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NSR database version of April 27, 2024.

Search: Author = H.J.Pirner

Found 52 matches.

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2018PI03      Phys.Rev. C 97, 054901 (2018)

H.J.Pirner, B.Z.Kopeliovich

Rapidity distributions of hadrons in proton-nucleus collisions

doi: 10.1103/PhysRevC.97.054901
Citations: PlumX Metrics


2016PI04      Phys.Rev. C 93, 034910 (2016)

H.J.Pirner, K.Reygers, B.Z.Kopeliovich

Deformed flux tubes produce azimuthal anisotropy in heavy ion collisions

doi: 10.1103/PhysRevC.93.034910
Citations: PlumX Metrics


2013PI04      Phys.Rev. C 87, 054906 (2013)

H.J.Pirner, K.Reygers, B.Z.Kopeliovich

Universal centrality dependence of particle multiplicities in heavy-ion collisions

doi: 10.1103/PhysRevC.87.054906
Citations: PlumX Metrics


2011DO05      Nucl.Phys. A856, 134 (2011)

S.Domdey, B.Z.Kopeliovich, H.J.Pirner

Jet-evolution in the quark-gluon plasma from RHIC to the LHC

doi: 10.1016/j.nuclphysa.2011.02.128
Citations: PlumX Metrics


2011KO05      Phys.Rev. C 83, 014912 (2011)

B.Z.Kopeliovich, I.K.Potashnikova, H.J.Pirner, I.Schmidt

Heavy quarkonium production: Nontrivial transition from pA to AA collisions

doi: 10.1103/PhysRevC.83.014912
Citations: PlumX Metrics


2011PI09      Phys.Rev. C 84, 015201 (2011)

H.J.Pirner, J.P.Vary

Boundary between hadron and quark-gluon structure of nuclei

doi: 10.1103/PhysRevC.84.015201
Citations: PlumX Metrics


2010AN05      Nucl.Phys. A832, 314 (2010)

D.Antonov, H.-J.Pirner, M.G.Schmidt

Pressure and interaction measure of the gluon plasma

doi: 10.1016/j.nuclphysa.2009.11.001
Citations: PlumX Metrics


2010NI05      Nucl.Phys. A833, 119 (2010)

J.Nian, H.J.Pirner

Wilson loop-loop correlators in AdS/QCD

doi: 10.1016/j.nuclphysa.2009.12.003
Citations: PlumX Metrics


2009DO09      Nucl.Phys. A825, 200 (2009)

S.Domdey, D.Grunewald, B.Z.Kopeliovich, H.J.Pirner

Transverse momentum broadening in semi-inclusive DIS on nuclei

doi: 10.1016/j.nuclphysa.2009.04.009
Citations: PlumX Metrics


2009PI05      Nucl.Phys. A819, 135 (2009)

H.J.Pirner, B.Galow, O.Schlaudt

An approach towards a constituent quark model on the light cone

doi: 10.1016/j.nuclphysa.2009.01.008
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2008DO14      Nucl.Phys. A808, 178 (2008)

S.Domdey, G.Ingelman, H.J.Pirner, J.Rathsman, J.Stachel, K.Zapp

QCD evolution of jets in the quark - gluon plasma

doi: 10.1016/j.nuclphysa.2008.04.010
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2008KO26      Phys.Rev. C 78, 055204 (2008)

B.Z.Kopeliovich, H.-J.Pirner, I.K.Potashnikova, I.Schmidt, A.V.Tarasov, O.O.Voskresenskaya

Quantum-mechanical description of in-medium fragmentation

doi: 10.1103/PhysRevC.78.055204
Citations: PlumX Metrics


2007AN26      Nucl.Phys. A789, 357 (2007)

D.Antonov, S.Domdey, H.-J.Pirner

A heavy quark-antiquark pair in hot QCD

doi: 10.1016/j.nuclphysa.2007.03.009
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2007BR06      Phys.Rev. D 75, 054031 (2007)

J.Braun, H.-J.Pirner

Effects of the running of the QCD coupling on the energy loss in the quark-gluon plasma

doi: 10.1103/PhysRevD.75.054031
Citations: PlumX Metrics


2007PI04      Nucl.Phys. A782, 158c (2007)

H.J.Pirner, D.Grunewald

Higher Twist Effects in Deep Inelastic Scattering on Nuclei

doi: 10.1016/j.nuclphysa.2006.10.053
Citations: PlumX Metrics


2006BR11      Phys.Lett. B 637, 58 (2006)

