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Search: Author = K.Niita

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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2486.

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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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2282.

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2129.

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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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
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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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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2079.

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
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2002IW03      J.Nucl.Sci.Technol.(Tokyo) 39, 1142 (2002)

H.Iwase, K.Niita, T.Nakamura

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1769.

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
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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
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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
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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
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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
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1997MA52      Prog.Theor.Phys.(Kyoto) 97, 579 (1997)

T.Maruyama, K.Niita

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
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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
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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
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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
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1996CH39      Phys.Rev. C54, 3302 (1996); Erratum Phys.Rev. C56, 1191 (1997)

S.Chiba, K.Niita, O.Iwamoto

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1983NI02      Nucl.Phys. A397, 141 (1983)

K.Niita, N.Takigawa

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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