NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = R.Muller Found 102 matches. Showing 1 to 100. [Next]2019ME02 Phys.Rev. A 99, 0525014 (2019) D.-M.Meier, J.Thielking, P.Glowacki, M.V.Okhapkin, R.A.Muller, A.Surzhykov, E.Peik Electronic level structure of Th+ in the range of the 229mTh isomer energy ATOMIC PHYSICS 232Th; measured frequencies; deduced levels, angular momenta. Comparison with theoretical calculations.
doi: 10.1103/PhysRevA.99.052514
2019MU07 Phys.Rev. A 99, 042517 (2019) R.A.Muller, A.V.Volotka, A.Surzhykov Excitation of the 229Th nucleus via a two-photon electronic transition NUCLEAR STRUCTURE 229Th; calculated nuclear excitations via a two-photon electron transition (NETP), enhancement factors.
doi: 10.1103/PhysRevA.99.042517
2018MU12 Phys.Rev. A 98, 020503 (2018) R.A.Muller, A.V.Maiorova, S.Fritzsche, A.V.Volotka, R.Beerwerth, P.Glowacki, J.Thielking, D.-M.Meier, M.Okhapkin, E.Peik, A.Surzhykov Hyperfine interaction with the 229Th nucleus and its low-lying isomeric state RADIOACTIVITY 229Th(IT); measured frequencies; deduced hyperfine spectra, magnetic dipole and electric quadrupole hyperfine constants. Comparison with theoretical calculations.
doi: 10.1103/PhysRevA.98.020503
1998SE04 Nucl.Phys. A629, 423c (1998) N.Severijns, M.Allet, K.Bodek, B.A.Brown, J.Camps, P.De Moor, J.Deutsch, M.Ferro-Luzzi, F.Gimeno-Nogues, J.Govaerts, B.R.Holstein, R.Kirchner, J.Lang, R.Muller, S.Navert, O.Naviliat-Cuncic, T.Otto, I.Pepe, R.Prieels, P.A.Quin, P.Schuurmans, J.Sromicki, E.Stephan, E.Thomas, A.Van Geert, L.Vanneste, B.Vereecke, J.Zejma Helicity Structure in Low- and Intermediate-Energy Weak Interaction RADIOACTIVITY 12N, 107In(β+); measured β+ polarization asymmetry from decay of polarized nuclei; deduced weak interaction helicity structure features, W gauge boson mass lower limit.
doi: 10.1016/S0375-9474(97)00719-7
1997ZE01 Phys.Rev. C55, 42 (1997) J.Zejma, M.Allet, K.Bodek, J.Lang, R.Muller, S.Navert, O.Naviliat-Cuncic, J.Sromicki, E.Stephan, L.Jarczyk, St.Kistryn, J.Smyrski, A.Strzalkowski, W.Glockle, J.Golak, D.Huber, H.Witala, P.A.Schmelzbach Cross Sections and Analyzing Powers A(y) in the Breakup Reaction 2H(p(pol), pp)n at 65 MeV: Star configurations NUCLEAR REACTIONS 2H(polarized p, 2p), E=65 MeV; measured σ(θ1, θ2) vs arc length, analyzing power for three star configurations; deduced effects of 3-body force.
doi: 10.1103/PhysRevC.55.42
1996AL10 Phys.Lett. 376B, 255 (1996) M.Allet, K.Bodek, J.Golak, W.Glockle, W.Hajdas, D.Huber, L.Jarczyk, H.Kamada, St.Kistryn, J.Lang, R.Muller, O.Naviliat-Cuncic, J.Smyrski, J.Sromicki, A.Strzalkowski, H.Witala, J.Zejma Effects of the Tucson-Melbourne Three-Nucleon Force in the Proton-Deuteron Breakup Process at E(p) = 65 MeV NUCLEAR REACTIONS 2H(polarized p, np), E=65 MeV; analyzed σ(θ1, θ2) vs arc length, analyzing power vs (θ1, θ2). Quasi-free breakup, Tucson-Melbourne three-nucleon force.
doi: 10.1016/0370-2693(96)00259-6
1996AL23 Phys.Lett. 383B, 139 (1996) M.Allet, K.Bodek, J.Camps, J.Deutsch, M.Ferro-Luzzi, F.Gimeno-Nogues, J.Govaerts, J.Lang, R.Muller, S.Navert, O.Naviliat-Cuncic, I.Pepe, R.Prieels, P.Quin, N.Severijns, J.Sromicki, E.Stephan, E.Thomas, J.Zejma Search for Right-Handed Weak Currents in the β-Asymmetry-Polarization Correlation from 12N Decay RADIOACTIVITY 12N(β+); measured β+ polarization, polarized source; deduced right-handed gauge boson mass lower limit.
doi: 10.1016/0370-2693(96)00724-1
1996AL34 Few-Body Systems 20, 27 (1996) M.Allet, K.Bodek, W.Hajdas, J.Lang, R.Muller, S.Navert, O.Naviliat-Cuncic, J.Sromicki, J.Zejma, L.Jarczyk, St.Kistryn, J.Smyrski, A.Strzalkowski, H.Witala, W.Glockle, J.Golak, D.Huber, H.Kamada Proton-Induced Deuteron Breakup at E(p)(lab) = 65 MeV in Quasi-Free Scattering Configurations NUCLEAR REACTIONS 2H(polarized p, 2p), E=65 MeV; measured σ(θ1, θ2), analyzing power vs arc length. Kinematically complete configurations, quasi-free scattering geometry. Faddeev calculations comparison, realistic interactions.
