NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = K.Niita Found 42 matches. 2018OG02 Phys.Rev. C 98, 024611 (2018) T.Ogawa, T.Sato, S.Hashimoto, K.Niita Cluster formation in relativistic nucleus-nucleus collisions NUCLEAR REACTIONS 12C(12C, 12C'), (56Fe, 56Fe'), (208Pb, 208Pb'), 40Ca(40Ca, 40Ca'), 107Ag(107Ag, 107Ag'), E=4, 158 GeV/nucleon; calculated inelastic σ(E). 197Au(C, X), E=10.6 GeV/nucleon; 28Si(Cu, X), E=14.5 GeV/nucleon; 208Pb(C, X), (Cu, X), E=158 GeV, nucleon; calculated charge distribution of reaction products. 28Si(Al, X), (Au, X), E=high; calculated transverse mass distributions of p, π+, π-, d, K-, and K+ in central and peripheral collisions. 208Pb(208Pb, X), E=20, 40, 80, 158 GeV/nucleon; calculated transverse mass distributions of p, p-bar, π-, K-, and K+ in central collisions. Calculations performed with JAMQMD algorithm. Comparison with experimental values.
doi: 10.1103/PhysRevC.98.024611
2015OG02 Phys.Rev. C 92, 024614 (2015); Pub.Note Phys.Rev. C 92, 029904 (2015) T.Ogawa, T.Sato, S.Hashimoto, D.Satoh, S.Tsuda, K.Niita Energy-dependent fragmentation cross sections of relativistic 12C NUCLEAR REACTIONS C(12C, X)11B/10B/10Be/9Be/7Be/8Li/7Li/6Li, E=100-400 MeV/nucleon; measured reaction products, time-of-flight, angular distribution of fragments, fragment production σ(E), double-differential neutron production cross sections at Heavy Ion Medical Accelerator in Chiba. Benchmarked theoretical nuclear reaction models implemented in the Particle and Heavy Ion Transport code System (PHITS) by combining JAERI quantum molecular dynamics nucleus-nucleus reaction model (JQMD) and the statistical decay Generalized Evaporation Model (GEM). Comparison with other theoretical calculations.
doi: 10.1103/PhysRevC.92.024614
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
2014HA21 Nucl.Data Sheets 118, 258 (2014) S.Hashimoto, O.Iwamoto, Y.Iwamoto, T.Sato, K.Niita New Approach for Nuclear Reaction Model in the Combination of Intra-nuclear Cascade and DWBA NUCLEAR REACTIONS 7Li(p, n), E=45 MeV;9Be(p, n), E=50 MeV; calculated σ(θ). Compared with data. 7Li(p, xn), E=39, 43 MeV;9Be(p, xn), E-35, 39 MeV;calculated σ(En, θ=00). Compared with data and other calculations. Intranuclear cascade plus DWBA.
doi: 10.1016/j.nds.2014.04.052
2011KA42 J.Korean Phys.Soc. 59, 2063s (2011) Y.Kasugai, N.Matsuda, Y.Iwamoto, Y.Sakamoto, H.Nakashima, H.Matsumura, N.Kinoshita, H.Iwase, T.Sanami, M.Hagiwara, H.Hirayama, H.Yashima, N.Sigyo, H.Arakawa, K.Ishibashi, N.Mokhov, A.Leveling, D.Boehnlein, K.Vaziri, G.Lauten, S.Wayne, V.Cupps, B.Kershisnik, S.Benesch, T.Nakamura, K.Oishi, K.Niita Shielding Experiments under JASMIN Collaboration at Fermilab (I) Overview of the Research Activities
doi: 10.3938/jkps.59.2063
2011MA77 J.Korean Phys.Soc. 59, 2055s (2011) N.Matsuda, Y.Kasugai, Y.Sakamoto, H.Nakashima, H.Matsumura, H.Iwase, N.Kinoshita, H.Hirayama, H.Yashima, N.Mokhov, A.Leveling, D.Boehnlein, K.Vazili, L.Gary, S.Wayne, K.Oishi, T.Nakamura, K.Ishibashi, K.Niita Shielding Experiments under JASMIN Collaboration at Fermilab (IV) Measurement and Analyses of High-Energy Neutron Spectra in the Anti-Proton Target Station
doi: 10.3938/jkps.59.2055
2011NI15 J.Korean Phys.Soc. 59, 827s (2011) K.Niita, Y.Iwamoto, T.Sato, N.Matsuda, Y.Sakamoto, H.Nakashima, H.Iwase, L.Sihver Event Generator Models in the Particle and Heavy Ion Transport Code System; PHITS NUCLEAR REACTIONS C(n, n'), (n, γ)E=15 MeV; calculated σ(En, θ). C(n, X), E=0-20 MeV; calculated Kerma factor, energy of produced photons. 56Fe(n, X), E=1.E-6-20 MeV; calculated displacement σ. Pb(n, n'), E=3 GeV; calculated σ(E, θ). Si(n, X), E=19 MeV; calculated deposit energy distribution. Quantum Molecular Dynamics, PHITS code. Compared to ENDF data.
