NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = A.Klein Found 114 matches. Showing 1 to 100. [Next]2021DO09 Nature(London) 590, 561 (2021), Pub.Correction Nature(London) 604, E26 (2022) J.Dove, B.Kerns, R.E.McClellan, S.Miyasaka, D.H.Morton, K.Nagai, S.Prasad, F.Sanftl, M.B.C.Scott, A.S.Tadepalli, C.A.Aidala, J.Arrington, C.Ayuso, C.L.Barker, C.N.Brown, W.C.Chang, A.Chen, D.C.Christian, B.P.Dannowitz, M.Daugherity, M.Diefenthaler, L.El Fassi, D.F.Geesaman, R.Gilman, Y.Goto, L.Guo, R.Guo, T.J.Hague, R.J.Holt, D.Isenhower, E.R.Kinney, N.Kitts, A.Klein, D.W.Kleinjan, Y.Kudo, C.Leung, P.-J.Lin, K.Liu, M.X.Liu, W.Lorenzon, N.C.R.Makins, M.Mesquita de Medeiros, P.L.McGaughey, Y.Miyachi, I.Mooney, K.Nakahara, K.Nakano, S.Nara, J.-C.Peng, A.J.Puckett, B.J.Ramson, P.E.Reimer, J.G.Rubin, S.Sawada, T.Sawada, T.-A.Shibata, D.Su, M.Teo, B.G.Tice, R.S.Towell, S.Uemura, S.Watson, S.G.Wang, A.B.Wickes, J.Wu, Z.Xi, Z.Ye The asymmetry of antimatter in the proton NUCLEAR REACTIONS 1,2H(p, μ+), (p, μ-), E=120 GeV; measured reaction products. 1H; deduced antimatter asymmetry in the proton.
doi: 10.1038/s41586-021-03282-z
2019KI04 Nucl.Phys. A982, 971c (2019) D.Kikola, S.J.Brodsky, G.Cavoto, C.Da Silva, F.Donato, M.G.Echevarria, E.G.Ferreiro, C.Hadjidakis, I.Hrivnacova, A.Klein, A.Kurepin, A.Kusina, J.P.Lansberg, C.Lorce, F.Lyonnet, Y.Makdisi, L.Massacrier, S.Porteboeuf, C.Quintans, A.Rakotozafindrabe, P.Robbe, W.Scandale, I.Schienbein, J.Seixas, H.S.Shao, A.Signori, N.Topilskaya, B.Trzeciak, A.Uras, J.Wagner, N.Yamanaka, Z.Yang, A.Zelenski A fixed-target programme at the LHC for heavy-ion, hadron, spin and astroparticle physics: AFTER@LHC
doi: 10.1016/j.nuclphysa.2018.09.063
2018TV01 Phys.Rev. C 97, 045204 (2018) V.Tvaskis, A.Tvaskis, I.Niculescu, D.Abbott, G.S.Adams, A.Afanasev, A.Ahmidouch, T.Angelescu, J.Arrington, R.Asaturyan, S.Avery, O.K.Baker, N.Benmouna, B.L.Berman, A.Biselli, H.P.Blok, W.U.Boeglin, P.E.Bosted, E.Brash, H.Breuer, G.Chang, N.Chant, M.E.Christy, S.H.Connell, M.M.Dalton, S.Danagoulian, D.Day, T.Dodario, J.A.Dunne, D.Dutta, N.El Khayari, R.Ent, H.C.Fenker, V.V.Frolov, D.Gaskell, K.Garrow, R.Gilman, P.Gueye, K.Hafidi, W.Hinton, R.J.Holt, T.Horn, G.M.Huber, H.Jackson, X.Jiang, M.K.Jones, K.Joo, J.J.Kelly, C.E.Keppel, J.Kuhn, E.Kinney, A.Klein, V.Kubarovsky, Y.Liang, G.Lolos, A.Lung, D.Mack, S.Malace, P.Markowitz, G.Mbianda, E.McGrath, D.Mckee, D.G.Meekins, H.Mkrtchyan, J.Napolitano, T.Navasardyan, G.Niculescu, M.Nozar, T.Ostapenko, Z.Papandreou, D.Potterveld, P.E.Reimer, J.Reinhold, J.Roche, S.E.Rock, E.Schulte, E.Segbefia, C.Smith, G.R.Smith, P.Stoler, V.Tadevosyan, L.Tang, J.Telfeyan, L.Todor, M.Ungaro, A.Uzzle, S.Vidakovic, A.Villano, W.F.Vulcan, G.Warren, F.Wesselmann, B.Wojtsekhowski, S.A.Wood, C.Yan, B.Zihlmann Measurements of the separated longitudinal structure function FL from hydrogen and deuterium targets at low Q2 NUCLEAR REACTIONS 1,2H(e, e'), E=2.24, 3.04, 4.41, 5.50 GeV; measured scattered electrons, differential σ(E, θ) using the high momentum spectrometer (HMS) and the short orbit spectrometer (SOS) at CEBAF-Thomas Jefferson National Accelerator (JLab) facility; deduced structure functions and longitudinal structure functions for protons and deuterons using Rosebluth separation technique, smaller longitudinal structure function and a smaller ratio of longitudinal to transverse cross section for deuteron than the proton, possible suppression of the gluonic distribution in nuclei. Comparison with parametrizations, previous experimental data, and theoretical predictions extrapolated to the beam energies investigated.
doi: 10.1103/PhysRevC.97.045204
2006HU09 Phys.Rev. C 73, 064004 (2006) B.Hu, M.K.Jones, P.E.Ulmer, H.Arenhovel, O.K.Baker, W.Bertozzi, E.J.Brash, J.Calarco, J.-P.Chen, E.Chudakov, A.Cochran, S.Dumalski, R.Ent, J.M.Finn, F.Garibaldi, S.Gilad, R.Gilman, C.Glashausser, J.Gomez, V.Gorbenko, J.-O.Hansen, J.Hovdebo, C.W.de Jager, S.Jeschonnek, X.Jiang, C.Keppel, A.Klein, A.Kozlov, S.Kuhn, G.Kumbartzki, M.Kuss, J.J.LeRose, M.Liang, N.Liyanage, G.J.Lolos, P.E.C.Markowitz, D.Meekins, R.Michaels, J.Mitchell, Z.Papandreou, C.F.Perdrisat, V.Punjabi, R.Roche, D.Rowntree, A.Saha, S.Strauch, L.Todor, G.Urciuoli, L.B.Weinstein, K.Wijesooriya, B.B.Wojtsekhowski, R.Woo Polarization transfer in the 2H(e(pol), e'p(pol))n reaction up to Q2 = 1.61 (GeV/c)2 NUCLEAR REACTIONS 1,2H(polarized e, e'p), E=1.669 GeV; measured recoil proton polarization vs momentum transfer, missing momentum; deduced form factor ratios. Comparison with model predictions.
doi: 10.1103/PhysRevC.73.064004
2004AM12 Phys.Rev. C 70, 035203 (2004) P.Ambrozewicz, J.Mitchell, J.Dunne, P.Markowitz, C.J.Martoff, J.Reinhold, B.Zeidman, D.J.Abbott, A.Ahmidouch, C.S.Armstrong, J.Arrington, K.A.Assamagan, K.Bailey, O.K.Baker, S.Beedoe, H.Breuer, R.Carlini, J.Cha, G.Collins, C.Cothran, W.J.Cummings, S.Danagoulian, D.Day, F.Duncan, D.Dutta, T.Eden, R.Ent, L.Ewell, H.T.Fortune, H.Gao, D.F.Geesaman, P.Gueye, K.K.Gustafsson, J.-O.Hansen, W.Hinton, C.E.Keppel, A.Klein, D.Koltenuk, D.J.Mack, R.Madey, D.G.Meekins, H.Mkrtchyan, R.M.Mohring, S.K.Mtingwa, G.Niculescu, I.Niculescu, T.G.O'Neill, D.Potterveld, J.W.Price, B.A.Raue, P.Roos, G.Savage, R.Sawafta, R.E.Segel, S.Stepanyan, V.Tadevosyan, L.Tang, B.P.Terburg, S.Wood, C.Yan, B.Zihlmann Near threshold electroproduction of the ω meson at Q2 ≈ 0.5 GeV2 NUCLEAR REACTIONS 1H(e, e'X), E=3.245 GeV; measured ω-meson production associated missing mass spectra, σ(θ); deduced possible resonance effects, other reaction mechanism features.
doi: 10.1103/PhysRevC.70.035203
2004KL02 Phys.Rev. C 69, 034338 (2004) A.Klein, P.Protopapas, S.G.Rohozinski, K.Starosta Kerman-Klein-Donau-Frauendorf model for odd-odd nuclei: Formal theory
doi: 10.1103/PhysRevC.69.034338
2003BE39 Phys.Lett. B 564, 199 (2003) J.Bermuth, P.Merle, C.Carasco, D.Baumann, R.Bohm, D.Bosnar, M.Ding, M.O.Distler, J.Friedrich, J.M.Friedrich, J.Golak, W.Glockle, M.Hauger, W.Heil, P.Jennewein, J.Jourdan, H.Kamada, A.Klein, M.Kohl, B.Krusche, K.W.Krygier, H.Merkel, U.Muller, R.Neuhausen, A.Nogga, Ch.Normand, E.Otten, Th.Pospischil, M.Potokar, D.Rohe, H.Schmieden, J.Schmiedeskamp, M.Seimetz, I.Sick, S.Sirca, R.Skibinski, G.Testa, Th.Walcher, G.Warren, M.Weis, H.Witala, H.Wohrle, M.Zeier The neutron charge from factor and target analyzing powers from 3He(pol)(e(pol), e'n) scattering NUCLEAR REACTIONS 3He(polarized e, e'n), E=854.5 MeV; measured particle spectra, asymmetries, analyzing power; deduced final state interaction effects. 1n deduced charge form factor. Polarized target.
