NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = Z.Zhao Found 105 matches. Showing 1 to 100. [Next]2024LI17 Phys.Rev. C 109, 034310 (2024) C.B.Li, Y.Zheng, T.X.Li, X.G.Wu, H.Y.Wu, M.Zheng, Z.H.Zhao, Y.Q.Li, R.Hong, Z.Y.He, J.Z.Li, J.L.Wang, C.Y.Guo, Z.X.Zhou, L.Ni, G.S.Li, X.H.Zhou, B.Guo, S.Y.Wang, M.L.Liu, Y.H.Zhang, C.Y.He, F.L.Liu, S.Wang, L.H.Zhu Lifetime measurements of the first 2+ states in 116, 118Te
doi: 10.1103/PhysRevC.109.034310
2024TE03 Phys.Rev. C 109, 034308 (2024) J.X.Teng, K.Y.Ma, J.B.Lu, H.C.Zhang, H.Wang, S.Y.Liu, D.Zhao, H.Y.Ye, J.Y.Li, X.J.Zhao, Z.H.Zhao, Y.C.Hao, Z.Qiao, Y.J.Ma, D.Yang, X.G.Wu, Y.Zheng, C.B.Li Possible multiple chiral doublet bands in odd-odd 128La
doi: 10.1103/PhysRevC.109.034308
2024WA14 Phys.Lett. B 850, 138503 (2024) J.G.Wang, Z.G.Gan, Z.Y.Zhang, M.H.Huang, L.Ma, M.M.Zhang, H.B.Yang, C.L.Yang, Y.H.Qiang, X.Y.Huang, Z.Zhao, S.Y.Xu, Z.C.Li, L.X.Chen, L.C.Sun, H.Zhou, X.Zhang, X.L.Wu, Y.L.Tian, Y.S.Wang, J.Y.Wang, W.X.Huang, M.L.Liu, Z.W.Lu, Y.He, Z.Z.Ren, S.G.Zhou, X.H.Zhou, H.S.Xu, V.K.Utyonkov, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov α-decay properties of new neutron-deficient isotope 203Ac RADIOACTIVITY 203Ac, 199Fr, 195At, 191Bi(α) [from 169Tm(40Ca, 6n)203Ac, E=226 MeV]; measured decay products, Eα, Iα; deduced α-particle energies, transitions T1/2, J, π, partial decay scheme, reduced α-decay widths, proton separation energies, the onset of deformation in neutron-deficient Ac isotopes. Comparison with systematics. The superconducting linear accelerator, China Accelerator Facility for superheavy Elements (CAFE2) at Institute of Modern Physics, Chinese Academy of Sciences.
doi: 10.1016/j.physletb.2024.138503
2024YA04 Phys.Rev.Lett. 132, 072502 (2024) H.B.Yang, Z.G.Gan, Y.J.Li, M.L.Liu, S.Y.Xu, C.Liu, M.M.Zhang, Z.Y.Zhang, M.H.Huang, C.X.Yuan, S.Y.Wang, L.Ma, J.G.Wang, X.C.Han, A.Rohilla, S.Q.Zuo, X.Xiao, X.B.Zhang, L.Zhu, Z.F.Yue, Y.L.Tian, Y.S.Wang, C.L.Yang, Z.Zhao, X.Y.Huang, Z.C.Li, L.C.Sun, J.Y.Wang, H.R.Yang, Z.W.Lu, W.Q.Yang, X.H.Zhou, W.X.Huang, N.Wang, S.G.Zhou, Z.Z.Ren, H.S.Xu Discovery of New Isotopes 160Os and 156W: Revealing Enhanced Stability of the N=82 Shell Closure on the Neutron-Deficient Side NUCLEAR REACTIONS 106Cd(58Ni, 4n)160Os, E=335 MeV; measured reaction products; deduced new isotopes, σ. The Spectrometer for Heavy Atoms and Nuclear Structure (SHANS), the Sector Focusing Cyclotron of the Heavy Ion Research Facility in Lanzhou (HIRFL), China. RADIOACTIVITY 160Os(α), 156W(β+); measured decay products, Eα, Iα; deduced α-particles energies, Q-values, T1/2, α-decay reduced widths, N=82 shell closure toward the proton drip line. Comparison with theoretical calculations.
doi: 10.1103/PhysRevLett.132.072502
2024ZH04 Phys.Rev. C 109, 014608 (2024) M.M.Zhang, Z.Y.Zhang, Z.G.Gan, N.Wang, H.Yao, J.G.Wang, M.H.Huang, L.Ma, H.B.Yang, C.L.Yang, Y.L.Tian, Y.S.Wang, J.Y.Wang, Y.H.Qiang, X.L.Wu, S.Y.Xu, X.Y.Huang, Z.C.Li, Z.Zhao, L.C.Sun, H.Zhou, X.Zhang, G.Xie, L.Zhu, J.H.Zheng, Y.J.Li, F.Guan, Z.W.Lu, W.X.Huang, Y.He, H.S.Xu, Z.Z.Ren, S.G.Zhou Experimental cross section study of 40Ca + 175Lu: Searching for new neutron-deficient Pa isotopes
doi: 10.1103/PhysRevC.109.014608
2024ZH19 Phys.Rev. C 109, 034314 (2024) Z.Zhao, Z.G.Gan, Z.Y.Zhang, J.G.Wang, M.H.Huang, L.Ma, H.B.Yang, M.M.Zhang, C.L.Yang, S.Y.Xu, X.Y.Huang, Z.C.Li, L.C.Sun, X.L.Wu, Y.S.Wang, Y.L.Tian, Y.H.Qiang, J.Y.Wang, W.X.Huang, Y.He, L.T.Sun, V.K.Utyonkov, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov Reinvestigation of the decay properties of 261, 262Bh at the gas-filled recoil separator SHANS2
doi: 10.1103/PhysRevC.109.034314
2023CH24 Chin.Phys.C 47, 054001 (2023) l.Chen, S.Xu, Z.Zhang, J.Wang, M.Huang, M.Zhang, L.Ma, H.Yang, C.Yang, X.Wu, H.Zhou, Z.Zhao, X.Huang, H.Zhou, X.Zhang, L.Sun, Z.Li, Z.Gan Reaction 55Mn + 159Tb : preparation for the synthesis of new elements NUCLEAR REACTIONS 159Tb(55Mn, X)210TH/211Th, E=257; measured reaction products, Eα, Iα. 292119, 295120; deduced σ. A gas-filled recoil separator known as the Spectrometer for Heavy Atoms and Nuclear Structure-2 (SHANS2) at CAFE2 in Lanzhou, China. RADIOACTIVITY 210,211Th(α); measured decay products, Eα, Iα; deduced α-particle energies and T1/2, equilibrium charge state of the recoiled nucleus 210Th. Comparison with available data.
doi: 10.1088/1674-1137/acb9e2
2023ZH14 Phys.Rev. C 107, 044310 (2023) Z.H.Zhao, C.B.Li, K.Y.Ma, X.G.Wu, Y.Zheng, Y.K.Pan, J.L.Wang, H.C.Zhang, Y.C.Hao, X.F.Li, G.S.Li, S.H.Yao, C.Y.He, B.B.Yu, X.P.Cao, S.P.Hu, J.B.Lu, Y.J.Ma, D.Yang, H.D.Wang, G.Y.Liu, L.Li, C.Xu, Y.Y.Cheng Possible antimagnetic rotational band in 114In NUCLEAR REACTIONS 110Pd(7Li, 3n)114In, E=26 MeV; analyzed Eγ, Iγ, γγ-coin, γγ(θ)(DCO) data from an experiment reported by 2011Li43 in Eur. Phys. Jour. A 47, 191 (2011) at the HI-13 tandem accelerator of CIAE, Beijing. 114In; deduced high-spin levels, Jπ, multipolarities, bands, possible anti-magnetic rotational band, spherical configurations; predicted B(E2) and I2/B(E2) from classical particle-rotor model calculations. Systematics of yrast states in 102,104,106,108,110Ag and 104,106,108,110,112,114In.
doi: 10.1103/PhysRevC.107.044310
2023ZH38 Phys.Rev. C 108, 024314 (2023) H.C.Zhang, K.Y.Ma, J.X.Teng, Z.H.Zhao, H.Wang, S.Y.Liu, Y.C.Hao, J.B.Lu, Y.J.Ma, D.Yang, X.G.Wu, Y.Zheng, C.B.Li New positive-parity bands in 110Ag and systematic studies in silver isotopes NUCLEAR REACTIONS 110Pd(7Li, X)110Ag, E=65 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ). 110Ag; deduced levels, J, π, high-spin states, δ, DCO ratios, positive-parity rotational bands structure, B(M1)/B(E2) ratios for inside band transitions, configurations. Systematics of alignment for the bands, B(M1)/B(E2) ratios and energy staggering parameters in 105Ag, 106Ag, 107Ag, 108Ag, 109Ag, 110Ag. Comparison to particle-rotor model and geometrical model based calculations. Investigated signature inversion in odd-odd and odd-A silver isotopes. Array consisting of 9 Compton-suppressed HPGe detectors, 2 planar-type HPGe detectors, and 1 clover detector at HI-13 tandem accelerator of China Institute of Atomic Energy (CIAE).
