NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = E.Kuhlmann Found 41 matches. 2008AB06 Phys.Lett. B 662, 14 (2008) M.Abdel-Bary, K.-Th.Brinkmann, H.Clement, J.Dietrich, E.Doroshkevich, S.Dshemuchadse, K.Ehrhardt, A.Erhardt, W.Eyrich, H.Freiesleben, A.Gillitzer, J.Gottwald, R.Jakel, L.Karsch, K.Kilian, E.Kuhlmann, H.P.Morsch, C.Pizzolotto, S.Reimann, J.Ritman, E.Roderburg, W.Schroeder, M.Schulte-Wissermann, T.Sefzick, G.Y.Sun, A.Teufel, W.Ullrich, R.Wenzel, P.Wintz, P.Wustner, P.Zupranski, for the COSY-TOF Collaboration Analyzing power Ay for ω meson production in proton-proton collisions NUCLEAR REACTIONS 1H(polarized p, p'X), E at 3065 MeV/c; measured Ay(θ), missing mass spectra for ω meson production.
doi: 10.1016/j.physletb.2008.02.035
2008AB11 Eur.Phys.J. A 36, 7 (2008) M.Abdel-Bary, K.-Th.Brinkmann, H.Clement, E.Doroshkevich, S.Dshemuchadse, A.Erhardt, W.Eyrich, H.Freiesleben, A.Gillitzer, R.Jakel, L.Karsch, K.Kilian, E.Kuhlmann, K.Moller, H.P.Morsch, L.Naumann, N.Paul, C.Pizzolotto, J.Ritman, E.Roderburg, W.Schroeder, M.Schulte-Wissermann, Th.Sefzick, A.Teufel, A.Ucar, W.Ullrich, P.Wintz, P.Wustner, P.Zupranski, and the COSY-TOF Collaboration Single π- production in np collisions for excess energies up to 90 MeV NUCLEAR REACTIONS 1H(d, pX), E at 1.85 GeV/c; measured σ(θ), σ(E'), invariant mass distributions; deduced final state interaction effects.
doi: 10.1140/epja/i2007-10543-x
2006AB42 Eur.Phys.J. A 29, 353 (2006) M.Abdel-Bary, K.-Th.Brinkmann, H.Clement, E.Doroshkevich, S.Dshemuchadse, A.Erhardt, W.Eyrich, H.Freiesleben, A.Gillitzer, R.Jakel, L.Karsch, K.Kilian, E.Kuhlmann, K.Moller, H.P.Morsch, L.Naumann, N.Paul, C.Pizzolotto, J.Ritman, E.Roderburg, P.Schonmeier, W.Schroeder, M.Schulte-Wissermann, G.Y.Sun, A.Teufel, A.Ucar, G.J.Wagner, M.Wagner, P.Wintz, P.Wustner, P.Zupranski, and the COSY-TOF Collaboration Study of spectator tagging in the reaction np → ppπ with a deuteron beam NUCLEAR REACTIONS 1H(d, 2pπ-), E=759 MeV; measured Ep, En, angular distributions; deduced quasifree reaction features.
doi: 10.1140/epja/i2006-10099-3
1998BI04 Phys.Lett. 420B, 217 (1998) R.Bilger, A.Bohm, H.Brand, S.Brand, K.-Th.Brinkmann, H.Clement, M.Dellert, H.Dennert, W.Eyrich, D.Filges, H.Freiesleben, M.Fritsch, R.Geyer, A.Hassan, J.Hauffe, P.Herrmann, B.Hubner, P.Jahn, K.Kilian, M.Kirsch, H.Koch, J.Kress, J.Krug, E.Kuhlmann, J.S.Lange, A.Metzger, P.Michel, K.Moller, M.Moosburger, H.P.Morsch, Ch.Nake, H.Nann, B.Naumann, L.Naumann, P.Ringe, E.Roderburg, M.Rogge, A.Schamlott, P.Schonmeier, A.Schulke, R.Sperl, M.Steinke, F.Stinzing, P.Turek, G.J.Wagner, S.Wirth, U.Zielinski Strangeness Production in the Reaction pp → K+ Λp in the Threshold Region NUCLEAR REACTIONS 1H(p, pX), E at 2.50, 2.75 GeV/c; measured total σ for pK+Λ final state, kaon, Λ, proton σ(E, θ), Λ-polarization.
