NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.W.Norbury Found 29 matches. 2023RA13 Nucl.Instrum.Methods Phys.Res. B542, 87 (2023) H.N.Ratliff, N.A.McGirl, M.R.Beach, L.A.Castellanos, M.S.Clowdsley, L.H.Heilbronn, C.LaTessa, J.W.Norbury, A.Rusek, M.Sivertz, A.P.Srikrishna, H.-C.Wang, C.Zeitlin Double-differential primary target neutron yields from dual-thick-target proton and heavy ion accelerator experiments NUCLEAR REACTIONS 27Al, C, H(Si, X), (C, X)1NN, E=400 MeV/nucleon; measured reaction products, En, In; deduced yields, σ(θ, E). The NASA Space Radiation Laboratory.
doi: 10.1016/j.nimb.2023.06.001
2021LU10 New Journal of Physics 23, 101201 (2021) F.Luoni, F.Horst, C.A.Reidel, A.Quarz, L.Bagnale, L.Sihver, U.Weber, R.B.Norman, W.de Wet, M.Giraudo, G.Santin, J.W.Norbury, M.Durante Total nuclear reaction cross-section database for radiation protection in space and heavy-ion therapy applications NUCLEAR REACTIONS 4He, 7Li, 12C, 28Si, 91Zr, 119Sn, 207Pb, 27Al, 64Cu, 107Ag, 238U(α, X), (12C, X), (56Fe, X), E<100 GeV/nucleon; analyzed available data; deduced σ, database for dose calculations. GSI-ESA-NASA collaboration.
doi: 10.1088/1367-2630/ac27e1
2018NO02 Nucl.Instrum.Methods Phys.Res. B418, 13 (2018) J.W.Norbury, N.Sobolevsky, C.M.Werneth SHIELD and HZETRN comparisons of pion production cross sections NUCLEAR REACTIONS 64Cu(p, π+), 27Al(α, π+), (20Ne, π+), 40Ar(40Ca, π+), 139La(139La, π-), 12C, 9Be(p, π-), (12C, π-), E<20 GeV; analyzed available data; deduced transport σ using HZETRN and SHIELD codes.
doi: 10.1016/j.nimb.2017.12.009
2014WE12 Phys.Rev. C 90, 064905 (2014) C.M.Werneth, K.M.Maung, W.P.Ford, J.W.Norbury, M.D.Vera Elastic differential cross sections for space radiation applications
doi: 10.1103/PhysRevC.90.064905
2012NO04 Radiat.Meas. 47, 315 (2012) J.W.Norbury, J.Miller, A.M.Adamczyk, L.H.Heilbronn, L.W.Townsend, S.R.Blattnig, R.B.Norman, S.B.Guetersloh, C.J.Zeitlin Nuclear data for space radiation COMPILATION Z<100; compiled elemental and isotopic σ, σ(θ), σ(θ, E).
doi: 10.1016/j.radmeas.2012.03.004
2012NO12 J.Phys.:Conf.Ser. 381, 012117 (2012) Nuclear physics and space radiation NUCLEAR REACTIONS Z≈4-100(α, p), (α, d), (α, t), (α, 3He), (α, α), E=0-280MeV/nucleon, 280 MeV/nucleon-3 GeV/nucleon; measured reaction products; deduced σ(E), σ(θ).
doi: 10.1088/1742-6596/381/1/012117
2009NO04 Phys.Rev. C 79, 037901 (2009); Erratum Phys.Rev. C 83, 059903 (2011) Pion cross section parametrizations for intermediate energy, nucleus-nucleus collisions
doi: 10.1103/PhysRevC.79.037901
2007NO01 J.Phys.(London) G34, 115 (2007) J.W.Norbury, L.W.Townsend, R.B.Norman Threshold meson production and cosmic ray transport NUCLEAR REACTIONS 1H(p, π0X), E=290-11500 MeV; 1H(p, K+X), E=1.58-50 GeV; C(C, π0X), E=60-11500 MeV/nucleon; Ni(Ni, K+X), E=0.8-50 MeV/nucleon; analyzed pion and kaon production σ. Implications for cosmic ray transport discussed.
doi: 10.1088/0954-3899/34/1/007
2007NO03 Nucl.Instrum.Methods Phys.Res. B254, 187 (2007) Parameterized total cross sections for pion production in nuclear collisions NUCLEAR REACTIONS F, Na, Cu, Pb(Ne, π+X), (Ne, π-X), K, Cl, Pb(Ar, π+X), (Ar, π-X), C, Pb(C, π-X), Ca(Ar, π0X), Zr(Kr, π0X), Au(Au, π0X), E ≈ 0.2-2.5 GeV/nucleon; C, F, Na, K, Cl, Cu, Pb(p, π-X), E ≈ 0.2-2.5 GeV; calculated pion production σ. Comparison with data.
