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NSR database version of April 11, 2024.

Search: Author = J.X.Li

Found 30 matches.

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2023LI51      Phys.Rev. C 108, 044604 (2023)

J.-X.Li, H.-F.Zhang

Possibility to synthesize Z > 118 superheavy nuclei with 54Cr projectiles

doi: 10.1103/PhysRevC.108.044604
Citations: PlumX Metrics


2023LI62      Chin.Phys.C 47, 124105 (2023)

J.-X.Li, H.-F.Zhang

Evaporation residue cross sections of superheavy nuclei based on optimized nuclear data

NUCLEAR REACTIONS 238U(48Ca, X), E not given; analyzed available data; deduced the evaporation residue σ in 3n and 4n channels using an optimized method for estimating atomic nucleus masses by combining the finite-range droplet model (FRDM) with the support vector machine algorithm.

doi: 10.1088/1674-1137/ad021f
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2023LU16      Phys.Rev.Lett. 131, 202502 (2023)

Z.-W.Lu, L.Guo, Z.-Z.Li, M.Ababekri, F.-Q.Chen, C.Fu, C.Lv, R.Xu, X.Kong, Y.-F.Niu, J.-X.Li

Manipulation of Giant Multipole Resonances via Vortex γ Photons

doi: 10.1103/PhysRevLett.131.202502
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2022LI27      Phys.Rev. C 105, 054606 (2022)

J.-X.Li, H.-F.Zhang

Predictions for the synthesis of the Z=119 superheavy element

NUCLEAR REACTIONS 238U, 237Np, 242,244Pu, 243Am, 245,248Cm, 249Bk, 249Cf(48Ca, X), (48Ca, 2n), (48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E*=20-60 MeV; calculated evaporation residue σ(E). 250Cf(45Sc, X), 244Cm(51V, X), 240Pu(55Mn, X), E*=30-60; calculated potential energy surface, evaporation residue σ(E). 248,249,250,251,252Cf(45Sc, 3n); calculated survival probability. 252,253,254Es(48Ca, 3n), E*=34 MeV;248,249,250,251,252Cf(45Sc, 3n), E*=38-40 MeV; 247,248,249Bk(50Ti, 3n), E*=35 MeV;242,244,243,244,245,246,247,248,249(51V, 3n), E*=35-38 MeV;241,242,243Am, E*=38 MeV;(54Cr, 3n), 236,238,239,240,241,242,243,244Pu(55Mn, 3n), E*=37-41 MeV; calculated evaporation residue σ(E) at maximum production energy. Calculations in the framework of dinuclear system (DNS) model. Comparison to available experimental data.

doi: 10.1103/PhysRevC.105.054606
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2022LI51      Phys.Rev. C 106, 034613 (2022)

J.-X.Li, H.-F.Zhang

Predictions for the synthesis of the Z=120 superheavy element

NUCLEAR REACTIONS 252Es(45Sc, X), (45Sc, 3n), (45Sc, 4n), E*=25-60 MeV; calculated evaporation residue σ(E), capture σ(Ε), survival probability, complete fusion probability, potential energy surface. 257Fm(50Ca, 3n), (50Ca, 4n), (50Ca, 5n), (51Ca, 3n), (51Ca, 4n), (51Ca, 5n), (52Ca, 3n), (52Ca, 4n), (52Ca, 5n), E*=34-54 MeV; 252Es(55Sc, 3n), (55Sc, 4n), (55Sc, 5n), (56Sc, 3n), (56Sc, 4n), (56Sc, 5n), (57Sc, 3n), (57Sc, 4n), (57Sc, 5n), E*=36-57 MeV; 251Cf(56Ti, 3n), (56Ti, 4n), (56Ti, 5n), (57Ti, 3n), (57Ti, 4n), (57Ti, 5n), (58Ti, 3n), (58Ti, 4n), (58Ti, 5n), E*=36-60 MeV; 249Bk(58V, 3n), (58V, 4n), (58V, 5n), (59V, 3n), (59V, 4n), (59V, 5n), (60V, 3n), (60V, 4n), (60V, 5n), E*=37-59 MeV; 248Cm(59Cr, 3n), (59Cr, 4n), (59Cr, 5n), (60Cr, 3n), (60Cr, 4n), (60Cr, 5n), (61Cr, 3n), (61Cr, 4n), (61Cr, 5n), E*=36-57 MeV; 243Am(64Mn, 3n), (64Mn, 4n), (64Mn, 5n), (65Mn, 3n), (65Mn, 4n), (65Mn, 5n), (66Mn, 3n), (66Mn, 4n), (66Mn, 5n), E*=37-58 MeV;E*=34-60; calculated evaporation residue σ(E) at maximum production energy. Calculations in the framework of dinuclear system (DNS) model. Comparison to available experimental data.

