NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = G.Doukellis Found 15 matches. 2003KA22 Nucl.Instrum.Methods Phys.Res. A505, 381 (2003) D.Karamanis, S.Andriamonje, P.A.Assimakopoulos, G.Doukellis, D.A.Karadimos, A.Karydas, M.Kokkoris, S.Kossionides, N.G.Nicolis, C.Papachristodoulou, C.T.Papadopoulos, N.Patronis, P.Pavlopoulos, G.Perdikakis, R.Vlastou, and the n-TOF Collaboration Neutron cross-section measurements in the Th-U cycle by the activation method NUCLEAR REACTIONS 232Th(n, 2n), E ≈ 7.5-11.5 MeV; measured σ. Activation technique, comparison with previous results.
doi: 10.1016/S0168-9002(03)01102-1
2000VL04 Eur.Phys.J. A 8, 361 (2000) R.Vlastou, C.T.Papadopoulos, C.Tsabaris, P.A.Assimakopoulos, A.A.Pakou, G.Doukellis, C.A.Kalfas, A.C.Xenoulis Fusion Cross-Section of the 7Li + 11B Reaction NUCLEAR REACTIONS 11B(7Li, X)10Be/12C/13C/14C/15N/16N/17N/16O/17O, E=5.5-19 MeV; measured Eγ, σ, total fusion σ; deduced total fusion angular momentum vs excitation energy. Comparison with statistical model calculations.
doi: 10.1007/s100530050045
1995DO36 Nucl.Instrum.Methods Phys.Res. A356, 408 (1995) G.Doukellis, S.Kossionides, G.Galios, T.Paradellis A System for Transmission Measurements of Total Neutron Cross Sections using Two Silicon Detectors NUCLEAR REACTIONS 11B(n, X), E=7.3-8.5 MeV; measured σ(E). New transmission measurement technique.
doi: 10.1016/0168-9002(94)01314-4
1993DO04 Nucl.Instrum.Methods Phys.Res. A327, 480 (1993) G.Doukellis, T.Paradellis, S.Kossionides Energy and Flux Measurements of the Neutrons Produced in a Gas Cell NUCLEAR REACTIONS 28Si(n, n), (n, p), (n, α), (n, n'), 28Si(n, α), E=7.88 MeV; measured neutron, charged particle spectra. Gas cell produced neutron flux, Monte Carlo simulations.
doi: 10.1016/0168-9002(93)90714-S
1990PA22 Z.Phys. A337, 211 (1990) T.Paradellis, S.Kossionides, G.Doukellis, X.Aslanoglou, P.Assimakopoulos, A.Pakou, C.Rolfs, K.Langanke Astrophysical S(E) Factor of 8Li(α, n0)11B and Inhomogeneous Big Bang Nucleosynthesis NUCLEAR REACTIONS, ICPND 11B(n, α), E=76-12.6 MeV; measured σ(E); deduced astrophysical factor for 8Li(α, n)11B. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23457. 1989DO03 Phys.Rev. C39, 2088 (1989) Reply to ' Comment on ' Fusion of 32S + 27Al and 19F + 40Ca and the Nucleus-Nucleus Potential ' ' NUCLEAR REACTIONS 27Al(32S, X), 40Ca(19F, X), E not given; analyzed fusion σ(E) analysis; deduced critical distance model validity.
doi: 10.1103/PhysRevC.39.2088
1989DO07 Nuovo Cim. 101A, 651 (1989) Reaction Rates for 26Al(n, p)26Mg and 26Al(n, α)23Na at T = (108-109)K NUCLEAR REACTIONS 26Al(n, p), (n, α), E=0-150 keV; analyzed σ(E); deduced reaction rates at stellar temperatures. 27Al deduced resonances, Γ, J, π, reaction strength factor.
doi: 10.1007/BF02848087
1988DO07 Phys.Rev. C37, 2233 (1988) Fusion of 32S + 27Al and 19F + 40Ca and the Nucleus-Nucleus Potential NUCLEAR REACTIONS, ICPND 27Al(32S, X), E=67-393 MeV; 40Ca(19F, X), E ≈ 25-100 MeV; calculated fusion σ(E); deduced fusion parameters, nucleus-nucleus potential.