doi: 10.1016/S0370-2693(97)01573-6
1995HA23 Nucl.Phys. A595, 287 (1995) D.Hager, K.Fuhrberg, T.Glebe, M.Hutt, M.Ludwig, M.Schumacher, B.E.Andersson, K.Hansen, B.Nilsson, B.Schroder, L.Nilsson, H.Freiesleben, E.Kuhlmann Elastic Scattering of 58 and 75 MeV Photons by 12C and 16O and Electromagnetic Polarizabilities of the Bound Nucleon NUCLEAR REACTIONS 16O, 12C(γ, γ), E=58, 75 MeV; measured σ(θ); deduced bound nucleon electromagnetic polarizabilities. Tagged photon beam.
doi: 10.1016/0375-9474(95)00379-4
1993RO29 Acta Phys.Pol. B24, 1629 (1993) E.Roderburg, R.Bilger, H.Brand, S.Brand, H.Clement, M.Dahmen, P.Cloth, V.Druke, W.Eyrich, H.Freiesleben, D.Filges, P.Jahn, K.Kilian, M.Kirsch, H.Koch, R.A.Kraft, J.Krug, E.Kuhlmann, S.Lange, H.Machner, H.Matthay, P.Michel, K.Moller, H.P.Morsch, C.Nake, B.Naumann, L.Naumann, W.Oelert, N.Paul, P.Ringe, E.Roderburg, K.Rohrich, A.Roser, M.Rogge, G.Schmidt, T.Sefzick, M.Steinke, F.Stinzing, V.Stobik, R.Stratmann, P.Turek, S.Wirtz, and the COSY-TOF Collaboration Studies of (Eta) and (Eta') Measurements with the Time of Flight Spectrometer at COSY NUCLEAR REACTIONS 2H(p, X), E at 0.88-1.5 GeV/c; compiled, reviewed, calculated eta production data. Monte Carlo simulations.
1993WA20 Nucl.Phys. A564, 595 (1993) M.Waters, H.Machner, D.Gotta, K.Kilian, P.Turek, D.Grzonka, G.Gaul, R.Santo, T.Manz, J.Ernst, E.Grosse, E.Kuhlmann Subthreshold π0-Production in the Reactions 24Mg(α, π0)X at 43 MeV.A and 24Mg(16O, π0)X at 24 and 33 MeV.A NUCLEAR REACTIONS 24Mg(16O, π0X), E=383, 522 MeV; 24Mg(α, π0X), E=172 MeV; measured σ(E(π0), θ(π0)).
doi: 10.1016/0375-9474(93)90215-J
1990ER04 JUL-Spez-562, p.11 (1990) J.Ernst, G.Gaul, D.Gotta, E.Grosse, D.Grzonka, K.Kilian, E.Kuhlmann, H.Machner, T.Manz, R.Santo, P.Turek, M.Waters Subthreshold π0 Production in Heavy Ion Collisions NUCLEAR REACTIONS 24Mg(16O, π0X), E=24-43 MeV/nucleon; measured invariant mass spectra.
1988DE18 Z.Phys. A330, 93 (1988) Gammadecay of Quasimolecular Resonances in the 12C + 12C System NUCLEAR REACTIONS, ICPND 12C(12C, γ), E(cm)=4.7-6 MeV; measured γ yield, σ(θ) vs E. 12C(12C, αγ), (12C, pγ), (12C, nγ), E(cm)=4.7-6 MeV; measured σ(E); deduced γ-ray strength. 24Mg resonances deduced Γ(capture)/Γ. Hauser-Feshbach calculations. Natural targets. NaI spectrometer.
