NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = J.Cugnon Found 86 matches. 2023RO03 Phys.Rev.Lett. 130, 132501 (2023) J.L.Rodriguez-Sanchez, J.Cugnon, J.-C.David, J.Hirtz, A.Kelic-Heil, I.Vidana Constraint of the Nuclear Dissipation Coefficient in Fission of Hypernuclei NUCLEAR REACTIONS 209Bi, 238U(p, F), E=1-2.4 GeV/nucleon; calculated hypernuclear fission σ. Comparison with experimental data.
doi: 10.1103/PhysRevLett.130.132501
2022RO02 Phys.Rev. C 105, 014623 (2022) J.L.Rodriguez-Sanchez, J.Cugnon, J.-C.David, J.Hirtz, A.Kelic-Heil, S.Leray Hypernuclei formation in spallation reactions by coupling the Liege intranuclear cascade model to the deexcitation code ABLA NUCLEAR REACTIONS 209Bi(p, X), E=10 GeV; 12C(Mg, X), E=1 GeV/nucleon; calculated separation energy of the Λ hyperon and S(2n) for 208Pb hypernuclei as a function of the hypernucleus mass number. 1H(136Xe, X), (208Pb, X), (238U, X), E=1000 MeV/nucleon; calculated production σ for Z=10-90 nuclei using INCL+ABLA07, INCL+ABLA, and INCL+SMM model calculations, probability of nuclear fission and evaporation residues surviving to the emission of light particles using ABLA and SMM models for 209Bi and 238U compound nuclei and hypernuclei, hypernuclear production cross sections as a function of the target mass number. 1H(238U, X), E=1.5, 3, 6 GeV/nucleon; calculated Λ-hypernuclei probability as a function of the hypernuclei mass number, isotopic production cross sections of Λ hypernuclei. Liege intranuclear cascade model coupled with a new version of the ablation (ABLA) model for the evaporation of Λ particles from hot hyperremnants during the intranuclear cascade stage. Comparison with available experimental data.
doi: 10.1103/PhysRevC.105.014623
2020HI03 Phys.Rev. C 101, 014608 (2020) J.Hirtz, J.-C.David, A.Boudard, J.Cugnon, S.Leray, I.Leya, J.L.Rodriguez-Sanchez, G.Schnabel Strangeness production in the new version of the Liege intranuclear cascade model NUCLEAR REACTIONS Ca(p, X), E=1.7 GeV; calculated transverse momentum versus rapidity distribution. 12C(p, X), E=1.6, 1.7 GeV; calculated mean momentum of K+ particles. 208Pb(p, X), E=10 GeV; calculated mass distribution of hyper-remnants. C(p, X), E=1.6, 2.3 GeV; Nb, Au(p, X), E=3.5 GeV; Be, Al, Cu, Ta(p, X), E=1.280 GeV; 208Pb(p, X), E=2.1 GeV; 208Pb(d, X), E=2.1 GeV/nucleon; Be, Al, Cu, Au(p, X), E=13.7 GeV; C, Al, Cu, Sn, Pb(π-, X), E=1020 MeV; Be, C, Cu, Sn, Pb(p, X), E=800-1000 MeV; calculated differential σ(E), total σ(E) and angular distributions for production of K+, K0 and K- using Liege intranuclear cascade model (INCL ++6), and compared with experimental data from various collaborations: KaoS-GSI, ITEP-Russia, ANKE-Julich, LBL-Berkeley, HADES-GSI, FOPI-GSI, E-802-BNL, LINP-Russia. Implementation of INCL in the Geant4 transport code. Relevance to design of new experiments for the study of strange particles and hypernuclei at HypHI, Panda, and CBM experiments at the FAIR facility.
doi: 10.1103/PhysRevC.101.014608
2018RO18 Phys.Rev. C 98, 021602 (2018) J.L.Rodriguez-Sanchez, J.-C.David, J.Hirtz, J.Cugnon, S.Leray Constraining the Λ-nucleus potential within the Liege intranuclear cascade model NUCLEAR REACTIONS 28Si, 89Y, 139La, 208Pb(π+, K+), E at 1.06 GeV/c; calculated scatter plot for kinetic energy of K+ particles emitted in the production of 28Si hypernucleus as a function of angle, correlations between the hyper-nucleus potential and the cross section of hypernuclei produced in the reactions. Liege intranuclear-cascade model (INCL) for the production of strange particles and hypernuclei. Comparison with previous theoretical calculations.
doi: 10.1103/PhysRevC.98.021602
2017MA27 Eur.Phys.J. A 53, 80 (2017) D.Mancusi, S.Lo Meo, N.Colonna, A.Boudard, M.A.Cortes-Giraldo, J.Cugnon, J.-C.David, S.Leray, J.Lerendegui-Marco, V.Vlachoudis On the role of secondary pions in spallation targets NUCLEAR REACTIONS 208Pb(p, n), (p, p'), (p, π+), (p, π-), (p, π0), E=0-20 GeV; calculated σ, σ(θ), σ(Eout), n, p, π multiplicity. 208Pb(p, n), (p, p'), (p, π+), (p, π-), (p, π0), E at 3-12 GeV/c; calculated σ, σ(θ). INCL++ and INCL4.6 coupled to ABLA07 or GEANT4. Compared with available data. Calculated and compared with data also reactions between 3 and 12 GeV/c for several targets which could not be identified.
doi: 10.1140/epja/i2017-12263-0
2017RO24 Phys.Rev. C 96, 054602 (2017) J.L.Rodriguez-Sanchez, J.-C.David, D.Mancusi, A.Boudard, J.Cugnon, S.Leray Improvement of one-nucleon removal and total reaction cross sections in the Liege intranuclear-cascade model using Hartree-Fock-Bogoliubov calculations NUCLEAR REACTIONS 1H(40Ca, 39Ca), (40Ca, 39K), (208Pb, 207Pb)(208Pb, 207Tl), (12C, 11C), (12C, 11B), (25Mg, 24Na), (56Fe, 55Fe), (56Fe, 55Mn), (74Ge, 73Ga), (136Xe, 135Xe), (136Xe, 135I), E(kinetic energy)=100-1200 MeV; calculated one-neutron- and one-proton-removal cross sections as a function of the kinetic energy. 1H(40Ca, 2p), E=392 MeV; 1H(197Au, 2p), E=200 MeV; calculated triple- and quadruple-differential cross sections for the production of protons. 1H(208Pb, X), (136Xe, X), E=1 GeV; calculated isotopic distributions of Z=81, 82 and 83 residues for 208Pb and Z=53, 54 and 55 residues for 136Xe. 1H(56Fe, X), (208Pb, X), (238U, X), E(K.E.)=10-3000 MeV; calculated total reaction cross sections as function of kinetic energy. 12C(18Ne, X), (19Ne, X), (20Ne, X), (21Ne, X), (22Ne, X), (23Ne, X), (24Ne, X), (25Ne, X), (26Ne, X), (28Ne, X), (29Ne, X), (20Mg, X), (22Mg, X), (23Mg, X), (24Mg, X), (25Mg, X), (27Mg, X), (29Mg, X), (30Mg, X), (31Mg, X), (32Mg, X), E=950 MeV/nucleon; 12C(9Be, X), (12C, X), (27Al, X), (64Zn, X), E<1050 MeV/nucleon; calculated total reaction cross sections. Liege Intranuclear-cascade (INLC) models. INCL++/ABLA07 calculations, and comparison with experimental data. NUCLEAR STRUCTURE 208Pb, 25Mg; calculated space-kinetic-energy density contours, proton and neutron densities for all nuclei between the proton and neutron drip lines using the Hartree-Fock-Bogoliubov approach based on the code HFBRAD.
