NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = J.C.David Found 41 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
2021VE06 Phys.Rev. C 104, 014615 (2021) M.Veicht, I.Kajan, J.-C.David, S.Chen, E.Strub, I.Mihalcea, D.Schumann Experiment-based determination of the excitation function for the production of 44Ti in proton-irradiated vanadium samples NUCLEAR REACTIONS V(p, X)44Ti, E=111-954 MeV; measured Eγ, Iγ using LEGe and HPGe detectors using stacked-foil technique at the Laboratoire National Saturne in Saclay and the Svedberg Laboratory in Uppsala between October 1995 and March 1996; deduced σ(E) and compared with previous experimental results, together with analysis of earlier σ(E) data for 59Co(p, X)52Fe, E=40-1500 MeV, and Fe(p, X)49Mn, E=300 MeV, consistent set of cross sections in proton-induced reactions. Comparison with Liege Intranuclear Cascade (INCL)/ABLA model calculations. Relevance to 44Ti/44gSc generator system as a future reliable tool for medical diagnosis.
doi: 10.1103/PhysRevC.104.014615
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
2016HA22 Eur.Phys.J.Plus 131, 233 (2016) B.Hammer-Rotzler, J.Neuhausen, V.Boutellier, M.Wohlmuther, L.Zanini, J.-C.David, A.Turler, D.Schumann Distribution and surface enrichment of radionuclides in lead-bismuth eutectic from spallation targets
doi: 10.1140/epjp/i2016-16233-1
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
2015DA10 Eur.Phys.J. A 51, 68 (2015) Spallation reactions: A successful interplay between modeling and applications NUCLEAR REACTIONS Fe(p, nx), E=1200, 3000 MeV; calculated σ(θ), neutron multiplicity using 17 models. Fe, Pb(p, nx), E=800, 1200, 1600 MeV; calculated neutron multiplicity. Fe(p, 3He), E=62 MeV;Ni(p, p'), E=175 MeV;Pb(p, 3He), E=63 MeV;Al(p, π-), E=2205 MeV;Pb(p, π+), E=730 MeV; calculated σ(θ, E). 56Fe(p, x), E=300 MeV/nucleon;56Fe(p, x)Ar, E=300, 1000 MeV; calculated mass distributions. Fe, Pb(p, x)24gNa, E=50-3200 MeV; calculated 24Na cumulative production. 17different models. Compared with available data.
doi: 10.1140/epja/i2015-15068-1
2015IS07 J.Radioanal.Nucl.Chem. 305, 345 (2015) Shams A.M.Issa, M.A.M.Uosif, R.Michel, J.-L.Flament, J.-C.David, S.Leray, U.Herpers The production of residual nuclides via 211, 1, 000, 1, 400 and 2, 530 MeV protons irradiation of natural uranium NUCLEAR REACTIONS U(p, X)237U/233Pa/232Pa/230Pa/141Ce/139Ce/140Ba/137Cs/136Cs/132Te/121Te/131I/127Xe/127Sb/126Sb/124Sb/122Sb/125Sn/115Cd/111Ag/110Ag/103Ru/95Zr, E=0.211, 1.0, 1.4, 2.53 GeV; measured reaction products, Eγ, Iγ; deduced σ. INCL4+ABLA code system calculations, comparison with available data.
doi: 10.1007/s10967-015-3985-9
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
2014BE29 Nucl.Data Sheets 119, 190 (2014) R.Bevilacqua, S.Pomp, K.Jansson, C.Gustavsson, M.Osterlund, V.Simutkin, M.Hayashi, S.Hirayama, Y.Naitou, Y.Watanabe, A.Hjalmarsson, A.Prokofiev, U.Tippawan, F.-R.Lecolley, N.Marie, S.Leray, J.-C.David, S.Mashnik Light-ion Production from O, Si, Fe and Bi Induced by 175 MeV Quasi-monoenergetic Neutrons NUCLEAR REACTIONS O, Si, Fe, 209Bi(n, x), E=175 MeV; measured Ep, Ip(θ), Ed, Id(θ), Eα, Iα(θ), other ejectiles using Medley spectrometer; deduced inclusive σ(θ); calculated inclusive σ(θ) using INCL.4.5-Abla07, MCNP6, CEM03.03, TALYS-1.2, PHITS.
doi: 10.1016/j.nds.2014.08.053
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
2014SC15 Nucl.Data Sheets 119, 288 (2014) Cross Sections and Excitation Functions for the Production of Long-lived Radionuclides in Nuclear Reactions of Lead and Bismuth with Protons NUCLEAR REACTIONS Pb, Bi(p, x), E=0.1-2.6 GeV. 26Al, 36Cl recalculated σ using ABLA and INCLA incorporated into INCL4.6-ABLA07.
