NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = Z.Y.Zhou Found 23 matches. 2018HE11 Chin.Phys.C 42, 074002 (2018) G.-Z.He, B.Shi, M.He, Z.-Y.Li, S.-L.Liu, X.-J.Chen, X.-C.Ruan, Q.-W.Zhang, Q.-W.Fan, H.Li, S.-Y.Wu, S.Jiang, Z.-Y.Zhou Cross-section measurement for the 93Nb(n, 2n)92gNb reaction at the neutron energy of 14.6 MeV by the AMS method NUCLEAR REACTIONS 93Nb(n, 2n), E=14.6 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with available data.
doi: 10.1088/1674-1137/42/7/074002
2014ZH35 Eur.Phys.J. A 50, 165 (2014) Comprehending heavy charmonia and their decays by hadron loop effects
doi: 10.1140/epja/i2014-14165-y
2012HE11 Phys.Rev. C 86, 014605 (2012) G.Z.He, S.Jiang, Z.Y.Zhou, M.He, W.Z.Tian, J.L.Zhang, L.J.Diao, H.Li Precise half-life measurement for the ground state of 94Nb RADIOACTIVITY 94Nb[from 93Nb(n, γ), E=thermal](β-); measured Eγ, Iγ, half-life using anti-Compton γ spectrometer and multicollector inductively coupled plasma mass spectrometry (MC-ICP-MS), isotopic ratios. Comparison with previous studies.
doi: 10.1103/PhysRevC.86.014605
2011RU13 J.Korean Phys.Soc. 59, 1729s (2011) X.C.Ruan, G.C.Chen, H.X.Huang, X.Li, Y.B.Nie, B.Zhou, Z.Y.Ma, J.Bao, Q.P.Zhong, Z.Y.Zhou, H.Q.Tang, J.S.Zhang, C.L.Lan, Y.L.Zhang, Y.M.Li Measurement of the Secondary Neutron Emission Differential and Double-Differential Cross Sections between 20 and 30 MeV NUCLEAR REACTIONS 9Be(n, n), (n, xn), E=21.65 MeV; measured In, En using TOF and BC501A; deduced σ, σ(θ), σ(E, θ); calculated TOF neutron spectra using Monte Carlo code STREUER, σ by LUNF code. Compared with other data.
doi: 10.3938/jkps.59.1729
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
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
2008WA04 Nucl.Instrum.Methods Phys.Res. B266, 561 (2008) T.F.Wang, A.K.M.M.H.Meaze, M.U.Khandaker, M.S.Rahman, G.N.Kim, L.P.Zhu, H.H.Xia, Z.Y.Zhou, Y.D.Oh, H.Kang, M.H.Cho, I.S.Ko, W.Namkung Measurement of the total neutron cross-section and resonance parameters of molybdenum using pulsed neutrons generated by an electron linac NUCLEAR REACTIONS Mo(n, X), E=0.01 - 200 eV; measured total cross sections using the neutron transmission technique. Deduced resonance parameters using the SAMMY code.
doi: 10.1016/j.nimb.2007.11.051
2007RU11 Phys.Rev. C 75, 057001 (2007) X.C.Ruan, Z.Y.Zhou, X.Li, J.Jiang, H.X.Huang, Q.P.Zhong, H.Q.Tang, B.J.Qi, J.Bao, B.Xin, W.von Witsch, H.Witala Experimental study of neutron-neutron quasifree scattering in the nd breakup reaction at 25 MeV NUCLEAR REACTIONS 2H(n, X), E=25 MeV; measured yields and neutron-neutron quasi free scattering cross section. Compared results to model calculations.
doi: 10.1103/PhysRevC.75.057001
2006ZH24 Nucl.Phys. A775, 212 (2006) An improved study of the kappa resonance and the non-exotic s wave π K scatterings up to √ s = 2.1 GeV of LASS data
doi: 10.1016/j.nuclphysa.2006.06.170
2005XI03 Phys.Rev. D 72, 012006 (2005) B.Xin, H.T.Wong, C.Y.Chang, C.P.Chen, H.B.Li, J.Li, F.S.Lee, S.T.Lin, V.Singh, F.Vannucci, S.C.Wu, Q.Yue, Z.Y.Zhou Production of electron neutrinos at nuclear power reactors and the prospects for neutrino physics NUCLEAR REACTIONS 235U, 239Pu(n, F), E=reactor; calculated neutrino yields from fission fragment decay. 50Cr, 54Fe, 58Ni, 63Cu, 151Eu, 103Rh(n, γ), E=reactor; calculated neutrino yields from residual nucleus decay.
