, M.P.Reiter, J.Ringuette, C.Scheidenberger, R.Silwal, C.Walls, H.L.Wang, Y.Wang, J.Yang, J.Dilling, A.A.Kwiatkowski Mapping the N=40 island of inversion: Precision mass measurements of neutron-rich Fe isotopes ATOMIC MASSES 63,64,65,65m,66,67,68,69,69m,70Fe; measured time-of-flight; deduced mass excess, S(2n), pairing gap. Systematics of S(2n) values for Z=24–28 isotope chains. Compared to mean-field calculations employing recent Woods-Saxon Hamiltonian and results from the multishell valence-space in-medium similarity renormalization group (VS-IMSRG). Comparison to recommended values from AME2020. TITAN (TRIUMF’s Ion Trap for Atomic and Nuclear science) Multiple-Reflection Time-of- Flight Mass Spectrometer.
doi: 10.1103/PhysRevC.105.L041301
2022SA30 Chin.Phys.Lett. 39, 062901 (2022) A.Salman, J.Zhou, J.Yang, J.Zhang, C.Huang, F.Ye, Z.Qin, X.Jiang, S.M.Amir, W.Kreuzpaintner, Z.Sun, T.Wang, X.Tong Development of Time-of-Flight Polarized Neutron Imaging at the China Spallation Neutron Source
doi: 10.1088/0256-307X/39/6/062901
2022YA11 Phys.Rev. C 105, 034348 (2022) J.Yang, J.Dudek, I.Dedes, A.Baran, D.Curien, A.Gaamouci, A.Gozdz, A.Pedrak, D.Rouvel, H.L.Wang, J.Burkat Exotic shape symmetries around the fourfold octupole magic number N=136: Formulation of experimental identification criteria NUCLEAR STRUCTURE N=122-164; calculated single-particle neutron levelsand Routhians as functions of α30, α31, α32 and α33 octupole deformations; deduced very large neutron shell gaps at N=136 for all the four octupole deformations, and N=136 as a "universal or fourfold octupole magic number". 208,212,216,218Pb, 218,220,222,224Ra, 220Po, 222Rn, 224Ra, 226Th; calculated contours of projections of the total nuclear energy surfaces on (α30, α20) planes for all the isotopes, (α31, α20), (α32, α20), and (α33, α20) planes for 218Pb, (α32, α20) planes for 218,220, 222,224Ra, and (α31, α20) and (α32, α20) planes for 220Po, 222Rn, 224Ra, 226Th. Discussed exotic point-group symmetries C2ν, D2d, Td (tetrahedral symmetry), and D3h in order to formulate spectroscopic criteria for experimental identifications through analysis of collective rotational bands generated by the symmetries. Macroscopic-microscopic method in multidimensional deformation spaces to analyze the expected exotic symmetries and octupole shape instabilities, tetrahedral point group symmetry, and realistic nuclear mean-field theory using phenomenological Woods-Saxon Hamiltonian combined with the Monte Carlo approach. Comparison with available experimental nuclear octupole deformations.
doi: 10.1103/PhysRevC.105.034348
2022YA26 Phys.Rev. C 106, 054314 (2022) J.Yang, J.Dudek, I.Dedes, A.Baran, D.Curien, A.Gaamouci, A.Gozdz, A.Pedrak, D.Rouvel, H.L.Wang Exotic symmetries as stabilizing factors for superheavy nuclei: Symmetry-oriented generalized concept of nuclear magic numbers NUCLEAR STRUCTURE Z=82-138, N=164-258; calculated single-particle proton and neutron energies, spherical orbital energies and shell gaps. 314Og; calculated Monte Carlo simulated probability distributions of single-particle level position uncertainties for protons and neutrons. 308122; calculated proton and neutron single-particle energies as functions of the octupole deformations α30, α31, α32 and α33 in the center of Z=114-130, N=166-206 region. 310Fl, 314Og, 318122, 322126, 326130; calculated potential-energy projection contours as functions of quadrupole deformation parameter α20 and octupole deformation parameters α30, α31, α32 and α33 for 310Fl, and α32 for others. 296,298,300,302,304,306,308,310,312,314,316Sg, 304,306,308,310,312,314,316,318,320,322,324Fl, 310Fl, 314,316,318,320,322,324,326,328,330,332,334124, 312Lv, 314Og, 316120, 318122, 320124, 322126, 324128, 326130, 328132, 330134, 332136; calculated nuclear shell energies as functions of octupole deformation parameters α30, α31, α32 and α33, comparisons of nuclear shell-energies as functions of quadrupole deformation α20, and octupole deformation parameters α30 (pear-shaped), α31, α32, and α33 for Z-114, N=190-210, and for N=196, Z=114-136 nuclei. 296,298,300,302,304,306,308,310,312,314,316Sg, 314,316,318,320,322,324,326,328,330,332,334124; calculated energies at the equilibrium before and after allowing the α32 minimization. 280,282,284,286,288,290,292,294,296,298,300,302,304,306,308,310,312,314,316,318,320Fl, 282,284,286,288,290,292,294,296,298,300,302,304,306,308,310,312,314,316,318,320,322Lv, 284,286,288,290,292,294,296,298,300,302,304,306,308,310,312,314,316,318,320,322,324Og, 286,288,290,292,294,296,298,300,302,304,306,308,310,312,314,316,318,320,322,324,326120, 288,290,292,294,296,298,300,302,304,306,308,310,312,314,316,318,320,322,324,326,328122, 290,292,294,296,298,300,302,304,306,308,310,312,314,316,318,320,322,324,326,328,330124, 292,294,296,298,300,302,304,306,308,310,312,314,316,318,320,322,324,326,328,330,332126, 294,296,298,300,302,304,306,308,310,312,314,316,318,320,322,324,326,328,330,332,334128, 296,298,300,302,304,306,308,310,312,314,316,318,320,322,324,326,328,330,332,334,336130; predicted quadrupole deformation α2, components of octupole deformation α30, α31, α32 and α33 for the ground states, energy differences between the nearest quadrupole-shape minima and octupole-deformed configurations; deduced spherical or octupole deformed, with dominance of octupole-tetrahedral geometry for a majority of superheavy nuclei, which lowers the ground-state energy by up to 8 MeV. Realistic phenomenological mean-field approach with the deformed Woods-Saxon potential and macroscopic-microscopic method to examine impact of exotic shapes of nuclei associated with the four-fold octupole degrees of freedom on the stabilization of superheavy nuclei in the mass range of Z=114-130, and N=166-206.