doi: 10.1016/S0370-2693(03)00725-1
2003CA09 Phys.Lett. B 559, 41 (2003) C.Carasco, J.Bermuth, P.Merle, P.Bartsch, D.Baumann, R.Bohm, D.Bosnar, M.Ding, M.O.Distler, J.Friedrich, J.M.Friedrich, J.Golak, W.Glockle, M.Hauger, W.Heil, P.Jennewein, J.Jourdan, H.Kamada, A.Klein, M.Kohl, K.W.Krygier, H.Merkel, U.Muller, R.Neuhausen, A.Nogga, Ch.Normand, E.Otten, Th.Pospischil, M.Potokar, D.Rohe, H.Schmieden, J.Schmiedeskamp, M.Seimetz, I.Sick, S.Sirca, R.Skibinski, G.Testa, Th.Walcher, G.Warren, M.Weis, H.Witala, H.Wohrle, M.Zeier Final state interaction effects in 3He(pol)(e(pol), e'p) NUCLEAR REACTIONS 3He(polarized e, e'p), E=854.5 MeV; measured Ep, σ(θ), asymmetries; deduced final-state interaction effects. Polarized target, comparison with model predictions.
doi: 10.1016/S0370-2693(03)00306-X
2003DU23 Phys.Rev. C 68, 064603 (2003) D.Dutta, D.van Westrum, D.Abbott, A.Ahmidouch, Ts.A.Amatuoni, C.Armstrong, J.Arrington, K.A.Assamagan, K.Bailey, O.K.Baker, S.Barrow, K.Beard, D.Beatty, S.Beedoe, E.Beise, E.Belz, C.Bochna, P.E.Bosted, H.Breuer, E.E.W.Bruins, R.Carlini, J.Cha, N.Chant, C.Cothran, W.J.Cummings, S.Danagoulian, D.Day, D.DeSchepper, J.-E.Ducret, F.Duncan, J.Dunne, T.Eden, R.Ent, H.T.Fortune, V.Frolov, D.F.Geesaman, H.Gao, R.Gilman, P.Gueye, J.O.Hansen, W.Hinton, R.J.Holt, C.Jackson, H.E.Jackson, C.Jones, S.Kaufmann, J.J.Kelly, C.Keppel, M.Khandaker, W.Kim, E.Kinney, A.Klein, D.Koltenuk, L.Kramer, W.Lorenzon, A.Lung, K.McFarlane, D.J.Mack, R.Madey, P.Markowitz, J.Martin, A.Mateos, D.Meekins, M.A.Miller, R.Milner, J.Mitchell, R.Mohring, H.Mkrtchyan, A.M.Nathan, G.Niculescu, I.Niculescu, T.G.O'Neill, D.Potterveld, J.W.Price, J.Reinhold, C.Salgado, J.P.Schiffer, R.E.Segel, P.Stoler, R.Suleiman, V.Tadevosyan, L.Tang, B.Terburg, T.P.Welch, C.Williamson, S.Wood, C.Yan, J.-C.Yang, J.Yu, B.Zeidman, W.Zhao, B.Zihlmann Quasielastic (e, e'p) reaction on 12C, 56Fe, and 197Au NUCLEAR REACTIONS 12C, 56Fe, 197Au(e, e'p), E=0.845-3.345 GeV; measured missing energy, momentum distributions; deduced spectral functions. Comparison with model predictions.
doi: 10.1103/PhysRevC.68.064603
2001AN39 Fizika(Zagreb) B10, 279 (2001) D.Androic, G.Backenstoss, D.Bosnar, T.Dooling, P.A.M.Gram, N.K.Gregory, A.Hoffart, C.H.Q.Ingram, A.Klein, K.Koch, J.Kohler, B.Kotlinski, M.Kroedel, G.Kyle, A.Lehmann, A.O.Mateos, K.Michaelian, T.Petkovic, M.Planinic, R.P.Redwine, D.Rowntree, N.Simicevic, R.Trezeciak, H.Ullrich, H.J.Weyer, M.Wildi, K.E.Wilson Multinucleon Emission following the Pion Absorption in N, Ar and Xe NUCLEAR REACTIONS N, Ar, Xe(π+, xnyp), E=118, 162, 239 MeV; measured total pion absorption σ, partial yields from several multinucleon emission channels.
2001JO09 Phys.Rev.Lett. 86, 4483 (2001) M.B.Johnson, B.Z.Kopeliovich, I.K.Potashnikova, P.L.McGaughey, J.M.Moss, J.C.Peng, G.T.Garvey, M.J.Leitch, M.R.Adams, D.M.Alde, H.W.Baer, M.L.Bartlett, C.N.Brown, W.E.Cooper, T.A.Carey, G.Danner, G.W.Hoffmann, Y.B.Hsiung, D.M.Kaplan, A.Klein, C.Lee, J.W.Lillberg, R.L.McCarthy, C.S.Mishra, M.J.Wang, and the FNAL E772 Collaboration Energy Loss of Fast Quarks in Nuclei NUCLEAR REACTIONS 2H, C, Ca, Fe, W(p, X), E at 800 GeV/c; measured dimuon Drell-Yan yields; deduced quark energy loss in nuclear environment.
doi: 10.1103/PhysRevLett.86.4483
2001KH19 Phys.Rev. C64, 064606 (2001) M.G.Khayat, P.G.Roos, N.S.Chant, A.P.Dvoredsky, H.Breuer, J.J.Kelly, B.S.Flanders, T.M.Payerle, F.Adimi, T.Gu, J.Huffman, A.Klein, T.Dooling, T.Greco, G.S.Kyle, T.Chang, Z.Lin, M.Wang, R.Meier, S.Ritt, K.Koch, J.Konter, S.Kovalev, S.Mango, B.Van Den Brandt, J.Lawrie Analyzing Power Reduction in Quasifree Pion-Nucleon Knockout Reactions NUCLEAR REACTIONS 7Li(π+, π+'p), E=240 MeV; measured σ(E, θ), Ay(θ); deduced spin dependence in Δ-nucleus potential. Polarized target, DWIA calculations.
doi: 10.1103/PhysRevC.64.064606
2001KL01 Phys.Rev. C63, 014316 (2001) Foundations of Self-Consistent Particle-Rotor Models and of Self-Consistent Cranking Models
doi: 10.1103/PhysRevC.63.014316
2001RE09 Nucl.Phys. A684, 470c (2001) J.Reinhold, D.Abbott, A.Ahmidouch, P.Ambrozewicz, C.S.Armstrong, J.Arrington, R.Asaturyan, K.Assamagan, S.Avery, K.Bailey, O.K.Baker, S.Beedoe, H.Bitao, W.Boeglin, H.Breuer, D.S.Brown, R.Carlini, J.Cha, N.Chant, E.Christy, A.Cochran, L.Cole, G.Collins, C.Cothran, J.Crowder, W.J.Cummings, S.Danagoulian, F.Dohrmann, F.Duncan, J.Dunne, D.Dutta, T.Eden, M.Elaasar, R.Ent, L.Ewell, H.Fenker, H.T.Fortune, Y.Fujii, L.Gan, H.Gao, K.Garrow, D.F.Geesaman, P.Gueye, K.Gustafsson, K.Hafidi, J.O.Hansen, W.Hinton, H.E.Jackson, H.Juengst, C.Keppel, A.Klein, D.Koltenuk, Y.Liang, J.H.Liu, A.Lung, D.Mack, R.Madey, P.Markowitz, C.J.Martoff, D.Meekins, J.Mitchell, T.Miyoshi, H.Mkrtchyan, R.Mohring, S.K.Mtingwa, B.Mueller, T.G.O'Neill, G.Niculescu, I.Niculescu, D.Potterveld, J.W.Price, B.A.Raue, P.E.Reimer, J.Roche, P.Roos, M.Sarsour, Y.Sato, G.Savage, R.Sawafta, J.P.Schiffer, R.E.Segel, A.Semenov, S.Stepanyan, V.Tadevosian, S.Tajima, L.Tang, B.Terburg, A.Uzzle, S.Wood, H.Yamaguchi, C.Yan, C.Yan, L.Yuan, B.Zeidman, M.Zeier, B.Zihlmann Electroproduction of Kaons and Light Hypernuclei NUCLEAR REACTIONS 2H, 3,4He(e, e'K+), E=3.245 MeV; measured hyperon production associated missing mass spectra. Comparison with Monte Carlo simulations.
doi: 10.1016/S0375-9474(01)00509-7
2001ZE06 Nucl.Phys. A691, 37c (2001) B.Zeidman, D.Abbott, A.Ahmidouch, P.Ambrozewicz, C.S.Armstrong, J.Arrington, R.Asaturyan, K.Assamagan, S.Avery, K.Bailey, O.K.Baker, S.Beedoe, H.Bitao, H.Breuer, D.S.Brown, R.Carlini, J.Cha, N.Chant, E.Christy, A.Cochran, L.Cole, G.Collins, C.Cothran, J.Crowder, W.J.Cummings, S.Danagoulian, F.Dohrmann, F.Duncan, J.Dunne, D.Dutta, T.Eden, M.Elaasar, R.Ent, L.Ewell, H.Fenker, H.T.Fortune, Y.Fujii, L.Gan, H.Gao, K.Garrow, D.Y.Geesaman, P.Gueye, K.Gustafsson, K.Hafidi, J.O.Hansen, W.Hinton, H.E.Jackson, H.Juengst, C.Keppel, A.Klein, D.Koltenuk, Y.Liang, J.H.Liu, A.Lung, D.Mack, R.Madey, P.Markowitz, C.J.Martoff, D.Meekins, J.Mitchell, T.Miyoshi, H.Mkrtchyan, R.Mohring, S.K.Mtingwa, B.Mueller, T.G.O'Neill, G.Niculescu, I.Niculescu, D.Potterveld, J.W.Price, B.A.Raue, P.E.Reimer, J.Reinhold, J.Roche, P.Roos, M.Sarsour, Y.Sato, G.Savage, R.Sawafta, J.P.Schiffer, R.E.Segel, A.Semenov, S.Stepanyan, V.Tadevosian, S.Tajima, L.Tang, B.Terburg, A.Uzzle, S.Wood, H.Yamaguchi, C.Yan, C.Yan, L.Yuan, M.Zeier, B.Zihlmann Electroproduction of Kaons on Light Nuclei NUCLEAR REACTIONS 1,2H, 3,4He(e, e'K+), E=3.245 GeV; measured hyperon production associated missing mass spectra; deduced possible hypernucleus bound states. Comparisons with model predictions.
