NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = H.R.Schelin Found 18 matches. 2013DE15 Eur.Phys.J. A 49, 51 (2013) V.V.Denyak, V.M.Khvastunov, S.A.Paschuk, H.R.Schelin Mass dependence of azimuthal asymmetry in the fission of 232Th and 233, 235, 236, 238U by polarized photons NUCLEAR REACTIONS 232Th(polarized γ, F), E=9.3 MeV;233,235,236,238U(polarized γ, F), E=7.9 MeV; measured bremsstrahlung induced fission products; deduced mass distributions, asymmetry.
doi: 10.1140/epja/i2013-13051-6
2010DE09 Phys.Atomic Nuclei 73, 395 (2010); Yad.Fiz. 73, 419 (2010) V.V.Denyak, V.M.Khvastunov, S.A.Paschuk, H.R.Schelin, A.A.Khomich, N.G.Shevchenko Excitation of Discrete Levels of 63Cu and 65Cu Nuclei in (e, e') Reactions NUCLEAR REACTIONS 63,65Cu(e, e'), E=120, 150, 225 MeV; measured Ee, Ie; 63,65Cu deduced level energies, multipolarities, B(E1), B(E2), B(E3).
doi: 10.1134/S1063778810030014
2004DE25 Yad.Fiz. 67, 906 (2004); Phys.Atomic Nuclei 67, 882 (2004) V.V.Denyak, V.M.Khvastunov, V.P.Likhachev, A.A.Nemashkalo, S.P.Paschuk, H.R.Schelin Excitation of Discrete Levels in 54Fe and 56Fe Nuclei by Means of (e, e') Reactions NUCLEAR REACTIONS 54,56Fe(e, e'), E=226 MeV; measured σ(E, θ). 54,56Fe deduced level energies, multipolarities.
doi: 10.1134/1.1755380
2004LI78 Braz.J.Phys. 34, 753 (2004) V.P.Likhachev, J.D.T.Arruda-Neto, M.T.F.da Cruz, H.Dias, S.B.Duarte, W.R.Carvalho, Jr., M.S.Hussein, A.C.S.Lima, L.F.R.Macedo, J.Mesa, S.A.Pashchuk, T.E.Rodrigues, G.Silva, H.R.Schelin, O.A.P.Tavares Residual Nucleus Excitation Energy in (e, e'p)- Reaction
doi: 10.1590/S0103-97332004000500012
2003LI25 Phys.Rev. C 68, 014615 (2003) V.P.Likhachev, J.D.T.Arruda-Neto, W.R.Carvalho, Jr., A.Deppman, I.G.Evseev, F.Garcia, M.S.Hussein, L.F.R.Macedo, A.Margaryan, J.Mesa, V.O.Nesterenko, O.Rodriguez, S.A.Pashchuk, H.R.Schelin, M.S.Vaudeluci Inclusive quasifree electrofission cross section for 238U NUCLEAR STRUCTURE 237,238U, 237Pa; calculated fissility vs excitation energy. NUCLEAR REACTIONS 238U(e, e'p), (e, e'), E=300 MeV; calculated σ(E, θ). 238U(e, F), E=100-250 MeV; measured fission σ; deduced reaction mechanism features.
doi: 10.1103/PhysRevC.68.014615
1997DE58 Acta Phys.Hung.N.S. 5, 13 (1997) F.Deak, A.Horvath, A.Kiss, Z.Seres, A.Galonsky, H.Hama, L.Heilbronn, D.W.Sackett, H.R.Schelin Production Rates of Excited Fragment Isotopes from the 36Ar + Ag Reaction at 35 MeV/nucleon NUCLEAR REACTIONS Ag(36Ar, X), E=35 MeV/nucleon; measured Z=3-5 excited fragments σ(θ) vs kinetic energy; deduced total production of neutron unbound states. Thermal model.
