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NSR database version of May 10, 2024.

Search: Author = J.Knoll

Found 23 matches.

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2011KN01      Phys.Rev. C 83, 044914 (2011)

J.Knoll

Suppression of back-to-back particle-antiparticle correlations in high-energy nuclear collisions

doi: 10.1103/PhysRevC.83.044914
Citations: PlumX Metrics


2010RI05      Phys.Rev. C 82, 025207 (2010)

F.Riek, J.Knoll

Self-consistent descriptions of vector mesons in hot matter reexamined

doi: 10.1103/PhysRevC.82.025207
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2009KN01      Nucl.Phys. A821, 235 (2009)

J.Knoll

Continuous decoupling of dynamically expanding systems

doi: 10.1016/j.nuclphysa.2009.01.079
Citations: PlumX Metrics


2007RI09      Phys.Rev. C 75, 059801 (2007)

F.Riek, H.van Hees, J.Knoll

Comment on "Nonperturbative finite T broadening of the ρ meson and dilepton emission in heavy-ion collisions"

doi: 10.1103/PhysRevC.75.059801
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2004RI14      Nucl.Phys. A740, 287 (2004)

F.Riek, J.Knoll

Selfconsistent description of vector-mesons in matter

doi: 10.1016/j.nuclphysa.2004.05.010
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2003IV02      Yad.Fiz. 66, 1950 (2003); Phys.Atomic Nuclei 66, 1902 (2003)

Yu.B.Ivanov, J.Knoll, D.N.Voskresensky

Self-Consistent Approach of Off-Shell Transport

doi: 10.1134/1.1619502
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2001IV03      Yad.Fiz. 64, No 4, 711 (2001); Phys.Atomic Nuclei 64, 652 (2001)

Yu.B.Ivanov, J.Knoll, H.van Hees, D.N.Voskresensky

Soft Modes, Resonances, and Quantum Transport

doi: 10.1134/1.1368223
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2001VA08      Nucl.Phys. A683, 369 (2001)

H.van Hees, J.Knoll

Finite Pion Width Effects on the Rho-Meson

doi: 10.1016/S0375-9474(00)00462-0
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2000IV03      Nucl.Phys. A672, 313 (2000)

Yu.B.Ivanov, J.Knoll, D.N.Voskresensky

Resonance Transport and Kinetic Entropy

doi: 10.1016/S0375-9474(99)00559-X
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1999IV11      Nucl.Phys. A657, 413 (1999)

Yu.B.Ivanov, J.Knoll, D.N.Voskresensky

Self-Consistent Approximations to Non-Equilibrium Many-Body Theory

doi: 10.1016/S0375-9474(99)00319-9
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1999KN03      Prog.Part.Nucl.Phys. 42, 177 (1999)

J.Knoll

Transport Dynamics of Broad Resonances

doi: 10.1016/S0146-6410(99)00072-1
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1995KN03      Phys.Lett. 351B, 43 (1995)

J.Knoll, D.N.Voskresensky

Non-Equilibrium Description of Bremsstrahlung in Dense Matter (Landau-Pomeranchuk-Migdal Effect)

doi: 10.1016/0370-2693(95)00387-Z
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1988KN02      Nucl.Phys. A483, 711 (1988)

J.Knoll, R.Shyam

Energetic Particle Emission from Nuclear Co-Operation

NUCLEAR REACTIONS 27Al(16O, π0X), E=25 MeV/nucleon; analyzed σ(θ).

doi: 10.1016/0375-9474(88)90093-0
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1986SH04      Nucl.Phys. A448, 322 (1986); Erratum Nucl.Phys. A459, 732 (1986)

R.Shyam, J.Knoll

Hard Photons from Co-Operative Effects in Intermediate Energy Heavy-Ion Collisions

NUCLEAR REACTIONS 238U(12C, γX), E=84 MeV/nucleon; calculated σ(θγ, Eγ). 238U(12C, γX), E=20-180 MeV/nucleon; calculated σ(E). Hard photons, cooperative model.

doi: 10.1016/0375-9474(86)90095-3
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1984SH02      Phys.Lett. 136B, 221 (1984)

