NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = H.J.Pirner Found 52 matches. 2018PI03 Phys.Rev. C 97, 054901 (2018) Rapidity distributions of hadrons in proton-nucleus collisions
doi: 10.1103/PhysRevC.97.054901
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
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
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
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
2011PI09 Phys.Rev. C 84, 015201 (2011) Boundary between hadron and quark-gluon structure of nuclei
doi: 10.1103/PhysRevC.84.015201
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
2010NI05 Nucl.Phys. A833, 119 (2010) Wilson loop-loop correlators in AdS/QCD
doi: 10.1016/j.nuclphysa.2009.12.003
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
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
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
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
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
2007BR06 Phys.Rev. D 75, 054031 (2007) Effects of the running of the QCD coupling on the energy loss in the quark-gluon plasma
doi: 10.1103/PhysRevD.75.054031
2007PI04 Nucl.Phys. A782, 158c (2007) Higher Twist Effects in Deep Inelastic Scattering on Nuclei
doi: 10.1016/j.nuclphysa.2006.10.053
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
2006RE04 Nucl.Phys. A769, 35 (2006) The nuclear matter stability in a non-local chiral quark model
doi: 10.1016/j.nuclphysa.2006.01.015
2006RE14 Nucl.Phys. A779, 197 (2006) Diquark Bose-Einstein condensation and nuclear matter
doi: 10.1016/j.nuclphysa.2006.08.013
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
2004PI04 Acta Phys.Pol. B35, 131 (2004) 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
2002AC15 Nucl.Phys. A711, 264c (2002) Nuclear modifications of fragmentation functions and rescaling models
doi: 10.1016/S0375-9474(02)01227-7
2002PI16 Phys.Rev. D66, 034020 (2002) 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
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
2001PI08 Phys.Lett. 512B, 297 (2001) Enhanced Minijet Production in A-A Collisions from Gluons with Large Transverse Momenta
doi: 10.1016/S0370-2693(01)00712-2
2001PI15 Phys.Lett. 521B, 279 (2001) Low x Scattering as a Critical Phenomenon
doi: 10.1016/S0370-2693(01)01209-6
2000DA05 Eur.Phys.J. A 7, 109 (2000) 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
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
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
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
1999SC41 Nucl.Phys. A660, 439 (1999) The Equation of State of Quarks and Mesons in a Renormalization Group Flow Picture
doi: 10.1016/S0375-9474(99)00409-1
1998PI09 Phys.Lett. 434B, 231 (1998) Hamiltonian Flow Equations for the Lipkin Model
doi: 10.1016/S0370-2693(98)00783-7
1997FR06 Nucl.Phys. A617, 496 (1997) P-Wave Polarization of the ρ-Meson and the Dilepton Spectrum in Dense Matter
doi: 10.1016/S0375-9474(97)00050-X
1997PI02 Nucl.Phys. A617, 395 (1997) Thermodynamics of Constituent Quarks
doi: 10.1016/S0375-9474(97)00061-4
1997SC41 Nucl.Phys. A627, 481 (1997) Application of the Heat-Kernel Method to the Constituent Quark Model at Finite Temperature
doi: 10.1016/S0375-9474(97)00601-5
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) Where to Look for Pion Condensation in Heavy Ion Collisions
doi: 10.1016/0370-2693(94)01437-H
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
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
1987CH02 Phys.Rev. C35, 760 (1987) 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
1987NA07 Ann.Phys.(Leipzig) 44, 13 (1987) 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
1986GU12 Nucl.Phys. A457, 555 (1986) 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
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
1986SC14 Phys.Lett. 173B, 19 (1986) 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
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
1982HI02 Phys.Lett. 109B, 338 (1982) 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
1981KR15 Nucl.Phys. A367, 333 (1981) 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
1981PI04 Nucl.Phys. A358, 413c (1981) 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
1980HE01 Nucl.Phys. A333, 514 (1980) 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
1979PI03 Nucl.Phys. A316, 461 (1979) 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
1976PI12 Phys.Rev. C14, 1665 (1976) 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
1975HU13 Phys.Lett. 59B, 215 (1975) 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
Back to query form |