1988PU01 Nucl.Phys. A480, 397 (1988) H.Putsch, T.M.Krischak, E.Kuhlmann Statistical Giant Resonance Effects in Heavy-Ion Radiative Capture NUCLEAR REACTIONS 9Be(12C, γ), 16O(7Li, γ), E(cm)=3-9 MeV; measured E(γ), σ(θ=90°). 21Ne deduced GDR statistical strength (S). Hauser-Feshbach calculations. Natural targets. NaI spectrometer.
doi: 10.1016/0375-9474(88)90403-4
1986BE33 Phys.Rev. C34, 1991 (1986) B.Bellenberg, H.Hemmert, E.Kuhlmann Width of the Second T = 3/2 State in 9Be NUCLEAR REACTIONS 7Li(d, γ), E ≈ 0.36 MeV; measured thick target yields. 9Be levels deduced Γ, Γd, Γγ, Γp, Γn, Γα. Enriched target, NaI crystal.
doi: 10.1103/PhysRevC.34.1991
1986GL02 Nucl.Phys. A452, 150 (1986) K.Glasner, L.Ricken, E.Kuhlmann Study of the 6Li + 16O Light Heavy-ion System around the Coulomb Barrier NUCLEAR REACTIONS, ICPND 16O(6Li, p), E=4.5-8 MeV; measured σ(E, θ, ); 16O(6Li, pγ), (6Li, nγ), (6Li, αγ), E=4.1-12.5 MeV; measured σ(E); deduced coherence width. 22Na deduced intermediate-structure resonance, Γ. Natural targets. Hauser-Feshbach calculations, statistical analysis.
doi: 10.1016/0375-9474(86)90513-0
1986SC28 Z.Phys. A325, 203 (1986) C.J.S.Scholz, L.Ricken, E.Kuhlmann Complete Fusion of 7Li + 16O in the Region of the Coulomb Threshold NUCLEAR REACTIONS, ICPND 16O(7Li, pγ), (7Li, nγ), (7Li, dγ), (7Li, tγ), (7Li, αγ), (7Li, 2αγ), (7Li, pαγ), (7Li, nαγ), (7Li, 2nγ), E=4-10 MeV; measured γ production σ(E), Eγ, Iγ, nγ-coin, γ yields; deduced model parameters, fusion σ(E), L(critical).
1985KU22 Z.Phys. A322, 527 (1985) Implications of Experimental Isospin Mixing Data on the Spreading Width NUCLEAR STRUCTURE A=20-140; calculated IAR spreading width, Coulomb matrix element mass dependence correlation.
doi: 10.1007/BF01412091
1985KU29 Z.Phys. A322, 701 (1985) Heavy-Ion Radiative Capture Observed in 9Be(12C, γ)21Ne NUCLEAR REACTIONS 9Be(12C, γ), E(cm)=3.5-6.6 MeV; measured Eγ, Iγ, σ(θ) vs E.
doi: 10.1007/BF01415155
1984BO36 Z.Phys. A318, 339 (1984) D.Bohle, K.Glasner, L.Ricken, E.Kuhlmann High Resolution Study of the 24Mg(α, γ0)28Si Capture Reaction NUCLEAR REACTIONS, ICPND 24Mg(α, γ), E=4.4-9.6 MeV; measured Eγ, Iγ, σ(E), σ(θ, Eγ, E), γ yields; deduced two-level interference role. 28Si deduced levels, Γ, E1, E2 contributions.
doi: 10.1007/BF01418093
1983BO19 Nucl.Phys. A405, 141 (1983) F.Borchers, H.De Jong, J.Krug, E.Kuhlmann Resonant Charged Particle Emission from 11B + p and 12C States at E(x) = 20-23 MeV NUCLEAR REACTIONS, ICPND 11B(p, p'), (p, α), E=4.5-7.55 MeV; measured σ(E, θ); deduced reaction σ. 12C deduced levels, J, π, reduced widths. Enriched target.
doi: 10.1016/0375-9474(83)90328-7
1983CA14 Phys.Rev. C28, 483 (1983); Erratum Phys.Rev. C29, 672 (1983) J.R.Calarco, S.S.Hanna, C.C.Chang, E.M.Diener, E.Kuhlmann, G.A.Fisher Absolute Cross Section for the Reaction 3H(p, γ0)4He and a Review of 4He(γ, p0)3H Measurements NUCLEAR REACTIONS 3H(p, γ0), E=8.34, 13.6 MeV; measured σ(θ=90°).