doi: 10.1103/PhysRevC.96.054602
2016TI04 Nucl.Instrum.Methods Phys.Res. A821, 136 (2016) Yu.E.Titarenko, V.F.Batyaev, K.V.Pavlov, A.Yu.Titarenko, V.M.Zhivun, M.V.Chauzova, S.A.Balyuk, P.V.Bebenin, A.V.Ignatyuk, S.G.Mashnik, S.Leray, A.Boudard, J.C.David, D.Mancusi, J.Cugnon, Y.Yariv, K.Nishihara, N.Matsuda, H.Kumawat, A.Yu.Stankovskiy Excitation functions of the natCr(p, x)44Ti, 56Fe(p, x)44Ti, natNi(p, x)44Ti and 93Nb(p, x)44Ti reactions at energies up to 2.6 GeV NUCLEAR REACTIONS Cr(p, x)44Ti, 56Fe(p, x)44Ti, Ni(p, x)44Ti, 93Nb(p, x)44Ti, E=0.04-2.6 GeV; measured reaction products, Eγ, Iγ; deduced cumulative yields, σ. Comparison with theoretical calculations, available data.
doi: 10.1016/j.nima.2016.03.046
2015MA16 Phys.Rev. C 91, 034602 (2015) D.Mancusi, A.Boudard, J.Carbonell, J.Cugnon, J.-C.David, S.Leray Improving the description of proton-induced one-nucleon removal in intranuclear-cascade models NUCLEAR REACTIONS 40Ca(p, 39Ca), (p, 39K), E=500-1000 MeV; 208Pb(p, 207Pb), (p, 207Tl), E=500-1000 MeV; calculated one-proton- and one-neutron-removal cross sections, mass distribution of the residues, isotopic distributions of Z=76-83 residues, double-differential cross sections for the production of neutrons. INCL/ABLA07, Isabel/ABLA07, CEM03.03 and Geant4s Bertini model, INCL/GEMINI++ calculations. Comparison with experimental data. NUCLEAR STRUCTURE 208Pb; calculated proton kinetic-energy and space densities, space-kinetic-energy density contours, proton and neutron densities using initial conditions of the standard intranuclear-cascade models (INCL).
doi: 10.1103/PhysRevC.91.034602
2014HA13 Nucl.Instrum.Methods Phys.Res. B333, 27 (2014) S.Hashimoto, Y.Iwamoto, T.Sato, K.Niita, A.Boudard, J.Cugnon, J.-C.David, S.Leray, D.Mancusi New approach to description of (d, xn)(d, xn) spectra at energies below 50 MeV in Monte Carlo simulation by intra-nuclear cascade code with Distorted Wave Born Approximation NUCLEAR REACTIONS Li, 9Be, C(d, n), (d, X), E=12-30 MeV; analyzed available data; calculated σ(θ), σ(θ, E). DWBA calculations, comparison with available data.
doi: 10.1016/j.nimb.2014.04.007
2014LE14 Nucl.Data Sheets 118, 312 (2014) S.Leray, A.Boudard, B.Braunn, J.Cugnon, J.C.David, A.Leprince, D.Mancusi Recent Developments of the Liege Intranuclear Cascade Model in View of its Use into High-energy Transport Codes NUCLEAR REACTIONS 12C(12C, n), E=135 MeV/nucleon; calculated σ(θ, En) using GEANT4 with INCL++, INCL4.2 and BIC. Compared to data. H, C, N, O(12C, x), E=95 MeV/nucleon; calculated light fragments yield at different angles using INCL++, BIC and QMD. Medical application, compared to data.
doi: 10.1016/j.nds.2014.04.067
2014MA92 Phys.Rev. C 90, 054602 (2014) D.Mancusi, A.Boudard, J.Cugnon, J.-C.David, P.Kaitaniemi, S.Leray Extension of the Liege intranuclear-cascade model to reactions induced by light nuclei NUCLEAR REACTIONS Cu(p, π+), E=730 MeV; calculated INCL++. Comparison with experimental data and INCL4.6 calculations. Pb(p, n), E=800 MeV; 1H(208Pb, X), E=1000 MeV/nucleon; calculated INCL++/G4 Excitation Handler. Comparison with experimental data and INCL4.6/ABLA07, INCL++/ABLA07, INCL++/ABLA V3 calculations. 12C(π+, n), E=220 MeV; Pb(π-, n), E=870 MeV; 209Bi(3He, X)207At/208At/209At/210At, E not given; calculated INCL++/ABLA07. Comparison with experimental data and INCL4.6/ABLA07 calculations. Cu(α, n), E=230 MeV/nucleon; C(12C, n), E=290 MeV/nucleon; 12C(C, X)1H/4He/7Li/11C, E=95 MeV/nucleon; 2H(208Pb, X), E(lab)=1000 MeV/nucleon; 9Be(86Kr, X), E=500 MeV/nucleon; 9Be(58Ni, X), E=140 MeV/nucleon; 12C(56Fe, X), E=1050 MeV/nucleon; calculated INCL++/G4 Excitation Handler. Comparison with experimental data and with INCL++/ABLA V3, INCL++/ABLA 07, QMD, Binary Cascade, Bertini calculations. 181Ta(p, π+), (p, π-), E=7117 MeV; calculated INCL++. Comparison with experimental data. Extension of the Liege intranuclear-cascade (INC) model to reactions induced by light ions.
doi: 10.1103/PhysRevC.90.054602
2013BO03 Phys.Rev. C 87, 014606 (2013) A.Boudard, J.Cugnon, J.-C.David, S.Leray, D.Mancusi New potentialities of the Liege intranuclear cascade model for reactions induced by nucleons and light charged particles NUCLEAR REACTIONS 9Be, 56Fe, Pb, 208Pb(n, X), 9Be, 12C, 16O, 56Fe, Fe, 120Sn, 208Pb, Pb, (p, X), E=<1 GeV; 56Fe(n, xn), E=65 MeV; 56Fe(p, xp), E=62 MeV; 58Ni(p, xp), E=175 MeV; 208Pb(p, xp), E=800 MeV; 197Au(p, xp), (p, xd), (p, xt), (p, x3He), (p, xα), (p, x6He), (p, x6Li), (p, x7Li), (p, x7Be), Pb(p, xn), 208Pb(p, xd), (p, xt), (p, x3He), (p, xα), E=1.2 GeV; 208Pb(p, X), E=1 GeV; 208Pb(p, π+), (p, π-), E=730 MeV; Fe(p, X), E=0.3, 1.0 GeV; Pb(p, X), E=0.5, 1.0 GeV; U(p, X), E=1.0 GeV; Ni(d, X), (α, X), E<100 MeV; Bi(d, X), (α, X), E<200 MeV; 209Bi(3He, X), E<100 MeV; 209Bi(α, xn), E<70 MeV; 209Bi(α, n), (α, p), (α, np), E<200 MeV; Bi(d, n), (d, 2n), (d, p), E<40 MeV; 181Ta(α, n), (α, 2n), (α, 3n), (α, 4n), E<70 MeV; 181Ta(3He, n), (3He, 2n), (3He, 3n), (3He, 4n), E=10-35 MeV; 56Fe, 60Ni(α, n), E<50 MeV; 59Co(3He, n), (3He, 2n), E<90 MeV; 63Cu(3He, p), E<60 MeV; 60Ni(d, n), E<30 MeV; calculated double differential σ(θ, E), total cross section, fragment mass, atomic number and energy distributions. Liege intranuclear cascade (INC) model (INCL4.6 and ABLA07v5). Comparison with standard version (INCL4.2), and with experimental data.
doi: 10.1103/PhysRevC.87.014606
2013DA03 Eur.Phys.J. A 49, 29 (2013) J.C.David, A.Boudard, J.Cugnon, S.Ghali, S.Leray, D.Mancusi, L.Zanini Modeling astatine production in liquid lead-bismuth spallation targets NUCLEAR REACTIONS 1H(136Xe, X)Ba, E=1 GeV;197Au(p, 3He), (p, α), E=1200 MeV;Pb(p, X)At, (p, X)Hg, E=1, 1.4 GeV;Bi(p, π-)At, E=1, 1.4 GeV;Bi(3He, xn), (α, xn), E=0-100 MeV [with LBE (lead-bismuth eutectic) target]; calculated σ, σ(E, θ), isotope yields, activity release using MCNPX, INCL4.6, ABLA07, Fluka. Compared with ISOLDE published data.
