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NSR database version of May 30, 2024.

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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
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics


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


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
Citations: PlumX Metrics


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
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
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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
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


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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


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
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


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
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.


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
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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
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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
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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
Citations: PlumX Metrics


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
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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
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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
Citations: PlumX Metrics


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


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


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22224.


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


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


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


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
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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1949.


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
Citations: PlumX Metrics

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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
Citations: PlumX Metrics

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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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
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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
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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
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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
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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
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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
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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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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
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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.


1975LA24      J.Phys.(London) B8, L339 (1975)

J.Lang, W.S.Watson

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
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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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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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1973LA24      Phys.Lett. 46B, 15 (1973)

J.Lang, M.Simonius

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
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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
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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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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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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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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
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1966LA19      Z.Naturforsch. 21a, 1729 (1966)

J.Lang

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
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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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