NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = F.Goldenbaum Found 39 matches. 2018SI19 Eur.Phys.J. A 54, 109 (2018) U.Singh, D.Filges, F.Goldenbaum, B.Kamys, Z.Rudy, S.K.Sharma The predictive power of spallation models for isotopic cross sections NUCLEAR REACTIONS 1H(136Xe, x), E=1000 MeV/nucleon; calculated isotopic σ of IMFs with Z=3-56 using INCL++ coupled to ABLA07, GEM2, GEMINI++ and SMM. Compared to available data.
doi: 10.1140/epja/i2018-12546-x
2017FI09 Phys.Rev. C 96, 064618 (2017) M.Fidelus, D.Filges, F.Goldenbaum, L.Jarczyk, B.Kamys, M.Kistryn, St.Kistryn, E.Kozik, P.Kulessa, H.Machner, A.Magiera, B.Piskor-Ignatowicz, K.Pysz, Z.Rudy, SushilK.Sharma, R.Siudak, M.Wojciechowski, for the PISA Collaboration Non-equilibrium processes in p + Ag collisions at GeV energies NUCLEAR REACTIONS Ag(p, X)1H/2H/3H/3He/4He/6He/6Li/7Li/8Li/9Li/7Be/9Be/10Be/10B/11B/12B, E=1.2, 1.9, 2.5 GeV; measured reaction products, double differential cross sections d2σ/dΩdE at seven angles using the beam from cooler synchrotron (COSY) of the Research Center in Julich; deduced reaction mechanism features from comparison with theoretical predictions using INCL4.6 code coupled to ABLA07, and GEMINI++, and GEM2, and SMM codes.
doi: 10.1103/PhysRevC.96.064618
2017SH21 Eur.Phys.J. A 53, 150 (2017) S.K.Sharma, B.Kamys, F.Goldenbaum, D.Filges Ranking and validation of spallation models for isotopic production cross sections of heavy residua NUCLEAR REACTIONS 1H(136Xe, x), E=500 MeV/nucleon; calculated isotopic σ (mass distributions), A-factor, both standardized and non-standardized H-factor and M-factors for elements of Z=41-56 using ABLA, GEM2, GEMINI and SMM codes. Compared to data.
doi: 10.1140/epja/i2017-12334-2
2016SH20 Eur.Phys.J. A 52, 171 (2016) S.K.Sharma, B.Kamys, F.Goldenbaum, D.Filges Ranking and validation of the spallation models for description of intermediate mass fragment emission from p + Ag collisions at 480 MeV incident proton beam energy NUCLEAR REACTIONS Ag(p, x), E=480 MeV; calculated intermediate mass fragments (6Li to 27Mg) σ(θ, E) using cascade code INCL4.6 combined with one of ABLA07, GEM2, GEMINI++, SMM; compared to published data; deduced reaction mechanisms, H- and M-factors for all intermediate mass fragments, ranking of model predictions.
doi: 10.1140/epja/i2016-16171-5
2014FI10 Phys.Rev. C 89, 054617 (2014) M.Fidelus, D.Filges, F.Goldenbaum, H.Hodde, A.Jany, L.Jarczyk, B.Kamys, M.Kistryn, St.Kistryn, St.Kliczewski, E.Kozik, P.Kulessa, H.Machner, A.Magiera, B.Piskor-Ignatowicz, K.Pysz, Z.Rudy, S.K.Sharma, R.Siudak, M.Wojciechowski, for the PISA Collaboration Sequential and simultaneous emission of particles from p + Al collisions at GeV energies NUCLEAR REACTIONS Al(p, X), E=1.2, 1.9, 2.5 GeV; measured particle spectra, σ(E, θ) of p, d, t, 3,4,6He, 6,7,8,9Li, 7,9,10Be, 10,11B by ΔE-E method using detector telescopes at COSY synchrotron of Julich Research Center under PISA collaboration. Comparison with intranuclear cascade model coupled to evaporation, and to statistical multifragmentation models.