doi: 10.1016/S0375-9474(01)00999-X
2000DO17 Phys.Rep. 335, 93 (2000) Self-Consistent Theory of Large-Amplitude Collective Motion: Applications to approximate quantization of nonseparable systems and to nuclear physics
doi: 10.1016/S0370-1573(99)00119-2
2000DU12 Phys.Rev. C61, 061602 (2000) D.Dutta, D.van Westrum, D.Abbott, A.Ahmidouch, Ts.A.Amatuni, C.Armstrong, J.Arrington, K.A.Assamagan, K.Bailey, O.K.Baker, S.Barrow, K.Beard, D.Beatty, S.Beedoe, E.Beise, J.E.Belz, C.Bochna, P.E.Bosted, H.Breuer, E.E.W.Bruins, R.Carlini, J.Cha, N.Chant, R.E.Chrien, C.Cothran, W.J.Cummings, S.Danagoulian, D.Day, D.DeSchepper, J.-E.Ducret, F.Duncan, J.Dunne, T.Eden, R.Ent, H.T.Fortune, V.Frolov, D.F.Geesaman, H.Gao, R.Gilman, P.Gueye, J.O.Hansen, W.Hinton, R.J.Holt, C.Jackson, H.E.Jackson, C.Jones, S.Kaufman, J.J.Kelly, C.Keppel, M.Khandaker, W.Kim, E.Kinney, A.Klein, D.Koltenuk, L.Kramer, W.Lorenzon, K.McFarlane, D.J.Mack, R.Madey, P.Markowitz, J.Martin, A.Mateos, D.Meekins, E.Meier, M.A.Miller, R.Milner, J.Mitchell, R.Mohring, H.Mkrtchyan, A.M.Nathan, G.Niculescu, I.Niculescu, T.G.O'Neill, D.Potterveld, J.W.Price, J.Reinhold, C.Salgado, J.P.Schiffer, R.E.Segel, P.Stoler, R.Suleiman, R.Sawafta, R.J.Sutter, V.Tadevosyan, L.Tang, B.Terburg, T.P.Welch, C.Williamson, S.Wood, C.Yan, J.-C.Yang, J.Yu, B.Zeidman, W.Zhao, B.Zihlmann Separated Spectral Functions for the Quasifree 12C(e, e'p) Reaction NUCLEAR REACTIONS 12C(e, e'p), E=0.845-3.245 GeV; measured transverse and longitudinal spectral functions vs proton energy; deduced momentum transfer dependence, role of multinucleon processes.
doi: 10.1103/PhysRevC.61.061602
2000GE20 Hyperfine Interactions 129, 271 (2000) W.Geithner, U.Georg, S.Kappertz, M.Keim, A.Klein, P.Lievens, R.Neugart, M.Neuroth, L.Vermeeren, S.Wilbert, and the ISOLDE Collaboration Measurement of nuclear moments and radii by collinear laser spectroscopy and by β-NMR spectroscopy NUCLEAR MOMENTS 7,9,10,11Be, 20,26,27,28,29,30,31Na, 32,33,34,35,36,37,38,39,40,46Ar; measured β assymetry, hfs; deduced μ, quadrupole moments, mean squared charge radii.
doi: 10.1023/A:1012642707147
2000KE09 Eur.Phys.J. A 8, 31 (2000) M.Keim, U.Georg, A.Klein, R.Neugart, M.Neuroth, S.Wilbert, P.Lievens, L.Vermeeren, B.A.Brown, and the ISOLDE Collaboration Measurement of the Electric Quadrupole Moments of 26-29Na NUCLEAR MOMENTS 26,27,28,29,30,31Na; measured β-NMR spectra; deduced μ. 26,27,28,29Na deduced quadrupole moments. Oriented nuclei, optical pumping. RADIOACTIVITY 26,27,28,29,30,31Na(β-) [from U(p, X)]; measured β-NMR spectra; deduced μ. 26,27,28,29Na deduced quadrupole moments. Oriented nuclei, optical pumping.
doi: 10.1007/s100500070117
2000KL07 Radiochim.Acta 88, 253 (2000) A.T.J.Klein, F.Rosch, S.M.Qaim Investigation of 50Cr(d, n)51Mn and natCr(p, x)51Mn Processes with Respect to the Production of the Positron Emitter 51Mn NUCLEAR REACTIONS 50Cr(d, n), (d, 2n), (d, t), (d, p), (d, 2p), (d, α), E=3-13 MeV; Cr(p, X)52Mn/54Mn/48Cr/49Cr/51Cr/48V/45Ti, E=18-38 MeV; measured production σ; deduced thick target yields. Radiochemical separation. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0771. 2000KO66 Eur.Phys.J. A 9, 537 (2000) B.Kotlinski, D.Androic, G.Backenstoss, D.Bosnar, H.Dobbeling, T.Dooling, M.Furic, P.A.M.Gram, N.K.Gregory, A.Hoffart, C.H.Q.Ingram, A.Klein, K.Koch, J.Kohler, M.Kroedel, G.Kyle, A.Lehmann, V.Markushin, A.O.Mateos, K.Michaelian, T.Petkovic, M.Planinic, R.P.Redwine, D.Rowntree, N.Simicevic, R.Trezeciak, H.J.Weyer, M.Wildi, K.E.Wilson, and the LADS Collaboration Pion Absorption Reactions on N, Ar and Xe NUCLEAR REACTIONS Ar(π+, 2pX), (π+, pdX), E=70, 118, 162, 239, 330 MeV; N, Xe(π+, 2pX), (π+, pdX), E=239 MeV; measured absorption reaction channels σ, proton spectra, particle multiplicities. Large-acceptance detector system.
doi: 10.1007/s100500070010
2000PL03 Phys.Rev. C61, 054604 (2000) M.Planinic, D.Androic, G.Backenstoss, D.Bosnar, T.Dooling, M.Furic, P.A.M.Gram, N.K.Gregory, A.Hoffart, C.H.Q.Ingram, A.Klein, K.Koch, J.Kohler, B.Kotlinski, M.Kroedel, G.Kyle, A.Lehmann, A.O.Mateos, K.Michaelian, T.Petkovic, R.P.Redwine, D.Rowntree, N.Simicevic, R.Trezeciak, H.Ullrich, H.J.Weyer, M.Wildi, K.E.Wilson, and the LADS Collaboration Pion Absorption on 4He into the ppd Final State NUCLEAR REACTIONS 4He(π+, pd), E=70, 118, 162, 239, 330 MeV; measured deuteron, proton spectra, σ(θ); deduced reaction mechanism features. Comparison with model predictions.
doi: 10.1103/PhysRevC.61.054604
1999DO04 Phys.Rev. C59, 2065 (1999) G.Do Dang, A.Klein, P.-G.Reinhard Self-Consistent Theory of Large Amplitude Collective Motion at Finite Excitation Energy
doi: 10.1103/PhysRevC.59.2065
1999DO25 Phys.Rev. C60, 044306 (1999) G.Do Dang, A.Klein, P.-G.Reinhard Model of a Self-Consistent Theory of Large Amplitude Collective Motion at Finite Excitation Energy
doi: 10.1103/PhysRevC.60.044306
1999LE33 Phys.Rev. C60, 024603 (1999) A.Lehmann, D.Androic, G.Backenstoss, D.Bosnar, T.Dooling, M.Furic, P.A.M.Gram, N.K.Gregory, A.Hoffart, C.H.Q.Ingram, A.Klein, K.Koch, J.Kohler, B.Kotlinski, M.Kroedel, G.Kyle, A.O.Mateos, K.Michaelian, T.Petkovic, M.Planinic, R.P.Redwine, D.Rowntree, N.Simicevic, R.Trezeciak, H.Ullrich, H.J.Weyer, M.Wildi, K.E.Wilson, and the LADS Collaboration Total Cross Sections of the Charge Exchange Reaction (π+, π0) on 2H, 3He, and 4He Across the Δ(1232) Resonance NUCLEAR REACTIONS 2H, 3,4He(π+, π0), 2H(π+, π+n), E=70, 118, 162, 239, 330 MeV; measured total σ; deduced multiple scattering contributions, role of resonance. Comparison with previous results, model predictions.
doi: 10.1103/PhysRevC.60.024603
1999ME24 Phys.Rev. C60, 052201 (1999) D.G.Meekins, D.J.Abbott, A.Ahmidouch, C.S.Armstrong, J.Arrington, K.Assamagan, O.K.Baker, S.P.Barrow, D.P.Beatty, D.H.Beck, S.Y.Beedoe, E.J.Beise, J.E.Belz, C.Bochna, P.E.Bosted, E.J.Brash, H.Breuer, R.V.Cadman, L.Cardman, R.D.Carlini, J.Cha, N.S.Chant, G.Collins, C.Cothran, W.J.Cummings, S.Danagoulian, F.A.Duncan, J.A.Dunne, D.Dutta, T.Eden, R.Ent, B.W.Filippone, T.A.Forest, H.T.Fortune, V.V.Frolov, H.Gao, D.F.Geesaman, R.Gilman, P.L.J.Gueye, K.K.Gustafsson, J.-O.Hansen, M.Harvey, W.Hinton, R.J.Holt, H.E.Jackson, C.E.Keppel, M.A.Khandaker, E.R.Kinney, A.Klein, D.M.Koltenuk, G.Kumbartzki, A.F.Lung, D.J.Mack, R.Madey, P.Markowitz, K.W.McFarlane, R.D.McKeown, Z.-E.Meziani, M.A.Miller, J.H.Mitchell, H.G.Mkrtchyan, R.M.Mohring, J.Napolitano, A.M.Nathan, G.Niculescu, I.Niculescu, T.G.O'Neill, B.R.Owen, S.F.Pate, D.H.Potterveld, J.W.Price, G.L.Rakness, R.D.Ransome, J.Reinhold, P.M.Rutt, C.W.Salgado, G.Savage, R.E.Segel, N.Simicevic, P.Stoler, R.Suleiman, L.Tang, B.P.Terburg, D.van Westrum, W.F.Vulcan, S.E.Williamson, M.T.Witkowski, S.A.Wood, C.Yan, B.Zeidman Coherent π0 Photoproduction on the Deuteron up to 4 GeV NUCLEAR REACTIONS 2H(γ, π0), E=0.8-4.0 GeV bremsstrahlung; measured σ(E, θ). Comparison with previous data, model predictions.
doi: 10.1103/PhysRevC.60.052201
1999PL04 Fizika(Zagreb) B8, 113 (1999) M.Planinic, D.Androic, G.Backenstoss, D.Bosnar, T.Dooling, M.Furic, P.A.M.Gram, N.K.Gregory, A.Hoffart, C.H.Q.Ingram, A.Klein, K.Koch, J.Kohler, B.Kotlinski, M.Kroedel, G.Kyle, A.Lehmann, A.O.Mateos, K.Michaelian, T.Petkovic, R.P.Redwine, D.Rowntree, N.Simicevic, R.Trezeciak, H.Ullrich, H.J.Weyer, M.Wildi, K.E.Wilson, and the LADS Collaboration Pion Absorption in 4He NUCLEAR REACTIONS 4He(π+, X), E=70-330 MeV; measured particle spectra; deduced absorption cross section and its decomposition in different exit channels. LADS detector.
