Nuclear Science References (NSR)

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NSR database version of April 25, 2024.

Search: Author = G.Fai

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2009AD05 Phys.Rev. C 80, 014903 (2009)

A.Adeluyi, G.G.Barnafoldi, G.Fai, P.Levai

Relativistic light-on-heavy nuclear collisions and the implied rapidity asymmetry

doi: 10.1103/PhysRevC.80.014903
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2007AD30 Phys.Rev. C 76, 054904 (2007)

A.Adeluyi, G.Fai

Hadron production in deuteron-gold collisions and nuclear parton distributions

doi: 10.1103/PhysRevC.76.054904
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2007BA13 Eur.Phys.J. C 49, 333 (2007)

G.G.Barnafoldi, P.Levai, G.Papp, G.Fai

Jet tomography in the forward direction at RHIC

NUCLEAR REACTIONS Cu(Cu, X), Au(Au, X), E(cm)=200 GeV/nucleon; analyzed particle suppression patterns; deduced source features, final state effects.

doi: 10.1140/epjc/s10052-006-0069-6
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2007FA02 Nucl.Phys. A783, 535c (2007)

G.Fai, P.Levai, G.Papp

From Di-hadron Correlations to Parton Intrinsic Transverse Momentum in Proton-proton Collisions

NUCLEAR REACTIONS ¹H(p, X), E(cm)=200 GeV; analyzed di-hadron correlations; deduced fragmentation width, partons intrinsic transverse momentum width.

doi: 10.1016/j.nuclphysa.2006.11.117
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2007LE03 Nucl.Phys. A783, 101c (2007)

P.Levai, G.G.Barnafoldi, G.Fai, G.Papp

Nuclear Effects in the dAu Collisions from Recent RHIC Data

NUCLEAR REACTIONS ¹H(p, X), ¹⁹⁷Au(d, X), E(cm)=200 GeV/nucleon; analyzed neutral pion transverse momentum spectra, nuclear modification factors.

doi: 10.1016/j.nuclphysa.2006.11.016
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2007NE13 Phys.Rev. C 76, 051902 (2007); Erratum Phys.Rev. C 76, 069903 (2007)

C.Nepali, G.Fai, D.Keane

Selection of special orientations in relativistic collisions of deformed heavy nuclei

doi: 10.1103/PhysRevC.76.051902
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2006AD27 Phys.Rev. C 74, 054904 (2006)

A.Adeluyi, G.Fai

Mass dependence of nuclear shadowing at small Bjorken-x from diffractive scattering

doi: 10.1103/PhysRevC.74.054904
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2006BA83 Nucl.Phys. A774, 801 (2006)

G.G.Barnafoldi, P.Levai, G.Papp, G.Fai

The Nuclear Modification Factor at Large Rapidities

NUCLEAR REACTIONS Au(d, X), E(cm)=200 GeV/nucleon; Au(Au, X), E(cm)=62.4, 200 GeV/nucleon; calculated nuclear modification factor for pion production. Perturbative QCD improved parton model. Comparison with data.

doi: 10.1016/j.nuclphysa.2006.06.139
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2006FA10 Nucl.Phys. A774, 557 (2006)

G.Fai, G.Papp, P.Levai

Di-hadron correlations and parton intrinsic transverse momentum

NUCLEAR REACTIONS ¹H(p, X), E(cm)=31, 45, 62, 200 GeV/nucleon; calculated di-jet correlations. Comparison to hadron-hadron and parton-parton correlations data. Randomization model.

doi: 10.1016/j.nuclphysa.2006.06.086
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2006LE12 Phys.Lett. B 634, 383 (2006)

P.Levai, G.Fai, G.Papp

Di-hadron correlations at ISR and RHIC energies

NUCLEAR REACTIONS ¹H(p, X), E(cm)=31, 45, 62, 200 GeV/nucleon; analysed parton transverse momentum distributions, fluctuations, two-particle correlations.

doi: 10.1016/j.physletb.2006.01.047
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2006NE04 Phys.Rev. C 73, 034911 (2006)

C.Nepali, G.Fai, D.Keane

Advantage of U+U over Au+Au collisions at constant beam energy

NUCLEAR REACTIONS U(U, X), E(cm)=200 GeV/nucleon; calculated particle multiplicities, transverse particle densities.