doi: 10.1140/epja/i2013-13029-4
2011CU04 J.Korean Phys.Soc. 59, 955s (2011) J.Cugnon, D.Mancusi, A.Boudard, S.Leray New Features of the INCL4 Model for Spallation Reactions NUCLEAR REACTIONS Be(p, X), E=1-3000 MeV;Fe, Pb(p, X), E=5-3000 MeV;Pb(n, X), E=10-3000 MeV; calculated σ. Au(p, α), E=1.2 GeV; calculated σ(θ). 208Pb, 238U(p, X), E=1 GeV; calculated residue mass spectrum. INCL4.5 with ABLA07 code. Comparison to data.
doi: 10.3938/jkps.59.955
2011CU05 J.Phys.:Conf.Ser. 312, 082019 (2011) J.Cugnon, A.Boudard, J.-C.David, A.Kelic-Heil, S.Leray, D.Mancusi, M.V.Ricciardi Production of heavy clusters (up to A=10) by coalescence during the intranuclear cascade phase of spallation reactions NUCLEAR REACTIONS 197Au(p, 6Li), (p, 7Be), E=1200 MeV; calculated spallation σ(θ, E) using Liege Intra-Nuclear Cascade model INCL4.5 plus ABLA07. Compared with data and older models. Also other energies between 1.2 and 2.5 GeV, targets from Al to Th and other clusters calculated, but their results not presented within the paper.
doi: 10.1088/1742-6596/312/4/082019
2011MA60 J.Korean Phys.Soc. 59, 943s (2011) D.Mancusi, J.Cugnon, A.Boudard, J.-C.David, S.Leray, R.J.Charity, A.Kelic-heil, M.V.Ricciardi Multifragmentation in Reactions of 1-GeV Protons with Iron Nuclei NUCLEAR REACTIONS 56Fe(p, X), E=1 GeV; calculated multifragmentation IMF residue yields, σ, charge distributions, 7Li, 10B longitudinal velocity distributions, neutron multiplicity, α multiplicity. GEMINI++, SPALADIN, ABLA07 codes with and without multifragmentation. Comparison to data.
doi: 10.3938/jkps.59.943
2011MA73 Phys.Rev. C 84, 064615 (2011) D.Mancusi, A.Boudard, J.Cugnon, J.-C.David, T.Gorbinet, S.Leray Elusiveness of evidence for multifragmentation in 1-GeV proton-nucleus reactions NUCLEAR REACTIONS 56Fe, 136Xe(p, X), E=1 GeV; calculated excitation energies, mass-loss, remnants distributions, residue production cross section, longitudinal velocity distributions, average multiplicity of particles, multifragmentation signatures, fragment correlations. Hybrid intranuclear cascade plus statistical deexcitation models, Monte Carlo simulations. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.064615
2011PE23 Nucl.Phys. A866, 16 (2011) Extension of the Liege intranuclear cascade model at incident energies between 2 and 12 GeV. Aspects of pion production
doi: 10.1016/j.nuclphysa.2011.07.004
2011TI03 Phys.Atomic Nuclei 74, 523 (2011); Yad.Fiz. 74, 548 (2011) Yu.E.Titarenko, V.F.Batyaev, A.Yu.Titarenko, M.A.Butko, K.V.Pavlov, S.N.Florya, R.S.Tikhonov, V.M.Zhivun, A.V.Ignatyuk, S.G.Mashnik, S.Leray, A.Boudard, J.Cugnon, D.Mancusi, Y.Yariv, K.Nishihara, N.Matsuda, H.Kumawat, G.Mank, W.Gudowski Measurement and simulation of the cross sections for nuclide production in 56Fe and natCr targets irradiated with 0.04- to 2.6-GeV protons NUCLEAR REACTIONS Cr(p, X)52Mn/54Mn/48Cr/49Cr/51Cr/48V/43Sc/44Sc/46Sc/47Sc/48Sc/38K/42K/43K/44K/45K/41Ar/34Cl/38Cl/39Cl/38S/29Al/27Mg/28Mg/22Na/24Na/7Be, 56Fe(p, X)55Co/56Co/57Co/52Fe/53Fe/52Mn/54Mn/56Mn/48Cr/49Cr/51Cr/48V/43Sc/44Sc/46Sc/47Sc/48Sc/47Ca/38K/42K/43K/44K/41Ar/34Cl/38Cl/39Cl/38S/29Al/27Mg/28Mg/22Na/24Na/7Be, E=42-2605 MeV; measured reaction products, Eγ, Iγ; deduced σ and uncertainties. Comparison with intranuclear cascade code calculations.
doi: 10.1134/S1063778811040168
2011TI04 Phys.Atomic Nuclei 74, 537 (2011); Yad.Fiz. 74, 561 (2011) Yu.E.Titarenko, V.F.Batyaev, A.Yu.Titarenko, M.A.Butko, K.V.Pavlov, S.N.Florya, R.S.Tikhonov, V.M.Zhivun, A.V.Ignatyuk, S.G.Mashnik, S.Leray, A.Boudard, J.Cugnon, D.Mancusi, Y.Yariv, K.Nishihara, N.Matsuda, H.Kumawat, G.Mank, W.Gudowski Measurement and simulation of the cross sections for nuclide production in 93Nb and natNi targets irradiated with 0.04- to 2.6-GeV protons NUCLEAR REACTIONS Ni(p, X)60Cu/61Cu/56Ni/57Ni/56Co/57Co/58Co/60Co/62Co/55Co/52Fe/53Fe/59Fe/52Mn/54Mn/56Mn/48Cr/49Cr/51Cr/43Sc/44Sc/46Sc/47Sc/48Sc/47Ca/38K/42K/43K/41Ar/34Cl/38Cl/39Cl/38S/29Al/27Mg/28Mg/22Na/24Na/7Be, 93Nb(p, X)90Mo/91Mo/93Mo/88Nb/89Nb/90Nb/91Nb/92Nb/85Zr/86Zr/87Zr/88Zr/89Zr/84Y/85Y/86Y/87Y/88Y/90Y/80Sr/81Sr/82Sr/83Sr/85Sr/79Rb/81Rb/82Rb/83Rb/84Rb/86Rb/76Kr/77Kr/79Kr/74Br/75Br/76Br/77Br/72Se/73Se/75Se/70As/71As/72As/74As/65Ga/66Ga/67Ga/69Ga/60Cu/61Cu/67Cu/57Ni/55Co/56Co/57Co/58Co/60Co/62Co/53Fe/59Fe/52Mn/54Mn/56Mn/48Cr/49Cr/51Cr/48V/43Sc/44Sc/46Sc/47Sc/48Sc/47Ca/42K/43K/41Ar/38Cl/39Cl/27Mg/28Mg/22Na/24Na/7Be, E=46-2605 MeV; measured reaction products, Eγ, Iγ; deduced σ and uncertainties. Comparison with intranuclear cascade code calculations.
