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Search: Author = D.Mancusi

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2022OG06      Eur.Phys.J. A 58, 153 (2022)

T.Ogawa, O.Litaize, D.Mancusi, A.Chebboubi, O.Serot

Post fission time evolution calculation by FIFRELIN coupled with PHITS and DCHAIN

NUCLEAR REACTIONS ²³⁵U(n, F), E thermal; calculated time evolution of total and gamma decay heat, mass distribution of fission fragments. Comparison with available data, FIFRELIN-DCHAIN interface.

doi: 10.1140/epja/s10050-022-00800-z
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2019GO06      Eur.Phys.J. A 55, 11 (2019)

T.Gorbinet, O.Yordanov, J.-E.Ducret, T.Aumann, Y.Ayyad, S.Bianchin, O.Borodina, A.Boudard, C.Caesar, E.Casarejos, B.Czech, S.Hlavac, J.Klimo, N.Kurz, C.Langer, T.Le Bleis, S.Leray, J.Lukasik, D.Mancusi, P.Pawlowski, S.Pietri, C.Rappold, M.-D.Salsac, H.Simon, M.Veselsky

Study of the reaction mechanisms of ¹³⁶Xe + p and ¹³⁶Xe + ¹²C at 1 A GeV with inverse kinematics and large-acceptance detectors

NUCLEAR REACTIONS ¹³⁶Xe(p, x), (¹²C, x), E = 1 GeV/nucleon; measured fragment yield vs charge using Forward MUSIC (IH₂) and a scintillator of TOF wall; calculated, simulated element production σ, total multiplicity data using GEANT4 with intranuclear cascade code INCL++ ver 6-0, fast collision and deexcitation ABRA and three deexcitation codes ABLA07, GEMINI++ and SMM.

doi: 10.1140/epja/i2019-12683-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2530.

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(E_out), 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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2016LE07      Eur.Phys.J. A 52, 100 (2016)

J.Lerendegui-Marco, S.Lo Meo, C.Guerrero, M.A.Cortes-Giraldo, C.Massimi, J.M.Quesada, M.Barbagallo, N.Colonna, D.Mancusi, F.Mingrone, M.Sabate-Gilarte, G.Vannini, V.Vlachoudis, for the n_TOF Collaboration

Geant4 simulation of the n_TOF-EAR2 neutron beam: Characteristics and prospects

doi: 10.1140/epja/i2016-16100-8
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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.

2015LO01      Nucl.Phys. A933, 43 (2015)

S.Lo Meo, D.Mancusi, C.Massimi, G.Vannini, A.Ventura

Fission induced by nucleons at intermediate energies

NUCLEAR REACTIONS ²⁰⁸Pb, Pb, ²⁰⁹Bi, ²³²Th, ^233,235,238U, U, ²³⁶Np, ²³⁹Pu(p, F), (n, F), E=100-1000 MeV;²³⁴U(n, F), E=100-1000 MeV; calculated fission σ using INCL++ cascade model coupled with different evaporation-fission models; deduced model parameters. Compared to available data, JENDL/HE-2007.

doi: 10.1016/j.nuclphysa.2014.09.040
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2015LO12      Eur.Phys.J. A 51, 160 (2015)

S.Lo Meo, M.A.Cortes-Giraldo, C.Massimi, J.Lerendegui-Marco, M.Barbagallo, N.Colonna, C.Guerrero, D.Mancusi, F.Mingrone, J.M.Quesada, M.Sabate-Gilarte, G.Vannini, V.Vlachoudis, for the n_TOF Collaboration

GEANT4 simulations of the n_TOF spallation source and their benchmarking

doi: 10.1140/epja/i2015-15160-6
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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s 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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2014AY03      Phys.Rev. C 89, 054610 (2014)

Y.Ayyad, J.Benlliure, E.Casarejos, H.Alvarez-Pol, A.Bacquias, A.Boudard, M.Caamano, T.Enqvist, V.Fohr, A.Kelic-Heil, K.Kezzar, S.Leray, D.Mancusi, C.Paradela, D.Perez-Loureiro, R.Pleskac, J.L.Rodriguez-Sanchez, D.Tarrio

Proton-induced fission of ¹⁸¹Ta at high excitation energies

NUCLEAR REACTIONS ¹H(¹⁸¹Ta, F), E=300, 500, 800, 1000 MeV/nucleon; measured energy losses of the tantalum beam particles, and fission products at GSI facility; deduced proton-induced total fission σ(E), Mass, charge, and excitation energy distributions of prefragments, average fission lifetime, temperature dependence of dissipative and transient effects at small deformation. Comparison with previous experimental data, and model calculations using INCL+ABLA, ISABEL+ABLA, and INCL+GEMINI++ statistical model codes. Benchmarking state-of-the-art reaction codes

doi: 10.1103/PhysRevC.89.054610
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1888.

