NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = E.Ungricht Found 29 matches. 1991MU01 Phys.Rev. C43, 957 (1991) S.Mukhopadhyay, S.Levenson, R.E.Segel, G.Garino, D.Geesaman, J.P.Schiffer, G.Stephans, B.Zeidman, E.Ungricht, H.Jackson, R.Kowalczyk, D.Ashery, E.Piasetzky, M.Moinester, I.Navon, L.C.Smith, R.C.Minehart, G.S.Das, R.R.Whitney, R.Mckeown, B.Anderson, R.Madey, J.Watson Pion Absorption by 3He at the Δ-Resonance Energy NUCLEAR REACTIONS 3He(π+, X), (π-, X), E=165 MeV; measured σ(θ1, θ2) vs momentum following pion absorption; deduced absorption mechanism.
doi: 10.1103/PhysRevC.43.957
1985JA09 J.Phys.(London) G11, 843 (1985) L.Jarczyk, B.Kamys, A.Magiera, A.Strzalkowski, A.Szczurek, K.Bodek, M.Hugi, J.Lang, R.Muller, E.Ungricht Reactions in the 9Be + 9Be System at Low Energies NUCLEAR REACTIONS, ICPND 9Be(9Be, p), (9Be, d), (9Be, t), (9Be, α), (9Be, 7Li), E(cm)=7 MeV; 9Be(9Be, 8Be), E(cm)=10 MeV; measured particle spectra, σ(θ); deduced optical potential parameters, fusion σ. 10Be level deduced spectroscopic factor. Statistical model, DWBA analyses.
doi: 10.1088/0305-4616/11/7/009
1985MU14 Phys.Rev. C32, 1558 (1985) T.Murakami, E.Ungricht, Y.-W.Lui, Y.Mihara, E.Takada, R.E.Tribble Alpha Transfer Reaction 16O(12C, 8Be(g.s.))20Ne: Key process in the 12C(16O, α) reaction NUCLEAR REACTIONS 16O(12C, 8Be), E=109 MeV; measured σ(θ). 20Ne levels deduced relative spectroscopic factors. DWBA analysis.
doi: 10.1103/PhysRevC.32.1558
1985MU18 Phys.Rev. C32, 2161 (1985) T.Murakami, N.Takahashi, Y.-W.Lui, E.Takada, D.M.Tanner, R.E.Tribble, E.Ungricht, K.Nagatani Search for a Direct Large-Cluster-Transfer Process in the 12,13C(20Ne, α) Reaction NUCLEAR REACTIONS 12,13C(20Ne, α), E=140.2 MeV; measured σ(Eα, θ); deduced sequential decay process. Hauser-Feshbach analysis.
doi: 10.1103/PhysRevC.32.2161
1985UN01 Phys.Rev. C31, 934 (1985) E.Ungricht, W.S.Freeman, D.F.Geesaman, R.J.Holt, J.R.Specht, B.Zeidman, E.J.Stephenson, J.D.Moses, M.Farkhondeh, S.Gilad, R.P.Redwine Tensor Polarization in Pion-Deuteron Elastic Scattering NUCLEAR REACTIONS 2H(π+, π+), E=140-256 MeV; measured tensor polarization t20(θ).
doi: 10.1103/PhysRevC.31.934
1984MU04 Phys.Rev. C29, 847 (1984) T.Murakami, E.Ungricht, N.Takahashi, Y.-W.Lui, Y.Mihara, R.E.Neese, E.Takada, D.M.Tanner, R.E.Tribble, K.Nagatani Origin of the Structures in the 12C(16O, α) Reaction: Dominance of 20Ne and 16O sequential α-decay processes NUCLEAR REACTIONS 12C(16O, α), E=112-191 MeV; measured σ(Eα, θα) vs E. 12C(16O, α12C), E=145 MeV; measured σ(θα, θ(12C)) vs (Q), (12C)(12C)(α)-coin; deduced reaction mechanism. 24Mg deduced resonances. 20Ne, 16O resonances deduced sequential α-decay.
