NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = R.Vogt Found 120 matches. Showing 1 to 100. [Next]2023GI01 Phys.Rev. C 107, 014612 (2023) N.P.Giha, S.Marin, J.A.Baker, I.E.Hernandez, K.J.Kelly, M.Devlin, J.M.O'Donnell, R.Vogt, J.Randrup, P.Talou, I.Stetcu, A.E.Lovell, O.Litaize, O.Serot, A.Chebboubi, C.-Y.Wu, S.D.Clarke, S.A.Pozzi Correlations between energy and γ-ray emission in 239Pu(n, f) NUCLEAR REACTIONS 239Pu(n, f), E=2-40 MeV; measured fragments, En, In, Eγ, Iγ, (fragments)γ-coin, (fragment)n-coin, nγ-coin; deduced γ spectrum, γ multiplicity, linear relation between incident neutron energy and γ multiplicity. Comparison to fission model calculations done with CGMF, FIFRELIN and FREYA codes. Multiplicity results are compared to ENDF/B-VIII.0 data and to experimental data on 238U(n, F), 239Pu(d, F), 233Pu(d, F), 240Pu(d, F) reactions. Broad-spectrum neutron beam produced via spallation reaction of an 800 MeV proton beam on W target (Los Alamos Neutron Science Center). Chi-Nu liquid scintillator array, a hemispherical array of 54 EJ-309 (n- and γ- measurement) surrounding multifoil parallel-plate avalanche counter (PPAC) serving as target and contain ing 239Pu (fragment measurement).
doi: 10.1103/PhysRevC.107.014612
2023SM04 Front. Astron. Space Sci. 10, 1228901 (2023) M.S.Smith, R.L.Vogt, K.A.LaBel Nuclear data for space exploration
doi: 10.3389/fspas.2023.1228901
2023VO05 Phys.Rev. C 108, 015201 (2023) Contribution from intrinsic charm production to fixed-target interactions with the SMOG Device at LHCb
doi: 10.1103/PhysRevC.108.015201
2022CH27 Phys.Rev. C 105, 055202 (2022) Quarkonium polarization in Pb+Pb collisions in the improved color evaporation model
doi: 10.1103/PhysRevC.105.055202
2022KO12 Phys. Rev. Res. 4, 021001 (2022) K.Kolos, V.Sobes, R.Vogt, C.E.Romano, M.S.Smith, L.A.Bernstein, D.A.Brown, M.T.Burkey, Y.Danon, M.A.Elsawi, B.L.Goldblum, L.H.Heilbronn, S.L.Hogle, J.Hutchinson, B.Loer, E.A.McCutchan, M.R.Mumpower, E.M.O'Brien, C.Percher, P.N.Peplowski, J.J.Ressler, N.Schunck, N.W.Thompson, A.S.Voyles, W.Wieselquist, M.Zerkle Current nuclear data needs for applications
doi: 10.1103/PhysRevResearch.4.021001
2022MA26 Phys.Rev. C 105, 054609 (2022) S.Marin, E.P.Sansevero, M.S.Okar, I.E.Hernandez, R.Vogt, J.Randrup, S.D.Clarke, V.A.Protopopescu, S.A.Pozzi Directional dependence of the event-by-event neutron-γ multiplicity correlations in 252Cf(sf) RADIOACTIVITY 252Cf(SF); analyzed Eg and En data collected at the Chi-Nu array at the Los Alamos Neutron Science Center with considering the angle between the emitted particles in addition to their individual energies; deduced nγ-correlations, enhancement of γ-emission around 0.7 and 1.2 MeV, directional alignment for Eγ below 0.7 MeV, correlation between fragment excitation energies and angular momentum. Comparison with model calculations.
doi: 10.1103/PhysRevC.105.054609
2022RA19 Phys.Rev. C 106, 014609 (2022) Probing fission fragment angular momenta by photon measurements RADIOACTIVITY 252Cf(SF); calculated relaxation times for wriggling, bending and twisting as function of neck radius, angular distribution of the collective E2 photons from fission fragments, average angular distribution coefficients, distribution of the opening angle between pairs of E2 photons emitted from even-even product partners. Discussed how certain photon measurements may helpin investigations the of the various rotational modes in fission. Simulations with fission event generator FREYA.
doi: 10.1103/PhysRevC.106.014609
2022VO05 Phys.Rev. C 106, 025201 (2022) Energy dependence of intrinsic charm production: Determining the best energy for observation
doi: 10.1103/PhysRevC.106.025201
2021GJ01 Phys.Rev. C 103, 034609 (2021) D.Gjestvang, S.Siem, F.Zeiser, J.Randrup, R.Vogt, J.N.Wilson, F.Bello-Garrote, L.A.Bernstein, D.L.Bleuel, M.Guttormsen, A.Gorgen, A.C.Larsen, K.L.Malatji, E.F.Matthews, A.Oberstedt, S.Oberstedt, T.Tornyi, G.M.Tveten, A.S.Voyles Excitation energy dependence of prompt fission γ-ray emission from 241Pu NUCLEAR REACTIONS 240Pu(d, pF)241Pu*, E=13.5 MeV; measured outgoing protons using SiRi, a silicon ΔE-E detector, fission fragments using NIFF, consisting of four parallel plate avalanche counters (PPACs), prompt fission γ rays (PFG), (particle)γ-coin using Oslo Scintillator Array (OSCAR) of 30 LaBr3:Ce scintillators for γ radiation at the Oslo Cyclotron Laboratory; deduced average total PFG multiplicity per fission, average total PFG energy released per fission, and the average PFG energy in the excitation range of 5.75-8.25 MeV. Comparison with simulations using the fission model FREYA, with previous experimental results, and evaluation in ENDF/B-VIII.0.
doi: 10.1103/PhysRevC.103.034609
2021MA51 Phys.Rev. C 104, L021601 (2021) P.Marevic, N.Schunck, J.Randrup, R.Vogt Angular momentum of fission fragments from microscopic theory NUCLEAR REACTIONS 239Pu(n, F), E=thermal; calculated angular-momentum distributions of 24 fission fragments over a wide range of fragment masses, and total average photon multiplicities. 239Pu(n, F)128Sn/132Sn/138Xe/130Sn/150Ce/110Ru/90Kr, E=thermal; calculated angular-momentum distributions of primary fission fragments, with binding energy calculated as a function of the quadrupole deformation parameter β2 using the HFB model; deduced dependency of nuclear shell structure and deformation on the angular momentum of the fragments. Calculations used fission model FREYA, and a starting set of 1545 scission configurations.