doi: 10.1103/PhysRevC.28.483
1983GL03 Phys.Rev. C27, 2977 (1983) K.Glasner, D.Bohle, G.Domogala, L.M.Ricken, J.A.Weismuller, E.Kuhlmann Test of Isospin Purity by Measuring Cross Correlations in Mirror Channel Reactions NUCLEAR REACTIONS 16O(6Li, p), (6Li, nγ), E=4-8 MeV; measured σ(E); deduced linear cross correlation coefficients, < σ(n) >/< σ(p) >, isospin conservation. 22Na deduced isospin mixing matrix element. Particle, γ-ray spectroscopy. Hauser-Feshbach calculations.
doi: 10.1103/PhysRevC.27.2977
1983KU01 Phys.Rev. C27, 948 (1983) E.Kuhlmann, K.A.Snover, G.Feldman, M.Hindi Alpha Capture into the Giant Quadrupole Resonance in 28Si NUCLEAR REACTIONS, ICPND 24Mg(α, γ), E=4.3-14 MeV; measured Eγ, Iγ, σ(E, Eγ, θγ); deduced E1, E2 capture σ. 28Si deduced E1, E2 transition strengths. Enriched target. Hauser-Feshbach formalism, isospin effects.
doi: 10.1103/PhysRevC.27.948
1983SN02 Phys.Rev. C27, 493 (1983) K.A.Snover, G.Feldman, M.M.Hindi, E.Kuhlmann, M.N.Harakeh, M.Sasao, M.Noumachi, Y.Fujita, M.Fujiwara, K.Hosono 27Al(p, γ)28Si and 27Al(3He, d)28Si to the Stretched 11.58 MeV (6-, 0) and 14.36 MeV (6-, 1) Levels NUCLEAR REACTIONS 27Al(p, γ), E ≈ 2876 keV; measured σ(Eγ, E). 28Si resonance deduced Γ, Γp, Γγ, configuration, B(M1). 27Al(3He, d), E=40, 60 MeV; measured σ(θ); deduced optical model parameters. 28Si levels deduced S, configuration. DWBA analysis.
doi: 10.1103/PhysRevC.27.493
1982RI04 Z.Phys. A306, 67 (1982) L.Ricken, D.Bohle, G.Domogala, K.Glasner, E.Kuhlmann Isoscalar E2 Transition Strengths in 10 ≤ A ≤ 48 Nuclei NUCLEAR REACTIONS 9Be(p, γ), E=320 keV; measured σ(Eγ), Iγ. 10B deduced isoscalar E2 transition strength upper limit, γ-branching ratio. Natural target, Ge(Li) detector. NUCLEAR STRUCTURE A=10-42; analyzed isoscalar E2 transition strength data; deduced neutron, proton matrix element vs mass.
doi: 10.1007/BF01413410
1981SC13 Nucl.Phys. A367, 145 (1981) J.Schwenzel, K.Glasner, P.Niermann, E.Kuhlmann Isospin Mixing Observed in the Reaction 12C(6Li, α)14N NUCLEAR REACTIONS 12C(6Li, α), E=3.2-8.0 MeV; measured σ(E, θ). 18F deduced level parameters, isospin mixing. Natural target. S-matrix analysis, Hauser-Feshbach calculations.
doi: 10.1016/0375-9474(81)90282-7
1980NI10 Z.Phys. A296, 263 (1980) P.Niermann, Z.El Tanahy, K.Glasner, J.Schwenzel, E.Kuhlmann T=1 States in 26Al NUCLEAR REACTIONS 25Mg(p, γ), E=0.3-0.4 MeV; measured σ(E, Eγ), Iγ(θ). 26Al deduced levels, γ-branching, J, π, T. Enriched target, Ge(Li), NaI(Tl) crystal detectors.