doi: 10.1103/PhysRevC.106.054314
2021BE23 Phys.Rev.Lett. 127, 112501 (2021) S.Beck, B.Kootte, I.Dedes, T.Dickel, A.A.Kwiatkowski, E.M.Lykiardopoulou, W.R.Plass, M.P.Reiter, C.Andreoiu, J.Bergmann, T.Brunner, D.Curien, J.Dilling, J.Dudek, E.Dunling, J.Flowerdew, A.Gaamouci, L.Graham, G.Gwinner, A.Jacobs, R.Klawitter, Y.Lan, E.Leistenschneider, N.Minkov, V.Monier, I.Mukul, S.F.Paul, C.Scheidenberger, R.I.Thompson, J.L.Tracy, Jr., M.Vansteenkiste, H.-L.Wang, M.E.Wieser, C.Will, J.Yang Mass Measurements of Neutron-Deficient Yb Isotopes and Nuclear Structure at the Extreme Proton-Rich Side of the N=82 Shell ATOMIC MASSES 150,151,152,153,154,155,156Yb; measured frequencies, TOF; deduced mass excess values. Comparison with systematics, AME2020 evaluation. TITAN's multiple-reflection time-of-flight mass spectrometer (MR-TOF-MS). RADIOACTIVITY 151Yb(IT); measured decay products; deduced excitation energy.
doi: 10.1103/PhysRevLett.127.112501
2021GA18 Phys.Rev. C 103, 054311 (2021) A.Gaamouci, I.Dedes, J.Dudek, A.Baran, N.Benhamouda, D.Curien, H.L.Wang, J.Yang Exotic toroidal and superdeformed configurations in light atomic nuclei: Predictions using a mean-field Hamiltonian without parametric correlations NUCLEAR STRUCTURE 28Si, 28,30,38,40Si, 32,40,42S, 36Ar, 40Ca, 44Ti, 48Cr, 56Ni, 52,56Fe, 82,84,100Zr; A≈30-50; calculated nuclear potential energy surfaces in (α20, α40) and (β2cos(γ+30°)), (β2sin(γ+30°)) planes using mean-field calculations in multidimensional deformation spaces with phenomenological Woods-Saxon Hamiltonian, Monte-Carlo Hamiltonian parameter adjustments based on doubly-magic spherical nuclei: 16O, 40Ca, 48Ca, 56Ni, 90Zr, 132Sn, 146Gd and 208Pb, parametric-correlation removal; tested parametric uncertainties, theoretical prediction uncertainty propagation with nucleon numbers; generated nuclear shape coexistence, low-energy toroidal shape excitations, superdeformed oblate and prolate shapes, exotic shapes and isomers. Comparison with available experimental information for deformation parameters.
doi: 10.1103/PhysRevC.103.054311
2021GA27 Appl.Radiat.Isot. 176, 109828 (2021) J.Gao, Z.Liao, W.Liu, Y.Hu, H.Ma, L.Xia, F.Li, T.Lan, Y.Yang, J.Yang, J.Liao, N.Liu Simple and efficient method for producing high radionuclidic purity 111In using enriched 112Cd target NUCLEAR REACTIONS 112Cd(p, 2n)111In, E=21 MeV; measured reaction products, Eγ, Iγ; deduced yields.
doi: 10.1016/j.apradiso.2021.109828
2021GO15 Phys.Rev. C 103, L041302 (2021) G.Gosta, A.Mentana, F.Camera, A.Bracco, S.Ceruti, G.Benzoni, N.Blasi, S.Brambilla, S.Capra, F.C.L.Crespi, A.Giaz, S.Leoni, B.Million, S.Riboldi, C.Porzio, S.Ziliani, O.Wieland, A.Nannini, M.Rocchini, N.Marchini, M.Ciemala, M.Kmiecik, A.Maj, B.Wasilewska, M.Zieblinski, D.Filipescu, J.Kaur, N.Marginean, S.Pascu, T.Glodariu, D.Ghita, V.Zamfir, J.J.Valiente-Dobon, G.de Angelis, F.Galtarossa, A.Goasduff, T.Bayram, A.Gadea, A.Montaner, I.Zanon, D.Brugnara, A.Gozzelino, G.Pasqualato, R.Menegazzo, A.Gottardo, G.Jaworski, S.Lenzi, D.Napoli, D.Testov, M.Siciliano, T.Marchi, D.Mengoni, D.Bazzacco, A.Boso, P.R.John, F.Recchia, R.Raabe, O.Poleshchuk, J.Yang Probing isospin mixing with the giant dipole resonance in the 60Zn compound nucleus NUCLEAR REACTIONS 32Si(28Si, X)60Zn*, E=86, 110 MeV; 32Si(30Si, X)62Zn*, E=75, 98 MeV; measured high-energy Eγ, Iγ using GALILEO array of 25 HPGe detectors and ten LaBr3(Ce) scintillators at the Tandem accelerator facility of INFN-Legnaro. 60,62Zn; deduced GDR parameters, Coulomb spreading widths, isospin mixing parameter at zero temperature and the isospin-symmetry-breaking correction for beta decay by analyzing experimental γ-spectra with statistical model calculations using a version of CASCADE code that included isospin formalism. Comparison of Coulomb spreading widths with the values for other mass regions deduced from GDR γ-decay measurements in other compound-nucleus reactions.