doi: 10.1103/PhysRevC.108.024314
2022HO01 J.Phys.(London) G49, 010502 (2022) C.R.Howell, M.W.Ahmed, A.Afanasev, D.Alesini, J.R.M.Annand, A.Aprahamian, D.L.Balabanski, S.V.Benson, A.Bernstein, C.R.Brune, J.Byrd, B.E.Carlsten, A.E.Champagne, S.Chattopadhyay, D.Davis, E.J.Downie, J.M.Durham, G.Feldman, H.Gao, C.G.R.Geddes, H.W.Griesshammer, R.Hajima, H.Hao, D.Hornidge, J.Isaak, R.V.F.Janssens, D.P.Kendellen, M.Kovash, P.P.Martel, U.-G.Meissner, R.Miskimen, B.Pasquini, D.R.Phillips, N.Pietralla, D.Savran, M.R.Schindler, M.H.Sikora, W.M.Snow, R.P.Springer, C.Sun, C.Tang, B.Tiburzi, A.P.Tonchev, W.Tornow, C.A.Ur, D.Wang, H.R.Weller, V.Werner, Y.K.Wu, J.Yan, Z.Zhao, A.Zilges, F.Z.Zomer International workshop on next generation gamma-ray source
doi: 10.1088/1361-6471/ac2827
2022HU12 Phys.Lett. B 834, 137484 (2022) M.H.Huang, Z.G.Gan, Z.Y.Zhang, L.Ma, J.G.Wang, M.M.Zhang, H.B.Yang, C.L.Yang, X.Y.Huang, Z.Zhao, S.Y.Xu, L.X.Chen, X.J.Wen, Y.F.Niu, C.X.Yuan, Y.L.Tian, Y.S.Wang, J.Y.Wang, M.L.Liu, Y.H.Qiang, W.Q.Yang, H.B.Zhang, Z.W.Lu, S.Guo, W.X.Huang, Y.He, Z.Z.Ren, S.G.Zhou, X.H.Zhou, H.S.Xu, V.K.Utyonkov, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov α decay of the new isotope 204Ac RADIOACTIVITY 204,205Ac(α) [from 169Tm(40Ca, xn), E=202, 210, 212, 214 MeV using SHANS2 separator at CAFE2 and SHANS separator at HRIFL, Lanzhou accelerator facility]; 200Fr, 196At(α) [from 204Ac α-decay chain]; measured evaporation residues (ERs), Eα, (ER)α-α-α correlated events, production cross sections, T1/2 of decays using two multiwire proportional counters for implanted events, double-sided silicon strip detectors (DSSSDs) for α particles, and a segmented clover Ge detector for γ radiation. 204,205Ac, 200Fr, 196At; deduced T1/2 of decays of ground-state decays, and Eα values, reduced α-width in Rasmussen formalism, favored α decay for 204Ac decay. 204Ac(p); no proton decay events observed. 201,201m,202,202m,203,204,205Fr, 204,205,206Ra(α); observed α spectra, (ERs)-α-α-correlated events. Comparison with previous available experimental results. Systematics of experimental and theoretical T1/2 and Q(α) values for 196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211At, 198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213Fr, 203,204,205,206,207,208,209,210,211,212,213,214,215Ac, 211,212,213,214,215,216,217Pa, using Hartree-Fock-BCS (HFBSC) method, and macroscopic-microscopic (MM) mass formula for theory.
doi: 10.1016/j.physletb.2022.137484
2022KA37 Eur.Phys.J. A 58, 185 (2022) A.Kaewsnod, K.Xu, Z.Zhao, X.Liu, S.Srisuphaphon, A.Limphirat, Y.Yan Study of N(1520) and N(1535) structures via γ* p → N* transitions
doi: 10.1140/epja/s10050-022-00837-0
2022LI18 Phys.Rev.Lett. 128, 132502 (2022) X.Li, M.W.Ahmed, A.Banu, C.Bartram, B.Crowe, E.J.Downie, M.Emamian, G.Feldman, H.Gao, D.Godagama, H.W.Griesshammer, C.R.Howell, H.J.Karwowski, D.P.Kendellen, M.A.Kovash, K.K.H.Leung, D.M.Markoff, J.A.McGovern, S.Mikhailov, R.E.Pywell, M.H.Sikora, J.A.Silano, R.S.Sosa, M.C.Spraker, G.Swift, P.Wallace, H.R.Weller, C.S.Whisnant, Y.K.Wu, Z.W.Zhao Proton Compton Scattering from Linearly Polarized Gamma Rays NUCLEAR REACTIONS 1H(polarized γ, γ'), E=83.4 MeV; measured reaction products, Eγ, Iγ; deduced σ(θ), electromagnetic dipole polarizabilities of the proton. The High Intensity Gamma-Ray Source facility at the Triangle Universities Nuclear Laboratory.
doi: 10.1103/PhysRevLett.128.132502
2022MA45 Phys.Rev. C 106, 064316 (2022) L.Ma, H.B.Yang, Z.Y.Zhang, J.C.Pei, M.H.Huang, M.M.Zhang, C.Y.Qiao, X.J.Bao, Y.L.Tian, C.L.Yang, Y.S.Wang, Z.Zhao, X.Y.Huang, S.Y.Xu, W.X.Huang, Z.Liu, X.H.Zhou, Z.G.Gan Attempts to produce new americium isotopes near N=126 NUCLEAR REACTIONS 191,193Ir(40Ar, xn)231Am*/233Am*, E=190-204 MeV; measured reaction products, Eα, (recoils)α-α-α correlated events, using SHANS gas-filled recoil separator, 16 position-sensitive Si-strip detectors (PSSDs) for evaporation residues, and eight side silicon detectors (SSDs) for α particles at the HRIFL-Lanzhou facility. 226,227,228Am; no evidence found for the detection of these nuclides, with upper limits of cross sections determined for the production of the compound nuclei of 231Am and 233Am; discussed nonobservation of new americium isotopes in terms of reduced survival probabilities of compound nuclei 231Am and 233Am due to their low fission barriers at high excitations. NUCLEAR STRUCTURE 226,227,228,229Am; calculated excitation functions for the production of these nuclides in 191,193Ir(40Ar, xn) using the statistical model code HIVAP. 230,231,232,233,234,235,236Am; evaluated shell correction energies and fission barriers from FRDM2012, KTUY2005, and WS2010. 226U, 227Np, 231,233Am; calculated fission barrier heights as functions of excitation energy and quadrupole deformation parameter β2 using microscopic finite-temperature Skyrme Hartree-Fock+BCS theory.
doi: 10.1103/PhysRevC.106.034316
2022YA27 Phys.Rev. C 106, 064311 (2022) H.B.Yang, Z.G.Gan, Z.Y.Zhang, M.H.Huang, L.Ma, M.M.Zhang, C.L.Yang, Y.L.Tian, Y.S.Wang, H.B.Zhou, X.J.Wen, J.G.Wang, Z.Zhao, S.Y.Xu, L.X.Chen, X.Y.Huang, C.X.Yuan, Y.F.Niu, H.R.Yang, W.X.Huang, Z.Liu, X.H.Zhou, Y.H.Zhang, S.G.Zhou, Z.Z.Ren, H.S.Xu, V.K.Utyonkov, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov, D.I.Solovyev Examining the impact of α-decay energies on the odd-even staggering in half-lives: α-decay spectroscopy of 207-209Ac RADIOACTIVITY 207,208,208m,209Ac(α)[from 176Hf(36Ar, X), E=197-199 MeV]; measured evaporation residues (ER), Eα, Iα, αα-coin, (ER)αα-coin; deduced T1/2, Q values, decay branches. 204mFr(IT) [from 208Ac(α)]; deduced T1/2, isomer level energy, tentative J and π for the newly found 80-keV isomer. 204Fr(α)[from 208,208mAc(α)]; deduced T1/2. Found new α-decay branching 208Ac and assigned to the transition from ground state to the excited (2+, 4+) state. Comparison to the calculations performed in the framework of Wentzel-Kramers-Brillouin approximation. Spectrometer for Heavy Atoms and Nuclear Structure (SHANS) at Sector Focusing Cyclotron of the Heavy Ion Research Facility in Lanzhou (HIRFL).
