NSR Query Results


Output year order : Descending
Format : Normal

NSR database version of May 2, 2024.

Search: Author = Huang Zuqia

Found 25 matches.

Back to query form



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
Citations: PlumX Metrics


2023HU10      Phys.Rev. C 107, 044309 (2023)

Z.Huang, G.X.Zhang, C.X.Yuan, G.L.Zhang, D.Mengoni, B.S.Cai, S.P.Hu, H.Q.Zhang, H.B.Sun, J.J.Valiente-Dobon, D.Testov, A.Goasduff, D.Bazzacco, D.R.Napoli, F.Galtarossa, F.Recchia, G.de Angelis, M.Siciliano, R.Menegazzo, S.M.Lenzi

Level scheme study of 91Mo: Weak-coupling approximation in the N=50 region

NUCLEAR REACTIONS 89Y(6Li, X)91Mo, E=34 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ). 91Mo; deduced levels, J, π, transition intensities, angular distribution from oriented nuclei (ADO) ratios, δ, T1/2 for two isomeric states, high-spin states, B(E2), configurations. Comparison with shell-model calculation employing the JUN45 interaction (KSHELL code). GALILEO ψ-ray spectrometer consisting of 25 Compton-suppressed HPGe tapered detectors at Tandem-XTU accelerator (INFN-LNL, Italy).

doi: 10.1103/PhysRevC.107.044309
Citations: PlumX Metrics


2023RE11      Phys.Rev. C 108, 044301 (2023)

Z.Ren, J.-B.Lu, G.-X.Dong, Y.Zheng, Y.-H.Wu, T.-J.Gao, P.-Y.Yang, Y.Hao, K.-Y.Ma, X.-G.Wu, C.-B.Li, Z.Huang, G.-X.Zhang, S.-P.Hu, H.-B.Sun, H.-Q.Zhang, D.Testov, J.J.Valiente-Dobon, A.Goasduff, M.Siciliano, F.Galtarossa, D.Mengoni, D.Bazzacco, G.-L.Zhang

Level scheme of 92Nb and observation of an oblate collective rotational band

doi: 10.1103/PhysRevC.108.044301
Citations: PlumX Metrics


2022HU22      Phys.Rev. C 106, 064331 (2022)

Z.Huang, G.X.Zhang, G.L.Zhang, S.P.Hu, S.M.Lenzi, D.Mengoni, J.L.Ferreira, Y.F.Lv, J.B.Lu, B.Paes, E.N.Cardozo, H.Q.Zhang, H.B.Sun, J.J.Valiente-Dobon, D.Testov, A.Goasduff, D.Bazzacco, P.R.John, D.R.Napoli, F.Galtarossa, F.Recchia, G.de.Angelis, M.Siciliano, R.Menegazzo, J.Lubian

Level scheme study of 92Mo: Searching for evidence of core excitation

NUCLEAR REACTIONS 89Y(6Li, 3n), E=34 MeV; measured Eγ, Iγ; γγ-coin, γγ(θ). 92Mo; deduced levels, J, π, δ, B(E1), T1/2 of excited states, high-spin states, angular distribution from the oriented nuclei (ADO) ratio, configurations. Comparison to JUN45 and JJGLEM shell-model calculation. GALILEO γ-array consisting of 25 Compton suppressed HPGe and 8 BGO crystals served as the anti-Compton shield of each HPGe at XTU Tandem accelerator (INFN Legnaro National Laboratory).

doi: 10.1103/PhysRevC.106.064331
Citations: PlumX Metrics


2022RE11      Phys.Rev. C 106, 024323 (2022), Erratum Phys.Rev. C 107, 049902 (2023)

Z.Ren, J.-B.Lu, G.-L.Zhang, Y.-H.Wu, T.-J.Gao, K.-Y.Ma, Z.Huang, G.-X.Zhang, M.-L.Wang, S.-P.Hu, H.-B.Sun, H.-Q.Zhang, D.Testov, P.R.John, J.J.Valiente-Dobon, A.Goasduff, M.Siciliano, F.Galtarossa, D.Mengoni, D.Bazzacco

Reinvestigation of the level structures of the N=49 isotones 89Zr and 91Mo

NUCLEAR REACTIONS 89Y(6Li, 4n2p)89Zr, (6Li, 4n)91Mo, E=34 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(ADO), (particle)γ-coin using GALILEO array with 25 BGO-Compton-suppressed HPGe detectors for γ rays, and EUCLIDES 4π Si-ball array for charged particles at the Tandem-XTU accelerator of INFN-LNL, Legnaro. 89Zr, 91Mo; deduced high-spin levels, J, π, ADO ratios, multipolarities, configurations. 91Nb, 92Mo; deduced ADO ratios for certain γ-transitions. Comparison with spherical-basis shell-model calculations.