S.J.Brodsky, H.J.Pirner, J.Raufeisen

Scaling properties of high pT inclusive hadron production

NUCLEAR REACTIONS 1H(p, X), E(cm)=19.4, 23.8, 27.4 GeV; analysed pion production invariant σ. Au(Au, X), E=130, 200 GeV; analysed proton production σ. Discussed QCD scaling violations.

doi: 10.1016/j.physletb.2006.03.079
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2006RE04      Nucl.Phys. A769, 35 (2006)

A.H.Rezaeian, H.-J.Pirner

The nuclear matter stability in a non-local chiral quark model

doi: 10.1016/j.nuclphysa.2006.01.015
Citations: PlumX Metrics


2006RE14      Nucl.Phys. A779, 197 (2006)

A.H.Rezaeian, H.J.Pirner

Diquark Bose-Einstein condensation and nuclear matter

doi: 10.1016/j.nuclphysa.2006.08.013
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2005AC24      Nucl.Phys. A761, 67 (2005)

A.Accardi, D.Grunewald, V.Muccifora, H.J.Pirner

Atomic mass dependence of hadron production in deep inelastic scattering on nuclei

NUCLEAR REACTIONS He, N, Ne, Kr, Xe(e+, e+'X), E=high; calculated charged hadron multiplicities. Pure absorption model, investigated mass number dependence. Comparison with data.

doi: 10.1016/j.nuclphysa.2005.05.201
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2004PI04      Acta Phys.Pol. B35, 131 (2004)

H.J.Pirner

Particle Production and Propagation in Nuclei


2003AC04      Nucl.Phys. A720, 131 (2003)

A.Accardi, V.Muccifora, H.J.Pirner

Hadron production in deep inelastic lepton-nucleus scattering

NUCLEAR REACTIONS N, Cu, Kr, Ne, Xe(e, e'X), E=high; calculated charged hadron multiplicities, rescaled fragmentation functions. Gluon radiation and nuclear absorbtion effects considered.

doi: 10.1016/S0375-9474(03)00670-5
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2002AC15      Nucl.Phys. A711, 264c (2002)

A.Accardi, H.J.Pirner

Nuclear modifications of fragmentation functions and rescaling models

doi: 10.1016/S0375-9474(02)01227-7
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2002PI16      Phys.Rev. D66, 034020 (2002)

H.J.Pirner, F.Yuan

Critical correlations of Wilson lines in SU(3) and the high energy γ*p cross section

NUCLEAR REACTIONS 1H(e, e'X), E=high; calculated proton structure functions, dipole-proton σ, correlation functions, critical point.

doi: 10.1103/PhysRevD.66.034020
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2002SH33      Nucl.Phys. A709, 131 (2002)

A.I.Shoshi, F.D.Steffen, H.J.Pirner

S-Matrix Unitarity, Impact Parameter Profiles, Gluon Saturation and High-Energy Scattering

NUCLEAR REACTIONS 1H(γ, X), (K+, X), (K-, X), (π+, X), (π-, X), (p, X), (p-bar, X), E=high; calculated total σ. 1H(γ, X), E(cm)=20-245 GeV; calculated σ(Q2). 1H(p, p), E(cm)=14-63 GeV; 1H(p-bar, p-bar), E(cm)=546, 1800 GeV; 1H(π+, π+), (π-, π-), (K+, K+), (K-, K-), E(cm)=19.5 GeV; calculated σ(θ). Loop-loop correlation model, comparisons with data.

doi: 10.1016/S0375-9474(02)01042-4
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2001PI08      Phys.Lett. 512B, 297 (2001)

H.-J.Pirner, F.Yuan

Enhanced Minijet Production in A-A Collisions from Gluons with Large Transverse Momenta

doi: 10.1016/S0370-2693(01)00712-2
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2001PI15      Phys.Lett. 521B, 279 (2001)

H.J.Pirner

Low x Scattering as a Critical Phenomenon

doi: 10.1016/S0370-2693(01)01209-6
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2000DA05      Eur.Phys.J. A 7, 109 (2000)

U.D'Alesio, H.J.Pirner

Target Fragmentation in pp, ep and γp Collisions at High Energies

NUCLEAR REACTIONS 1H(p, nX), (γ, nX), E=high; calculated neutron production σ, neutron spectra. Several models compared.

doi: 10.1007/s100500050018
Citations: PlumX Metrics


2000ME03      Phys.Rev. C61, 035202 (2000)

J.Meyer, G.Papp, H.-J.Pirner, T.Kunihiro

Renormalization Group Flow Equation at Finite Density

doi: 10.1103/PhysRevC.61.035202
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2000SC01      Phys.Lett. 473B, 25 (2000)

