NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.Sromicki Found 50 matches. 2003FE07 Nucl.Phys. A721, 457c (2003) W.Fetscher, K.Bodek, A.Budzanowski, N.Danneberg, C.Hilbes, l.Jarczyk, K.Kirch, S.Kistryn, J.Klement, K.Kohler, A.Kozela, J.Lang, X.Morelle, T.Schweizer, J.Smyrski, J.Sromicki, E.Stephan, A.Strzalkowski, J.Zejma Polarized Muon Decay: Measurement of the Polarization Vector of the Decay Positrons as a Test of Time Reversal Invariance
doi: 10.1016/S0375-9474(03)01098-4
2003HU06 Phys.Rev.Lett. 90, 202301 (2003) R.Huber, J.Lang, S.Navert, J.Sromicki, K.Bodek, St.Kistryn, J.Zejma, O.Naviliat-Cuncic, E.Stephan, W.Haeberli Search for Time-Reversal Violation in the β Decay of Polarized 8Li Nuclei RADIOACTIVITY 8Li(β-) [from 7Li(polarized d, p)]; measured β-decay asymmetry from polarized source, electrons transverse polarization; deduced time reversal violating triple correlation parameter, scalar leptoquark mass limit. Comparison with model.
doi: 10.1103/PhysRevLett.90.202301
2001BI08 Nucl.Phys. A684, 536c (2001) R.Bieber, K.Bodek, K.Ermisch, W.Glockle, J.Golak, M.N.Harakeh, N.Kalantar-Nayestanaki, St.Kistryn, J.Kuros-Zolnierczuk, J.Lang, A.Micherdzinska, R.Skibinski, M.Sokolowski, J.Sromicki, E.Stephan, A.Strzalkowski, M.Volkerts, H.Witala, J.Zejma, W.Zipper Search for Three-Nucleon Force Effects in dp-Breakup Reaction NUCLEAR REACTIONS 2H(p, np), E=65 MeV; analyzed σ(θ), Ay(θ); deduced role of three-nucleon force.
doi: 10.1016/S0375-9474(01)00378-5
2001BO23 Few-Body Systems 30, 65 (2001) K.Bodek, J.Golak, L.Jarczyk, St.Kistryn, J.Kuros-Zolnierczuk, J.Lang, A.Micherdzinska, R.Skibinski, J.Smyrski, M.Sokolowski, J.Sromicki, A.Strzalkowski, H.Witala, J.Zejma, W.Zipper Proton-Induced Deuteron Breakup Reaction at 65 MeV: Unspecific configurations NUCLEAR REACTIONS 2H(polarized p, 2p), E=65 MeV; measured σ(E, θ(1), θ(2)), Ay(θ). Kinematically complete measurement. Comparisons with several model predictions.
doi: 10.1007/s006010170018
2001TH18 Nucl.Phys. A694, 559 (2001) E.Thomas, R.Prieels, M.Allet, K.Bodek, J.Camps, J.Deutsch, F.Gimeno-Nogues, J.Govaerts, J.Lang, O.Naviliat-Cuncic, I.Pepe, P.Quin, N.Severijns, J.Sromicki Positron Polarization in the Decay of Polarized 12N: A precision tests of the standard model RADIOACTIVITY 12N(β+) [from 12C(polarized p, n)]; measured positrons longitudinal polarization following decay of polarized source; deduced constraints on mass of right-handed gauge boson. Comparison with standard model predictions.
doi: 10.1016/S0375-9474(01)01083-1
2000BO16 Nucl.Phys. A663-664, 907c (2000) K.Bodek, A.Budzanowski, N.Danneberg, W.Fetscher, C.Hilbes, M.Janousch, L.Jarczyk, K.Kirch, S.Kistryn, J.Klement, K.Kohler, A.Kozela, J.Lang, G.Llosa Llacer, M.Markiewicz, X.Morelle, T.Schweizer, J.Smyrski, J.Sromicki, E.Stephan, A.Strzalkowski, J.Zejma Measurement of the Transverse Polarization of Positrons from the Decay of Polarized Muons: A status report
doi: 10.1016/S0375-9474(99)00794-0
2000SR02 Nucl.Instrum.Methods Phys.Res. A440, 609 (2000) T Violation in the Weak Scalar and Tensor Interaction: Neutron and nuclei
doi: 10.1016/S0168-9002(99)01050-5
1999SR01 Phys.Rev.Lett. 82, 57 (1999) J.Sromicki, K.Bodek, D.Conti, St.Kistryn, J.Lang, S.Navert, O.Naviliat-Cuncic, E.Stephan, C.Sys, J.Zejma, W.Haeberli, E.Reichert, M.Steigerwald Polarization in Mott Scattering of Multi-MeV Electrons from Heavy Nuclei NUCLEAR REACTIONS Pb(polarized e, e'), E=14 MeV; measured σ(θ), scattering asymmetry, analyzing power A; deduced target thickness effects.