NUCLEAR STRUCTURE 89Zr, 91Mo; calculated levels, J, π, components of the wave functions and their partitions for spherical configurations for protons and neutrons. Comparison with experimental data. Systematics of energies in N=49 isotones: 9/2+, 13/2+, 17/2+, 21/2+, 23/2+ and 25/2+ states in 89Zr, 91Mo, 93Ru, 95Pd, and those of 8+, 9+, 10+, 12+, 13+ and 14+ in 88Y, 90Nb, 92Tc, 94Rh.

doi: 10.1103/PhysRevC.106.024323
Citations: PlumX Metrics

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


2021HU07      Chin.Phys.C 45, 024001 (2021)

Z.Huang, B.Chen, L.Qin, Q.Zhang, F.Zhang, T.Wang, K.Fang

Measurement of astrophysical S-factor for 9Be(d, α0)7Li and 9Be(d, α1)7Li* reactions at low energies

NUCLEAR REACTIONS 9Be(d, α), E=66-94 keV; measured reaction products, Eα, Iα; deduced thick target yields, S-factors. Comparison with available data.

doi: 10.1088/1674-1137/abca1d
Citations: PlumX Metrics


2021HU12      Eur.Phys.J. A 57, 137 (2021)

Z.Huang, G.X.Zhang, S.P.Hu, B.Paes, E.N.Cardozo, J.L.Ferreira, M.J.Ermamatov, G.L.Zhang, J.B.Lu, M.Mazzocco, Y.F.Lv, H.Q.Zhang, H.B.Sun, D.Testov, P.R.John, J.J.Valiente-Dobon, A.Goasduff, M.Siciliano, F.Galtarossa, F.Recchia, D.Mengoni, D.Bazzacco, J.Lubian, X.B.Qin, H.M.Zhao

Angular distribution of γ rays emitted by oriented nuclei: the case of 92Mo formed in the reaction 6Li + 89Y

NUCLEAR REACTIONS 89Y(6Li, X)92Mo, E=34 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, J, π, γ-ray angular distributions, E1, M2 transition strengths, mixing ratios and T1/2. Comparison with the NushellX calculation using the jjglem interaction.

doi: 10.1140/epja/s10050-021-00443-6
Citations: PlumX Metrics

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


2020ZH14      Astrophys.J. 893, 126 (2020)

Q.Zhang, Z.Huang, J.Hu, B.Chen, S.Hou, T.Wang, K.Fang

Astrophysical S(E) for the 9Be(p, d)8Be and 9Be(p, α)6Li Reactions by Direct Measurement

NUCLEAR REACTIONS 9Be(p, d), (p, α), E=34-100 KeV/nucleon; measured reaction products, Eα, Iα; deduced yields, S-factors, resonance parameters, reaction rates. Comparison with available data.

doi: 10.3847/1538-4357/ab8222
Citations: PlumX Metrics


2019CH04      Phys.Rev. A 99, 012710 (2019)

L.Chen, X.Shan, X.Zhao, X.Zhu, X.Hu, Y.Wu, W.Feng, D.Guo, R.Zhang, Y.Gao, Z.Huang, J.Wang, X.Ma, X.Chen

Two-body fragmentation dynamics of N2Oq+(q=2, 3) induced by electron-capture collisions with 5.7 - keV/u Xe15+

NUCLEAR REACTIONS N, O(Xe, Xe'), E=5.7 keV/nucleon; measured reaction products; deduced kinetic energy release (KER) distributions for the ion-pair products. Comparison with calculations.

doi: 10.1103/PhysRevA.99.012710
Citations: PlumX Metrics


2019LV02      Chin.Phys.C 43, 104102 (2019)

Y.-F.Lv, J.-B.Lu, G.-L.Zhang, Y.-H.Wu, C.-X.Yuan, G.-J.Fu, G.-X.Zhang, Z.Huang, M.-L.Wang, S.-P.Hu, H.-B.Sun, H.-Q.Zhang, C.-Q.Li, K.-Y.Ma, Y.-J.Ma, Yu.-Z.Liu, D.Testov, P.R.John, J.J.Valiente-Dobon, A.Goasduff, M.Siciliano, F.Galtarossa, F.Recchia, D.Mengoni, D.Bazzacco

Low-lying states of 92, 93Nb excited in the reactions induced by the weakly-bound nucleus 6Li near the Coulomb barrier

NUCLEAR REACTIONS 89Y(6Li, X)92Nb/93Nb, E=34 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, level schemes.

doi: 10.1088/1674-1137/43/10/104102
Citations: PlumX Metrics

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


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
Citations: PlumX Metrics

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


2019WA15      Appl.Radiat.Isot. 147, 144 (2019)

Q.Wang, Y.Han, B.Chen, Z.Huang, S.Tamaki, Is.Murata, T.Wang, K.Fang

Cross sections of (n, x) reactions on cerium isotopes induced by D-T neutrons

NUCLEAR REACTIONS 136,138,140,142Ce(n, 2n), 140,142Ce(n, p), (n, α), 142Ce(n, γ), E ∼ 14 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with ENDF/B-VII.1, CENDL-3.1, JENDL-4.0 libraries, TALYS-1.8 code calculations.

doi: 10.1016/j.apradiso.2019.03.012
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32768.