doi: 10.1103/PhysRevC.106.064311
2022ZH45 Phys.Rev. C 106, 024305 (2022) M.M.Zhang, Y.L.Tian, Y.S.Wang, Z.Y.Zhang, Z.G.Gan, H.B.Yang, M.H.Huang, L.Ma, C.L.Yang, J.G.Wang, C.X.Yuan, C.Qi, A.N.Andreyev, X.Y.Huang, S.Y.Xu, Z.Zhao, L.X.Chen, J.Y.Wang, M.L.Liu, Y.H.Qiang, G.S.Li, W.Q.Yang, R.F.Chen, H.B.Zhang, Z.W.Lu, X.X.Xu, L.M.Duan, H.R.Yang, W.X.Huang, Z.Liu, X.H.Zhou, Y.H.Zhang, H.S.Xu, N.Wang, H.B.Zhou, X.J.Wen, S.Huang, W.Hua, L.Zhu, X.Wang, Y.C.Mao, X.T.He, S.Y.Wang, W.Z.Xu, H.W.Li, Y.F.Niu, L.Guo, Z.Z.Ren, S.G.Zhou Fine structure in the α decay of the 8+ isomer in 216, 218U RADIOACTIVITY 216,216m,218,218mU(α)[218U from 182W(40Ar, 4n), E=190 MeV, 184W(40Ca, 2nα), E=206 MeV, 216U from 180W(40Ar, 4n), E=191 MeV]; measured evaporation residues (EVRs), Eα, Iα, (EVR)α1-α2-correlations, T1/2 using position-sensitive strip detectors (PSSDs) for α detection, and SHANS separator at HIRFL-Lanzhou. 216,216m,218,218mU; deduced T1/2, Q-values, α-branching ratio, α-decay hindrance factors. 204Rn, 208,210Ra, 212,214Th(α)[from 216,218U α-decay chains]; measured Eα, T1/2. 212Th; deduced level, J, π, identification of the first 2+ state. 215Ra, 212,213,216Ac, 211,212,213,214,216,216m,217Th, 216,217,217m,218Pa, 217,218,219U; observed Eα from their decays from (EVR)α-correlations. Comparison with previous experimental data.
doi: 10.1103/PhysRevC.106.024305
2021AC08 Eur.Phys.J. A 57, 261 (2021) A.Accardi, A.Afanasev, I.Albayrak, S.F.Ali, M.Amaryan, J.R.M.Annand, J.Arrington, A.Asaturyan, H.Atac, H.Avakian, T.Averett, C.Ayerbe Gayoso, X.Bai, L.Barion, M.Battaglieri, V.Bellini, R.Beminiwattha, F.Benmokhtar, V.V.Berdnikov, J.C.Bernauer, V.Bertone, A.Bianconi, A.Biselli, P.Bisio, P.Blunden, M.Boer, M.Bondi, K.-T.Brinkmann, W.J.Briscoe, V.Burkert, T.Cao, A.Camsonne, R.Capobianco, L.Cardman, M.Carmignotto, M.Caudron, L.Causse, A.Celentano, P.Chatagnon, J.-P.Chen, T.Chetry, G.Ciullo, E.Cline, P.L.Cole, M.Contalbrigo, G.Costantini, A.D'Angelo, L.Darme, D.Day, M.Defurne, M.De Napoli, A.Deur, R.De Vita, N.D'Hose, S.Diehl, M.Diefenthaler, B.Dongwi, R.Dupre, H.Dutrieux, D.Dutta, M.Ehrhart, L.El Fassi, L.Elouadrhiri, R.Ent, J.Erler, I.P.Fernando, A.Filippi, D.Flay, T.Forest, E.Fuchey, S.Fucini, Y.Furletova, H.Gao, D.Gaskell, A.Gasparian, T.Gautam, F.-X.Girod, K.Gnanvo, J.Grames, G.N.Grauvogel, P.Gueye, M.Guidal, S.Habet, T.J.Hague, D.J.Hamilton, O.Hansen, D.Hasell, M.Hattawy, D.W.Higinbotham, A.Hobart, T.Horn, C.E.Hyde, H.Ibrahim, A.Ilyichev, A.Italiano, K.Joo, S.J.Joosten, V.Khachatryan, N.Kalantarians, G.Kalicy, B.Karky, D.Keller, C.Keppel, M.Kerver, M.Khandaker, A.Kim, J.Kim, P.M.King, E.Kinney, V.Klimenko, H.-S.Ko, M.Kohl, V.Kozhuharov, B.T.Kriesten, G.Krnjaic, V.Kubarovsky, T.Kutz, L.Lanza, M.Leali, P.Lenisa, N.Liyanage, Q.Liu, S.Liuti, J.Mammei, S.Mantry, D.Marchand, P.Markowitz, L.Marsicano, V.Mascagna, M.Mazouz, M.McCaughan, B.McKinnon, D.McNulty, W.Melnitchouk, A.Metz, Z.-E.Meziani, S.Migliorati, M.Mihovilovic, R.Milner, A.Mkrtchyan, H.Mkrtchyan, A.Movsisyan, H.Moutarde, M.Muhoza, C.Munoz Camacho, J.Murphy, P.Nadel-Turonski, E.Nardi, J.Nazeer, S.Niccolai, G.Niculescu, R.Novotny, J.F.Owens, M.Paolone, L.Pappalardo, R.Paremuzyan, B.Pasquini, E.Pasyuk, T.Patel, I.Pegg, C.Peng, D.Perera, M.Poelker, K.Price, A.J.R.Puckett, M.Raggi, N.Randazzo, M.N.H.Rashad, M.Rathnayake, B.Raue, P.E.Reimer, M.Rinaldi, A.Rizzo, Y.Roblin, J.Roche, O.Rondon-Aramayo, F.Sabatie, G.Salme, E.Santopinto, R.Santos Estrada, B.Sawatzky, A.Schmidt, P.Schweitzer, S.Scopetta, V.Sergeyeva, M.Shabestari, A.Shahinyan, Y.Sharabian, S.Sirca, E.S.Smith, D.Sokhan, A.Somov, N.Sparveris, M.Spata, H.Spiesberger, M.Spreafico, S.Stepanyan, P.Stoler, I.Strakovsky, R.Suleiman, M.Suresh, P.Sznajder, H.Szumila-Vance, V.Tadevosyan, A.S.Tadepalli, A.W.Thomas, M.Tiefenback, R.Trotta, M.Ungaro, P.Valente, M.Vanderhaeghen, L.Venturelli, H.Voskanyan, E.Voutier, B.Wojtsekhowski, M.H.Wood, S.Wood, J.Xie, W.Xiong, Z.Ye, M.Yurov, H.-G.Zaunick, S.Zhamkochyan, J.Zhang, S.Zhang, S.Zhao, Z.W.Zhao, X.Zheng, J.Zhou, C.Zorn An experimental program with high duty-cycle polarized and unpolarized positron beams at Jefferson Lab
doi: 10.1140/epja/s10050-021-00564-y
2021LA03 Phys.Rev. C 103, 034311 (2021) G.Laskaris, W.Ji, X.Yan, J.Zhou, W.R.Zimmerman, M.W.Ahmed, T.Averett, A.Deltuva, A.C.Fonseca, H.Gao, J.Golak, A.Kafkarkou, H.J.Karwowski, B.Lalremruata, J.Manfredi, J.M.Mueller, P.U.Sauer, R.Skibinski, A.P.Smith, M.B.Tsang, H.R.Weller, H.Witala, Y.K.Wu, Z.W.Zhao First measurement of the asymmetry and the Gerasimov-Drell-Hearn integrand from the 3He((pol)(γ(pol), p)2H reaction at an incident photon energy of 29 MeV NUCLEAR REACTIONS 3He(polarized γ, p)2H, E=29 MeV; measured Ep, Ip, p(θ), time-of-flight, spin-dependent asymmetry and total σ using a circularly polarized, monoenergetic γ-ray beam and a longitudinally polarized 3He target, and an array of depleted silicon surface barrier detectors at the High Intensity γ-ray Source (HIγS) facility at TUNL; deduced contribution from the two-body photo-disintegration to the 3He Gerasimov-Drell-Hearn (GDH) integrands, and compared with the state-of-the art three-nucleon system calculations.
doi: 10.1103/PhysRevC.103.034311
2021MA66 Phys.Rev. C 104, 044310 (2021) L.Ma, Z.Y.Zhang, H.B.Yang, M.H.Huang, M.M.Zhang, Y.L.Tian, C.L.Yang, Y.S.Wang, Z.Zhao, W.X.Huang, Z.Liu, X.H.Zhou, Z.G.Gan α-decay properties of 220Pa RADIOACTIVITY 220,220mPa(α)[from 187Re(40Ar, 3nα), E=198.7 MeV]; 216Ac(α)[from 220Pa(α)]; measured Eα, Iα, half-lives of decays of 220,220mPa using position-sensitive 16-strip detectors (PSSDs) at the Sector-Focusing Cyclotron and SHANS recoil separator of HIRF-Lanzhou. 220Pa, 216Ac; deduced levels, J, π, Q(α), reduced α-width, new isomer in 220Pa. Comparison with previous experimental data. Systematics of reduced α widths of N=129, Z=84-93 isotones.
doi: 10.1103/PhysRevC.104.044310
2021YA06 Nucl.Phys. A1008, 122137 (2021) H.Yang, Z.Zhao, X.Li, H.Yang, X.Bao Predictions for the α decay of proton-rich nuclei in the range of 86 ≤ Z ≤ 98 RADIOACTIVITY 186,188,190,192Rn, 191,195Fr, 193,195,197,199Ra, 195,199,203Ac, 199,201,203,205,207,209,211,213,215,217Th, 201,205,209,213Pa, 203,205,207,209,211,213,217U, 207,211,215,219,223Np, 210,212,214,216,218,220,222,224,226Pu, 213,217,221,225,231,237Am, 216,218,220,222,224,226,228,230,232Cm, 219,223,227,231,235,239Bk, 221,223,225,227,229,231,233,235Cf, 187,189,191Rn, 189,193Fr, 192,194,196,198,200Ra, 197,201Ac, 198,200,202,204,206,208,210,212,214,216,219Th, 203,207,211,215,219Pa, 204,206,208,210,212,214,220U, 209,213,217,221Np, 209,211,213,215,217,219,221,223,225,227Pu, 215,219,223,227,233Am, 215,217,219,221,223,225,227,229,231,235Cm, 221,225,229,233,237,241Bk, 222,224,226,228,230,232,234,236Cf(α); calculated T1/2 using Universal Decay Law (UDL) and MUDL.
