NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = J.X.Li Found 30 matches. 2023LI51 Phys.Rev. C 108, 044604 (2023) Possibility to synthesize Z > 118 superheavy nuclei with 54Cr projectiles
doi: 10.1103/PhysRevC.108.044604
2023LI62 Chin.Phys.C 47, 124105 (2023) 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
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
2022LI27 Phys.Rev. C 105, 054606 (2022) 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
2022LI51 Phys.Rev. C 106, 034613 (2022) 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
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
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
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
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
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
2011HA38 Chin.Phys.C 35, 821 (2011) 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1997LI26 Physica C277, 133 (1997) Spin Gap and Nuclear Magnetic Relaxations in the Cuprate Superconductors
doi: 10.1016/S0921-4534(97)00067-1
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