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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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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2545.

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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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
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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.

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2266.

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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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23130.

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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2014SC15      Nucl.Data Sheets 119, 288 (2014)

D.Schumann, J.-Ch.David

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
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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
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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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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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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
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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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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1907.

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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0927.

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1591.

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1710.

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0810.

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
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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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1412.

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1411.

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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0839.

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
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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
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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
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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
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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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