doi: 10.1007/s006010050029
1996SR02 Phys.Rev. C53, 932 (1996) J.Sromicki, M.Allet, K.Bodek, W.Hajdas, J.Lang, R.Muller, S.Navert, O.Naviliat-Cuncic, J.Zejma, W.Haeberli Study of Time Reversal Violation in β Decay of Polarized 8Li RADIOACTIVITY 8Li(β-) [from 7Li(polarized d, p), E=10 MeV]; measured electron transverse polarizations, time reversal violating triple correlation R. Polarization transfer, Mott scattering, vector polarized source.
doi: 10.1103/PhysRevC.53.932
1995BA05 Nucl.Phys. A581, 131 (1995) J.Balewski, K.Bodek, L.Jarczyk, B.Kamys, St.Kistryn, A.Strzalkowski, W.Hajdas, R.Muller, B.Dechant, J.Krug, W.Lubcke, H.Ruhl, G.Spangardt, M.Steinke, M.Stephan, D.Kamke, R.Henneck, H.Witala, W.Glockle, J.Golak Differential Cross Section for Elastic n + d Scattering and n + d Break-Up Quasi Free-Scattering at 67 MeV NUCLEAR REACTIONS 2H(n, n), E=67 MeV; measured σ(θ). 2H(n, np), E=67 MeV; measured σ(θn, En) for np quasi-free scattering. Rigorous Faddeev calculations.
doi: 10.1016/0375-9474(94)00440-X
1995MU23 Z.Phys. A353, 103 (1995) Hadron Production in Proton-Proton Interactions at Medium Energies NUCLEAR REACTIONS 1H(p, X), E ≈ 5-10 GeV; analyzed various particle production σ(E), missing mass spectra collision model, partonic structure of hadrons based empirical matrix element.
1994AL21 Phys.Rev. C50, 602 (1994) M.Allet, K.Bodek, W.Hajdas, J.Lang, R.Muller, O.Naviliat-Cuncic, J.Sromicki, J.Zejma, L.Jarczyk, St.Kistryn, J.Smyrski, A.Strzalkowski, W.Glockle, J.Golak, H.Witala, B.Dechant, J.Krug, P.A.Schmelzbach Cross Section and Analyzing Power A(y) in the Breakup Reaction 2H(p(pol), pp)n at 65 MeV: Collinearity configurations NUCLEAR REACTIONS 2H(polarized p, 2p), E=65 MeV; measured σ(θ1, θ2) vs arc length, analyzing power. Kinematically complete configurations.
doi: 10.1103/PhysRevC.50.602
1993CO07 Phys.Lett. 304B, 60 (1993) A.Converse, M.Allet, W.Haeberli, W.Hajdas, J.Lang, J.Liechti, H.Luscher, M.A.Miller, R.Muller, O.Naviliat-Cuncic, P.A.Quin, J.Sromicki Measurement of the Asymmetry Parameter for 35Ar β-Decay as a Test of the CVC Hypothesis RADIOACTIVITY 35Ar(β+) [from 35Cl(polarized p, n)35Ar, E=9.2 MeV]; measured β-decay, βγ-coin, asymmetry parameter, Eβ, Iβ; deduced conserved vector current hypothesis implications. Polarized source.
doi: 10.1016/0370-2693(93)91400-H
1993MU13 Phys.Rev. C48, 981 (1993) R.Muller, R.Baran, U.Bohnert, P.Helbig, G.Herrmann, A.Hofmann, O.Jakel, H.Kruger, D.Malz, W.Menzel, H.-W.Ortner, L.Schweinzer, S.Wirth ππ-Angular Correlations for π-p → π+π-n in the Region of the Δ Dominance NUCLEAR REACTIONS 1H(π-, π+π-), E=284 MeV; measured σ(θ(π+), θ(π-)) vs E(π+), invariant mass distribution; deduced reaction mechanism. Weinberg's Lagrangian based models, relativistic corrections, contribution of nonlinear terms.
doi: 10.1103/PhysRevC.48.981
1993OR01 Phys.Rev. C47, R447 (1993) H.-W.Ortner, U.Bohnert, D.Malz, R.Muller, M.Dillig, O.Jakel Extraction of Total Cross Section Data for the π-p → π+π-n Reaction NUCLEAR REACTIONS 1H(π-, π-π+), E=284 MeV; analyzed data; deduced independent phase space variables distribution assumptions validity features.
doi: 10.1103/PhysRevC.47.R447
1992AL01 Phys.Rev.Lett. 68, 572 (1992) M.Allet, W.Hajdas, J.Lang, H.Luscher, R.Muller, O.Naviliat-Cuncic, J.Sromicki, A.Converse, W.Haeberli, M.A.Miller, P.A.Quin Search for Time-Reversal Violation in the Beta Decay of 8Li RADIOACTIVITY 8Li [from 7Li(polarized d, p), E=10 MeV]; measured electron transverse polarization; deduced time reversal violating triple correlation parameter.