doi: 10.1103/PhysRevC.104.L021601
2021MA54 Phys.Rev. C 104, 024602 (2021) S.Marin, M.S.Okar, E.P.Sansevero, I.E.Hernandez, C.A.Ballard, R.Vogt, J.Randrup, P.Talou, A.E.Lovell, I.Stetcu, O.Serot, O.Litaize, A.Chebboubi, S.D.Clarke, V.A.Protopopescu, S.A.Pozzi Structure in the event-by-event energy-dependent neutron-γ multiplicity correlations in 252Cf(sf) RADIOACTIVITY 252Cf(SF); analyzed Eγ and E(n) data collected at the Chi-Nu array at the Los Alamos Neutron Science Center with the application of the normalized differential multiplicity covariances; deduced neutron-γ correlations, evidence for enhancements in neutron-γ correlations around Eγ=0.7 and 1.2 MeV. Comparison with model calculations. Relevance to disagreement in the literature about correlations between neutron-γ competition and fragment properties.
doi: 10.1103/PhysRevC.104.024602
2021RA14 Phys.Rev.Lett. 127, 062502 (2021) Generation of Fragment Angular Momentum in Fission NUCLEAR REACTIONS 235,238U, 239Pu(n, F), E not given; calculated fission fragments distribution. Comparison with available data. The fission model FREYA. RADIOACTIVITY 252CF(SF); calculated fission fragments distribution. Comparison with available data. The fission model FREYA.
doi: 10.1103/PhysRevLett.127.062502
2021VO02 Phys.Rev. C 103, 014610 (2021) Angular momentum effects in fission NUCLEAR REACTIONS 235U(n, F), E=0.1, 20 MeV; calculated distribution of the opening angle between the spins of the two primary fission fragments, angular distribution of the evaporated neutrons relative to the spin direction of the emitting fragment, mean number of photons emitted as a function of the sum of spins of two primary fragments, contour plot of the velocity distribution of evaporated neutrons, distribution of neutron-neutron opening angle in the plane transverse to the direction of the light product nucleus. 235U(n, F), E>0, <1, >2 MeV; calculated laboratory angular distribution of the evaporated neutrons relative to the direction of the light primary fragment, with and without a rotational boost. 235U(n, F), E>2, <2 MeV; calculated two-neutron angular correlations. 235,235mU(n, F), E=thermal; calculated neutron multiplicity as a function of TKE. Calculations used fission simulation model FREYA, a Monte Carlo approach.
doi: 10.1103/PhysRevC.103.014610
2021VO04 Phys.Rev. C 103, 035204 (2021) Limits on intrinsic charm production from the SeaQuest experiment
doi: 10.1103/PhysRevC.103.035204
2020KL01 Phys.Rev. C 102, 015808 (2020) S.R.Klein, S.A.Robertson, R.Vogt Nuclear effects in high-energy neutrino interactions NUCLEAR REACTIONS He, Li, C, O, Ne, Na, Mg, Al, Si, S, Ca, V, Fe, Ni, Cu(ν, ν), (ν-bar, ν-bar), (ν, X)(ν-bar, X), E=1-10000 TeV; calculated nuclear modification factors for charged current and neutral current interactions with neutrinos and antineutrinos relative to deuterium target using EPS09 and EPPS16 sets at next-to-leading order, based on standard QCD; investigated role of two nuclear effects: shadowing and violation of isospin invariance in ultra-high-energy neutrino interactions. Relevance to study of neutrinos using neutrino telescopes such as IceCube, KM3NeT, and Baikal-GVD, and to probing the earth through neutrino absorption tomography.
doi: 10.1103/PhysRevC.102.015808
2020MA20 Nucl.Instrum.Methods Phys.Res. A968, 163807 (2020) S.Marin, V.A.Protopopescu, R.Vogt, M.J.Marcath, S.Okar, M.Hua, P.Talou, P.F.Schuster, S.D.Clarke, S.A.Pozzi Event-by-event neutron-photon multiplicity correlations in 252Cf(sf) RADIOACTIVITY 252Cf(SF); analyzed available data using unfolding techniques in comparison with predictions of model-based calculations; deduced a significant event-by-event neutron-photon emission competition following the spontaneous fission of 252Cf.
doi: 10.1016/j.nima.2020.163907
2020VO02 Phys.Rev. C 101, 024910 (2020) bb-bar kinematic correlations in cold nuclear matter
doi: 10.1103/PhysRevC.101.024910
2019RA13 Phys.Rev. C 99, 054619 (2019) Sensitivity of neutron observables to the model input in simulations of 252Cf(sf) RADIOACTIVITY 252Cf(SF); analyzed mass distribution, total kinetic energy (TKE), width of the total kinetic energy distribution of fission fragments; calculated neutron multiplicity distribution, neutron multiplicity covariance matrix elements, factorial moments of the neutron multiplicity distribution, neutron spectra, angular distribution of two neutrons, neutron energy-energy correlation, anticorrelation between average total kinetic energy and average neutron multiplicity using the FREYA code. Comparison with experimental data. COMPILATION 252Cf; compiled experimental data for spontaneous fission of 252Cf for mass-dependent fragment yields, the mass-dependent average total fragment kinetic energy (TKE), and the associated TKE dispersion σ(TKE, A) based on entries in the EXFOR database from 1963 to 2014.
doi: 10.1103/PhysRevC.99.054619
2019SC12 Phys.Rev. C 100, 014605 (2019) P.F.Schuster, M.J.Marcath, S.Marin, S.D.Clarke, M.Devlin, R.C.Haight, R.Vogt, P.Talou, I.Stetcu, T.Kawano, J.Randrup, S.A.Pozzi High resolution measurement of tagged two-neutron energy and angle correlations in 252Cf (sf) RADIOACTIVITY 252Cf(SF); measured prompt neutron time of flight, angular distribution of neutrons, nn-coin, prompt neutron emission anisotropy, correlations in angle and energy between prompt neutrons emitted in spontaneous fission using fission chamber and the Chi-Nu liquid scintillator detector array at LANSCE-LANL facility. Comparison with simulations produced by the fission event generators CGMF, FREYA, and MCNPX-POLIMI IPOL(1)=1.