doi: 10.1103/PhysRevC.103.L041302
2021MA72 Phys.Rev. C 104, L051301 (2021) P.T.MacGregor, D.K.Sharp, S.J.Freeman, C.R.Hoffman, B.P.Kay, T.L.Tang, L.P.Gaffney, E.F.Baader, M.J.G.Borge, P.A.Butler, W.N.Catford, B.D.Cropper, G.de Angelis, J.Konki, Th.Kroll, M.Labiche, I.H.Lazarus, R.S.Lubna, I.Martel, D.G.McNeel, R.D.Page, O.Poleshchuk, R.Raabe, F.Recchia, J.Yang Evolution of single-particle structure near the N=20 island of inversion NUCLEAR REACTIONS 2H(28Mg, p)29Mg, E=9.47 MeV/nucleon, [secondary 28Mg beam from Si(p, X), E=1.4 GeV, followed resonant ionization by the resonance ionization laser ion source (RILIS), and mass separated and injected into an ion trap at the HIE-ISOLDE-CERN Linac facility]; measured E(p), I(p), σ(θ) using ISOLDE Solenoidal Spectrometer. 29Mg; deduced levels, J, π, L-transfers, spectroscopic factors, vacancies deduced from summed spectroscopic factors, binding energies of single-particle centroids. Comparison with shell-model calculations. Detailed σ(θ) data are tabulated in the Supplemental Material.
doi: 10.1103/PhysRevC.104.L051301
2021XI05 Chin.Phys.C 48, 084106 (2021) C.Xiu, Y.Zhang, M.-J.Li, J.Yang, Y.-X.Chen Effects of an odd particle on shape phase transitions in odd-even systems
doi: 10.1088/1674-1137/ac05a0
2021YA24 Phys.Rev. C 104, 024605 (2021) Influence of the treatment of initialization and mean-field potential on the neutron to proton yield ratios
doi: 10.1103/PhysRevC.104.024605
2020GO02 Acta Phys.Pol. B51, 683(2020) G.Gosta, S.Ceruti, A.Mentana, M.Ciemala, F.Camera, A.Bracco, G.Benzoni, N.Blasi, G.Bocchi, S.Brambilla, F.C.L.Crespi, A.Giaz, S.Leoni, B.Million, O.Wieland, M.Kmiecik, A.Maj, B.Wasilewska, M.Zieblinski, D.Filipescu, D.Ghita, V.Zamfir, J.J.Valiente-Dobon, g.De Angelis, F.Galtarossa, A.Goasduff, G.Jaworski, D.R.Napoli, D.Testov, M.Siciliano, T.Marchi, D.Mengoni, D.Bazzacco, A.Boso, P.R.John, R.Recchia R.Raabe, O.Poleshchuk, J.Yang Isospin Symmetry in the 60Zn Nucleus
doi: 10.5506/APhysPolB.51.683
2020HU06 Appl.Radiat.Isot. 160, 109133 (2020) Y.Hu, Y.Tang, F.Li, J.Gao, Y.Yang, J.Yang, J.Liao, N.Liu Production of 98Tc with high isotopic purity NUCLEAR REACTIONS 98Mo(p, n)98Tc, E=9.4 MeV; measured reaction products, Eγ, Iγ; deduced production technology.
doi: 10.1016/j.apradiso.2020.109133
2020OV01 Acta Phys.Pol. B51, 731 (2020) J.D.Ovejas, A.Knyazev, I.Martel, O.Tengblad, M.J.G.Borge, J.Cederkall, N.Keeley, K.Rusek, C.Garcia-Ramos, L.A.Acosta, A.A.Arokiaraj, M.Babo, T.Cap, N.Ceylan, G.De Angelis, A.Di Pietro, J.P.Fernandez, P.Figuera, L.Fraile, H.Fynbo, D.Galviz, J.H.Jensen, B.Jonson, R.Kotak, T.Kurtukian, M.Madurga, G.Marquinez-Duran, M.Munch, A.K.Orduz, R.Honorio, A.Pakou, T.Perez, L.Peralta, A.Perea, R.Raabe, M.Renaud, K.Riisager, A.M.Sanchez-Benitez, J.Sanchez-Segovia, O.Sgouros, V.Soukeras, P.Teubig, S.Vinals, M.Wolinska-Cichocka, R.Wolski, J.Yang Halo Effects in the Low-Energy Scattering of 15C with Heavy Targets
doi: 10.5506/APhysPolB.51.731
2020TA03 Phys.Rev.Lett. 124, 062502 (2020) T.L.Tang, B.P.Kay, C.R.Hoffman, J.P.Schiffer, D.K.Sharp, L.P.Gaffney, S.J.Freeman, M.R.Mumpower, A.Arokiaraj, E.F.Baader, P.A.Butler, W.N.Catford, G.de Angelis, F.Flavigny, M.D.Gott, E.T.Gregor, J.Konki, M.Labiche, I.H.Lazarus, P.T.MacGregor, I.Martel, R.D.Page, Zs.Podolyak, O.Poleshchuk, R.Raabe, F.Recchia, J.F.Smith, S.V.Szwec, J.Yang First Exploration of Neutron Shell Structure below Lead and beyond N=126 NUCLEAR REACTIONS 2H(206Hg, p), E=7.38 MeV/nucleon; measured reaction products, Ep, Ip. 207Hg; deduced excitation energies, J, π, σ(θ). Comparison with theoretical calculations.
doi: 10.1103/physrevlett.124.062502
2020YA25 Phys.Rev. C 102, 054308 (2020) Dirac oscillator: An alternative basis for nuclear structure calculations NUCLEAR STRUCTURE 40,48Ca, 132Sn, 208Pb; calculated binding energies per nucleon, charge radii, neutron skin thicknesses, baryon (neutron + proton) densities. Dirac oscillator (harmonic-oscillator supplemented a strong spin-orbit coupling) on a fully relativistic basis within the framework of covariant density-functional theory. Comparison with results obtained with often-used Runge-Kutta method.