doi: 10.1016/j.nds.2014.08.079
2014ZA09 Nucl.Data Sheets 119, 292 (2014) L.Zanini, U.Koster, J.C.David, Y.Tall, M.Andersson, K.Berg, S.Cormon, M.Fallot, Y.Foucher, H.Franberg, F.Groschel, A.Guertin, T.Kirchner, S.Leray, E.Manfrin, E.Noah, H.Ravn, T.Stora, N.Thiolliere, M.Wohlmuther Measurement of Volatile Radionuclides Production and Release Yields followed by a Post-Irradiation Analysis of a Pb/Bi Filled Ta Target at ISOLDE NUCLEAR REACTIONS Ta, Pb, Bi(p, x), E=1, 1.4 GeV; measured spallation fragments; deduced yields; calculated yields using MCNPX with INCL.4.6 and Abla07 and CEM03.
doi: 10.1016/j.nds.2014.08.080
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
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
2011LE29 J.Korean Phys.Soc. 59, 791s (2011) S.Leray, J.C.David, M.Khandaker, G.Mank, A.Mengoni, N.Otsuka, D.Filges, F.Gallmeier, A.Konobeyev, R.Michel Results from the IAEA Benchmark of Spallation Models COMPILATION Fe(p, n), E=1.2 GeV;Pb(p, n), E=63 MeV, 3 GeV; compiled calculated σ(En, θ). Fe, Pb(p, n), E=800, 1200, 1600 MeV; compiled calculated neutron multiplicity. Ta(p, d), E=1200 MeV; compiled calculated σ(θ, E). 56Fe, 208Pb(p, X), E=1000 MeV; compiled calculated yields. Pb(p, X)82Kr, E=70-3200 MeV; compiled, calculated σ.
doi: 10.3938/jkps.59.791
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
2011SC13 J.Phys.(London) G38, 065103 (2011) D.Schumann, J.Neuhausen, R.Michel, V.Alfimov, H.-A.Synal, J.-C.David, A.Wallner Excitation functions for the production of long-lived residue nuclides in the reaction natBi(p;xn, yp)Z NUCLEAR REACTIONS Bi(p, X)108Ag/10Be/26Al/129I/36Cl, E=100-2600 MeV; measured reaction products, Eγ, Iγ; deduced σ. Chemical separation, AMS measurements, comparison with spallation model INCL4 and experimental data.
doi: 10.1088/0954-3899/38/6/065103
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
2010CH49 Eur.Phys.J. A 45, 131 (2010) S.P.Chabod, J.-Ch.David, D.Ene, D.Ridikas, N.Thiolliere In-target radioactive nuclei production rates with EURISOL single-stage target configuration NUCLEAR REACTIONS C, O, Al, Si, Ta, Pb, U(p, X)Li/Be/Ne/Mg/Ar/Ni/Ga/Kr/Sn/Hg/Fr, E=0.5-2.0 GeV; calculated thick target spallation isotopic yields using MCNPX and CINDER codes. Compared INCL4/ABLA and CEM2k modules within MCNPX.
doi: 10.1140/epja/i2010-10989-7
2009EN02 Nucl.Technology 168, 513 (2009) D.Ene, J.-C.David, D.Dore, B.Rapp, D.Ridikas Preliminary Shielding Assessment of EURISOL Postaccelerator
doi: 10.13182/NT09-A9235
2008AM01 Nucl.Instrum.Methods Phys.Res. B266, 2 (2008) K.Ammon, I.Leya, B.Lavielle, E.Gilabert, J.-C.David, U.Herpers, R.Michel Cross sections for the production of helium, neon and argon isotopes by proton-induced reactions on iron and nickel NUCLEAR REACTIONS Fe, Ni(p, X)3He/4He/21Ne/22Ne/36Ar/38Ar, E < 1.6 GeV; measured cross sections and excitation functions.
doi: 10.1016/j.nimb.2007.10.024
2008LE31 Nucl.Instrum.Methods Phys.Res. B 266, 1030 (2008) I.Leya, J.-C.David, S.Leray, R.Wieler, R.Michel Production of noble gas isotopes by proton-induced reactions on bismuth NUCLEAR REACTIONS 209Bi(p, x), E=102 MeV-2.5 GeV; measured products, 3He, 21Ne, 22Ne, 36Ar, 38Ar, 78Kr, 80Kr, 81Kr, 82Kr, 83Kr, 84Kr, 85Kr, 86Kr, 124Xe, 126Xe, 128Xe, 129Xe, 130Xe, 131Xe, 132Xe, 134Xe; deduced σ, σ(E). Data were imported from EXFOR entry O1710.
doi: 10.1016/j.nimb.2008.02.032
2007RI15 Eur.Phys.J. A 32, 1 (2007) D.Ridikas, A.Barzakh, V.Blideanu, J.C.David, D.Dore, D.Fedorov, X.Ledoux, F.Moroz, V.Panteleev, R.Plukiene, A.Plukis, A.Prevost, O.Shcherbakov, A.Vorobyev Measurement of delayed neutron yields and time spectra from 1 GeV protons interacting with thick natPb targets NUCLEAR REACTIONS Pb(p, X)17N/87Br/88Br, E=1 GeV; measured delayed neutron yields and precursor production cross sections.