doi: 10.1016/j.nuclphysa.2021.122137
2021YA21 Nucl.Phys. A1014, 122250 (2021) H.Yang, Z.Zhao, X.Li, Y.Cai, X.Bao Predictions for the α decay of superheavy nuclei of Z=119-120 isotopes RADIOACTIVITY 284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316119, 287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316120(α); calculated Q-values, T1/2 using unified fission model (UFM) with considering the preformation factor.
doi: 10.1016/j.nuclphysa.2021.122250
2021ZH43 Eur.Phys.J. A 57, 240 (2021) S.Zhao, A.Camsonne, D.Marchand, M.Mazouz, N.Sparveris, S.Stepanyan, E.Voutier, Z.W.Zhao Double deeply virtual Compton scattering with positron beams at SoLID
doi: 10.1140/epja/s10050-021-00551-3
2020CA06 Chin.Phys.C 44, 031001 (2020) J.Cao, G.-y.Huang, Y.-F.Li, Y.Wang, L.-J.Wen, Z.-z.Xing, Z.-h.Zhao, S.Zhou Towards the meV limit of the effective neutrino mass in neutrinoless double-beta decays RADIOACTIVITY 130Te, 136Xe(2β-); analyzed available data; deduced Majorana neutrino mass limits.
doi: 10.1088/1674-1137/44/3/031001
2020CA09 Chin.Phys.C 44, 031001 (2020) J.Cao, G.-yu.Huang, Y.-F.Li, Y.Wang, L.-J.Wen, Z.-z.Xing, Z.-h.Zhao, S.Zhou Towards the meV limit of the effective neutrino mass in neutrinoless double-beta decays RADIOACTIVITY 136Xe(2β-); analyzed available data; deduced importance of neutrino Majorana mass sensitivity in future experiments.
doi: 10.1088/1674-1137/44/3/031001
2020LI10 Phys.Rev. C 101, 034618 (2020) X.Li, M.W.Ahmed, A.Banu, C.Bartram, B.Crowe, E.J.Downie, M.Emamian, G.Feldman, H.Gao, D.Godagama, H.W.Griesshammer, C.R.Howell, H.J.Karwowski, D.P.Kendellen, M.A.Kovash, K.K.H.Leung, D.Markoff, S.Mikhailov, R.E.Pywell, M.H.Sikora, J.A.Silano, R.S.Sosa, M.C.Spraker, G.Swift, P.Wallace, H.R.Weller, C.S.Whisnant, Y.K.Wu, Z.W.Zhao Compton scattering from 4He at the TUNL HIγS facility NUCLEAR REACTIONS 4He(polarized γ, γ), E=81.3 MeV, 100% circularly and linearly polarized γ-ray beam via Compton backscattering from HiγS at TUNL; measured Compton scattered photons at different angles, time-of-flight spectra using an array of large NaI(Tl) detectors; deduced differential σ(θ). Comparison with previous experimental data from Lund at Eγ=87 MeV.
doi: 10.1103/PhysRevC.101.034618
2020ZH32 Phys.Rev. C 102, 035204 (2020) Z.-H.Zhao, H.-Y.Cao, H.-Q.Zhou Two-photon-exchange effects in e+e- → π+π- at small √s
doi: 10.1103/PhysRevC.102.035204
2017GA08 Phys.Rev. C 95, 055202 (2017) H.Gao, H.Huang, T.Liu, J.Ping, F.Wang, Z.Zhao Search for a hidden strange baryon-meson bound state from φ production in a nuclear medium
doi: 10.1103/PhysRevC.95.055202
2017SI26 Phys.Rev. C 96, 055209 (2017) M.H.Sikora, M.W.Ahmed, A.Banu, C.Bartram, B.Crowe, E.J.Downie, G.Feldman, H.Gao, H.W.Griesshammer, H.Hao, C.R.Howell, H.J.Karwowski, D.P.Kendellen, M.A.Kovash, X.Li, D.M.Markoff, S.Mikhailov, V.Popov, R.E.Pywell, J.A.Silano, M.C.Spraker, P.Wallace, H.R.Weller, C.S.Whisnant, Y.K.Wu, W.Xiong, X.Yan, Z.W.Zhao Compton scattering from 4He at 61 MeV NUCLEAR REACTIONS 4He(γ, γ'), E=61 MeV; measured Eγ, Iγ, Compton scattering differential σ(θ) using NaI(Tl) detectors and liquid 4He target at HIγS facility at TUNL. Data interpreted using phenomenological model sensitive to the dipole isoscalar electromagnetic polarizabilities of the nucleon. Comparison with previous experimental data. Benchmarks for future calculations from effective field theories and lattice quantum chromodynamics.
doi: 10.1103/PhysRevC.96.055209
2017XI07 Eur.Phys.J. C 77, 192 (2017) The effective neutrino mass of neutrinoless double-beta decays: how possible to fall into a well
doi: 10.1140/epjc/s10052-017-4777-x
2017ZH42 At.Data Nucl.Data Tables 119, 314 (2017) Z.L.Zhao, K.Wang, S.Li, R.Si, C.Y.Chen, Z.B.Chen, J.Yan, Yu.Ralchenko Multi-configuration Dirac-Hartree-Fock calculations of forbidden transitions within the 3dk ground configurations of highly charged ions (Z = 72-83) ATOMIC PHYSICS Z=72-83; calculated Energy levels and transition rates for the ground states of highly charged ions using an extensive self-consistent multi-configuration Dirac-Hartree-Fock (MCDHF) method.
doi: 10.1016/j.adt.2017.01.002
2015XI04 Eur.Phys.J. C 75, 423 (2015) Z.-z.Xing, Z.-h.Zhao, Y.-L.Zhou How to interpret a discovery or null result of the 0ν2β decay
doi: 10.1140/epjc/s10052-015-3656-6
2014KA56 Sci. Rep. 4, 5484 (2014) D.Kang, H.Sun, J.Dai, W.Chen, Z.Zhao, Y.Hou, J.Zeng, J.Yuan Nuclear quantum dynamics in dense hydrogen
doi: 10.1038/srep05484
2014YE04 At.Data Nucl.Data Tables 100, 1189 (2014) J.Ye, Z.Zhao, Y.Zhu, J.Li, X.Zhang Experimental study of single-electron detachment for Cu-, Ag-, Au-, Co- and Ir- in collisions with Kr and Xe NUCLEAR REACTIONS Cu, Ag, Co, Ir(Kr, e), (Xe, e), E=10-30 keV; measured reaction products, Eβ, Iβ; deduced σ. Comparison with available data.
doi: 10.1016/j.adt.2014.02.005
2013ZH12 Ann.Nucl.Energy 57, 327 (2013) L.Zhang, W.Chen, Z.Zhao, X.Jiang, W.Guo Calculation of effective delayed neutron fraction with modified library of Monte Carlo code NUCLEAR REACTIONS 233U(n, F), E thermal; calculated delayed neutron fraction. Comparison with available data.
doi: 10.1016/j.anucene.2013.02.011
2011GE07 J.Korean Phys.Soc. 59, 1052s (2011) Z.G.Ge, Z.X.Zhao, H.H.Xia, Y.X.Zhuang, T.J.Liu, J.S.Zhang, H.C.Wu The Updated Version of Chinese Evaluated Nuclear Data Library (CENDL-3.1) COMPILATION Z=1-98(n, X), E=1.E-5 eV-20 MeV; compiled, evaluated σ, dσ.
doi: 10.3938/jkps.59.1052
2011WA40 J.Korean Phys.Soc. 59, 1681s (2011) W.M.Wang, X.Li, Z.X.Zhao, Z.Y.Zhou, H.C.Wu, T.F.Wang, G.N.Kim, M.W.Lee, K.S.Kim, M.H.Cho, I.S.Ko, W.Namkung Total Cross-Section Measurements of 169Tm below 100 eV NUCLEAR REACTIONS 169Tm(n, X), E=0.01-100 eV; measured En, In using ToF; deduced σ, transmission coefficients, resonance parameters using R-matrix code SAMMY; calculated, fitted neutron transmission coefficients. Comparison of σ with other data and Mughabghab; resonance parameters with Mughabghab.
doi: 10.3938/jkps.59.1681
2011ZH39 J.Korean Phys.Soc. 59, 1063s (2011) Progress of China Nuclear Data Evaluation COMPILATION 90Zr(n, X), E=0.2-20 MeV; evaluated total σ. 238Pu(n, f); evaluated σ. 238U(n, n'), E not given; evaluated neutron TOF spectra. 16O(n, n), E=14.1 MeV; evaluated σ(E, θ). Compared to other evaluations and data.