doi: 10.1103/PhysRevC.102.054308
2019AK14 Phys.Rev. D 100, 115020 (2019) D.Akimov, J.B.Albert, P.An, C.Awe, P.S.Barbeau, B.Becker, V.Belov, M.A.Blackston, A.Bolozdynya, B.Cabrera-Palmer, M.Cervantes, J.I.Collar, R.L.Cooper, J.Daughhetee, M.del Valle Coello, J.A.Detwiler, M.D'Onofrio, Y.Efremenko, E.M.Erkela, S.R.Elliott, L.Fabris, M.Febbraro, W.Fox, A.Galindo-Uribarri, M.P.Green, K.S.Hansen, M.R.Heath, S.Hedges, T.Johnson, M.Kaemingk, L.J.Kaufman, A.Khromov, A.Konovalov, E.Kozlova, A.Kumpan, L.Li, J.T.Librande, J.M.Link, J.Liu, K.Mann, D.M.Markoff, H.Moreno, P.E.Mueller, J.Newby, D.S.Parno, S.Penttila, D.Pershey, D.Radford, R.Rapp, H.Ray, J.Raybern, O.Razuvaeva, D.Reyna, G.C.Rich, D.Rudik, J.Runge, D.J.Salvat, K.Scholberg, A.Shakirov, G.Simakov, G.Sinev, W.M.Snow, V.Sosnovtsev, B.Suh, R.Tayloe, K.Tellez-Giron-Flores, R.T.Thornton, I.Tolstukhin, J.Vanderwerp, R.L.Varner, C.J.Virtue, G.Visser, C.Wiseman, T.Wongjirad, J.Yang, Y.-R.Yen, J.Yoo, C.-H.Yu, J.Zettlemoyer First constraint on coherent elastic neutrino-nucleus scattering in argon NUCLEAR REACTIONS Ar, 133Cs, 127I, Ge, 23Na(ν, ν), E, 100 MeV; measured reaction products, nuclear recoils; deduced a limit on coherent elastic neutrino-nucleus scattering.
doi: 10.1103/PhysRevD.100.115020
2019DU22 Acta Phys.Pol. B50, 685 (2019) J.Dudek, I.Dedes, J.Yang, A.Baran, D.Curien, T.Dickel, A.Gozdz, D.Rouvel, H.L.Wang High-rank Symmetries in Nuclei: Challenges for Prediction Capacities of the Nuclear Mean-field Theories NUCLEAR STRUCTURE 226Th; calculated total nuclear energy surfaces. Discussed the possible structure of rotational bands in cases of tetrahedral and octahedral nuclear symmetries. Mean-field approach with the phenomenological “universal” Woods–Saxon Hamiltonian.
doi: 10.5506/aphyspolb.50.685
2019GO35 Acta Phys.Pol. B50, 481 (2019) G.Gosta, S.Ceruti, A.Mentana, M.Ciemala, F.Camera, A.Bracco, G.Benzoni, N.Blasi, G.Bocchi, S.Brambilla, F.C.L.Crespi, A.Giaz, S.Leoni, B.Million, O.Wieland, M.Kmiecik, A.Maj, B.Wasilewska, M.Zieblinski, D.Filipescu, D.Ghita, V.Zamfir, J.J.Valiente-Dobon, G.de Angelis, F.Galtarossa, A.Goasduff, G.Jaworski, D.R.Napoli, D.Testov, M.Siciliano, T.Marchi, D.Mengoni, D.Bazzacco, A.Boso, P.R.John, F.Recchia, R.Raabe, O.Poleshchuk, J.Yang Study of the Isospin Symmetry in 60Zn NUCLEAR REACTIONS 28,30Si(32Si, X)60Zn/62Zn, E=75, 86, 98, 110 MeV; measured reaction products, Eγ, Iγ, γγ-coin, nγ-coin. Analysis of compound nuclei decay. GALILEO HPGe-array, EUCLIDES Si-array and Neutron Wall detectors.
doi: 10.5506/aphyspolb.50.481
2019MO32 Phys.Rev. C 100, 044615 (2019) 15C: From halo effective field theory structure to the study of transfer, breakup, and radiative-capture reactions NUCLEAR REACTIONS 14C(d, p)15C, E=14, 17.06 MeV; analyzed experimental data for differential σ(θ, E) using leading-order (LO) halo-EFT description of 15C with a finite-range adiabatic distorted wave approximation (FR-ADWA) model; deduced asymptotic normalization coefficient (ANC) of 15C ground state. 208Pb(15C, X), E=68, 605 MeV/nucleon; analyzed experimental data from GSI and RIKEN for differential breakup σ(E) using NLO eikonal-based model. 14C(n, γ)15C, E=10-1000 keV; calculated σ(E) using ANC extracted from (d, p) data. 15C; calculated E1 strength from the 1/2+ ground state to its 14C-n continuum based on the halo-EFT structure of 15C at NLO, and compared to experimental data. Relevance of 14C(n, γ)15C reaction in production of heavy elements in inhomogeneous big-bang nucleosynthesis.
doi: 10.1103/PhysRevC.100.044615
2019NI10 Chin.Phys.C 43, 113001 (2019) K.Ni, Y.Lai, A.Abdukerim, W.Chen, X.Chen, Y.Chen, X.Cui, Y.Fan, D.Fang, C.Fu, L.Geng, K.Giboni, F.Giuliani, L.Gu, X.Guo, K.Han, C.He, D.Huang, Y.Huang, Y.Huang, Z.Huang, P.Ji, X.Ji, Y.Ju, K.Liang, H.Liu, J.Liu, W.Ma, Y.Ma, Y.Mao, Y.Meng, P.Namwongsa, J.Ning, X.Ning, X.Ren, C.Shang, L.Si, A.Tan, A.Wang, H.Wang, M.Wang, Q.Wang, S.Wang, X.Wang, Z.Wang, M.Wu, S.Wu, J.Xia, M.Xiao, P.Xie, B.Yan, J.Yang, Y.Yang, C.Yu, J.Yuan, D.Zhang, H.Zhang, T.Zhang, L.Zhao, Q.Zheng, J.Zhou, N.Zhou, X.Zhou Searching for neutrino-less double beta decay of 136Xe with PandaX-II liquid xenon detector RADIOACTIVITY 136Xe(2β-); measured decay products, Eβ, Iβ; deduced T1/2 and Majorana neutrino mass limits. Comparison with available data.