1999RO19 Phys.Rev.Lett. 83, 4257 (1999) D.Rohe, P.Bartsch, D.Baumann, J.Becker, J.Bermuth, K.Bohinc, R.Bohm, S.Buttazzoni, T.Caprano, N.Clawiter, A.Deninger, S.Derber, M.Ding, M.Distler, A.Ebbes, M.Ebert, I.Ewald, J.Friedrich, J.M.Friedrich, R.Geiges, T.Grossmann, M.Hauger, W.Heil, A.Honegger, P.Jennewein, J.Jourdan, M.Kahrau, A.Klein, M.Kohl, K.W.Krygier, G.Kubon, A.Liesenfeld, H.Merkel, K.Merle, P.Merle, M.Muhlbauer, U.Muller, R.Neuhausen, E.W.Otten, Th.Petitjean, Th.Pospischil, M.Potokar, G.Rosner, H.Schmieden, I.Sick, S.Sirca, R.Surkau, A.Wagner, Th.Walcher, G.Warren, M.Weis, H.Wohrle, M.Zeier Measurement of the Neutron Electric Form Factor Gen at 0.67 (GeV/c)2 via 3He(pol)(e(pol), e'n) NUCLEAR REACTIONS 3He(polarized e, e'n), E=854 MeV; measured electron spectra, neutron spectra, asymmetries. 1n deduced electric form factor. Polarized target.
doi: 10.1103/PhysRevLett.83.4257
1999RO20 Phys.Rev. C60, 054610 (1999) D.Rowntree, D.Androic, G.Backenstoss, D.Bosnar, H.Breuer, T.Dooling, M.Furic, P.A.M.Gram, N.K.Gregory, A.Hoffart, C.H.Q.Ingram, A.Klein, K.Koch, J.Kohler, B.Kotlinski, M.Kroedel, G.Kyle, A.Lehmann, A.O.Mateos, K.Michaelian, T.Petkovic, M.Planinic, R.P.Redwine, N.Simicevic, R.Trezeciak, H.J.Weyer, M.Wildi, K.E.Wilson, and the LADS Collaboration π+ Absorption on N and Ar NUCLEAR REACTIONS N, Ar(π+, X), E=118, 162, 239 MeV; measured total absorption σ, final state particle multiplicities; deduced average number of participating nucleons.
doi: 10.1103/PhysRevC.60.054610
1998AB18 Phys.Rev.Lett. 80, 5072 (1998) D.Abbott, A.Ahmidouch, Ts.A.Amatuni, C.Armstrong, J.Arrington, K.A.Assamagan, K.Bailey, O.K.Baker, S.Barrow, K.Beard, D.Beatty, S.Beedoe, E.Beise, J.E.Belz, C.Bochna, H.Breuer, E.E.W.Bruins, R.Carlini, J.Cha, N.Chant, C.Cothran, W.J.Cummings, S.Danagoulian, D.Day, D.DeSchepper, J.-E.Ducret, F.Duncan, J.Dunne, D.Dutta, T.Eden, R.Ent, H.T.Fortune, V.Frolov, D.F.Geesaman, H.Gao, R.Gilman, P.Gueye, J.O.Hansen, W.Hinton, R.J.Holt, C.Jackson, H.E.Jackson, C.E.Jones, S.Kaufman, J.J.Kelly, C.Keppel, M.Khandaker, W.Kim, E.Kinney, A.Klein, D.Koltenuk, L.Kramer, W.Lorenzon, K.McFarlane, D.J.Mack, R.Madey, P.Markowitz, J.Martin, A.Mateos, D.Meekins, M.A.Miller, R.Milner, J.Mitchell, R.Mohring, H.Mkrtchyan, A.M.Nathan, G.Niculescu, I.Niculescu, T.G.O'Neill, D.Potterveld, J.W.Price, J.Reinhold, C.Salgado, J.P.Schiffer, R.E.Segel, P.Stoler, R.Suleiman, V.Tadevosyan, L.Tang, B.Terburg, D.van Westrum, P.Welch, C.Williamson, S.Wood, C.Yan, J.-C.Yang, J.Yu, B.Zeidman, W.Zhao, B.Zihlmann Quasifree (e, e'p) Reactions and Proton Propagation in Nuclei NUCLEAR REACTIONS C, Fe, 197Au(e, e'p), E=2.45, 3.25 GeV; measured σ(θ), σ(Q2); deduced nuclear medium effects.
doi: 10.1103/PhysRevLett.80.5072
1998BO29 Phys.Rev.Lett. 81, 4576 (1998) C.Bochna, B.P.Terburg, D.J.Abbott, A.Ahmidouch, C.S.Armstrong, J.Arrington, K.A.Assamagan, O.K.Baker, S.P.Barrow, D.P.Beatty, D.H.Beck, S.Y.Beedoe, E.J.Beise, J.E.Belz, P.E.Bosted, E.J.Brash, H.Breuer, R.V.Cadman, L.Cardman, R.D.Carlini, J.Cha, N.S.Chant, G.Collins, C.Cothran, W.J.Cummings, S.Danagoulian, F.A.Duncan, J.A.Dunne, D.Dutta, T.Eden, R.Ent, B.W.Filippone, T.A.Forest, H.T.Fortune, V.V.Frolov, H.Gao, D.F.Geesaman, R.Gilman, P.L.J.Gueye, K.K.Gustafsson, J.-O.Hansen, M.Harvey, W.Hinton, R.J.Holt, H.E.Jackson, C.E.Keppel, M.A.Khandaker, E.R.Kinney, A.Klein, D.M.Koltenuk, G.Kumbartzki, A.F.Lung, D.J.Mack, R.Madey, P.Markowitz, K.W.McFarlane, R.D.McKeown, D.G.Meekins, Z.-E.Meziani, M.A.Miller, J.H.Mitchell, H.G.Mkrtchyan, R.M.Mohring, J.Napolitano, A.M.Nathan, G.Niculescu, I.Niculescu, T.G.O'Neill, B.R.Owen, S.F.Pate, D.H.Potterveld, J.W.Price, G.L.Rakness, R.Ransome, J.Reinhold, P.M.Rutt, C.W.Salgado, G.Savage, R.E.Segel, N.Simicevic, P.Stoler, R.Suleiman, L.Tang, D.van Westrum, W.F.Vulcan, S.Williamson, M.T.Witkowski, S.A.Wood, C.Yan, B.Zeidman Measurements of Deuteron Photodisintegration up to 4.0 GeV NUCLEAR REACTIONS 2H(γ, p), E=0.4-4 GeV; measured σ(θ). Quark-gluon string model, reduced nuclear amplitude analysis, asymptotic meson exchange model.
doi: 10.1103/PhysRevLett.81.4576
1998GE13 Eur.Phys.J. A 3, 225 (1998) U.Georg, W.Borchers, M.Keim, A.Klein, P.Lievens, R.Neugart, M.Neuroth, P.M.Rao, Ch.Schulz, and the ISOLDE Collaboration Laser Spectroscopy Investigation of the Nuclear Moments and Radii of Lutetium Isotopes NUCLEAR MOMENTS 161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179Lu; measured hfs, spins, Q, μ, radii for ground, isomeric states; deduced Nilsson configurations. Collinear laser spectroscopy.
doi: 10.1007/s100500050172
1997LE08 Phys.Rev. C55, 2931 (1997) A.Lehmann, D.Androic, G.Backenstoss, D.Bosnar, H.Breuer, H.Dobbeling, T.Dooling, M.Furic, P.A.M.Gram, N.K.Gregory, A.Hoffart, C.H.Q.Ingram, A.Klein, K.Koch, J.Kohler, B.Kotlinski, M.Kroedel, G.Kyle, A.O.Mateos, K.Michaelian, T.Petkovic, M.Planinic, R.P.Redwine, D.Rowntree, U.Sennhauser, N.Simicevic, R.Trezeciak, H.Ullrich, M.Wang, M.H.Wang, H.J.Weyer, M.Wildi, K.E.Wilson, and the LADS Collaboration Pion Absorption on 3He and 4He with Emission of Three Energetic Protons NUCLEAR REACTIONS 3,4He(π+, 3p), E=70, 118, 162, 239, 330 MeV; measured total absorption σ for complete set of variables; deduced initial, final state interaction signatures related features. Final state interaction, 3N phase space. Large acceptance detector system.
doi: 10.1103/PhysRevC.55.2931
1997LE18 Phys.Rev. C56, 1872 (1997) A.Lehmann, D.Androic, G.Backenstoss, D.Bosnar, H.Breuer, H.Dobbeling, T.Dooling, M.Furic, P.A.M.Gram, N.K.Gregory, A.Hoffart, C.H.Q.Ingram, A.Klein, K.Koch, J.Kohler, B.Kotlinski, M.Kroedel, G.Kyle, A.O.Mateos, K.Michaelian, T.Petkovic, M.Planinic, R.P.Redwine, D.Rowntree, U.Sennhauser, N.Simicevic, R.Trezeciak, H.Ullrich, M.Wang, M.H.Wang, H.J.Weyer, M.Wildi, K.E.Wilson Multinucleon Pion Absorption on 4He into the pppn Final State NUCLEAR REACTIONS 4He(π+, 3p), (π+, n2p), (π+, n3p), E=70, 118, 162, 239, 330 MeV; measured total absorption σ, differential σ over complete set of variables; deduced initial-, final-state interaction effects, no evidence for "double-Δ" mechanism.