doi: 10.1103/PhysRevC.89.054617
2014SH21 Nucl.Data Sheets 119, 307 (2014) S.K.Sharma, D.Filges, F.Goldenbaum, B.Kamys Dependence and Influence of Projectile Energy and Target Mass on the Production of Light Charged Particles and Intermediate Mass Fragments in Proton Induced Reactions NUCLEAR REACTIONS 19C, 27Al, Ni, 108Ag, 197Au(p, x), E=1.2, 1.9, 2.5 GeV; measured charged particles up to A=8; deduced σ(θ, E); calculated σ(θ, E) using INCL4.6 cascade model for fast stage and SMM, ABLA07 and GEMINI++ for emission from residual.
doi: 10.1016/j.nds.2014.08.084
2014SH36 Acta Phys.Pol. B45, 1963 (2014) S.K.Sharma, B.Kamys, F.Goldenbaum, D.Filges Validation of Spallation Models for p+Al Reactions at 180 MeV Incident Proton Beam Energy NUCLEAR REACTIONS 27Al(p, X), E=180 MeV; measured reaction fragments; deduced σ and σ(θ) for fragment production. Comparison with theoretical calculations.
doi: 10.5506/APhysPolB.45.1963
2010BU08 Phys.Rev. C 82, 034605 (2010) A.Budzanowski, M.Fidelus, D.Filges, F.Goldenbaum, H.Hodde, L.Jarczyk, B.Kamys, M.Kistryn, St.Kistryn, St.Kliczewski, A.Kowalczyk, E.Kozik, P.Kulessa, H.Machner, A.Magiera, B.Piskor-Ignatowicz, K.Pysz, Z.Rudy, R.Siudak, M.Wojciechowski, for the PISA Collaboration Comparison of nonequilibrium processes in p+Ni and p+Au collisions at GeV energies NUCLEAR REACTIONS Ni(p, X)p/d/t/3He/4He/6Li/7Li/8Li/7Be/9Be, 10Be/10B, 11B, E=1.2, 1.9, 2.5 GeV; measured particle spectra, double differential σ(E, θ). Comparison with data from 182Au+p system.
doi: 10.1103/PhysRevC.82.034605
2009BU11 Phys.Rev. C 80, 037603 (2009) A.Buttkewitz, H.H.Duhm, F.Goldenbaum, H.Machner, W.Strauss Fission studies with 140 MeV α particles NUCLEAR REACTIONS Ag, 139La, 165Ho, 197Au(α, F), E=140 MeV; measured fission fragments and σ; deduced total kinetic energies, fragment masses, excitation function and binary fission probabilities. Comparison with previous studies.
doi: 10.1103/PhysRevC.80.037603
2009BU15 Phys.Rev. C 80, 054604 (2009) A.Budzanowski, M.Fidelus, D.Filges, F.Goldenbaum, H.Hodde, L.Jarczyk, B.Kamys, M.Kistryn, St.Kistryn, St.Kliczewski, A.Kowalczyk, E.Kozik, P.Kulessa, H.Machner, A.Magiera, B.Piskor-Ignatowicz, K.Pysz, Z.Rudy, R.Siudak, M.Wojciechowski, for the PISA Collaboration Variation of nonequilibrium processes in the p+Ni system with beam energy NUCLEAR REACTIONS Ni(p, p), (p, d), (p, t), (p, 3He), (p, α), (p, 6Li), (p, 7Li), (p, 7Be), (p, 9Be), (p, 10B), (p, 11B), E=175 MeV; measured σ and double differential σ(θ). Comparison with calculations using two-step microscopic model.