doi: 10.1088/1674-1137/43/11/113001
2019SH30 Eur.Phys.J. A 55, 138 (2019) R.Shi, X.Tuo, J.Yang, Y.Cheng, H.Zheng, Q.Wang, C.Deng A peak shape model with high-energy tailing for high-resolution alpha-particle spectra
doi: 10.1140/epja/i2019-12827-x
2019YA20 Phys.Rev. C 100, 054301 (2019) J.Yang, J.A.Hernandez, J.Piekarewicz Electroweak probes of ground state densities NUCLEAR REACTIONS 40Ar, 48Ca, 50Ti, 50Ni, 132Xe, 208Pb(e, e), (ν, ν), at momentum transfer q=0-3 fm-1; calculated ground state charge densities for 50Ti, 50Ni and 208Pb, form factors (weak and charge), neutron skin thickness, point proton and neutron charge density. Calculations used relativistic mean-field models, and three electroweak experiments to constrain the neutron distribution of atomic nuclei: (1) parity-violating elastic electron scattering, (2) coherent elastic neutrino-nucleus scattering, and (3) elastic electron scattering on mirror pair unstable nuclei. Comparison and relevance to experimental data from the ongoing PREX-II, and upcoming CREX campaigns at Jefferson Lab.
doi: 10.1103/PhysRevC.100.054301
2018HU01 Phys.Rev. A 97, 013424 (2018) Q.-Q.Hu, C.Freier, Y.Sun, B.Leykauf, V.Schkolnik, J.Yang, M.Krutzik, A.Peters Observation of vector and tensor light shifts in 87Rb using near-resonant, stimulated Raman spectroscopy ATOMIC PHYSICS 87Rb; measured relative frequency; deduced the differential vector and tensor light shifts, Raman spectra, implications for higher fidelities for applications of neutral atoms in quantum information and precision measurements.
doi: 10.1103/PhysRevA.97.013424
2018YA02 Phys.Rev. C 97, 014314 (2018) Difference in proton radii of mirror nuclei as a possible surrogate for the neutron skin NUCLEAR STRUCTURE 48Ca, 208Pb; analyzed relations between the neutron-skin thickness and the difference in proton radii between a few neutron-deficient nickel isotopes and their mirror nuclei: 54Ni and 54Fe, 52Ni and 52Cr, and 50Ni and 50Ti, stellar radii for neutron stars as a function of the difference in proton radii between 50Ni and 50Ti; verified correlation between the differences in the charge radii of mirror nuclei and neutron-skin thickness of neutron-rich nuclei and the slope of the symmetry energy in the relativistic framework.
doi: 10.1103/PhysRevC.97.014314
2018YA22 Phys.Rev. C 98, 054602 (2018) Systematic analysis of the peripherality of the 10Be (d, p) 11Be transfer reaction and extraction of the asymptotic normalization coefficient of 11Be bound states NUCLEAR REACTIONS 10Be(d, p), E=12, 15, 18, 21.4 MeV; analyzed experimental data differential σ(θ, E) populating the g.s. of 11Be using adiabatic distorted wave approximation (ADWA) and a Halo-EFT description of 11Be at leading order; deduced asymptotic normalization coefficients (ANCs). 11Be; calculated parameters of the Gaussian 10Be-neutron potentials, and reduced radial wave function.
doi: 10.1103/PhysRevC.98.054602
2017DI02 Phys.Rev. C 95, 024301 (2017) B.Ding, Z.Liu, D.Seweryniak, P.J.Woods, H.L.Wang, J.Yang, H.L.Liu, C.N.Davids, M.P.Carpenter, T.Davinson, R.V.F.Janssens, R.D.Page, A.P.Robinson, J.Shergur, S.Sinha, S.Zhu, X.D.Tang, J.G.Wang, T.H.Huang, W.Q.Zhang, M.D.Sun, X.Y.Liu, H.Y.Lu First identification of excited states in 117Ba using the recoil-β-delayed proton tagging technique NUCLEAR REACTIONS 64Zn(58Ni, 3n2p), E=305 MeV; measured Eγ, Iγ, (delayed protons)γ-coin, recoil-βp decay tagging using fragment mass analyzer (FMA), and Gammasphere array at ATLAS-ANL facility. 117Ba; deduced high-spin levels, J, π, bands, alignments, Routhian energies, configurations. Comparison with cranked shell-model calculations. Level-spacing systematics for negative- and positive-parity bands in 117,119,121,123,125,127,129Ba.
doi: 10.1103/PhysRevC.95.024301
2016WA01 At.Data Nucl.Data Tables 108, 15 (2016) C.Wang, H.Liu, F.Hu, J.Li, S.Liu, Y.Ding, J.Yang, G.Jiang Transition probabilities of the low-lying levels of Kr XXIV ATOMIC PHYSICS Kr; calculated energy levels, radiative rates, and wavelengths. Multiconfigurational Dirac-Hartree-Fock (MCDHF) method, comparison with available data.
doi: 10.1016/j.adt.2015.07.004
2016YA04 Prog.Theor.Exp.Phys. 2016, 063D03 (2016) J.Yang, H.-L.Wang, Q.-Z.Chai, M.-L.Liu, F.-R.Xu Evolution of shape and rotational structure in neutron-deficient 118-128Ba nuclei NUCLEAR STRUCTURE 118,120,122,124,126,128Ba; calculated deformation Routhian curves, LN pairing gaps of protons and neutrons, angular momenta. Comparison with available data.