doi: 10.1103/PhysRevC.106.034613
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2022LI57      Phys.Rev. C 106, 044601 (2022)

J.-X.Li, W.-X.Wang, H.-F.Zhang

Properties and synthesis of the superheavy nucleus 298114Fl

NUCLEAR REACTIONS 238U(64Ti, X), E*=32-60 MeV;242Pu(48Ca, X), E*=25-60 MeV; calculated capture σ(E), fusion probabilities, fusion barrier, potential-energy surfaces, survival probabilities in the 4n channels. 238U(64Ti, 4n)298Fl, E*=33-60 MeV; 242Pu, 244Pu(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E*=30-60 MeV; calculated evaporation residue σ(E). Dinuclear system model. Suggested 238U(64Ti, 4n) at 43 MeV excitation energy as preferred way for the synthesis of 298Fl. Comparison with available experimental data.

NUCLEAR STRUCTURE 284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304Fl, 292HS, 293Mt, 294Ds, 295Rg, 296Cn, 297Nh, 299Mc, 300Lv, 301Ts, 302Og, 303119, 304120; calculated S(n), S(2n). Finite-range droplet model (FRDM2012). Discuss the evidence that 298Fl could be spherical double-magic nucleus and also the center of the stability island of superheavy nuclei.

RADIOACTIVITY 284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304Fl, 292HS, 293Mt, 294Ds, 295Rg, 296Cn, 297Nh, 299Mc, 300Lv, 301Ts, 302Og, 303119, 304120(α), (SF); calculated Q-value, T1/2. Finite-range droplet model (FRDM2012).

doi: 10.1103/PhysRevC.106.044601
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2021MA39      Phys.Rev. C 103, L061302 (2021)

W.H.Ma, D.Patel, Y.Y.Yang, J.S.Wang, Y.Kanada-En'yo, R.F.Chen, J.Lubian, Y.L.Ye, Z.H.Yang, Z.Z.Ren, S.Mukherjee, J.B.Ma, S.L.Jin, P.Ma, J.X.Li, Y.S.Song, Q.Hu, Z.Bai, M.R.Huang, X.Q.Liu, Y.J.Zhou, J.Chen, Z.H.Gao, F.F.Duan, S.Y.Jin, S.W.Xu, G.M.Yu, G.Z.Shi, Q.Wang, T.F.Wang, X.Y.Ju, Z.G.Hu, Y.H.Zhang, X.H.Zhou, H.S.Xu, G.Q.Xiao, W.L.Zhan

Observation of 6He + t cluster states in 9Li

NUCLEAR REACTIONS 208Pb(9Li, X), E=32.7 MeV/nucleon, [secondary 9Li beam from 9Be(12C, X), E=53.7 MeV/nucleon, followed by separation and purification of fragments using RIBLL1 at HIRFL-Lanzhou facility]; measured reaction products and outgoing charged particles, angular distributions of charged particles using Si telescope and CsI(Tl) scintillator array. 9Li; deduced resonant states, relative energy spectrum of 6He+t cluster states from the decay of 9Li resonances, differential breakup cross-section, isoscalar monopole transition matrix element M(IS0) and monopole strength B(IS0), energy-weighted sum rule (EWSR) for the transferred angular momentum. DWBA and CDCC analysis of angular distributions, and GCM calculations for the cluster states in 9Li. Relevance to differences between the triton and α clusters, and impact of these differences on the formation of nuclei containing triton clusters.

doi: 10.1103/PhysRevC.103.L061302
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0273. Data from this article have been entered in the XUNDL database. For more information, click here.


