NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = J.Lang Found 112 matches. Showing 1 to 100. [Next]2019AN10 Phys.Rev. C 99, 064313 (2019), Erratum Phys.Rev. C 107, 029901 (2023) S.A.S.Andres, C.Hornung, J.Ebert, W.R.Plass, T.Dickel, H.Geissel, C.Scheidenberger, J.Bergmann, F.Greiner, E.Haettner, C.Jesch, W.Lippert, I.Mardor, I.Miskun, Z.Patyk, S.Pietri, A.Pihktelev, S.Purushothaman, M.P.Reiter, A.-K.Rink, H.Weick, M.I.Yavor, S.Bagchi, V.Charviakova, P.Constantin, M.Diwisch, A.Finlay, S.Kaur, R.Knobel, J.Lang, B.Mei, I.D.Moore, J.-H.Otto, I.Pohjalainen, A.Prochazka, C.Rappold, M.Takechi, Y.K.Tanaka, J.S.Winfield, X.Xu High-resolution, accurate multiple-reflection time-of-flight mass spectrometry for short-lived, exotic nuclei of a few events in their ground and low-lying isomeric states ATOMIC MASSES 93,94Ru, 94Rh, 96,97Pd, 100Ag, 107Cd, 114,116,133,134Te, 114,134Sb, 117,119,133,134I, 119Xe, 124,125,126Cs, 211,212,213Fr, 211Po, 212,213,218,220Rn, 212,217At; 134mSb, 133mTe, 133m,134mI, 134mXe, 211mPo; measured mass excess and isomer energies using multiple-reflection time-of-flight mass spectrometry (MR-TOF-MS) with the FRS Ion Catcher at GSI. Isotopes produced in 9Be(238U, F), E=300, 1000 MeV/nucleon; 9Be(124Xe, X), E=600 MeV/nucleon reactions using FRS separator at GSI. Comparison with AME-2016 evaluation. Systematics of S(2n) values in N=123-136 Pb, Bi, Po, At, Rn, Fr, Ra, Ac, Th isotopes, and compared with theoretical predictions.
doi: 10.1103/PhysRevC.99.064313
2013PU02 Europhys.Lett. 104, 42001 (2013) S.Purushothaman, M.P.Reiter, E.Haettner, P.Dendooven, T.Dickel, H.Geissel, J.Ebert, C.Jesch, W.R.Plass, M.Ranjan, H.Weick, F.Amjad, S.Ayet, M.Diwisch, A.Estrade, F.Farinon, F.Greiner, N.Kalantar-Nayestanaki, R.Knobel, J.Kurcewicz, J.Lang, I.D.Moore, I.Mukha, C.Nociforo, M.Petrick, M.Pfutzner, S.Pietri, A.Prochazka, A.-K.Rink, S.Rinta-Antila, C.Scheidenberger, M.Takechi, Y.K.Tanaka, J.S.Winfield, M.I.Yavor First experimental results of a cryogenic stopping cell with short-lived, heavy uranium fragments produced at 1000 MeV/u
doi: 10.1209/0295-5075/104/42001
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
2002PA13 Phys.Rev.Lett. 88, 102302 (2002) I.Passchier, L.D.van Buuren, D.Szczerba, R.Alarcon, Th.S.Bauer, D.J.Boersma, J.F.J.van den Brand, H.J.Bulten, R.Ent, M.Ferro-Luzzi, M.Harvey, P.Heimberg, D.W.Higinbotham, S.Klous, H.Kolster, J.Lang, B.L.Militsyn, D.Nikolenko, G.J.L.Nooren, B.E.Norum, H.R.Poolman, I.Rachek, M.C.Simani, E.Six, H.de Vries, K.Wang, Z.-L.Zhou Spin-Momentum Correlations in Quasielastic Electron Scattering from Deuterium NUCLEAR REACTIONS 2H(polarized e, e'p), E=720 MeV; measured proton, electron energy spectrum, (proton)(electron)-coin, spin correlation parameter vs missing momentum. Polarized target, comparison with theoretical results including different nucleon-nucleon potentials and S, D states.