doi: 10.1093/ptep/ptw074
2015WA25 Phys.Rev. C 92, 024303 (2015) H.-L.Wang, J.Yang, M.-L.Liu, F.-R.Xu Evolution of ground-state quadrupole and octupole stiffnesses in even-even barium isotopes NUCLEAR STRUCTURE 112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148,150Ba; calculated ground-state deformation parameters β2, γ, β3, potential energy curves as function of (β2, γ, β4) and (β2, β3, β4, β5) deformation, quadrupole and octupole stiffnesses, single-particle Fermi energies, pairing gaps, energies of first excited 2+, 4+, 3- and the second 2+ states. 114Ba; calculated single-particle levels, energy curves. Potential energy surface method with standard Liquid drop model and Lipkin-Nogami pairing model. Discussed importance of nonaxial and reflection-asymmetric deformation degrees of freedom in the calculation of potential energy surfaces, especially for actinides and superheavy nuclei. Comparison with available experimental data.
doi: 10.1103/PhysRevC.92.024303
2015ZH27 Phys.Rev. C 92, 024906 (2015) Squeezed correlations of φ-meson pairs for hydrodynamic sources in high-energy heavy-ion collisions
doi: 10.1103/PhysRevC.92.024906
2012YA17 Eur.Phys.J. A 48, 149 (2012) T.Yang, TaoJiang, R.Ze, H.Wu, Y.He, J.Yang, C.Yang Preparation of the 178m2Hf isomer used in the induced gamma decay experiment by X-ray from synchrotron radiation facility NUCLEAR REACTIONS 176Yb(α, 2n)178m2Hf, (α, X), E≈27 MeV; measured Eγ, Iγ after cooling using HPGe; deduced isomeric state (after radiochemical separation).
doi: 10.1140/epja/i2012-12149-7
2012YI01 Phys.Rev. C 86, 024914 (2012) H.-J.Yin, J.Yang, W.-N.Zhang, L.-L.Yu Two-particle interferometry for the sources undergoing a first-order QCD phase transition in high-energy heavy ion collisions
doi: 10.1103/PhysRevC.86.024914
2011IS13 Phys.Rev. C 84, 065802 (2011) Finite temperature effects on anisotropic pressure and equation of state of dense neutron matter in an ultrastrong magnetic field
doi: 10.1103/PhysRevC.84.065802
2010IS03 Ukr.J.Phys. 55, 515 (2010) Magnetization of Dense Neutron Matter in a Strong Magnetic Field
2010YA01 Radiochim.Acta 98, 59 (2010) J.Yang, S.Zhang, Y.Ding, F.Shu, J.Zhang A new value of 93Zr half-life RADIOACTIVITY 93Zr(β-); measured Eγ, Iγ; deduced T1/2.
doi: 10.1524/ract.2010.1678
2009IS06 Phys.Rev. C 80, 065801 (2009) Spin-polarized states in neutron matter in a strong magnetic field
doi: 10.1103/PhysRevC.80.065801
2006IS03 Phys.Atomic Nuclei 69, 1220 (2006) Antiferromagnetism of Nuclear Matter in the Model with Effective Gogny Interaction
doi: 10.1134/S1063778806070209
2004IS02 Phys.Rev. C 69, 025801 (2004) Spin polarized states in strongly asymmetric nuclear matter
doi: 10.1103/PhysRevC.69.025801
2004IS06 Nucl.Phys. A734, E112 (2004) A.A.Isayev, S.I.Bastrukov, J.Yang Pairing effects in low density domain of nuclear matter
doi: 10.1016/j.nuclphysa.2004.03.033
2004IS15 Yad.Fiz. 67, 1867 (2004); Phys.Atomic Nuclei 67, 1840 (2004) A.A.Isayev, S.I.Bastrukov, J.Yang np Pairing Correlations in Low-Density Region of Nuclear Matter
doi: 10.1134/1.1811188
2004IS17 Phys.Rev. C 70, 064310 (2004) Antiferromagnetic spin phase transition in nuclear matter with effective Gogny interaction
doi: 10.1103/PhysRevC.70.064310
2004PU01 J.Radioanal.Nucl.Chem. 260, 143 (2004) Cross section measurements for (n, p) and (n, 2n) reactions of rare-earth isotopes at neutron energies from 13.5 to 14.6 MeV NUCLEAR REACTIONS 142,148,150Nd(n, 2n), E=13.5-14.6 MeV; 146Nd, 141Pr, 139La, 158Gd(n, p), E=13.5-14.6 MeV; measured σ. Activation technique, comparison with previous results.
doi: 10.1023/B:JRNC.0000027073.70271.99
2003PU08 Appl.Radiat.Isot. 58, 723 (2003) Cross-section measurements for (n, 2n), (n, p) and (n, n'α) reactions on gallium isotopes in the neutron energy range of 13.5 - 14.6 MeV NUCLEAR REACTIONS 69Ga(n, 2n), (n, p), E=13.5-14.6 MeV; 71Ga(n, p), (n, n'α), E=13.5-14.6 MeV; measured σ. Activation technique.
doi: 10.1016/S0969-8043(03)00090-3
2000WA16 Phys.Rev. C61, 064904 (2000) F.Wang, H.Liu, H.Sorge, N.Xu, J.Yang Systematic Study of the Kaon to Pion Multiplicity Ratios in Heavy-Ion Collisions NUCLEAR REACTIONS 1H(p, X), E(cm)=4-20 GeV; 197Au(197Au, X), Pb(Pb, X), E(cm)=1-200 GeV/nucleon; calculated kaon-to-pion multiplicity ratios. Relativistic quantum molecular dynamics model, comparisons with data.
doi: 10.1103/PhysRevC.61.064904
1999CH18 Int.J.Mod.Phys. E8, 159 (1999) Light Baryon Spectrum in a Chiral Quark Model
doi: 10.1142/S0218301399000124
1999KO06 Appl.Radiat.Isot. 50, 361 (1999) X.Kong, R.Wang, Y.Wang, J.Yang Cross Sections for 13.5-14.7 MeV Neutron Induced Reactions on Palladiim Isotopes NUCLEAR REACTIONS 102,105,106Pd(n, p), 106,108Pd(n, α), 102,110Pd(n, 2n), E=13.5-14.7 MeV; measured σ. Activation technique.