2018SO04      Eur.Phys.J. A 54, 35 (2018)

Y.-S.Song, L.-Y.Hu, Y.-W.Hou, H.-L.Liu, Z.-Y.Xie, K.Zhou, J.-X.Li, J.-R.Zhou, W.Zeng, C.-J.Gui, J.-S.Wang, Y.-Y.Yang, P.Ma, J.-B.Ma, S.-L.Jin, Z.Bai, M.-R.Huang, W.-H.Ma, M.-H.Zhao, Y.-J.Zhou, Y.Li

Quasielastic scattering of 17C from a carbon target at 40 MeV/nucleon

NUCLEAR REACTIONS 12C(17C, 17C'), E=40 MeV/nucleon; measured 17C energy, angle using DSSD detector and CsI(Tl) array; deduced σ(θ); calculated σ(θ) using CC with optical potential of Woods-Saxon form; deduced optical potential parameters from the fit to the data, contribution of inelastic scattering to the total σ(θ), significant at large angles. 11,12,13,17C(17C, 17C'), E=40 MeV/nucleon; calculated elastic, inelastic σ(θ); deduced target radii, 17C radius not being anomalously large.

doi: 10.1140/epja/i2018-12460-3
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0216.


2013TA01      Chin.Phys.Lett. 30, 012101 (2013)

Z.-H.Tang, J.X.Li, J.-X.Ji, T.Zhou

Cluster Structure in Be Isotopes within Point-Coupling Covariant Density Functional

NUCLEAR STRUCTURE 6,8,10,12,14Be; calculated total energy, single-particle energies vs. quadrupole deformation parameter. Point-coupling covariant density functional theory.

doi: 10.1088/0256-307X/30/1/012101
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2012JI01      Chin.Phys.C 36, 43 (2012)

J.-X.Ji, J.-X.Li, R.Han, J.-S.Wang, Q.Hu

The neutron halo structure of 17B studied with the relativistic Hartree-Bogoliubov theory

NUCLEAR STRUCTURE 13,17B; calculated total binding energy, proton and neutron density distributions, single-particle levels. RCHB calculations with the three effective interactions.

doi: 10.1088/1674-1137/36/1/007
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2011HA38      Chin.Phys.C 35, 821 (2011)

R.Han, J.-X.Ji, J.-X.Li

A relativistic continuum Hartree-Bogoliubov theory description of N = 3 isotones

NUCLEAR STRUCTURE 6,7,8,9Li, 7Be, 8B, 9C; calculated rms radius, density distributions of proton and neutron, energy levels, J, π. Relativistic continuum Hartree-Bogoliubov theory.

NUCLEAR REACTIONS 12C(9C, X), (8B, X), E not given; calculated σ. Glauber model.

doi: 10.1088/1674-1137/35/9/006
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2010HA18      Chin.Phys.Lett. 27, 092101 (2010)

R.Han, J.-X.Li, J.-M.Yao, J.-X.Ji, J.-S.Wang, Q.Hu

Effects of Pairing Correlations on Formation of Proton Halo in 9C

NUCLEAR STRUCTURE 9C; calculated binding energy, density distributions of protons and neutrons; deduced proton halo. RCHB calculations.

doi: 10.1088/0256-307X/27/9/092101
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2010LI05      Chin.Phys.Lett. 27, 032501 (2010)

J.-X.Li, P.-P.Liu, J.-S.Wang, Z.-G.Hu, R.-S.Mao, C.Li, R.-F.Chen, Z.-Y.Sun, H.-S.Xu, G.-Q.Xiao, Z.-Y.Guo

Experimental Study on the Exotic Structure of 12N in RIBLL

NUCLEAR REACTIONS Si(12N, X), E=32.6 MeV/nucleon; measured TOF; deduced transmission efficiency, total reaction σ, rms radii for core and halo.

doi: 10.1088/0256-307X/27/3/032501
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0064.


