NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = H.J.Emrich Found 17 matches. 1997TE11 Phys.Rev. C56, 2597 (1997) L.A.A.Terremoto, V.P.Likhachev, M.N.Martins, H.J.Emrich, G.Fricke, T.Krohl, K.W.Neff Giant Resonances in the 26Mg(e, e'α0)22Ne Reaction NUCLEAR REACTIONS 26Mg(e, e'α), E=14-26 MeV; measured eα-coin, σ(Eα, Ee, θ(α), θ(e)); deduced multipole components, sum rules. 22Ne deduced resonances.
doi: 10.1103/PhysRevC.56.2597
1995DE23 Phys.Rev. C52, 61 (1995) D.J.DeAngelis, J.R.Calarco, J.E.Wise, H.J.Emrich, R.Neuhausen, H.Weyand Multipole Strength in 12C from the (e, e'α) Reaction for Momentum Transfers up to 0.61 fm -1 NUCLEAR REACTIONS 12C(e, e'p), (e, e'α), E=124.1, 183.4 MeV; measured σ(θ(e'), θ(α)), σ(θ(e'), θ(p)) vs energy transfer. 12C deduced B(E2), EWSR strength.
doi: 10.1103/PhysRevC.52.61
1993DE10 Phys.Rev.Lett. 70, 2872 (1993) D.De Angelis, J.R.Calarco, J.E.Wise, H.J.Emrich, R.Neuhausen, H.Weyand Isoscalar E2 Strength in 12C from the (e, e'α) Reaction NUCLEAR REACTIONS 12C(e, e'α), E=124.1-183.4 MeV; measured σ(θ(e), θ(α)) vs energy transfer. 12C deduced GQR associated EWSR, B(E2).
doi: 10.1103/PhysRevLett.70.2872
1992FR05 Phys.Rev.Lett. 68, 1667 (1992) J.P.Fritsch, H.J.Emrich, A.Grasmuck, R.Neuhausen, S.Schardt, N.Zimmermann, J.R.Calarco, M.Potokar Isoscalar E2 Strength in 16O from the (e, e'α) Reaction NUCLEAR REACTIONS 16O(e, e'α), E=124.1, 183.4 MeV; measured σ(θ(e), θα). 16O deduced isoscalar electric quadrupole strength distribution.
doi: 10.1103/PhysRevLett.68.1667
1991BR13 Nucl.Phys. A527, 369c (1991) V.Breton, P.Bricault, L.S.Cardman, H.J.Emrich, B.Frois, D.Goutte, P.Gueye, F.W.Hersman, D.B.Isabelle, C.W.de Jager, N.Kalantar-Nayestanaki, A.W.Linzey, L.C.Maximon, E.A.J.M.Offermann, X.H.Phan, S.K.Platchkov, D.Rychel, I.Sick, H.de Vries, S.E.Williamson Experimental Measurements of Dispersive Effects in Electron and Positron Scattering from Nuclei NUCLEAR REACTIONS 12C(e, e), E=238-690 MeV; measured σ; deduced energy dependence causes. Comparison with static analysis fits. Other data analyzed.
doi: 10.1016/0375-9474(91)90126-Q
1991PO06 Nucl.Phys. A527, 372c (1991) M.Potokar, J.R.Calarco, J.E.Wise, N.Zimmermann, H.Weyand, H.J.Emrich, J.P.Fritsch, A.Grasmuck, R.Neuhausen, S.Schardt Separation of the Longitudinal and Transverse Amplitudes for the Giant Dipole Resonances of 12C and 16O from Measurement of the (e, e'p0) Angular Correlations NUCLEAR REACTIONS 12C, 16O(e, e'p), E not given; measured σ(θ(e'), θ(p)) vs energy transfer. 12C, 16O deduced GDR amplitudes features.
doi: 10.1016/0375-9474(91)90126-Q
1990WE07 Nucl.Phys. A510, 1 (1990) Th.Weber, R.D.Heil, U.Kneissl, W.Wilke, Th.Kihm, K.T.Knopfle, H.J.Emrich (e, e'f) Coincidence Experiments on 235U and 238U NUCLEAR REACTIONS 235,238U(e, e'F), E=78-183 MeV; measured σ(θ(e'), E, θ(fragment)), in-, out-of-plane fission fragment σ(θ), fragment time-of-flight differences. 235,238U deduced multipole strength distributions for giant E0, E1, E2, E3 resonances, fission characteristics.
doi: 10.1016/0375-9474(90)90286-U
1989KA36 Phys.Rev.Lett. 63, 2032 (1989) N.Kalantar-Nayestanaki, C.W.de Jager, E.A.J.M.Offermann, H.de Vries, L.S.Cardman, H.J.Emrich, F.W.Hersman, H.Miska, D.Rychel Energy Dependence of Dispersive Effects in 12C NUCLEAR REACTIONS 12C(e, e), E=238-690 MeV; measured σ at form factor minimum; deduced higher order processes role.
