NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = F.Vogler Found 33 matches. 1988OL02 Phys.Rev. C37, 2665 (1988) R.Olszewski, R.Baran, A.Hofmann, S.Krell, H.W.Ortner, J.Orzechowsky, G.Schmidtlein, F.Vogler, W.List, G.R.Smith, D.Dehnhard, M.Thies Medium Effects in (π, π'γ) Angular Correlations on 12C(2+) NUCLEAR REACTIONS 12C(π, π'γ), E=116, 140, 162, 180, 226 MeV; measured π(γ)-coin, πγ(θ). Isobar-hole model.
doi: 10.1103/PhysRevC.37.2665
1987KR06 Nucl.Instrum.Methods Phys.Res. A255, 531 (1987) S.Krell, A.Hofmann, R.Olszewski, H.W.Ortner, F.Vogler Determination of the Efficiency of Gamma Detectors from Particle-Gamma Angular Correlations NUCLEAR REACTIONS 12C(α, α'γ), E=11 MeV; measured αγ(θ, φ); deduced detector efficiency.
doi: 10.1016/0168-9002(87)91223-X
1986OL07 Phys.Rev.Lett. 57, 2143 (1986) R.Olszewski, R.Baran, A.Hofmann, S.Krell, H.W.Ortner, J.Orzechowski, G.Schmidtlein, F.Vogler, G.R.Smith, W.List, D.Dehnhard, M.Thies Test of the Δ-Hole Model through the Energy Dependence of (π, π'γ) Angular Correlations on 12C NUCLEAR REACTIONS 12C(π, π'γ), E=116, 140, 162, 180, 226 MeV; measured πγ(θ), πγ(φ); deduced isobar-nucleus dynamics role. NaI detectors. Isobar-hole model.
doi: 10.1103/PhysRevLett.57.2143
1984KY01 Phys.Rev.Lett. 52, 974 (1984) G.S.Kyle, P.-A.Amaudruz, Th.S.Bauer, J.J.Domingo, C.H.Q.Ingram, J.Jansen, D.Renker, J.Zichy, R.Stamminger, F.Vogler Interference Effects in 16O(π(±), π(±)p)15N and Δ-Nucleus Interactions NUCLEAR REACTIONS 16O(π+, π+p), (π-, π-p), E=240 MeV; measured σ(Ep), σ(E(15N)), σ(Eπ, θπ, θp); deduced σ(π+)/σ(π-), quasifree process, isobar-nucleus interaction interference effects. Kinematically complete experiment.
doi: 10.1103/PhysRevLett.52.974
1984SM03 Phys.Rev. C29, 2206 (1984) G.R.Smith, E.L.Mathie, E.T.Boschitz, C.R.Ottermann, S.Mango, J.A.Konter, M.Daum, M.Meyer, R.Olszewski, F.Vogler Measurements of the Vector Analyzing Power iT11 in the πd(pol) Elastic Scattering Reaction between 117 and 325 MeV NUCLEAR REACTIONS 2H(π+, π+), E=117-325 MeV; measured iT11(θ) vs E; deduced dibaryon resonance effects. Vector polarized target. Faddeev calculation comparison.
doi: 10.1103/PhysRevC.29.2206
1984VO04 Phys.Lett. 134B, 161 (1984) F.Vogler, R.Olszewski, M.Meyer, E.L.Mathie, G.R.Smith, E.Boschitz, S.Chakravarti, D.Dehnhard, M.Thies Measurement of the 12C(π, π'γ)12C(2+, T = 0; 4.44 MeV) Angular Correlations: A test of the isobar-hole model NUCLEAR REACTIONS 12C(π+, π+'), E=162 MeV; measured σ(θ), σ(θπ, θγ); deduced isobar-hole model validity.
doi: 10.1016/0370-2693(84)90662-2
1983MA74 Phys.Rev. C28, 2558 (1983) E.L.Mathie, G.R.Smith, E.T.Boschitz, M.Meyer, F.Vogler, M.Daum, S.Mango, J.A.Konter Search for Rapid Angular and Energy Dependence of d(sigma)/d(Omega) and iT11 in Large Angle π-d Elastic Scattering NUCLEAR REACTIONS 2H(π, π), E=117-151 MeV; measured σ(θ), iT11(θ); deduced smooth energy dependence. Polarized target.