doi: 10.1103/PhysRevC.73.034911
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2005BA21 Nucl.Phys. A749, 291c (2005)

G.G.Barnafoldi, P.Levai, G.Papp, G.Fai

Rapidity Asymmetry in pA and dAu Collisions

NUCLEAR REACTIONS Be(p, X), E(cm)=30.7 GeV/nucleon; ¹⁹⁷Au(d, X), E(cm)=200 GeV/nucleon; calculated neutral pions yields, rapidity asymmetry; deduced nuclear scattering and shadowing effects. Perturbative QCD, comparison with data.

doi: 10.1016/j.nuclphysa.2004.12.054
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2005FA02 Phys.Rev. C 71, 014901 (2005)

G.Fai, J.Qiu, X.Zhang

Probing small-x gluons by low-mass Drell-Yan pairs at colliders

NUCLEAR REACTIONS ¹H(p, X), (p-bar, X), E=high; calculated Drell-Yan production σ(Q²), rapidity, transverse momentum distributions, dependence on small-x gluons.

doi: 10.1103/PhysRevC.71.014901
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2004BA72 J.Phys.(London) G30, S1125 (2004)

G.G.Barnafoldi, G.Papp, P.Levai, G.Fai

Cronin effect at different rapidities at RHIC

NUCLEAR REACTIONS ¹⁹⁷Au(d, X), E(cm)=200 GeV/nucleon; calculated neutral pion spectra, yields, nuclear modification factor. Comparison with data.

doi: 10.1088/0954-3899/30/8/073
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2004FA21 Acta Phys.Hung.N.S. 19, 255 (2004)

G.Fai

Particle Production in Nuclear Collisions from pQCD

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E(cm)=130 GeV/nucleon; calculated particle yields, transverse momentum spectra. Perturbative QCD, comparison with data.

doi: 10.1556/APH.19.2004.3-4.17
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2004FA23 J.Phys.(London) G30, S1037 (2004)

G.Fai, J.Qiu, X.Zhang

Probing small-x gluons by low-mass Drell-Yan pairs at RHIC and LHC

doi: 10.1088/0954-3899/30/8/054
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2004ZH39 J.Phys.(London) G30, L49 (2004)

X.Zhang, G.Fai

The charged-hadron/pion ratio at the Relativistic Heavy Ion Collider

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E(cm)=200 GeV/nucleon; calculated charged-hadron to pion yield ratio vs transverse momentum, nuclear medium effects. Perturbative QCD, non-universal transverse momentum broadening, comparison with data.

doi: 10.1088/0954-3899/30/12/L03
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2003BB12 Acta Phys.Hung.N.S. 18, 79 (2003)

G.G.Barnafoldi, P.Levai, G.Papp, G.Fai, Y.Zhang

Perturbative QCD Results on Pion Production in pp, pA and AA Collisions

NUCLEAR REACTIONS ¹H, Be, W(p, X), S, Au(S, X), Pb(Pb, X), E=high; calculated pion yields, transverse momentum spectra. Perturbative QCD, comparisons with data.

doi: 10.1556/APH.18.2003.1.9
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2003FA09 Phys.Lett. B 567, 243 (2003)

G.Fai, J.Qiu, X.Zhang

Full transverse-momentum spectra of low-mass Drell-Yan pairs at LHC energies

NUCLEAR REACTIONS ¹H, Pb(p, X), Pb(Pb, X), E(cm)=5.5 TeV; calculated Drell-Yan pair transverse momentum distributions. QCD perturbation theory.

doi: 10.1016/j.phyletb.2003.05.007
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2003ZH44 Acta Phys.Hung.N.S. 18, 21 (2003)

X.Zhang, G.Fai

Resummed pQCD for W^± and Z⁰ Transverse Momentum Spectra at RHIC and LHC

NUCLEAR REACTIONS ¹H(p, X), Pb(Pb, X), ¹⁹⁷Au(¹⁹⁷Au, X), E=high; calculated W and Z bosons transverse momentum spectra. Resummation formalism, power corrections.

doi: 10.1556/APH.18.2003.1.3
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2002LE04 Nucl.Phys. A698, 631c (2002)