doi: 10.1103/PhysRevLett.68.572
1992CO06 Phys.Rev. C45, 2320 (1992) A.Converse, W.Haeberli, W.Hajdas, St.Kistryn, J.Lang, J.Liechti, H.Luscher, R.Muller, J.Smyrski, J.Sromicki Absolute Calibration of the Transverse Analyzing Power in Proton-Carbon Elastic Scattering at 50.24 MeV NUCLEAR REACTIONS C(polarized p, p), E=50.24 MeV; measured analyzing power vs θ; deduced transverse analyzing power calibration.
doi: 10.1103/PhysRevC.45.2320
1992KI19 Nucl.Phys. A548, 49 (1992) St.Kistryn, W.Hajdas, J.Lang, R.Muller, J.Balewski, K.Bodek, L.Jarczyk, B.Kamys, A.Strzalkowski, B.Dechant, J.Krug, W.Lubcke, H.Ruhl, G.Spangardt, M.Steinke, M.Stephan, D.Kamke, R.Henneck, H.Witala, T.Cornelius, W.Glockle, J.Golak Analyzing Power of the 2H(n(pol), np)n Breakup Reaction at 67 MeV in Selected Kinematical Configurations NUCLEAR REACTIONS 2H(polarized n, np), E=67 MeV; measured analyzing power vs θn for np quasifree scattering, final state interactions. Rigorous Faddeev calculations.
doi: 10.1016/0375-9474(92)90076-V
1991LI32 Nucl.Phys. A533, 292 (1991) J.Liechti, M.Allet, A.Converse, J.Deutsch, F.Gimeno-Nogues, J.Lang, H.Luscher, R.Muller, O.Naviliat-Cuncic, R.Prieels, P.A.Quin, N.Severijns, J.Sromicki Production of Polarized 12N with the 12C(p(pol), 12N(pol))n0 Reaction NUCLEAR REACTIONS 12C(polarized p, 12N), E=50, 72 MeV; measured polarization transfer coefficient vs θ. DWBA analysis. RADIOACTIVITY 12N [from 12C(polarized p, 12N), E=50, 72 MeV]; measured β-decay asymmetry.
doi: 10.1016/0375-9474(91)90491-N
1990OR03 Phys.Rev.Lett. 64, 2759 (1990) H.-W.Ortner, R.Baran, U.Bohnert, M.Dillig, G.Herrmann, A.Hofmann, P.Helbig, O.Jakel, W.Kluge, H.Kruger, D.Malz, H.Matthay, R.Muller, W.Menzel, L.Schweinzer, S.Wirth Kinematically Complete Measurement of the Reaction π-p → π+π-n in the Region of Δ Dominance as a Test of Chiral Lagrangians NUCLEAR REACTIONS 1H(π-, π-π+), E=247-330 MeV; measured π+π-(θ); deduced σ(θ(π+), σ(π-)) vs π+ momentum. Kinematically complete experiment.
doi: 10.1103/PhysRevLett.64.2759
1990SR03 J.Phys.(Paris), Colloq.C-6, 527 (1990) J.Sromicki, M.Allet, A.Converse, W.Hajdas, J.Lang, H.Luscher, R.Muller, O.Naviliat-Cuncic, W.Haeberli, M.A.Miller, P.A.Quin An Experiment to Investigate Time Reversal Invariance in the Decay of 8Li RADIOACTIVITY 8Li [from 7Li(polarized d, p), E=10 MeV]; measured time reversal violating parameter.
1989KI03 Phys.Lett. 219B, 58 (1989) S.Kistryn, J.Lang, J.Liechti, H.Luscher, Th.Maier, R.Muller, M.Simonius, J.Smyrski, J.Sromicki, W.Haeberli Measurement of Parity Nonconservation in Proton-Deuteron Scattering at 43 MeV NUCLEAR REACTIONS 2H(polarized p, p), E=43 MeV; measured σ asymmetry; deduced longitudinal analyzing power.
doi: 10.1016/0370-2693(89)90837-X
1989SM05 Nucl.Phys. A501, 319 (1989) J.Smyrski, St.Kistryn, J.Lang, J.Liechti, H.Luscher, Th.Maier, R.Muller, M.Simonius, J.Sromicki, F.Foroughi, W.Haeberli A Precision Measurement of the Analyzing Power A(y) in pp Elastic Scattering at 50.04 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=50.04 MeV; measured analyzing power vs θ. Phase shift, potential model predictions comparisons.
doi: 10.1016/0375-9474(89)90296-0
1988BA27 Phys.Rev. C37, 2892 (1988) R.Baran, J.Gotz, A.Hofmann, D.Malz, R.Muller, R.Olszewski, H.W.Ortner, D.Dehnhard Excitation Function of the 15.11 MeV (1+, T=1) State in 12C from (π, π'γ) Angular Correlations NUCLEAR REACTIONS 12C(π, π'γ), E=116, 140, 162, 180, 226 MeV; measured σ(E(π)), πγ-coin. 12C levels deduced relative σ(ratio) vs E.