doi: 10.1103/PhysRevC.29.847
1984UN01 Phys.Rev.Lett. 52, 333 (1984) E.Ungricht, W.S.Freeman, D.F.Geesaman, R.J.Holt, J.R.Specht, B.Zeidman, E.J.Stephenson, J.D.Moses, M.Farkhondeh, S.Gilad, R.P.Redwine Tensor Polarization in π-d Scattering and Pion Absorption NUCLEAR REACTIONS 2H(π+, π+), E=134-256 MeV; measured deuteron tensor polarization vs θ, E; deduced pion absorption treatment inadequacy.
doi: 10.1103/PhysRevLett.52.333
1983MU04 Phys.Lett. 120B, 319 (1983) T.Murakami, E.Ungricht, N.Takahashi, Y.-W.Lui, Y.Mihara, R.E.Neese, E.Takada, D.M.Tanner, R.E.Tribble, K.Nagatani Energy Dependence of the 12C(16O, α) Reaction NUCLEAR REACTIONS 12C(16O, αX), E=112-191 MeV; measured σ(θ, Eα) vs E; deduced reaction mechanism.
doi: 10.1016/0370-2693(83)90453-7
1983SR01 Nucl.Phys. A406, 390 (1983) J.Sromicki, M.Hugi, J.Lang, R.Muller, E.Ungricht, L.Jarczyk, B.Kamys, A.Magiera, Z.Rudy, A.Strzalkowski, B.Zebik The Role of Particle Transfer in Large-Angle Scattering of 1p-Shell Nuclei NUCLEAR REACTIONS 9Be(10B, 10B), 11B(12C, 12C), (12C, 12C'), 13C(14N, 14N), 15N(16O, 16O), E(cm)=9.5-20 MeV; measured σ(θ), σ(E); deduced reaction mechanism. Optical model, compound nucleus, proton transfer direct reaction model analysis.
doi: 10.1016/0375-9474(83)90468-2
1982HU06 Phys.Rev. C25, 2403 (1982) M.Hugi, J.Lang, R.Muller, J.Sromicki, E.Ungricht, K.Bodek, L.Jarczyk, B.Kamys, A.Strzalkowski, H.Witala Energy Dependence of 9Be + 12C Cross Sections: Resonances or fluctuations NUCLEAR REACTIONS 12C(9Be, p), (9Be, d), (9Be, t), (9Be, α), (9Be, 8Be), (9Be, 9Be), E(cm)=5.9-15.4 MeV; measured σ(θ) vs E; deduced no channel correlations, no resonances. Statistical model.
doi: 10.1103/PhysRevC.25.2403
1982TA07 Phys.Lett. 110B, 445 (1982) N.Takahashi, E.Ungricht, T.Murakami, Y.-W.Lui, R.Neese, D.Tanner, R.Tribble, K.Nagatani Comparative Study of Compound Components in 14N(14N, α) and 12C(16O, α) Reactions NUCLEAR REACTIONS 14N(14N, α), E=111 MeV; measured σ(θ, E). One-step evaporation calculations.
doi: 10.1016/0370-2693(82)91035-8
1981HU07 J.Phys.(London) G7, 1395 (1981) M.Hugi, L.Jarczyk, B.Kamys, J.Lang, R.Muller, J.Sromicki, A.Strzalkowski, E.Ungricht, G.Willim, Z.Wrobel, W.Zipper Potential Model for Fusion and Angular Momentum Localisation NUCLEAR REACTIONS 9Be(12C, 12C), E(cm)=11.4 MeV; 16O(16O, 16O), E(cm)=19 MeV; 9Be(28Si, 28Si), E(cm)=15.1 MeV; 24Mg(16O, 16O), E(cm)=24 MeV; 40Ca(16O, 16O), E(cm)=40 MeV; 12C(16O, 16O), E(cm)=72 MeV; 28Si(6Li, 6Li), E(cm)=16.5 MeV; 28Si(12C, 12C), E(cm)=18.9 MeV; 24Mg(32S, 32S), E(cm)=47.1 MeV; 62Ni(35Cl, 35Cl), E(cm)=63.9 MeV; analyzed σ(θ); 9Be(12C, X), E(cm)=4-16 MeV; 12C(16O, X), E(cm)=8-28 MeV; 16O(16O, X), E(cm)=12-40 MeV; 28Si(6Li, X), E(cm)=6-20 MeV; 28Si(9Be, X), E(cm)=8-22 MeV; 28Si(12C, X), E(cm)=12-25 MeV; 24Mg(16O, X), E(cm)=18-44 MeV; 40Ca(16O, X), E(cm)=24-54 MeV; 24Mg(32S, X), E(cm)=30-52 MeV; 62Ni(35Cl, X), E(cm)=60-110 MeV; calculated σ(E). Double folding model.
