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NSR database version of May 20, 2024.

Search: Author = G.Wolschin

Found 53 matches.

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2021KE03      Eur.Phys.J. A 57, 47 (2021)

B.Kellers, G.Wolschin

Centrality dependence of limiting fragmentation

doi: 10.1140/epja/s10050-021-00349-3
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2018SI11      Phys.Rev. C 97, 044913 (2018)

A.Simon, G.Wolschin

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
Citations: PlumX Metrics

2017FO06      Eur.Phys.J. A 53, 37 (2017)

F.Forndran, G.Wolschin

Relativistic diffusion model with nonlinear drift

doi: 10.1140/epja/i2017-12228-3
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2017HO29      Eur.Phys.J. A 53, 241 (2017)

J.Hoelck, G.Wolschin

Electromagnetic field effects on Υ-meson dissociation in PbPb collisions at LHC energies

doi: 10.1140/epja/i2017-12441-0
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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
Citations: PlumX Metrics

2016WO06      Nucl.Phys. A956, 729 (2016)


Upsilon suppression in the QGP at the LHC

doi: 10.1016/j.nuclphysa.2016.01.043
Citations: PlumX Metrics

2016WO08      Eur.Phys.J. A 52, 238 (2016)


Baryon stopping probes deconfinement

doi: 10.1140/epja/i2016-16238-3
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2015SC05      Eur.Phys.J. A 51, 18 (2015)

P.Schulz, G.Wolschin

Analysis of pPb collisions at LHC energies in the relativistic diffusion model

doi: 10.1140/epja/i2015-15018-y
Citations: PlumX Metrics

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
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2013NE03      Phys.Rev. C 87, 024911 (2013)

F.Nendzig, G.Wolschin

Υ suppression in PbPb collisions at energies available at the CERN Large Hadron Collider

doi: 10.1103/PhysRevC.87.024911
Citations: PlumX Metrics

2013NE17      Nucl.Phys. 910-911, 458c (2013)

F.Nendzig, G.Wolschin

Υ Suppression in PbPb Collisions at √ sNN=2.76 TeV

doi: 10.1016/j.nuclphysa.2012.12.110
Citations: PlumX Metrics

2012RO24      Phys.Rev. C 86, 024902 (2012)

D.M.Rohrscheid, G.Wolschin

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
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2011ME06      Europhys.Lett. 94, 62003 (2011)

Y.Mehtar-Tani, G.Wolschin

Stopping in central Pb+Pb collisions at SPS energies and beyond

doi: 10.1209/0295-5075/94/62003
Citations: PlumX Metrics

2010ME06      Nucl.Phys. A834, 276c (2010)

Y.Mehtar-Tani, G.Wolschin

Baryon stopping probes geometric scaling

doi: 10.1016/j.nuclphysa.2009.12.058
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2009ME04      Phys.Rev.Lett. 102, 182301 (2009)

Y.Mehtar-Tani, G.Wolschin

Baryon Stopping as a New Probe of Geometric Scaling

doi: 10.1103/PhysRevLett.102.182301
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2009ME16      Phys.Rev. C 80, 054905 (2009)

Y.Mehtar-Tani, G.Wolschin

Baryon stopping and saturation physics in relativistic collisions

doi: 10.1103/PhysRevC.80.054905
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2009WO01      Nucl.Phys. A820, 295c (2009)


Nonlinear diffusion and particle production in relativistic systems

doi: 10.1016/j.nuclphysa.2009.01.073
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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
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2007KU01      Ann.Phys.(Leipzig) 16, 67 (2007)

R.Kuiper, G.Wolschin

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
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2007KU05      Europhys.Lett. 78, 22001 (2007)

R.Kuiper, G.Wolschin

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
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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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics

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
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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
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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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
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1983DE18      Phys.Lett. 125B, 109 (1983)

J.De Kam, G.Wolschin

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
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1983LI04      Phys.Rev. C27, 590 (1983)

J.Q.Li, G.Wolschin

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
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1982BL06      Phys.Lett. 112B, 113 (1982)

A.H.Blin, G.Wolschin

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
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1980RI01      Z.Phys. A294, 17 (1980)

C.Riedel, G.Wolschin

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
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1980SC17      Z.Phys. A296, 215 (1980)

R.Schmidt, G.Wolschin

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
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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
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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
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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
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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
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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
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1978WO12      Phys.Rev.Lett. 41, 691 (1978)

G.Wolschin, W.Norenberg

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
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1977GL03      Nucl.Phys. A281, 486 (1977)

N.K.Glendenning, G.Wolschin

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
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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)

N.K.Glendenning, G.Wolschin

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
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1976GL08      Nucl.Phys. A269, 223 (1976)

N.K.Glendenning, G.Wolschin

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
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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
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1975GL03      Phys.Rev.Lett. 34, 1642 (1975)

N.K.Glendenning, G.Wolschin

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
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1974LO18      Nucl.Phys. A236, 457 (1974)

K.P.Lohs, G.W.Wolschin

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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Note: The following list of authors and aliases matches the search parameter G.Wolschin: , G.W.WOLSCHIN