K.Schwenzer, J.Meyer, H.J.Pirner

Unifying Nucleon and Quark Dynamics at Finite Baryon Number Density

doi: 10.1016/S0370-2693(99)01462-8
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1999DA19      Eur.Phys.J. C 9, 601 (1999)

U.D'Alesio, A.Metz, H.J.Pirner

Soft and Hard Pomeron in the Structure Function of the Proton at Low x and Low Q2

NUCLEAR REACTIONS 1H(γ, X), E(cm)=10-200 GeV; calculated σ, structure function F2; deduced hard, soft Pomeron contributions. Comparisons with data.

doi: 10.1007/s100520050561
Citations: PlumX Metrics


1999SC41      Nucl.Phys. A660, 439 (1999)

B.-J.Schaefer, H.-J.Pirner

The Equation of State of Quarks and Mesons in a Renormalization Group Flow Picture

doi: 10.1016/S0375-9474(99)00409-1
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1998PI09      Phys.Lett. 434B, 231 (1998)

H.J.Pirner, B.Friman

Hamiltonian Flow Equations for the Lipkin Model

doi: 10.1016/S0370-2693(98)00783-7
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1997FR06      Nucl.Phys. A617, 496 (1997)

B.Friman, H.J.Pirner

P-Wave Polarization of the ρ-Meson and the Dilepton Spectrum in Dense Matter

doi: 10.1016/S0375-9474(97)00050-X
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1997PI02      Nucl.Phys. A617, 395 (1997)

H.J.Pirner, M.Wachs

Thermodynamics of Constituent Quarks

doi: 10.1016/S0375-9474(97)00061-4
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1997SC41      Nucl.Phys. A627, 481 (1997)

B.-J.Schaefer, H.-J.Pirner

Application of the Heat-Kernel Method to the Constituent Quark Model at Finite Temperature

doi: 10.1016/S0375-9474(97)00601-5
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1996BA10      Z.Phys. A353, 397 (1996)

S.Baumgartner, H.J.Pirner, K.Konigsmann, B.Povh

How to Determine the Pion Cloud of the Constituent Quark

NUCLEAR REACTIONS 1H(e, e'X), E=high; calculated semi-inclusive pion production; deduced consituent quark pion cloud defining kinematic regions. Model with physical quark fluctuating with some probability to quark plus pion.


1995PI04      Phys.Lett. 343B, 25 (1995)

H.J.Pirner, D.N.Voskresensky

Where to Look for Pion Condensation in Heavy Ion Collisions

doi: 10.1016/0370-2693(94)01437-H
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1993SC03      Z.Phys. A344, 317 (1993)

A.G.Schneider-Neureither, H.J.Pirner, B.Kerbikov, J.Mahalanabis

Scattering Length Expansion of the Coupled Channels (p-bar)p → (lambda-bar)(lambda → (lambda-bar)(lambda) → (lambda-bar)(lambda) Near the Lambda Production Threshold

NUCLEAR REACTIONS 1H(p-bar, X), E ≤ 1550 MeV/c; analyzed (lambda-bar)(lambda) production scattering length, σ, σ(θ), polarization data. Coupled-channels approach.

doi: 10.1007/BF01303026
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1990YE04      Phys.Rev. C42, 1665 (1990)

G.Yen, J.P.Vary, A.Harindranath, H.J.Pirner

Quark Cluster Model for Deep-Inelastic Lepton-Deuteron Scattering

NUCLEAR REACTIONS 2H(e, e'X), E ≈ 10-20 GeV; analyzed data; deduced quasifree nucleon knockout contribution. Quark cluster model.

doi: 10.1103/PhysRevC.42.1665
Citations: PlumX Metrics


1987CH02      Phys.Rev. C35, 760 (1987)

G.Chanfray, H.J.Pirner

Nuclear Binding and Quark Confinement

NUCLEAR STRUCTURE 9Be, 12C, 56Fe, 197Au; calculated binding potential, bound to free nucleon rms radii ratio. 17F, 17O, 15O, 15N, 41Sc, 41Ca; calculated Nolen-Schiffer anomaly. Color dielectric model.

doi: 10.1103/PhysRevC.35.760
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1987NA07      Ann.Phys.(Leipzig) 44, 13 (1987)

O.Nachtmann, H.J.Pirner

Color Conductivity at High Resolution: A new phenomenon of nuclear physics

NUCLEAR STRUCTURE 1n, 1,2H, Fe; calculated structure functions, ratios. Extended quark, gluon models.

doi: 10.1002/andp.19874990103
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1986GU12      Nucl.Phys. A457, 555 (1986)