doi: 10.1103/PhysRevC.80.054604
2008BU18 Phys.Rev. C 78, 024603 (2008) A.Budzanowski, M.Fidelus, D.Filges, F.Goldenbaum, H.Hodde, L.Jarczyk, B.Kamys, M.Kistryn, St.Kistryn, St.Kliczewski, A.Kowalczyk, E.Kozik, P.Kulessa, H.Machner, A.Magiera, B.Piskor-Ignatowicz, K.Pysz, Z.Rudy, R.Siudak, M.Wojciechowski, and the PISA Collaboration Competition of coalescence and "fireball" processes in nonequilibrium emission of light charged particles from p + Au collisions NUCLEAR REACTIONS Au(p, pX), (p, dX), (p, tX), (p, αX), (p, 3HeX), (p, X)6He/6Li/7Li/8Li/9Li/7Be/9Be/10Be/10B/11B/12B; E=1.2-1.9 GeV; analyzed σ(θ, E).
doi: 10.1103/PhysRevC.78.024603
2008NU01 Eur.Phys.J. A 38, 115 (2008) K.Nunighoff, Ch.Pohl, S.Koulikov, F.Cantargi, H.Conrad, D.Filges, H.Gluckler, F.Goldenbaum, R.Granada, G.Hansen, T.Matzerath, N.Paul, S.Petriw, H.Schaal, H.Soltner, H.Stelzer, W.Ninaus, M.Wohlmuther Neutron experiments with cryogenic methane hydrate and mesitylene moderators NUCLEAR REACTIONS Hg(p, nX), E=1.3 GeV; measured spallation neutron spectra, effects of methane hydrate and mesitylene moderators. Comparison with Monte Carlo simulation.
doi: 10.1140/epja/i2008-10661-y
2007BU17 Phys.Rev. C 76, 014618 (2007) A.Bubak, A.Budzanowski, D.Filges, F.Goldenbaum, A.Heczko, H.Hodde, L.Jarczyk, B.Kamys, M.Kistryn, St.Kistryn, St.Kliczewski, A.Kowalczyk, E.Kozik, P.Kulessa, H.Machner, A.Magiera, W.Migdal, N.Paul, B.Piskor-Ignatowicz, M.Puchala, K.Pysz, Z.Rudy, R.Siudak, M.Wojciechowski, P.Wustner, for the PISA Collaboration Non-equilibrium emission of complex fragments from p + Au collisions at 2.5 GeV proton beam energy
doi: 10.1103/PhysRevC.76.014618
2006BO14 Nucl.Instrum.Methods Phys.Res. A562, 733 (2006) V.Bollini, A.Bubak, A.Budzanowski, J.Cugnon, D.Filges, F.Goldenbaum, A.Heczko, H.Hodde, L.Jarczyk, B.Kamys, M.Kistryn, St.Kistryn, St.Kliczewski, A.Kowalczyk, P.Kulessa, H.Machner, A.Magiera, W.Migdal, K.Nunighoff, N.Paul, B.Piskor-Ignatowicz, K.Pysz, Z.Rudy, R.Siudak, M.Wojciechowski, E.Kozik Light charged particle and intermediate mass fragment cross-sections in GeV proton-induced reactions NUCLEAR REACTIONS Ni(p, X), E=1.9 GeV; measured fragment yields, spectra.
doi: 10.1016/j.nima.2006.02.034
2006HE02 Nucl.Phys. A765, 426 (2006) C.-M.Herbach, D.Hilscher, U.Jahnke, V.G.Tishchenko, J.Galin, A.Letourneau, A.Peghaire, D.Filges, F.Goldenbaum, L.Pienkowski, W.U.Schroder, J.Toke Charged-particle evaporation and pre-equilibrium emission in 1.2 GeV proton-induced spallation reactions NUCLEAR REACTIONS Al, Ti, Fe, Ni, Cu, Zr, Ag, Ho, Ta, W, Au, Pb, Th(p, X), E=1.2 GeV; measured light charged particle production σ, σ(E, θ), multiplicities, neutron multiplicities; deduced role of pre-equilibrium emission. Intra-nuclear cascade and statistical evaporation model analysis, NESSI detector.