doi: 10.1016/j.nimb.2006.11.054
2006NO06 J.Phys.(London) G32, B31 (2006) Pair production from nuclear collisions and cosmic ray transport NUCLEAR REACTIONS 12C, 27Al, 56Fe, 197Au(12C, X), (28Si, X), (56Fe, X), E=3, 5, 10, 50 GeV/nucleon; calculated electron-positron pair production σ. Application to cosmic ray transport codes discussed.
doi: 10.1088/0954-3899/32/9/B01
2000AH07 Phys.Rev. D62, 116001 (2000) S.C.Ahern, J.W.Norbury, W.J.Poyser Graviton Production in Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS 40Ca(40Ca, X), 208Pb(208Pb, X), E=high; calculated graviton production σ. Semiclassical Weizsacker-Williams method.
doi: 10.1103/PhysRevD.62.116001
2000BL18 Phys.Rev. D62, 094030 (2000) S.R.Blattnig, S.R.Swaminathan, A.T.Kruger, M.Ngom, J.W.Norbury Parametrizations of Inclusive Cross Sections for Pion Production in Proton-Proton Collisions NUCLEAR REACTIONS 1H(p, π0X), (p, π+X), (p, π-X), E(cm)=7-63 GeV; analyzed pion production σ; deduced parameters.
doi: 10.1103/PhysRevD.62.094030
1999TO06 Nucl.Instrum.Methods Phys.Res. B149, 401 (1999) L.W.Townsend, C.R.Ramsey, R.K.Tripathi, F.A.Cucinotta, J.W.Norbury Optical Model Methods of Predicting Nuclide Production Cross Sections from Heavy Ion Fragmentation NUCLEAR REACTIONS C(40Ar, X), E=1.65 GeV/nucleon; H(36Ar, X), E=765 MeV/nucleon; calculated isotope production σ. H, C, 27Al, Cu, Pb(56Fe, X), E=1.05 GeV/nucleon; C(137La, X), E=1.2 GeV/nucleon; calculated element production σ. Optical potential abrasion-ablation-FSI fragmentation model. Comparisons with data.
doi: 10.1016/S0168-583X(98)00957-4
1998NO02 Phys.Rev. C57, 1525 (1998) Heavy Ion Beam Lifetimes at Relativistic and Ultrarelativistic Colliders NUCLEAR REACTIONS U(U, X), E=high; calculated Coulomb dissociation, fission σ; deduced beam lifetime related features. Weizsacker-Williams formula.
doi: 10.1103/PhysRevC.57.1525
1996MA06 J.Phys.(London) G22, 315 (1996) K.M.Maung, J.W.Norbury, D.E.Kahana Proportionally Off-Mass-Shell Equation for Unequal Mass Systems
doi: 10.1088/0954-3899/22/3/005
1995WH01 Phys.Rev. C51, 1566 (1995) Higher-Order Corrections to Coulomb Fission NUCLEAR REACTIONS 27Al, Cu, Ag, U(U, F), E=120 MeV/nucleon; calculated higher order effects contribution to fission σ. Comparison to data, other models.
doi: 10.1103/PhysRevC.51.1566
1993NO03 Phys.Rev. C47, 406 (1993) Explanation of Recent Observations of Very Large Electromagnetic Dissociation Cross Sections NUCLEAR STRUCTURE Pb, Ag, Cu, 27Al, C, Ti, U, 120Sn, 197Au, 89Y; calculated electromagnetic dissociation σ for projectiles with A=12-139 on these targets; deduced higher order corrections role.
doi: 10.1103/PhysRevC.47.406
1993NO06 Phys.Rev. C48, 1915 (1993) Explanation of Recent Observations of Very Large Electromagnetic Dissociation Cross Sections. II. Higher Order Corrections NUCLEAR REACTIONS 197Au(12C, X), (20Ne, X), (40Ar, X), (56Fe, X), (139La, X), (197Au, X), (238U, X), (16O, X), (32S, X), E ≥ 0.15 GeV/nucleon; calculated electromagnetic dissociation σ; deduced higher order corrections role. Weizsacker-Williams theory.
doi: 10.1103/PhysRevC.48.1915
1992NO02 Phys.Rev. C45, 3024 (1992) Two Neutron Removal in Relativistic Nucleus-Nucleus Reactions NUCLEAR REACTIONS 59Co(12C, X)57Co/58Co, 59Co(20Ne, X)57Co/58Co, 59Co(56Fe, X)57Co/58Co, 59Co(139La, X)57Co/58Co, E=relativistic; 197Au(12C, X), (20Ne, X), (40Ar, X), (56Fe, X), (139La, X)195Au/196Au, E=relativistic; calculated one-, two-nucleon removal σ. Weizsacker-Williams theory.