doi: 10.3938/jkps.59.1063
2010WA16 Chin.Phys.C 34, 177 (2010) W.-M.Wang, X.Li, Z.-X.Zhao, Z.-Y.Zhou, H.-W.Yu, H.-C.Wu, Y.-X.Wei, T.F.Wang, G.N.Kim, M.W.Lee, K.S.Kim, M.H.Cho, I.S.Ko, W.Namkung Measurement of neutron cross sections and resonance parameters of 169Tm below 100 eV NUCLEAR REACTIONS 169Tm(n, X), E=0.001-100 eV; measured neutron time-of-flight (TOF), En, In; deduced total σ, resonance parameters. Comparison with SAMMY and Atlas of Neutron Resonances.
doi: 10.1088/1674-1137/34/2/004
2009YA25 Chin.Phys.C 33, Supplement 1, 196 (2009) W.-F.Yang, Z.-Z.Zhao, S.-G.Yuan, Y.-B.Xu, X.T.Lu Dependence of the cross sections for Ir isotopes on the values of Qgg in the heavy ion collision NUCLEAR REACTIONS 197Au(12C, X)184Ir/185Ir/186Ir/187Ir/189Ir/190Ir/192Ir/194Ir/195Ir/196Ir, E=47 MeV/nucleon; measured Eγ, Iγ; deduced σ.
doi: 10.1088/1674-1137/33/S1/063
2009ZH07 Phys.Rev. C 79, 024614 (2009); Erratum Phys.Rev. C 79, 049901 (2009) Mass parameters for relative and neck collective motions in heavy ion fusion reactions NUCLEAR REACTIONS 90Zr(90Zr, X), E not given; 110Pd(110Pd, X), E not given; 138Ba(138Ba, X), E not given; calculated mass parameter for relative and neck motion in fusion reaction using microscopic transport model.
doi: 10.1103/PhysRevC.79.024614
2008LU11 Chin.Phys.Lett. 25, 3932 (2008) X.-H.Lu, Y.-X.Zhang, Z.-X.Li, Z.-X.Zhao Equation of State for Isospin Asymmetric Matter of Nucleons and Deltas
doi: 10.1088/0256-307X/25/11/026
2007WI09 Phys.Rev. C 76, 018501 (2007) E.L.Wilds, Jr., R.H.France III, J.E.McDonald, Z.Zhao, M.Gai Upper limits on the first-forbidden rank-one β decay of 20F RADIOACTIVITY 20F(β-); measured Eβ, Eγ, Eα. Deduced first forbidden decay branching ratios.
doi: 10.1103/PhysRevC.76.018501
2004FA02 Nucl.Instrum.Methods Phys.Res. B215, 16 (2004) A semiempirical approach to study the excitation functions for (n, p) reaction on the basis of evaporation and exciton models below 20 MeV NUCLEAR REACTIONS 56Fe, 60Ni, 181Ta, 197Au(n, p), E ≈ 0-20 MeV; calculated σ. Semiempirical approach, comparison with data. COMPILATION A=23-209; compiled, analyzed (n, p) cross sections; deduced parameters.
doi: 10.1016/S0168-583X(03)01819-6
2004FA11 Nucl.Sci.Eng. 147, 63 (2004) S.Fan, X.Shi, F.Yan, H.Zhang, Z.Zhao A Systematics to Investigate the (n, α) Cross Section with Energy Below 20 MeV Based on the Evaporation and Exciton Models NUCLEAR REACTIONS 54Fe, 93Nb, 184W, 197Au(n, α), E < 20 MeV; calculated σ. Evaporation and exciton models, comparison with data. Other targets discussed.
doi: 10.13182/NSE04-A2419
2004FA18 Nucl.Instrum.Methods Phys.Res. B222, 44 (2004) S.Fan, W.Luo, F.Yan, H.Zhang, Z.Zhao MSDM calculations of primary isotopic yields from proton-induced reaction on 208Pb at energy of 1 GeV NUCLEAR REACTIONS 208Pb(p, X), E=1 GeV; calculated spallation fragments isotopic yields. Many stage dynamical model, Ignatyuk formula, comparison with data.
doi: 10.1016/j.nimb.2003.02.018
2003FA15 Nucl.Sci.Eng. 144, 219 (2003) S.Fan, J.Rong, H.Zhang, Z.Zhao The Fragment Distribution of Nb, Au, and Pb from Proton-Induced Reactions with energies Ranging from 100 MeV to 3 GeV NUCLEAR REACTIONS Nb, 197Au, Pb(p, X), E=0.1-3 GeV; calculated fragment mass distributions. Pb(p, X)54Mn/74As/75Se/83Rb/85Sr/96Nb/95mTc/96Tc/101mRu/102Rh/106mAg/110mAg/120Sb/124Sb/119mTe/121mTe/168Tm/196Au/205Bi, E=1.6 GeV; calculated production σ. Many-stage dynamical model, cascade-exciton model, comparison with data.
doi: 10.13182/NSE03-A2355
2003FR32 Phys.Rev. C 68, 057302 (2003) Absolute branching ratio of β-delayed γ-ray emission of 18N RADIOACTIVITY 18N(β-) [from Be(18O, X)]; measured β-delayed Eα, Eγ; deduced absolute branching ratio.
doi: 10.1103/PhysRevC.68.057302
2002FA11 Nucl.Sci.Eng. 142, 195 (2002) Analysis for Cross Sections of (p, xn) Reactions on 208Pb at Intermediate Energies by Using Quantum Molecular Dynamics NUCLEAR REACTIONS 208Pb(p, nX), E=590, 800, 1500 MeV; calculated neutron spectra, σ(E, θ). Quantum molecular dynamics, comparison with data.
doi: 10.13182/NSE02-A2299
2001SC40 Eur.Phys.J. C 21, 473 (2001) H.-Ch.Schroder, A.Badertscher, P.F.A.Goudsmit, M.Janousch, H.J.Leisi, E.Matsinos, D.Sigg, Z.G.Zhao, D.Chatellard, J.-P.Egger, K.Gabathuler, P.Hauser, L.M.Simons, A.J.R.El Hassani The Pion-Nucleon Scattering Lengths from Pionic Hydrogen and Deuterium ATOMIC PHYSICS, Mesic-atoms 1,2H(π-, X), E at rest; measured X-ray spectra; deduced strong-interaction energy level shift, decay widths, pion-nucleon scattering length. NUCLEAR REACTIONS 1,2H(π-, X), E at rest; measured X-ray spectra; deduced strong-interaction energy level shift, decay widths, pion-nucleon scattering length.
2000HE19 Nucl.Instrum.Methods Phys.Res. B172, 177 (2000) M.He, S.Jiang, S.Jiang, Q.Chen, J.Qin, S.Wu, Y.Dong, Z.Zhao Measurement of 79Se and 64Cu with PXAMS RADIOACTIVITY 79Se(β-); 64Cu(EC), (β-); measured X-ray spectra vs time; deduced T1/2. Projectile X-ray accelerator mass spectrometry.
doi: 10.1016/S0168-583X(00)00393-1
2000ZH29 Nucl.Phys. A675, 13c (2000) Z.Zhao, for the BES Collaboration Recent Results from the BES Collaboration
doi: 10.1016/S0375-9474(00)00209-8
1999FA01 Eur.Phys.J. A 4, 61 (1999) Analysis of Proton-Induced Reactions on 208Pb with Incident Energy 590 MeV and 322 MeV NUCLEAR REACTIONS 208Pb(p, xn), (p, xp), E=590 MeV; analyzed σ(En, θ), σ(Ep, θ). 208Pb(p, X), E=322 MeV; analyzed residuals mass, charge distributions; deduced reaction mechanism features. Quantum molecular dynamics calculations.
doi: 10.1007/s100500050204
1999SC40 Phys.Lett. 469B, 25 (1999) H.-Ch.Schroder, A.Badertscher, P.F.A.Goudsmit, M.Janousch, H.J.Leisi, E.Matsinos, D.Sigg, Z.G.Zhao, D.Chatellard, J.-P.Egger, E.Jeannet, K.Gabathuler, P.Hauser, L.M.Simons, A.J.R.El Hassani Determination of the πN Scattering Lengths from Pionic Hydrogen ATOMIC PHYSICS, Mesic-atoms 1H; measured X-ray spectra; deduced pionic hydrogen level energy, width, πN scattering lengths.
doi: 10.1016/S0370-2693(99)01237-X
1998HE36 High Energy Phys. and Nucl.Phys. (China) 22, 1057 (1998) J.He, S.Yuan, W.Yang, Z.Li, T.Ma, K.Fang, S.Shen, Z.Gan, Q.Pan, Z.Chen, T.Guo, W.Mou, D.Su, Y.Xu, J.Guo, H.Liu, L.Shi, Z.Zhao, H.Ma A new isotope of hafnium: 186Hf
1998YU02 Phys.Rev. C57, 1506 (1998) S.Yuan, W.Yang, Z.Li, J.He, T.Ma, K.Fang, S.Shen, Z.Gan, Q.Pan, Z.Chen, T.Guo, W.Mou, D.Su, Y.Xu, J.Guo, H.Liu, L.Shi, Z.Zhao, H.Ma Production and Identification of a New Heavy Neutron-Rich Isotope 186Hf NUCLEAR REACTIONS W(18O, X), E=60 MeV/nucleon; measured Eγ, Iγ(t); deduced evidence for 186Hf. Transfer reaction, chemical separation of source. RADIOACTIVITY 186Hf(β-) [from W(18O, X)]; measured Eγ, Iγ(t), T1/2.
