NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = G.Wolschin Found 53 matches. 2021KE03 Eur.Phys.J. A 57, 47 (2021) Centrality dependence of limiting fragmentation
doi: 10.1140/epja/s10050-021-00349-3
2019DI10 Phys.Rev. C 100, 024906 (2019) V.H.Dinh, J.Hoelck, G.Wolschin Hot-medium effects on Υ yields in pPb collisions at √ sNN = 8.16 TeV
doi: 10.1103/PhysRevC.100.024906
2018SI11 Phys.Rev. C 97, 044913 (2018) Examining nonextensive statistics in relativistic heavy-ion collisions NUCLEAR REACTIONS 208Pb(208Pb, X), E(cm)=17.2 GeV/nucleon; 197Au(197Au, X), E(cm)=200 GeV/nucleon; analyzed data from SPS and RHIC (BRAHMS) for stopping rapidity distributions, and dN/dy for protons minus antiprotons. Nonextensive statistics (q-statistics) fails to reproduce data, while linear relativistic diffusion model with expansion reproduces the data. Linear Fokker-Planck equations (FPE).
doi: 10.1103/PhysRevC.97.044913
2017FO06 Eur.Phys.J. A 53, 37 (2017) Relativistic diffusion model with nonlinear drift
doi: 10.1140/epja/i2017-12228-3
2017HO04 Phys.Rev. C 95, 024905 (2017) J.Hoelck, F.Nendzig, G.Wolschin In-medium Υ suppression and feed-down in UU and PbPb collisions
doi: 10.1103/PhysRevC.95.024905
2017HO29 Eur.Phys.J. A 53, 241 (2017) Electromagnetic field effects on Υ-meson dissociation in PbPb collisions at LHC energies
doi: 10.1140/epja/i2017-12441-0
2016WO05 Phys.Rev. C 94, 024911 (2016) Beyond the thermal model in relativistic heavy-ion collisions NUCLEAR REACTIONS 208Pb(208Pb, X), E=2.76, 5.02 TeV/nucleon pair; 197Au(197Au, X), E=62.4, 200 GeV/nucleon pair; 208Pb(p, X), E=5.02 TeV; calculated pT and pseudorapidity distributions of produced charged hadrons, rapidity distributions of net protons (protons minus antiprotons). Three-sources Relativistic Diffusion Model (RDM). Comparison with experimental data from ALICE, NA49, PHOBOS, RHIC, and LHC collaborations.
doi: 10.1103/PhysRevC.94.024911
2016WO06 Nucl.Phys. A956, 729 (2016) Upsilon suppression in the QGP at the LHC
doi: 10.1016/j.nuclphysa.2016.01.043
2016WO08 Eur.Phys.J. A 52, 238 (2016) Baryon stopping probes deconfinement
doi: 10.1140/epja/i2016-16238-3
2015SC05 Eur.Phys.J. A 51, 18 (2015) Analysis of pPb collisions at LHC energies in the relativistic diffusion model
doi: 10.1140/epja/i2015-15018-y
2015WO01 Phys.Rev. C 91, 014905 (2015) Ultraviolet energy dependence of particle production sources in relativistic heavy-ion collisions
doi: 10.1103/PhysRevC.91.014905
2013NE03 Phys.Rev. C 87, 024911 (2013) Υ suppression in PbPb collisions at energies available at the CERN Large Hadron Collider
doi: 10.1103/PhysRevC.87.024911
2013NE17 Nucl.Phys. 910-911, 458c (2013) Υ Suppression in PbPb Collisions at √ sNN=2.76 TeV
doi: 10.1016/j.nuclphysa.2012.12.110
2012RO24 Phys.Rev. C 86, 024902 (2012) Centrality dependence of charged-hadron pseudorapidity distributions in PbPb collisions at energies available at the CERN Large Hadron Collider in the relativistic diffusion model
doi: 10.1103/PhysRevC.86.024902
2011ME06 Europhys.Lett. 94, 62003 (2011) Stopping in central Pb+Pb collisions at SPS energies and beyond
doi: 10.1209/0295-5075/94/62003
2010ME06 Nucl.Phys. A834, 276c (2010) Baryon stopping probes geometric scaling
doi: 10.1016/j.nuclphysa.2009.12.058
2009ME04 Phys.Rev.Lett. 102, 182301 (2009) Baryon Stopping as a New Probe of Geometric Scaling
doi: 10.1103/PhysRevLett.102.182301
2009ME16 Phys.Rev. C 80, 054905 (2009) Baryon stopping and saturation physics in relativistic collisions
doi: 10.1103/PhysRevC.80.054905
2009WO01 Nucl.Phys. A820, 295c (2009) Nonlinear diffusion and particle production in relativistic systems
doi: 10.1016/j.nuclphysa.2009.01.073
2008WO02 Eur.Phys.J. A 36, 111 (2008) G.Wolschin, M.Biyajima, T.Mizoguchi Diffusion or bounce back in relativistic heavy-ion collisions?