1998HU12      Nucl.Phys. A637, 79 (1998)

Z.Huang, H.J.Lu, I.Sarcevic

Partonic Picture of Nuclear Shadowing at Small x

doi: 10.1016/S0375-9474(98)00210-3
Citations: PlumX Metrics


1997FE07      Phys.Rev. C56, 1637 (1997)

D.Fein, Z.Huang, P.Valerio, I.Sarcevic

What is the Brightest Source for Dilepton Emissions at Ultrarelativistic Energies ( Question )

NUCLEAR REACTIONS 197Au(197Au, X), E=high; calculated heavy quark differential production σ, dimuon mass spectra.

doi: 10.1103/PhysRevC.56.1637
Citations: PlumX Metrics


1996WA18      Phys.Rev.Lett. 77, 231 (1996)

X.-N.Wang, Z.Huang, I.Sarcevic

Jet Quenching in the Direction Opposite to a Tagged Photon in High-Energy Heavy-Ion Collisions

NUCLEAR REACTIONS 197Au(197Au, X), E=high; analyzed jet fragmentation produced charged hadrons p(t) spectrum, other data; deduced jet energy loss in dense matter related features.

doi: 10.1103/PhysRevLett.77.231
Citations: PlumX Metrics


1995AS02      Phys.Rev.Lett. 74, 3126 (1995)

M.Asakawa, Z.Huang, X.-N.Wang

How Disoriented Chiral Condensates Form: Quenching versus annealing

doi: 10.1103/PhysRevLett.74.3126
Citations: PlumX Metrics


1995AS06      Nucl.Phys. A590, 575c (1995)

M.Asakawa, Z.Huang, X.-N.Wang

Formation of Disoriented Chiral Condensates Through Quenching and Annealing

doi: 10.1016/0375-9474(95)00281-5
Citations: PlumX Metrics


1995HU17      Nucl.Instrum.Methods Phys.Res. A356, 397 (1995)

F.Huang, S.Bao, J.Liu, W.Cao, Z.Huang, L.Zhu, L.Hou

The Inelastic Scattering Neutron Angular Distribution of Reaction 7Li(n, n'γ)7Li(*)(478 keV) Derived from Shape Analysis of the Doppler Broadened γ Spectra at 9, 9.5 and 10 MeV

NUCLEAR REACTIONS 7Li(n, n'γ), E=9, 9.5, 10 MeV; measured σ(θn), Doppler broadened γ spectra. DWBA analysis.

doi: 10.1016/0168-9002(94)01257-1
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31442.


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.


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.


1991CA25      Chin.J.Nucl.Phys. 13, No 1, 17 (1991)

Z.Cao, Z.Huang, J.Liu, Q.Chen, D.Ding

High Energy Gamma-Ray Spectrometer at CIAE

NUCLEAR REACTIONS 12C(p, γ), E=14.24 MeV; 3H(p, γ), E=0.5 MeV; 7Li(p, γ), E=0.441 MeV; 11B(p, γ), E=0.163 MeV; 19F(α, pγ), E=0.340 MeV; measured γ-spectra. NaI(Tl) γ-ray spectrometer, plastic anti-coincidence shield.

RADIOACTIVITY 137Cs, 22Na; measured γ-spectra. NaI(Tl) γ-ray spectrometer, plastic anti-coincidence shield.


1991HU05      Chin.J.Nucl.Phys. 13, No 2, 97 (1991)

Z.Huang, L.Zhu, L.Ho, X.Shi, D.Ding

The Measurement of 12C(n, γ)13C Reaction in the Pygmy Resonance Region

NUCLEAR REACTIONS 12C(n, γ), E=7-14 MeV; measured σ(θ) vs E, Eγ, Iγ, γ(θ). 13C deduced pygmy resonance γ-multipolarity.


1991HU06      Chin.J.Nucl.Phys. 13, No 2, 147 (1991)

Z.Huang, P.He, Z.Su, C.Zhou

New Sets of Back-Shifted Level Density Parameters

NUCLEAR STRUCTURE A=44-250; analyzed data; deduced level density parameters. Back-shifted level density formula.


1989HU15      Chin.J.Nucl.Phys. 11, No. 4, 55 (1989)

Z.Huang, J.Liu, Z.Cao, H.Wang, D.Ding

A Study of 12C(n, γ)13C Reaction Induced by 14.2 MeV Neutrons

NUCLEAR REACTIONS 12C(n, γ), E=14.2 MeV; measured γ(θ); deduced γ-multipolarity. Direct-semidirect model.


1982SA32      Chin.J.Nucl.Phys. 4, 318 (1982)

Sa Benhao, Su Zongdi, Zhang Guishan, Shi Yijing, Huang Zuqia

Direct Simulation of Deep Inelastic Scattering of Heavy-Ions. (I). One Parameter Distribution

NUCLEAR REACTIONS 58Ni(40Ar, X), E=280 MeV; analyzed data; deduced single nucleon transfer probability. Statistical spectroscopy method, direct simulation, Lagrange equation.


Back to query form