doi: 10.1103/PhysRevC.57.1506
1997BA18 Phys.Lett. 392B, 278 (1997) A.Badertscher, M.Daum, R.Frosch, P.F.A.Goudsmit, W.Hajdas, M.Janousch, P.-R.Kettle, V.Markushin, J.Schottmuller, Z.G.Zhao Experimental Determination of the Kinetic Energy Distribution of π-p Atoms in Liquid Hydrogen NUCLEAR REACTIONS 1H(π-, π0), E at 117 MeV/c; measured neutron tof spectra; deduced π-p-atom kinetic energy distribution in liquid hydrogen. ATOMIC PHYSICS 1H(π-, π0), E at 117 MeV/c; measured neutron tof spectra; deduced π-p-atom kinetic energy distribution in liquid hydrogen.
doi: 10.1016/S0370-2693(96)01545-6
1997CH44 Nucl.Phys. A625, 855 (1997) D.Chatellard, J.-P.Egger, E.Jeannet, A.Badertscher, M.Bogdan, P.F.A.Goudsmit, M.Janousch, H.J.Leisi, E.Matsinos, H.-Ch.Schroder, D.Sigg, Z.G.Zhao, E.C.Aschenauer, K.Gabathuler, P.Hauser, L.M.Simons, A.J.R.El Hassani X-Ray Spectroscopy of the Pionic Deuterium Atom NUCLEAR REACTIONS 1,2H(π-, X), E at 85 MeV/c; measured X-ray spectra; deduced 1S-level strong interaction shift, width, pionic deuterium S-wave scattering length. ATOMIC PHYSICS, Mesic-Atoms 1,2H(π-, X), E at 85 MeV/c; measured X-ray spectra; deduced 1S-level strong interaction shift, width, pionic deuterium S-wave scattering length.
doi: 10.1016/S0375-9474(97)00466-1
1997JA13 Phys.Lett. 414B, 237 (1997) M.Janousch, A.Badertscher, P.F.A.Goudsmit, H.J.Leisi, E.Matsinos, P.Weber, Z.G.Zhao Destructive Interference of s and p Waves in 180° π-p Elastic Scattering NUCLEAR REACTIONS 1H(π-, π-), E=43.6-72 MeV; measured σ(θ); deduced destructive interference.
doi: 10.1016/S0370-2693(97)01169-6
1997YA03 Z.Phys. A357, 353 (1997) W.F.Yang, Z.Z.Zhao, Z.W.Li, W.T.Mou The Decay of 189W RADIOACTIVITY 189W(β-) [from 192Os(n, α), E=14.7 MeV]; measured Eγ, Iγ. 189Re deduced transitions.
doi: 10.1007/s002180050254
1997YA18 High Energy Phys. and Nucl.Phys. (China) 21, 958 (1997) W.Yang, S.Yuan, Z.Li, J.He, T.Ma, K.Fang, S.Shen, Z.Gan, Q.Pan, W.Mou, D.Su, Z.Chen, T.Guo, J.Guo, H.Liu, L.Shi, Z.Zhao, H.Ma A new neutron-rich isotope: 186Hf
1996HU13 Physica C272, 297 (1996) Superconducting Behaviours of Melt Textured Nd(1+x)Ba(2-x)Cu3O(y) Undergoing Heat Treatments in Flowing Argon and Oxygen
doi: 10.1016/S0921-4534(96)00605-3
1996LI46 J.Radioanal.Nucl.Chem. 212, 409 (1996) Yield of Near-Target Product Interaction of 47 MeV/A 12C Ion with Bismuth Targets NUCLEAR REACTIONS, ICPND 209Bi(12C, X)185Pt/186Pt/187Pt/188Pt/189Pt/191Pt/197Pt/197mPt/191Au/192Au/193Au/194Au/195Au/196Au/196mAu/199Au/191Hg/192Hg/193Hg/193mHg/195Hg/195mHg/197Hg/197mHg/203Hg, E=47 MeV/A; measured residuals near-target production, independent, cumulative yields; deduced charge distribution widths.
doi: 10.1007/BF02163286
1996SI21 Nucl.Phys. A609, 269 (1996); Erratum Nucl.Phys. A617, 526 (1997) D.Sigg, A.Badertscher, M.Bogdan, P.F.A.Goudsmit, H.J.Leisi, H.-Ch.Schroder, Z.G.Zhao, D.Chatellard, J.-P.Egger, E.Jeannet, E.C.Aschenauer, K.Gabathuler, L.M.Simons, A.J.R.El Hassani The Strong Interaction Shift and Width of the Ground State of Pionic Hydrogen ATOMIC PHYSICS, Mesic-Atoms 1H(π-, X), E at rest; measured X-ray spectra; deduced strong interaction shift, width.
doi: 10.1016/S0375-9474(96)00280-1
1996YA16 J.Radioanal.Nucl.Chem. 214, 439 (1996) Yield Distribution of Iodine Isotopes Formed by the Interaction of 47 MeV/u 12C with 133Cs NUCLEAR REACTIONS, ICPND 133Cs(12C, X)121I/123I/124I/126I/128I/130I/131I, E=47 MeV/nucleon; measured Eγ, Iγ; deduced production σ. Activation technique.
doi: 10.1007/BF02163831
1995BA19 Nucl.Phys. A585, 49c (1995) A.Badertscher, E.C.Aschenauer, M.Bogdan, D.Chatellard, J.-P.Egger, P.F.A.Goudsmit, K.Gabathuler, P.Hauser, A.J.R.El Hassani, E.Jeannet, M.Janousch, H.J.Leisi, E.Matsinos, H.-Ch.Schroder, D.Sigg, L.M.Simons, Z.G.Zhao Measurement of the Strong Interaction Shift and Width of the 1S State in Pionic Hydrogen ATOMIC PHYSICS, Mesic-Atoms 1H(π-, X), E at rest; measured X-ray spectra; deduced 3P-1S transition energy, line shape. NUCLEAR REACTIONS 1H(π-, X), E at rest; measured X-ray spectra; deduced 3P-1S transition energy, line shape.
doi: 10.1016/0375-9474(94)00542-U
1995CH50 Phys.Rev.Lett. 74, 4157 (1995) D.Chatellard, J.-P.Egger, E.Jeannet, A.Badertscher, M.Bogdan, P.F.A.Goudsmit, H.J.Leisi, E.Matsinos, H.-Ch.Schroder, D.Sigg, Z.G.Zhao, E.C.Aschenauer, K.Gabathuler, P.Hauser, L.M.Simons, A.J.R.El Hassani Determination of the S-Wave Scattering Length in Pionic Deuterium with a High Resolution Crystal Spectrometer NUCLEAR REACTIONS 2H(π-, X), E at 85 MeV/c; measured X-ray spectra; deduced 1S level strong interaction shift, total decay width. ATOMIC PHYSICS, Mesic-Atoms 2H(π-, X), E at 85 MeV/c; measured X-ray spectra; deduced 1S level strong interaction shift, total decay width.
doi: 10.1103/PhysRevLett.74.4157
1995DA25 Phys.Lett. 361B, 179 (1995) M.Daum, R.Frosch, W.Hajdas, M.Janousch, P.-R.Kettle, St.Ritt, Z.G.Zhao Search for a Neutral Particle of Mass 33.9 MeV in Pion Decay
doi: 10.1016/0370-2693(95)01165-M
1995SI25 Phys.Rev.Lett. 75, 3245 (1995) D.Sigg, A.Badertscher, M.Bogdan, P.F.A.Goudsmit, H.J.Leisi, E.Matsinos, H.-Ch.Schroder, Z.G.Zhao, D.Chatellard, J.-P.Egger, E.Jeannet, E.C.Aschenauer, K.Gabathuler, L.M.Simons, A.J.R.El Hassani Strong Interaction Shift and Width of the 1s Level in Pionic Hydrogen NUCLEAR REACTIONS 1H(π-, X), E at rest; measured pionic X-rays; deduced strong interaction shift, width. ATOMIC PHYSICS, Mesic-Atoms 1H(π-, X), E at rest; measured pionic X-rays; deduced strong interaction shift, width.
doi: 10.1103/PhysRevLett.75.3245
1995ZH25 Chin.Phys.Lett. 12, 148 (1995) L.Zhu, Z.Huang, L.Hou, D.Ding, P.Zhang, Z.Zhao Study of Giant Dipole Resonance in Hot Rotating Nucleus 132Ce NUCLEAR REACTIONS 116Sn(16O, X), E=85 MeV; measured γ multiplicity distribution. 132Ce deduced deformation parameter spin dependence, GDR parameters. Hot rotating nucleus.
1995ZH46 Chin.J.Nucl.Phys. 17, No 2, 154 (1995) Calculation of Gamma Production Data from Neutron Induced Reactions on Thirteen Targets NUCLEAR REACTIONS Zn, Zr, Mo, Cd, In, Sb, Hf, Pb, 181Ta, Ti, 197Au(n, n'), (n, γ), (n, 2n), (n, 3n), E ≤ 20 MeV; calculated γ spectra, multiplicities related features.