doi: 10.1134/S106377881104017X
2011TI05 Phys.Atomic Nuclei 74, 551 (2011); Yad.Fiz. 74, 574 (2011) Yu.E.Titarenko, V.F.Batyaev, A.Yu.Titarenko, M.A.Butko, K.V.Pavlov, S.N.Florya, R.S.Tikhonov, V.M.Zhivun, A.V.Ignatyuk, S.G.Mashnik, S.Leray, A.Boudard, J.Cugnon, D.Mancusi, Y.Yariv, K.Nishihara, N.Matsuda, H.Kumawat, G.Mank, W.Gudowski Measurement and simulation of the cross sections for nuclide production in natW and 181Ta targets irradiated with 0.04- to 2.6-GeV protons NUCLEAR REACTIONS W(p, X)176Re/177Re/178Re/179Re/181Re/182Re/183Re/184Re/186Re/174W/176W/177W/178W/181W/172Ta/173Ta/174Ta/175Ta/176Ta/177Ta/178Ta/182Ta/183Ta/184Ta/168Hf/170Hf/171Hf/172Hf/173Hf/175Hf/179Hf/180Hf/181Hf/167Lu/169Lu/170Lu/171Lu/172Lu/173Lu/162Yb/166Yb/167Yb/169Yb/161Tm/162Tm/163Tm/165Tm/166Tm/167Tm/168Tm/156Er/157Er/159Er/160Er/161Er/156Ho/160Ho/152Dy/155Dy/157Dy/147Tb/148Tb/149Tb/150Tb/151Tb/152Tb/153Tb/155Tb/145Gd/146Gd/147Gd/149Gd/151Gd/153Gd/145Eu/146Eu/147Eu/148Eu/149Eu/140Pm/143Pm/144Pm/136Nd/139Nd/134Pr/136Pr/130Ce/132Ce/133Ce/134Ce/135Ce/139Ce/130La/132La/126Ba/128Ba/131Ba/133Ba/127Cs/129Cs/120Xe/122Xe/123Xe/125Xe/127Xe/120I/114Te/117Te/119Te/121Te/113Sb/115Sb/118Sb/120Sb/113Sn/108In/109In/110In/111In/105Ag/106Ag/110Ag/100Pd/99Rh/100Rh/102Rh/97Ru/103Ru/94Tc/96Tc/93Mo/90Nb/88Zr/89Zr/86Y/87Y/88Y/83Sr/85Sr/82Rb/83Rb/84Rb/77Br/75Se/74As/65Zn/69Zn/56Co/58Co/60Co/59Fe/52Mn/54Mn/48V/44Sc/46Sc/48Sc/28Mg/22Na/24Na/7Be, Ta(p, X)174W/176W/177W/178W/172Ta/173Ta/174Ta/175Ta/176Ta/177Ta/178Ta/180Ta/168Hf, 170Hf/171Hf/172Hf/173Hf/175Hf/179Hf/180Hf/181Hf/167Lu/169Lu/170Lu/171Lu/172Lu/173Lu/162Yb/166Yb/167Yb/169Yb/161Tm/162Tm/163Tm/165Tm/166Tm/167Tm/168Tm/156Er/157Er/159Er/160Er/161Er/156Ho/160Ho/152Dy/155Dy/157Dy/148Tb/149Tb/150Tb/151Tb/152Tb/153Tb/155Tb/145Gd/146Gd/147Gd/149Gd/151Gd/153Gd/145Eu/146Eu/147Eu/148Eu/149Eu/140Pm/143Pm/144Pm/136Nd/139Nd/134Pr/136Pr/138Pr/130Ce/132Ce/133Ce/134Ce/135Ce/139Ce/130La/132La/128Ba/131Ba/133Ba/127Cs/129Cs/122Xe/123Xe/127Xe/114Te/117Te/119Te/121Te/113Sb/115Sb/118Sb/120Sb/108In/109In, 110In, 111In, 105Ag/106Ag/110Ag/100Pd/99Rh/100Rh/102Rh/97Ru/103Ru/96Tc/93Mo/90Nb/88Zr/89Zr/86Y/87Y/88Y/83Sr/85Sr/82Rb/83Rb/84Rb/77Br/75Se/74As/65Zn/69Zn/56Co/58Co/60Co/59Fe/52Mn/54Mn/48V/44Sc/46Sc/48Sc/28Mg/22Na/24Na/7Be, E=43-2605 MeV; measured reaction products, Eγ, Iγ; deduced σ and uncertainties. Comparison with intranuclear cascade code calculations.
doi: 10.1134/S1063778811040181
2011TI06 Phys.Atomic Nuclei 74, 573 (2011); Yad.Fiz. 74, 596 (2011) Yu.E.Titarenko, V.F.Batyaev, A.Yu.Titarenko, M.A.Butko, K.V.Pavlov, S.N.Florya, R.S.Tikhonov, V.M.Zhivun, A.V.Ignatyuk, S.G.Mashnik, S.Leray, A.Boudard, J.Cugnon, D.Mancusi, Y.Yariv, K.Nishihara, N.Matsuda, H.Kumawat, G.Mank, W.Gudowski Measurement and simulation of the cross sections for the production of 148Gd in thin natW and 181Ta targets irradiated with 0.4- to 2.6-GeV protons NUCLEAR REACTIONS W, 181Ta(p, X)148Gd, E=0.4-2.6 GeV; measured reaction products, Eα, Iα; deduced σ. Direct α-spectrometry without chemical separation, comparison with other experimental data and cascade code calculations.
doi: 10.1134/S1063778811040193
2011TI12 Phys.Rev. C 84, 064612 (2011) Yu.E.Titarenko, V.F.Batyaev, M.A.Butko, D.V.Dikarev, S.N.Florya, K.V.Pavlov, A.Yu.Titarenko, R.S.Tikhonov, V.M.Zhivun, A.V.Ignatyuk, S.G.Mashnik, A.Boudard, S.Leray, J.-C.David, J.Cugnon, D.Mancusi, Y.Yariv, H.Kumawat, K.Nishihara, N.Matsuda, G.Mank, W.Gudowski Verification of high-energy transport codes on the basis of activation data NUCLEAR REACTIONS Cr, 56Fe, Ni, 93Nb, 181Ta, W, Pb, 209Bi, 208Pb(p, X), E=40-2600 MeV; analyzed production cross sections data at ITEP with high-energy transport codes (HETC): MCNPX, CEM03.02, INCL4.2+ABLA, INCL4.5+ABLA07, PHITS, CASCADE.07. Predictive accuracy of the HETC tested here indicates that all codes need further improvements. NUCLEAR REACTIONS 208Pb(p, X)7Be/46Sc/59Fe/72Zn/72Ga/74As/75Se/82Br/83Rb/86Rb/85Sr/87Y/88Y/90mY/88Zr/89Zr/95Zr/97Zr/92mNb/95Nb/96Nb/99Mo/96Tc/103Ru/101Rh/102Rh/105Rh/106mAg/110mAg/114mIn/117mSn/120mSb/119mTe/121Te/121mTe/123mTe/127Xe/139Ce/169Yb/169Lu/170Lu/171Lu/173Lu/172Hf/175Hf/176Ta/177Ta/177W/178W/178Re/179Re/181Re/182mRe/183Re/180Os/181Os/182Os/183mOs/185Os/183Ir/184Ir/185Ir/186Ir/186mIr/187Ir/188Ir/189Ir/190Ir/192Ir/184Pt/186Pt/187Pt/188Pt/189Pt/191Pt/190Au/191Au/192Au/193Au/194Au/195Au/196Au/198Au/198mAu/190Hg/191Hg/192Hg/193Hg/193mHg/195Hg/195mHg/197mHg/203Hg/195Tl/196mTl/197Tl/198Tl/198mTl/199Tl/200Tl/201Tl/202Tl/195mPb/196Pb/197mPb/198Pb/199Pb/200Pb/201Pb/202mPb/203Pb/204mPb/202Bi/203Bi/204Bi/205Bi/206Bi/207Bi, E=500 MeV; measured production cross sections at ITEP. Comparison with cross sections measured at GSI in the inverse kinematics approach.
doi: 10.1103/PhysRevC.84.064612
2010MA58 Phys.Rev. C 82, 044610 (2010) D.Mancusi, R.J.Charity, J.Cugnon Unified description of fission in fusion and spallation reactions NUCLEAR REACTIONS 90Zr(64Ni, X), 139La, 159W, 169Tm, 181Ta, 197Au(19F, X), 100Mo(60Ni, X), 150Sm(18O, X), 165Ho(28Si, X), 170Er, 186W(30Si, X), 184W(32S, X), 182W, 204Pb(12C, X), 208Pb(16O, X), E<10 MeV/nucleon; 208Pb(p, X), E=500, 1000 MeV; 181Ta(p, X), E=150-1200 MeV; 197Au, 238U(p, X), E=1 GeV; Au, Bi, U(p, X), E=2.5 GeV; calculated σ for fusion and evaporation residues as function of evaporation residue energy, residual mass distributions, fission probability using Monte-Carlo statistical models for fission in fusion and spallation reactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.82.044610
2009AO04 Nucl.Phys. A828, 52 (2009) Production of Z+1 and A+1 isotopes in proton-induced reactions on AZ nuclei NUCLEAR REACTIONS 208Pb, 209Bi(p, X), E=10-2000 MeV; analyzed σ using intra-nuclear cascade model and the effect of pion production.