doi: 10.1103/PhysRevC.56.1872
1997PR01 Phys.Rev. C55, 699 (1997) Derivation and Assessment of Strong Coupling Core-Particle Model from Kerman-Klein-Donau-Frauendorf Theory NUCLEAR STRUCTURE 157Gd; calculated levels, B(λ). 157Tb; calculated levels. Semi-microscopic core-particle coupling method.
doi: 10.1103/PhysRevC.55.699
1997PR03 Phys.Rev. C55, 1810 (1997) Possible Solution of the Coriolis Attenuation Problem NUCLEAR STRUCTURE 157Gd, 159Dy; calculated negative parity energy levels. 157Tb; calculated positive energy levels. 163Er; calculated levels; deduced Coriolis coupling attenuation related features.
doi: 10.1103/PhysRevC.55.1810
1997PR04 Phys.Rev.Lett. 78, 4347 (1997) Application of the Kerman-Klein Method to the Solution of a Spherical Shell Model for a Deformed Rare-Earth Nucleus NUCLEAR STRUCTURE 158Gd; calculated particle number, ground state properties, different contributions to the moment of inertia.
doi: 10.1103/PhysRevLett.78.4347
1996AB02 Phys.Rev.Lett. 76, 587 (1996) K.Abe, T.Akagi, P.L.Anthony, R.Antonov, R.G.Arnold, T.Averett, H.R.Band, J.M.Bauer, H.Borel, P.E.Bosted, V.Breton, J.Button-Shafer, J.P.Chen, T.E.Chupp, J.Clendenin, C.Comptour, K.P.Coulter, G.Court, D.Crabb, M.Daoudi, D.Day, F.S.Dietrich, J.Dunne, H.Dutz, R.Erbacher, J.Fellbaum, A.Feltham, H.Fonvieille, E.Frlez, D.Garvey, R.Gearhart, J.Gomez, P.Grenier, K.A.Griffioen, S.Hoibraten, E.W.Hughes, C.Hyde-Wright, J.R.Johnson, D.Kawall, A.Klein, S.E.Kuhn, M.Kuriki, R.Lindgren, T.J.Liu, R.M.Lombard-Nelsen, J.Marroncle, T.Maruyama, X.K.Maruyama, J.McCarthy, W.Meyer, Z.-E.Meziani, R.Minehart, J.Mitchell, J.Morgenstern, G.G.Petratos, R.Pitthan, D.Pocanic, C.Prescott, R.Prepost, P.Raines, B.Raue, D.Reyna, A.Rijllart, Y.Roblin, L.S.Rochester, S.E.Rock, O.A.Rondon, I.Sick, L.C.Smith, T.B.Smith, M.Spengos, F.Staley, P.Steiner, S.St.Lorant, L.M.Stuart, F.Suekane, Z.M.Szalata, H.Tang, Y.Terrien, T.Usher, D.Walz, J.L.White, K.Witte, C.C.Young, B.Youngman, H.Yuta, G.Zapalac, B.Zihlmann, D.Zimmermann, and the E143 Collaboration Measurements of the Proton and Deuteron Spin Structure Function g2 and Asymmetry A2 NUCLEAR STRUCTURE 1,2H; analyzed data; deduced spin structure function, asymmetry data. Polarized ammonia targets, (polarized e, e') reaction. NUCLEAR REACTIONS 1,2H(polarized e, e'), E=29.1 GeV; measured spin asymmetries. 1,2H deduced spin structure functions. Polarized ammonia targets.
doi: 10.1103/PhysRevLett.76.587
1996AN06 Phys.Rev. C53, R2591 (1996) D.Androic, G.Backenstoss, D.Bosnar, H.Breuer, H.Dobbeling, T.Dooling, M.Furic, P.A.M.Gram, N.K.Gregory, A.Hoffart, C.H.Q.Ingram, A.Klein, K.Koch, J.Kohler, B.Kotlinski, M.Kroedel, G.Kyle, A.Lehmann, A.O.Mateos, K.Michaelian, T.Petkovic, R.P.Redwine, D.Rowntree, U.Sennhauser, N.Simicevic, R.Trezeciak, H.Ullrich, M.Wang, M.H.Wang, H.J.Weyer, M.Wildi, K.E.Wilson, and the LADS Collaboration Evidence of Initial State Interactions in Multinucleon Pion Absorption NUCLEAR REACTIONS 3,4He, N, Ar(π+, X), E=239 MeV; measured proton kinetic energy spectra, σ(θ) for 3p final states; deduced initial state interactions role in pion absorption.
doi: 10.1103/PhysRevC.53.R2591
1996BA32 Phys.Lett. 379B, 60 (1996) G.Backenstoss, D.Bosnar, H.Breuer, H.Dobbeling, T.Dooling, M.Furic, P.A.M.Gram, N.K.Gregory, A.Hoffart, C.H.Q.Ingram, A.Klein, K.Koch, J.Kohler, B.Kotlinski, M.Kroedel, G.Kyle, A.Lehmann, A.O.Mateos, K.Michaelian, T.Petkovic, R.P.Redwine, D.Rowntree, U.Sennhauser, N.Simicevic, R.Trezeciak, H.Ullrich, M.Wang, M.H.Wang, H.J.Weyer, M.Wildi, K.E.Wilson, and the LADS Collaboration Contribution of Initial State Interactions to the Three-Nucleon Absorption of Pions by 3He NUCLEAR REACTIONS 3He(π+, xp), E=118-239 MeV; measured proton distribution following pion absorption; deduced initial state interactions role.
doi: 10.1016/0370-2693(96)00326-7
1996KE08 Hyperfine Interactions 97/98, 543 (1996) M.Keim, U.Georg, A.Klein, R.Neugart, M.Neuroth, S.Wilbert, P.Lievens, L.Vermeeren, and the ISOLDE Collaboration Optical Polarization of Neutron-Rich Sodium Isotopes and β-NMR Measurements of Quadrupole Moments RADIOACTIVITY 26,27,28,29,30,31Na(β-); measured β-NMR; deduced quadrupole interaction constants in some cases. 27,28Na deduced electric quadrupole moment relative to 26Na. On-beam polarization by optical pumping.
doi: 10.1007/BF02150197
1996KL04 Nucl.Phys. A607, 1 (1996) A.Klein, B.A.Brown, U.Georg, M.Keim, P.Lievens, R.Neugart, M.Neuroth, R.E.Silverans, L.Vermeeren, and the ISOLDE Collaboration Moments and Mean Square Charge Radii of Short-Lived Argon Isotopes NUCLEAR MOMENTS 36,38,40Ar; measured isotope shifts, hfs; deduced hyperfine constants, spins I, μ, electric quadrupole moments, mean square charge radii. Collinear fast-beam laser spectroscopy, collisional ionization and β-detection. Shell model. RADIOACTIVITY 32,33,34,35Ar(β+); 37Ar(EC); 39,46Ar(β-); measured isotope shifts, hfs; deduced hyperfine constants, spins I, μ, electric quadrupole moments, mean square charge radii. Collinear fast-beam laser spectroscopy, collisional ionization and β-detection. Shell model.
doi: 10.1016/S0375-9474(96)00192-3
1996LI25 Europhys.Lett. 33, 11 (1996) P.Lievens, E.Arnold, W.Borchers, U.Georg, M.Keim, A.Klein, R.Neugart, L.Vermeeren, R.E.Silverans On the Odd-Even Staggering of Mean-Square Charge Radii in the Light Krypton and Strontium Region NUCLEAR MOMENTS 75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,96Kr, 78,79,80,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100Sr; analyzed rms charge radii differential changes; deduced odd-even staggering related features.
doi: 10.1209/epl/i1996-00296-0
1996PR02 Phys.Rev. C53, 1655 (1996) P.Protopapas, A.Klein, N.R.Walet Further Application of a Semimicroscopic Core-Particle Coupling Method to the Properties of 155,157Gd and 159Dy NUCLEAR STRUCTURE 157,154,156Gd, 159,158,160Dy; calculated levels, B(λ) in some cases. Generalized semi-microscopic core-particle coupling method.
doi: 10.1103/PhysRevC.53.1655
1996PR04 Phys.Rev. C54, 638 (1996) P.Protopapas, A.Klein, N.R.Walet Application of a Semimicroscopic Core-Particle Coupling Method to the Backbending in Odd Deformed Nuclei NUCLEAR STRUCTURE 180W; analyzed levels, B(E2). 164Yb; calculated levels, B(E2). 179W; calculated levels. 166Hf; calculated levels, g factors. 165Lu; calculated levels, B(M1). Semi-microscopic core-particle coupling method.
doi: 10.1103/PhysRevC.54.638
1996RA05 Phys.Rev. C53, 1005 (1996) B.A.Raue, T.A.Greco, M.G.Khayat, F.Adimi, B.van den Brandt, H.Breuer, T.Chang, N.S.Chant, H.Chen, T.A.Dooling, A.P.Dvoredsky, B.S.Flanders, T.Gu, J.P.Haas, P.Hautle, J.Huffman, J.J.Kelly, A.Klein, K.Koch, J.A.Konter, A.I.Kovalev, G.S.Kyle, J.J.Lawrie, Z.Lin, S.Mango, P.Markowitz, R.Meier, T.Payerle, S.Ritt, P.G.Roos, M.Wang Analyzing Powers for 1H(pol)(π+, π+p) at T(π) = 165 and 240 MeV NUCLEAR REACTIONS 1H(π+, π+p), E=165, 240 MeV; measured analyzing power vs θ. Polarized target.
