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NSR database version of May 24, 2024.

Search: Author = J.Sromicki

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2000SR02      Nucl.Instrum.Methods Phys.Res. A440, 609 (2000)

J.Sromicki

T Violation in the Weak Scalar and Tensor Interaction: Neutron and nuclei

doi: 10.1016/S0168-9002(99)01050-5
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1999SR06      Nucl.Phys. (Supplement) A654, 967c (1999)

J.Sromicki

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
Citations: PlumX Metrics


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
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


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
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


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0213.


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


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
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


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


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
Citations: PlumX Metrics


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


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
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


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.


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


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


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


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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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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1813.


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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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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1786.


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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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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