1994MC10 J.Phys.(London) B27, 5295 (1994) M.R.McNeir, Y.C.Yu, D.L.Weathers, D.K.Marble, Z.Zhao, J.L.Duggan, F.D.McDaniel, G.Lapicki L-Shell X-Ray Production Cross Sections in 26Fe, 28Ni, 29Cu, 30Zn, 31Ga and 32Ge by 0.5 to 8.0 MeV He Ions NUCLEAR REACTIONS Fe, Ni, Cu, Zn, Ga, Ge(α, X), E=0.5-8 MeV; measured L X-ray production σ. Windowless Si(Li) detector. Model comparison. ATOMIC PHYSICS Fe, Ni, Cu, Zn, Ga, Ge(α, X), E=0.5-8 MeV; measured L X-ray production σ. Windowless Si(Li) detector. Model comparison.
doi: 10.1088/0953-4075/27/21/020
1994MO33 Phys.Rev.Lett. 73, 2680 (1994) T.Motobayashi, N.Iwasa, Y.Ando, M.Kurokawa, H.Murakami, J.Ruan, S.Shimoura, S.Shirato, N.Inabe, M.Ishihara, T.Kubo, Y.Watanabe, M.Gai, R.H.France III, K.I.Hahn, Z.Zhao, T.Nakamura, T.Teranishi, Y.Futami, K.Furutaka, Th.Delbar Coulomb Dissociation of 8B and the 7Be(p, γ)8B Reaction at Low Energies NUCLEAR REACTIONS, ICPND 208Pb(8B, p7Be), E=46.5 MeV/nucleon; measured projectile Coulomb dissociation yield; deduced 7Be(p, γ) reaction σ, astrophysical S-factor S17 vs E.
doi: 10.1103/PhysRevLett.73.2680
1994SU30 Phys.Rev. B50, 651 (1994) B.J.Suh, F.Borsa, M.Xu, D.R.Torgeson, W.J.Zhu, Y.Z.Huang, Z.X.Zhao 199Hg Knight Shift and Spin-Lattice Relaxation in HgBa2CuO(4+δ) NUCLEAR MOMENTS 199Hg; measured NMR spectra; deduced Knight shift, spin-lattice relaxation in HgBa2CuO(4+δ).
doi: 10.1103/PhysRevB.50.651
1994ZE06 Phys.Rev. C50, 746 (1994) J.Y.Zeng, Y.A.Lei, T.H.Jin, Z.J.Zhao Blocking Effect and Odd-Even Differences in the Moments of Inertia of Rare-Earth Nuclei NUCLEAR STRUCTURE 155,157,159Eu, 157,159,161,163Tb, 159,161,163,165,167Ho, 163,165,167,169,171,173Tm, 169,171,173,175Lu; analyzed moments of inertia odd-even differences. 160,161,162Dy, 164,165,166Er, 171Lu, 170Yb, 172Hf; calculated bandhead moments of inertia; deduced blocked levels associated features. Particle-number conserving treatment.
doi: 10.1103/PhysRevC.50.746
1994ZE07 Phys.Rev. C50, 1388 (1994) Reduction of Nuclear Moment of Inertia Due to Pairing Interaction NUCLEAR STRUCTURE 160,162,164Dy, 162,164,166,168,170Er, 166,168,170,172,174,176Yb, 170,172,174,176,178,180,182Hf, 176,178,180,182,184,186W; calculated nucleon pairing strengths, ground bands moment of inertia. Cranked shell model, particle number conserving treatment.
doi: 10.1103/PhysRevC.50.1388
1994ZH02 Phys.Rev. C49, R592 (1994) L.Zhang, G.Jin, J.Zhao, W.Yang, Y.Yang, Z.Zhao, J.Zheng, X.Sun, J.Wang, Z.Li, Z.Qin, G.Guo, Y.Luo, J.Zylicz, J.-Y.Zhang Observation of the New Neutron-Rich Nuclide 208Hg NUCLEAR REACTIONS Pb(12C, X), E=30 MeV/nucleon; measured Eγ, Iγ, following 208Tl-decay; deduced evidence for 208Hg, production σ. RADIOACTIVITY 208Hg(β-) [from Pb(12C, X), E=30 MeV/nucleon]; measured Eγ, Iγ, decay curve; deduced T1/2. 208Tl transition deduced T1/2.
doi: 10.1103/PhysRevC.49.R592
1994ZH49 High Energy Phys. and Nucl.Phys. (China) 18, 296 (1994) L.Zhang, G.Jin, J.Zhao, W.Yang, Y.Yang, Z.Zhao, J.Zheng, X.Sun, J.Wang, Z.Li, Z.Qin, G.Guo Identification of 208Hg
1993BA75 Nucl.Instrum.Methods Phys.Res. A335, 470 (1993) A.Badertscher, M.Bogdan, P.F.A.Goudsmit, L.Knecht, H.J.Leisi, H.Ch.Schroder, D.Sigg, Z.G.Zhao, D.Chatellard, J.-P.Egger, E.Jeannet, E.C.Aschenauer, K.Gabathuler, L.M.Simons, A.J.R.El-Hassani A High Resolution Reflecting Crystal Spectrometer to Measure 3 keV Pionic Hydrogen and Deuterium X-Rays NUCLEAR REACTIONS 9Be(π-, X), E at rest; measured pionic X-ray spectra. High resolution crystal spectrometer. ATOMIC PHYSICS, Mesic-Atoms 9Be(π-, X), E at rest; measured pionic X-ray spectra. High resolution crystal spectrometer.
doi: 10.1016/0168-9002(93)91232-C
1993HU13 Chin.J.Nucl.Phys. 15, No 3, 243 (1993) X.Huang, Z.Huang, Z.Zhao, D.Zhou Contribution from Distant Levels to the Neutron Cross Sections NUCLEAR STRUCTURE 60Ni, 177Hf, 56Fe, 234U; analyzed (n, n) data. Picket fence model approach to distant levels contribution.
1993RU05 Phys.Rev. C48, 2078 (1993) S.L.Rugari, R.H.France III, B.J.Lund, Z.Zhao, M.Gai, P.A.Butler, V.A.Holliday, A.N.James, G.D.Jones, R.J.Poynter, R.J.Tanner, K.L.Ying, J.Simpson Broken Reflection Symmetry in 114Xe NUCLEAR REACTIONS 60Ni(58Ni, 2n2p), E=243 MeV; measured γγ-, γn-, γnn-, γ(recoil)-coin, γ(θ). 114Xe deduced levels, J, π, B(λ), ratios, enhanced E1 transitions, broken reflection symmetry evidence.
doi: 10.1103/PhysRevC.48.2078
1993YA21 High Energy Phys. and Nucl.Phys. (China) 17, 1055 (1993) W.Yang, Z.Zhao, Z.Li, W.Mou, S.Zhu, X.Xie, S.Yuan, T.Zhang, Q.Pan, J.Wang, S.Xu New Gamma Rays from the Neutron-Rich Isotope 189W Decay
1993YU03 Z.Phys. A346, 187 (1993) S.Yuan, T.Zhang, S.Xu, Z.Li, Q.Pan, Z.Zhao, W.Yang, X.Zhang, W.Li, X.Yin, Y.Du, Y.Wang The Synthesis and Identification of New Heavy Neutron-Rich Nuclide 237Th NUCLEAR REACTIONS 238U(n, 2p), E=14 MeV; measured Eγ, Iγ; deduced evidence for 237Th. RADIOACTIVITY 237Th(β-) [from 238U(n, 2p), E=14 MeV]; measured Eγ, Iγ, decay curve; deduced T1/2.
doi: 10.1007/BF01306078
1993ZH06 Phys.Rev.Lett. 70, 2066 (1993); Erratum Phys.Rev.Lett. 70, 3524 (1993) Z.Zhao, R.H.France III, K.S.Lai, S.L.Rugari, M.Gai, E.L.Wildes Astrophysical S Factor of 12C(α, γ)16O from the Beta-Delayed Alpha-Particle Emission of 16N RADIOACTIVITY 16N(β-) [from 15N(d, p), E=9 MeV]; measured β-delayed Eα, Iα; deduced p-wave astrophysical S-factor for 12C(α, γ) reaction, astrophysical implications.
doi: 10.1103/PhysRevLett.70.2066
1993ZH07 Nucl.Phys. A553, 489c (1993) L.Zhang, S.Yuan, G.Jin, T.Zhang, J.Zhao, Q.Pan, W.Yang, X.Zhang, Y.Yang, S.Xu, Z.Zhao, J.Zheng, X.Sun, W.Li, Y.Luo, B.Wei Synthesis and Identification of New Heavy Nuclides Far Off Stability NUCLEAR REACTIONS Pb(12C, X), E=30 MeV/nucleon; measured γ-spectra; deduced evidence for 208Hg, production <σ>. RADIOACTIVITY 208Hg(β-) [from Pb(12C, X), E=30 MeV/nucleon]; 185Hf(β-) [from 186W(n, 2p), E=14 MeV]; measured γ-spectra, decay rates; deduced T1/2. 185Ta deduced new transition.
doi: 10.1016/0375-9474(93)90645-E
1993ZH13 Phys.Rev. C48, 429 (1993) Z.Zhao, R.H.France III, K.S.Lai, M.Gai, E.L.Wildes, R.A.Kryger, J.A.Winger, K.B.Beard Study of the Beta-Delayed Alpha-Particle Emission of 16N RADIOACTIVITY 16N(β-) [from 9Be(18O, X), E=80 MeV/nucleon]; measured β-delayed Eα, Iα, Eγ, Iγ; deduced 12C(α, γ) reaction, massive stars helium burning process implications. 16O level deduced β-decay branching ratio.
doi: 10.1103/PhysRevC.48.429
1993ZH35 Chin.J.Nucl.Phys. 15, No 3, 227 (1993) L.Zhang, G.Jin, J.Zhao, W.Yang, Y.Yang, Z.Zhao, J.Zheng, X.Sun, J.Wang, Z.Li, Z.Qin, G.Guo Observation of New Neutron-Rich Isotope 208Hg NUCLEAR REACTIONS Pb(12C, X), E=30 MeV/nucleon; measured γ spectra, decay curves; deduced evidence for 208Hg, production σ. RADIOACTIVITY 208Hg(β-) [from Pb(12C, X), E=30 MeV/nucleon]; measured γ spectra, decay curves; deduced T1/2.