1997LI15 Phys.Rev. C56, 250 (1997) I.Licot, N.Added, N.Carlin, G.M.Crawley, S.Danczyk, J.Finck, D.Hirata, H.Laurent, D.J.Morrissey, M.M.de Moura, H.R.Schelin, J.Stasko, M.Steiner, A.A.P.Suaide, A.Szanto de Toledo, E.M.Szanto, M.Thoennessen, J.A.Winger Reaction Cross Sections and Radii for f-p Shell Exotic Neutron-Rich Nuclei NUCLEAR REACTIONS, ICPND Si(41Ar, X), (42Ar, X), (43Ar, X), (44Ar, X), (45Ar, X), (46Ar, X), (44K, X), (45K, X), (46K, X), (47K, X), (48K, X), (49K, X), (46Ca, X), (47Ca, X), (48Ca, X), (49Ca, X), (50Ca, X), (51Ca, X), (49Sc, X), (50Sc, X), (51Sc, X), (52Sc, X), (53Sc, X), E=52-69 MeV/nucleon; measured reaction σ. 41,42,43,44,45,46Ar, 44,45,46,47,48,49K, 46,47,48,49,50,51Ca, 49,50,51,52,53Sc deduced strong absorption radii, neutron separation energies. Comparison to Glauber model, RMF theory.
doi: 10.1103/PhysRevC.56.250
1995DE24 Phys.Rev. C52, 219 (1995) F.Deak, A.Horvath, A.Kiss, Z.Seres, A.Galonsky, C.K.Gelbke, H.Hama, L.Heilbronn, D.Krofcheck, W.G.Lynch, D.W.Sackett, H.R.Schelin, M.B.Tsang, J.Kasagi, T.Murakami Internal Excitation of Intermediate Mass Fragments from Collisions of 36Ar + Ag Nuclei at 35 MeV/nucleon NUCLEAR REACTIONS Ag(36Ar, X), E=35 MeV/nucleon; measured intermediate mass fragments (Li-Mg) population ratios.
doi: 10.1103/PhysRevC.52.219
1994HO02 Phys.Rev. C49, 1012 (1994) A.Horvath, F.Deak, A.Kiss, Z.Seres, A.Galonsky, C.K.Gelbke, H.Hama, L.Heilbronn, D.Krofcheck, W.G.Lynch, D.W.Sackett, H.R.Schelin, M.B.Tsang, J.Kasagi, T.Murakami Fragment Isotope Spectra from the 36Ar + Ag Reaction at 35 MeV/nucleon NUCLEAR REACTIONS Ag(36Ar, X), E=35 MeV/nucleon; measured inclusive fragment σ(E, θ); deduced total fragment production σ charge, mass dependence.
doi: 10.1103/PhysRevC.49.1012
1993AN15 Phys.Rev. C48, R2154 (1993) R.M.Anjos, N.Added, N.Carlin, L.Fante, Jr., M.C.S.Figueira, R.Matheus, H.R.Schelin, E.M.Szanto, C.Tenreiro, A.Szanto de Toledo, S.J.Sanders Fission Decay of Very Light Nuclear Systems NUCLEAR REACTIONS 10,11B(16O, X), (17O, X), (18O, X), 9Be(19F, X), E < 5 MeV/nucleon; measured σ(fragment θ); deduced fusion followed by fission evidence.
doi: 10.1103/PhysRevC.48.R2154
1993SC04 Nucl.Sci.Eng. 113, 184 (1993) H.R.Schelin, A.Galonsky, C.K.Gelbke, H.Hama, L.Heilbronn, D.Krofcheck, W.G.Lynch, D.Sackett, M.B.Tsang, X.Yang, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.Kasagi, T.Murakami Neutron Production in Heavy-Ion Reactions at 35 and 50 MeV/Nucleon NUCLEAR REACTIONS Ag(14N, xn), E=50 MeV/nucleon; measured neutron spectra. Moving source model analysis.