doi: 10.1103/PhysRevC.37.2892
1988JA14 Acta Phys.Pol. B19, 951 (1988) L.Jarczyk, B.Kamys, J.Romanski, A.Strzalkowski, M.Godlewski, J.Lang, R.Muller, J.Smyrski, J.Sromicki, H.H.Wolter Study of the Mechanism of the Five-Nucleon Transfer Reaction 12C(13C, 8Be)17O NUCLEAR REACTIONS, ICPND 12C(13C, 8Be), E(cm)=13.8-16.38 MeV; measured σ(E), σ(θ). 12C(13C, 9Be), E(cm)=13.8 MeV; 16O(9Be, 8Be), E(cm)=10.3, 12.8 MeV; measured σ(θ). 12C(13C, 13C), E=28.17, 34.67 MeV; analyzed σ(θ); deduced reaction mechanism, cluster transfer estimates.
1988LA03 Nucl.Phys. A477, 77 (1988) J.Lang, J.Liechti, R.Muller, P.A.Schmelzbach, J.Smyrski, M.Godlewski, L.Jarczyk, A.Stralkowski, H.Witala Analyzing Power of the Reaction 12C(d(pol), p) Leading to Bound and Unbound States in 13C NUCLEAR REACTIONS, MECPD 12C(polarized d, p), E=12 MeV; measured σ(θ), iT11(θ), T20(θ), T21(θ), T22(θ). 13C levels deduced spectroscopic factors. DWBA calculation.
doi: 10.1016/0375-9474(88)90361-2
1987HA31 Helv.Phys.Acta 60, 776 (1987) W.Haeberli, S. Jaccard, S.Kistryn, J.Lang, J.Liechti, Th. Maier, R.Muller, F.Nessi-Tedaldi, M.Simonius, J.Smyrski, J.Sromicki Precision Measurement of Parity Violation in 45 MeV pp Scattering NUCLEAR REACTIONS 1H(polarized p, p), E=45 MeV; measured σ helicity dependence; deduced nucleon-nucleon interaction parity violation.
1987KI09 Phys.Rev.Lett. 58, 1616 (1987) S.Kistryn, J.Lang, J.Liechti, Th.Maier, R.Muller, F.Nessi-Tedaldi, M.Simonius, J.Smyrski, S.Jaccard, W.Haeberli, J.Sromicki Precision Measurement of Parity Nonconservation in Proton-Proton Scattering at 45 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=45 MeV; measured longitudinal analyzing power; deduced parity nonconservation. Gas target, ionization chamber.
doi: 10.1103/PhysRevLett.58.1616
1986GO18 Phys.Rev. C34, 1229 (1986) M.Godlewski, J.Lang, R.Muller, P.A.Schmelzbach, J.Sromicki, L.Jarczyk, A.Strzalkowski, H.Witala, G.Baur Polarization Effects in Sub-Coulomb Breakup of Deuterons NUCLEAR REACTIONS 197Au, 208Pb(polarized d, np), E=9, 10.5, 12 MeV; measured σ(θn, θp, Ep), asymmetry following breakup, tensor analyzing power vs θn, θp, φ. Solid state detector, liquid scintillator. DWBA.
doi: 10.1103/PhysRevC.34.1229
1986LA29 Phys.Rev. C34, 1545 (1986) J.Lang, Th.Maier, R.Muller, F.Nessi-Tedaldi, Th.Roser, M.Simonius, J.Sromicki, W.Haeberli Parity Nonconservation in Elastic pα Scattering NUCLEAR REACTIONS 4He(polarized p, p), E=46 MeV; measured positive, negative helicity σ; deduced parity nonconserving longitudinal analyzing power. Pressurized target, ionization chamber.
doi: 10.1103/PhysRevC.34.1545
1986NA09 Phys.Rev. C34, 218 (1986) A.A.Naqvi, F.Kappeler, F.Dickmann, R.Muller Fission Fragment Properties in Fast-Neutron-Induced Fission of 237Np NUCLEAR REACTIONS 237Np(n, F), E=0.8, 5.55 MeV; measured correlated fission fragment kinetic energies, velocities; deduced fragment mass and energy distributions, variances, average neutron multiplicities.
doi: 10.1103/PhysRevC.34.218
1985JA01 Phys.Rev. C31, 12 (1985) L.Jarczyk, B.Kamys, A.Strzalkowski, A.Szczurek, M.Godlewski, J.Lang, R.Muller, J.Sromicki p - 11B Spectroscopic Factor from the Interference of Potential Scattering and Elastic Transfer at Low Energies NUCLEAR REACTIONS 12C(11B, 11B), E=10.4, 12.4, 14.57 MeV; measured σ(θ). 12C deduced 1p3/2 asymptotic strength and proton spectroscopic factor. Optical model, exact finite-range DWBA, direct proton transfer.
doi: 10.1103/PhysRevC.31.12
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
1985LA01 Phys.Rev.Lett. 54, 170 (1985); Erratum Phys.Rev.Lett. 54, 2729 (1985) J.Lang, Th.Maier, R.Muller, F.Nessi-Tedaldi, Th.Roser, M.Simonius, J.Sromicki, W.Haeberli Parity Nonconservation in Elastic pα Scattering and the Determination of the Weak Meson-Nucleon Coupling Constants NUCLEAR REACTIONS 4He(polarized p, p), E=46 MeV; measured analyzing power vs θ; deduced parity nonconservation, weak meson-nucleon coupling constants.