doi: 10.1103/PhysRevC.37.2233
1988DO11 Nucl.Phys. A485, 369 (1988) G.Doukellis, G.Hlawatsch, B.Kolb, A.Miczaika, G.Rosner, B.Sedelmeyer Evaporation Residues from the Fusion of 32S on 27Al at E = 142-227 MeV NUCLEAR REACTIONS, MECPD 27Al(32S, X), E=142-227 MeV; measured σ(E, θ, A) for evaporation residue products; deduced L(max), limitations to fusion-evaporation.
doi: 10.1016/0375-9474(88)90108-X
1987DO06 Nucl.Phys. A467, 511 (1987) The 26Mg(p, n)26Al and 23Na(α, n)26Al Reactions near Threshold NUCLEAR REACTIONS, ICPND 26Mg(p, n), E=5.3-7 MeV; 23Na(α, n), E=3.9-5.9 MeV; 26Mg(p, p'), 26Mg(p, α), E=5.3-6.1 MeV; measured σ(E), σ(E, E(n), θ), σ(E, E(p), θ), σ(E, E(α), θ); deduced thermonuclear reaction rate. 26Al deduced levels, resonance strengths, Γ, J, π, p, α-induced reaction rate. Enriched 26Mg target.
doi: 10.1016/0375-9474(87)90542-2
1983WA22 Phys.Rev. C28, 1538 (1983) S.Wald, I.Tserruya, Z.Fraenkel, G.Doukellis, H.Gemmeke, H.L.Harney Neutron, Proton, and Alpha Emission in Deep Inelastic Collisions of 16O on Three Ca Isotopes at 102 and 142 MeV NUCLEAR REACTIONS 40,44,48Ca(16O, X), E=102, 142 MeV; measured σ(fragment θ) for X=C, N, O, F. 40,44,48Ca(16O, nX), (16O, pX), (16O, αX), E=102, 142 MeV; measured projectile fragment (light particle)-coin; deduced light particle multiplicities, production mechanism.
doi: 10.1103/PhysRevC.28.1538
1982RO10 Nucl.Phys. A385, 174 (1982) G.Rosner, G.Hlawatsch, B.Kolb, G.Doukellis, J.B.Natowitz, Th.Walcher Possible Contribution of Low-l Waves to the Deep Inelastic Collisions of 32S with 27Al NUCLEAR REACTIONS 27Al(32S, X), E=152.6, 175 MeV; measured σ(θ), (fragment)(fragment)(θ), (fragment)(fragment)-coin versus (Q); deduced no (L)-window. Deep inelastic reactions, TDHF.
doi: 10.1016/0375-9474(82)90495-X
1982WA03 Phys.Rev. C25, 1118 (1982) S.Wald, I.Tserruya, Z.Fraenkel, G.Doukellis, H.Gemmeke, H.L.Harney Neutron, Proton, and Alpha Emission in Deep Inelastic Collisions of 16O on 48Ca at 142 MeV NUCLEAR REACTIONS 48Ca(16O, nX), (16O, pX), (16O, αX), E=142 MeV; measured nX-, pX-, αX-coin; deduced σ(θ), σ(E) for n-, p-, α-emission. Statistical evaporation, heavy fragments rest frame.
doi: 10.1103/PhysRevC.25.1118
1981PO04 Nucl.Phys. A357, 237 (1981) F.Porto, S.Sambataro, K.Kusterer, Liu Ken Pao, G.Doukellis, H.L.Harney Reaction and Fusion Cross Sections for 32S on 27Al and 48Ti NUCLEAR REACTIONS 48Ti(32S, 32S), (32S, X), E(cm)=96 MeV; 27Al(32S, 32S), (32S, X), E(cm)=66.4, 73.2 MeV; measured σ(θ, elastic), σ(θ, evaporation residues); deduced σ(reaction).
doi: 10.1016/0375-9474(81)90636-9
1974DO09 Nucl.Phys. A229, 47 (1974) G.Doukellis, C.McKenna, R.Finlay, J.Rapaport, H.J.Kim Low Lying States of 96Tc NUCLEAR REACTIONS 96Mo(p, nγ), E=3.8-5.5 MeV; measured σ(E, En, θ), σ(E, Eγ). 96Tc deduced levels, J, π, quadrupole moment. Enriched target.
doi: 10.1016/0375-9474(74)90674-5
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