NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = X.S.Chen Found 17 matches. 2013PA22 Nucl.Phys. A913, 206 (2013) High-order cumulants from the 3-dimensional O(1, 2, 4) spin models
doi: 10.1016/j.nuclphysa.2013.06.010
2010WA43 Nucl.Phys. A844, 85c (2010) F.Wang, X.-S.Chen, X.-F.Lu, W.-M.Sun, T.Goldman Gauge invariance and canonical quantization applied in the study of internal structure of gauge field systems
doi: 10.1016/j.nuclphysa.2010.05.019
2004CH19 Phys.Rev. C 69, 045201 (2004) X.-S.Chen, D.Qing, W.-M.Sun, H.-S.Zong, F.Wang Spin-orbital structure of the nucleon magnetic moment
doi: 10.1103/PhysRevC.69.045201
2004CH37 Phys.Rev. C 70, 015201 (2004) X.-S.Chen, R.G.E.Timmermans, W.-Mi.Sun, H.-S.Zong, F.Wang Examination of the strangeness contribution to the nucleon magnetic moment NUCLEAR STRUCTURE 1n, 1H; calculated strangeness contribution to magnetic moment. Meson cloud model.
doi: 10.1103/PhysRevC.70.015201
2002ZO02 Phys.Rev. C66, 015201 (2002) H.-S.Zong, X.-S.Chen, F.Wang, C.-H.Chang, E.-G.Zhao Nonperturbative Aspects of Axial Vector Vertex in the Global Color Symmetry Model
doi: 10.1103/PhysRevC.66.015201
2001CH45 Phys.Rev.Lett. 87, 012001 (2001) Strange Quark Polarization of the Nucleon: A parameter-independent prediction of the chiral potential model NUCLEAR STRUCTURE 1n, 1H; calculated strange quark polarization. One-loop calculation, chiral potental model.
doi: 10.1103/PhysRevLett.87.012001
1999CH19 Chin.Phys.Lett. 16, 403 (1999) Why the Constituent Quark Model Works for Baryon Magnetic Moments
doi: 10.1088/0256-307X/16/6/005
1998QI01 Phys.Rev. C57, R31 (1998) Spin Content of the Nucleon in a Valence and Sea Quark Mixing Model NUCLEAR STRUCTURE 1n, 1H; calculated magnetic moments. Dynamical valence and sea quark mixing model.
doi: 10.1103/PhysRevC.57.R31
1998QI04 Phys.Rev. D58, 114032 (1998) Is Nucleon Spin Structure Inconsistent with the Constituent Quark Model ?
doi: 10.1103/PhysRevD.58.114032
1996BI17 Z.Phys. A356, 3 (1996) N.Bijnens, I.Ahmad, A.N.Andreyev, J.C.Batchelder, C.R.Bingham, D.Blumenthal, B.C.Busse, X.S.Chen, L.F.Conticchio, C.N.Davids, M.Huyse, R.V.F.Janssens, P.Mantica, H.Penttila, W.Reviol, D.Seweryniak, P.Van Duppen, W.B.Walters, J.Wauters, B.E.Zimmerman Fine Structure in the α Decay of 192Po RADIOACTIVITY 192Po(α) [from 160Dy(36Ar, X), E=175.6 MeV]; measured α-spectra; deduced T1/2, fine structure, α-branching ratio. 188Pb deduced level, J, π.
doi: 10.1007/s002180050137
1987ST04 Z.Phys. A326, 139 (1987) E.Stiliaris, H.G.Bohlen, X.S.Chen, B.Gebauer, A.Miczaika, W.von Oertzen, W.Weller, T.Wilpert Mass Measurement and Spectroscopy of 57Cu with the 58Ni(14N, 15C)-Reaction NUCLEAR REACTIONS 58Ni(14N, 15C), E=150 MeV; measured σ(E(15C)). 57Cu deduced levels, J, π, mass. Enriched target, magnetic spectrometer.