doi: 10.1007/BF01415840
1979KU06 Nucl.Phys. A318, 125 (1979) E.Kuhlmann, F.Borchers, H.De Jong, J.Krug Intermediate Structure Effects in the Reaction 23Na(p, α)20Ne NUCLEAR REACTIONS 23Na(p, α), E=4.0-8.0 MeV; measured σ(E;Eα, θ). 24Mg deduced Γ.
doi: 10.1016/0375-9474(79)90474-3
1979KU10 Phys.Rev. C20, 5 (1979) E.Kuhlmann, J.R.Calarco, V.K.C.Cheng, D.G.Mavis, J.R.Hall, S.S.Hanna E1 and E2 Strength in 32S and 34S Observed in α-Capture Reactions NUCLEAR REACTIONS 28Si(α, γ0), E=5-16 MeV; 30Si(α, γ0), E=4-15 MeV; measured σ(E, Eγ, θγ). 32,34S deduced E1, E2 strengths. Enriched targets.
doi: 10.1103/PhysRevC.20.5
1979KU13 Phys.Rev. C20, 415 (1979) Isospin Mixing in the Giant Dipole Resonance NUCLEAR REACTIONS 20,22Ne, 28,30Si(α, γ), E=4-16 MeV; measured σ(E). 24Mg, 32S deduced Coulomb matrix elements, isospin mixing in giant dipole region.
doi: 10.1103/PhysRevC.20.415
1978KU04 J.Phys.(London) G4, 239 (1978) Isoscalar and Isovector E2 Matrix Elements in the Mass A = 26 System NUCLEAR REACTIONS 25Mg(p, γ), E=0.30-0.34 MeV; measured σ(E, Eγ, θ). 26Al deduced levels, γ-branching.
doi: 10.1088/0305-4616/4/2/013
1977FI01 Phys.Rev. C15, 921 (1977) H.Fischer, D.Kamke, H.J.Kittling, E.Kuhlmann, H.Plicht, R.Schormann Electric Moments and Charge Deformation Parameters in 152,154Sm, 156Gd, And 166Er NUCLEAR REACTIONS 152,154Sm, 156Gd, 166Er(α, α'), E=11.25-12.00 MeV; measured σ(Eα', θ). 152,154Sm, 156Gd, 166Er levels deduced M(E2), M(E4), β2, β4. Enriched targets.
doi: 10.1103/PhysRevC.15.921
1977SC33 Phys.Rev. C16, 2165 (1977) R.Schormann, H.Fischer, E.Kuhlmann Amomalous Large Hexadecapole Charge Deformation Parameter in 154Gd NUCLEAR REACTIONS 154Gd(α, α'), E=11.8 MeV; measured σ(Eα'). 154Gd deduced β2, β4. Enriched target.
doi: 10.1103/PhysRevC.16.2165
1975KU06 Phys.Rev. C11, 1525 (1975) E.Kuhlmann, E.Ventura, J.R.Calarco, D.G.Mavis, S.S.Hanna E1 and E2 Strength in 24Mg and 26Mg Observed in α-Capture Reactions NUCLEAR REACTIONS 20Ne(α, γ), E=2.5-20 MeV; 22Ne(α, γ), E=4.5-16 MeV; measured σ(E, Eγ, θ(γ)). 24,26Mg deduced E1, E2 strength. Enriched targets.
doi: 10.1103/PhysRevC.11.1525
1974HA01 Phys.Rev.Lett. 32, 114 (1974) S.S.Hanna, H.F.Glavish, R.Avida, J.R.Calarco, E.Kuhlmann, R.LaCanna Evidence for a Giant Quadrupole Resonance in 16O NUCLEAR REACTIONS 15N(polarized p, γ), E=8.69, 12.6, 14.5 MeV; measured σ(E;θ), A(θ). 16O deduced resonances, J, π.
doi: 10.1103/PhysRevLett.32.114
1974KU12 Phys.Rev. C10, 1593 (1974) Analog Transitions in the A = 30 System NUCLEAR REACTIONS 29Si(p, γ), E=0.7-0.75 MeV; measured σ(E, Eγ, θ). 30P level deduced γ-branching.
