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NSR database version of May 24, 2024.

Search: Author = Z.Y.Zhou

Found 23 matches.

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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
Citations: PlumX Metrics


2014ZH35      Eur.Phys.J. A 50, 165 (2014)

Z.-Y.Zhou, Z.Xiao

Comprehending heavy charmonia and their decays by hadron loop effects

doi: 10.1140/epja/i2014-14165-y
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32682.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30830.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31603.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31657.


2006ZH24      Nucl.Phys. A775, 212 (2006)

Z.Y.Zhou, H.Q.Zheng

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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0903.


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
Citations: PlumX Metrics


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
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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
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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
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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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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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