doi: 10.1103/PhysRevC.53.1005
1996VE04 J.Phys.(London) G22, 1517 (1996) L.Vermeeren, P.Lievens, R.E.Silverans, U.Georg, M.Keim, A.Klein, R.Neugart, M.Neuroth, F.Buchinger, and the ISOLDE Collaboration The Mean Square Nuclear Charge Radius of 39Ca RADIOACTIVITY 39Ca(β+) [from Ti(p, X), E=1 GeV]; measured hfs; deduced magnetic dipole hyperfine interaction constants, isotope shift relative to 40Ca, mean square charge radius. Data on other Ca isotopes discussed.
doi: 10.1088/0954-3899/22/10/014
1995AB02 Phys.Rev.Lett. 74, 346 (1995) K.Abe, T.Akagi, P.L.Anthony, R.Antonov, R.G.Arnold, T.Averett, H.R.Band, J.M.Bauer, H.Borel, P.E.Bosted, V.Breton, J.Button-Shafer, J.P.Chen, T.E.Chupp, J.Clendenin, C.Comptour, K.P.Coulter, G.Court, D.Crabb, M.Daoudi, D.Day, F.S.Dietrich, J.Dunne, H.Dutz, R.Erbacher, J.Fellbaum, A.Feltham, H.Fonvieille, E.Frlez, D.Garvey, R.Gearhart, J.Gomez, P.Grenier, K.A.Griffioen, S.Hoibraten, E.W.Hughes, C.Hyde-Wright, J.R.Johnson, D.Kawall, A.Klein, S.E.Kuhn, M.Kuriki, R.Lindgren, T.J.Liu, R.M.Lombard-Nelsen, J.Marroncle, T.Maruyama, X.K.Maruyama, J.McCarthy, W.Meyer, Z.-E.Meziani, R.Minehart, J.Mitchell, J.Morgenstern, G.G.Petratos, R.Pitthan, D.Pocanic, C.Prescott, R.Prepost, P.Raines, B.Raue, D.Reyna, A.Rijllart, Y.Roblin, L.S.Rochester, S.E.Rock, O.A.Rondon, I.Sick, L.C.Smith, T.B.Smith, M.Spengos, F.Staley, P.Steiner, S.St.Lorant, L.M.Stuart, F.Suekane, Z.M.Szalata, H.Tang, Y.Terrien, T.Usher, D.Walz, J.L.White, K.Witte, C.C.Young, B.Youngman, H.Yuta, G.Zapalac, B.Zihlmann, D.Zimmermann, and the E143 Collaboration Precision Measurement of the Proton Spin Structure Function g1(p) NUCLEAR REACTIONS 1H(polarized e, e'), E=9.7-29.1 GeV; measured asymmetry. 1H deduced spin structure function g1(p). Polarized 15NH3 target.
doi: 10.1103/PhysRevLett.74.346
1995KE04 Nucl.Phys. A586, 219 (1995) M.Keim, E.Arnold, W.Borchers, U.Georg, A.Klein, R.Neugart, L.Vermeeren, R.E.Silverans, P.Lievens Laser-Spectroscopy Measurements of 72-96Kr Spins, Moments and Charge Radii NUCLEAR MOMENTS 78,80,82,83,84,86Kr; measured isotope shifts, hfs; deduced hyperfine constants, J, μ, electric quadrupole moments, mean square charge radii. Collinear fast beam laser spectroscopy, collisional ionization detection. RADIOACTIVITY 72,74,75,77,79Kr(EC), (β+); 81,76Kr(EC); 80m,83m,85mKr(IT); 85,87,88,89,90,91,92,93,94,95,96Kr(β-); measured isotope shifts, hfs; deduced hyperfine constants, J, μ, electric quadrupole moments, mean square charge radii. Collinear fast beam laser spectroscopy, collisional ionization detection.
doi: 10.1016/0375-9474(94)00786-M
1994AL28 Phys.Rev.Lett. 73, 1336 (1994) T.Alteholz, D.Androic, G.Backenstoss, D.Bosnar, H.Breuer, A.Brkovic, H.Dobbeling, T.Dooling, W.Fong, M.Furic, P.A.M.Gram, N.K.Gregory, J.P.Haas, A.Hoffart, C.H.Q.Ingram, A.Klein, K.Koch, J.Kohler, B.Kotlinski, M.Kroedel, G.Kyle, A.Lehmann, Z.N.Lin, G.Mahl, A.O.Mateos, K.Michaelian, S.Mukhopadhyay, T.Petkovic, R.P.Redwine, D.Rowntree, R.Schumacher, U.Sennhauser, N.Simicevic, F.D.Smit, G.van der Steenhoven, D.R.Tieger, R.Trezeciak, H.Ullrich, M.Wang, M.H.Wang, H.J.Weyer, M.Wildi, K.E.Wilson, and the LADS Collaboration Large-Solid-Angle Study of Pion Absorption on 3He NUCLEAR REACTIONS 3He(π+, X), E=118-239 MeV; measured proton energy spectra following absorption; deduced total absorption σ(E), two-, three-nucleon absorption relative contributions. Large acceptance detector system.
doi: 10.1103/PhysRevLett.73.1336
1994AR19 Z.Phys. A349, 337 (1994) E.Arnold, J.Bonn, A.Klein, P.Lievens, R.Neugart, M.Neuroth, E.W.Otten, H.Reich, W.Widdra The Quadrupole Moment of the Neutron-Halo Nucleus 11Li RADIOACTIVITY 9,11Li(β-); measured β-NMR, polarized source; deduced quadrupole moment ratio. Model comparison. In-beam laser induced nuclear polarization.
doi: 10.1007/BF01288986
1994DO01 Phys.Lett. 322B, 11 (1994) Generation of Collective Subspaces and Self-Consistent Cranking Operatrs NUCLEAR STRUCTURE 28Si; calculated cranking operator radial, spin dependences. Large amplitude collective motion.
doi: 10.1016/0370-2693(94)90483-9
1994KL01 Phys.Rev. C49, 840 (1994) Classical Mappings of the Symplectic Model and Their Application to the Theory of Large-Amplitude Collective Motion
doi: 10.1103/PhysRevC.49.840
1994KL02 Phys.Rev. C49, 1428 (1994) Quantum Theory of Large Amplitude Collective Motion: Natural fit between the Born-Oppenheimer and Kerman-Klein methods
doi: 10.1103/PhysRevC.49.1428
1994KL03 Phys.Rev. C49, 1439 (1994) Quantum Theory of Large Amplitude Collective Motion: Bosonization of all degrees of freedom
doi: 10.1103/PhysRevC.49.1439
1994PR04 Phys.Rev. C50, 245 (1994) P.Protopapas, A.Klein, N.R.Walet Calculation of the Properties of the Rotational Bands of 155,157Gd NUCLEAR STRUCTURE 155,157Gd; calculated levels, B(λ). Particle-core coupling model, Klein-Kerman approach, Donau-Frauendorf modifications.
doi: 10.1103/PhysRevC.50.245
1994YE06 Phys.Rev. C50, 897 (1994) Y.-F.Yen, B.Brinkmoller, D.Dehnhard, M.A.Franey, S.M.Sterbenz, Y.-J.Yu, B.Berman, G.R.Burleson, K.Cranston, A.Klein, G.S.Kyle, R.Alarcon, T.Averett, J.R.Comfort, J.J.Gorgen, B.G.Ritchie, J.R.Tinsley, M.Barlett, G.W.Hoffmann, K.Johnson, C.F.Moore, M.Purcell, H.Ward, A.Williams, J.A.Faucett, S.J.Greene, J.J.Jarmer, J.A.McGill, C.L.Morris, S.I.Penttila, N.Tanaka, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith, M.A.Khandaker, S.Chakravarti Pion Elastic Scattering from Polarized 13C in the Energy Region of the P33 Resonance NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=130-180 MeV; 13C(π+, π+), E=223 MeV; 13C(π-, π-), E=226 MeV; measured analyzing power A(y)(θ), σ(θ); deduced spin-flip transition quadrupole component role. Polarized, unpolarized target. DWIA calculations, optical, Δ-hole models.
doi: 10.1103/PhysRevC.50.897
1993SI20 Hyperfine Interactions 78, 247 (1993) R.E.Silverans, L.Vermeeren, A.Klein, R.Neugart, C.Schulz, P.Lievens The Electronic Field Shift Factor of the 4s2S1/2-4p2P(J) Transitions in Ca II NUCLEAR MOMENTS 40,42,43,46,48Ca; measured isotope shifts relative to 44Ca. Fast ion beam collinear laser spectroscopy. RADIOACTIVITY 45Ca(β-); measured isotope shifts relative to 44Ca. Fast ion beam collinear laser spectroscopy.
doi: 10.1007/BF00568146
1992AR07 Phys.Lett. 281B, 16 (1992) E.Arnold, J.Bonn, A.Klein, R.Neugart, M.Neuroth, E.W.Otten, P.Lievens, H.Reich, W.Widdra, and the ISOLDE Collaboration Quadrupole Moment of 11Li RADIOACTIVITY 9,11Li; measured β-asymmetry; deduced quadrupole coupling constants in LiNbO3. 9,11Li deduced quadrupole moments ratio. β-NMR spectroscopy, neutral atom fast beam optical pumping.
doi: 10.1016/0370-2693(92)90266-7
1992KL05 Int.J.Mod.Phys. E1, 95 (1992) Quantum Corrections to the Cranking Model
doi: 10.1142/S0218301392000059
1992LE16 Phys.Lett. 294B, 157 (1992) M.Leitch, H.W.Baer, A.Klein, C.S.Mishra, Z.Weinfeld, E.Piasetzky, Y.Ezra, R.Weiss, C.Allgower, J.R.Comfort, J.Tinsley, D.H.Wright Energy Dependence of Low-Energy Pion Double-Charge-Exchange on the Calcium Isotopes NUCLEAR REACTIONS 42,44,48Ca(π+, π-), E=25-65 MeV; measured σ(θ) vs E; deduced energy dependence. Model comparison.