doi: 10.1016/j.nuclphysa.2005.10.014
2006HE16 Nucl.Instrum.Methods Phys.Res. A562, 729 (2006) C.-M.Herbach, D.Hilscher, U.Jahnke, V.G.Tishchenko, J.Galin, A.Letourneau, A.Peghaire, D.Filges, F.Goldenbaum, L.Pienkowski, W.U.Schroder, J.Toke Systematic investigation of 1.2-GeV proton-induced spallation reactions on targets between Al and U NUCLEAR REACTIONS Al, Ti, Fe, Ni, Cu, Zr, Ag, Ho, Ta, W, Au, Pb, Th(p, X), E=1.2 GeV; measured neutron and light charged particle multiplicities, inelastic σ.
doi: 10.1016/j.nima.2006.02.033
2006MA26 Phys.Rev. C 73, 044606 (2006) H.Machner, D.G.Aschman, K.Baruth-Ram, J.Carter, A.A.Cowley, F.Goldenbaum, B.M.Nangu, J.V.Pilcher, E.Sideras-Haddad, J.P.F.Sellschop, F.D.Smit, B.Spoelstra, D.Steyn Isotopic production cross sections in proton-nucleus collisions at 200 MeV NUCLEAR REACTIONS 27Al, 59Co, 197Au(p, X), E=200 MeV; measured intermediate mass fragments isotopic production σ, σ(E, θ).
doi: 10.1103/PhysRevC.73.044606
2005TI12 Phys.Rev.Lett. 95, 162701 (2005) V.Tishchenko, C.-M.Herbach, D.Hilscher, U.Jahnke, J.Galin, F.Goldenbaum, A.Letourneau, W.-U.Schroder Fast Decision in Favor of the Slow Fission Process NUCLEAR REACTIONS Au, Bi, U(p, X), E=2.5 GeV; measured light particle multiplicities, fission fragments, σ; deduced fission probability vs excitation energy for excited target-like nuclei. Comparison with statistical-model calculations.
doi: 10.1103/PhysRevLett.95.162701
2004NU04 Eur.Phys.J. A 22, 519 (2004) K.Nunighoff, Ch.Pohl, V.Bollini, A.Bubak, H.Conrad, D.Filges, H.Gluckler, F.Goldenbaum, G.Hansen, B.Lensing, R.-D.Neef, N.Paul, D.Prasuhn, K.Pysz, H.Schaal, H.Soltner, H.Stelzer, H.Tietze-Jaensch, W.Bernnat, J.Keinert, M.Mattes, W.Ninaus, S.Koulikov, A.Smirnov, M.Wohlmuther Ice moderator experiments at very low temperatures: Comparison of experimental data with Monte Carlo simulations using new scattering law data S(α, βT) NUCLEAR REACTIONS Hg(p, nX), E=1.3 GeV; measured spallation neutron spectra, effects of ice moderator. Comparison with Monte Carlo simulation.
doi: 10.1140/epja/i2004-10060-6
2003JA07 Nucl.Instrum.Methods Phys.Res. A508, 295 (2003) U.Jahnke, C.-M.Herbach, D.Hilscher, V.Tishchenko, J.Galin, A.Letourneau, B.Lott, A.Peghaire, F.Goldenbaum, L.Pienkowski A combination of two 4π detectors for neutrons and charged particles. Part I. The Berlin neutron ball - a neutron multiplicity meter and reaction detector NUCLEAR REACTIONS Pb(p, X), E=0.8-2.5 GeV; 238U(20Ne, X), E=290 MeV; Cu, Ho, Au, U(p-bar, X), E=1.2 GeV; measured neutron multiplicity distributions.
doi: 10.1016/S0168-9002(03)01652-8
2002LE32 Nucl.Phys. A712, 133 (2002) A.Letourneau, A.Bohm, J.Galin, B.Lott, A.Peghaire, M.Enke, C.-M.Herbach, D.Hilscher, U.Jahnke, V.Tishchenko, D.Filges, F.Goldenbaum, R.D.Neef, K.Nunighoff, N.Paul, G.Sterzenbach, L.Pienkowski, J.Toke, U.Schroder Composite-particle emission in the reaction p + Au at 2.5 GeV NUCLEAR REACTIONS 197Au(p, X), E=2.5 GeV; measured light charged particle spectra, neutron and light charged particle multiplicities, yields; deduced excitation energy distribution. 197Au(p, pX), (p, dX), (p, tX), (p, 3HeX), (p, αX), (p, 6LiX), (p, 7LiX), E=2.5 GeV; measured σ(E, θ), σ. Spallation reaction, comparison with coalescence model predictions.