P.Levai, G.Papp, G.Fai, M.Gyulassy, G.G.Barnafoldi, I.Vitev, Y.Zhang

Discovery of Jet Quenching at RHIC and the Opacity of the Produced Gluon Plasma

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E(cm)=130 GeV/nucleon; analyzed pion spectra, yields; deduced static plasma opacity, related features.

doi: 10.1016/S0375-9474(01)01445-2
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2002LE23 J.Phys.(London) G28, 2059 (2002)

P.Levai, G.Papp, G.Fai, M.Gyulassy

K⁺/π⁺ Probes of Jet Quenching in AA Collisions

doi: 10.1088/0954-3899/28/7/371
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2002PA08 Nucl.Phys. A698, 627c (2002)

G.Papp, G.G.Barnafoldi, G.Fai, P.Levai, Y.Zhang

Multiple Scattering and p_t-Broadening at RHIC Energies

doi: 10.1016/S0375-9474(01)01444-0
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2002ZH07 Phys.Rev. C65, 034903 (2002)

Y.Zhang, G.Fai, G.Papp, G.G.Barnafoldi, P.Levai

High-p_T Pion and Kaon Production in Relativistic Nuclear Collisions

NUCLEAR REACTIONS Be, Ti, W(p, X), E=high; ¹H(p, X), (p-bar, X), E=high; S(S, X), Pb(Pb, X), ¹⁹⁷Au(¹⁹⁷Au, X), E=high; calculated pion and kaon spectra, production σ. Comparisons with data.

doi: 10.1103/PhysRevC.65.034903
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2002ZH19 Phys.Rev. C65, 064901 (2002)

X.Zhang, G.Fai

Nuclear Effects on Gauge Boson Production at Relativistic Energies

NUCLEAR REACTIONS ¹H, ¹⁹⁷Au(p, X), Pb(Pb, X), E=high; calculated gauge boson production σ, transverse momentum distributions.

doi: 10.1103/PhysRevC.65.064901
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2002ZH32 Phys.Lett. 545B, 91 (2002)

X.Zhang, G.Fai

Z⁰ Production as a Test of Nuclear Effects at the LHC

NUCLEAR REACTIONS ¹H(p, X), E(cm)=14 TeV; Pb(Pb, X), E(cm)=5.5 TeV; calculated Z⁰ transverse momentum distributions, shadowing effects.

doi: 10.1016/S0370-2693(02)02558-3
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2002ZH41 Phys.Rev.Lett. 89, 272301 (2002)

X.Zhang, G.Fai, P.Levai

Decisive Role of Fragmentation Functions in Hard Hadron Production

NUCLEAR REACTIONS ¹H(p, X), E=high; calculated particles transverse momentum, fragmentation functions. Comparison with data.

doi: 10.1103/PhysRevLett.89.272301
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2001BA67 J.Phys.(London) G27, 1767 (2001)

G.G.Barnafoldi, G.Fai, P.Levai, G.Papp, Y.Zhang

Jets and Produced Particles in pp Collisions from SPS to RHIC Energies for Nuclear Applications

NUCLEAR REACTIONS ¹H(p, X), E(cm)=20-200 GeV; calculated jet, photon, particle production σ, energy-dependent correction factors.

doi: 10.1088/0954-3899/27/8/306
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2001PA51 Acta Phys.Pol. B32, 4069 (2001)

G.Papp, P.Levai, G.G.Barnafoldi, Y.Zhang, G.Fai

Differences in High p_T Meson Production between CERN SPS and RHIC Heavy Ion Collisions

NUCLEAR REACTIONS S, ¹⁹⁷Au(S, X), Pb(Pb, X), ¹⁹⁷Au(¹⁹⁷Au, X), E=high; calculated pion yields, transverse momenta. Perturbative QCD improved parton model.

2000PA06 Phys.Rev. C61, 021902 (2000)

G.Papp, P.Levai, G.Fai

Saturating Cronin Effect in Ultrarelativistic Proton-Nucleus Collisions

NUCLEAR REACTIONS ¹H, Be, Ti, W(p, π⁰X), (p, γX), E(cm)=20-60 GeV; analyzed σ; deduced nuclear contributions, Cronin effect saturation.

doi: 10.1103/PhysRevC.61.021902
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1998JO19 Acta Phys.Hung.N.S. 8, 343 (1998)

C.W.Johnson, G.Fai

Saturation Properties of Nuclear Matter with Nonlocal Confining Solitons

1998SO16 Phys.Rev. C58, 1689 (1998)