2010LI18      Chin.Phys.C 34, 452 (2010)

J.-X.Li, P.-P.Liu, J.-S.Wang, Z.-G.Hu, R.-S.Mao, Z.-Y.Sun, C.Li, R.-F.Chen, H.-S.Xu, G.-Q.Xiao, Z.-Y.Guo

Measurement of the total reaction cross section for the mirror nuclei 12N and 12B

NUCLEAR REACTIONS Si(12N, X), E=34.9 MeV/nucleon; Si(12B, X), E=54.4 MeV/nucleon; measured reaction products; deduced total reaction σ, 12N halo structure. Comparison with Glauber model and experimental data.

doi: 10.1088/1674-1137/34/4/006
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0067.


2010ZH04      Chin.Phys.Lett. 27, 022103 (2010)

M.-F.Zhong, J.-X.Li, D.-G.Zhang, R.Han, J.-X.Ji, L.-X.Chen

Clustering Structure of 10Be Studied with the Deformed RMF + BCS Method

NUCLEAR STRUCTURE 8,10Be; calculated nucleon density distribution, binding energies; deduced two-neutron skin, 2-α clustering structure and 2-n clustering phenomena. Deformed relativistic mean field (RMF) model and BCS theory.

doi: 10.1088/0256-307X/27/2/022103
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2006OZ02      Nucl.Instrum.Methods Phys.Res. B247, 155 (2006)

A.Ozawa, Y.Z.Cai, Z.Q.Chen, M.Chiba, D.Q.Fang, Z.G.Guo, T.Izumikawa, J.X.Li, R.S.Mao, T.Ohnishi, W.Q.Shen, T.Suda, Z.Y.Sun, T.Suzuki, I.Tanihata, W.D.Tian, J.S.Wang, M.Wang, Y.B.Wei, G.Q.Xiao, Z.G.Xiao, T.Yamaguchi, Y.Yamaguchi, A.Yoshida, W.L.Zhan, H.Y.Zhang, T.Zheng, C.Zhong

Measurements of the interaction cross-sections for 14Be and 14, 15B as projectiles with a new scheme at RIBLL

NUCLEAR REACTIONS C(14Be, X), (14B, X), (15B, X), E ≈ 50 MeV/nucleon; measured interaction σ.

doi: 10.1016/j.nimb.2006.01.054
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1984.


2005WE01      Chin.Phys.Lett. 22, 61 (2005)

Y.-B.Wei, Y.-G.Ma, X.-Z.Cai, C.Zhong, J.-G.Chen, H.-Y.Zhang, D.-Q.Fang, K.Wang, G.-L.Ma, W.Guo, W.-D.Tian, W.-Q.Shen, W.-L.Zhan, G.-Q.Xiao, H.-S.Xu, Z.-Y.Sun, J.-X.Li, Z.-Y.Guo, M.Wang, Z.-Q.Chen, Z.-G.Hu, L.-X.Chen, C.Li, R.-S.Mao, J.Bai

Parallel Momentum Distribution of 28Si Fragments from 29P

NUCLEAR REACTIONS 12C(29P, 28SiX), E=30.7 MeV/nucleon; measured fragments parallel momentum distribution. 28Si, 29P deduced particle density distributions, related features. Glauber model and Skyrme-Hartree-Fock calculations.

doi: 10.1088/0256-307X/22/1/018
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2004LI19      Phys.Rev. C 69, 034326 (2004)

Z.H.Liu, M.Ruan, Y.L.Zhao, H.Q.Zhang, F.Yang, Z.Y.Ma, C.J.Lin, B.Q.Chen, Y.W.Wu, W.L.Zhan, Z.Y.Guo, G.Q.Xiao, H.S.Xu, Z.Y.Sun, J.X.Li, Z.J.Chen

Evidence for enhancement of the total reaction cross sections for 27, 28P with a 28Si target and examination of possibly relevant mechanisms

NUCLEAR REACTIONS Si(23Na, X), (24Mg, X), (25Mg, X), (25Al, X), (26Al, X), (26Si, X), (27Si, X), (27P, X), (28P, X), E ≈ 20-40 MeV/nucleon; measured reaction σ; deduced reaction mechanism features. Secondary beams from 36Ar fragmentation. Modified Glauber model analysis.

doi: 10.1103/PhysRevC.69.034326
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0802.