doi: 10.1016/S0375-9474(02)01133-8
2001FI16 Eur.Phys.J. A 11, 467 (2001) D.Filges, F.Goldenbaum, M.Enke, J.Galin, C.-M.Herbach, D.Hilscher, U.Jahnke, A.Letourneau, B.Lott, R.-D.Neef, K.Nunighoff, N.Paul, A.Peghaire, L.Pienkowski, H.Schaal, U.Schroder, G.Sterzenbach, A.Tietze, V.Tishchenko, J.Toke, M.Wohlmuther Spallation Neutron Production and the Current Intra-Nucler Cascade and Transport Codes NUCLEAR REACTIONS W, Hg, Pb(p, X), E=1.2-2.5 GeV; measured neutron and reaction probability for thick targets. Au(p, X), E=0.4-2.5 GeV; calculated pions, neutrons and protons multiplicities and kinetic energies. Systematic comparison of different computer codes. Application to radioactive nuclei production discussed.
doi: 10.1007/s100500170058
2001LO04 Phys.Rev. C63, 034616 (2001) B.Lott, F.Goldenbaum, A.Bohm, W.Bohne, T.von Egidy, P.Figuera, J.Galin, D.Hilscher, U.Jahnke, J.Jastrzebski, M.Morjean, G.Pausch, A.Peghaire, L.Pienkowski, D.Polster, S.Proschitzki, B.Quednau, H.Rossner, S.Schmid, W.Schmid Thermal Excitation and Decay of Nuclei from Antiproton-Nucleus Interactions at 1.22 GeV NUCLEAR REACTIONS 12C, Cu, Y, 92,100Mo, 107Ag, Sn, 165Ho, 197Au, Bi, 238U(p-bar, X), E=1.22 GeV; measured light charged particle, intermediate mass fragment, neutron multiplicities, spectra, excitation energy distributions. 197Au, 238U(p-bar, X), E=1.22 GeV; measured fission probability, fragment kinetic energy distributions. Comparisons with model predictions.
doi: 10.1103/PhysRevC.63.034616
2000LE31 Nucl.Instrum.Methods Phys.Res. B170, 299 (2000) A.Letourneau, J.Galin, F.Goldenbaum, B.Lott, A.Peghaire, M.Enke, D.Hilscher, U.Jahnke, K.Nunighoff, D.Filges, R.D.Neef, N.Paul, H.Schaal, G.Sterzenbach, A.Tietze Neutron Production in Bombardments of Thin and Thick W, Hg, Pb Targets by 0.4, 0.8, 1.2, 1.8 and 2.5 GeV Protons NUCLEAR REACTIONS W, Hg, Pb(p, nX), E=0.4, 0.8, 1.2, 1.8, 2.5 GeV; measured neutron multiplicity distributions, yield vs target thickness. Comparison with model prediction. Application to neutron source discussed.
doi: 10.1016/S0168-583X(00)00259-7
2000PI02 Phys.Lett. 472B, 15 (2000) L.Pienkowski, W.Bohne, T.von Egidy, P.Figuera, J.Galin, F.Goldenbaum, D.Hilscher, U.Jahnke, J.Jastrzebski, B.Lott, M.Morjean, G.Pausch, A.Peghaire, D.Polster, S.Proschitzki, B.Quednau, H.Rossner, S.Schmid, W.Schmid Vaporization and Multifragmentation in the Reaction 1.2 GeV (p-bar) + Cu and Ag NUCLEAR REACTIONS Cu, Ag(p-bar, X), E=1.2 GeV; measured particle energy, (particle)(particle)-coin, excitation energy and mass distributions, particle multiplicities, ratio of vaporization to reaction σ. Intranuclear cascade and statistical model calculations.
