NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = D.Rendic Found 37 matches. 2007TU04 Nucl.Phys. A787, 337c (2007) A.Tumino, C.Spitaleri, G.G.Rapisarda, S.Cherubini, S.Blagus, M.Bogovac, V.Crucilla, Z.Elekes, Z.Fulop, M.Gulino, G.Gyurky, G.Kiss, M.La Cognata, L.Lamia, Dj.Miljanic, M.Milin, F.Mudo, A.Mukhamedzhanov, R.G.Pizzone, D.Rendic, S.Romano, M.L.Sergi, E.Somorjai No signature of nuclear-Coulomb interference in the proton-proton elastic scattering via the Trojan Horse Method NUCLEAR REACTIONS 2H(p, 2p), E=5, 6 MeV; measured Ep, Ip, σ(E, θ). Plane wave impulse approximation, Trojan horse method.
doi: 10.1016/j.nuclphysa.2006.12.053
2004SO35 Fizika(Zagreb) B 13, 433 (2004) N.Soic, S.Blagus, M.Bogovac, W.Catford, S.Cherubini, N.Clarke, E.Costanzo, L.Donadille, S.Fazinic, M.Freer, B.Fulton, B.Greenhalgh, K.Jones, M.Lattuada, P.Leask, D.Mahboub, M.Milin, D.Miljanic, D.Rendic, S.Romano, C.Spitaleri, T.Tadic, D.Watson, D.Weisser, M.Zadro Experimental evidence for molecular structures in light nuclei NUCLEAR REACTIONS 7Li(7Li, 2α), E=8, 30 MeV; 9Be(7Li, 7Li), (7Li, α6Li), (7Li, α7Li), E=52 MeV; 7Li(9Be, α9Be), (9Be, α10Be), E=70 MeV; measured excitation energy spectra. 9,10Be, 13,14C deduced excited states, cluster structures.
2001MI39 Fizika(Zagreb) B10, 235 (2001) D.Miljanic, N.Soic, S.Blagus, S.Cherubini, E.Costanzo, M.Lattuada, M.Milin, A.Musumarra, R.G.Pizzone, D.Rendic, S.Romano, C.Spitaleri, A.Tumino, M.Zadro 10Be and Molecular States NUCLEAR REACTIONS 7Li(7Li, α), E=8, 30 MeV; 9Be(7Li, 6Li), E=52 MeV; measured excitation energy spectra, Eα following residual nucleus decay. 10Be deduced levels, J, π, molecular states.
2001MU30 Phys.Rev. C64, 068801 (2001) A.Musumarra, R.G.Pizzone, S.Blagus, M.Bogovac, P.Figuera, M.Lattuada, M.Milin, D.Miljanic, M.G.Pellegriti, D.Rendic, C.Rolfs, N.Soic, C.Spitaleri, S.Typel, H.H.Wolter, M.Zadro Improved Information on the 2H(6Li, α)4He Reaction Extracted via the ' Trojan Horse ' Method NUCLEAR REACTIONS 6Li(6Li, 2α), E(cm)=10-800 keV; measured σ; deduced astrophysical S-factor, electron screening potential energy.
doi: 10.1103/PhysRevC.64.068801
2001SP04 Phys.Rev. C63, 055801 (2001) C.Spitaleri, S.Typel, R.G.Pizzone, M.Aliotta, S.Blagus, M.Bogovac, S.Cherubini, P.Figuera, M.Lattuada, M.Milin, D.Miljanic, A.Musumarra, M.G.Pellegriti, D.Rendic, C.Rolfs, S.Romano, N.Soic, A.Tumino, H.H.Wolter, M.Zadro ' Trojan Horse ' Method Applied to 2H(6Li, α)4He at Astrophysical Energies NUCLEAR REACTIONS 6Li(6Li, 2α), E=6 MeV; measured Eα, Iα(θ), αα-coin. 2H(6Li, α), E(cm)=13-750 keV; deduced astrophysical S-factor. Kinematically complete measurement, Trojan Horse method.
doi: 10.1103/PhysRevC.63.055801
1999GO15 Phys.Rev. C60, 037601 (1999) N.Godinovic, S.Blagus, M.Bogovac, M.Lattuada, M.Milin, D.Miljanic, D.Rendic, N.Soic, C.Spitaleri, M.Zadro 7Li(d, αα)n Reaction and the 2+ Isospin-Mixed Doublet in 8Be NUCLEAR REACTIONS 7Li(d, 2α), E=3-6 MeV; measured Eα, Iα, αα-coin; deduced 8Be isospin-mixed state contribution, related reaction mechanism features. 8Be level deduced configuration.
