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NSR database version of May 19, 2024.

Search: Author = X.S.Chen

Found 17 matches.

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2013PA22      Nucl.Phys. A913, 206 (2013)

X.Pan, L.Chen, X.S.Chen, Y.Wu

High-order cumulants from the 3-dimensional O(1, 2, 4) spin models

doi: 10.1016/j.nuclphysa.2013.06.010
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2001CH45      Phys.Rev.Lett. 87, 012001 (2001)

X.-B.Chen, X.-S.Chen, F.Wang

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
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1999CH19      Chin.Phys.Lett. 16, 403 (1999)

X.-S.Chen, D.Qing, F.Wang

Why the Constituent Quark Model Works for Baryon Magnetic Moments

doi: 10.1088/0256-307X/16/6/005
Citations: PlumX Metrics


1998QI01      Phys.Rev. C57, R31 (1998)

D.Qing, X.-S.Chen, F.Wang

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
Citations: PlumX Metrics


1998QI04      Phys.Rev. D58, 114032 (1998)

D.Qing, X.-S.Chen, F.Wang

Is Nucleon Spin Structure Inconsistent with the Constituent Quark Model ?

doi: 10.1103/PhysRevD.58.114032
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1681.


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
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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
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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
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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
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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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