doi: 10.1016/S0370-2693(99)01410-0
2000VO14 Eur.Phys.J. A 8, 197 (2000) T.von Egidy, P.Figuera, J.Galin, F.Goldenbaum, Ye.S.Golubeva, M.Hasinoff, D.Hilscher, A.S.Iljinov, U.Jahnke, M.Krause, W.Kurcewicz, X.Ledoux, B.Lott, L.Maier, M.Manrique de Lara, G.Pausch, L.Pienkowski, B.Quednau, W.Schott, W.U.Schroder, J.Toke Neutrons Produced by 1.22 GeV Antiproton Interactions with Nuclei NUCLEAR REACTIONS Al, Cu, Ag, Ho, Ta, Au, Pb, Bi, U(p-bar, X), E=1.22 GeV; measured neutron production σ(En, θ); deduced fast and evaporated neutron multiplicities, source temperatures, mass dependence effect.
doi: 10.1007/s100500070106
1999EN04 Nucl.Phys. A657, 317 (1999) M.Enke, C.-M.Herbach, D.Hilscher, U.Jahnke, O.Schapiro, A.Letourneau, J.Galin, F.Goldenbaum, B.Lott, A.Peghaire, D.Filges, R.-D.Neef, K.Nunighoff, N.Paul, H.Schaal, G.Sterzenbach, A.Tietze, L.Pienkowski Evolution of a Spallation Reaction: Experiment and Monte Carlo Simulation NUCLEAR REACTIONS Fe, Ta, W, 197Au, Hg, Pb, U(p, X), E=1.2, 1.8 GeV; measured reaction σ, neutrons, H, He production σ, σ(E), σ(θ); deduced pre-equilibrium emission, other reaction mechanism features. Comparison with Monte Carlo simulation.
doi: 10.1016/S0375-9474(99)00345-0
1999GO09 Phys.Rev.Lett. 82, 5012 (1999); Erratum Phys.Rev.Lett. 83, 2094 (1999) F.Goldenbaum, M.Morjean, J.Galin, E.Lienard, B.Lott, A.Peghaire, Y.Perier, M.Chevallier, D.Dauvergne, R.Kirsch, J.C.Poizat, J.Remillieux, C.Cohen, A.L'Hoir, G.Prevot, D.Schmaus, J.Dural, M.Toulemonde, D.Jacquet Fission Time Evolution with Excitation Energy from a Crystal Blocking Experiment NUCLEAR REACTIONS Si(238U, X), E=24 MeV/nucleon; measured projectile-like fragments fission T1/2 vs excitation energy. Crystal target, blocking technique.
doi: 10.1103/PhysRevLett.82.5012
1999JA14 Phys.Rev.Lett. 83, 4959 (1999) U.Jahnke, W.Bohne, T.von Egidy, P.Figuera, J.Galin, F.Goldenbaum, D.Hilscher, J.Jastrzebski, B.Lott, M.Morjean, G.Pausch, A.Peghaire, L.Pienkowski, D.Polster, S.Proschitzki, B.Quednau, H.Rossner, S.Schmid, W.Schmid Prevalence of Fission and Evaporation in the Decay of Heavy Nuclei Excited Up to 1000 MeV with Energetic Antiprotons NUCLEAR REACTIONS 165Ho, 197Au, 238U(p-bar, X), E=1.22 GeV; measured fission fragments, heavy residues kinetic energy vs excitation energy, intermediate mass fragments multiplicity; deduced fission, heavy residue production probabilities. Comparison with statistical model.
doi: 10.1103/PhysRevLett.83.4959
1999LO22 Nucl.Phys. (Supplement) A654, 803c (1999) B.Lott, W.Bohne, J.Eades, T.von Egidy, P.Figuera, H.Fuchs, J.Galin, K.Gulda, F.Goldenbaum, D.Hilscher, U.Jahnke, J.Jastrzebski, W.Kurcewicz, M.Morjean, G.Pausch, A.Peghaire, L.Pienkowski, D.Polster, S.Proschitzki, B.Quednau, H.Rossner, S.Schmid, W.Schmid, P.Ziem Formation and Decay of Nuclei Heated with High-Energy Antiprotons NUCLEAR REACTIONS 197Au, 238U(p-bar, X), E=1.22 GeV; measured fission probability and intermediate mass fragment vs excitation energy. Absence of multifragmentation discussed.