doi: 10.1103/PhysRevC.60.037601
1996SO17 Europhys.Lett. 34, 7 (1996) N.Soic, S.Blagus, M.Bogovac, S.Fazinic, M.Lattuada, M.Milin, D.Miljanic, D.Rendic, C.Spitaleri, T.Tadic, M.Zadro 6He + α Clustering in 10Be NUCLEAR REACTIONS 7Li(7Li, α6He), (7Li, 2α), E=8 MeV; measured (Q-value) spectra, αα-, α(6He)-coin. 10Be deduced levels, decay characteristics. Kinematically complete measurement.
doi: 10.1209/epl/i1996-00407-y
1994ZA10 Nuovo Cim. 107A, 185 (1994) M.Zadro, M.Bogovac, G.Calvi, M.Lattuada, D.Miljanic, D.Rendic, C.Spitaleri, B.Vlahovic, H.Witala, W.Glockle, J.Golak, H.Kamada Proton-Induced Deuteron Break-Up at E(lab)(p) = 22.7 MeV NUCLEAR REACTIONS 2H(p, np), E=22.7 MeV; measured σ(θ1, θ2) vs arc length. Different kinematically complete configurations. Models comparison.
doi: 10.1007/BF02781551
1989TO08 Fizika(Zagreb) 21, 209 (1989) P.Tomas, S.Blagus, M.Bogovac, D.Hodko, M.Krcmar, D.Miljanic, V.Pravdic, D.Rendic, M.Vajic, M.Vukovic Deuterium Nuclear Fusion in Metals at Room Temperature NUCLEAR REACTIONS 2H(d, n), E=low; measured no significant neutron excess above background. Heavy water electrolysis, PdD nuclear fusion.
1987ZA01 Nucl.Sci.Eng. 95, 79 (1987) M.Zadro, S.Blagus, D.Miljanic, D.Rendic The (n, t) Reaction on 9Be at 14.6 MeV NUCLEAR REACTIONS 9Be(n, t), E=14.6 MeV; measured σ(θ), σ. Counter telescope.
doi: 10.13182/NSE87-A20434
1986MI14 Radiat.Eff. 94, 245 (1986) D.Miljanic, S.Blagus, M.Zadro, D.Rendic The 7Li(n, αx) Reactions and the States of 4H NUCLEAR REACTIONS 7Li(n, α), E=14.6 MeV; measured α(residue)-coin. 4H deduced resonance, reduced width.
1984MI04 Nucl.Phys. A419, 351 (1984) The (n, 3He) Reactions on 40Ca and Other Nuclei at E(n) = 14.6 MeV NUCLEAR REACTIONS 40Ca(n, 3He), E=14.6 MeV; measured σ(θ); deduced Coulomb effects role. Investigated cross section behaviour. Natural target.
doi: 10.1016/0375-9474(84)90397-X
1983BL17 Nucl.Instrum.Methods 216, 415 (1983) S.Blagus, D.Miljanic, D.Rendic Three and Four Body Nuclear Reactions in Special Kinematical Conditions NUCLEAR REACTIONS 7Li(d, 2α), E=160 keV; measured αα-coin. Kinematically complete experiment, different loci.
doi: 10.1016/0167-5087(83)90508-2
1981MI16 Fizika(Zagreb) 13, Suppl.No.2, 33 (1981) D.J.Miljanic, M.Zadro, D.Rendic The 40Ca(n, 3He)38Ar Reaction at E(n) = 14.6 MeV NUCLEAR REACTIONS 40Ca(n, 3He), E=14.6 MeV; measured σ(θ); deduced reaction mechanism, σ(total). Proportional counter telescope.
1980MI02 Nucl.Phys. A334, 189 (1980) D.Miljanic, S.Blagus, V.Pecar, D.Rendic 14.6 MeV Neutron Scattering and Reactions on Lithium Isotopes NUCLEAR REACTIONS 7Li(n, 7Li), 6,7Li(n, 6Li), (n, 6He), E=14.6 MeV; measured σ(E(7Li), θ), σ(E(6Li), θ), σ(E(6He), θ). Enriched targets.
doi: 10.1016/0375-9474(80)90062-7
1976JU04 Fizika 8, 81 (1976) M.Jurcevic, A.Ljubicic, D.Rendic Decay of 93Nb-m RADIOACTIVITY 93mNb; measured Eγ, α(K); deduced λ.
1976PA23 Fizika 8, 73 (1976) Is There an Anomaly in the Backward Cross Section of n-t Scattering Around 14 MeV (Question) NUCLEAR REACTIONS 3H(n, n), E=13.94-14.94 MeV; measured σ; analyzed data E=6-23 MeV.
