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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1287.


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 Geant4¬Ěs 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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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2011PE23      Nucl.Phys. A866, 16 (2011)

S.Pedoux, J.Cugnon

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0901.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0906.


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
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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
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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
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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
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2009AO04      Nucl.Phys. A828, 52 (2009)

T.Aoust, J.Cugnon

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
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2006AO03      Phys.Rev.C 74, 064607 (2006)

Th.Aoust, J.Cugnon

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
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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
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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
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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
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2004AO06      Eur.Phys.J. A 21, 79 (2004)

Th.Aoust, J.Cugnon

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
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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
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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
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2003CU01      Eur.Phys.J. A 16, 393 (2003)

J.Cugnon, P.Henrotte

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
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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
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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
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2000CU04      Ann.Phys.(Paris) 25, 93 (2000)

J.Cugnon

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1996CU04      Ann.Phys.(Paris) 21, 537 (1996)

J.Cugnon

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
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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
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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
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1995GO11      Z.Phys. A351, 199 (1995)

P.-B.Gossiaux, J.Cugnon

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
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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
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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
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1994CU03      Yad.Fiz. 57, No 9, 1705 (1994); Phys.Atomic Nuclei 57, 1635 (1994)

J.Cugnon

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
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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
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1992CU02      Nucl.Phys. A542, 559 (1992)

J.Cugnon

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
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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
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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
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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
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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
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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
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1989CU06      Ann.Phys.(Paris) 14, 49 (1989)

J.Cugnon, J.Vandermeulen

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
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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
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1989CU10      Z.Phys. A334, 435 (1989)

J.Cugnon, C.Volant

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
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1988CU05      Nucl.Phys. A485, 271 (1988)

J.Cugnon, P.Deneye, A.Lejeune

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
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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
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1987CU01      Nucl.Phys. A462, 751 (1987)

J.Cugnon

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
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1987CU02      Z.Phys. A327, 187 (1987)

J.Cugnon

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
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1986CU03      Nucl.Phys. A452, 738 (1986)

J.Cugnon, D.L'Hote

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
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1984CU01      Phys.Lett. 134B, 392 (1984)

J.Cugnon, R.M.Lombard

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
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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
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1981CU03      Nucl.Phys. A355, 477 (1981)

J.Cugnon, S.E.Koonin

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
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1981CU08      Z.Phys. A301, 59 (1981)

J.Cugnon, O.Harouna

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
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1980CU05      Phys.Lett. 91B, 177 (1980)

J.Cugnon, O.Harouna

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
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1980CU07      Phys.Rev. C21, 2342 (1980)

J.Cugnon, R.Sartor

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
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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
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1979CU03      Nucl.Phys. A331, 213 (1979)

J.Cugnon, H.Doubre, H.Flocard

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
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1976HA58      J.Phys.(Paris) 37, 1377 (1976)

O.Harouna, J.Cugnon

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
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1973CU01      Z.Phys. 261, 359 (1973)

J.Cugnon

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
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1973CU02      Nucl.Phys. A208, 333 (1973)

J.Cugnon

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
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1972CU01      Nucl.Phys. A186, 561 (1972)

J.Cugnon

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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