doi: 10.1016/j.nuclphysa.2009.06.025
2006AO03 Phys.Rev.C 74, 064607 (2006) Pion physics in the Liege intranuclear cascade model NUCLEAR REACTIONS 12C, 208Pb(p, π+X), (p, π-X), E=730 MeV; calculated pion production σ(E, θ). 12C, 56Fe, 93Nb, 209Bi(π+, X), E ≈ 80-320 MeV; calculated reaction σ. 27Al, 56Fe, 63Cu, 209Bi(π+, X), 27Al, 63Cu, 120Sn, 197Au(π-, X), E ≈ 40-300 MeV; calculated absorption σ. 12C, Ni, 181Ta(π+, pX), (π-, pX), E=220 MeV; 208Pb(π+, nX), E=870 MeV; calculated proton emission σ(E, θ). U(π+, F), E=80 MeV; calculated fission fragment mass yield. 209Bi, 235U(π+, F), E=50-250 MeV; calculated fission σ. Liege intranuclear cascade model, comparison with data.
doi: 10.1103/PhysRevC.74.064607
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
2006LE22 Nucl.Instrum.Methods Phys.Res. A562, 760 (2006) I.Leya, R.Wieler, J.-C.David, S.Leray, L.Donadille, J.Cugnon, R.Michel Production of noble gas isotopes by proton-induced reactions on lead and bismuth NUCLEAR REACTIONS Pb, Bi(p, X)3He/4He/21Ne/22Ne/81Kr/82Kr/85Kr/126Xe/132Xe, E ≈ 10-2600 MeV; measured production σ.
doi: 10.1016/j.nima.2006.02.049
2005LE04 Nucl.Instrum.Methods Phys.Res. B229, 1 (2005) I.Leya, R.Wieler, J.-C.David, S.Leray, L.Donadille, J.Cugnon, R.Michel Production of noble gas isotopes by proton-induced reactions on lead NUCLEAR REACTIONS Pb(p, X)3He/4He/21Ne/22Ne/36Ar/38Ar/78Kr/80Kr/81Kr/82Kr/83Kr/84Kr/85Kr/86Kr/124Xe/126Xe/128Xe/129Xe/130Xe/131Xe/132Xe/134Xe, E=44-2595 MeV; measured production σ; deduced reaction mechanism features. Mini-stack approach, comparisons with model predictions.
doi: 10.1016/j.nimb.2004.11.009
2004AO06 Eur.Phys.J. A 21, 79 (2004) Effects of isospin and energy dependences of the nuclear mean field in spallation reactions NUCLEAR REACTIONS 56Fe, 208Pb(p, X), E=256, 800 MeV; calculated particle multiplicities, neutron and proton production σ(E, θ); deduced isospin and energy dependence effects. Intranuclear-cascade model, comparison with data.
doi: 10.1140/epja/i2003-10186-y
2004BO24 Nucl.Phys. A740, 195 (2004) A.Boudard, J.Cugnon, S.Leray, C.Volant A new model for production of fast light clusters in spallation reactions NUCLEAR REACTIONS 197Au(p, nX), (p, pX), (p, dX), (p, tX), (p, 3HeX), (p, αX), E=2.5 GeV; Cu, Bi(p, pX), (p, dX), (p, tX), E=542 MeV; 208Pb(p, nX), E=1200 MeV; calculated light particle spectra, σ(E, θ). 197Au(p, X), E=2.5 GeV; 208Pb(p, X), E=1, 1.2 GeV; calculated particle multiplicities with and without cluster emission. Intranuclear cascade model, surface percolation procedure, comparisons with data.
doi: 10.1016/j.nuclphysa.2004.05.003
2004KL06 Phys.Rev. C 69, 044311 (2004) B.Klos, S.Wycech, A.Trzcinska, J.Jastrzebski, T.Czosnyka, M.Kisielinski, P.Lubinski, P.Napiorkowski, L.Pienkowski, F.J.Hartmann, B.Ketzer, R.Schmidt, T.von Egidy, J.Cugnon, K.Gulda, W.Kurcewicz, E.Widmann Strong interaction and E2 effect in even-A antiprotonic Te atoms ATOMIC PHYSICS 122,124,126,128,130Te(p-bar, X), E at 106, 300 MeV/c; measured X-ray spectra from antiprotonic atoms; deduced level widths and shifts, nuclear resonance effect. 122,124,126,128,130Te deduced relative neutron, proton radii, neutron density at periphery.
doi: 10.1103/PhysRevC.69.044311
2003CU01 Eur.Phys.J. A 16, 393 (2003) The low-energy limit of validity of the intranuclear cascade model NUCLEAR REACTIONS 12C, 27Al, 54Fe, 58Ni, 197Au, 209Bi(p, pX), E ≈ 25-250 MeV; 27Al, 48Ca, 90Zr, 120Sn, 208Pb(p, nX), E ≈ 25-250 MeV; 54Fe, 93Nb, 120Sn, 208Pb(n, nX), E ≈ 15-65 MeV; 208Pb(n, pX), E ≈ 63-97 MeV; calculated σ(E, θ). Intranuclear cascade model, comparison with data.
doi: 10.1140/epja/i2002-10096-6
2002BO45 Phys.Rev. C66, 044615 (2002) A.Boudard, J.Cugnon, S.Leray, C.Volant Intranuclear cascade model for a comprehensive description of spallation reaction data NUCLEAR REACTIONS Fe, Pb, U(p, X), E ≈ 10-2000 MeV; analyzed total reaction σ. Pb(p, nX), E=113-1600 MeV; Pb(d, nX), E=1600 MeV; Al, Zr, Th(p, nX), E=1200 MeV; calculated neutron spectra, σ(θ). Pb(p, pX), E=730 MeV; calculated proton spectra, σ(θ). 1H(208Pb, X), (197Au, X), (56Fe, X), E=high; calculated fragments isotopic yields. Intranuclear cascade model, comparisons with data.
doi: 10.1103/PhysRevC.66.044615
2001CU01 Phys.Rev. C63, 027301 (2001) J.Cugnon, S.Wycech, J.Jastrzebski, P.Lubinski Geometrical Effects in Antiproton Annihilation on Nuclei
doi: 10.1103/PhysRevC.63.027301
2000CU04 Ann.Phys.(Paris) 25, 93 (2000) Spallation Reactions
2000CU05 Phys.Rev. C62, 064308 (2000) J.Cugnon, A.Lejeune, H.-J.Schulze Hypernuclei in the Skyrme-Hartree-Fock Formalism with a Microscopic Hyperon-Nucleon Force NUCLEAR STRUCTURE 13C, 17O, 29Si, 41Ca, 91Zr, 141Ce, 209Pb; calculated Λ hypernucleus single-particle levels. 40Ca, 90Zr, 208Pb; calculated multi-Λ hypernuclei density profiles, radii, binding energies. Skyrme-Hartree-Fock model.
doi: 10.1103/PhysRevC.62.064308
2000PO10 Phys.Lett. 482B, 349 (2000) E.C.Pollacco, J.Brzychczyk, C.Volant, R.Legrain, R.G.Korteling, D.S.Bracken, K.Kwiatkowski, K.B.Morley, E.Renshaw Foxford, V.E.Viola, N.R.Yoder, H.Breuer, J.Cugnon Evaporation Residue as a Dominant Exit Channel at High Thermal Energies in 3He + Ag Reactions NUCLEAR REACTIONS Ag(3He, X), E=1.8 GeV; measured fragments energy, mass, coincidences; deduced heavy fragment excitation, reaction mechnism features.
doi: 10.1016/S0370-2693(00)00551-7
1998BR20 Phys.Rev. C58, R1372 (1998) J.Brzychczyk, E.C.Pollacco, C.Volant, D.Lacroix, R.Legrain, K.Kwiatkowski, D.S.Bracken, K.B.Morley, E.Renshaw Foxford, V.E.Viola, N.R.Yoder, J.Cugnon, R.G.Korteling, H.Breuer Diversity of Fragment Sizes in Multifragmentation of Gold Nuclei Induced by Relativistic 3He Ions NUCLEAR REACTIONS 197Au(3He, X), E=4.8 GeV; measured fragments charge, multiplicity distributions; deduced possible phase transition.