doi: 10.3938/jkps.59.827
2011NI17 J.Korean Phys.Soc. 59, 1640s (2011) K.Niita, H.Iwase, Y.Iwamoto, T.Sato, N.Matsuda, Y.Sakamoto, H.Nakashima, L.Sihver Applicability of the PHITS Code to Heavy Ion Accelerator Facilities NUCLEAR REACTIONS 208Pb(12C, n), E=400 MeV/nucleon; calculated σ(En, θ) using JQMD (JAERI Quantum Molecular Dynamics) incorporated into PHITS code. Compared with data.
doi: 10.3938/jkps.59.1640
2011WA32 J.Korean Phys.Soc. 59, 1040s (2011) Y.Watanabe, K.Kosako, S.Kunieda, S.Chiba, R.Fujimoto, H.Harada, M.Kawai, F.Maekawa, T.Murata, H.Nakashima, K.Niita, N.Shigyo, S.Shimakawa, N.Yamano, T.Fukahori Status of JENDL High Energy File COMPILATION Z=1-95(n, X), (p, X), E=0-3 GeV; compiled, evaluated σ, dσ.
doi: 10.3938/jkps.59.1040
2010IW04 Nucl.Instrum.Methods Phys.Res. A 620, 484 (2010) Y.Iwamoto, D.Satoh, M.Hagiwara, H.Yashima, Y.Nakane, A.Tamii, H.Iwase, A.Endo, H.Nakashima, Y.Sakamoto, K.Hatanaka, K.Niita Measurements and Monte Carlo calculations of neutron production cross-sections at 180-degree for the 140MeV proton incident reactions on carbon, iron, and gold NUCLEAR REACTIONS C(p, x), Fe(p, x), 197Au(p, x), E=140 MeV; measured products, Eν, Iν; deduced σ(θ, E). Data were imported from EXFOR entry E2282.
doi: 10.1016/j.nima.2010.03.101
2009IW07 Nucl.Instrum.Methods Phys.Res. A 598, 687 (2009) Y.Iwamoto, Y.Sakamoto, N.Matsuda, Y.Nakane, K.Ochiai, H.Kaneko, K.Niita, T.Shibata, H.Nakashima Measurements of double-differential neutron-production cross-sections for the 9Be(p, xn) and 9Be(d, xn) reactions at 10 MeV NUCLEAR REACTIONS 9Be(d, x), 9Be(p, x), E=10 MeV; measured products, Eν, Iν; deduced σ(θ, E). Data were imported from EXFOR entry E2129.