doi: 10.1016/S0375-9474(00)88550-4
1999PI10 Nucl.Phys. A655, 269c (1999) L.Pienkowski, W.Bohne, J.Eades, T.von Egidy, P.Figuera, H.Fuchs, J.Galin, F.Goldenbaum, Ye.S.Golubeva, K.Gulda, D.Hilscher, A.S.Iljinov, U.Jahnke, J.Jastrzebski, W.Kurcewicz, B.Lott, M.Morjean, G.Pausch, A.Peghaire, D.Polster, S.Proschitzki, B.Quednau, H.Rossner, S.Schmid, W.Schmid, P.Ziem Decay of Hot Nuclei Formed with Energetic Antiprotons (PS208) NUCLEAR REACTIONS Ho, 197Au, U(p-bar, X), E=1.22 GeV; measured neutron multiplicity, fragment mass distributions, fission probability.
doi: 10.1016/S0375-9474(99)00212-2
1998HI21 Nucl.Instrum.Methods Phys.Res. A414, 100 (1998) D.Hilscher, U.Jahnke, F.Goldenbaum, L.Pienkowski, J.Galin, B.Lott Neutron Production by Hadron-Induced Spallation Reactions in Thin and Thick Pb and U Targets from 1 to 5 GeV NUCLEAR REACTIONS Pb(p, X), (π+, X), U(p, X), E=1.22-4.15 GeV; measured neutron multiplicity distributions vs incident energy, target thickness. Pb, U(p, X), (π+, X), Pb(p-bar, X), (d, X), (π-, X), (K+, X), E ≈ 1-5 GeV; measured mean neutron multiplicity; deduced neutron production mechanism features. Implications for spallation neutron source discussed.
doi: 10.1016/S0168-9002(98)00531-2
1998LO20 Nucl.Instrum.Methods Phys.Res. A414, 117 (1998) B.Lott, F.Cnigniet, J.Galin, F.Goldenbaum, D.Hilscher, A.Lienard, A.Peghaire, Y.Perier, X.Qian Neutron Multiplicity Distributions for 200 MeV Proton-, Deuteron- and 4He-Induced Spallation Reactions in Thick Pb Targets NUCLEAR REACTIONS Pb(p, X), E=197 MeV; Pb(d, X), E=188 MeV; Pb(α, X), E=214 MeV; measured neutron multiplicity distributions; deduced mean multiplicity per incident particle, secondary production contribution. Thick targets. Implications for spallation neutron source discussed.
doi: 10.1016/S0168-9002(98)00532-4
1998MO05 Nucl.Phys. A630, 200c (1998) M.Morjean, M.Chevallier, C.Cohen, D.Dauvergne, J.Dural, J.Galin, F.Goldenbaum, D.Jacquet, R.Kirsch, E.Lienard, B.Lott, A.Peghaire, Y.Perier, J.C.Poizat, G.Prevot, J.Remillieux, D.Schmaus, M.Toulemonde Fission Lifetime Measured by the Blocking Technique as a Function of Excitation Energy in the 24 A.MeV 238U + 28Si Reaction NUCLEAR REACTIONS 28Si(238U, X), E=24 MeV/nucleon; measured projectile-like fragments fission T1/2 vs excitation energy. Blocking technique.