doi: 10.1088/0305-4616/7/10/017
1981HU08 Nucl.Phys. A368, 173 (1981) M.Hugi, J.Lang, R.Muller, E.Ungricht, K.Bodek, L.Jarczyk, B.Kamys, A.Magiera, A.Strzalkowski, G.Willim Fusion and Direct Reactions for Strongly and Weakly Bound Projectiles NUCLEAR REACTIONS 28Si(6Li, p), (6Li, d), (6Li, α), (6Li, 6Li), E(cm)=10.7, 16.5, 20.6 MeV; 28Si(9Be, p), (9Be, α), (9Be, 8Be), (9Be, 9Be), E(cm)=9.1, 10.6, 12.9, 15.1, 17.4, 19.7, 22.7 MeV; 28Si(12C, p), (12C, d), (12C, α), E(cm)=15.4, 18.9, 25.2 MeV; measured σ(θ); deduced σ(fusion), σ(direct), σ(reaction). Optical, statistical model analyses.
doi: 10.1016/0375-9474(81)90739-9
1981HU12 Fizika(Zagreb) 13, Suppl.No.1, 13 (1981) M.Hugi, J.Lang, R.Muller, J.Sromicki, E.Ungricht, L.Jarczyk, A.Strzalkowski, H.Witala Statistical Significance of the Deviation Function in a Search for Resonances NUCLEAR REACTIONS 9Be(12C, p), (12C, d), (12C, t), (12C, α), (12C, 8Be), (12C, 12C), E(cm)=6-15 MeV; measured σ(θ, E); deduced deviation function confidence limits.
1981JA09 Nucl.Phys. A369, 191 (1981) L.Jarczyk, B.Kamys, A.Magiera, J.Sromicki, A.Strzalkowski, G.Willim, Z.Wrobel, D.Balzer, K.Bodek, M.Hugi, J.Lang, R.Muller, E.Ungricht Energy Dependence of Fusion and Reaction Cross Sections in the 9Be + 12C System NUCLEAR REACTIONS 12C(9Be, p), (9Be, d), (9Be, t), (9Be, α), E=12, 14, 17, 20, 23.5, 27 MeV; measured σ(E, θ); deduced σ(reaction), σ(fusion), L(cut-off) from the interaction potential.
doi: 10.1016/0375-9474(81)90015-4
1981LA15 Phys.Lett. 104B, 369 (1981) J.Lang, M.Hugi, R.Muller, J.Sromicki, E.Ungricht, H.Witala, L.Jarczyk, A.Strzalkowski Statistical Significance of the Deviation Function in a Search for Resonances NUCLEAR REACTIONS 9Be(12C, d), (12C, α), (12C, 8Be), E(cm)=6-15 MeV; calculated σ(E); deduced resonance structure. Statistical model, energy-dependent deviation function.