doi: 10.1103/PhysRevC.100.014605
2019VO01 Nucl.Phys. A982, 751c (2019) Quarkonium Production and Polarization in an Improved Color Evaporation Model
doi: 10.1016/j.nuclphysa.2018.08.003
2018AL10 Nucl.Phys. A972, 18 (2018) J.L.Albacete, F.Arleo, G.G.Barnafoldi, G.Biro, D.d'Enterria, B.Ducloue, K.J.Eskola, E.G.Ferreiro, M.Gyulassy, S.M.Harangozo, I.Helenius, Z.-B.Kang, P.Kotko, S.A.Kulagin, K.Kutak, J.P.Lansberg, T.Lappi, P.Levai, Z.-W.Lin, G.Ma, Y.-Q.Ma, H.Mantysaari, H.Paukkunen, G.Papp, R.Petti, A.H.Rezaeian, P.Ru, S.Sapeta, B.Schenke, S.Schlichting, H.-S.Shao, P.Tribedy, R.Venugopalan, I.Vitev, R.Vogt, E.Wang, X.-N.Wang, R.Xing, R.Xu, B.-W.Zhang, H.-F.Zhang, W.-N.Zhang Predictions for cold nuclear matter effects in p+Pb collisions at √ SNN = 8.16 TeV
doi: 10.1016/j.nuclphysa.2017.11.015
2018MA25 Phys.Rev. C 97, 044622 (2018) M.J.Marcath, R.C.Haight, R.Vogt, M.Devlin, P.Talou, I.Stetcu, J.Randrup, P.F.Schuster, S.D.Clarke, S.A.Pozzi Measured and simulated 252Cf(sf) prompt neutron-photon competition RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, E(n), I(n), nγ-coin, time of flight distributions for neutrons and photons, event-by-event neutron-photon correlation using Chi-Nu liquid scintillator array of 45 liquid organic scintillation detectors and a fission chamber at LANL; deduced neutron and photon multiplicities. Comparison with MCPNX-PoliMi simulation with CGMF and FREYA models.
doi: 10.1103/PhysRevC.97.044622
2018TA05 Eur.Phys.J. A 54, 9 (2018) P.Talou, R.Vogt, J.Randrup, M.E.Rising, S.A.Pozzi, J.Verbeke, M.T.Andrews, S.D.Clarke, P.Jaffke, M.Jandel, T.Kawano, M.J.Marcath, K.Meierbachtol, L.Nakae, G.Rusev, A.Sood, I.Stetcu, C.Walker Correlated prompt fission data in transport simulations COMPILATION 235U, 239Pu(n, F), E=thermal;252Cf(SF); compiled average prompt fission neutron multiplicity vs fragment mass, prompt fission neutron σ(En), γ-decay energy spectrum σ(Eγ), γ multiplicity, n-n angular correlation. Calculated σ, yields using FREYA and CGMF codes. Compared with data.
doi: 10.1140/epja/i2018-12455-0
2018VE01 Phys.Rev. C 97, 044601 (2018) J.M.Verbeke, L.F.Nakae, R.Vogt Neutron-neutron angular correlations in spontaneous fission of 252Cf and 240Pu RADIOACTIVITY 240Pu, 252Cf(SF); measured E(n), nn-coin, nn(θ), time-of-flight using array of 77 scintillation detectors with improved discrimination between neutrons and photons. Simulations using customized version of MCNPX 2.7.0 with the LLNL Fission Library/FREYA; deduced partition of excitation energy between the two fission fragments. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.97.044601
2018VO11 Phys.Rev. C 98, 034907 (2018) Heavy flavor azimuthal correlations in cold nuclear matter
doi: 10.1103/PhysRevC.98.034907
2017CL01 Phys.Rev. C 95, 064612 (2017) S.D.Clarke, B.M.Wieger, A.Enqvist, R.Vogt, J.Randrup, R.C.Haight, H.Y.Lee, B.A.Perdue, E.Kwan, C.Y.Wu, R.A.Henderson, S.A.Pozzi Measurement of the energy and multiplicity distributions of neutrons from the photofission of 235U NUCLEAR REACTIONS 235U(γ, F), E<800 MeV white photon source; measured E(n), I(n), neutron time-of-flight spectrum, prompt fission neutron spectrum, neutron multiplicity distribution, average energy of correlated photofission neutron pairs as function of the angle between detectors at the WNR-15L beam line at LANSCE-LANL. Comparison with simulations using FREYA and MCNPX-POLIMI codes.
doi: 10.1103/PhysRevC.95.064612
2017VO13 Phys.Rev. C 96, 064620 (2017) Improved modeling of photon observables with the event-by-event fission model FREYA RADIOACTIVITY 252Cf(SF); calculated photon spectrum, average total photon energy, average photon multiplicity, and energy per photon as a function of fragment mass, total photon energy and the photon multiplicity as functions of total fragment kinetic energy with and without the GDR and RIPL-3, mean total photon energy, mean photon multiplicity and energy per photon as functions of fragment mass number, average fragment angular momentum as function of fragment mass, total photon energy, and photon multiplicity as functions of total fragment kinetic energy TKE, photon multiplicity distributions. Calculations using FREYA (Fission Reaction Event Yield Algorithm) code. Comparison with experimental data. NUCLEAR REACTIONS 233,235U, 239Pu(n, F), E=thermal; calculated total photon energy and photon multiplicity, energy per photon as function of fragment mass, total photon energy as a function of total fragment kinetic energy (TKE), photon energy spectrum. Calculations using FREYA (Fission Reaction Event Yield Algorithm) code. Comparison with experimental data.
doi: 10.1103/PhysRevC.96.064620
2016CA03 Nucl.Data Sheets 131, 1 (2016) R.Capote, Y.-J.Chen, F.-J.Hambsch, N.V.Kornilov, J.P.Lestone, O.Litaize, B.Morillon, D.Neudecker, S.Oberstedt, T.Ohsawa, N.Otuka, V.G.Pronyaev, A.Saxena, O.Serot, O.A.Shcherbakov, N.-C.Shu, D.L.Smith, P.Talou, A.Trkov, A.C.Tudora, R.Vogt, A.S.Vorobyev Prompt Fission Neutron Spectra of Actinides NUCLEAR REACTIONS 232Th, 233,234,235,238U, 237Np, 239Pu(n, F), E<30 MeV; calculated prompt fission En, In; Comparison with available data.
doi: 10.1016/j.nds.2015.12.002
2016VO09 Nucl.Phys. A956, 697 (2016) Cold nuclear matter effects on J/ψ and Υ production in p+Pb collisions at 5 TeV and Pb+Pb collisions at 5.1 TeV
doi: 10.1016/j.nuclphysa.2015.12.013
2016WA03 Phys.Rev. C 93, 014606 (2016) T.Wang, G.Li, L.Zhu, Q.Meng, L.Wang, H.Han, W.Zhang, H.Xia, L.Hou, R.Vogt, J.Randrup Correlations of neutron multiplicity and γ-ray multiplicity with fragment mass and total kinetic energy in spontaneous fission of 252Cf RADIOACTIVITY 252Cf(SF); measured E(n), I(n), Eγ, Iγ; deduced total kinetic energy (TKE), neutron and γ-ray multiplicities, correlations of neutron and γ-ray multiplicities, ratio of average γ-ray yield to the average neutron multiplicity as function of fragment mass, γ-ray multiplicity as a function of the total fragment kinetic energy TKE.