doi: 10.1016/j.nima.2008.10.019
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
2009NA20 Nucl.Technology 168, 482 (2009) H.Nakashima, Y.Sakamoto, Y.Iwamoto, N.Matsuda, Y.Kasugai, Y.Nakane, F.Masukawa, N.V.Mokhov, A.F.Leveling, D.J.Boehnlein, K.Vaziri, T.Sanami, H.Matsumura, M.Hagiwara, H.Iwase, N.Kinoshita, H.Hirayama, K.Oishi, T.Nakamura, H.Arakawa, N.Shigyo, K.Ishibashi, H.Yashima, N.Nakao, K.Niita Experimental Studies of Shielding and Irradiation Effects at High-Energy Accelerator Facilities
doi: 10.13182/NT09-A9229
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
2007SA56 Nucl.Instrum.Methods Phys.Res. A583, 507 (2007) D.Satoh, T.Kurosawa, T.Sato, A.Endo, M.Takada, H.Iwase, T.Nakamura, K.Niita Reevaluation of secondary neutron spectra from thick targets upon heavy-ion bombardment NUCLEAR REACTIONS C, Al, Cu, Pb(C, X), E=400 MeV/nucleon; C, Cu(Si, X), E=800 MeV/nucleon; C, Al, Cu, Pb(Fe, X), E=400 MeV/nucleon; C, Al, Cu, Pb(Xe, X), E=400 MeV/nucleon; analyzed experimental data of secondary neutron spectra, comparisons with calculations using Monte-Carlo heavy-ion transport code PHITS.
doi: 10.1016/j.nima.2007-09-023
2002HI14 Nucl.Phys. A707, 193 (2002) Y.Hirata, A.Ohnishi, Y.Nara, T.Kido, T.Maruyama, N.Otuka, K.Niita, H.Takada, S.Chiba Sideward Peak of Intermediate Mass Fragments in High Energy Proton Induced Reactions NUCLEAR REACTIONS 197Au(p, X), E=12 GeV; calculated fragments energy, angle, and mass distributions; deduced intermediate mass fragment formation and sideward enhancement mechanism features. Transport and nonequilibrated percolation models.
doi: 10.1016/S0375-9474(02)00747-9
2002IW03 J.Nucl.Sci.Technol.(Tokyo) 39, 1142 (2002) Development of General-Purpose Particle and Heavy Ion Transport Monte Carlo Code NUCLEAR REACTIONS 208Pb(p, nX), E=3 GeV; 27Al(p, nX), E=256 MeV; C(Ne, nX), Cu(C, nX), E=135 MeV/nucleon; C(C, nX), E=290 MeV/nucleon; C, Al, Cu, Pb(C, nX), E=100, 400 MeV/nucleon; C, Al, Cu, Pb(Fe, nX), E=400 MeV/nucleon; calculated neutron spectra, σ(E, θ). High-energy transport code, comparison with data.
doi: 10.1080/18811248.2002.9715305
2001CH06 Phys.Rev. C63, 024602 (2001) S.Chikazumi, T.Maruyama, S.Chiba, K.Niita, A.Iwamoto Quantum Molecular Dynamics Simulation of Expanding Nuclear Matter and Nuclear Multifragmentation
doi: 10.1103/PhysRevC.63.024602
2001IW05 Phys.Rev. C64, 054609 (2001) Y.Iwata, T.Murakami, H.Sato, H.Iwase, T.Nakamura, T.Kurosawa, L.Heilbronn, R.M.Ronningen, K.Ieki, Y.Tozawa, K.Niita Double-Differential Cross Sections for the Neutron Production from Heavy-Ion Reactions at Energies E/A = 290-600 MeV NUCLEAR REACTIONS C, Cu, Pb(C, nX), (Ne, nX), (Ar, nX), E=290-600 MeV/nucleon; measured neutron spectra, σ(En, θ), integrated σ; deduced equilibrium and pre-equilibrium components, related reaction mechanism features. Comparison with moving-source model predictions.