doi: 10.1103/PhysRevLett.54.170
1984GO10 Phys.Lett. 144B, 173 (1984) M.Godlewski, J.Lang, R.Muller, P.A.Schmelzbach, J.Sromicki, L.Jarczyk, A.Strzalkowski, H.Witala Break-Up of Polarized Deuterons in the Coulomb Field of Heavy Nuclei NUCLEAR REACTIONS 208Pb(polarized d, p), E=9 MeV; measured σ(θn, θp, Ep), analyzing power T20(θ) following breakup. 197Au(polarized d, p), E=12 MeV; measured asymmetry vs θn, θp, tensor analyzing powers T20, T21, T21 vs θp following breakup. DWBA analysis.
doi: 10.1016/0370-2693(84)91797-0
1984MU05 Phys.Rev. C 29, 885 (1984) R.Muller, A.A.Naqvi, F.Kappeler, F.Dickmann Fragment velocities, energies, and masses from fast neutron induced fission of 235U NUCLEAR REACTIONS 235U(n, F), E=0.5, 5.55 MeV; measured fission products, En, In; deduced fragment velocities and masses, total kinetic energies and their variances, the number of prompt fission neutrons.
doi: 10.1103/physrevc.29.885
1983JA09 Phys.Rev. C28, 700 (1983) L.Jarczyk, B.Kamys, Z.Rudy, A.Strzalkowski, H.Witala, M.Hugi, J.Lang, R.Muller, J.Sromicki, H.H.Wolter Energy Dependence of 9Be + 12C Cross Sections: Nonstatistical component of the mean cross section NUCLEAR REACTIONS 12C(9Be, α), (9Be, 8Be), (9Be, 9Be), E(cm)=5.9-15.4 MeV; calculated σ(θ) vs E; deduced nonstatistical contribution reaction mechanism. DWBA, coupled-channels model analyses, one-, two-step transfer processes.
doi: 10.1103/PhysRevC.28.700
1983KA17 Nucl.Phys. A406, 193 (1983) B.Kamys, L.Jarczyk, Z.Rudy, A.Strzalkowski, H.H.Wolter, J.Lang, R.Muller, J.Sromicki Contribution of Two-Step Processes to the Elastic Scattering of 9Be on 12C NUCLEAR REACTIONS 12C(9Be, 9Be), (9Be, 9Be'), (9Be, 8Be), E=20-45 MeV; analyzed σ(θ); deduced higher order processes role. Optical model, DWBA, potential scattering, direct interaction interference, incoherent compound nucleus contribution.
doi: 10.1016/0375-9474(83)90290-7
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
1982BE51 Z.Phys. A309, 65 (1982) B.Bellinghausen, A.Christ, H.J.Gassen, G.Goerigk, R.Muller, G.Noldeke, T.Reichelt, H.Stanek, P.Stipp Coherent π0 Photoproduction on 12C, 13C and 16O in the Δ(1232) Resonance Region NUCLEAR REACTIONS 12,13C, 16O(γ, π0), E=300-450 MeV; measured production σ(θ) vs E; deduced isobar resonance parameters, pion production mechanism.
doi: 10.1007/BF01420152
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
1981BE13 Nucl.Phys. A358, 373c (1981) B.Bellinghausen, A.Christ, H.J.Gassen, G.Goerigk, R.Muller, G.Noldeke, T.Reichelt, H.Stanek, P.Stipp Measurement of Coherent π0 Photoproduction on Light Nuclei in the P33 Region NUCLEAR REACTIONS 3He, Li, 9Be(γ, π0), E=500 MeV bremsstrahlung; measured σ(θ) vs energy, momentum transfers. Liquid 3He target.
doi: 10.1016/0375-9474(81)90342-0
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.
1981HU13 Helv.Phys.Acta 54, 645 (1981) M.Hugi, J.Lang, R.Muller, J.Sromicki, L.Jarczyk, B.Kamys, A.Strzalkowski, A.Szczurek, B.Zebik Two Step Process Contribution to the Elastic Proton Transfer NUCLEAR REACTIONS 13C(14N, 14N), E(cm)=16.9 MeV; 11B(12C, 12C), E(cm)=14.6 MeV; measured σ(θ). Optical model, multi-step processes, compound nuclear effects.
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
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
1980JA18 Acta Phys.Pol. B11, 641 (1980) L.Jarczyk, B.Kamys, K.Seliger, Z.Wrobel, J.Lang, R.Muller, C.M.Schweizer-Teodorescu Investigation of Nucleon-Unbound States in 29Si and 29P by the Reaction 28Si(d, pn) NUCLEAR REACTIONS 28Si(d, p), (d, n), E=11 MeV; measured σ(θp, θn, En), σ(θn, θp, Ep), σ(θp, θn). 29Si, 29P deduced resonances, J, π, Γ. DWBA analysis, stripping to unbound states.