1985BO39 Z.Phys. A322, 241 (1985) H.G.Bohlen, X.S.Chen, J.G.Cramer, P.Frobrich, B.Gebauer, H.Lettau, A.Miczaika, W.von Oertzen, R.Ulrich, T.Wilpert Refractive Scattering and the Nuclear Rainbow in the Interaction of 12,13C with 12C at 20 MeV/N NUCLEAR REACTIONS 12C(13C, 13C), (12C, 12C), (12C, 12C'), (13C, 13C'), E=240 MeV; 12C(13C, 12C), E=260 MeV; 12C(12C, 13C), E=240 MeV; measured σ(θ); deduced refractive scattering, nuclear rainbow effects, cutoff (L). S-matrix approach.
doi: 10.1007/BF01411889
1984LE13 Nucl.Phys. A423, 175 (1984) S.Leray, X.S.Chen, G.Y.Fan, C.Gregoire, H.Ho, C.Mazur, C.Ngo, A.Pfoh, M.Ribrag, L.Schad, E.Tomasi, J.P.Wurm Investigation of Fast Fission in the 35Cl + 238U System NUCLEAR REACTIONS 238U(35Cl, F), E=250-350 MeV; measured fission fragment mass distribution characteristics; deduced fast fission evidence.
doi: 10.1016/0375-9474(84)90304-X
1983CH16 Nucl.Phys. A401, 143 (1983) X.S.Chen, C.Ngo, E.Tomasi, M.Barranco, X.Vinas, H.Ngo Real Part of the Nuclear Interaction Potential between α or p and Excited Heavy Nuclei NUCLEAR REACTIONS 56Fe, 208Pb(p, p), (α, α), E not given; calculated interaction potentials. 40Ca, 51V, 56Fe, 59Co, 60,62Ni, 63Cu, 90Zr, 116Sn, 181Ta, 197Au, 208Pb, 233,238U(α, X), (p, p), E not given; calculated fusion barrier, proton potential barrier vs temperature. Double folding model.
doi: 10.1016/0375-9474(83)90341-X
1983LA22 Nucl.Phys. A407, 233 (1983) G.La Rana, G.Nebbia, E.Tomasi, C.Ngo, X.S.Chen, S.Leray, P.Lhenoret, R.Lucas, C.Mazur, M.Ribrag, C.Cerruti, S.Chiodelli, A.Demeyer, D.Guinet, J.L.Charvet, M.Morjean, A.Peghaire, Y.Pranal, L.Sinopoli, J.Uzureau, R.De Swiniarski Linear Momentum Transfer Investigated in the 20Ne + 197Au and 209Bi Systems at 30 MeV/u NUCLEAR REACTIONS 197Au, 209Bi(20Ne, F), E=30 MeV/nucleon; measured fission (fragment)(fragment)-correlation, σ(fragment A), σ(fragment E); deduced fission σ, most probable projectile to nucleus linear momentum transfer. Monte Carlo simulation.
doi: 10.1016/0375-9474(83)90317-2
1983NE06 Z.Phys. A311, 247 (1983) G.Nebbia, E.Tomasi, C.Ngo, X.S.Chen, G.La Rana, S.Leray, P.Lhenoret, R.Lucas, C.Mazur, M.Ribrag, C.Cerruti, S.Chiodelli, A.Demeyer, D.Guinet, J.L.Charvet, M.Morjean, Y.Pranal, A.Peghaire, L.Sinopoli, J.Uzureau, R.de Swiniarski Investigation of Linear Momentum Transfer on the 20Ne + 197Au System at 30 MeV/A NUCLEAR REACTIONS 197Au(20Ne, F), E=30 MeV/nucleon; measured fission (fragment)(fragment)(θ), (fragment)(fragment)(φ); deduced projectile to fissioning nucleus momentum transfer. Tof telescope, solid state detectors.
doi: 10.1007/BF01415111
1982TO13 Nucl.Phys. A389, 69 (1982) E.Tomasi, X.S.Chen, S.Leray, C.Ngo, M.Barranco, X.Vinas, H.Ngo Calculation of Interaction Potentials between Two Heavy Ions at Finite Temperature NUCLEAR REACTIONS 40Ca(40Ca, X), 63Cu(24Mg, X), 109Ag(40Ar, X), E(cm) ≈ 66-200 MeV; calculated σ(fusion) vs E. Thomas-Fermi model, finite temperature nuclear densities.
doi: 10.1016/0375-9474(82)90291-3
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