doi: 10.1103/PhysRevC.64.054609
2000CH05 Phys.Lett. 476B, 273 (2000) S.Chikazumi, T.Maruyama, K.Niita, A.Iwamoto QMD Simulation of Expanding Nuclear Matter
doi: 10.1016/S0370-2693(00)00161-1
2000KI10 Nucl.Phys. A663-664, 877c (2000) T.Kido, T.Maruyama, K.Niita, S.Chiba MD Simulation Study for Nuclear Matter
doi: 10.1016/S0375-9474(99)00736-8
2000NA03 Phys.Rev. C61, 024901 (2000) Y.Nara, N.Otuka, A.Ohnishi, K.Niita, S.Chiba Relativistic Nuclear Collisions at 10A GeV Energies from p + Be to Au + Au with the Hadronic Cascade Model NUCLEAR REACTIONS 1n, 1H(p, X), (π+, X), (π-, X), (K+, X), (K-, X), E(cm) ≈ 1-3 GeV; analyzed total, elastic, pion and hyperon production σ. Be(p, X), 27Al, Cu, 197Au(p, X), (Si, X), E at 14.6 GeV/c; calculated proton, pion, kaon invariant cross sections, transverse momenta; 197Au(197Au, X), E at 11.6 GeV/c; calculated protons, pions rapidity, transverse mass; deduced mass dependence of collision dynamics. Hadronic cascade model, comparisons with data.
doi: 10.1103/PhysRevC.61.024901
1999MB10 Nucl.Phys. (Supplement) A654, 908c (1999) T.Maruyama, K.Niita, K.Oyamatsu, T.Maruyama, S.Chiba, A.Iwamoto Nuclear Matter Structure Studied with Quantum Molecular Dynamics
doi: 10.1016/S0375-9474(00)88570-X
1998MA04 Phys.Rev. C57, 655 (1998) T.Maruyama, K.Niita, K.Oyamatsu, T.Maruyama, S.Chiba, A.Iwamoto Quantum Molecular Dynamics Approach to the Nuclear Matter Below the Saturation Density
doi: 10.1103/PhysRevC.57.655
1997MA52 Prog.Theor.Phys.(Kyoto) 97, 579 (1997) Multifragmentation Through Exotic Shape Nuclei in α(5 GeV/u) + Au Collisions NUCLEAR REACTIONS 197Au(α, X), E=5 GeV/nucleon; calculated light, intermediate fragments σ(θ); deduced annular intermediate shape. Quantum molecular dynamics approach.
doi: 10.1143/PTP.97.579
1997MA71 Prog.Theor.Phys.(Kyoto) 98, 87 (1997) T.Maruyama, K.Niita, T.Maruyama, A.Iwamoto On the IMF Multiplicity in Au + Au Reactions NUCLEAR REACTIONS 197Au(197Au, X), E=100, 250, 400 MeV/nucleon; calculated intermediate mass fragment multiplicity distributions. Quantum molecular dynamics approach, evaporation model. Comparison with data.
doi: 10.1143/PTP.98.87
1996CH10 Phys.Rev. C53, 1824 (1996) S.Chiba, M.B.Chadwick, K.Niita, T.Maruyama, T.Maruyama, A.Iwamoto Nucleon-Induced Preequilibrium Reactions in Terms of the Quantum Molecular Dynamics NUCLEAR REACTIONS 58Ni(p, xp), E=120, 200 MeV; 90Zr(p, xp), (p, xn), E=160 MeV; 27Al(p, xp), (p, xn), E=90 MeV; 90Zr(p, xn), E=160 MeV; analyzed σ(θ, E(nucleon)); deduced multiple pre-equilibrium particle emission role. Quantum molecular dynamics approach.
doi: 10.1103/PhysRevC.53.1824
1996CH15 Phys.Rev. C54, 285 (1996) S.Chiba, O.Iwamoto, T.Fukahori, K.Niita, T.Maruyama, T.Maruyama, A.Iwamoto Analysis of Proton-Induced Fragment Production Cross Sections by the Quantum Molecular Dynamics Plus Statistical Decay Model NUCLEAR REACTIONS, ICPND 56Fe(p, n), (p, 3n2p), (p, 3n3p), (p, 5n4p), (p, 3n6p), (p, 4n6p), (p, 5n6p), (p, 6n8p), E=threshold-5 GeV; 27Al(p, n3p), (p, 3n3p), (p, 5n5p), (p, 11n10p), E ≤ 6 GeV; analyzed residuals production σ(E). Quantum molecular dynamics plus statistical decay models.