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
1978BO14 Nucl.Phys. A299, 465 (1978) K.Bodek, L.Jarczyk, B.Kamys, Z.Wrobel, R.Muller, J.Unternahrer, J.Lang Investigation of Nucleon-Unbound States in 25Mg and 25Al Nuclei NUCLEAR REACTIONS 24Mg(d, pn), E=10.5 MeV; measured σ(Ep, θ(p); En, θn). 25Mg, 25Al deduced levels, J, π, Γ. Enriched target.
doi: 10.1016/0375-9474(78)90383-4
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
1978UN01 Phys.Rev.Lett. 40, 1077 (1978) J.Unternahrer, J.Lang, R.Muller Breakup of 9Be in the Coulomb Field of Heavy Nuclei NUCLEAR REACTIONS Ag(9Be, n2α), 197Au(9Be, 2α), E=18-26 MeV; measured σ(E, θ).
doi: 10.1103/PhysRevLett.40.1077
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
1977LA11 Phys.Rev. C16, 1448 (1977) J.Lang, R.Muller, J.Unternahrer, L.Jarczyk, B.Kamys, A.Strzalkowski Neutron Spectroscopic Factor of 9Be from (9Be, 8Be) Reactions NUCLEAR REACTIONS 28Si, 40Ca(9Be, 8Be), E=20 MeV; measured σ(θ). 29Si, 41Ca levels deduced S. Finite-range DWBA analysis.
doi: 10.1103/PhysRevC.16.1448
1977RI03 Nucl.Phys. A278, 163 (1977) M.Richter, W.Henning, H.-J.Korner, R.Muller, K.E.Rehm, H.P.Rother, H.Schaller, H.Spieler Elastic Scattering of 32S + 32S, 40Ca + 40Ca and 32S + 40,48Ca NUCLEAR REACTIONS 32S, 40Ca, 48Ca(32S, 32S), 40Ca(40Ca, 40Ca), E=58-130 MeV; θlab=13-70°; measured σ(E, θ). Optical model analysis.
doi: 10.1016/0375-9474(77)90191-9
1976RO13 Nucl.Phys. A269, 511 (1976) H.-P.Rother, W.Henning, H.-J.Korner, R.Muller, K.E.Rehm, M.Richter, H.Spieler The (18O, 20Ne) Reaction on the Even Ni Isotopes and the Mass of 62Fe NUCLEAR REACTIONS 58,60,62,64Ni(18O, 20Ne), E=63 MeV; measured σ(E(20Ne), θ); deduced Q. 62Fe deduced mass excess. DWBA analysis.
doi: 10.1016/0375-9474(76)90696-5
1976SU12 Helv.Phys.Acta 49, 863 (1976) M.Suter, W.Wolfli, G.Bonani, C.Stoller, R.Muller Proton-Proton bremsstrahlung bei 11 und 13 MeV NUCLEAR REACTIONS 1H(p, p), E=11, 13 MeV; measured σ.
1976TE01 Phys.Rev. C14, 775 (1976) C.M.Teodorescu, P.Viatte, S.Micek, R.Muller, J.Lang, J.Unternahrer, L.Jarczyk Particle Unbound States in 29Si and 29P by the Reaction 28Si(d, pn) NUCLEAR REACTIONS 28Si(d, np), E=11 MeV; measured σ(Ep, θ(p), θn). 29Si deduced resonances. 29P deduced resonances, J, π, Γ. DWBA analysis.
doi: 10.1103/PhysRevC.14.775
1976VI06 Helv.Phys.Acta 49, 569 (1976) P.Viatte, S.Micek, R.Muller, J.Lang, J.Unternahrer, C.M.Teodorescu, L.Jarczyk Der Deuteronenaufbruch an mittelschweren Kernen NUCLEAR REACTIONS 40Ca(d, pn), E=11 MeV; 58Ni(d, pn), E=10 MeV; measured pn(θ). 41Sc, 59Cu deduced resonances, J, π, Γ.
1975LE27 Rev.Mod.Phys. 47, S1 (1975) H.W.Lewis, R.J.Budnitz, A.W.Castleman, D.E.Dorfan, F.C.Finlayson, R.L.Garwin, L.C.Hebel, S.M.Keeny, Jr., R.A.Muller, T.B.Taylor, G.F.Smoot, F.von Hippel, H.Bethe, W.K.H.Panofsky, V.F.Weisskopf Report to the American Physical Society by the study group on light-water reactor safety
doi: 10.1103/RevModPhys.47.S1
1975MU15 Z.Phys. A275, 305 (1975) Precision Measurement of the Nuclear Magnetic Dipole Moment of 175Lu by Optical Pumping of Free Lu+ Ions NUCLEAR MOMENTS 175Lu; measured μ. Optical pumping.