doi: 10.1103/PhysRevC.93.014606
2015KU21 Phys.Rev. C 92, 024908 (2015) Quarkonia suppression in PbPb collisions at √ sNN = 2.76 TeV
doi: 10.1103/PhysRevC.92.024908
2015VE02 Comput.Phys.Commun. 191, 178 (2015) J.M.Verbeke, J.Randrup, R.Vogt Fission Reaction Event Yield Algorithm, FREYA - For event-by-event simulation of fission
doi: 10.1016/j.cpc.2015.02.002
2015VO13 Phys.Rev. C 92, 034909 (2015) Shadowing effects on J/ψ and Υ production at energies available at the CERN Large Hadron Collider
doi: 10.1103/PhysRevC.92.034909
2014CH24 Nucl.Data Sheets 118, 1 (2014) M.B.Chadwick, E.Dupont, E.Bauge, A.Blokhin, O.Bouland, D.A.Brown, R.Capote, A.Carlson, Y.Danon, C.De Saint Jean, M.Dunn, U.Fischer, R.A.Forrest, S.C.Frankle, T.Fukahori, Z.Ge, S.M.Grimes, G.M.Hale, M.Herman, A.Ignatyuk, M.Ishikawa, N.Iwamoto, O.Iwamoto, M.Jandel, R.Jacqmin, T.Kawano, S.Kunieda, A.Kahler, B.Kiedrowski, I.Kodeli, A.J.Koning, L.Leal, Y.O.Lee, J.P.Lestone, C.Lubitz, M.MacInnes, D.McNabb, R.McKnight, M.Moxon, S.Mughabghab, G.Noguere, G.Palmiotti, A.Plompen, B.Pritychenko, V.Pronyaev, D.Rochman, P.Romain, D.Roubtsov, P.Schillebeeckx, M.Salvatores, S.Simakov, E.Sh.Soukhovitskii, J.C.Sublet, P.Talou, I.Thompson, A.Trkov, R.Vogt, S.van der Marck The CIELO Collaboration: Neutron Reactions on 1H, 16O, 56Fe, 235, 238U, and 239Pu COMPILATION 1H, 16O, 56Fe, 235,238U, 239Pu(n, x), E≈0-20 MeV; analyzed available data on σ, neutron multiplicity, criticality using ENDF/B-VII.1, JENDL-4.0, JEFF-3.1, ROSFOND 2010, CENDL-3.1, EAF-2010 evaluated nuclear libraries, Atlas of Neutron Resonances, Neutron Cross Section Standards evaluations; deduced recommendations for CIELO library, parameters, Maxwellian-averaged, thermal, californium σ, Westcott factors, resonance integrals. Compared with available data.
doi: 10.1016/j.nds.2014.04.002
2014MU01 Phys.Rev. C 89, 034615 (2014) J.M.Mueller, M.W.Ahmed, R.H.France, M.S.Johnson, H.J.Karwowski, L.S.Myers, J.Randrup, M.H.Sikora, M.C.Spraker, S.Stave, J.R.Tompkins, R.Vogt, H.R.Weller, C.S.Whisnant, W.R.Zimmerman Prompt neutron polarization asymmetries in photofission of 232Th, 233, 235, 238U, 237Np, and 239, 240Pu NUCLEAR REACTIONS 232Th, 233,235,238U, 237Np, 239,240Pu(polarized γ, F), E=5.3-7.6 MeV; measured E(n), I(n), time-of flight spectrum, angular distribution, and polarization asymmetry of prompt neutrons generated by fission, θ(fragment) at HIγS-TUNL facility; deduced angular distribution coefficients b and c, and compared with predicted values from FREYA computer code of event-by-event Monte Carlo prompt neutron+γ-ray emission calculation. Discussed differences in polarization asymmetries between the even-even actinides and odd-A actinides.
doi: 10.1103/PhysRevC.89.034615
2014RA09 Phys.Rev. C 89, 044601 (2014) Refined treatment of angular momentum in the event-by-event fission model freya RADIOACTIVITY 252Cf(SF); calculated angular correlation of evaporated neutrons, angular distribution of neutrons relative to the direction of the angular momentum of the emitted nucleus, photon multiplicity distribution using refined event-by-event fission model FREYA code. Treatment of angular momenta in FREYA. Comparison with experimental data. NUCLEAR REACTIONS 239Pu(n, F), E=thermal; calculated distribution of the angle between the post-evaporation fragment angular momentum and that of the of the initial compound nucleus using improved FREYA code.
doi: 10.1103/PhysRevC.89.044601
2014TA16 Nucl.Data Sheets 118, 227 (2014) P.Talou, T.Kawano, I.Stetcu, R.Vogt, J.Randrup Monte Carlo Predictions of Prompt Fission Neutrons and Photons: a Code Comparison RADIOACTIVITY 252Cf(SF); calculated neutron, γ average kinetic energy, neutron multiplicity, γ multiplicity from different fission fragments. Compared with
doi: 10.1016/j.nds.2014.04.043
2014VO04 Nucl.Data Sheets 118, 220 (2014) Event-by-event Modeling of Prompt Neutrons and Photons from Neutron-induced and Spontaneous Fission with FREYA NUCLEAR REACTIONS 235U, 239Pu(n, F), E not given (probably low); calculated neutron, γ average kinetic energy, neutron multiplicity, γ multiplicity from fission fragments. Compared with other calculations and data. RADIOACTIVITY 252Cf(SF); calculated neutron, γ average kinetic energy, neutron multiplicity, γ multiplicity from fission fragments. Compared with other calculations and data.
doi: 10.1016/j.nds.2014.04.041
2014VO06 Nucl.Phys. A928, 222 (2014) J/ψ's are jazzy
doi: 10.1016/j.nuclphysa.2014.03.022
2014VO13 Nucl.Phys. A932, 494c (2014) Predictions for p + Pb collisions at √ sNN = 5 TeV: Expectations vs. data
doi: 10.1016/j.nuclphysa.2014.07.004
2014VO14 Phys.Rev. C 90, 064623 (2014) Neutron angular correlations in spontaneous and neutron-induced fission NUCLEAR REACTIONS 235U(n, F), E>0.425 keV; calculated nn(θ, E(n)) between two neutrons emitted in fission using event-by-event models of fission, FREYA. Comparison with experimental data, including that for thermal-neutron induced fission. RADIOACTIVITY 252Cf(SF); calculated nn(θ) between two neutrons emitted as a function of the opening angle, neutron multiplicity distribution using event-by-event models of fission, FREYA. Comparison with experimental data.