doi: 10.1103/PhysRevD.72.012006
2004ZH08 Nucl.Phys. A733, 235 (2004) H.Q.Zheng, Z.Y.Zhou, G.Y.Qin, Z.G.Xiao, J.J.Wang, N.Wu The k resonance in s wave πK scatterings
doi: 10.1016/j.nuclphysa.2003.12.021
2002WA10 Phys.Lett. 536B, 203 (2002) M.Z.Wang, Q.Yue, J.R.Deng, W.P.Lai, H.B.Li, J.Li, Y.Liu, B.J.Qi, X.C.Ruan, C.H.Tang, H.Q.Tang, H.T.Wong, S.C.Wu, B.Xin, Z.Y.Zhou Nuclear Recoil Measurement in CsI(Tl) Crystal for Cold Dark Matter Detection NUCLEAR REACTIONS I, Cs(n, n), E ≈ 8 MeV; measured nuclear recoil spectra in scintillator crystal, σ(θ). Implications for dark matter search discussed. Comparison with optical model predictions.
doi: 10.1016/S0370-2693(02)01836-1
1995ZH58 Nucl.Instrum.Methods Phys.Res. B100, 524 (1995) Z.Y.Zhou, Y.Y.Zhou, Y.Zhang, W.D.Xu, G.Q.Zhao, J.Y.Tang, F.J.Yang Simultaneous Analysis of Light Elements using Non-Rutherford Helium Backscattering NUCLEAR REACTIONS Ti, O, C, N(α, α), E=3.83, 4.33 MeV; O(α, α), E=6.8-8.9 MeV; measured σ relative to Rutherford vs E.
doi: 10.1016/0168-583X(95)00328-2
1994SE12 Z.Phys. A349, 25 (1994) H.L.Seifert, J.M.Wouters, D.J.Vieira, H.Wollnik, X.G.Zhou, X.L.Tu, Z.Y.Zhou, G.W.Butler Mass Measurement of Neutron-Rich Isotopes from 51Ca to 72Ni NUCLEAR REACTIONS Th(p, F), E=800 MeV; measured fission fragment tof spectra, other features. 51Ca, 52,53,54Sc, 54,55,56Ti, 56,57,58,59,60V, 57,58,59,60,61,62Cr, 60,61,62,63,64,65Mn, 63,64,65,66,67Fe, 66,67,68,69Co, 67,68,69,70,71,72Ni deduced mass excess, two-neutron separation energies.
doi: 10.1007/BF01296329
1991ZH24 Phys.Lett. 260B, 285 (1991) X.G.Zhou, X.L.Tu, J.M.Wouters, D.J.Vieira, K.E.G.Lobner, H.L.Seifert, Z.Y.Zhou, G.W.Butler Direct Mass Measurements of the Neutron-Rich Isotopes of Fluorine Through Chlorine NUCLEAR REACTIONS Th(p, X), E=800 MeV; measured fragment mass, charge state ratio, velocity histograms. 24,25,26,27F, 27,28,29Ne, 30,31,32Na, 30,31,32,33,34Mg, 33,34,35,36Al, 36,37,38Si, 38,39,40,41P, 40,41,42,43S, 41,42,43,44Cl deduced mass excess.
doi: 10.1016/0370-2693(91)91613-Z
1990TU01 Z.Phys. A337, 361 (1990) X.L.Tu, X.G.Zhou, D.J.Vieira, J.M.Wouters, Z.Y.Zhou, H.L.Seifert, V.G.Lind Direct Mass Measurements of the Neutron-Rich Isotopes of Chlorine through Iron NUCLEAR REACTIONS Th(p, X), (p, F), E not given; measured fragment charge, mass spectra; deduced neutron, proton pairing energy vs neutron excess, binding energy enhancement around 53Sc. 41,42,43,44,45Cl, 47Ar, 50K, 51,52Ca, 52,53,54,55Sc, 54,55,56,57Ti, 56,57,58,59,60V, 57,58,59,60,61,62Cr, 60,61,62,63,64Mn, 63,64,65,66Fe; deduced mass excess. Tof isochronous spectrometer. Model comparison. ATOMIC MASSES Th(p, X), (p, F), E not given; measured fragment charge, mass spectra; deduced neutron, proton pairing energy vs neutron excess, binding energy enhancement around 53Sc. 41,42,43,44,45Cl, 47Ar, 50K, 51,52Ca, 52,53,54,55Sc, 54,55,56,57Ti, 56,57,58,59,60V, 57,58,59,60,61,62Cr, 60,61,62,63,64Mn, 63,64,65,66Fe; deduced mass excess. Tof isochronous spectrometer. Model comparison.