doi: 10.1103/PhysRevLett.63.2032
1989WE01 Phys.Rev.Lett. 62, 129 (1989) Th.Weber, R.D.Heil, U.Kneissl, W.Wilke, H.J.Emrich, Th.Kihm, K.T.Knopfle Evidence for Different Mass Splits in Fission Decays of Giant Multipole Resonances from 235,238U(e, e'f) Reactions NUCLEAR REACTIONS 235,238U(e, e'F), E=185 MeV; measured fission (fragment)(fragment)-coin. 235,238U deduced giant multipole resonance fission decay features, Γ(S)/Γ(A).
doi: 10.1103/PhysRevLett.62.129
1989WE12 Nucl.Phys. A502, 279c (1989) Th.Weber, W.Wilke, H.J.Emrich, R.D.Heil, Th.Kihm, U.Kneissl, K.T.Knopfle, U.Seemann, F.Steiper, H.Stroher Evidence for Different Fission Fragment Mass Asymmetries for Specific Nuclear Excitations Studied in (e, e'F) and (γ, F) Reactions NUCLEAR REACTIONS 236U(e, e'F), E not given; measured fission fragment σ(θ). 235,238U(e, e'F), E=185 MeV; measured fission fragment spectra; deduced symmetric, asymmetric fission yield ratios, excitation multipolarity role.
doi: 10.1016/0375-9474(89)90668-4
1988WE18 Phys.Lett. 215B, 469 (1988) Th.Weber, R.D.Heil, U.Kneissl, W.Wilke, H.J.Emrich, Th.Kihm, K.T.Knopfle Near Barrier Fission Channels (J(π), K) in 238U for Spins J(π) = 0+, 1-, and 2+ from (e, e'f) Angular Correlation Measurements NUCLEAR REACTIONS 238U(e, e'F), E=185 MeV; measured fission (fragment)(fragment)(θ), in-plane, out-of-plane; deduced partial fission channel σ. 238U levels deduced fission barriers.
doi: 10.1016/0370-2693(88)91343-3
1987WE09 Phys.Rev.Lett. 59, 2028 (1987) Th.Weber, R.D.Heil, U.Kneissl, W.Pecho, W.Wilke, H.J.Emrich, Th.Kihm, K.T.Knopfle Multipole Strength Distributions and Form Factors for E1, E2/E0, and E3 from 238U(e, e'f) Coincidence Experiments NUCLEAR REACTIONS 238U(e, e'F), E=78, 183, 124 MeV; measured fission (fragment)(fragment)-coin. 238U deduced multipole strength distributions, form factors.
doi: 10.1103/PhysRevLett.59.2028
1986KI09 Phys.Rev.Lett. 56, 2789 (1986) Th.Kihm, K.T.Knopfle, H.Riedesel, P.Voruganti, H.J.Emrich, G.Fricke, R.Neuhausen, R.K.M.Schneider E1 and E2-E0 Form Factors and Strength Distributions from 28Si(e, e'p) and 28Si(e, e'α) Coincidence Scattering NUCLEAR REACTIONS 28Si(e, e'p), (e, e'α), E=183.5 MeV; measured e'p-, e'α-coin, σ(E(e')). 28Si deduced form factors, giant resonances, multipole transition strength distribution.
doi: 10.1103/PhysRevLett.56.2789
1986OF01 Phys.Rev.Lett. 57, 1546 (1986) E.A.J.M.Offermann, L.S.Cardman, H.J.Emrich, G.Fricke, C.W.de Jager, H.Miska, D.Rychel, H.de Vries Search for Dispersive Effects in Elastic Electron Scattering from 12C NUCLEAR REACTIONS 12C(e, e), E=238, 374.5, 419, 747.2 MeV; analyzed from factor; deduced dispersive effect induced energy dependence.
doi: 10.1103/PhysRevLett.57.1546
1985WO06 Nucl.Phys. A438, 711 (1985) U.Worsdorfer, H.J.Emrich, H.Miska, D.Rychel, R.Gyufko, C.A.Wiedner Determination of the Transition Charge Densities of the Low-Lying 2+ States in 34S NUCLEAR REACTIONS 34S(e, e'), E=120, 240, 320 MeV; measured σ(θ, E(e')). 34S levels deduced B(E2), transition densities. Enriched targets.
doi: 10.1016/0375-9474(85)90014-4
1983EM01 Nucl.Phys. A396, 401c (1983) H.J.Emrich, G.Fricke, G.Mallot, H.Miska, H.-G.Sieberling, J.M.Cavedon, B.Frois, D.Goutte Radial Distribution of Nucleons in the Isotopes 48,40Ca NUCLEAR REACTIONS 48Ca(e, e), E=350, 600 MeV; measured σ(θ). 48,40Ca(e, e), E=100, 210, 320 MeV; measured σ(θ) ratio. 40,48Ca deduced radial charge distribution, differences, neutron distribution difference.
doi: 10.1016/0375-9474(83)90034-9
1983RY04 Phys.Lett. 130B, 5 (1983) D.Rychel, H.J.Emrich, H.Miska, R.Gyufko, C.A.Wiedner Charge Distribution of the Even Sulphur Isotopes from Elastic Electron Scattering NUCLEAR REACTIONS 32,34,36S(e, e), E=120, 240, 320 MeV; measured σ(θ); deduced σ. 32,34,36S deduced rms radii, differences, charge distributions.
doi: 10.1016/0370-2693(83)91051-1
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