doi: 10.1140/epja/i2007-10368-7
2007SA19 Eur.Phys.J. A 31, 512 (2007) B.Saghai, J.-C.David, B.Julia-Diaz, T.-S.H.Lee Search for missing baryon resonances via associated strangeness photoproduction NUCLEAR REACTIONS 1H(γ, K+X), E ≈ 1.1, 1.3 GeV; analyzed hyperon production σ(θ), polarization observables.
doi: 10.1140/epja/i2006-10226-2
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
2006RI08 Nucl.Instrum.Methods Phys.Res. A562, 710 (2006) D.Ridikas, M.-L.Giacri, M.B.Chadwick, J.-C.David, D.Dore, X.Ledoux, A.Van Lauwe, W.B.Wilson Status of the photonuclear activation file: Reaction cross-sections, fission fragments and delayed neutrons NUCLEAR REACTIONS 181Ta(γ, n), (γ, 2n), E=5-25 MeV; 241Am(γ, n), (γ, 2n), (γ, F), E=5-20 MeV; analyzed σ. 235U(γ, F), E=15 MeV bremsstrahlung; analyzed fission fragment mass distribution.
doi: 10.1016/j.nima.2006.02.028
2006SC16 Nucl.Instrum.Methods Phys.Res. A562, 1057 (2006) D.Schumann, R.Michel, G.Korschinek, K.Knie, J.-C.David Excitation functions for the production of 60Fe and 53Mn in the reaction natPb(p, xp/yn)Z NUCLEAR REACTIONS Pb(p, X)60Fe/53Mn, E ≈ 100-2600 MeV; measured excitation functions. Comparison with model predictions.
doi: 10.1016/j.nima.2006.02.094
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
1996DA13 Phys.Rev. C53, 2613 (1996) J.C.David, C.Fayard, G.H.Lamot, B.Saghai Electromagnetic Production of Associated Strangeness NUCLEAR REACTIONS 1H(γ, X), E=1-2.1 GeV; calculated σ(θ), σ(E) for strangeness production. 1H(polarized γ, X), E=1.45 GeV; calculated Λ-polarization asymmetry. Feynman diagrammatic techniques, isobaric approach.
doi: 10.1103/PhysRevC.53.2613
1976RI10 Nucl.Phys. A267, 253 (1976) H.Richel, G.Albouy, G.Auger, J.C.David, J.M.Lagrange, M.Pautrat, C.Roulet, H.Sergolle, J.Vanhorenbeeck On the Decay of 203Bi RADIOACTIVITY 203Bi [from Pb(p, xn)]; measured Eγ, Iγ, I(ce), γγ-coin; deduced ICC, log ft. 203Pb deduced levels, J, π, multipolarities.
doi: 10.1016/0375-9474(76)90658-8
1975RO15 Nucl.Instrum.Methods 125, 29 (1975) C.Roulet, G.Albouy, G.Auger, M.P.Bourgarel, J.C.David, J.M.Lagrange, B.Monsanglant, M.Pautrat, H.Richel, H.Sergolle, J.Vanhorenbeeck A Device for in-Beam g-Factor Measurements for Isomeric States in the Range of a Few Hundred Nanoseconds NUCLEAR REACTIONS W(16O, 4nγ), E=97 MeV; measured γ(θ, H, t). 194,196,198Pb levels deduced T1/2, g.
doi: 10.1016/0029-554X(75)90549-2
1973AL26 Nucl.Instrum.Methods 113, 509 (1973) G.Albouy, J.C.David, J.M.Lagrange, M.Pautrat, C.Roulet, H.Sergolle, J.Vanhorenbeeck Mesures de Vies Moyennes en Ligne sur Faisceau d'Ions Lourds dans la Gamme de la Microseconde NUCLEAR REACTIONS 182,184,186W(16O, 4nγ), 188,190,192Os(12C, 4nγ); measured Eγ, γ(t). 194,196,198,200Pb deduced levels, T1/2.
doi: 10.1016/0029-554X(73)90744-1
1973PA03 Nucl.Phys. A201, 449 (1973) M.Pautrat, G.Albouy, J.C.David, J.M.Lagrange, N.Poffe, C.Roulet, H.Sergolle, J.Vanhorenbeeck, H.Abou-Leila Etude des Isotopes du Plomb de Masse 200, 198, 196 et 194 Formes par Reaction (Ions Lourds, xn) NUCLEAR REACTIONS Os(12C, 4n), W(16O, 4n), Re(14N, 5n), E=60-100 MeV;measured Eγ, Iγ, σ(E, Eγ), Iγ(θ), γγ-coin, γγ-delay. 194,196,198,200Pb deduced levels, J, π, T1/2. Enriched, natural targets.
doi: 10.1016/0375-9474(73)90314-X
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