R.Shyam, J.Knoll

Subthreshold Pion Production in Nucleus-Nucleus Collisions - A Cooperative Process

NUCLEAR REACTIONS 12C(12C, πX), E=85 MeV/nucleon; calculated σ(θ, E(π)); deduced pion production mechanism.

doi: 10.1016/0370-2693(84)91150-X
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1984SH18      Nucl.Phys. A426, 606 (1984); Erratum Nucl.Phys. A459, 732 (1986)

R.Shyam, J.Knoll

A Cooperative Mechanism of Subthreshold Pion Production

NUCLEAR REACTIONS 12C(12C, π+X), E=85, 75 MeV/nucleon; 208Pb, 7Li(12C, X), E=85 MeV/nucleon; 12C(12C, π0X), E=84, 74, 60 MeV/nucleon; 40Ca(40Ar, π0X), E=44 MeV/nucleon; 27Al, 58Ni(14N, π0X), E=35 MeV/nucleon; Na, F(20Ne, π-X), E=183 MeV/nucleon; calculated σ(θ, E(π)) vs momentum; deduced subthreshold pion production mechanism. Statistical model.

doi: 10.1016/0375-9474(84)90167-2
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1982NA10      Phys.Rev.Lett. 48, 1780 (1982)

S.Nagamiya, H.Hamagaki, P.Hecking, S.Kadota, R.Lombard, Y.Miake, E.Moeller, S.Schnetzer, H.Steiner, I.Tanihata, S.Bohrmann, J.Knoll

Production of Negative Pions with 183-MeV/Nucleon Ne Beams

NUCLEAR REACTIONS Na, F, Pb(Ne, π-), E=183 MeV/nucleon; measured pion production σ; deduced reaction mechanism. NaF target.

doi: 10.1103/PhysRevLett.48.1780
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1981BO10      Nucl.Phys. A356, 498 (1981)

S.Bohrmann, J.Knoll

Finite Particle Number Effects in High-Energy Nuclear Collisions: Implications on pion spectra

NUCLEAR REACTIONS Na, F(Ne, π-), (Ne, p), K, Cl(Ar, π-), C(C, π-), E=800 MeV/nucleon; C, Cu(p, π-), E=1.05, 2.1 GeV; calculated σ(θ(π)) vs pion momentum; deduced sensitivity to finite particle number. Statistical model, kinetic equilibration.

doi: 10.1016/0375-9474(81)90203-7
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1979KN03      Phys.Rev. C20, 773 (1979)

J.Knoll

Statistical Picture of High Energy Nuclear Collisions

NUCLEAR REACTIONS 12C(p, 2p), E=640 MeV; Ta(p, X), E=800 MeV; calculated inclusive one-, two-proton coin spectra. Statistical model.

doi: 10.1103/PhysRevC.20.773
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1977HU08      Nucl.Phys. A290, 460 (1977)

J.Hufner, J.Knoll

Rows on Rows - A Theory for Collisions between Heavy Ions at High Energy

NUCLEAR REACTIONS 208Pb(α, p), (α, π-), E=2.1 GeV/c; 238U(20Ne, p), E=200, 400 MeV/nucleon; calculated σ(θ).

doi: 10.1016/0375-9474(77)90448-1
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1974KN05      Nucl.Phys. A229, 333 (1974)

J.Knoll, R.Rosenfelder

Longitudinal and Transverse Dispersion Corrections in Electron Scattering

NUCLEAR REACTIONS 40Ca(e, e), E=250, 500 MeV; calculated dispersion corrections.

doi: 10.1016/0375-9474(74)90791-X
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1974KN06      Phys.Lett. 52B, 131 (1974)

J.Knoll, R.Schaeffer

Semiclassical Approximation with Complex Trajectories

NUCLEAR REACTIONS 16O(16O, 16O), E=50, 300 MeV; 58Ni(α, α), E=139 MeV; calculated σ(θ).

doi: 10.1016/0370-2693(74)90069-0
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1973KN01      Nucl.Phys. A201, 289 (1973)

J.Knoll

High Momentum Transfer Approach to Inelastic Electron Scattering on Nuclei and Model-Independent Description of Nuclear Transition Densities

doi: 10.1016/0375-9474(73)90066-3
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