1992ZH15 Chin.J.Nucl.Phys. 14, No 1, 67 (1992) Theoretical Calculation of Neutron Induced Data of 19F and Uncertainities of Parameters NUCLEAR REACTIONS 19F(n, n'), (n, 2p), (n, p), (n, α), (n, np), (n, nα), E=2-20 MeV; analyzed data; deduced model parameters covariance matrix. Several nuclear model codes.
1992ZH44 High Energy Phys. and Nucl.Phys. (China) 16, 767 (1992) L.Zhang, G.Jin, J.Zhao, W.Yang, Y.Yang, Z.Zhao, J.Zheng, X.Sun, Z.Li, Z.Qin, J.Wang, G.Guo New Neutron-Rich Isotope 208Hg
1991MA66 Nucl.Instrum.Methods Phys.Res. B56/57, 33 (1991) D.K.Marble, F.D.McDaniel, M.R.McNeir, Y.C.Yu, Z.Y.Zhao, D.K.Wilson, D.L.Weathers, J.L.Duggan, R.M.Wheeler, R.P.Chaturvedi, G.Lapicki, V.Zoran Direct Ionization in K-Shell X-Ray Production in Fluorine by Highly-Charged Lithium, Boron, and Oxygen Ions NUCLEAR REACTIONS 19F(7Li, X), E=1.5-4 MeV; 19F(10B, X), E=2-10 MeV; 19F(16O, X), E=3-12 MeV; measured K-shell X-ray production σ(E). Solid YF3 target. Model comparison. ATOMIC PHYSICS 19F(7Li, X), E=1.5-4 MeV; 19F(10B, X), E=2-10 MeV; 19F(16O, X), E=3-12 MeV; measured K-shell X-ray production σ(E). Solid YF3 target. Model comparison.
doi: 10.1016/0168-583X(91)95964-F
1991MC02 Nucl.Instrum.Methods Phys.Res. B54, 531 (1991) F.D.McDaniel, D.K.Marble, J.L.Duggan, M.R.McNeir, Y.C.Yu, Z.Y.Zhao, D.L.Weathers, P.S.Elliott, R.M.Wheeler, R.P.Chaturvedi, G.Lapicki X-Ray Production in Fluorine by Highly Charged Boron, Carbon, and Oxygen Ions NUCLEAR REACTIONS 19F(B, X), (C, X), E=10 MeV; 19F(O, X), E=8, 10, 12 MeV; measured K X-ray production σ; deduced direct ionization, electron capture contributions. ATOMIC PHYSICS 19F(B, X), (C, X), E=10 MeV; 19F(O, X), E=8, 10, 12 MeV; measured K X-ray production σ; deduced direct ionization, electron capture contributions.
doi: 10.1016/0168-583X(91)95433-E
1991RU01 Phys.Rev. C43, 1298 (1991); Erratum Phys.Rev. C43, 2899 (1991) S.L.Rugari, R.H.France, B.J.Lund, S.D.Smolen, Z.Zhao, M.Gai, K.G.Lynn Upper Limits on Emission of Neutrons from Ti in Pressurized D2 Gas Cells: A test of evidence for ' cold fusion ' NUCLEAR REACTIONS 2H(n, n), E=low; measured neutron energies; deduced reaction rate, neutron bursts rate upper limits, cold fusion. Tof, pressurized D2 gas cells, Ti alloy chips containers.
doi: 10.1103/PhysRevC.43.1298
1991YU05 Phys.Rev. A44, 7252 (1991) Y.C.Yu, M.R.McNeir, D.L.Weathers, J.L.Duggan, F.D.McDaniel, D.K.Marble, Z.Y.Zhao, G.Lapicki K-Shell X-Ray Production in 6C, 8O, 9F, 11Na, 12Mg, and 13Al by 0.5-8.0-MeV Helium Ions NUCLEAR REACTIONS C, O, 19F, 23Na, Mg, 27Al(α, X), E=0.5-8 MeV; measured K-shell X-ray production σ. ATOMIC PHYSICS C, O, 19F, 23Na, Mg, 27Al(α, X), E=0.5-8 MeV; measured K-shell X-ray production σ.
doi: 10.1103/PhysRevA.44.7252
1991ZH19 Chin.J.Nucl.Phys. 13, No 1, 37 (1991) Systematics of Excitation Function for (n, n+p) and (n, n+α) Reaction NUCLEAR REACTIONS, ICPND 27Al, 28Si, 31P, 32S, 40Ca, 47,48,49Ti, 50Cr, 54,56Fe, 58,60Ni, 63Cu, 64Zn, 80Se, 128Te, 186W(n, np), E=13.7-21.2 MeV; 23Na, 51V, 58Ni, 63,65Cu, 64,70Zn, 71Ga, 76Ge, 92Mo, 99Tc, 115In, 165Ho, 176Yb, 197Au(n, nα), E=12.6-19.9 MeV; calculated σ(E). Evaporation model, preequilibrium emission.
1991ZH22 Chin.J.Nucl.Phys. 13, No 2, 139 (1991) Systematics of Excitation Functions for (n, γ) Reaction Above 4 MeV NUCLEAR REACTIONS 40Ca, 89Y, 140Ce, 165Ho, 208Pb(n, γ), E ≈ 0.5-20 MeV; calculated σ(E). Statistical theory, exciton model.
1989GA01 Phys.Rev.Lett. 62, 874 (1989) M.Gai, S.L.Rugari, R.H.France III, B.J.Lund, Z.Zhao, D.A.Bromley, B.A.Lincoln, W.W.Smith, M.J.Zarcone, Q.C.Kessel Collective Band Structure and Origin of Enhanced E1 Decays in 18O NUCLEAR REACTIONS 14C(α, γ), E=1.14 MeV; measured γ-spectra. 18O deduced transition, branching ratio, B(E2).
doi: 10.1103/PhysRevLett.62.874
1989ZH04 Phys.Rev. C39, 1985 (1989) Z.Zhao, M.Gai, B.J.Lund, S.L.Rugari, D.Mikolas, B.A.Brown, J.A.Nolen, Jr., M.Samuel Beta Decay of 18N to Alpha Particle Emitting States in 18O and a Proposed Search for Parity Violation in 18O RADIOACTIVITY 18N(β-) [from Ta(22Ne, X), E=35 MeV/nucleon]; measured absolute β-decay branching ratios; deduced log ft, Gamow-Teller matrix elements. 18O(α) [from 18N β-decay]; measured total β-delayed α-yield. 18O deduced possible new levels.
doi: 10.1103/PhysRevC.39.1985
1989ZH15 Chin.J.Nucl.Phys. 11, No.3, 71 (1989) Systematics of (n, γ) Reaction Excitation Function NUCLEAR STRUCTURE A=60-200; analyzed (n, γ) reaction σ(E); deduced data systematics.
1988FA12 High Energy Phys. and Nucl.Phys. (China) 12, 229 (1988) W.Fan, Z.Zhao, X.Sun, W.Mu, J.Ma, W.Yang, X.Xie, L.Zhao, J.Yu The decay study of 73Br
1988ZH08 Nucl.Sci.Eng. 99, 367 (1988) Systematics of Excitation Function for (n, Charged-Particle) Reactions NUCLEAR REACTIONS 92Zr(n, α), E ≈ 9-20 MeV; 89Y, 94Zr(n, α), E ≈ 10-20 MeV; 34S, 74Se(n, p), E ≈ 5-20 MeV; calculated σ(E).
1988ZH10 Z.Phys. A331, 113 (1988) Z.Zhao, J.Yan, A.Gelberg, R.Reinhardt, W.Lieberz, A.Dewald, R.Wirowski, K.O.Zell, P.von Brentano New Excited States of the Nucleus 129Xe NUCLEAR REACTIONS 126Te(α, n), E=16 MeV; measured γγ-coin. 129Xe deduced levels, J, π, transitions, band structure.
Back to query form [Next] Note: The following list of authors and aliases matches the search parameter Z.Zhao: , Z.G.ZHAO, Z.H.ZHAO, Z.J.ZHAO, Z.L.ZHAO, Z.W.ZHAO, Z.X.ZHAO, Z.Y.ZHAO, Z.Z.ZHAO |