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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2013AU02      Phys.Rev. C 88, 041602 (2013)

L.Audirac, A.Obertelli, P.Doornenbal, D.Mancusi, S.Takeuchi, N.Aoi, H.Baba, S.Boissinot, A.Boudard, A.Corsi, A.Gillibert, T.Isobe, A.Jungclaus, V.Lapoux, J.Lee, S.Leray, K.Matsui, M.Matsushita, T.Motobayashi, D.Nishimura, S.Ota, E.C.Pollacco, G.Potel, H.Sakurai, C.Santamaria, Y.Shiga, D.Sohler, D.Steppenbeck, R.Taniuchi, H.Wang

Evaporation-cost dependence in heavy-ion fragmentation

NUCLEAR REACTIONS ¹H, ¹²C(¹⁰⁴Sn, X)¹⁰⁰Sn/¹⁰¹Sn/¹⁰²Sn/¹⁰³Sn/¹⁰⁴Sn, E=155 MeV/nucleon; ¹H, ¹²C(¹¹²Sn, X)¹⁰⁵Sn/¹⁰⁶Sn/¹⁰⁷Sn/¹⁰⁸Sn/¹⁰⁹Sn/¹¹⁰Sn/¹¹¹Sn/¹¹²Sn/, E=173 MeV/nucleon, [secondary ^104,112Sn beams from ⁹Be(¹²⁴Xe, X) primary reaction]; measured particle spectra, TOF, σ for multi-nucleon removal using BigRIPS and ZDS spectrometers at RIBF-RIKEN facility. Comparison with previous experimental data, and with cascade and deexcitation model (INCL-ABLA) calculations.

doi: 10.1103/PhysRevC.88.041602
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2444.

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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2013CI02      Acta Phys.Pol. B44, 611 (2013)

M.Ciemala, M.Kmiecik, M.Krzysiek, A.Maj, K.Mazurek, R.Charity, D.Mancusi

Gamma-decay of the GDR in the GEMINI++ Code

NUCLEAR REACTIONS ⁴⁰Ca(⁴⁸Ti, X)⁸⁸Mo, E=300, 450, 600 MeV; calculated yields, experimental γ-spectra, GDR parameters. GEMINI++ with Monte Carlo code cascade.

doi: 10.5506/APhysPolB.44.611
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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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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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0904.

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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0905.

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.

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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2009MA04      Phys.Rev. C 79, 014614 (2009)

D.Mancusi, K.Niita, T.Maruyama, L.Sihver

Stability of nuclei in peripheral collisions in the JAERI quantum molecular dynamics model

NUCLEAR REACTIONS ⁴⁰Ca(⁴⁰Ca, ⁴⁰Ca), E=1 GeV/nucleon; ⁵⁶Fe(p, xn), E=113 MeV; ²⁰⁸Pb(p, xn), E=3 GeV; Al(⁵⁶Fe, X), E=1 GeV; calculated σ(θ). R-JAERI quantum molecular dynamics model. Comparisons with JAERI quantum molecular dynamics model and experimental data.

doi: 10.1103/PhysRevC.79.014614
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2008ZE02      Phys.Rev. C 77, 034605 (2008)

C.Zeitlin, S.Guetersloh, L.Heilbronn, J.Miller, A.Fukumura, Y.Iwata, T.Murakami, L.Sihver, D.Mancusi

Fragmentation cross sections of medium-energy ³⁵Cl, ⁴⁰Ar, and ⁴⁸Ti beams on elemental targets

NUCLEAR REACTIONS H, C, Al, Cu, Sn, Pb(³⁵Cl, X), E=290, 400, 650 MeV/nucleon; H, C, Al, Cu, Sn, Pb(⁴⁰Ar, X), E=650, 1000 MeV/nucleon; H, C, Al, Cu, Sn, Pb(⁴⁸Ti, X), E=1000 MeV/nucleon; measured charge changing cross sections, fragment production cross sections.

doi: 10.1103/PhysRevC.77.034605
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1609.

2007LA29      Nucl.Phys. A791, 434 (2007)

C.La Tessa, L.Sihver, C.Zeitlin, J.Miller, S.Guetersloh, L.Heilbronn, D.Mancusi, Y.Iwata, T.Murakami

Test of weak and strong factorization in nucleus-nucleus collisions at several hundred MeV/nucleon

NUCLEAR REACTIONS H, C, Al, Cu, Sn, Pb(⁴⁰Ar, X), E=400 MeV/nucleon; C, Al, Cu, Sn, Pb(¹²C, X), (²⁰Ne, X), (²⁸Si, X), E=290, 400 MeV/nucleon; measured partial and total charge changing cross sections. Deduced factorization parameters.

doi: 10.1016/j.nuclphysa.2007.04.016
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2056.

2007LA30      Nucl.Phys. A791, 451 (2007)

C.La Tessa, L.Sihver, D.Mancusi, C.Zeitlin, J.Miller, S.Guetersloh, L.Heilbronn

Weak and strong factorization properties in nucleus-nucleus collisions in the energy region 290-2100 MeV/nucleon

doi: 10.1016/j.nuclphysa.2007.04.025
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2007MA01      Nucl.Instrum.Methods Phys.Res. B254, 30 (2007)

D.Mancusi, L.Sihver, K.Gustafsson, C.La Tessa, S.B.Guetersloh, C.J.Zeitlin, J.Miller, L.H.Heilbronn, K.Niita, T.Sato, H.Nakashima, T.Murakami, Y.Iwata

PHITS - benchmark of partial charge-changing cross sections for intermediate-mass systems

NUCLEAR REACTIONS H, C, Al, Cu, Sn, Pb(⁴⁰Ar, X), E=400 MeV/nucleon; calculated partial charge-changing σ.

doi: 10.1016/j.nimb.2006.10.070
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