F.Guttner, H.J.Pirner

Quark Percolation in Nuclei

NUCLEAR STRUCTURE 2H, 3He, 9Be, 12C, 56Fe, 197Au; calculated structure function ratio, effective quark cluster confinement rms radii, cluster probabilities; deduced effective color confinement size.

doi: 10.1016/0375-9474(86)90468-9
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1986SA02      Phys.Rev. C33, 1062 (1986)

M.Sato, S.A.Coon, H.J.Pirner, J.P.Vary

Quark Cluster Probabilities in Nuclei

NUCLEAR STRUCTURE 2,3H, 3,4He; calculated quark cluster probabilities, color singlet cluster of 3, 6, 9, 12 quarks. 9Be, 12C, 16O, 20Ne, 24Mg, 27Al, 40Ca, 56Fe, 58Ni, 90Zr, 107Ag, 184W, 197Au, 208Pb, 238U deduced quark cluster probabilities. Realistic nuclear interactions.

doi: 10.1103/PhysRevC.33.1062
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1986SC14      Phys.Lett. 173B, 19 (1986)

A.Schuh, H.J.Pirner

The Nucleon in the Colour Dielectric Model

NUCLEAR STRUCTURE 1H; calculated μ, rms radius; deduced g(A)/g(V). Color dielectric model.

doi: 10.1016/0370-2693(86)91222-0
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1984GU21      Nucl.Phys. A429, 389 (1984)

F.Guttner, G.Chanfray, H.J.Pirner, B.Povh

Analysis of Pion Electroproduction Data in Terms of a Pion Distribution Function of the Proton

NUCLEAR REACTIONS 1H(e, e'π), E not given; analyzed pion production data. 1H deduced pion distribution function.

doi: 10.1016/0375-9474(84)90688-2
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1982HI02      Phys.Lett. 109B, 338 (1982)

B.Hiller, H.J.Pirner

Coherent π- Production in He3 + Li6 → π- + X at 303 MeV/N

NUCLEAR REACTIONS 6Li(3He, π-), E=303 MeV/nucleon; calculated production σ(θ, E(π)). Weizsacker-Williams approximation.

doi: 10.1016/0370-2693(82)91084-X
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1981KR15      Nucl.Phys. A367, 333 (1981)

H.Krimm, A.Klar, H.J.Pirner

Inelastic Scattering of Fast Particles on Nuclei

NUCLEAR REACTIONS 12C, 6Li, 40Ca, Pb(p, pX), E=800 MeV; calculated σ(θ) vs proton momentum. Eikonal approximation, multiple scattering.

doi: 10.1016/0375-9474(81)90652-7
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1981PI04      Nucl.Phys. A358, 413c (1981)

H.J.Pirner, J.P.Vary

Deep Inelastic Electron Scattering from 3He

NUCLEAR REACTIONS 3He(e, e'), E=10.95 GeV; calculated inelastic structure function. Deep inelastic scattering, quark model.

doi: 10.1016/0375-9474(81)90355-9
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1980HE01      Nucl.Phys. A333, 514 (1980)

P.Hecking, H.J.Pirner

How Does the Proximity of Pion Condensation Influence the Cross Section 12C + 12C → p + X at 800 MeV/N < question >

NUCLEAR REACTIONS 12C(12C, p), E=800 MeV/nucleon; calculated σ. Transport theory at pion condensation threshold.

doi: 10.1016/0375-9474(80)90113-X
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1979PI03      Nucl.Phys. A316, 461 (1979)

H.J.Pirner, B.Schurmann

Non-Equilibrium Processes in Heavy-Ion Collisions at Relativistic Energies

NUCLEAR REACTIONS 12C(12C, X), Na(20Ne, X), E=800 MeV/nucleon; calculated inclusive σ for p, π. Transport theory with two-coupled Fokker-Planck equations.

doi: 10.1016/0375-9474(79)90048-4
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1976PI12      Phys.Rev. C14, 1665 (1976)

H.J.Pirner

Excitation of the Giant Dipole Resonance in 12C(π, π')12C*

NUCLEAR REACTIONS 12C(π, π'), E=180 MeV; calculated σ(E) to giant resonance in 12C. Glauber theory.

doi: 10.1103/PhysRevC.14.1665
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1975HU13      Phys.Lett. 59B, 215 (1975)

J.Hufner, H.J.Pirner, M.Thies

The Pion-Induced Knock-Out Reaction 12C(π±, πN)11C

NUCLEAR REACTIONS 12C(π+, πX), (π-, πX), E < 400 MeV; calculated σ(E), reaction ratio.

doi: 10.1016/0370-2693(75)90029-5
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