doi: 10.1140/epja/i2007-10550-y
2007KU01 Ann.Phys.(Leipzig) 16, 67 (2007) From RHIC to LHC: a relativistic diffusion approach NUCLEAR REACTIONS Cu(Cu, X), Au(Au, X), E(cm)=19.6-200 GeV/nucleon; Pb(Pb, X), E(cm)=5.52 TeV/nucleon; calculated charged hadron multiplicity, rapidity distributions, related features. Three-sources relativistic diffusion model.
doi: 10.1002/andp.200610225
2007KU05 Europhys.Lett. 78, 22001 (2007) Hadron production in heavy relativistic systems NUCLEAR REACTIONS Cu(Cu, X), Au(Au, X), E(cm)=19.6, 62.4, 130, 200 GeV/nucleon; calculated charged hadron yields, pseudorapidity distributions.
doi: 10.1209/0295-5075/78/22001
2007WO04 Nucl.Phys. A787, 68c (2007) From RHIC to LHC: A relativistic diffusion approach NUCLEAR REACTIONS Cu(Cu, X), Au(Au, X), E(cm)=19.6, 62.4, 130, 200 GeV/nucleon; Pb(Pb, X), E(cm)=5.5 TeV/nucleon; calculated net-proton rapidity spectra, charged hadron distribution function. Relativistic diffusion model.
doi: 10.1016/j.nuclphysa.2006.12.016
2006WO02 Phys.Lett. B 633, 38 (2006) G.Wolschin, M.Biyajima, T.Mizoguchi, N.Suzuki Local thermalization in the d + Au system NUCLEAR REACTIONS 197Au(d, X), E(cm)=200 GeV/nucleon; analyzed charged particle rapidity spectra, pseudorapidity vs centrality; deduced model parameters, size of thermal equilibrium region. Relativistic diffusion model.
doi: 10.1016/j.physletb.2005.10.096
2006WO05 Europhys.Lett. 74, 29 (2006) Rapidity equilibration and longitudinal expansion at RHIC NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=4.9-200 GeV/nucleon; analyzed net-proton rapidity spectra; deduced local equilibration. Relativistic diffusion model.
doi: 10.1209/epl/i2005-10517-0
2006WO06 Ann.Phys.(Leipzig) 15, 369 (2006) G.Wolschin, M.Biyajima, T.Mizoguchi, N.Suzuki Time evolution of relativistic d + Au and Au + Au collisions NUCLEAR REACTIONS 197Au(d, X), (197Au, X), E(cm)=200 GeV/nucleon; calculated hadron pseudorapidity distributions. Relativistic diffusion model, three sources of particle production, comparison with data.
doi: 10.1002/andp.200510182
2006WO08 Eur.Phys.J. A 29, 113 (2006) Rapidity equilibration in d + Au and Au + Au systems NUCLEAR REACTIONS 197Au(d, X), (197Au, X), E(cm)=200 GeV/nucleon; calculated charged hadron rapidity spectra. Relativistic diffusion model, comparison with data.
doi: 10.1140/epja/i2005-10308-7
2005WO02 Nucl.Phys. A752, 484c (2005) Diffusion and local deconfinement in relativistic systems NUCLEAR REACTIONS Pb(Pb, X), 197Au(197Au, X), E=high; analyzed net proton rapidity spectra; deduced possible deconfinement signal. Relativistic diffusion model.
doi: 10.1016/j.nuclphysa.2005.02.053
2004WO03 Phys.Rev. C 69, 024906 (2004) Diffusion and local deconfinement in relativistic systems NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; analyzed proton rapidity spectra, related data; deduced parton deconfinement. Relativistic diffusion model, generalized Fokker-Planck equation.
doi: 10.1103/PhysRevC.69.024906
2003WO06 Phys.Lett. B 569, 67 (2003) Anomalous net-baryon-rapidity spectra at RHIC NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; calculated net-proton rapidity spectra, non-equilibrium components; deduced possible quark-gluon plasma signature. Relativistic diffusion model.
doi: 10.1016/j.physletb.2003.07.043
2003WO07 Pramana 60, 1035 (2003) Strong-coupling diffusion in relativistic systems NUCLEAR REACTIONS Pb(Pb, X), 197Au(197Au, X), E=high; calculated proton rapidity spectra, role of nonequilibrium strong-coupling effects.