1975SU04 Phys.Lett. 58B, 36 (1975) M.Suter, W.Wolfli, G.Bonani, C.Stoller, R.Muller Proton-Proton Bremsstrahlung at 11 and 13 MeV NUCLEAR REACTIONS 1H(p, p), E=11, 13 MeV; measured σ.
doi: 10.1016/0370-2693(75)90720-0
1975VI05 Phys.Lett. 59B, 35 (1975) P.Viatte, S.Micek, R.Muller, J.Lang, J.Unternahrer, C.M.Teodorescu, L.Jarczyk Study of the Deuteron Break-up on 40Ca NUCLEAR REACTIONS 40Ca(d, np), E=10.5-11.0 MeV; measured σ(E, En, Ep(t), θ). 41Sc deduced resonances, J, π, p-width.
doi: 10.1016/0370-2693(75)90149-5
1974BU10 Phys.Lett. 50B, 333 (1974) A.Buta, J.Lang, S.Micek, R.Muller, J.Unternahrer, P.Viatte Deuteron Break-up and Proton Scattering on 58Ni NUCLEAR REACTIONS 58Ni(p, p), (p, p'), E=2-8 MeV; measured σ(Ep, θ). 58Ni(d, pn), E=10, 12 MeV; measured pn-coin, pn(θ), En, σ(Ep, θ(p), θ(n)). 59Cu deduced resonances.
doi: 10.1016/0370-2693(74)90683-2
1974MU01 Phys.Lett. 48B, 25 (1974) R.Muller, F.Gonnenwein, F.Kappeler, A.Ernst, J.Scheer Search for Fission Shape Isomers in (n, f) Reactions Induced by Neutrons of About 1 MeV NUCLEAR REACTIONS 236U, 240Pu(n, F), E=0.5-2.5 MeV; measured σ(isomer)/σ(prompt).
doi: 10.1016/0370-2693(74)90447-X
1973JA07 Phys.Rev. C8, 68 (1973) L.Jarczyk, J.Lang, R.Muller, D.Balzer, P.Viatte, P.Marmier Breakup of Deuterons in the Fields of Heavy Nuclei NUCLEAR REACTIONS Au, Pb(d, np), E=7, 12 MeV; measured σ(Ep, np-coin., θ(np)).
doi: 10.1103/PhysRevC.8.68
1973RE15 Phys.Lett. 46B, 353 (1973) K.-E.Rehm, W.Henning, R.Muller, M.Richter, H.-P.Rother, H.Schaller Study of Optimum Q-Value in 16O Induced Reactions on Even Zr Isotopes NUCLEAR REACTIONS 90,96Zr(16O, 12C), 96Zr(16O, 14C), E=50-60 MeV; measured σ(θ). Deduced optimum Q dependence.
doi: 10.1016/0370-2693(73)90137-8
1972JA08 Phys.Lett. 39B, 191 (1972) L.Jarczyk, J.Lang, R.Muller, A.Pollitzer, J.F.Valley, W.Wolfli, P.Marmier Deuteron Breakup in the Field of a Heavy Nucleus, Au(d, np)Au NUCLEAR REACTIONS Au(d, np), E=12 MeV; measured σ(En, Ep, θ(n), θ(p)).
doi: 10.1016/0370-2693(72)90771-X
1972LA03 Phys.Rev.Lett. 28, 623 (1972) J.Lang, J.F.Valley, R.Muller, P.Marmier Reaction Mechanism and Symmetry Axes in Particle-Particle Correlations NUCLEAR REACTIONS 12C(d, n), E=6 MeV; measured σ(θ(n), θ(p)).
doi: 10.1103/PhysRevLett.28.623
1972PE16 Phys.Lett. 41B, 151 (1972) U.Peyer, J.Hall, R.Muller, M.Suter, W.Wolfli Bremsstrahlung in α-α Scattering NUCLEAR REACTIONS 4He(α, α'γ), E=12.5-19.0 MeV; measured bremsstrahlung σ(E).
doi: 10.1016/0370-2693(72)90448-0
1972VA10 Nucl.Phys. A184, 577 (1972) J.F.Valley, J.Lang, R.Muller, P.Marmier Neutron-Proton Correlations for the Reaction 12C(d, n)13N*(p)12C NUCLEAR REACTIONS 12C(d, pn), E=5.5-6.5 MeV; measured σ(Ep, En, θ(p), θ(n), phi(np)). Natural target.
doi: 10.1016/0375-9474(72)90430-7
1971HA62 Phys.Lett. 37B, 53 (1971) Bremsstrahlung in Deuteron-Proton Scattering NUCLEAR REACTIONS 1H(d, d'γ), E=7, 8, 9 MeV; measured bremsstrahlung σ.
doi: 10.1016/0370-2693(71)90568-5
1971TH08 Nucl.Phys. A170, 17 (1971) G.Thievent, J.Lang, R.Muller, P.Marmier Energy Dependence of Proximity Scattering NUCLEAR REACTIONS 7Li(d, nα), E=2.07-2.25 MeV; measured σ(E(α1), E(α2), θ(α1), θ(α2)).
doi: 10.1016/0375-9474(71)90680-4
1971WO07 Phys.Rev.Lett. 27, 271 (1971) Bremsstrahlung in Proton-α-Particle Scattering NUCLEAR REACTIONS 4He(α, α'γ), E=7-12 MeV; measured σ(E).
doi: 10.1103/PhysRevLett.27.271
1969TH02 Phys.Letters 30B, 23 (1969) G.Thievent, J.Lang, R.Muller, P.Marmier Energy Dependence of Proximity Scattering NUCLEAR REACTIONS 7Li(d, nα), E = 2.07-2.25 MeV; measured σ(E;En, Eα, θ(α)); deduced energy dependence of proximity scattering.