doi: 10.1103/PhysRevLett.88.102302
2002VA11 Phys.Rev.Lett. 89, 012001 (2002) L.D.Van Buuren, D.Szczerba, R.Alarcon, D.J.Boersma, J.F.J.van den Brand, H.J.Bulten, R.Ent, M.Ferro-Luzzi, M.Harvey, P.Heimberg, D.W.Higinbotham, S.Klous, H.Kolster, J.Lang, B.L.Militsyn, D.Nikolenko, B.E.Norum, I.Passchier, H.R.Poolman, I.Rachek, M.C.Simani, E.Six, H.de Vries, Z.-L.Zhou Spin-Dependent Electron-Proton Scattering in the Δ-Excitation Region NUCLEAR REACTIONS 1H(polarized e, e'), E=720 MeV; measured σ(E, θ), spin correlation parameters. Polarized target, comparison with model predictions.
doi: 10.1103/PhysRevLett.89.012001
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
2001VA32 Nucl.Instrum.Methods Phys.Res. A474, 209 (2001) L.D.van Buuren, D.Szczerba, J.F.J.van den Brand, H.J.Bulten, M.Ferro-Luzzi, S.Klous, H.Kolster, J.Lang, F.A.Mul, H.R.Poolman, M.C.Simani Performance of a Hydrogen/Deuterium Polarized Gas Target in a Storage Ring NUCLEAR REACTIONS 1H(polarized e, e'), 2H(polarized e, e'p), E=720 MeV; measured asymmetry; deduced target polarization features.
doi: 10.1016/S0168-9002(01)00885-3
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
2000PA22 Nucl.Phys. A663-664, 421c (2000) I.Passchier, L.D.van Buuren, D.Szczerba, R.Alarcon, Th.S.Bauer, D.Boersma, J.F.J.van den Brand, H.J.Bulten, M.Ferro-Luzzi, D.W.Higinbotham, C.W.de Jager, S.Klous, H.Kolster, J.Lang, D.Nikolenko, G.J.Nooren, B.E.Norum, H.R.Poolman, I.Rachek, M.C.Simani, E.Six, H.de Vries, K.Wang, Z.-L.Zhou The Charge Form Factor of the Neutron from 2H(pol)(e(pol), e'n)p NUCLEAR REACTIONS 2H(polarized e, e'n), (polarized e, e'p), E=720 MeV; measured (particle)(electron)-coin, sideways spin-correlation parameter. 1n deduced charge form factor. Polarized target.
doi: 10.1016/S0375-9474(99)00673-9
2000VA07 Nucl.Phys. A663-664, 1049c (2000) L.D.van Buuren, D.Szczerba, J.F.J.van den Brand, H.J.Bulten, M.Ferro-Luzzi, H.Kolster, J.Lang, M.C.Simani, F.Mul High Density Polarized Hydrogen/Deuterium Internal Target NUCLEAR REACTIONS 2H(e, e'p), E not given; measured asymmetry. Polarized target.
doi: 10.1016/S0375-9474(99)00767-8
1999BO12 Phys.Rev.Lett. 82, 3755 (1999) M.Bouwhuis, R.Alarcon, T.Botto, J.F.J.van den Brand, H.J.Bulten, S.Dolfini, R.Ent, M.Ferro-Luzzi, D.W.Higinbotham, C.W.de Jager, J.Lang, D.J.J.de Lange, N.Papadakis, I.Passchier, H.R.Poolman, E.Six, J.J.M.Steijger, N.Vodinas, H.de Vries, Z.-L.Zhou Measurement of T20 in Elastic Electron-Deuteron Scattering NUCLEAR REACTIONS 2H(e, e), E=704 MeV; measured T20 vs momentum transfer. Polarized target. Comparison with nonrelativistic calculation.
doi: 10.1103/PhysRevLett.82.3755
1999FE14 Nucl.Phys. (Supplement) A654, 1009c (1999) M.Ferro-Luzzi, R.Alarcon, N.van Bakel, T.Bauer, D.Boersma, T.Botto, M.Bouwhuis, J.F.J.van den Brand, L.van Buuren, H.-J.Bulten, R.Ent, D.Geurts, M.Harvey, P.Heimberg, D.W.Higinbotham, C.W.de Jager, S.Klous, H.Kolster, J.Lang, B.Militsyn, B.E.Norum, I.Passchier, H.R.Poolman, M.C.Simani, E.Six, J.J.M.Steijger, D.Szczerba, H.de Vries, Z.L.Zhou Electron Scattering at NIKHEF with Polarized Beam and Targets NUCLEAR REACTIONS 2H(e, e'), E=900 MeV; measured tensor analyzing powers. 3He(polarized e, e'n), (polarized e, e'p), E=900 MeV; measured spin correlation parameters. Polarized targets, comparisons with model predictions.