doi: 10.1016/S0969-8043(97)10144-0
1998KO37 Appl.Radiat.Isot. 49, 1529 (1998) Cross Sections for (n, 2n), (n, p) and (n, α) Reactions on Rare-Earth Isotopes at 14.7 MeV NUCLEAR REACTIONS 154Sm, 162Er, 168Yb, 174,176Hf(n, 2n), 142Ce, 144,148,150Sm, 160,162,163Dy, 166,167,168Er, 174Yb(n, p), 150,152,154Sm, 159Tb, 153Eu, 162,164Dy, 168Er, 169Tm, 178,180Hf(n, α), E=14.7 MeV; measured σ. Activation technique. Comparison with previous measurements.
doi: 10.1016/S0969-8043(98)00018-9
1998KO59 Radiochim.Acta 81, 63 (1998) X.Kong, Y.Wang, R.Wang, J.Yuan, J.Yang Cross Section Measurements for (n, d*), (n, t) and (n, n'α) Reactions at 14 MeV NUCLEAR REACTIONS 92Mo, 106Cd, 142Ce(n, d), (n, np), 46Ti, 54Fe, 58Ni, 90Zr, 92Mo, 204Pb(n, t), 51V, 65Cu, 92Mo, 182W(n, n'α), E ≈ 14.7 MeV; measured activation σ. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32515. 1998YA17 Nucl.Instrum.Methods Phys.Res. A413, 239 (1998) New Data on Alpha-Particle Emission Probabilities of Several Actinide Nuclides RADIOACTIVITY 233U, 238Pu, 242,244Cm, 241,243Am(α); measured α spectra, emission probability.
doi: 10.1016/S0168-9002(98)00147-8
1997KO44 Radiochim.Acta 76, 11 (1997) X.Kong, Y.Wang, J.Yang, J.Yuan Cross Sections for (n, p), (n, α) and (n, 2n) Reactions on Rare-Earth Isotopes at 14.7 MeV NUCLEAR REACTIONS 140Ce, 153Eu, 159Tb, 172,173Yb(n, p), E=14.7 MeV; 151Eu, 174Yb(n, α), E=14.7 MeV; 136,138,140,142Ce, 156,158Dy, 169Tm, 170,176Yb, 176Hf(n, 2n), E=14.7 MeV; measured σ. Activation technique. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31763. 1994XI05 Proc.Intern.Conf.Nuclear Data for Science and Technology, Gatlinburg, Tennesse, 9-13 May, 1994, J.K.Dickens, Ed., American Nuclear Society, Vol.1, p.251 (1994) Y.J.Xia, X.-G.Long, X.-B.Luo, Z.Yang, M.Liu, F.He, C.Wang, X.F.Pen, J.Yang Activation cross section measurement for the Eu-(n, γ) reactions NUCLEAR REACTIONS 151Eu(n, γ), 153Eu(n, γ), E=22 keV-1.1 MeV; measured products, 152Eu, Eγ, Iγ; deduced σ, σ(E). Data were imported from EXFOR entry 32623.
1994YA12 Nucl.Instrum.Methods Phys.Res. A338, 498 (1994) Analysis Technique of Multiplet Alpha Spectra RADIOACTIVITY 241Am, 244Cm(α); calculated α-emission probabilities. 240,239Pu(α); calculated activity ratio in Pu samples. Multiplet α-spectra analysis.
doi: 10.1016/0168-9002(94)91333-1
1994YU02 Chin.J.Nucl.Phys. 16, No 1, 59 (1994) J.Yuan, X.Kong, J.Yang, Y.Wang Cross Section Measurement for 108Cd(n, p)108mAg Reaction NUCLEAR REACTIONS 108Cd(n, p), E=14.6 MeV; measured residual isomer production σ. Activation technique.
1993LI53 Nucl.Instrum.Methods Phys.Res. A336, 150 (1993) Z.Li, Y.Cheng, C.Yan, J.Yang, Q.Zhang, S.Li, K.Zhao, X.Lu, C.Jiang Beijing Q3D Magnetic Spectrometer and Its Applications NUCLEAR REACTIONS 56Fe(α, α'), E=35 MeV; 152Sm(12C, 12C), (12C, 12C'), E=63.2 MeV; measured particle momentum spectra. Q3D magnetic spectrometer.
doi: 10.1016/0168-9002(93)91091-Z
1993ZH19 Chin.J.Nucl.Phys. 15, No 1, 39 (1993) Y.Zhang, J.Yang, J.He, J.Zhang Breakup Energy of Singlet Deuteron Measured for d + d → d(*) + d(*) Four-Body Reaction at 15.7 MeV NUCLEAR REACTIONS 2H(d, X), E=15.7 MeV; measured particle spectra following 4-body breakup; deduced singlet deuteron breakup energy. Kinematically complete experiment.
1992KO17 Chin.J.Nucl.Phys. 14, No 3, 239 (1992) X.Kong, Y.Wang, J.Yang, J.Yuan, X.Wang Cross Section Measurements for 98Mo(n, α)95Zr, 95Mo(n, p)95mNb, 95Mo(n, p)95gNb and 181Ta(n, p)181Hf Reactions NUCLEAR REACTIONS 98Mo(n, α), 95Mo, 181Ta(n, p), E=13.5-14.8 MeV; measured σ(E). Activation technique, 27Al(n, α), 93Nb(n, 2n) standard reactions.