doi: 10.1016/S0375-9474(97)00757-4
1997PI09 Phys.Rev. C56, 1909 (1997) L.Pienkowski, F.Goldenbaum, D.Hilscher, U.Jahnke, J.Galin, B.Lott Neutron Multiplicity Distributions for 1.94 to 5 GeV/c Proton-, Antiproton-, Pion-, Kaon-, and Deuteron-Induced Spallation Reactions on Thin and Thick Targets NUCLEAR REACTIONS Pb, U(p, X), E=1.22-4.15 GeV; Ag, 165Ho, 197Au(p, X), E=1.22 GeV; measured neutron multiplicity distributions; Pb(p, X), (p-bar, X), (π+, X), (π-, X), (d, X), (K+, X), E=1-6 GeV; measured mean neutron multiplicity. Comparison to intra-, internuclear cascade model calculations.
doi: 10.1103/PhysRevC.56.1909
1997SC27 Z.Phys. A359, 27 (1997) S.Schmid, W.Schmid, F.J.Hartmann, T.von Egidy, D.Hilscher, W.Bohne, P.Figuera, F.Goldenbaum, U.Jahnke, D.Polster, P.Ziem, J.Galin, B.Lott, M.Morjean, A.Peghaire, B.Quednau, K.Gulda, J.Jastrzebski, W.Kurcewicz, L.Pienkowski, G.Pausch, J.Eades, A.S.Iljinov, M.V.Mebel Probability of Fission Induced by 1.2 GeV Antiprotons NUCLEAR REACTIONS 238U, 232Th, 209Bi, 197Au, 165Ho, 119Sn, Ag, 100Mo, 89Y, Cu(p-bar, F), E=1.2 GeV; measured annihilation σ, absolute fission probability vs fragment mass, neutron multiplicity, fission fragment folding angle distributions. Monte Carlo calculations. 4π neutron, particle detectors.
doi: 10.1007/s002180050363
1996GO25 Phys.Rev.Lett. 77, 1230 (1996) F.Goldenbaum, W.Bohne, J.Eades, T.von Egidy, P.Figuera, H.Fuchs, J.Galin, Ye.S.Golubeva, K.Gulda, D.Hilscher, A.S.Iljinov, U.Jahnke, J.Jastrzebski, W.Kurcewicz, B.Lott, M.Morjean, G.Pausch, A.Peghaire, L.Pienkowski, D.Polster, S.Proschitzki, B.Quednau, H.Rossner, S.Schmid, W.Schmid, P.Ziem Heating of Nuclei with Energetic Antiprotons NUCLEAR REACTIONS Cu, Ho, 197Au, U(p-bar, X), E=1.2 GeV; measured neutron multiplicity vs charged particle multiplicity, excitation energy distribution; deduced nuclei decay mechanism.
doi: 10.1103/PhysRevLett.77.1230
1995FI04 Z.Phys. A352, 315 (1995) P.Figuera, W.Bohne, B.Drescher, F.Goldenbaum, D.Hilscher, U.Jahnke, B.Lott, L.Pienkowski, P.Ziem Maximum Excitation Energy in Fusion-Evaporation Reactions from Light Particle Multiplicity Measurements in 32S + 58Ni at 25 MeV/A NUCLEAR REACTIONS 58Ni(32S, X), E=25 MeV/nucleon; measured (light particle)(evaporation residue)-coin; deduced system maximum excitation energy.
doi: 10.1007/BF01289504
1995VO14 Z.Naturforsch. 50a, 1077 (1995) T.von Egidy, F.J.Hartmann, S.Schmid, W.Schmid, K.Gulda, J.Jastrzebski, W.Kurcewicz, P.Lubinski, L.Pienkowski, A.Trzcinska, D.Hilscher, W.Bohne, F.Goldenbaum, U.Jahnke, D.Polster, H.Rossner, A.S.Iljinov, D.I.Ivanov, M.V.Mebel, V.G.Nedorezov, A.S.Sudov, J.Eades, S.Neumaier Nuclear Physics with Antiprotons NUCLEAR REACTIONS 197Au(p-bar, X), E at rest; 197Au(p-bar, X), E=1.2 GeV; 197Au(p, X), E=1, 6 GeV; compiled, reviewed residuals yields vs mass number. 234U(p-bar, F), E at rest; 234U(p-bar, F), E=fast; measured neutron spectra following fission; deduced absolute fission probabilities.
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