doi: 10.1103/PhysRevC.58.R1372
1998LE12 Phys.Rev. C57, 2375 (1998) X.Ledoux, H.G.Bohlen, J.Cugnon, H.Fuchs, J.Galin, B.Gatty, B.Gebauer, D.Guerreau, D.Hilscher, D.Jacquet, U.Jahnke, M.Josset, S.Leray, B.Lott, M.Morjean, B.M.Quednau, G.Roschert, H.Rossner, A.Peghaire, L.Pienkowski, R.H.Siemssen, C.Stephan Formation and Decay of Hot Nuclei in 475 MeV, 2 GeV Proton- and 2 GeV 3He-Induced Reactions on Ag, Bi, Au, and U NUCLEAR REACTIONS 107Ag, 197Au, 209Bi, 238U(p, X), E=0.475, 2 GeV; 107Ag, 197Au, 209Bi, 238U(3He, X), E=2 GeV; measured neutron multiplicity distributions, light-, intermediate-charged particle energy distributions, fission fragments; deduced compound nucleus temperature, other reaction mechanism features. Comparison with two-step cascade process model.
doi: 10.1103/PhysRevC.57.2375
1998SC01 Phys.Rev. C57, 704 (1998) H.-J.Schulze, M.Baldo, U.Lombardo, J.Cugnon, A.Lejeune Hyperonic Nuclear Matter in Brueckner Theory
doi: 10.1103/PhysRevC.57.704
1997CO03 Phys.Rev. C55 1404 (1997) M.Colonna, J.Cugnon, E.C.Pollacco Resilience of Nuclear Matter in Light Ion Induced Reactions NUCLEAR REACTIONS Ag(3He, X), E=1.6 GeV/nucleon; calculated nucleon density distribution in reaction plane, excitation energy time evolution, average fragment number of given mass. Intranuclear cascade model.
doi: 10.1103/PhysRevC.55.1404
1997CU04 Nucl.Phys. A620, 475 (1997) J.Cugnon, C.Volant, S.Vuillier Improved Intranuclear Cascade Model for Nucleon-Nucleus Interactions NUCLEAR REACTIONS Fe, Pb(p, xn), E=256-800 MeV; calculated σ(θ, En). 209Bi(n, xd), E=540 MeV; calculated σ(θ, Ed). 197Au(p, X), E=1 GeV; calculated residue mass spectra. Intranuclear cascade model.
doi: 10.1016/S0375-9474(97)00186-3
1997CU05 Phys.Rev. C56, 2431 (1997) J.Cugnon, S.Leray, E.Martinez, Y.Patin, S.Vuillier New Constraints on the Δ Production Cross Section NUCLEAR REACTIONS 1H(n, p), E=400, 800, 1150, 1600 MeV; analyzed σ(Ep, θ); deduced parameters, Δ production σ, isospin conservation role.
doi: 10.1103/PhysRevC.56.2431
1997CU06 Nucl.Phys. A625, 729 (1997) J.Cugnon, C.Volant, S.Vuillier Nucleon and Deuteron Induced Spallation Reactions NUCLEAR REACTIONS Pb(p, X), E=256, 597, 1200, 2000 MeV; calculated residual mass distributions; Fe, Pb(p, X), E=800 MeV; calculated neutron production σ(θ, En); Pb(p, X), E=1000 MeV; calculated target residue, fragment Z, N distributions; Pb(d, X), E=1600 MeV; calculated neutron production σ(En). Intranuclear cascade model, other reactions considered.
doi: 10.1016/S0375-9474(97)00602-7
1996CU01 Nucl.Phys. A598, 515 (1996) J.Cugnon, M.Jaminon, B.Van den Bossche Phase Transition and Thermodynamics of a Hot and Dense System in a Scaled NJL Model
doi: 10.1016/0375-9474(95)00501-3
1996CU04 Ann.Phys.(Paris) 21, 537 (1996) Relativistic and Ultrarelativistic Heavy-Ion Collisions. Theoretical Aspects
1996CU05 Nucl.Instrum.Methods Phys.Res. B111, 215 (1996) J.Cugnon, D.L'Hote, J.Vandermeulen Simple Parametrization of Cross-Sections for Nuclear Transport Studies up to the GeV Range NUCLEAR REACTIONS 1n, 1H(p, X), (π+, X), E=high; analyzed σ(θ), total σ; deduced parameters. Transport calculations.
doi: 10.1016/0168-583X(95)01384-9
1996SC10 Phys.Lett. 375B, 1 (1996) H.-J.Schulze, J.Cugnon, A.Lejeune, M.Baldo, U.Lombardo Medium Polarization Effects on Neutron Matter Superfluidity
doi: 10.1016/0370-2693(96)00213-4
1995CU02 Nucl.Phys. A587, 596 (1995) J.Cugnon, A.Dolgolenko, A.Sibirtsev, J.Vandermeulen Double Strangeness Production in Low-Energy Antiproton-Nucleus Annihilation NUCLEAR REACTIONS Xe(p-bar, X), E at 0-0.9 GeV/c; calculated double strangeness yields; deduced different mechanisms role.
doi: 10.1016/0375-9474(95)00006-M
1995GO11 Z.Phys. A351, 199 (1995) Importance of Gluon-Gluon and Quark-Antiquark Contributions to Charmonium Production in Proton-Proton and Antiproton-Proton Collisions NUCLEAR REACTIONS 1H(p, X), E=high; analyzed charmonium states production data; deduced gluon-gluon, quark-antiquark contributions role.
doi: 10.1007/BF01289530
1995SC41 Phys.Rev. C52, 2785 (1995) H.-J.Schulze, J.Cugnon, A.Lejeune, M.Baldo, U.Lombardo Status of the Brueckner-Hartree-Fock Approximation to the Nuclear Matter Binding Energy with the Paris Potential
doi: 10.1103/PhysRevC.52.2785
1995SC43 Phys.Lett. 355B, 21 (1995) H.-J.Schulze, A.Lejeune, J.Cugnon, M.Baldo, U.Lombardo Hypernuclear Matter in the Brueckner-Hartree-Fock Approximation
doi: 10.1016/0370-2693(95)00665-8
1994CU03 Yad.Fiz. 57, No 9, 1705 (1994); Phys.Atomic Nuclei 57, 1635 (1994) Nuclear Multifragmentation: Antiprotons versus photons and heavy ions NUCLEAR REACTIONS Pb, 197Au(p, X), E=0.2-20 GeV; Pb(p-bar, X), E ≤ 5 GeV; Ba, Th(Ar, X), E ≤ 0.1 GeV; compiled, reviewed this, other reaction data, analyses; deduced suitable reaction for multi-fragmentation studies.
1994PI06 Acta Phys.Pol. B25, 737 (1994) L.Pienkowski, S.Leray, J.Galin, D.Guerreau, X.Ledoux, B.Lott, M.Morjean, A.Peghaire, H.-G.Bohlen, H.Fuchs, B.Gebauer, D.Hilscher, U.Jahnke, G.Roschert, H.Rossner, B.Gatty, D.Jacquet, C.Stephan, R.Siemssen, J.Cugnon Thermal Excitation Energy Distribution of 475 MeV and 2 GeV Proton and 3He Induced Reactions in Heavy Nuclei NUCLEAR REACTIONS U, 209Bi, 197Au, Ag(p, xn), E=0.475, 2 GeV; Ag, 197Au, 209Bi, U(3He, xn), E=2 GeV; measured neutron multiplicity distributions; deduced thermal excitation energy distribution. Intra-nuclear cascade model analysis.