doi: 10.1103/PhysRevC.90.064623
2013MC06 Phys.Rev. C 87, 054910 (2013) D.McGlinchey, A.D.Frawley, R.Vogt Impact-parameter dependence of the nuclear modification of J/ψ production in d+Au collisions at √ sNN=200 GeV
doi: 10.1103/PhysRevC.87.054910
2013NE01 Phys.Rev. C 87, 014908 (2013) R.E.Nelson, R.Vogt, A.D.Frawley Narrowing the uncertainty on the total charm cross section and its effect on the J/ψ cross section
doi: 10.1103/PhysRevC.87.014908
2013VO04 Phys.Rev. C 87, 044602 (2013) Event-by-event study of photon observables in spontaneous and thermal fission RADIOACTIVITY 252Cf(SF); analyzed prompt photon multiplicity distribution as function of fragment mass and TKE, average neutron multiplicity as a function of fragment TKE, neutron-photon correlations, nn(θ). Event-by-event FREYA fission model by assuming no competition between prompt photon and neutron emissions. NUCLEAR REACTIONS 235U(n, F), E=thermal; analyzed prompt photon multiplicity distribution, neutron-photon correlations. Event-by-event FREYA fission model by assuming no competition between prompt photon and neutron emissions.
doi: 10.1103/PhysRevC.87.044602
2013VO11 Nucl.Phys. 910-911, 231c (2013) R.Vogt, R.E.Nelson, A.D.Frawley Improving the J/ψ Production Baseline at RHIC and the LHC
doi: 10.1016/j.nuclphysa.2012.12.106
2012DI05 Phys.Rev. C 85, 034906 (2012) Charmonium production and corona effect
doi: 10.1103/PhysRevC.85.034906
2012KU32 Phys.Rev. C 86, 054907 (2012) Components of the dilepton continuum in Pb+Pb collisions at √ sNN =2.76 TeV
doi: 10.1103/PhysRevC.86.054907
2012VO01 Phys.Rev. C 85, 024608 (2012) R.Vogt, J.Randrup, D.A.Brown, M.A.Descalle, W.E.Ormand Event-by-event evaluation of the prompt fission neutron spectrum from 239Pu(n, f) NUCLEAR REACTIONS 239Pu(n, F), E<20 MeV; analyzed chance fission probability, probability for pre-equilibrium neutron emission, fragment mass yields, total and average fragment kinetic energies, neutron multiplicity, prompt neutron spectra, neutron-neutron correlation coefficient contour plots. Event-by-event fission model FREYA with multichance fission and pre-equilibrium neutron emission. Comparison with ENDF-B/VII.0 evaluation.
doi: 10.1103/PhysRevC.85.024608
2011BR16 J.Korean Phys.Soc. 59, 1084s (2011) D.Brown, B.Beck, M.-A.Descalle, R.Hoffman, E.Ormand, P.Navratil, N.Summers, I.Thompson, R.Vogt, W.Younes, R.Barnowski Overview of the 2009 Release of the Evaluated Nuclear Data Library (ENDL2009) COMPILATION 27Al(n, γ), (n, X), E=1.E-8-20 MeV;27Al(n, 2n), E=10-20 MeV;181Ta, 187Re(n, γ), (n, x), E=1.E-11-20 MeV;181Ta, 187Re(n, 2n), E=5-20 MeV;76,77,78Kr, 122,123,124Xe(n, X), E=0-20 MeV; calculated, evaluated σ. TALYS code. ENDL2009 library, 585 transport-ready evaluations in neutron sub-library and 35 in charged-particle sub-libraries.
doi: 10.3938/jkps.59.1084
2011CH57 Nucl.Data Sheets 112, 2887 (2011) M.B.Chadwick, M.Herman, P.Oblozinsky, M.E.Dunn, Y.Danon, A.C.Kahler, D.L.Smith, B.Pritychenko, G.Arbanas, R.Arcilla, R.Brewer, D.A.Brown, R.Capote, A.D.Carlson, Y.S.Cho, H.Derrien, K.Guber, G.M.Hale, S.Hoblit, S.Holloway, T.D.Johnson, T.Kawano, B.C.Kiedrowski, H.Kim, S.Kunieda, N.M.Larson, L.Leal, J.P.Lestone, R.C.Little, E.A.McCutchan, R.E.MacFarlane, M.MacInnes, C.M.Mattoon, R.D.McKnight, S.F.Mughabghab, G.P.A.Nobre, G.Palmiotti, A.Palumbo, M.T.Pigni, V.G.Pronyaev, R.O.Sayer, A.A.Sonzogni, N.C.Summers, P.Talou, I.J.Thompson, A.Trkov, R.L.Vogt, S.C.van der Marck, A.Wallner, M.C.White, D.Wiarda, P.G.Young ENDF/B-VII.1 Nuclear Data for Science and Technology: Cross Sections, Covariances, Fission Product Yields and Decay Data COMPILATION Z=1-118; compiled, analyzed decay data, Maxwellian averaged neutron capture σ, neutron-induced fission σ. NUCLEAR REACTIONS 1,2H, 3He, 6,7Li, 7,9Be, 10,11B, C, 14,15N, 16,17O, 19F, 22,23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,33,34,36S, 35,37Cl, 36,38,40Ar, 39,40,41K, 40,42,43,44,46,48Ca, 45Sc, 46,47,48,49,50Ti, 50,51V, 50,52,53,54Cr, 55Mn, 54,56,57,58Fe, 58,59Co, 58,59,60,61,62,64Ni, 63,65Cu, 65,66,67,68,70Zn, 69,71Ga, 70,72,73,74,76Ge, 74,75As, 74,76,77,78,79,80,82Se, 79,81Br, 78,80,82,83,84,85,86Kr, 85,86,87Rb, 84,86,87,88,89,90Sr, 89,90,91Y, 90,91,92,93,94,95,96Zr, 93,94,95Nb, 92,94,95,96,97,98,99,100Mo, 99Tc, 96,98,99,100,101,102,103,104,105,106Ru, 103,105Rh, 102,104,105,106,107,108,110Pd, 107,109,110,111Ag, 106,108,110,111,112,113,114,115,116Cd, 113,115In, 112,113,114,115,116,117,118,119,120,122,123,124,125,126Sn, 121,123,124,125,126Sb, 120,122,123,124,125,126,127,128,129,130,132Te, 127,129,130,131,135I, 123,124,126,128,129,130,131,132,133,134,135,136Xe, 133,134,135,136,137Cs, 130,132,133,134,135,136,137,138,140Ba, 138,139,140La, 136,138,139,140,141,142,143,144Ce, 141,142,143Pr, 142,143,144,145,146,147,148,150Nd, 147,148,149,151Pm, 144,147,148,149,150,151,152,153,154Sm, 151,152,153,154,155,156,157Eu, 152,153,154,155,156,157,158,160Gd, 159,160Tb, 156,158,160,161,162,163,164Dy, 165,166Ho, 162,164,166,167,168,170Er, 168,169,170Tm, 175,176Lu, 174,176,177,178,179,180Hf, 180,181,182Ta, 180,182,183,184,186W, 185,187Re, 191,193Ir, 197Au, 196,198,199,200,201,202,204Hg, 203,205Tl, 204,206,207,208Pb, 209Bi, 223,224,225,226Ra, 225,226,227Ac, 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,249,250Bk, 246,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), E=30 keV; calculated Maxwellian-averaged σ using ENDF/B-VII.1 evaluated neutron library. Comparison with ENDF/B-VII.0 and KADONIS values. NUCLEAR REACTIONS 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,249,250Bk, 246,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), (n, F), E=thermal; calculated thermal σ. Comparison with ENDF/B-VII.0, JENDL-4.0 and Atlas of Neutron Resonances values.