doi: 10.1103/PhysRevC.54.285
1996CH39 Phys.Rev. C54, 3302 (1996); Erratum Phys.Rev. C56, 1191 (1997) Time Scale of the Preequilibrium Process in Intermediate-Energy Nucleon-Induced Reactions NUCLEAR REACTIONS 56Fe(p, X), E=0.1-1.5 GeV; calculated two colliding nucleons average kinetic energy over average time bin of 5fm/c; deduced thermal equilibrium attainment time scale related features. Quantum molecular dynamics approach.
doi: 10.1103/PhysRevC.54.3302
1996MA02 Phys.Rev. C53, 297 (1996) T.Maruyama, K.Niita, A.Iwamoto Extension of Quantum Molecular Dynamics and Its Application to Heavy-Ion Collisions NUCLEAR STRUCTURE 12C, 93Nb, 197Au; calculated density distribution, Gaussian widths. NUCLEAR REACTIONS, ICPND 12C(12C, X), E=29 MeV/nucleon; 27Al(40Ar, X), E=44 MeV/nucleon; calculated σ vs fragment mass. 16O(16O, X), E ≤ 200 MeV; calculated fusion σ(E). Extended quantum molecular dynamics method.
doi: 10.1103/PhysRevC.53.297
1995CH49 Phys.Rev. C52, 2800 (1995) M.B.Chadwick, S.Chiba, K.Niita, T.Maruyama, A.Iwamoto Quantum Molecular Dynamics and Multistep-Direct Analyses of Multiple Preequilibrium Emission NUCLEAR REACTIONS 90Zr(p, xp), E=160 MeV; calculated angle-integrated σ for primary, multiple preequilibrium emission. Quantum molecular dynamics, multi-step direct analysis.
doi: 10.1103/PhysRevC.52.2800
1995MA72 Phys.Lett. 358B, 34 (1995) T.Maruyama, T.Maruyama, K.Niita Relativistic Effects in Simulations of the Fragmentation Process with the Microscopic Framework NUCLEAR REACTIONS Ca(Ca, X), E=1.05 GeV/nucleon; calculated p-, α-multiplicities vs impact parameter, fragment production σ vs mass, relativistic effects. Statistical decay model, Lorentz covariant RQMD, noncovariant QMD approaches.
doi: 10.1016/0370-2693(95)00976-R
1995NI12 Phys.Rev. C52, 2620 (1995) K.Niita, S.Chiba, T.Maruyama, T.Maruyama, H.Takada, T.Fukahori, Y.Nakahara, A.Iwamoto Analysis of the (N, xN') Reactions by Quantum Molecular Dynamics Plus Statistical Decay Model NUCLEAR REACTIONS 1n, 1H(p, X), E=0.5-3 GeV; calculated elastic, inelastic, total, pion production σ(E). 27Al(p, xp), (p, xπ-), E=3.17 GeV; 56Fe(p, xn), E=113, 597 MeV; 208Pb(p, xn), E=0.256-3 GeV; calculated σ(θ, E(particle)). Quantum molecular dynamics model.
doi: 10.1103/PhysRevC.52.2620
1991BA13 Phys.Lett. 256B, 331 (1991) G.Batko, W.Cassing, U.Mosel, K.Niita, Gy.Wolf Antiproton Production in p-Nucleus and Nucleus-Nucleus Collisions NUCLEAR REACTIONS 28Si(28Si, X), E=2.1 GeV/nucleon; 63Cu(p, X), E=4-6.1 GeV; calculated p-bar production invariant σ. Vlasov-Uehling-Uhlenbeck transport theory.
doi: 10.1016/0370-2693(91)91771-M
1991HA20 Nucl.Phys. A535, 120 (1991) S.Hannuschke, W.Cassing, U.Mosel, K.Niita Microscopic Analysis of Deeply Inelastic Heavy-Ion Collisions NUCLEAR REACTIONS 100Mo(100Mo, X), E=23.7 MeV/nucleon; calculated sticking limit in transfer reaction, fragment mass fluctuation vs total kinetic energy loss. 92Mo(92Mo, X), E=19.5 MeV/nucleon; calculated γ-production probability vs total kinetic energy loss. Microscopic transport approach.