2004LI57      Chin.Phys.Lett. 21, 1711 (2004)

Z.-H.Liu, M.Ruan, Y.-L.Zhao, H.-Q.Zhang, F.Yang, Z.-Y.Ma, C.-J.Lin, B.-Q.Chen, Y.-W.Wu, W.-L.Zhan, Z.-Y.Guo, G.-Q.Xiao, H.-S.Xu, Z.-Y.Sun, J.-X.Li, Z.-Q.Chen

Possible Experimental Evidence of a Moderate Proton Halo in 29S

NUCLEAR REACTIONS 28Si(29Si, X), (27Si, X), (28P, X), (27P, X), E ≈ 40 MeV/nucleon; measured reaction σ. 29S deduced proton halo features. Modified Glauber theory analysis.

doi: 10.1088/0256-307X/21/9/009
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2002CA04      Phys.Rev. C65, 024610 (2002)

X.Z.Cai, H.Y.Zhang, W.Q.Shen, Z.Z.Ren, J.Feng, D.Q.Fang, Z.Y.Zhu, W.Z.Jiang, Y.G.Ma, C.Zhong, W.L.Zhan, Z.Y.Guo, G.Q.Xiao, J.S.Wang, Y.T.Zhu, J.C.Wang, J.X.Li, M.Wang, J.F.Wang, Z.J.Ning, Q.J.Wang, Z.Q.Chen

Existence of a Proton Halo in 23Al and Its Significance

NUCLEAR REACTIONS 12C(19F, X), (20Ne, X), (21Na, X), (22Mg, X), (23Al, X), (24Al, X), (25Al, X), (26Al, X), (27Al, X), (28Al, X), E ≈ 20-35 MeV/nucleon; measured reaction σ. 23Al deduced proton halo. Comparison with model prediction.

doi: 10.1103/PhysRevC.65.024610
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0546.


2002CH31      Chin.Phys.Lett. 19, 921 (2002)

T.Chen, Y.-L.Ye, Z.-H.Li, D.-X.Jiang, H.Hua, X.-Q.Li, Q.-J.Wang, Y.-C.Ge, D.-Y.Pang, Z.-Y.Di, G.-M.Jin, G.-Q.Xiao, Z.-Y.Guo, Z.-G.Xiao, H.-W.Wang, B.-G.Zhang, H.-Y.Wu, J.-X.Li, Z.-Y.Sun, W.-L.Zhan

Quasi-Elastic Scattering of a Secondary 6He Beam on a 9Be Target at 25MeV/Nucleon

NUCLEAR REACTIONS 9Be(6He, 6He), E=25 MeV/nucleon; measured σ(θ); deduced optical model parameters..

doi: 10.1088/0256-307X/19/7/311
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2002ZH30      Nucl.Phys. A707, 303 (2002)

H.Y.Zhang, W.Q.Shen, Z.Z.Ren, Y.G.Ma, W.Z.Jiang, Z.Y.Zhu, X.Z.Cai, D.Q.Fang, C.Zhong, L.P.Yu, Y.B.Wei, W.I.Zhan, Z.Y.Guo, G.Q.Xiao, J.S.Wang, J.C.Wang, Q.J.Wang, J.X.Li, M.Wang, Z.Q.Chen

Measurement of Reaction Cross Section for Proton-Rich Nuclei (A < 30) at Intermediate Energies

NUCLEAR REACTIONS C(12C, X), (13C, X), (14C, X), (13N, X), (14N, X), (15N, X), (16N, X), (17N, X), (15O, X), (16O, X), (17O, X), (18O, X), (19O, X), (17F, X), (18F, X), (19F, X), (20F, X), (21F, X), (19Ne, X), (20Ne, X), (21Ne, X), (22Ne, X), (21Na, X), (22Na, X), (23Na, X), (24Na, X), (22Mg, X), (23Mg, X), (24Mg, X), (25Mg, X), (26Mg, X), (23Al, X), (24Al, X), (25Al, X), (26Al, X), (27Al, X), (28Al, X), (26Si, X), (27Si, X), (28Si, X), (29Si, X), (27P, X), (28P, X), (29S, X), E=18-33 MeV; measured reaction σ. 17F, 23Al, 27P deduced radii, halo features. Secondary beams from 36Ar fragmentation. Comparison with model predictions.

doi: 10.1016/S0375-9474(02)01007-2
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0715.