doi: 10.1103/PhysRevC.45.3024
1991NO01 Phys.Rev. C43, R368 (1991) Relativistic Coulomb Fission NUCLEAR REACTIONS 238U, 239Pu(12C, F), (28Si, F), (197Au, F), (238U, F), E=relativistic; calculated Coulomb fission σ(E).
doi: 10.1103/PhysRevC.43.R368
1990NO09 Phys.Rev. C42, 2259 (1990); Erratum Phys.Rev. C46, 819 (1992) Charge Dependence and Electric Quadrupole Effects on Single-Nucleon Removal in Relativistic and Intermediate Energy Nuclear Collisions NUCLEAR REACTIONS 59Co, 12C, 89Y, 238U, 197Au(12C, X), (20Ne, X), E=2.1 GeV; 89Y, 197Au(40Ar, X), E=2.1 GeV; 89Y, 59Co, 12C(20Ne, X), E=2.1 GeV; 197Au, 59Co, 12C(56Fe, X), E=1.7 GeV; 197Au, 12C(139La, X), E=1.26, 1.7 GeV; calculated multipole σ.
doi: 10.1103/PhysRevC.42.2259
1988NO01 Phys.Rev. C37, 407 (1988); Erratum Phys.Rev. C37, 2266 (1988) Angular and Spectral Distributions for Subthreshold Pion Production NUCLEAR REACTIONS 27Al(14N, π0), E=35 MeV/nucleon; calculated σ(θ).
doi: 10.1103/PhysRevC.37.407
1986DE15 Nucl.Phys. A454, 733 (1986) P.A.Deutchman, J.W.Norbury, L.W.Townsend Theoretical Contributions to Coherent Pion Production in Subthreshold and Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS 12C(16O, π), E=85, 400 MeV/nucleon; calculated coherent pion production σ.
doi: 10.1016/0375-9474(86)90115-6
1986DE34 Phys.Rev. C34, 2377 (1986) P.A.Deutchman, K.M.Maung, J.W.Norbury, J.O.Rasmussen, L.W.Townsend Δ Excitations and Shell-Model Information in Heavy-Ion, Charge-Exchange Reactions NUCLEAR STRUCTURE 12B, 12N; calculated nucleon, isobar particle states. NUCLEAR REACTIONS 12C(12C, 12B), (12C, 12N), E not given; calculated σ(θ), coherent pion production σ. Multipole expansion, harmonic oscillator.
doi: 10.1103/PhysRevC.34.2377
1986NO01 Phys.Rev. C33, 377 (1986) Theoretical Estimates of Photoproduction Cross Sections for Neutral Subthreshold Pions in Carbon-Carbon Collisions NUCLEAR REACTIONS 12C(12C, π0), E=34-300 MeV; calculated σ(E); deduced negligible photoprocess contribution to pion production.
doi: 10.1103/PhysRevC.33.377
1986TO10 Phys.Rev. C34, 1491 (1986) L.W.Townsend, J.W.Wilson, F.A.Cucinotta, J.W.Norbury Comparison of Abrasion Model Differences in Heavy Ion Fragmentation: Optical versus geometric models NUCLEAR REACTIONS C(40Ar, X), E=213 MeV/nucleon; calculated fragment isotope production σ for X=Ar, Si, Mg. Geometric, optical abrasion models.
doi: 10.1103/PhysRevC.34.1491
1985NO06 Phys.Rev.Lett. 55, 681 (1985) J.W.Norbury, F.A.Cucinotta, P.A.Deutchman, L.W.Townsend Theoretical Spectral Distributions and Total Cross Sections for Neutral Subthreshold Pion Production in Carbon-Carbon Collisions NUCLEAR REACTIONS 12C(12C, π0), E=20-100 MeV/nucleon; calculated pion production σ(E), spectral distribution. Particle-hole theory, coherent isobar formation, decay.
doi: 10.1103/PhysRevLett.55.681
1985TO05 Can.J.Phys. 63, 135 (1985) L.W.Townsend, J.W.Wilson, J.W.Norbury A Simplified Optical Model Description of Heavy-Ion Fragmentation NUCLEAR REACTIONS 12C(40Ar, X), E=213 MeV/nucleon; calculated production σ(A) for X=S, P, Si, Al. Abrasion-ablation fragmentation model.
doi: 10.1139/p85-021
1984TO03 Nucl.Phys. A415, 520 (1984) L.W.Townsend, P.A.Deutchman, R.L.Madigan, J.W.Norbury Pion Production via Isobar Giant Resonance Formation and Decay NUCLEAR REACTIONS 12C(16O, π+), (16O, π-), (16O, π0), E=1 GeV/nucleon; 23Na, 19F(20Ne, π+), (20Ne, π-), (20Ne, π0), E=400 MeV/nucleon; 12C(12C, π+), (12C, π-), (12C, π0), E=85 MeV/nucleon; calculated pion production σ; deduced isobar giant resonance decay role. Spin, isospin formalism.
doi: 10.1016/0375-9474(84)90316-6
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