1987JI02 Nucl.Instrum.Methods Phys.Res. B28, 82 (1987) W.G.Jin, G.Q.Zhao, Q.Y.Shao, Y.H.Ren, X.J.Wu, Z.Y.Zhou Lifetime Measurement of the 28Si Compound State at 13.095 MeV by the Blocking Effect NUCLEAR REACTIONS 27Al(p, α), E=1565 keV; measured axial, planar blocking dips. 24Mg level deduced T1/2, Γ.
doi: 10.1016/0168-583X(87)90040-1
1985ZH05 Phys.Rev. C31, 1941 (1985) Z.Y.Zhou, E.C.Schloemer, M.D.Cable, M.Ahmed, J.E.Reiff, J.Cerny Additional Beta-Delayed Protons form the T(z) = -(3/2) Nuclei 21Mg, 25Si, 29S, and 41Ti RADIOACTIVITY 21Mg, 25Si, 29S, 41Ti(β+p) [from 20Ne, 24Mg, 28Si, 40Ca(3He, 2n), E=31.5-41.5 MeV]; measured β-delayed Ep, Ip; deduced log ft. 21Na, 25Al, 29P, 41Sc levels deduced relative Ip.
doi: 10.1103/PhysRevC.31.1941
1984CA29 Phys.Rev. C30, 1276 (1984) M.D.Cable, J.Honkanen, E.C.Schloemer, M.Ahmed, J.E.Reiff, Z.Y.Zhou, J.Cerny Beta-Delayed Two-Proton Decays of 22Al and 26P RADIOACTIVITY 22Al(β+p) [from 24Mg(3He, p4n)]; 26P(β+p) [from 28Si(3He, p4n)]; measured beta-delayed two-proton pp-coin, Ep. 21Na, 25Al deduced levels, p-branching.
doi: 10.1103/PhysRevC.30.1276
1983CA01 Phys.Rev.Lett. 50, 404 (1983) M.D.Cable, J.Honkanen, R.F.Parry, S.H.Zhou, Z.Y.Zhou, J.Cerny Discovery of Beta-Delayed Two-Proton Radioactivity: 22Al RADIOACTIVITY 22Al(β+p) [from 24Mg(3He, 4np), E=110 MeV]; measured β-delayed pp-coin, total E(2p); deduced 2p, 1p emission relative intensity. Single step 2He emission, 21Na intermediate state sequential decay discussed.
doi: 10.1103/PhysRevLett.50.404
1983CA06 Phys.Lett. 123B, 25 (1983) M.D.Cable, J.Honkanen, R.F.Parry, S.H.Zhou, Z.Y.Zhou, J.Cerny Beta-Delayed Proton Decay of the T(z) = -2 Isotope 26P NUCLEAR REACTIONS 28Si(3He, 4np), E=110-130 MeV; measured Ep, Ip; deduced evidence for 26P. RADIOACTIVITY 26P(β+p) [from 28Si(3He, 4np), E=110-130 MeV]; measured β-delayed Ep, Ip. 26P deduced T1/2. 26Si deduced T=2 level mass excess.
doi: 10.1016/0370-2693(83)90950-4
1983HO23 Phys.Lett. 133B, 146 (1983) J.Honkanen, M.D.Cable, R.F.Parry, S.H.Zhou, Z.Y.Zhou, J.Cerny Beta-Delayed Two-Proton Decay of 26P RADIOACTIVITY 26P(β+p) [from 28Si(3He, xnyp), E=110 MeV]; measured β-delayed two-proton Ep, Ip, summed spectra; deduced two-proton emission mechanism, decay scheme.
doi: 10.1016/0370-2693(83)90547-6
1982CA16 Phys.Rev. C26, 1778 (1982) M.D.Cable, J.Honkanen, R.F.Parry, H.M.Thierens, J.M.Wouters, Z.Y.Zhou, J.Cerny Beta-Delayed Proton Decay of an Odd-Odd T(z) = (-2) Isotope, 22Al RADIOACTIVITY 22Al(β+), (p) [from 24Mg(3He, 4np), E=110 MeV]; measured β-delayed Ep, Ip, T1/2. 22Mg level deduced mass excess, Iβ.
doi: 10.1103/PhysRevC.26.1778
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