2002ZH49      Prog.Theor.Phys.(Kyoto), Suppl. 146, 33 (2002)

H.-Y.Zhang, W.-Q.Shen, Z.-Z.Ren, Y.-G.Ma, X.-Z.Cai, D.-Q.Fang, Z.-Y.Zhu, W.-Z.Jiang, C.Zhong, L.-P.Yu, Y.-B.Wei, W.-L.Zhan, Z.-Y.Guo, G.-Q.Xiao, J.-S.Wang, J.-C.Wang, Q.-J.Wang, J.-X.Li, M.Wang, Z.-Q.Chen

Possible Proton Halo and Skin in Light Proton-Rich Nucleus

NUCLEAR REACTIONS C(15N, X), (17N, X), (16O, X), (18O, X), (17F, X), (19F, X), (21F, X), (20Ne, X), (22Ne, X), (21Na, X), (23Na, X), (22Mg, X), (24Mg, X), (23Al, X), (25Al, X), (26Si, X), (27P, X), E=30 MeV/nucleon; measured reaction σ. 17F deduced proton skin features. 23Al, 27P deduced proton halo features. Transmission method, Glauber model analysis, relativistic density-dependent Hartree calculations.

doi: 10.1143/PTPS.146.33
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2001CA43      Chin.Phys.Lett. 18, 1189 (2001)

X.-Z.Cai, W.-Q.Shen, J.Feng, D.-Q.Fang, Z.-Y.Zhu, W.-Z.Jiang, Y.-G.Ma, H.-Y.Zhang, C.Zhong, L.-P.Yu, W.-L.Zhan, Z.-Y.Guo, G.-Q.Xiao, J.-S.Wang, Y.-T.Zhu, J.-C.Wang, J.-X.Li, M.Wang, J.-F.Wang, Z.-J.Ning, Q-J.Wang, Z.-Q.Chen

Total Reaction Cross Section Measurements at Intermediate Energy for the Proton Halo Candidate 23Al and Its Neighbours

NUCLEAR REACTIONS C(19F, X), (20Ne, X), (21Na, X), (22Mg, X), (23Al, X), E ≈ 25-36 MeV/nucleon; measured reaction σ. 23Al deduced possible halo features. Secondary beams from 36Ar fragmentation.

doi: 10.1088/0256-307X/18/9/311
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2001FA09      Chin.Phys.Lett. 18, 753 (2001)

D.-Q.Fang, W.-Q.Shen, J.Feng, X.-Z.Cai, Y.-G.Ma, H.-Y.Zhang, P.-Y.Hu, W.-L.Zhan, Z.-Y.Guo, G.-Q.Xiao, J.-X.Li, M.Wang, J.-F.Wang, Z.-J.Ning, J.-C.Wang, J.-S.Wang, Q.-J.Wang, Z.-Q.Chen

Production of Light Nuclei from 36Ar and 40Ar Fragmentation at About 60 MeV/Nucleon

NUCLEAR REACTIONS Be(36Ar, X), E=69 MeV/nucleon; Be(40Ar, X), E=55 MeV/nucleon; measured fragments isotopic yields; deduced isospin effect. Comparison with model predictions.

doi: 10.1088/0256-307X/18/6/313
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2001FA11      Eur.Phys.J. A 10, 381 (2001)

D.Q.Fang, W.Q.Shen, J.Feng, X.Z.Cai, Y.G.Ma, H.Y.Zhang, P.Y.Hu, W.L.Zhan, Z.Y.Guo, G.Q.Xiao, J.X.Li, M.Wang, J.F.Wang, Z.J.Ning, J.Q.Wang, J.S.Wang, Q.J.Wang, Z.Q.Chen