doi: 10.1016/0370-2693(69)90276-7
1967WO08 Helv.Phys.Acta 40, 946 (1967) W.Wolfli, R.Bosch, J.Lang, R.Muller, P.Marmier Einfang von Protonen durch Deuteronen NUCLEAR REACTIONS 2H(p, γ), E=2-12 MeV; measured reaction products, Eγ, Iγ; deduced σ(θ). Comparison with available data using a detailed balance principle.
doi: 10.5169/seals-113803
1966LA18 Nucl.Phys. 88, 576(1966) J.Lang, R.Muller, W.Wolfli, R.Bosch, P.Marmier Direct Determination of a Short Nuclear Lifetime (Approx. 10-20 s) By the Proximity Scattering Method NUCLEAR REACTIONS 12C(d, pn), E = 5.39 MeV; measured σ(Ep, θ(n), θ(p), phi(np)). 13N deduced T1/2(3.5 MeV level group).
doi: 10.1016/0029-5582(66)90416-0
1966WO04 Phys.Letters 22, 75 (1966) W.Wolfli, R.Bosch, J.Lang, R.Muller, P.Marmier Proton Capture by Deuterons NUCLEAR STRUCTURE 2H; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)90067-9
1965BO35 Helv.Phys.Acta 38, 753 (1965) R.Bosch, J.Lang, R.Muller, W.Wolfli Kernphotoeffekt an H3 NUCLEAR STRUCTURE 3H; measured not abstracted; deduced nuclear properties.
1965BO43 Phys.Lett. 15, 243 (1965) R.Bosch, J.Lang, R.Muller, W.Wolfli Ground state wave function of 3H and 3He NUCLEAR REACTIONS 3H(γ, n) E=3.7-33 MeV; analyzed available data, σ. 3H, 3He; deduced ground state wave functions.
doi: 10.1016/0031-9163(65)91232-1
1965LA08 Phys.Letters 15, 248 (1965) J.Lang, R.Muller, W.Wolfli, R.Bosch, P.Marmier A Direct Measurement of a Short Nuclear Lifetime (Approx.10-20 s) Using Proximity Scattering NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(65)91234-5
1965MA62 Nucl.Phys. 74, 377 (1965) A.Manfredini, M.Muchnik, L.Fiore, C.Ramorino, H.G.De Carvalho, J.Lang, R.Muller 238U fission induced by low-energy monochromatic γ-rays: cross sections between 5 and 8 MeV NUCLEAR REACTIONS 238U(γ, f), E=5.4-7.7 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry M0535.
doi: 10.1016/0029-5582(65)90089-1
1964BO05 Phys. Letters 8, 120 (1964) R.Bosch, J.Lang, R.Muller, W.Wolfli Photodisintegration of H3 NUCLEAR STRUCTURE 3H; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(64)90734-6
1963BO32 Helv.Phys.Acta 36, 657 (1963) R.Bosch, J.Lang, R.Muller, W.Wolfli Untersuchung des Kernphotoeffektes an Be9 und H2 mit diskreten Gammaenergien zwischen 2, 75 und 9, 0 MeV NUCLEAR STRUCTURE 9Be, 2H; measured not abstracted; deduced nuclear properties. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG0023. 1962BO08 Phys.Letters, 1, 114 (1962) R.Bosch, J.Lang, R.Muller, W.Wolfli Messung der Polarisation der Photoneutronen vom Be9 NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
1962BO21 Helv.Phys.Acta. 35, 288 (1962) R.Bosch, J.Lang, R.Muller, W.Wolfli Untersuchung des Kernphotoeffektes an Be mit Diskreten Gammaenergien Zwischen 5, 4 und 9, 0 MeV NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
1962JA08 Z.Angew.Math.Phys. 13, 117 (1962); Phys.Abstr. 65, 1179, Abstr.12212 (1962) L.Jarczyk, J.Lang, R.Muller, W.Wolfli Investigation of the Reaction Bi209(n, γ)Bi210 with a Gamma-Gamma Coincidence Method NUCLEAR STRUCTURE 210Bi; measured not abstracted; deduced nuclear properties.
doi: 10.1007/BF01594134
1961JA18 Helv.Phys.Acta 34, 457 (1961) L.Jarczyk, J.Long, R.Muller, W.Wolfli Untersuchung der Reaktion Bi209(n, γ)Bi210 mit einer Gamma-Gamma-Koinzidenzmethode NUCLEAR STRUCTURE 210Bi; measured not abstracted; deduced nuclear properties.
1961JA19 Helv.Phys.Acta. 34, 483 (1961) L.Jarczyk, J.Lang, R.Muller, W.Wolfli (n, γ)-Spektren und Wirkungsquerschnitte von Lithium, Beryllium und Kohlenstoff Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22510. 1961LA18 Helv.Phys.Acta 34, 812 (1961) Messung der Polarisation der Photoneutronen am Be9 NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
Back to query form [Next] Note: The following list of authors and aliases matches the search parameter R.Muller: , R.A.MULLER |