doi: 10.1016/S0375-9474(00)88589-9
1999PA23 Phys.Rev.Lett. 82, 4988 (1999) I.Passchier, R.Alarcon, Th.S.Bauer, D.Boersma, J.F.J.van den Brand, L.D.van Buuren, H.J.Bulten, M.Ferro-Luzzi, P.Heimberg, D.W.Higinbotham, C.W.de Jager, S.Klous, H.Kolster, J.Lang, B.L.Militsyn, D.Nikolenko, G.J.L.Nooren, B.E.Norum, H.R.Poolman, I.Rachek, M.C.Simani, E.Six, D.Szczerba, H.de Vries, K.Wang, Z.-L.Zhou Charge Form Factor of the Neutron from the Reaction 2H(pol)(e(pol), e'n)p NUCLEAR REACTIONS 2H(polarized e, e'n), E=720 MeV; measured asymmetry, spin correlation parameter. 1n deduced charge form factor. Polarized gas target.
doi: 10.1103/PhysRevLett.82.4988
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
1999ZH03 Phys.Rev.Lett. 82, 687 (1999) Z.-L.Zhou, M.Bouwhuis, M.Ferro-Luzzi, E.Passchier, R.Alarcon, M.Anghinolfi, H.Arenhovel, R.van Bommel, T.Botto, J.F.J.van den Brand, H.J.Bulten, S.Choi, J.Comfort, S.M.Dolfini, R.Ent, C.Gaulard, D.W.Higinbotham, C.W.de Jager, E.Konstantinov, J.Lang, W.Leidemann, D.J.de Lange, M.A.Miller, D.Nikolenko, N.Papadakis, I.Passchier, H.R.Poolman, S.G.Popov, I.Rachek, M.Ripani, E.Six, J.J.M.Steijger, M.Taiuti, O.Unal, N.Vodinas, H.de Vries Tensor Analyzing Powers for Quasielastic Electron Scattering from Deuterium NUCLEAR REACTIONS 2H(e, e'p), E=565 MeV; measured missing momentum spectrum, tensor analyzing power vs θ. Comparison with model. Polarized target.
doi: 10.1103/PhysRevLett.82.687
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
1998FE01 Nucl.Phys. A631, 190c (1998) M.Ferro-Luzzi, R.Alarcon, T.Bauer, D.Boersma, T.Botto, M.Bouwhuis, J.F.J.van den Brand, H.J.Bulten, L.van Buuren, R.Ent, D.Geurts, M.Harvey, P.Heimberg, D.Higinbotham, C.W.de Jager, J.Lang, D.J.de Lange, B.Norum, I.Passchier, H.R.Poolman, M.van der Putte, E.Six, J.Steijger, D.Szczerba, O.Unal, H.de Vries, Z.-L.Zhou Spin-Dependent Electromagnetic Response of Few-Body Systems NUCLEAR REACTIONS 2H(e, e), (e, e'), E not given; measured tensor analyzing powers. Polarized targets.
doi: 10.1016/S0375-9474(98)00023-2
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.
1997VA08 Phys.Rev.Lett. 78, 1235 (1997) J.F.J.van den Brand, H.J.Bulten, M.Ferro-Luzzi, Z.-L.Zhou, R.Alarcon, T.Botto, M.Bouwhuis, S.Dolfini, R.Ent, P.Heimberg, D.Higinbotham, C.W.de Jager, J.Lang, D.J.de Lange, G.J.Nooren, N.Papadakis, I.Passchier, H.R.Poolman, J.J.M.Steijger, O.Unal, N.Vodinas, H.de Vries Evidence for Nuclear Tensor Polarization of Deuterium Molecules in Storage Cells
doi: 10.1103/PhysRevLett.78.1235
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
1996FE03 Phys.Rev.Lett. 77, 2630 (1996) M.Ferro-Luzzi, M.Bouwhuis, E.Passchier, Z.-L.Zhou, R.Alarcon, M.Anghinolfi, R.van Bommel, T.Botto, J.F.J.van den Brand, M.Buchholz, H.J.Bulten, S.Choi, J.Comfort, S.Dolfini, R.Ent, C.Gaulard, D.Higinbotham, C.W.de Jager, E.P.van Klaveren, E.Konstantinov, J.Lang, D.J.de Lange, M.A.Miller, D.Nikolenko, G.J.Nooren, N.Papadakis, I.Passchier, H.R.Poolman, S.G.Popov, I.Rachek, M.Ripani, E.Six, J.J.M.Steijger, M.Taiuti, O.Unal, N.Vodinas, H.de Vries Measurement of Tensor Analyzing Powers for Elastic Electron Scattering from a Polarized 2H Target Internal to a Storage Ring NUCLEAR REACTIONS 2H(e, e), E=565 MeV; measured absolute T20, T22 vs momentum transfer. Tensor polarized target.