1994PI08 Phys.Lett. 336B, 147 (1994) L.Pienkowski, H.G.Bohlen, J.Cugnon, H.Fuchs, J.Galin, B.Gatty, B.Gebauer, D.Guerreau, D.Hilscher, D.Jacquet, U.Jahnke, M.Josset, X.Ledoux, S.Leray, B.Lott, M.Morjean, A.Peghaire, G.Roschert, H.Rossner, R.H.Siemssen, C.Stephan Hot Nuclei in Reactions Induced by 475 MeV, 2 GeV 1H and 2 GeV 3He NUCLEAR REACTIONS Ag, 197Au, 209Bi, U(p, nX), E=0.475, 2 GeV; Ag, 197Au, 209Bi, U(3He, nX), E=2 GeV; measured inclusive neutron multiplicity distributions. Intranuclear cascade analysis.
doi: 10.1016/0370-2693(94)00910-4
1993BA22 Nucl.Phys. A556, 409 (1993) V.V.Barmin, V.G.Barylov, G.V.Davidenko, V.S.Demidov, A.G.Dolgolenko, V.M.Golubchikov, V.A.Matveev, A.G.Meshkovsky, G.S.Mirosidi, A.N.Nikitenko, V.A.Shebanov, N.N.Shishov, B.S.Volkov, N.K.Zombkovskaya, A.D.Andryakov, E.V.Demidova, V.A.Ergakov, Yu.V.Trebukhovsky, C.Guaraldo, J.Cugnon, J.Vandermeulen Strange-Particle Production in (p-bar)Xe Annihilation at Rest and at 0.4-0.9 GeV/c NUCLEAR REACTIONS 131Xe(p-bar, X), E at rest, E at 0.4-9.9 GeV/c; measured strangeness, double strangeness production, proton, pion mean multiplicities. Comparison with intranuclear cascade model. Bubble chamber.
doi: 10.1016/0375-9474(93)90369-9
1992CU02 Nucl.Phys. A542, 559 (1992) Antideuteron Annihilation on Nuclei NUCLEAR REACTIONS 98Mo(d-bar, X), E=0.5 GeV; calculated fragment yield vs mass number. 98Mo(d-bar, X), E=1, 10 GeV; calculated fragment production σ vs mass. Cascade plus percolation model.
doi: 10.1016/0375-9474(92)90257-K
1991LE06 Phys.Rev. C43, 2711 (1991) M.-C.Lemaire, M.Trzaska, J.P.Alard, J.Augerat, D.Bachelier, N.Bastid, J.-L.Boyard, C.Cavata, P.Charmensat, P.Dupieux, P.Gorodetzky, J.Gosset, T.Hennino, J.-C.Jourdain, A.Le Merdy, D.L'Hote, B.Lucas, J.Marroncle, G.Montarou, M.-J.Parizet, J.Poitou, D.Qassoud, P.Radvanyi, B.Ramstein, A.Rahmani, M.Roy-Stephan, O.Valette, P.Zupranski, J.Cugnon, J.Vandermeulen Charged-Pion Production in Noninclusive Proton-Nucleus Interactions at 0.8 and 1.6 GeV Incident Energies NUCLEAR REACTIONS 12C, 93Nb, Pb(p, xπ+), (p, xπ-), (p, X), E=800, 2100 MeV; measured pion multiplicity, light charged particle production vs impact parameter. Intranuclear cascade model.
doi: 10.1103/PhysRevC.43.2711
1991TR04 Z.Phys. A340, 325 (1991) M.Trzaska, D.Pelte, M.-C.Lemaire, J.P.Alard, J.Augerat, D.Bachelier, N.Bastid, J.-L.Boyard, C.Cavata, P.Charmensat, J.Cugnon, P.Dupieux, P.Gorodetzky, J.Gosset, T.Hennino, J.-C.Jourdain, A.Le Merdy, D.L'Hote, B.Lucas, J.Marroncle, G.Montarou, M.-J.Parizet, J.Poitou, D.Quassoud, P.Radvanyi, B.Ramstein, A.Rahmani, M.Roy-Stephan, O.Valette, J.Vandermeulen, P.Zupranski Excitation of the Δ(1232)-Resonance in Proton-Nucleus Collisions NUCLEAR REACTIONS C, 93Nb, Pb(p, π+), (p, π-), E=0.8, 1.6 GeV; measured pion-proton correlated invariant mass spectra; deduced Δ(1232) resonance parameters. Intranuclear cascade model.
doi: 10.1007/BF01294681
1990CU01 Phys.Rev. C41, 1701 (1990) J.Cugnon, P.Deneye, J.Vandermeulen Strangeness Production in Antiproton Annihilation on Nuclei NUCLEAR REACTIONS 1H(p-bar, X), E at 1-6 GeV/c; calculated annihilation σ(E), lambda production missing mass spectrum, rapidity distribution. Cascade-type model.
doi: 10.1103/PhysRevC.41.1701
1990CU03 Nucl.Phys. A513, 636 (1990) J.Cugnon, P.Deneye, J.Vandermeulen Hypernucleus Formation After Antiproton Annihilation on Nuclei NUCLEAR REACTIONS 209Bi, 238U(p-bar, X), E at rest; calculated partial hypernucleon formation yields following p-bar annihilation. Intranuclear cascade model.
doi: 10.1016/0375-9474(90)90402-8
1990CU04 Nucl.Phys. A517, 533 (1990) J.Cugnon, P.Deneye, J.Vandermeulen Antiproton Annihilation at Rest on Light Nuclei: Rescattering, strange-particle yield and B = 1 annihilation NUCLEAR REACTIONS 2H, 3,4He, 14N, 20Ne(p-bar, X), E at rest; calculated annihilation particle spectra. Intranuclear cascade model.
doi: 10.1016/0375-9474(90)90216-9
1989CU06 Ann.Phys.(Paris) 14, 49 (1989) Antiproton-Nucleus Interaction NUCLEAR REACTIONS 12C(p-bar, p-bar), E=46.8 MeV; 20Ne(p-bar, p-bar), E at 193-608 MeV/c; 12C, 20Ne, 89Y, 238U(p-bar, xπ), E=600 MeV; compiled this, other data analysis; deduced p-bar annihilation dynamics, hypernucleus production, strangeness formation.
1989CU07 Phys.Rev. C40, 1822 (1989) J.Cugnon, P.Deneye, J.Vandermeulen Role of Mesonic Resonances in Antiproton Annihilation on Nuclei NUCLEAR REACTIONS 12C, 238U(p-bar, X), E at 608 MeV/c; calculated p-bar annihilation pion, other mesonic absorption probability. Simplified cascade scheme.
doi: 10.1103/PhysRevC.40.1822
1989CU08 Nucl.Phys. A500, 701 (1989) J.Cugnon, P.Deneye, J.Vandermeulen Multipion Dynamics following Antiproton Annihilation on Nuclei NUCLEAR REACTIONS 12C, 238U(p-bar, π+X), 20Ne(p-bar, π-X), 12C(p-bar, pX), E at 608 MeV/c; calculated inclusive pion, proton production σ vs momentum. Intranuclear cascade model.
doi: 10.1016/0375-9474(89)90236-4
1989CU10 Z.Phys. A334, 435 (1989) Multifragmentation in the Intranuclear Cascade - Percolation Approach NUCLEAR REACTIONS Xe(p, X), E=3.8 GeV; calculated fragment yield vs mass, O, Ne production σ(θ). 232Th(α, X), E=1.05 GeV/nucleon; calculated primary fragment production σ vs mass. Other high energy heavy ion data analyzed. Intranuclear cascade model.