doi: 10.1103/PhysRevC.28.2558
1983VO08 Phys.Rev. C28, 1925 (1983) F.Vogler, J.Bottcher, W.Eyrich, A.Hofmann, M.Meyer, U.Scheib Deuteron-Gamma Angular Correlations in the Reactions 24,26Mg, 28,30Si(d, d1γ) at E(d) = 10 MeV NUCLEAR REACTIONS 24,26Mg, 28,30Si(d, d'γ), E=10 MeV; measured σ(θ), dγ(θ); deduced optical model parameter restrictions, reaction mechanism. 24,26Mg, 28,30Si deduced shape. Coupled-channels, DWBA analyses. Enriched targets.
doi: 10.1103/PhysRevC.28.1925
1982BO18 Phys.Rev.Lett. 48, 1667 (1982) J.Bolger, E.Boschitz, E.L.Mathie, G.R.Smith, M.Meyer, F.Vogler, S.Mango, J.A.Konter, G.S.Mutchler, J.Arvieux Further Measurements of iT11 in π - d(pol) Scattering as an Investigation of Dibaryon Resonance Effects NUCLEAR REACTIONS 2H(π+, π+), E=219, 256, 275, 294 MeV; measured iT11(θ); deduced dibaryon resonance effects. Polarized target. Faddeev calculations.
doi: 10.1103/PhysRevLett.48.1667
1982SM05 Phys.Rev. C25, 3228 (1982) G.R.Smith, J.Bolger, E.Boschitz, E.L.Mathie, G.Proebstle, M.Meyer, F.Vogler, S.Mango Measurement of the Vector Analyzing Power iT11 for the πd → 2p Reaction with a Polarized Target NUCLEAR REACTIONS 2H(π+, 2p), E=256 MeV; measured iT11(θ). Legendre polynomial analysis. Polarized target.
doi: 10.1103/PhysRevC.25.3228
1981BO01 Phys.Rev.Lett. 46, 167 (1981) J.Bolger, E.Boschitz, G.Probstle, G.R.Smith, S.Mango, F.Vogler, R.R.Johnson, J.Arvieux Evidence for a Dibaryon Signal in the Measurement of Elastic π+-d(pol) Scattering NUCLEAR REACTIONS 2H(π+, π+), E=142, 256 Mev; measured vector analyzing power vs θ; deduced dibaryon resonance effects at high energy. Faddeev calculations at low energies. Polarized target.
doi: 10.1103/PhysRevLett.46.167
1980AR05 Phys.Lett. 90B, 371 (1980) J.Arvieux, J.P.Albanese, M.Buenerd, J.Bolger, E.Boschitz, G.Probstle, F.Vogler, K.Gabathuler, P.A.M.Gram, J.Jansen, R.E.Mischke Pionic Excitation of Giant Resonances in 89Y NUCLEAR REACTIONS 89Y(π+, π+), (π-, π-), (π+, π+'), (π-, π-'), E=163, 240 MeV; measured σ(θ). 89Y deduced giant multipole resonance energies, energy-weighted sum rule, Γ. DWIA analysis.
doi: 10.1016/0370-2693(80)90951-X
1979EY02 Phys.Rev.Lett. 43, 1369 (1979) W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler, H.Rebel Decay of the Isoscalar Giant Resonances in 208Pb NUCLEAR REACTIONS 208Pb(α, α'), E=104 MeV; measured α'γ(θ). 208Pb deduced T=0, GQR, fine structure following n decay.
doi: 10.1103/PhysRevLett.43.1369
1979RO09 Phys.Lett. 88B, 51 (1979) H.Rost, W.Eyrich, A.Hofmann, U.Scheib, F.Vogler, H.Rebel A Study of the Giant Resonance Region of 40Ca by Inelastic Scattering Of 104 MeV α-Particles NUCLEAR REACTIONS 40Ca(α, α'), E=104 MeV; measured σ(θ). 40Ca resonances deduced L, β2, energy-weighted sum rule strengths for E2. DWBA analysis.