Isospin Dependence of the Isotopic Distributions from 36Ar and 40Ar Fragmentation at About 60 MeV/nucleon

NUCLEAR REACTIONS Be(36Ar, X), E=69 MeV/nucleon; Be(40Ar, X), E=55 MeV/nucleon; measured fragments isotopic yields; deduced isospin effects. Comparison with modified statistical abrasion-ablation model predictions.

doi: 10.1007/s100500170103
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2001FA15      Chin.Phys.Lett. 18, 1033 (2001)

D.-Q.Fang, W.-Q.Shen, J.Feng, X.-Z.Cai, Y.-G.Ma, H.-Y.Zhang, C.Zhong, W.-L.Zhan, Z.-Y.Guo, G.-Q.Xiao, J.-S.Wang, J.-C.Wang, J.-X.Li, M.Wang, J.-F.Wang, Z.-J.Ning, Q.-J.Wang, Z.-Q.Chen

Measurements of Total Reaction Cross Sections for Exotic Nuclei Close to the Proton Drip-Line at Intermediate Energies and Observation of a Proton Halo in 27P

NUCLEAR REACTIONS 12C(19O, X), (20F, X), (21F, X), (21Ne, X), (22Ne, X), (22Na, X), (23Na, X), (24Na, X), (23Mg, X), (24Mg, X), (25Mg, X), (26Mg, X), (24Al, X), (25Al, X), (26Al, X), (27Al, X), (28Al, X), (26Si, X), (27Si, X), (28Si, X), (29Si, X), (27P, X), (28P, X), (29S, X), E=18-33 MeV/nucleon; measured total reaction σ. 27P deduced proton halo. Secondary beams from 36Ar fragmentation.

doi: 10.1088/0256-307X/18/8/312
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2001FA23      Eur.Phys.J. A 12, 335 (2001)

D.Q.Fang, W.Q.Shen, J.Feng, X.Z.Cai, H.Y.Zhang, Y.G.Ma, C.Zhong, Z.Y.Zhu, W.Z.Jiang, W.L.Zhan, Z.Y.Guo, G.Q.Xiao, J.S.Wang, J.Q.Wang, J.X.Li, M.Wang, J.F.Wang, Z.J.Ning, Q.J.Wang, Z.Q.Chen

Evidence for a Proton Halo in 27P Through Measurements of Reaction Cross-Sections at Intermediate Energies

NUCLEAR REACTIONS 12C(19O, X), (20F, X), (21F, X), (19Ne, X), (20Ne, X), (21Ne, X), (22Ne, X), (23Na, X), (24Na, X), (23Mg, X), (25Mg, X), (26Mg, X), (24Al, X), (25Al, X), (26Al, X), (27Al, X), (28Al, X), (26Si, X), (27Si, X), (28Si, X), (29Si, X), (27P, X), (28P, X), (29S, X), E=30 MeV/nucleon; measured reaction σ following fragmentation of 36Ar primary beam. 27P deduced proton-halo characteristics, neutron, proton and matter radii. Comparison with Glauber model calculations.

doi: 10.1007/s100500170011
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1998SU29      Chin.Phys.Lett. 15, 790 (1998)

Z.-Y.Sun, W.-L.Zhan, Z.-Y.Guo, G.-Q.Xiao, J.-C.Wang, J.-X.Li, S.-H.Jiang, X.-W.Meng, L.-J.Qin, Q.-J.Wang

Separation and Identification of Isotopes Produced from 20Ne + Be Reaction by Radioactive Ion Beam Line in Lanzhou

NUCLEAR REACTIONS, ICPND 9Be(20Ne, X), E=80 MeV/nucleon; measured fragments isotopic yields. Projectile fragmentation, radioactive beam production.

doi: 10.1088/0256-307X/15/11/004
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1997LI26      Physica C277, 133 (1997)

J.-X.Li, C.-D.Gong

Spin Gap and Nuclear Magnetic Relaxations in the Cuprate Superconductors

doi: 10.1016/S0921-4534(97)00067-1
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