1988CU03 Phys.Rev. C38, 795 (1988) J.Cugnon, P.Deneye, J.Vandermeulen Charge Distribution and Charge Correlation in the Annihilation of Antiprotons on Nuclei NUCLEAR REACTIONS Ne(p-bar, π+), (p-bar, π-), E at 608 MeV/c; calculated pion multiplicities. Schematic model.
doi: 10.1103/PhysRevC.38.795
1988CU05 Nucl.Phys. A485, 271 (1988) Spin and Spin-Isospin Polarized Nuclear Matter NUCLEAR REACTIONS 59Co(n, n), E ≈ 0.3-31 MeV; 27Al(p, p), E=18 MeV; 59Co(p, p), E=47.5 MeV; 89Y, 87Rb(p, p), E=5 MeV; calculated model parameters. Optical model.
doi: 10.1016/0375-9474(88)90102-9
1988JA09 Nucl.Phys. A484, 542 (1988) P.Jasselette, J.Cugnon, J.Vandermeulen Residual Mass Distribution following p(p-bar)-Nucleus Annihilation NUCLEAR REACTIONS 238U(p-bar, F), E not given; calculated fission probability vs evaporation neutron number. 165Ho, 98Mo(p-bar, X), E not given; calculated fragment mass distribution shapes. Projectile annihilation.
doi: 10.1016/0375-9474(88)90309-0
1987CU01 Nucl.Phys. A462, 751 (1987) Proton-Nucleus Interaction at High Energy NUCLEAR REACTIONS Ca, 197Au(p, X), E ≤ 100 GeV; calculated time evolutions, density profiles, projectile energy losses, energy, mass dependences, stopping powers. Intranuclear cascade model.
doi: 10.1016/0375-9474(87)90575-6
1987CU02 Z.Phys. A327, 187 (1987) Negative Binomial Multiplicity Distributions and Intranuclear Cascade NUCLEAR REACTIONS Ca, 98Mo, Au(p, X), E=0.5, 2, 5 GeV; Ca(Ca, X), E=0.8 GeV/nucleon; analyzed nucleon multiplicity probability distributions. Intranuclear cascade model.
1987LH01 Phys.Lett. 198B, 139 (1987) D.L'Hote, J.P.Alard, J.Augerat, R.Babinet, F.Brochard, Z.Fodor, L.Fraysse, J.Girard, P.Gorodetzky, J.Gosset, C.Laspalles, M.C.Lemaire, B.Lucas, G.Montarou, M.J.Parizet, J.Poitou, C.Racca, W.Schimmerling, J.C.Tamain, Y.Terrien, J.Valerio, J.Cugnon, J.Vandermeulen Exclusive Measurements of Mean Pion Multiplicities in 4He-Nucleus Reactions from 200 to 800 MeV/Nucleon NUCLEAR REACTIONS C, Cu, Pb(α, π+), (α, π-), E=200, 600, 800 MeV/nucleon; C, Pb(α, π+), (α, π-), E=400 MeV/nucleon; measured mean pion multiplicities. Cylindrical drift chamber.
doi: 10.1016/0370-2693(87)91484-5
1986CU03 Nucl.Phys. A452, 738 (1986) Properties and Causes of the Collective Flow NUCLEAR REACTIONS Ca(Ca, X), 93Nb(93Nb, X), 197Au(197Au, X), E=400 MeV/nucleon; calculated collective flow mass, energy dependences.
doi: 10.1016/0375-9474(86)90224-1
1984CU01 Phys.Lett. 134B, 392 (1984) Kaon Production in High Energy Nucleus-Nucleus Collisions NUCLEAR REACTIONS Na, F(Ne, K+), E=2.1 GeV/nucleon; calculated kaon production σ; deduced rescattering role. Three-dimensional cascade model.
doi: 10.1016/0370-2693(84)91368-6
1983CA25 Nucl.Phys. A411, 524 (1983) M.Cahay, J.Cugnon, J.Vandermeulen Pion Multiplicity in Central Nucleus-Nucleus Collisions NUCLEAR REACTIONS 2H(π+, p), E ≈ 0-350 MeV; calculated σ(E). K, Cl(40Ar, xπ-), E=0.4-2 GeV; calculated pion multiplicity vs E. Intranuclear cascade model, two-nucleon pion reabsorption, off-shell effects, pion source renormalization in nuclear medium.
doi: 10.1016/0375-9474(83)90543-2
1981CU03 Nucl.Phys. A355, 477 (1981) Pion Spectra and the Geometry of Nuclear Collisions NUCLEAR REACTIONS C(C, π+), (C, π-), Ca(Ar, π+), E=1.05 GeV; F, Na(Ne, π+), (Ne, π-), E=0.4, 0.8 GeV; calculated σ(inclusive), pion multiplicity vs impact parameter, σ(π+)/σ(π-); U(Ne, p), E=393 MeV/nucleon; calculated invariant σ; deduced Δ-resonance, baryon-baryon interaction roles in collision dynamics, Coulomb distortion effects. Monte Carlo method.
doi: 10.1016/0375-9474(81)90537-6
1981CU08 Z.Phys. A301, 59 (1981) The Particle-Vibration Coupling Form Factor NUCLEAR STRUCTURE 56Ni, 90Zr, 140Ce, 208Pb; calculated isoscalar, isovector octupole vibration, L=1, Fermi transition form factors; 40Ca, 90Zr; calculated L=1, Gamow-Teller transition form factor. Particle-vibration coupling, static zero-range effective interaction.
doi: 10.1007/BF01412464
1980CU05 Phys.Lett. 91B, 177 (1980) The Particle-Vibration Coupling Form Factor NUCLEAR STRUCTURE 40,48Ca, 56Ni, 90Zr, 140Ce, 208Pb; calculated particle-vibration coupling form factor.
doi: 10.1016/0370-2693(80)90424-4
1980CU07 Phys.Rev. C21, 2342 (1980) Factorization in High-Energy Nucleus-Nucleus Fragmentation Cross Sections NUCLEAR REACTIONS 63Cu(27Al, X), (107Ag, X), E=relativistic; calculated fragmentation probability function. Abrasion-ablation model.
doi: 10.1103/PhysRevC.21.2342
1979BI01 Z.Phys. A290, 157 (1979) R.Bimbot, D.Gardes, J.Cugnon, R.da Silveira Simple Formulae for Heavy Ion Subcoulomb Transfer Probabilities. Application to One and Two-Proton Transfers in Bismuth NUCLEAR REACTIONS 209Bi(14N, 13C), (14N, 12B), E=50-70 MeV; 209Bi(16O, 15N), (16O, 14C), E=70-80 MeV; 209Bi(19F, 18O), (19F, 17N), E=70-90 MeV; 209Bi(40Ar, 39Cl), (40Ar, 38S), E=150-170 MeV; 209Bi(40Ca, 39K), (40Ca, 38Ar), E=150-180 MeV; 209Bi(57Fe, 55Mn), (56Fe, 54Cr), E=200-230 MeV; 209Bi(63Cu, 62Ni), (63Cu, 61Co), E=220-250 MeV; calculated σ(E). DWBA approach.
doi: 10.1007/BF01408110
1979CU03 Nucl.Phys. A331, 213 (1979) A Microscopic Description of Nuclear Molecules: Application to the 12C + 12C System NUCLEAR REACTIONS 12C(12C, 12C), 12C(12C, 12C'), E(cm)=10-30 MeV; calculated σ(E, θ). Coupled channels approach, oblate 12C ion interaction from Hartree-fork method.
doi: 10.1016/0375-9474(79)90310-5
1976HA58 J.Phys.(Paris) 37, 1377 (1976) Largeurs Totales en Photon et Modele de Capture de Valence NUCLEAR STRUCTURE 41,43,44,45Ca, 51,53,54,55Cr, 52V, 58Fe, 59,61Ni, 60Co; calculated Γγ for E=th (n, γ) resonances.
doi: 10.1051/jphys:0197600370120137700
1973CU01 Z.Phys. 261, 359 (1973) Effect of Ground State Correlations on the Imaginary Part of the Optical-Model Potential NUCLEAR REACTIONS 39K(p, X), E=24 MeV; measured nothing, calculated σ(absorption).
doi: 10.1007/BF01399334
1973CU02 Nucl.Phys. A208, 333 (1973) Calculation of the Imaginary Part of the Nucleon-Nucleus Optical-Model Potential NUCLEAR REACTIONS 39K(p, p'), E=14.5 MeV; calculated imaginary part of nucleon-nucleus optical-model potential.
doi: 10.1016/0375-9474(73)90380-1
1972CU01 Nucl.Phys. A186, 561 (1972) Doorway Parameters of the Resonances in Subthreshold Neutron-Induced Fission NUCLEAR REACTIONS, Fission 240Pu(n, F), E < 2.2 keV; calculated σ(E); analyzed resonance groups.
doi: 10.1016/0375-9474(72)90984-0
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