doi: 10.1016/0370-2693(79)90111-4
1979SC05 Phys.Lett. 80B, 180 (1979) S.Schneider, W.Eyrich, A.Hofmann, U.Scheib, F.Vogler The Influence of Deformations of the Optical Potential on Analyzing Power and p1-γ Angular Correlation in the Reaction 114Cd(p, p') NUCLEAR REACTIONS 114Cd(p, p'), E=11 MeV; measured σ(θ), A(θ), pγ(θ); deduced influence of β, spin-orbit β in optical potential. Coupled-channels analysis.
doi: 10.1016/0370-2693(79)90192-8
1979SC15 Phys.Rev. C20, 71 (1979) S.Schneider, W.Eyrich, A.Hofmann, U.Scheib, F.Vogler Reaction 114Cd(p, p') by Use of Polarized Protons and Proton-γ Angular Correlations NUCLEAR REACTIONS 114Cd(p, p'), (p, p'γ), (polarized p, p'), (polarized p, p'γ), E=11 MeV; measured σ(θ), A(θ), pγ(θ), spin flip probability. 114Cd deduced evidence against oblate deformation for harmonic vibrator model. Coupled-channel analysis. Enriched target.
doi: 10.1103/PhysRevC.20.71
1978BU04 Nucl.Phys. A297, 231 (1978) W.Buck, T.Rohwer, G.Staudt, A.Ziemke, F.Vogler Observation of the Isoscalar Giant Resonance in the Reaction 10B(d, α)8Be(g.s.) NUCLEAR REACTIONS 10B(d, α), E=0.8-9.0 MeV; measured σ(E;θ). 12C deduced isoscalar giant resonance. Enriched target.
doi: 10.1016/0375-9474(78)90273-7
1978DR05 Nucl.Phys. A301, 205 (1978) W.Draxler, W.Eyrich, A.Hofmann, U.Scheib, F.Vogler Evidence for Detour Transitions in Internal Bremsstrahlung of 90Y RADIOACTIVITY 90Sr, 90Y; measured γ CP (internal bremsstrahlung). 90Y deduced evidence for detour transitions. 90Sr+90Y source.
doi: 10.1016/0375-9474(78)90261-0
1978EY02 Fizika, Suppl. 10, 45 (1978) W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler, H.Rebel The Deformation of 26Mg from Particle-Gamma Angular Correlations NUCLEAR REACTIONS 24,26Mg, 28Si(α, α'), E=104 MeV; measured αγ(θ). 24,26Mg, 28Si level deduced β. Coupled-channels analysis.
1978HO25 Nuovo Cim. 53A, 396 (1978) P.Holleczek, A.Hofmann, U.Scheib, F.Vogler Deuteron Break-up Model Analyses of Cross-Section, Analysing Power and Angular Correlation of the Reactions 52Cr(d, p) and 58Ni(d, p) NUCLEAR REACTIONS 52Cr, 58Ni(d, p), E=10 MeV; 52Cr, 58Ni(p, p), E=5.45 MeV; calculated σ(θ), vector analyzing power, pγ(θ). Johnson-Soper adiabatic model.
1977EY03 Nucl.Phys. A287, 119 (1977) W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler, H.Rebel Alpha-Gamma Angular Correlations in the Reaction 24Mg(α, α1γ) at E = 104 MeV NUCLEAR REACTIONS 24Mg(α, α'γ), E=104 MeV; measured in-plane α'γ(θ). 24Mg deduced sign of the quadrupole deformation parameter. Coupled channels analyses, enriched target.
doi: 10.1016/0375-9474(77)90567-X
1977SC12 Lett.Nuovo Cim. 18, 301 (1977) The (d, d1) Vector Analysing Power of the Reaction 24Mg(d, d1) and the d1-γ Angular Correlation NUCLEAR REACTIONS 24Mg(polarized d, d'), E=10 MeV; measured A(θ).
doi: 10.1007/BF02784849
1976EY02 Phys.Lett. 63B, 406 (1976) W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler, H.Rebel Alpha-Gamma Angular Correlation Measurements as a Sensitive Method Determining the Sign of the Nuclear Quadrupole Deformation NUCLEAR REACTIONS 24Mg(α, α'γ), E=104 MeV; measured γγ(θ). 24Mg levels deduced sign of β2.