doi: 10.1016/0370-2693(81)90700-0
1980BO11 Nucl.Phys. A339, 353 (1980) K.Bodek, M.Hugi, J.Lang, R.Muller, E.Ungricht, K.Jankowski, W.Kipper, L.Jarczyk, A.Strzalkowski, G.Willim, H.Witala The Energy Dependence of Fusion in the 9Be + 28Si System NUCLEAR REACTIONS 28Si(9Be, p), (9Be, d), (9Be, α), E=12-30 MeV; measured σ(Ep, θ), σ(Ed, θ). 28Si(9Be, 9Be), E=12, 17, 23, 30 MeV; measured σ(θ); deduced fusion parameters, fusion σ(E), reaction σ(E). Optical, statistical model analyses.
doi: 10.1016/0375-9474(80)90099-8
1980BO14 Phys.Lett. 92B, 79 (1980) K.Bodek, M.Hugi, J.Lang, R.Muller, A.Schiltz, J.Sromicki, E.Ungricht, L.Jarczyk, A.Strzalkowski Transfer Processes in the Elastic Scattering of 10B on 9Be NUCLEAR REACTIONS 9Be(10B, 10B), E=9.5, 14.2 MeV; measured σ(θ). Optical model, compound nucleus, proton transfer effects.
doi: 10.1016/0370-2693(80)90308-1
1980BO21 J.Phys.(London) G6, 1017 (1980) K.Bodek, M.Hugi, L.Jarczyk, B.Kamys, J.Lang, R.Muller, M.Porebska, J.Sromicki, A.Strzalkowski, E.Ungricht, D.Balzer Nuclear Reactions in the 13C + 9Be System at CM Energies around 11.6 MeV NUCLEAR REACTIONS 13C(9Be, p), (9Be, d), (9Be, t), (9Be, α), E(cm)=11.4 MeV; 13C(9Be, 8Be), E(cm)=11.8 MeV; measured σ(θ); deduced σ(fusion), l(fusion).
doi: 10.1088/0305-4616/6/8/010
1980BO29 Helv.Phys.Acta 53, 306 (1980) K.Bodek, M.Hugi, L.Jarczyk, J.Lang, R.Mueller, A.Schiltz, J.Sromicki, A.Strzalkowski, E.Ungricht Transferprozesse bei der Elastischen Streuung von 10B an 9Be NUCLEAR REACTIONS 9Be(10B, 10B), E=9.5, 14.2 MeV; measured σ(θ); deduced reaction mechanism.
1980HU09 J.Phys.(London) G6, 1257 (1980) M.Hugi, L.Jarczyk, B.Kamys, J.Lang, R.Muller, A.Strzalkowski, E.Ungricht, W.Zipper Fusion and the Potential for Elastic Scattering NUCLEAR REACTIONS 28Si(6Li, 6Li), E(cm)=10.7, 16.5, 20.6 MeV; 28Si(9Be, 9Be), E=10.6, 15.1, 19.7, 22.7 MeV; 28Si(12C, 12C), E=15.4, 18.9, 25.2 MeV; calculated σ(fusion), l(fusion); deduced strong absorption localization, barrier radii. Woods-Saxon optical , folding potential analyses.
doi: 10.1088/0305-4616/6/10/012
1979BO06 Phys.Lett. 82B, 369 (1979) K.Bodek, M.Hugi, J.Lang, R.Muller, E.Ungricht, L.Jarczyk, B.Kamys, A.Strzalkowski A Search for Resonances in 9Be + 12C Reactions in the Energy Range from 11.4 MeV to 14.8 MeV (CM) NUCLEAR REACTIONS 9Be(12C, p), (12C, d), (12C, t), (12C, α), (12C, 8Be), 12C(9Be, p), (9Be, d), (9Be, t), (9Be, α), E(cm)=11.4-14.8 MeV; measured excitation curves, σ(θ(8Be)). DWBA analysis, n-, α-transfer, compound nucleus formation.
doi: 10.1016/0370-2693(79)90244-2
1979JA04 Nucl.Phys. A316, 139 (1979) L.Jarczyk, J.Okolowicz, A.Strzalkowski, K.Bodek, M.Hugi, J.Lang, R.Muller, E.Ungricht Large Angle Elastic Scattering of 9Be Ions on Carbon Isotopes NUCLEAR REACTIONS 12C(9Be, 9Be), E=20.0, 26.0 MeV; 9Be(13C, 13C), E=28.1, 36.2 MeV; measured σ(θ). Optical model, finite range DWBA calculations.