1973AN25 Nucl.Instrum.Methods 113, 93 (1973) E.Andrade, D.Rendic, V.A.Otte, G.C.Phillips Charged Particle Mass Identification by Energy-Time-of-Flight Technique NUCLEAR REACTIONS 12C(d, X), E=12 MeV; measured σ(E(X), mass(X)).
doi: 10.1016/0029-554X(73)90483-7
1973SA03 Nucl.Phys. A202, 49 (1973) J.Sandler, G.S.Mutchler, W.von Witsch, V.A.Otte, G.C.Phillips, D.Rendic Rescattering and Neutron-Proton Final-State Interaction in the 12C(d, pn)12C Reaction NUCLEAR REACTIONS 12C(d, np), E=5.00, 5.15, 5.39, 5.50, 9.20, 9.85 MeV; measured σ(Ep, θ(p)=θ(n)); deduced p-n final-state interaction.
doi: 10.1016/0375-9474(73)90240-6
1972AN02 Nucl.Phys. A183, 145 (1972) E.Andrade, V.Valkovic, D.Rendic, G.C.Phillips Angular Distributions of Quasi-Free Scattering Contributions in Deuteron Break-up by Protons and Deuterons NUCLEAR REACTIONS 2H(p, pn), E=12.5 MeV; 2H(d, pn), E=12.5 MeV; measured σ(E(p1), E(p2), Ep, En, θ(1)=-θ(2)=15-60°), (Ed, Ep, Ed, En, θ(1)=-θ(2)=15-40°).
doi: 10.1016/0375-9474(72)90935-9
1972VA04 Nucl.Phys. A182, 225 (1972) V.Valkovic, N.Gabitzsch, D.Rendic, I.Duck, G.C.Phillips Coincidence Spectra from d + d → d + p + n and p + d → p + p + n Reactions with Neutron Detection at Zero Degrees NUCLEAR REACTIONS 2H(p, pn), E=10 MeV; 2H(d, np), E=10 MeV; measured σ(Ep, En, θ(n)=0°, θ(p)=15-40°), σ(Ep, En, θ(n)=0°, θ(d)=15-35°).
doi: 10.1016/0375-9474(72)90273-4
1972VO01 Nucl.Phys. A180, 402 (1972) W.von Witsch, M.Ivanovich, D.Rendic, V.Valkovic, G.C.Phillips, K.Schafer Decay of 12C via the 11B(p, 2α)α Reaction NUCLEAR REACTIONS 11B(p, 2α)α, E=1.39, 1.98, 2.62 MeV; measured σ(E(α1), E(α2), θ(α1), θ(α2)). 12C resonance deduced J, π. Enriched target.
doi: 10.1016/0375-9474(72)90869-X
1971MU18 Nucl.Phys. A172, 469 (1971) G.S.Mutchler, D.Rendic, D.E.Velkley, W.E.Sweeney, Jr., G.C.Phillips The (d, n) Reaction on 1p Shell Nuclei at E = 11.8 MeV NUCLEAR REACTIONS 10,11B(d, n), 12,13C(d, n), E=11.8 MeV; measured σ(En, θ). 11,12C, 13,14N deduced absolute S. Enriched targets.
doi: 10.1016/0375-9474(71)90038-8
1971OT02 Phys.Rev. C4, 322 (1971) V.A.Otte, W.von Witsch, J.Sandler, D.Rendic, G.C.Phillips Singlet Deuteron p-n Correlations in the 13C(p, pn)12C Reaction NUCLEAR REACTIONS 13C(p, pn), E=7.9-12.5 MeV; measured σ(E;Ep, θ(p), θ(n)); deduced singlet deuteron contribution.
doi: 10.1103/PhysRevC.4.322
1971RE19 Nucl.Phys. A178, 49 (1971) D.Rendic, N.D.Gabitzsch, V.Valkovic, W.von Witsch, G.C.Phillips d + 11B → 3α + n Four-Body Break-up and States in 9Be NUCLEAR REACTIONS 11B(d, 3α)n, E=10.425, 12.0 MeV; measured α-α, α-n coin spectra. Enriched target.
doi: 10.1016/0375-9474(71)90184-9
1971SW10 Phys.Lett. 37B, 183 (1971) W.E.Sweeney, Jr., V.Valkovic, D.Rendic, G.C.Phillips On the Observation of Rescattering Effects in the Reaction 7Li(d, nα)4He NUCLEAR REACTIONS 7Li(d, nα), E=2.07, 2.09 MeV; measured σ(En, Eα, θ(n), θ(α)); deduced rescattering effects.