doi: 10.1016/j.nds.2011.11.002
2011KI31 Phys.Rev. C 84, 054907 (2011) Prospects for quarkonia production studies in U + U collisions
doi: 10.1103/PhysRevC.84.054907
2011NE06 Nucl.Phys. A855, 400c (2011) R.Nelson, R.Vogt, C.Lourenco, H.Wohri Bottom production from fixed-target to LHC energies
doi: 10.1016/j.nuclphysa.2011.02.090
2011VO05 Nucl.Phys. A855, 453c (2011) J/ψ production and absorption in p + A and d+Au collisions
doi: 10.1016/j.nuclphysa.2011.02.104
2011VO11 Phys.Rev. C 84, 044621 (2011) Event-by-event study of neutron observables in spontaneous and thermal fission RADIOACTIVITY 238U, 240Pu, 244Cm, 252Cf(SF); calculated yields, total fragment kinetic energies, neutron multiplicities, prompt fission neutron spectra, angular correlations between two neutrons. Event-by-event fission model FREYA for fission neutron correlations. Comparison with experimental data. NUCLEAR REACTIONS 235U(n, F), 239Pu(n, F), E=thermal; calculated yields, total fragment kinetic energies, prompt fission neutron spectra, angular correlations between two neutrons. Event-by-event fission model FREYA for fission neutron correlations. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.044621
2011VO12 J.Korean Phys.Soc. 59, 895s (2011) R.Vogt, J.Randrup, J.Pruet, W.Younes Calculation of 239Pu Fission Observables in an Event-by-Event Simulation NUCLEAR REACTIONS 239Pu(n, f), E=0.5-5.5 MeV; calculated prompt σ(En), fragment TKE, average neutron multiplicity, correlation coefficients using FREYA event generator. Comparison to data.
doi: 10.3938/jkps.59.895
2011VO13 J.Korean Phys.Soc. 59, 899s (2011) Generalized Energy-Dependent Q Values for Fission NUCLEAR REACTIONS 232Th, 235,238U, 239Pu, 252Cf(n, f), E=0-20 MeV; calculated energy release vs En.
doi: 10.3938/jkps.59.899
2010VO03 Phys.Rev. C 81, 044903 (2010) Cold nuclear matter effects on J/ψ and γ production at energies available at the CERN Large Hadron Collider (LHC)
doi: 10.1103/PhysRevC.81.044903
2009RA18 Phys.Rev. C 80, 024601 (2009) Calculation of fission observables through event-by-event simulation NUCLEAR REACTIONS 235U, 239Pu(n, X), E=0.53 MeV; calculated kinetic energy and dispersions of neutrons, total energies of fission fragments, multiplicity of neutrons emitted by fission fragments, neutron-neutron angular correlations and neutron-photon correlations using a new computational model, the fission reaction event yield algorithm (FREYA).
doi: 10.1103/PhysRevC.80.024601
2009VO08 Phys.Rev. C 80, 044611 (2009) R.Vogt, J.Randrup, J.Pruet, W.Younes Event-by-event study of prompt neutrons from 239Pu(n, f) NUCLEAR REACTIONS 239Pu(n, f), E=0.5-5.5 MeV; analyzed prompt neutron spectra from 0.1 to 10 MeV, fragment kinetic energies and excitation energies for fragment A=80-160, and average neutron multiplicities as a function of fragment mass number using Monte Carlo model FREYA. Comparisons with experimental data and ENDF-B/VII evaluations.
doi: 10.1103/PhysRevC.80.044611
2009VO13 Nucl.Phys. A827, 454c (2009) Understanding Heavy Flavor Production at RHIC
doi: 10.1016/j.nuclphysa.2009.05.098
2007VO09 J.Phys.(London) G34, S759 (2007) R.Vogt, C.Lourenco, M.J.Leitch Cold nuclear matter effects on J/ψ and ψ' production
doi: 10.1088/0954-3899/34/8/S90
2006DJ01 Phys.Lett. B 632, 81 (2006) M.Djordjevic, M.Gyulassy, R.Vogt, S.Wicks Influence of bottom quark jet quenching on single electron tomography of Au + Au NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; calculated quark jet quenching, nuclear modification factor for single electrons.
doi: 10.1016/j.physletb.2005.09.087
2006DJ06 Nucl.Phys. A774, 689 (2006) M.Djordjevic, M.Gyulassy, R.Vogt, S.Wicks The single electron puzzle at RHIC NUCLEAR REACTIONS Au(Au, X), E(cm)=200 GeV/nucleon; calculated charm and bottom quark spectra, single electron nuclear modification factor.
doi: 10.1016/j.nuclphysa.2006.06.115
2006ST03 Phys.Rev.Lett. 96, 082001 (2006) Probing Small x Parton Densities in Ultraperipheral AA and pA Collisions at the CERN Large Hadron Collider NUCLEAR REACTIONS Pb(p, X), E(cm)=8.8 TeV/nucleon; Pb(Pb, X), E(cm)=5.5 TeV/nucleon; calculated dijet and quark-pair photoproduction rates in ultraperipheral collisions.
doi: 10.1103/PhysRevLett.96.082001
2006VO16 Nucl.Phys. A774, 661 (2006) QCD predictions of heavy quark production at RHIC NUCLEAR REACTIONS 1H(p, X), E(cm)=200 GeV/nucleon; calculated transverse momentum distributions of charm and bottom quarks, charm and bottom hadrons and electrons from hadron decay. Perturbative QCD analysis.
doi: 10.1016/j.nuclphysa.2006.06.109
2005VO08 Nucl.Phys. A752, 447c (2005) Heavy Ion Physics at the LHC NUCLEAR REACTIONS Pb(Pb, X), E(cm)=17, 200, 5500 GeV/nucleon; Pb(p, X), E(cm)=8.8 TeV/nucleon; calculated particle yields, quark-gluon plasma features.