doi: 10.1007/BF02707026
1999WO06 Eur.Phys.J. A 5, 85 (1999) Relativistic Diffusion Model NUCLEAR REACTIONS 32S, 197Au(32S, X), E at 200 GeV/c/nucleon; Pb(208Pb, X), E at 158 GeV/c/nucleon; calculated proton rapidity spectra; deduced role of diffusion, nonequilibrium effects. Linear Fokker-Planck equation.
doi: 10.1007/s100500050260
1999WO08 Europhys.Lett. 47, 30 (1999) Test of the Einstein Relation in Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS Ni(Ni, X), E=1.06, 1.45, 1.93 GeV/nucleon; 27Al(Si, X), 197Au(197Au, X), E=high; analyzed proton rapidity spectra; deduced deviation from dissipation-fluctuation theorem. Relativistic diffusion model.
doi: 10.1209/epl/i1999-00346-7
1996WO12 Z.Phys. A355, 301 (1996) Diffusion Model for Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS 197Au(O, X), (p, X), E=200 GeV/nucleon; 64Cu(16O, X), E at 60, 200 GeV/c; 108Ag, 184W(32S, X), E at 200 GeV/c; 27Al(28Si, X), E at 14.6 GeV/c; 197Au(197Au, X), E at 11.4 GeV/c; calculated transverse energy distributions, relaxation variation times, relativistic collisions. Transport model.
doi: 10.1007/s002180050112
1994WO05 Ann.Phys.(Leipzig) 3, 276 (1994) Quark-Gluon Plasma Formation in Heavy-Ion Collisions NUCLEAR REACTIONS Pb(Pb, X), 16O(16O, X), E=high; calculated quark-gluon plasma (energy density x transit time) vs E.
doi: 10.1002/andp.19945060405
1983DE18 Phys.Lett. 125B, 109 (1983) Population of Isomeric States in Muonic Atoms NUCLEAR REACTIONS 234,236U, 237Np, 238,240,242Pu, 241,243Am(μ-, F), E at rest; calculated isomer, ground state population vs fission barrier parameters; deduced enhancement over nucleon induced reactions. Radiationless muonic transition, GDR effects, three-step muonic cascade.
doi: 10.1016/0370-2693(83)91246-7
1983LI04 Phys.Rev. C27, 590 (1983) Distribution of the Dissipated Angular Momentum in Heavy-Ion Collisions NUCLEAR REACTIONS 238U(208Pb, X), E=8.5 MeV/nucleon; calculated average fragment energy, angular momentum loss. 154Sm(84Kr, X), E=5.7, 7 MeV/nucleon; calculated σ(fragment E), angular momentum loss, variance. Transport equation, nonequilibrium statistical model.
doi: 10.1103/PhysRevC.27.590
1982BL06 Phys.Lett. 112B, 113 (1982) Muon-Induced Prompt Fission of Uranium NUCLEAR REACTIONS, Fission 238U(μ-, F), E at rest; calculated prompt fission probabilities, Γn/Γf. Bohr-Wheeler model, radiationless muon transitions.
doi: 10.1016/0370-2693(82)90308-2
1980RI01 Z.Phys. A294, 17 (1980) Statistical Fluctuations in Dissipative Heavy-Ion Collisions NUCLEAR REACTIONS 209Bi(136Xe, X), E=6.62 MeV/nucleon; 166Er(86Kr, X), E=8.12 MeV/nucleon; calculated σ(fragment θ, Z, E). Statistic fluctuations, Fokker-Planck equation.
doi: 10.1007/BF01473118
1980SC17 Z.Phys. A296, 215 (1980) Mass Transport in Anharmonic Potentials NUCLEAR REACTIONS 238U(238U, X), E=7.42 MeV/nucleon; calculated mass distribution, transport coefficients. Focker-Planck equation, shell correction effects.
doi: 10.1007/BF01415835
1979RI04 Z.Phys. A290, 47 (1979) C.Riedel, G.Wolschin, W.Norenberg Relaxation Times in Dissipative Heavy-Ion Collisions NUCLEAR REACTIONS 166Er(86Kr, X), E=5.99, 8.18 MeV/nucleon; 209Bi(136Xe, X), E=8.31, 6.62 MeV/nucleon; calculated relaxation times for dissipation of radial kinetic energy, relative angular momentum, development of deformations. Classical model for dissipative HI collisions; deduced empirical mass transport coefficients.
doi: 10.1007/BF01408479
1979WO02 Nucl.Phys. A316, 146 (1979) Angular-Momentum Transport in Heavy-Ion Collisions NUCLEAR REACTIONS 144Sm(86Kr, X), E=490 MeV; 209Bi(86Kr, X), E=610 MeV; 197Au(86Kr, X), E=618, 860 MeV; calculated mean intrinsic angular momentum of fragments, standard deviation, alignment of heavy fragment. Fokker-Planck equation.