C.-S.Song, G.Fai

Medium Effect on Photon Production in Ultrarelativistic Nuclear Collisions

NUCLEAR REACTIONS ¹⁹⁷Au(³²S, X), E=200 GeV/nucleon; calculated photon yield vs transverse momentum; deduced medium effects.

doi: 10.1103/PhysRevC.58.1689
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1997JO19 Phys.Rev. C56, 3353 (1997)

C.W.Johnson, G.Fai

High-Density Nuclear Matter with Nonlocal Confining Solitons

doi: 10.1103/PhysRevC.56.3353
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1997NE09 Acta Phys.Hung.N.S. 5, 27 (1997)

J.J.Neumann, B.Lavrenchuk, G.Fai

Feedback from Freeze-Out in Hydrodynamics

1996FA10 Phys.Lett. 373B, 5 (1996)

G.Fai, P.Danielewicz

Non-Equilibrium Modifications of the Nuclear Equation of State

doi: 10.1016/0370-2693(96)00088-3
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1996JO18 Phys.Lett. 386B, 75 (1996)

C.W.Johnson, G.Fai, M.R.Frank

The Hadron-Quark Transition with a Lattice of Nonlocal Confining Solitons

doi: 10.1016/0370-2693(96)00936-7
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1996NE01 Phys.Rev. C53, R14 (1996)

J.J.Neumann, D.Seibert, G.Fai

Electron-Positron Pairs from Thermal Resonances in Ultrarelativistic Nuclear Collisions

NUCLEAR REACTIONS ¹⁹⁷Au(S, X), E=ultrarelativistic; calculated e⁺e^- production from ρ⁰-, ω-decay. Equation of state approach, massless pion gas, quark-gluon plasma first-order phase transition.

doi: 10.1103/PhysRevC.53.R14
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1995NE02 Phys.Rev. C51, 1460 (1995)

J.J.Neumann, D.Seibert, G.Fai

Thermal Photon Production in High-Energy Nuclear Collisions

NUCLEAR REACTIONS ¹⁹⁷Au(S, X), Pb(Pb, X), E at super proton synchrotron; calculated photon spectra. Boost-invariant, one-dimensional fluid dynamics model.

doi: 10.1103/PhysRevC.51.1460
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1994NE03 Phys.Lett. 329B, 419 (1994)

J.J.Neumann, G.Fai

Classical Lagrangian Model of the Pauli Principle

doi: 10.1016/0370-2693(94)91084-7
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1994SE11 Phys.Rev. C50, 2532 (1994)

D.Seibert, G.Fai

Heavy-Resonance Production in High-Energy Nuclear Collisions

doi: 10.1103/PhysRevC.50.2532
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1990FA10 Phys.Scr. T32, 81 (1990)

G.Fai

Multifragmentation Theory

NUCLEAR REACTIONS ²³⁸U(³⁶Ar, X), E=35 MeV/nucleon; ¹⁹⁷Au, Ag(C, X), E=30 MeV/nucleon; Xe(p, X), E ≥ 30 MeV; analyzed data. Multifragmentation theory.

doi: 10.1088/0031-8949/1990/T32/014
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1990JA03 Nucl.Phys. A509, 195 (1990)

B.Jakobsson, G.Jonsson, L.Karlsson, V.Kopljar, B.Noren, K.Soderstrom, F.Schussler, E.Monnand, H.Nifenecker, G.Fai, J.P.Bondorf, K.Sneppen

On the Observation of a Transition from Fusion to Multifragmentation in High Multiplicity ¹⁶O Induced Reactions

NUCLEAR REACTIONS Br, Ag(¹⁶O, X), E=94 MeV/nucleon; measured high multiplicity collision charge distribution; deduced charge distribution moments.

doi: 10.1016/0375-9474(90)90381-U
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1989YU02 Phys.Rev. C40, 1448 (1989)

H.J.Yuan, H.L.Lin, G.Fai, S.A.Moszkowski

Proton Mean-Free Path in Nuclear Matter and in Finite Nuclei

NUCLEAR STRUCTURE ⁴⁰Ca, ⁹⁰Zr, ²⁰⁸Pb; calculated proton mean free path vs Ep. Green's function method, Skyrme interaction.