doi: 10.1016/0370-2693(76)90381-6
1976EY03 Nucl.Instrum.Methods 138, 543 (1976) W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler Measurement and Evaluation of Particle-γ Angular Correlations for the Study of Nuclear Reaction Mechanisms NUCLEAR REACTIONS 52Cr(d, pγ); measured pγ-coin. 24Mg(d, d'γ); measured d'γ-coin.
doi: 10.1016/0029-554X(76)90321-9
1975EY01 Phys.Rev. C11, 1658 (1975) W.Eyrich, S.Schneider, A.Hofmann, F.Vogler Gamma-Decay Data from Particle-γ Correlation Functions at Fixed γ Angles NUCLEAR REACTIONS 52Cr(d, pγ), E=10 MeV; measured σ(Ep, θ), pγ(θ). 53Cr levels deduced γ-mixing.
doi: 10.1103/PhysRevC.11.1658
1975PR08 Nucl.Phys. A255, 64 (1975) Investigation of Backward α-Particle Scattering in 24Mg and 28Si Through α-γ Angular Correlations NUCLEAR REACTIONS 24Mg(α, α'γ), E=15.5-17.0 MeV; 28Si(α, α'γ), E=15.0-16.2 MeV; measured reaction plane double-differential cross sections; Hauser-Feshbach analyses of angular correlations. Enriched targets.
doi: 10.1016/0375-9474(75)90147-5
1975SC12 Phys.Rev.Lett. 34, 1586 (1975) d-γ Angular Correlations as a Test for the Importance of Multistep Processes in the Reaction 24Mg(d, d') NUCLEAR REACTIONS 24Mg(d, d'γ), E=10 MeV; measured d'γ(θ), σ(Ed', θ); deduced optical, deformation parameters.
doi: 10.1103/PhysRevLett.34.1586
1974EY03 Phys.Rev. C10, 2512 (1974) W.Eyrich, S.Schneider, A.Hofmann, U.Scheib, F.Vogler Proton-γ Angular Correlations in the Reaction 52Cr(d, pγ)53Cr NUCLEAR REACTIONS 52Cr(d, pγ), E=10 MeV; measured σ(Ep, Eγ, θ), pγ-coin. 53Cr transitions deduced L.
doi: 10.1103/PhysRevC.10.2512
1974PR12 Phys.Rev. C10, 1577 (1974) Study of the Reaction 26Mg(p, αγ)23Na Through α-γ Angular Correlations NUCLEAR REACTIONS 26Mg(p, αγ), E=9.5, 9.75, 10.0, 10.25 MeV; measured σ(E, Eα, θ), αγ(θ). Hauser-Feshbach analysis, enriched target.
doi: 10.1103/PhysRevC.10.1577
1974VO01 Phys.Rev. C9, 242 (1974) F.Vogler, M.Berg, A.Hofmann, H.Wagner Proton-γ Angular Correlations in the Reaction 24Mg(d, pγ)25Mg NUCLEAR REACTIONS 24Mg(d, pγ), E=10 MeV; measured σ(Ep, Eγ, θ), pγ(θ). 25Mg deduced transitions.
doi: 10.1103/PhysRevC.9.242
1973SC05 Nucl.Phys. A203, 177 (1973) U.Scheib, A.Hofmann, G.Philipp, F.Vogler The Effect of the Potential Parameters on the Spectroscopic Factors of The 24Mg(d, p)25Mg Reaction NUCLEAR REACTIONS 24Mg(d, p), E=10 MeV; measured σ(Ep, θ). 25Mg levels deduced S, dependence on potential parameters. Enriched target.
doi: 10.1016/0375-9474(73)90431-4
1973WA32 Phys.Lett. 47B, 497 (1973) Determination and DWBA Analyses of Transition Matrix Elements in the Reaction 26Mg(α, α'γ)26Mg NUCLEAR REACTIONS 26Mg(α, α'), E=15 MeV; measured σ(θ).
doi: 10.1016/0370-2693(73)90025-7
1971HO31 Lett.Nuovo Cim. 2, 133 (1971) An Examination of Coupled-Channel Calculations for the Reaction 24Mg(d, p)25Mg NUCLEAR REACTIONS 24Mg(d, p), E=10 MeV; measured σ(θ). Coupled channel analysis.
doi: 10.1007/BF02772736
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