doi: 10.1016/0370-2693(92)90676-U
1992LI29 Nucl.Instrum.Methods Phys.Res. B70, 532 (1992) P.Lievens, E.Arnold, W.Borchers, F.Buchinger, U.Georg, A.Klein, W.Neu, R.Neugart, M.Neuroth, C.Schulz, R.E.Silverans, L.Vermeeren, and the ISOLDE Collaboration Very High Sensitivity in Collinear Laser Spectroscopy: Resonance detection by particle counting techniques RADIOACTIVITY 77Sr(β+); measured hfs. Resonance detection by particle counting techniques, high sensitivity in collinear laser spectroscopy, other beams discussed, on-line separator.
doi: 10.1016/0168-583X(92)95977-Y
1992MA20 Phys.Rev. A45, 4675 (1992) A.-M.Martensson-Pendrill, A.Ynnerman, H.Warston, L.Vermeeren, R.E.Silverans, A.Klein, R.Neugart, C.Schulz, P.Lievens, and the ISOLDE Collaboration Isotope Shifts and Nuclear-Charge Radii in Singly Ionized 40-48Ca NUCLEAR MOMENTS 40,42,43,44,46,48Ca; measured isotope shifts relative to 44Ca; deduced rms charge radii difference. Fast-ion-beam collinear laser spectroscopy. Many-body perturbation theory. RADIOACTIVITY 45,47Ca; measured isotope shifts relative to 44Ca; deduced rms charge radii difference. Fast-ion-beam collinear laser spectroscopy. Many-body perturbation theory.
doi: 10.1103/PhysRevA.45.4675
1992VE02 Phys.Rev.Lett. 68, 1679 (1992) L.Vermeeren, R.E.Silverans, P.Lievens, A.Klein, R.Neugart, Ch.Schultz, F.Buchinger Ultrasensitive Radioactive Detection of Collinear-Laser Optical Pumping: Measurement of the Nuclear Charge Radius of 50Ca NUCLEAR MOMENTS 40,42,43,45,46,48Ca; measured isotope shift. 40,42,43,45,46,48,50Ca deduced rms charge radii. Other data included. Ultrasensitive detection scheme, on-line collinear-laser spectroscopy. RADIOACTIVITY 50Ca; measured isotope shift. 40,42,43,45,46,48,50Ca deduced rms charge radii. Other data included. Ultrasensitive detection scheme, on-line collinear-laser spectroscopy.
doi: 10.1103/PhysRevLett.68.1679
1992WA01 Phys.Rev. C45, 249 (1992) Quantum Corrections to the Potential Energy for Large Amplitude Collective Motion NUCLEAR STRUCTURE 28Si; calculated level energies. Large amplitude collective motion, semi-classical theory, quantum corrections.
doi: 10.1103/PhysRevC.45.249
1991GO14 Phys.Rev.Lett. 66, 2193 (1991) J.J.Gorgen, J.R.Comfort, J.R.Tinsley, T.Averett, J.DeKorse, G.Franklin, B.G.Ritchie, G.Kyle, A.Klein, B.Berman, G.Burleson, K.Cranston, J.A.Faucett, J.J.Jarmer, J.N.Knudson, S.Penttila, N.Tanaka, B.Brinkmoller, D.Dehnhard, Y.-F.Yen, S.Hoibraten, H.Breuer, B.S.Flanders, M.A.Khandaker, D.L.Naples, D.Zhang, M.L.Barlett, G.W.Hoffmann, M.Purcell Analyzing Powers for Pion Charge Exchange on Polarized 13C NUCLEAR REACTIONS 13C(π+, π0), E=163 MeV; measured σ(θ), analyzing power vs θ. Polarized target.
doi: 10.1103/PhysRevLett.66.2193
1991VE02 Nucl.Phys. A533, 505 (1991) D.Vetterli, W.Boeglin, P.Egelhof, R.Henneck, M.Jaskola, A.Klein, H.Muhry, I.Sick, D.Trautmann, G.Baur Effects of Vacuum Polarization on Sub-Coulomb 12C-12C Scattering (I) NUCLEAR REACTIONS 12C(12C, 12C), E=4 MeV; measured relative σ(θ); deduced vacuum polarization. High precision.
doi: 10.1016/0375-9474(91)90530-J
1991WA10 Phys.Rev. C43, 2254 (1991) Theory of Large-Amplitude Collective Motion Applied to the Structure of 28Si NUCLEAR STRUCTURE 28Si; calculated levels, nuclear shape. Large amplitude collective motion, adiabatic limit.
doi: 10.1103/PhysRevC.43.2254
1991YE01 Phys.Rev.Lett. 66, 1959 (1991) Y.-F.Yen, B.Brinkmoller, D.Dehnhard, S.M.Sterbenz, Y.-J.Yu, B.Berman, G.R.Burleson, K.Cranston, A.Klein, G.S.Kyle, R.Alarcon, T.Averett, J.R.Comfort, J.J.Gorgen, B.G.Ritchie, J.R.Tinsley, M.Barlett, G.W.Hoffmann, K.Johnson, C.F.Moore, M.Purcell, H.Ward, A.Williams, J.A.Faucett, S.J.Greene, J.J.Jarmer, J.A.McGill, C.L.Morris, S.Penttila, N.Tanaka, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith, M.A.Khandaker, S.Chakravarti Asymmetry Measurement of Pion Elastic Scattering from Polarized 13C in the Energy Region of the P33 Resonance NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=132-226 MeV; measured analyzing power vs θ. Polarized target.
doi: 10.1103/PhysRevLett.66.1959
1990GO36 J.Phys.(Paris), Colloq.C-6, 583 (1990) J.Gorgen, J.Comfort, T.Averett, J.DeKorse, G.Franklin, B.Ritchie, J.Tinsley, G.Kyle, B.Berman, G.R.Burleson, K.Cranston, A.Klein, J.A.Faucett, J.Jarmer, J.N.Knudson, S.Penttila, N.Tanaka, B.Brinkmoller, D.Dehnhard, Y.F.Yen, H.Breuer, M.A.Khandaker, D.L.Naples, B.S.Flanders, D.Zhang, M.Barlett, G.W.Hoffmann, M.Purcell, S.Hoibraten Analyzing Power Measurements for the (π+, π0) Reaction on a Polarized 13C Target at T(π+) = 163 MeV NUCLEAR REACTIONS 13C(π+, π0), E=163 MeV; measured σ(θ), analyzing power vs θ. Polarized target. DWIA analyses.
1990YE06 J.Phys.(Paris), Colloq.C-6, 587 (1990) Y.-F.Yen, B.Brinkmoller, D.Dehnhard, S.M.Sterbenz, Y.-J.Yu, B.Berman, G.R.Burleson, K.Cranston, A.Klein, G.S.Kyle, R.Alarcon, T.Averett, J.R.Comfort, J.Gorgen, B.Ritchie, J.R.Tinsley, G.W.Hoffmann, K.Johnson, C.F.Moore, M.Purcell, H.Ward, A.Williams, J.A.Faucett, S.J.Greene, J.Jarmer, J.A.McGill, C.L.Morris, S.Penttila, N.Tanaka, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith, S.Hoibraten, M.Khandaker, S.Chakravarti Pion Elastic Scattering from Polarized 13C in the Energy Region of the [3, 3] Resonance NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=114-226 MeV; measured analyzing power vs θ. Polarized target. DWIA analyses.
1989BR17 Phys.Rev. C40, R475 (1989) F.P.Brady, T.D.Ford, J.L.Romero, C.M.Castaneda, J.R.Drummond, E.L.Hjort, N.S.P.King, B.McEachern, D.S.Sorenson, Z.Aung, A.Klein, W.G.Love, J.K.Wambach Gamow-Teller and Spin-Dipole Strength in 90Zr(n, p) at 65 MeV NUCLEAR REACTIONS 90Zr(n, p), E=65 MeV; measured σ(θp, Ep). 90Y deduced Gamow-Teller, spin dipole transition strength.
doi: 10.1103/PhysRevC.40.R475
1989VE03 Phys.Rev.Lett. 62, 1453 (1989) D.Vetterli, W.Boeglin, P.Egelhof, R.Henneck, M.Jaskola, A.Klein, H.Muhry, G.R.Plattner, I.Sick, D.Trautmann, G.Baur, A.Weller Effects of Vacuum Polarization in Hadron-Hadron Scattering NUCLEAR REACTIONS 12C(12C, 12C), E=4 MeV; measured σ(θ), Mott scattering; deduced Coulomb interaction related vaccum polarization.
doi: 10.1103/PhysRevLett.62.1453
1988BA07 Helv.Phys.Acta 61, 219 (1988) G.Baur, W.Boeglin, P.Egelhof, R.Henneck, M.Jaskola, A.Klein, H.Muhry, G.R.Plattner, I.Sick, D.Trautmann, D.Vetterli Effects of the Vacuum Polarization on Coulomb 12C - 12C-Scattering NUCLEAR REACTIONS 12C(12C, 12C), E=4 MeV; measured σ(θ); deduced Coulomb scattering vacuum polarization role.