doi: 10.1016/0375-9474(79)90676-6
1979JA05 J.Phys.(London) G5, 565 (1979) L.Jarczyk, B.Kamys, A.Strzalkowski, M.Hugi, J.Lang, R.Muller, E.Ungricht Neutron and Alpha-Particle Transfer Processes in the Reaction 12C(9Be, 8Be)13C NUCLEAR REACTIONS 12C(9Be, 8Be), E=20 MeV; measured σ(θ). 13C levels deduced S for n-, α-transfer. Finite range DWBA analysis.
doi: 10.1088/0305-4616/5/4/020
1979JA22 Nucl.Phys. A325, 510 (1979) L.Jarczyk, B.Kamys, J.Okolowicz, J.Sromicki, A.Strzalkowski, H.Witala, Z.Wrobel, M.Hugi, J.Lang, R.Muller, E.Ungricht Light Charged-Particle Production in the 9Be + 12C Reaction at 11.4 MeV c.m. Energy NUCLEAR REACTIONS 12C(9Be, p), (9Be, d), (9Be, t), (9Be, α), E(cm)=11.4 MeV; measured σ(θ); deduced σ(fusion), cutoff L, reaction mechanism, spin selectivity .
doi: 10.1016/0375-9474(79)90029-0
1979UN01 Nucl.Phys. A313, 376 (1979) E.Ungricht, D.Balzer, M.Hugi, J.Lang, R.Muller, L.Jarczyk, B.Kamys, A.Strzalkowski Elastic Scattering of 9Be on Light Target Nuclei NUCLEAR REACTIONS 9Be, 12C, 13C, 16O(9Be, 9Be), E=14, 20, 26 MeV; measured σ(θ). 9Be(9Be, 9Be), E=9-22 MeV; measured σ(E); deduced optical model parameters.
doi: 10.1016/0375-9474(79)90507-4
1978JA07 Phys.Rev. C17, 2106 (1978) L.Jarczyk, J.Okolowicz, A.Strzalkowski, H.Witala, W.Zipper, J.Lang, R.Muller, E.Ungricht, J.Unternahrer Localization of Various Reaction Processes for Weakly Bound Heavy Projectiles NUCLEAR REACTIONS 28Si(9Be, 9Be), (9Be, α), (9Be, p), E=20 MeV; measured σ(E, θ); deduced fusion σ.
doi: 10.1103/PhysRevC.17.2106
1978UN02 Helv.Phys.Acta 51, 115 (1978) J.Unternahrer, M.Hugi, J.Lang, R.Muller, E.Ungricht, L.Jarczyk, B.Kamys, A.Strzalkowski Kernreaktionen mit 9Be NUCLEAR REACTIONS Mg, Al, Si, Ca, Ni, Ag, Au(9Be, 9Be), E=14, 20, 26 MeV; measured σ(θ). Optical model analysis. 28Si, 40Ca(9Be, 8Be), E=20 MeV; measured σ(θ). 9Be deduced S. DWBA analysis. Ag(9Be, n8Be), E=18, 20, 23, 26 MeV; measured σ(E(Be), θ(n), θ(Be)). Comparison with semi-classical model.
1977BA71 Nucl.Phys. A293, 518 (1977) R.Balzer, M.Hugi, B.Kamys, J.Lang, R.Muller, E.Ungricht, J.Unternahrer, L.Jarczyk, A.Strzalkowski Elastic Scattering of 9Be on Heavy Target Nuclei NUCLEAR REACTIONS Mg, 27Al, 28Si, 40Ca, 58Ni, Ag, 197Au(9Be, 9Be), E=14, 20, 26 MeV; measured σ(θ). 28Si(9Be, 9Be), E=14-20 MeV; measured σ(E); deduced optical model parameters.
doi: 10.1016/0375-9474(77)90111-7
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