1992WA17 Nucl.Sci.Eng. 111, 314 (1992) Y.Wang, J.Yuan, J.Yang, H.Wang, Y.Shui, Z.Ren Cross-Section Measurement for 109Ag(n, 2n)108mAg Reaction NUCLEAR REACTIONS 109Ag(n, 2n), E=13.64-14.8 MeV; measured σ relative 93Nb(n, 2n) reaction. Activation method.
doi: 10.13182/NSE92-A23944
1991LU08 Phys.Rev. A44, 1843 (1991) F.Lu, S.Wu, Y.Wang, W.Shi, P.Shi, L.Song, J.Yang, J.Tang, T.Yang Optical Isotope Shifts in the 5702-Angstrom Line of Nd II by Collinear Fast-Beam-Laser Spectroscopy NUCLEAR MOMENTS 142,144,146,148,150Nd; measured optical isotope shift; deduced rms charge radii changes. Collinear fast-beam laser spectroscopy.
doi: 10.1103/PhysRevA.44.1843
1991LU10 Chin.J.Nucl.Phys. 13, No 3, 203 (1991) H.Lu, W.Yu, W.Zhao, Y.Zhao, Y.Wang, J.Yuan, H.Wang, Z.Ren, J.Yang, Z.Shi Research of Activation Cross Sections for Long-Lived Radionuclides on Elements of Cu, Mo, Ag, Eu and Tb NUCLEAR REACTIONS 109Ag, 151,153Eu, 159Tb(n, 2n), E=14 MeV; measured reaction σ. Activation method. Evaporation plus preequilibrium exciton model analyses.
1990WA15 Chin.J.Nucl.Phys. 12, No 1, 89 (1990) C.Wang, Y.Xia, J.Yang, Z.Yang, S.Wang Measurement of Neutron Capture Cross Sections of Natural Hafnium NUCLEAR REACTIONS Hf(n, γ), E=10-100 keV; measured σ(E). Gold standard.
1990XI04 Chin.J.Nucl.Phys. 12, No 3, 261 (1990) Y.Xia, C.Wang, J.Yang, Z.Yang, M.Liu Measurement of Maxwellian Averaged Neutron Capture Cross Section of 140,142Ce, 139La and 181Ta at kT = 24 keV NUCLEAR REACTIONS 140,142Ce, 139La, 181Ta(n, γ), E ≤ 250 keV; measured Eγ, Iγ following capture; deduced Maxwellian averaged capture σ. Hyperpure Ge detector.
1990XI06 Chin.J.Nucl.Phys. 12, No 4, 375 (1990) Y.Xia, C.Wang, J.Yang, Z.Yang, S.Wang Measurement of Neutron Capture Cross Section of Wolfram NUCLEAR REACTIONS W(n, γ), E=11.2-99.9 keV; measured capture σ(E).
1989WA34 Chin.J.Nucl.Phys. 11, No. 4, 63 (1989) C.Wang, Y.Xia, J.Yang, Z.Yang, S.Wang Measurement of Neutron Capture Cross Sections of Ag in Energy Range from 10 to 100 keV NUCLEAR REACTIONS Ag(n, γ), E=0.01-0.1 MeV; measured capture σ(E).
1989XI01 Chin.J.Nucl.Phys. 11, No.2, 75 (1989) Y.Xia, J.Yang, Z.Yang, W.Zhao, W.Yu Measurement of Neutron Capture Cross Sections of 169Tm in the Energy Range from 10 to 100 keV NUCLEAR REACTIONS 169Tm(n, γ), E=10-100 keV; measured capture σ(E).
1988XI02 Chin.J.Nucl.Phys. 10, 102 (1988) Xia Yijun, Yang Jingfu, Yang Zhihua, Zhao Wenrong, Yu Weixiang Measurement of the Neutron Capture Cross Section of 169Tm in the Energy Range from 10 to 100 keV NUCLEAR REACTIONS 169Tm(n, γ), E=10-100 keV; measured capture σ(E). Moxon-Rae detector, 197Au standard. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30998. 1988XI03 Chin.J.Nucl.Phys. 10, 227 (1988) Xia Yijun, Yang Jingfu, Guo Huachong, Wang Minhua, Xie Bizheng, Wang Shimin Measurement of the Neutron Capture Cross Section of 93Nb NUCLEAR REACTIONS 93Nb(n, γ), E=10-100 keV; measured capture σ(E). Moxon-Rae detectors, 197Au as standard. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32504. 1987CH23 J.Radioanal.Nucl.Chem. 111, 63 (1987) Chen Qingjiang, Su Shuxin, Guo Jinru, Yang Jingxia, Chen Yundong, Li Xueliang, Zhang Hongdi, Lin Fa, Sun Shuying, Zhang Shulan Absolute Determination of the Spontaneous Fission Yield of 252Cf by Radiochemical Method RADIOACTIVITY 252Cf(SF); measured fission fragment absolute yields vs mass; deduced average neutron number per fission. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30793. 1987LI23 Chin.J.Nucl.Phys. 9, 207 (1987) Liu Genbao, Yang Jingqin, Jiang Dazhen, Zhang Yingchi, Xu Nu, Xu Jianjun, Cheng Xiaowu Study of p-p Quasi-Free Scattering in the Reaction D(p, pp)n NUCLEAR REACTIONS 2H(p, 2p), E=7.3-16.5 MeV; measured σ(E1, θ1, θ2). Enriched target. Impulse approximation.
1987ZH11 Scientica Sinica 30, 826 (1987) Zhang Yinghi, Liu Genbao, Jiang Dazhen, Yang Jinqing, Xu Nu, Xu Jianjun 2He Intermediate Process in the Reaction of D(d, 2He)2n at 15.7 MeV NUCLEAR REACTIONS, MECPD 2H(d, 2p), E=15.7 MeV; measured σ(Ep, θp1, θp2); deduced 2He resonant state.
1981YA11 Chin.J.Nucl.Phys. 3, 373 (1981) Yang Jinqing, Ni Xinbo, Chang Yingji, Cheng Xiaowu Angular Distributions of (α, p) Reactions by 31.2 MeV α Particles NUCLEAR REACTIONS 51V, Fe, 59Co(α, p), E=31.2 MeV: measured σ(θ). Legendre polynominal analysis.
1980YA12 Chin.J.Nucl.Phys. 2, 155 (1980) Yang Jinqing, Ni Xinbai, Chang Yingqi, Jiang Dazhen, Cheng Xiaowu (α, p) Reactions Induced by 31.2 MeV α Particles NUCLEAR REACTIONS Al, V, Fe, Co(α, p), E=31.2 MeV; measured σ(Ep); deduced equilibrium, preequilibrium components. Statistical, hybrid models.
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