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Search: Author = R.Muller

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22717.


1995MU23      Z.Phys. A353, 103 (1995)

R.Muller

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22265.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2392.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0552.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21834.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1550.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0634.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21834.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1950.


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
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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
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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
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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
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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
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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
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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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0890.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2157.


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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0895.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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1975MU15      Z.Phys. A275, 305 (1975)

R.Muller, E.W.Weber

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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
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1971HA62      Phys.Lett. 37B, 53 (1971)

J.Hall, W.Wolfli, R.Muller

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
Citations: PlumX Metrics


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
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1971WO07      Phys.Rev.Lett. 27, 271 (1971)

W.Wolfli, J.Hall, R.Muller

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
Citations: PlumX Metrics


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
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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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0535.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0464.


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
Citations: PlumX Metrics


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)

J.Lang, R.Muller, W.Wolfli

Messung der Polarisation der Photoneutronen am Be9

NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.


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