doi: 10.1103/PhysRevLett.77.2630
1996LA05 Phys.Lett. 366B, 18 (1996) J.T.A.Lang, J.E.Paton, A.M.Green Perturbative Static Four-Quark Potentials
doi: 10.1016/0370-2693(95)01324-5
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
1996ZH33 Nucl.Instrum.Methods Phys.Res. A379, 212 (1996) Z.-L.Zhou, M.Ferro-Luzzi, J.F.J.van den Brand, M.Buchholz, H.J.Bulten, M.Doets, J.Lang, J.Neal Ion-Extraction Polarimetry for Polarized Internal Targets
doi: 10.1016/0168-9002(96)00589-X
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
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
1991RU04 Nucl.Phys. A524, 377 (1991) H.Ruhl, B.Dechant, J.Krug, W.Lubcke, G.Spangardt, M.Steinke, M.Stephan, D.Kamke, J.Balewski, K.Bodek, L.Jarczyk, A.Strzalkowski, W.Hajdas, St.Kistryn, R.Mueller, J.Lang, R.Henneck, H.Witala, Th.Cornelius, W.Glockle Analyzing Power in n(pol) + d Elastic Scattering at 67 MeV NUCLEAR REACTIONS 2H(polarized n, n), E=67 MeV; measured analyzing power vs θ. Faddeev calculations. Scintillation target.
doi: 10.1016/0375-9474(91)90275-B
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
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
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
1984BA54 Phys.Rev. C30, 1409 (1984) R.Balzer, R.Henneck, Ch.Jacquemart, J.Lang, F.Nessi-Tedaldi, T.Roser, M.Simonius, W.Haeberli, S.Jaccard, W.Reichart, Ch.Weddigen Parity Violation in Proton-Proton Scattering at 45 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=44.8 MeV; measured parity nonconserving longitudinal analyzing power. Longitudinally polarized beam, pressurized H2 target, cylindrical ionization chamber scattered proton detector.
doi: 10.1103/PhysRevC.30.1409
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
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
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.
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.
1979BA65 Helv.Phys.Acta 52, 420 (1979) R.Balzer, R.Henneck, C.Jacquemart, J.Lang, M.Simonius, W.Haeberli, S.Jaccard, L.Rezzonico, C.Weddigen Messung der Paritatsverletzung in Proton-Proton-Streuung bei 50 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=50 MeV; measured asymmetry.
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
1978BR01 Phys.Rev.Lett. 40, 306 (1978) H.Brandle, L.Grenacs, J.Lang, L.Ph.Roesch, V.L.Telegdi, P.Truttmann, A.Weiss, A.Zehnder Measurement of the Correlation between Alignment and Electron Momentum in 12B → 12C(g.s) Decay by a Novel Technique: Another Search for Second-Class Currents RADIOACTIVITY 12B; measured β(θ, H, t); deduced gradient coupling, recoil term parameter α. Oriented nuclei.
doi: 10.1103/PhysRevLett.40.306
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
1977WO01 J.Phys.(London) G3, L33 (1977) W.Wolfli, J.Lang, G.Bonani, M.Suter, C.Stoller, H.-U.Nissen Evidence for Primordial Superheavy Elements (Question) NUCLEAR STRUCTURE A > 200; calculated X-ray lines in monazites, cheralites; deduced no evidence for superheavy elements.
doi: 10.1088/0305-4616/3/2/004
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.
1975LA24 J.Phys.(London) B8, L339 (1975) The photoabsorption coefficients of krypton and xenon from 48 A to 210 A NUCLEAR REACTIONS Ar, Xe(γ, X), E not given; measured reaction products; deduced photoabsorption coefficients.
doi: 10.1088/0022-3700/8/14/005
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
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
1973LA24 Phys.Lett. 46B, 15 (1973) Analysis of Angular Correlations in Sequential Decay Processes NUCLEAR REACTIONS 10B(α, α); analyzed data for σ(θ).
doi: 10.1016/0370-2693(73)90462-0
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
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
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
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
1966LA19 Z.Naturforsch. 21a, 1729 (1966) Koinzidenzmessungen an Einfang-γ-Strahlen von 149Sm NUCLEAR STRUCTURE 150Sm; measured not abstracted; deduced nuclear properties.
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.
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