doi: 10.13182/NSE93-A24007
1992ME06 Nucl.Sci.Eng. 111, 132 (1992) A.C.Merchant, P.E.Hodgson, H.R.Schelin The Interaction of 1- to 20-MeV Neutrons with 238U NUCLEAR REACTIONS 238U(n, n), (n, n'), E=1-20 MeV; 238U(n, 2n), (n, 3n), E=threshold-20 MeV; analyzed σ(E), other data. Optical potential, dispersion relation approach.
doi: 10.13182/NSE92-A23929
1991SA10 Phys.Rev. C44, 384 (1991) D.Sackett, A.Galonsky, C.K.Gelbke, H.Hama, L.Heilbronn, D.Krofcheck, W.Lynch, H.R.Schelin, M.B.Tsang, X.Yang, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.Kasagi, T.Murakami Neutron Inclusive Measurements of 36Ar + Ag Reactions at 35 MeV/Nucleon NUCLEAR REACTIONS Ag(36Ar, nX), E=35 MeV/nucleon; measured inclusive σ(θ, E); deduced neutron multiplicities, nuclear temperatures. Moving source fits.
doi: 10.1103/PhysRevC.44.384
1990DE25 Phys.Rev. C42, 1029 (1990) F.Deak, A.Kiss, Z.Seres, A.Galonsky, L.Heilbronn, H.R.Schelin Light Fragments from 14N + Ag Collisions at 35 MeV/Nucleon NUCLEAR REACTIONS Ag(14N, X), E=35 MeV/nucleon; measured σ(fragment θ, En, θn); deduced model parameters. Moving source model.
doi: 10.1103/PhysRevC.42.1029
1989SC08 Phys.Rev. C39, 1827 (1989) H.R.Schelin, A.Galonsky, C.K.Gelbke, L.Heilbronn, W.G.Lynch, T.Murakami, M.B.Tsang, X.Yang, G.Zhang, B.A.Remington, F.Deak, A.Kiss, Z.Seres, J.Kasagi Neutron Inclusive Measurements in 14N + Ag Reactions at 35 MeV/Nucleon NUCLEAR REACTIONS Ag(14N, nX), E=35 MeV/nucleon; measured σ(θn, En); deduced angle integrated σ.
doi: 10.1103/PhysRevC.39.1827
1986HU06 Nucl.Phys. A458, 397 (1986) M.S.Hussein, E.Farrelly-Pessoa, H.R.Schelin, R.A.Douglas Isospin Mixing in Compound Nuclear Reactions: A study in the 11B(p, n)11C system at E(p) = 14.3 MeV NUCLEAR REACTIONS 11B(p, n), E=14.3 MeV; calculated σ(θ). 12C levels deduced isopsin purity. DWBA, Hauser-Feshbach calculations.
doi: 10.1016/0375-9474(86)90042-4
1985SC08 Nucl.Sci.Eng. 89, 87 (1985) H.R.Schelin, E.Farrelly Pessoa, W.R.Wylie, J.L.Cardoso, Jr., R.A.Douglas The 10,11B(p, n)10,11C Reactions Between E(p) = 13.7 and 14.7 MeV NUCLEAR REACTIONS 10,11B(p, n), E=13.7-14.7 MeV; measured absolute σ(θ) vs E.
doi: 10.13182/NSE85-A17886
1984SC04 Nucl.Phys. A414, 67 (1984) H.R.Schelin, E.Farrelly Pessoa, W.R.Wylie, E.W.Cybulska, K.Nakayama, L.M.Fagundes, R.A.Douglas The 12C(d, n)13N Reaction between E(d) = 7.0 and 13.0 MeV NUCLEAR REACTIONS 12C(d, n), E=7, 9.1, 13 MeV; measured σ(En), σ(E), absolute σ(θ). 12C(d, n), E=10.6-13 MeV; measured σ(E). 13N levels deduced S. Hauser-Feshbach reduction factors. Tof. DWBA analysis.
doi: 10.1016/0375-9474(84)90497-4
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