doi: 10.1103/PhysRevC.10.1593
1974KU18 Z.Phys. 271, 49 (1974) E.Kuhlmann, A.Hofmann, W.Albrecht High Spin States in 21Ne NUCLEAR REACTIONS 18O(α, nγ), E=9-10.5 MeV; measured nγ-coin, σ(E, Eγ, θ), nγ(θ). 21Ne levels deduced K, J, π, γ-branching ratios.
doi: 10.1007/BF01676400
1974VE01 Nucl.Phys. A219, 157 (1974) E.Ventura, J.Calarco, C.C.Chang, E.M.Diener, E.Kuhlmann, W.E.Meyerhof Resonant Structure Observed in the 3He(3He, γ)6Be Capture Reaction NUCLEAR REACTIONS 3He(3He, γ), E=12-27 MeV; measured σ(E, θ). 6Be deduced resonances, J, π, L. Results compared with theoretical predictions. Enriched 3He gas target.
doi: 10.1016/0375-9474(74)90089-X
1973KU15 Nucl.Phys. A213, 82 (1973) E.Kuhlmann, W.Albrecht, A.Hofmann The γ-Ray Decay of Levels in 30S NUCLEAR REACTIONS 28Si(3He, n), E=7.0-10.0 MeV; measured n-γ(θ), Doppler-shift attenuation. 30S deduced levels, T1/2, J, γ-branchings. Natural, enriched targets.
doi: 10.1016/0375-9474(73)90183-8
1972RO17 Nucl.Phys. A189, 641 (1972) C.Rolfs, H.P.Trautvetter, E.Kuhlmann, F.Riess A Study of Excited States of 21Ne NUCLEAR REACTIONS 18O(α, nγ), E=4.9-11.5 MeV; measured Eγ, γγ, nγ-coin, σ(E;Eγ, θ(γ), θ(nγ), θ(γγ)), DSA. 21Ne deduced levels, J, π, γ-mixing, T1/2. Enriched target.
doi: 10.1016/0375-9474(72)90319-3
1972RO20 Nucl.Phys. A191, 209 (1972) C.Rolfs, R.Kraemer, F.Riess, E.Kuhlmann A Study of the Low-Lying States in 22Mg NUCLEAR REACTIONS 20Ne(3He, nγ), E=4.3-11.5 MeV; measured Eγ, Iγ, DSA, nγ(θ), nγ-, nγγ-coin. 22Mg deduced levels, γ-branching, J, γ-mixing, π, T1/2. Enriched target.
doi: 10.1016/0375-9474(72)90603-3
1971RO11 Nucl.Phys. A167, 449 (1971) C.Rolfs, E.Kuhlmann, F.Riess, R.Kraemer The 4433 and 6450 keV States in 21Ne NUCLEAR REACTIONS 18O(α, nγ), E=7.5-11.5 MeV; measured Eγ, σ(Eγ, En, θ(γγ), θ(nγ)), γγ-coin, nγγ-triple correlation, Doppler shift attenuation. 21Ne deduced levels, J, π, γ-mixing, T1/2. Enriched target.
doi: 10.1016/0375-9474(71)90056-X
1969RO11 Nucl.Phys. A129, 231 (1969) C.Rolfs, W.Trost, E.Kuhlmann, R.Kramer, F.Riess Study on the Low-Lying States of 21Na NUCLEAR REACTIONS 20Ne(d, nγ), E=2.37-5.32 MeV; measured Eγ, nγ-coin, nγγ, nγ(θ). 21Na deduced levels, γ-branching, J, delta(E2/M1). Natural, enriched targets.
doi: 10.1016/0375-9474(69)90924-5
1969RO22 Nucl.Phys. A137, 481 (1969) C.Rolfs, W.Trost, F.Riess, R.Kramer, E.Kuhlmann The 3576 and 3616 keV States in 18Ne NUCLEAR REACTIONS 16O(3He, nγ), E = 9.5 - 11.5 MeV; measured σ(E;En, Eγ1, Eγ2, θ(nγ)). 18Ne deduced levels, γ-branching, J, σ(n), π. Natural target.
doi: 10.1016/0375-9474(69)90086-4
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