doi: 10.1016/j.nuclphysa.2005.02.050
2005VO10 Phys.Rev. C 71, 054902 (2005) Shadowing and absorption effects on J/ψ production in dA collisions NUCLEAR REACTIONS 1H(p, X), 197Au(d, X), Pb(p, X), (d, X), E=high; calculated J/ψ yields, rapidity distributions, medium modification effects.
doi: 10.1103/PhysRevC.71.054902
2005VO11 J.Phys.(London) G31, S773 (2005) Open and hidden charm production at RHIC and LHC
doi: 10.1088/0954-3899/31/6/018
2005VO16 Eur.Phys.J. C 43, 113 (2005) Open and hidden charm production in dA collisions at RHIC and LHC NUCLEAR REACTIONS 1H(p, X), 197Au(d, X), E=high; calculated open and hidden charm production σ, transverse momentum spectra, shadowing and absorption effects. Comparison with data.
doi: 10.1140/epjc/s2005-02220-3
2004DA31 J.Phys.(London) G30, 1787 (2004) A.Dainese, R.Vogt, M.Bondila, K.J.Eskola, V.J.Kolhinen D-meson enhancement in pp collisions at the LHC due to nonlinear gluon evolution NUCLEAR REACTIONS 1H(p, X), E(cm)=14 TeV; calculated D-meson production σ, transverse momentum, enhancement due to nonlinear effects.
doi: 10.1088/0954-3899/30/12/002
2004ES02 J.Phys.(London) G30, S1171 (2004) K.J.Eskola, V.J.Kolhinen, R.Vogt Enhanced charm hadroproduction due to nonlinear corrections to the DGLAP equations NUCLEAR REACTIONS 1H(p, X), E(cm)=5.5, 8.8, 14 TeV; calculated charm production σ(pT), effects of nonlinear scale evolution.
doi: 10.1088/0954-3899/30/8/083
2004VO20 Phys.Rev. C 70, 064902 (2004) Shadowing effects on the nuclear suppression factor, RdAu, in d + Au interactions NUCLEAR REACTIONS 197Au(d, X), E(cm)=200 GeV/nucleon; analyzed charged hadron spectra, nuclear supression factor vs centrality, transverse momentum. Initial state shadowing approach.
doi: 10.1103/PhysRevC.70.064902
2003KI04 Nucl.Phys. A715, 549c (2003) N.Kidonakis, E.Laenen, S.Moch, R.Vogt Understanding Bottom Production
doi: 10.1016/S0375-9474(02)01515-4
2003KL07 Phys.Rev. C 67, 047901 (2003) Nuclear shadowing and high-pT hadron spectra in relativistic heavy ion collisions NUCLEAR REACTIONS 1H(p, X), 197Au(197Au, X), E(cm)=200 GeV/nucleon; calculated hadron transverse momentum distributions, shadowing effects.
doi: 10.1103/PhysRevC.67.047901
2003KL11 Phys.Rev. C 68, 017902 (2003) Deuteron photodissociation in ultraperipheral relativistic heavy-ion on deuteron collisions NUCLEAR REACTIONS 197Au(d, np), E(cm)=200 GeV/nucleon; Pb(d, np), E(cm)=6.2 TeV; calculated deuteron photodissociation σ.
doi: 10.1103/PhysRevC.68.017902
2003KL14 Phys.Rev.Lett. 91, 142301 (2003) Inhomogeneous Shadowing Effects on J/ψ Production in d A Collisions NUCLEAR REACTIONS 197Au(d, X), E(cm)=200 GeV/nucleon; Pb(d, X), E(cm)=6.2 TeV/nucleon; calculated shadowing effects, spatial effects in J/ψ production.
doi: 10.1103/PhysRevLett.91.142301
2003VO09 Int.J.Mod.Phys. E12, 211 (2003) The A Dependence of Open Charm and Bottom Production NUCLEAR REACTIONS 1H(p, X), 197Au(p, X), (197Au, X), Pb(p, X), (Pb, X), E=high; calculated heavy quark production σ, transverse momentum, rapidity, nuclear effects, related features.
doi: 10.1142/S0218301303001272
2003VO14 Nucl.Phys. A726, 134 (2003) Ξ- and Ω distributions in hadron-nucleus interactions NUCLEAR REACTIONS 1H, C, Cu(n, X), E=260 GeV; 1H, C, Cu(π-, X), E=345 GeV; calculated strange quark production associated σ(x), leading particle effect. Comparisons with data, Ξ-- and Σ--induced reactions also discussed.
doi: 10.1016/j.nuclphysa.2003.07.003
2003VO20 Acta Phys.Hung.N.S. 17, 75 (2003) The Usage of the K Factor in Heavy Ion Physics
doi: 10.1556/APH.17.2003.1.9
2003VO21 Acta Phys.Hung.N.S. 18, 11 (2003) Heavy Quark Production in Heavy Ion Colliders NUCLEAR REACTIONS 1H(π-, X), (p, X), E=high; calculated quark-antiquark pair production σ. Perturbative QCD, comparisons with data.
doi: 10.1556/APH.18.2003.1.2
2002GU19 Nucl.Phys. A705, 396 (2002) Asymmetries between Strange and Antistrange Particle Production in Pion-Proton Interaction NUCLEAR REACTIONS 1H(π-, X), E=500 GeV; calculated strange and antistrange hadron production σ(x), asymmetries. Intrinsic charm model.
doi: 10.1016/S0375-9474(02)00658-9
2002KL15 Phys.Rev. C66, 044906 (2002) Heavy quark photoproduction in ultraperipheral heavy ion collisions NUCLEAR REACTIONS O(O, X), Si(Si, X), Ar(Ar, X), I(I, X), Pb(Pb, X), 197Au(197Au, X), O, Si, Ar, I, Pb, 197Au(p, X), E=high; calculated heavy quark production rates, transverse momentum and rapidity distributions, invariant mass spectra in peripheral collisions.
doi: 10.1103/PhysRevC.66.044906
2002VO04 Nucl.Phys. A700, 539 (2002) Are the J/ψ and χc A Dependencies the Same ?
doi: 10.1016/S0375-9474(01)01313-6
2001ES09 Nucl.Phys. A696, 729 (2001) K.J.Eskola, V.J.Kolhinen, R.Vogt Obtaining the Nuclear Gluon Distribution from Heavy Quark Decays to Lepton Pairs in pA Collisions NUCLEAR REACTIONS 1H, 197Au, 208Pb(p, X), E=high; calculated lepton pair production σ from heavy quark decays; deduced role of nuclear modifications to gluon distributions.
doi: 10.1016/S0375-9474(01)01221-0
2001KL08 Eur.Phys.J. C 21, 563 (2001) Photoproduction of Top Quarks in Peripheral Heavy Ion Collisions NUCLEAR REACTIONS O(O, X), Pb(Pb, X), E=high; calculated top quark production σ, rapidity distributions.