doi: 10.1103/PhysRevLett.82.57
1999SR06 Nucl.Phys. (Supplement) A654, 967c (1999) Time Reversal Tests in Nuclear and Neutron Beta Decay RADIOACTIVITY 8Li(β-); analyzed data from polarized source; deduced time-reversal violation features. Proposed neutron decay experiment discussed.
doi: 10.1016/S0375-9474(00)88582-6
1998BO08 Nucl.Phys. A631, 687c (1998) K.Bodek, W.Glockle, J.Golak, L.Jarczyk, St.Kistryn, B.Kozlowska, J.Lang, A.Micherdzinska, O.Naviliat-Cuncic, J.Smyrski, M.Sokolowski, J.Sromicki, A.Strzalkowski, H.Witala, J.Zejma, W.Zipper Proton Induced Deuteron Breakup Reaction at 65 MeV: Unspecific configurations NUCLEAR REACTIONS 2H(polarized p, 2p), E=65 MeV; measured σ(φ(12), θ(1), θ(2)), A(y). Comparison with theory.
doi: 10.1016/S0375-9474(98)00092-X
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
1997BE40 Acta Phys.Pol. B28, 1659 (1997) C.P.Bee, D.Conti, M.Hadri, St.Kistryn, J.Lang, O.Naviliat-Cuncic, J.Sromicki, E.Stephan, K.Bodek, J.Smyrski, A.Strzalkowski, J.Zejma, L.Grenacs, R.Abela, P.Boni, F.Foroughi, W.Zipper, A.Proykova Polarimetry of 16N(gs) Produced in μ--Capture on 16O Nuclei RADIOACTIVITY 16N(β-) [from 16O(polarized μ-, ν), E at 50 MeV/c]; measured βγ-coin, T1/2. Stacked target method.
1997SE20 Pisma Zh.Eksp.Teor.Fiz. 66, 765 (1997); JETP Lett. 66, 802 (1997) A.P.Serebrov, V.A.Mityukhlyaev, A.A.Zakharov, T.Bowles, G.Greene, J.Sromicki Solid Deuterium Source of Ultracold Neutrons Based on a Pulsed Spallation Source
doi: 10.1134/1.567601
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
1995ZE01 Phys.Rev. C51, 1494 (1995) V.J.Zeps, E.G.Adelberger, A.Garcia, C.A.Gossett, H.E.Swanson, W.Haeberli, P.A.Quin, J.Sromicki Parity Mixing of the 0+-0- I = 1 Doublet in 14N NUCLEAR REACTIONS, ICPND 13C(polarized p, p), E=1.1-2.2 MeV; 13C(p, γ), E=0.45-3 MeV; measured σ(E). 14N levels deduced ΔI=0 parity-mixing matrix element, levels parameters. Enriched targets. S-matrix analysis.
doi: 10.1103/PhysRevC.51.1494
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
1994CO27 Helv.Phys.Acta 67, 777 (1994) D.Conti, K.Bodek, H.K.Kayser, J.Lang, S.Navert, O.Naviliat, E.Reichert, J.Sromicki, K.-H.Steffens, M.Steigerwald, E.Stephan, J.Zejma Spin Dependence in Scattering of 14 MeV Electrons from Lead Nuclei NUCLEAR REACTIONS Pb(polarized e, e), E=14 MeV; measured left-right asymmetry; deduced final nuclear size effects role.
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
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
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
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.
1989HO05 Nucl.Instrum.Methods Phys.Res. A274, 207 (1989) D.Holslin, J.McAnich, J.Sromicki, P.A.Quin, W.Haeberli New Instrumental Effects in Fast Neutron Polarization Measurements NUCLEAR REACTIONS 1H(polarized n, n), E=10 MeV; measured analyzing power vs θ; deduced instrumental effects role.
doi: 10.1016/0168-9002(89)90381-1
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
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.
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
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
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
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
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
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
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
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
1980BO29 Helv.Phys.Acta 53, 306 (1980) K.Bodek, M.Hugi, L.Jarczyk, J.Lang, R.Mueller, A.Schiltz, J.Sromicki, A.Strzalkowski, E.Ungricht Transferprozesse bei der Elastischen Streuung von 10B an 9Be NUCLEAR REACTIONS 9Be(10B, 10B), E=9.5, 14.2 MeV; measured σ(θ); deduced reaction mechanism.
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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