doi: 10.1016/0370-2693(71)90046-3
1971VA03 Phys.Rev.Lett 26, 394 (1971) V.Valkovic, D.Rendic, V.A.Otte, G.C.Phillips Comparison of p-p and n-p Quasi-Free Scattering in p + d → p + p + n Reaction NUCLEAR REACTIONS 2H(p, 2p), (p, pn), E=12 MeV; measured σ(Ep1, Ep2), σ(Ep, En).
doi: 10.1103/PhysRevLett.26.394
1971VA14 Nucl.Phys. A166, 547 (1971) V.Valkovic, D.Rendic, V.A.Otte, W.von Witsch, G.C.Phillips Nucleon-Nucleon Quasi-Free Scattering in the p + d → p + p + n Reaction at Low Bombarding Energies NUCLEAR REACTIONS 2H(p, 2p)n, E=4.5-13 MeV; measured σ(E;Ep, En, θ(p), θ(n)); deduced p-p, p-n quasi-free scattering contributions.
doi: 10.1016/0375-9474(71)90906-7
1971VO07 Nucl.Phys. A172, 633 (1971) W.von Witsch, M.Ivanovich, V.A.Otte, D.Rendic, G.C.Phillips Final-State Interactions in the 6Li(d;6Li, p)n Reaction NUCLEAR REACTIONS 6Li(d, 6Li)pn , E=10 MeV; measured σ(E(6Li), Ep, θ(6Li), θ(p)). Enriched target.
doi: 10.1016/0375-9474(71)90050-9
1970MI14 Nucl.Phys. A156, 193 (1970) D.Miljanic, V.Valkovic, D.Rendic, M.Furic Angular Distribution of Tritons from the 11B(n, t)9Be Reaction at 14.4 MeV NUCLEAR REACTIONS 11B(n, t), E=14.4 MeV; measured σ(Et, θ). Enriched target.
doi: 10.1016/0375-9474(70)91125-5
1970VA25 Phys.Lett. 33B, 208 (1970) V.Valkovic, W.Von Witsch, D.Rendic, G.C.Phillips Proton-Proton Quasi-Free Scattering in the p + d → p + p + n Reaction For E = 4.5-13.0 MeV NUCLEAR REACTIONS 2H(p, 2p)n, E=4.5-13 MeV; measured σ(E;Ep1, Ep2, θ(p1), θ(p2)).
doi: 10.1016/0370-2693(70)90573-3
1970VO15 Phys.Rev. C2, 2144 (1970) W.von Witsch, M.Ivanovich, D.Rendic, J.Sandler, G.C.Phillips Proton-Neutron Final-State Interactions in the D(d, dp)n Reaction NUCLEAR REACTIONS 2H(d, dp), E=11, 13 MeV; measured σ(Ep, Ed); deduced p-n final-state interaction.
doi: 10.1103/PhysRevC.2.2144
1968RE07 Nucl.Phys. A117, 113(1968) D.Rendic, B.Antolkovic, G.Paic, M.Turk, P.Tomas 14.4 MeV Neutron-Induced Reactions on 19F NUCLEAR REACTIONS 19F(n, p), (n, d), (n, t), (n, α), E=14.4 MeV; measured σ(Ep, θ), σ(Ed, θ), σ(Et, θ), σ(Eα, θ). 18O levels deduced S. Natural target.
doi: 10.1016/0375-9474(68)90864-6
1967AN03 Phys.Rev. 159, 777 (1967) B.Antolkovic, G.Paic, P.Tomas, D.Rendic Study of Neutron-Induced Reactions on He3 at E=14.4 MeV NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.159.777
1967AN08 Izv.Akad.Nauk SSSR, Ser.Fiz. 31, 110 (1967); Bull.Acad.Sci.USSR, Phys.Ser. 31, 107 (1968) B.Antolkovic, G.Paic, D.Rendic, P.Tomas Interaction of 14.4 MeV Neutrons with N14 NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
1967PA03 Nucl.Phys. A96, 476(1967) The 9Be(n, α0)6He Reaction Induced by 14.4 MeV Neutrons NUCLEAR REACTIONS 9Be(n, α), 9Be(n, 6He), E = 14.4 MeV; measured σ(Eα, θ), σ(E(6He), θ).
doi: 10.1016/0375-9474(67)90728-2
1967RE01 Nucl.Phys. A91, 604(1967) The Reaction 14N(n, t)12C at E =14.4 MeV NUCLEAR REACTIONS 14N(n, t), E = 14.4 MeV; measured σ(Et, θ). Natural target.
doi: 10.1016/0375-9474(67)90579-9
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