doi: 10.1016/0375-9474(91)90519-C
1990CA15 Phys.Lett. 238B, 25 (1990) W.Cassing, G.Batko, U.Mosel, K.Niita, O.Schult, Gy.Wolf Subthereshold K+-Production in Proton-Nucleus Reactions NUCLEAR REACTIONS U, 12C(p, X), E ≈ 1 GeV; calculated K+, π0 differential production probability.
doi: 10.1016/0370-2693(90)92094-Y
1990GO24 Phys.Rev. C42, 2125 (1990) M.Gonin, L.Cooke, K.Hagel, Y.Lou, J.B.Natowitz, R.P.Schmitt, S.Shlomo, B.Srivastava, W.Turmel, H.Utsunomiya, R.Wada, G.Nardelli, G.Nebbia, G.Viesti, R.Zanon, B.Fornal, G.Prete, K.Niita, S.Hannuschke, P.Gonthier, B.Wilkins Dynamical Effects on the De-Excitation of Hot Nuclei with A ≈ 160 NUCLEAR REACTIONS 100Mo(60Ni, F), E=550, 655 MeV; measured charged particle, neutron muliplicities, evaporation residues velocities, fission fragments energies; deduced hot nuclear properties.
doi: 10.1103/PhysRevC.42.2125
1988KO09 Phys.Lett. 206B, 395 (1988) V.Koch, U.Mosel, T.Reitz, C.Jung, K.Niita Influence of the Momentum Dependence of Nuclear Interactions on Heavy-Ion Potentials NUCLEAR REACTIONS 16O(16O, 16O), E=100 MeV/nucleon; calculated potential vs internuclear distance.
doi: 10.1016/0370-2693(88)91598-5
1988NI03 Nucl.Phys. A482, 525c (1988) K.Niita, A.L.de Paoli, W.Bauer, T.S.Biro, W.Cassing, U.Mosel Hard Photons from Heavy-Ion Collisions NUCLEAR REACTIONS 16O(16O, Xγ), E=80 MeV/nucleon; 12C(12C, Xγ), E=84 MeV/nucleon; 12C(14N, Xγ), E=40, 30, 20 MeV/nucleon; calculated σ(θ, Eγ). 40Ca(40Ca, πX), E ≈ 20-120 MeV/nucleon; calculated pion production σ(E).
doi: 10.1016/0375-9474(88)90608-2
1987BI20 Nucl.Phys. A475, 579 (1987) T.S.Biro, K.Niita, A.L.De Paoli, W.Bauer, W.Cassing, U.Mosel Microscopic Theory of Photon Production in Proton-Nucleus and Nucleus-Nucleus Collisions NUCLEAR REACTIONS 27Al, C, 2H(p, Xγ), E=140 MeV; calculated σ(Eγ). 12C(12C, Xγ), E=84 MeV/nucleon; 12C(14N, Xγ), E=20, 30, 40 MeV/nucleon; calculated σ(θγ, Eγ). Microscopic model.
doi: 10.1016/0375-9474(87)90080-7
1984NI05 Z.Phys. A316, 309 (1984) Pre-Equilibrium Light Particle Emission in Heavy Ion Induced Reactions NUCLEAR REACTIONS 93Nb(14N, pX), E=132, 208 MeV; 181Ta(14N, pX), E=115 MeV; 27Al, 197Au(16O, pX), E=140, 215, 310 MeV; 90Zr(16O, pX), E=215, 310 MeV; 93Nb(α, pX), E=30.5, 42.55 MeV; calculated σ(θ), σ(θ, Ep), σ(θ, Eα). Preequilibrium emission model.
doi: 10.1007/BF01439903
1983NI02 Nucl.Phys. A397, 141 (1983) Quasi-Linear Response Theory of Statistical Heavy-Ion Collisions (II). Analysis of the friction tensor and the energy transport NUCLEAR REACTIONS 232Th(40Ar, X), E=388 MeV; 209Bi(136Xe, X), E=1130 MeV; calculated light fragment mean trajectories, σ(fragment θ, E). Quasilinear response theory, deep inelastic collisions.
doi: 10.1016/0375-9474(83)90082-9
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