doi: 10.1103/PhysRevC.40.1448
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1988FA09 Nucl.Phys. A487, 397 (1988)

G.Fai, J.Randrup

Hot Nuclei in a Nucleon Vapor

NUCLEAR STRUCTURE A=20; A=40; A=100; calculated hot nucleus parameters.

doi: 10.1016/0375-9474(88)90620-3
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1986MA51 Phys.Rev. C34, 1342 (1986)

R.Madey, J.Varga, G.Fai, A.F.Barghouty, B.D.Anderson, A.R.Baldwin, R.Cecil, J.W.Watson, G.D.Westfall

Angular Distributions of Low-Energy Neutrons from 390-MeV/Nucleon Ne + Pb Collisions

NUCLEAR REACTIONS Pb(Ne, nX), E=390 MeV/nucleon; measured σ(θn). TOF, plastic scintillators. Three source model calculations.

doi: 10.1103/PhysRevC.34.1342
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1985MA44 Phys.Rev.Lett. 55, 1453 (1985)

R.Madey, J.Varga, A.R.Baldwin, B.D.Anderson, R.A.Cecil, G.Fai, P.C.Tandy, J.W.Watson

Inclusive Neutron Spectra at 0° from the Reactions Pb(Ne, n)X and NaF(Ne, n)X at 390 and 790 MeV per Nucleon

NUCLEAR REACTIONS Pb, Na, F(Ne, nX), E=390, 790 MeV/nucleon; measured inclusive σ(En, θ=0°); deduced projectile evaporation. Natural Pb, NaF targets.

doi: 10.1103/PhysRevLett.55.1453
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1984BO40 Nucl.Phys. A430, 445 (1984)

J.P.Bondorf, M.N.De, G.Fai, A.O.T.Karvinen

Spectator Recoil in Intermediate-Energy Heavy Ion Collisions

NUCLEAR REACTIONS ¹⁰⁸Ag(⁴⁰Ca, X), (¹²C, X), E=86 MeV/nucleon; ¹⁰⁸Ag(²⁰Ne, X), E=170 MeV/nucleon; calculated fragment recoil momentum vs spectator mass.

doi: 10.1016/0375-9474(84)90048-4
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1980BO01 Nucl.Phys. A333, 285 (1980)

J.P.Bondorf, J.N.De, G.Fai, A.O.T.Karvinen, B.Jakobsson, J.Randrup

Promptly Emitted Particles in Nuclear Collisions

NUCLEAR REACTIONS ¹⁵⁸Gd(¹²C, X), E=152 MeV; ¹⁴⁶Nd(¹⁶O, X), E=126.5 MeV; ¹⁵⁸Gd(α, X), E=45 MeV; ¹³⁶Xe(⁴⁵Sc, X), E=1360 MeV; calculated σ(E) for 1, 2 prompt nucleons. Proximity model, coupling of internal nucleon motion to relative nuclear motion.

doi: 10.1016/0375-9474(80)90234-1
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1979BO15 Phys.Lett. 84B, 162 (1979)

J.P.Bondorf, J.N.De, A.O.T.Karvinen, G.Fai, B.Jakobsson

Prompt Emission of Nucleons in Heavy-Ion Collisions

NUCLEAR REACTIONS ¹⁴⁶Nd(¹⁶O, n), E=126.5 MeV; ¹⁵⁸Gd(¹²C, n), E=152 MeV; calculated σ(E, θn, En); deduced mechanism of production of quasifree prompt emission. Sharp surface model.

doi: 10.1016/0370-2693(79)90273-9
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1979JA11 Phys.Lett. 82B, 35 (1979)

B.Jakobsson, J.P.Bondorf, G.Fai

Production of Pions in Heavy Ion Reactions below 500 MeV/Nucleon

NUCLEAR REACTIONS ¹⁶O, ¹⁰⁸Ag, ²³⁸U(²⁰Ne, π⁺), (²⁰Ne, π^-), E=250 MeV/nucleon; ²³⁸U(¹⁶O, π⁺), (¹⁶O, π^-), E not given; Li, Na, Ba, Pb(¹²C, π^-), (⁴⁰Ar, π^-), E=400 MeV/nucleon; calculated production σ, average multiplicity, absorption probability. Glauber multiple-scattering formalism with independent NN-scattering, two-step isobar model.