doi: 10.1007/s100520100739
2001VO19 Phys.Rev. C64, 044901 (2001) Shadowing Effects on Vector Boson Production NUCLEAR REACTIONS 1H(p, X), E=14 TeV; Pb(Pb, X), E=5.5 TeV/nucleon; calculated vector boson rapidity distributions; deduced role of nuclear modification to nuclear structure function.
doi: 10.1103/PhysRevC.64.044901
2000EM01 Phys.Rev. C61, 044904 (2000) V.Emelyanov, A.Khodinov, S.R.Klein, R.Vogt Effect of Shadowing on Initial Conditions, Transverse Energy, and Hard Probes in Ultrarelativistic Heavy Ion Collisions NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV; Pb(Pb, X), E(cm)=5.5 TeV; calculated quark, antiquark, gluon rapidity distributions, transverse energy distributions, particle production impact parameter dependences, related features; deduced shadowing effects.
doi: 10.1103/PhysRevC.61.044904
2000VO03 Phys.Rev. C61, 035203 (2000) xF Dependence of ψ and Drell-Yan Production NUCLEAR REACTIONS 9Be, 184W(p, X), E=120, 800 GeV; analyzed ψ, ψ', Drell-Yan production vs longitudinal momentum fraction; dedcuced absorption, shadowing, other nuclear effects.
doi: 10.1103/PhysRevC.61.035203
2000VO20 Prog.Part.Nucl.Phys. 45, S105 (2000) Physics of the Nucleon Sea Quark Distributions
1999BB15 Nucl.Phys. A661, 205c (1999) S.A.Bass, M.Bleicher, W.Cassing, A.Dumitru, H.J.Drescher, K.J.Eskola, M.Gyulassy, D.Kharzeev, Y.V.Kovchegov, Z.Lin, D.Molnar, J.Y.Ollitrault, S.Pratt, B.R.Schlei, H.Sorge, J.Rafelski, R.Rapp, D.H.Rischke, J.B.Schaffner, A.M.Snigirev, D.K.Srivastava, J.Stachel, D.Teaney, R.Thews, S.E.Vance, I.Vitev, R.Vogt, X.N.Wang, B.Zhang, J.Zimanyi Last Call for RHIC Predictions
doi: 10.1016/S0375-9474(99)85024-6
1999EM01 Phys.Rev. C59, R1860 (1999) V.Emelyanov, A.Khodinov, S.R.Klein, R.Vogt Impact Parameter Dependence of J/ψ and Drell-Yan Production in Heavy Ion Collisions at √ sNN = 17.3 GeV NUCLEAR REACTIONS 1H(p, X), Pb(Pb, X), U(S, X), E=high; calculated J/ψ, Drell-Yan production σ impact parameter dependence; deduced role of shadowing.
doi: 10.1103/PhysRevC.59.R1860
1999EM02 Nucl.Phys. A661, 649c (1999) V.Emelyanov, A.Khodinov, S.R.Klein, R.Vogt Shadowing Effects on Particle and Transverse Energy Production
doi: 10.1016/S0375-9474(99)85109-4
1999EM03 Yad.Fiz. 62, No 12, 2259 (1999); Phys.Atomic Nuclei 62, 2081 (1999) V.M.Emelyanov, A.I.Khodinov, S.R.Klein, R.Vogt Transverse-Energy Distribution of Particles at RHIC and Spatial Dependence of Nuclear Structure Functions NUCLEAR REACTIONS 197Au(197Au, X), E(cm) ≈ 100 GeV/nucleon; calculated fragments transverse energy spectra; deduced dependence on nuclear structure functions.
1999GU06 Nucl.Phys. B539, 189 (1999) Leading Charm in Hadron-Nucleus Interactions in the Intrinsic Charm Model NUCLEAR REACTIONS 1H(p, X), (π-, X), (Σ-, X), E=330, 650 GeV; Cu(Σ-, X), (π-, X), E=650 GeV; Cu(p, X), E=800 GeV; calculated charm production σ(x). Modified intrinsic charm model. Comparisons with data.
doi: 10.1016/S0550-3213(98)00748-2
1999KI04 Phys.Rev. D59, 074014 (1999) Soft-Gluon Resummation for Heavy Quark Production in Hadronic Collisions NUCLEAR REACTIONS 1H(p-bar, X), E(cm)=1.8 TeV; calculated heavy quark production σ. Soft-gluon resummation, deep inelastic scattering scheme.
doi: 10.1103/PhysRevD.59.074014
1999LI19 Nucl.Phys. B544, 339 (1999) Energy loss Effects on Heavy Quark Production in Heavy-Ion Collisions at √ s = 5.5 A TeV NUCLEAR REACTIONS Pb(Pb, X), E(cm)=5.5 TeV/nucleon; calculated dileptons rapidity, invariant mass; deduced heavy quark supression due to parton energy loss.
doi: 10.1016/S0550-3213(98)00833-5
1999SP02 Phys.Lett. 458B, 137 (1999) C.Spieles, R.Vogt, L.Gerland, S.A.Bass, M.Bleicher, L.Frankfurt, M.Strikman, H.Stocker, W.Greiner Dissociation of Expanding c(c-bar) States in Heavy Ion Collisions NUCLEAR REACTIONS Pb(Pb, X), E=160; calculated J/ψ, Drell-Yan production yields, transverse energy. Comparison with data.
doi: 10.1016/S0370-2693(99)00579-1
1999SP08 Phys.Rev. C60, 054901 (1999) C.Spieles, R.Vogt, L.Gerland, S.A.Bass, M.Bleicher, H.Stocker, W.Greiner Modeling J/ψ Production and Absorption in a Microscopic Nonequilibrium Approach NUCLEAR REACTIONS Pb(Pb, X), 197Au(S, X), U(p, X), (S, X), E=high; calculated J/ψ production σ, rapidity distributions, survival probability. Ultrarelativistic quantum molecular dynamics model. Comparisons with data.
doi: 10.1103/PhysRevC.60.054901
1999SP10 J.Phys.(London) G25, 2351 (1999) C.Spieles, R.Vogt, L.Gerland, S.A.Bass, M.Bleicher, H.Stocker, W.Greiner Dissociation of J/ψ by Mesons: Thermal versus nonequilibrium scenario NUCLEAR REACTIONS Pb(Pb, X), E=160 GeV; calculated meson-induced J/ψ dissociation rates. Comparison of thermal gas and microscopic transport scenarios.
doi: 10.1088/0954-3899/25/12/305
1999VO05 Phys.Rep. 310, 197 (1999) J/ψ Production and Suppression
doi: 10.1016/S0370-1573(98)00074-X
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