doi: 10.1016/0375-9474(79)90677-8
1979WO08 Phys.Lett. 88B, 35 (1979) Shape Relaxation in Heavy-Ion Collisions NUCLEAR REACTIONS 166Er(86Kr, X), E=5.99 MeV/nucleon; calculated mean values, fwhm of intrinsic angular momentum, deformation, dissipated energy vs L. Dissipative slow evolution of fragment deformation.
doi: 10.1016/0370-2693(79)90107-2
1978HU05 Phys.Lett. 73B, 289 (1978) J.Hufner, C.Sander, G.Wolschin On the Similarity of Fragment Yields in Heavy Ion Reactions at 20 MeV/A NUCLEAR REACTIONS 208Pb(16O, X), E=20, 2100 MeV/nucleon; calculated σ similarities.
doi: 10.1016/0370-2693(78)90516-6
1978SC28 Nucl.Phys. A311, 247 (1978) R.Schmidt, V.D.Toneev, G.Wolschin Mass Transport and Dynamics of the Relative Motion in Deeply Inelastic Heavy-Ion Collisions NUCLEAR REACTIONS 120Sn(132Xe, X), E=5.9 MeV/nucleon; 238U(238U, X), E=7.42 MeV/nucleon; calculated multidifferential σ based on Fokker-Planck equation for deeply inelastic HI collisions.
doi: 10.1016/0375-9474(78)90513-4
1978WO12 Phys.Rev.Lett. 41, 691 (1978) Angular-Momentum Dissipation in Heavy-Ion Collisions NUCLEAR REACTIONS 166Er(86Kr, X), E=5.99 MeV/nucleon; calculated γ-multiplicity.
doi: 10.1103/PhysRevLett.41.691
1977GL03 Nucl.Phys. A281, 486 (1977) Indirect Transitions in Two-Nucleon Transfer Reactions between Heavy Ions NUCLEAR REACTIONS 60,62,64Ni, 122Sn(16O, 18O); calculated σ(θ).
doi: 10.1016/0375-9474(77)90511-5
1977WO08 Nukleonika 22, 1165 (1977) Mass Transport in Deeply Inelastic Heavy Ion Collisions NUCLEAR REACTIONS 166Er(86Kr, X), E=515 MeV; 120Sn(132Xe, X), E=779 MeV; 238U(238U, X), E=1766 MeV; calculated element distributions. Fokker-Planck equation, deep inelastic collisions, HI reactions.
1976GL06 Phys.Rev.Lett. 36, 1532 (1976) Physical Basis for Enhanced Forward Cross Sections in Heavy-Ion Reactions NUCLEAR REACTIONS 60Ni(18O, 16O), E=65 MeV; 58Ni(18O, 18O), (18O, 18O'), E=60 MeV; 62Ni(16O, 18O), E=70.7 MeV; calculated σ(θ).
doi: 10.1103/PhysRevLett.36.1532
1976GL08 Nucl.Phys. A269, 223 (1976) Two-Particle Transfer Contributions to Elastic and Inelastic Heavy Ion Scattering NUCLEAR REACTIONS 18O(16O, 16O), E=24, 28, 32 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(76)90408-5
1976ST18 Phys.Rev. C14, 1824 (1976) R.Stock, U.Jahnke, D.L.Hendrie, J.Mahoney, C.F.Maguire, W.F.W.Schneider, D.K.Scott, G.Wolschin Contribution of Alpha Cluster Exchange to Elastic and Inelastic 16O + 20Ne Scattering NUCLEAR REACTIONS 16O(20Ne, 16O), (20Ne, 20Ne), E=50 MeV; measured σ(θ). Optical model, DWBA, CCBA analyses.
doi: 10.1103/PhysRevC.14.1824
1975GL03 Phys.Rev.Lett. 34, 1642 (1975) Enhancement of Forward-Angle Cross Sections in Heavy-Ion Reactions Because of Projectile Excitation NUCLEAR REACTIONS 122Sn(16O, 18O), E=62.2, 104 MeV; calculated σ(E(18O), θ); deduced reaction mechanism.
doi: 10.1103/PhysRevLett.34.1642
1974LO18 Nucl.Phys. A236, 457 (1974) Nuclear Auger Effect in Muonic Atoms NUCLEAR STRUCTURE, Mesic-Atoms 207Pb, 209Bi; calculated muonic En, In.
doi: 10.1016/0375-9474(74)90267-X
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