1988LE15 J.Phys.(Paris) 49, 885 (1988) S.Le Boiteux, A.Klein, J.R.Rios Leite, M.Ducloy Doppler - Free Spectroscopy and Isotopic Shift of the Mg I Resonance Line at 285 nm NUCLEAR MOMENTS 24,25,26Mg; measured isotope shifts. Doppler free saturated absorption spectroscopy.
doi: 10.1051/jphys:01988004906088500
1987FO10 Phys.Lett. 195B, 311 (1987) T.D.Ford, J.L.Romero, F.P.Brady, C.M.Castaneda, J.R.Drummond, B.McEachern, D.S.Sorenson, Zin Aung, N.S.P.King, A.Klein, W.G.Love Excitation of Isovector Monopole and Quadrupole Giant Resonances in 90Zr(n, p) at 65 MeV NUCLEAR REACTIONS 90Zr(n, p), E=65 MeV; measured σ(E(p), θ(p)), σ(θ(p)). 90Y deduced isovector monopole, quadrupole giant resonances. RPA-DWA analyses.
doi: 10.1016/0370-2693(87)90023-2
1987KL03 Phys.Lett. 187B, 253 (1987) A.Klein, C.Gysin, R.Henneck, J.Jourdan, M.Pickar, G.R.Plattner, I.Sick, J.P.Egger π-Nucleus Quasi-Free Scattering and Multistep Processes NUCLEAR REACTIONS 3He(π+, π+'), (π+, π+'p), E=170-320 MeV; measured inclusive σ(Eπ', θπ'), πp-coin; deduced pion multi-step processes. Enriched liquid target.
doi: 10.1016/0370-2693(87)91091-4
1987KL06 Nucl.Phys. A472, 605 (1987) A.Klein, C.Gysin, R.Henneck, J.Jourdan, M.Pickar, G.R.Plattner, I.Sick, J.P.Egger Quasi-Elastic Pion Scattering on Helium-3 NUCLEAR REACTIONS 3He(π+, π+'), (π-, π-'), (π+, π+'p), (π-, π-'p), E=170, 220, 270, 320 MeV; measured inclusive σ(θ(π), E(π)), σ(θ(π), θ(p)) vs proton momentum. DWIA calculation.
doi: 10.1016/0375-9474(87)90048-0
1986AU03 Nucl.Phys. A452, 398 (1986) A Microscopic Phenomenological Approach to the Spreading Widths of Giant Resonances NUCLEAR STRUCTURE 208Pb; calculated isoscalar, isovector dipole, monopole, quadrupole strengths, giant resonance spreading width. Hartree-Fock RPA, extended response functions.
doi: 10.1016/0375-9474(86)90205-8
1986JO05 Helv.Phys.Acta 59, 185 (1986) J.Jourdan, M.Baumgartner, S.Burzynski, P.Egelhof, A.Klein, M.A.Pickar, G.R.Plattner, W.D.Ramsay, H.W.Roser, I.Sick, J.Torre P-D(pol) Radiative Capture and the 3He D-State NUCLEAR REACTIONS 1H(polarized d, γ), E=29.2, 45.3 MeV; measured tensor analyzing power vs θ; deduced reaction mechanism. 3He deduced E1 contribution, D-state component. Faddeev calculations.
1986JO06 Nucl.Phys. A453, 220 (1986) J.Jourdan, M.Baumgartner, S.Burzynski, P.Egelhof, R.Henneck, A.Klein, M.A.Pickar, G.R.Plattner, W.D.Ramsay, H.W.Roser, I.Sick, J.Torre p-d(pol) Radiative Capture and the 3He D-State NUCLEAR REACTIONS 1H(polarized d, γ), E=29.2, 45.3 MeV; measured tensor analyzing power A(θ=90°).
doi: 10.1016/0375-9474(86)90011-4
1986KL01 Phys.Rev.Lett. 56, 700 (1986) Antinucleon Charge-Exchange Reaction as a Probe of Longitudinal Spin Excitations NUCLEAR REACTIONS 90Zr(p-bar, n-bar), E=175 MeV; calculated σ; deduced longitudinal spin excitation probe selectivity. 90Zr(p-bar, p-bar'), E=175 MeV; calculated longitudinal, isovector transition potentials.
doi: 10.1103/PhysRevLett.56.700
1986KL02 Phys.Rev. C33, 1920 (1986) Polarization Transfer and Spin-Parity Composition of the Charge-Exchange Continuum NUCLEAR REACTIONS 90Zr(polarized p, n), E=120, 160, 500 MeV; 48,40Ca(polarized p, n), E=135 MeV; calculated transverse polarization coefficient, spin-flip σ(θ=0°); deduced natural parity spin-flip strength.
doi: 10.1103/PhysRevC.33.1920
1985AU01 Phys.Rev. C51, 682 (1985) N.Auerbach, A.Klein, E.R.Siciliano Isospin Composition of Giant Resonances and Asymmetries in π+ Compared to π- Inelastic Scattering NUCLEAR REACTIONS 40,48Ca, 90Zr, 120Sn, 208Pb(π+, π+'), (π-, π-'), E not given; calculated σ(θ), ratios. Microscopic model. NUCLEAR STRUCTURE 40,48Ca, 90Zr, 120Sn, 208Pb; calculated GQR, total strengths. 120Sn; calculated T=0, GQR transition densities. RPA, isoscalar, isovector modes.
doi: 10.1103/PhysRevC.51.682
1985JO05 Phys.Lett. 162B, 269 (1985) J.Jourdan, M.Baumgartner, S.Burzynski, P.Egelhof, A.Klein, M.A.Pickar, G.R.Plattner, W.D.Ramsay, H.W.Roser, I.Sick, J.Torre 1H + 2H(pol) Radiative Capture and the 3He D-State NUCLEAR REACTIONS 1H(polarized d, γ), E=29.2, 45.3 MeV; measured tensor analyzing power for θ=96°; deduced 3He D-state role. Faddeev calculations.
doi: 10.1016/0370-2693(85)90920-7
1985KL01 Phys.Rev. C31, 710 (1985) Continuum Charge-Exchange Spectra and the Quenching of Gamow-Teller Strength NUCLEAR REACTIONS 90Zr(p, n), E=200 MeV; calculated σ(θ, En), θ<10°. 90Nb deduced Gamow-Teller transition strength characteristics. Charge exchange, Hartree-Fock RPA, Skyrme interaction.
doi: 10.1103/PhysRevC.31.710
1985KL07 Phys.Rev. C32, 1998 (1985) A.Klein, E.R.Siciliano, N.Auerbach Continuum Spectra for 165 MeV Pion-Nucleus Single Charge Exchange NUCLEAR REACTIONS 40Ca, 90Zr, 120Sn(π+, π0), (π-, π0), E=165 MeV; calculated σ(θ, E(π)); deduced giant isovector resonances role. Single scattering approximation.
doi: 10.1103/PhysRevC.32.1998
1984AU02 Phys.Rev. C29, 526 (1984) N.Auerbach, M.B.Johnson, A.Klein, E.R.Siciliano Nuclear Structure Effects in Pion Single Charge Exchange NUCLEAR REACTIONS 90Zr, 120Sn, 208Pb(π-, π0), (π+, π0), E=100-300 MeV; calculated IAR, isovector monopole resonance transition densities; deduced structure effects role. DWIA model.
doi: 10.1103/PhysRevC.29.526
1984AU07 Nucl.Phys. A422, 480 (1984) A Microscopic Theory of Muon Capture in Nuclei NUCLEAR STRUCTURE 40,48Ca, 60Ni, 90Zr, 140Ce, 208Pb; calculated binding energies, muon capture rates. Microscopic model.
doi: 10.1016/0375-9474(84)90360-9
1984AU08 Nucl.Phys. A422, 501 (1984) Excitation of Giant Resonances in the Ca Isotopes in (π±, π0) Reactions NUCLEAR REACTIONS 40,42,44,46,48Ca(π+, π0), (π-, π0), E=165 MeV; calculated σ(θ) for isovector monopole, GDR excitations. Microscopic charge exchange RPA, sum rule transition densities. NUCLEAR STRUCTURE 40,42,44,46,48Ca; calculated radial moments, transition densities, isovector monopole, GDR. Microscopic RPA, sum rule approach.
doi: 10.1016/0375-9474(84)90361-0
1984AU11 Phys.Rev. C30, 1032 (1984) Structure of Isovector Spin Excitations in Nuclei NUCLEAR STRUCTURE 60,62,64Ni; calculated isovector spin excitations. 90,92,94,96Zr; calculated M1, Gamow-Teller excitation energies. 90Zr, 208Pb; calculated spin isovector monople, strength distribution, transition density, charge exchange nonenergy weighted sum rule. 60Ni; calculated spin isovector monopole, charge exchange nonenergy weighted sum rule. Hartree-Fock, charge exchange, RPA.
doi: 10.1103/PhysRevC.30.1032
1984BO01 At.Data Nucl.Data Tables 30, 27 (1984) Energies of Ground-State Bands of Even Nuclei from Generalized Variable Moment of Inertia Models NUCLEAR STRUCTURE A=78-256; analyzed ground state band levels; deduced best fit parameters. Generalized variable moment of inertia models.
doi: 10.1016/0092-640X(84)90007-X
1984BO16 Phys.Rev. C29, 1879 (1984) Generalized Phenomenological Models of the Yrast Band NUCLEAR STRUCTURE 122,124,126,130,132,144,146Ba, 156,158,160,162,164,166,168,170Er, 152,154,156,158,160Gd, 158,160,162,164,166,168,170,172,174Yb, 172,174,176,178,180,182,184,186,188,190,192Os, 172,174,176,178,180,182,184,186,188W, 118,120,122,124,126,128Xe; analyzed yrast band systematics; deduced model parameter dependences. Generalized phenomenological models.
doi: 10.1103/PhysRevC.29.1879
1983AU01 Nucl.Phys. A395, 77 (1983) A Microscopic Theory of Giant Electric Isovector Resonances NUCLEAR STRUCTURE 48Ca, 90Zr, 120Sn, 208Pb; calculated levels, dipole, quadrupole isospin components, charge exchange analog strength distributions. Self-consistent Hartree-Fock, RPA.
doi: 10.1016/0375-9474(83)90090-8
1983AU03 Phys.Rev. C27, 1818 (1983) Transition Densities for Charge-Exchange Components of Giant Isovector Resonances and the Proton-Neutron Density Distributions in Nuclei NUCLEAR REACTIONS 40Ca(π+, π0), (π-, π0), E not given; calculated σ for giant resonances excitation. RPA transition densities. NUCLEAR STRUCTURE 40Ca; calculated isovector giant resonances, strengths, charge exchange component transition densities. RPA, sum rules.
doi: 10.1103/PhysRevC.27.1818
1983AU07 Phys.Rev. C28, 2075 (1983) Excitation of Giant Electric Isovector Resonances in Pion Charge Exchange Reactions NUCLEAR STRUCTURE 40,48Ca, 60Ni, 90Zr, 120Sn, 140Ce, 208Pb; calculated proton, neutron charge rms radii, charge exchange dipole, monopole, quadrupole energies, total transition strength distribution, transition densities. Hartree-Fock, RPA approximations, sum rule method. NUCLEAR REACTIONS 40,48Ca, 60Ni, 90Zr, 120Sn, 140Ce, 208Pb(π-, π0), (π+, π0), E not given; calculated isovector monopole, dipole, quadrupole excitation σ(θ), σ(θ, E(π0)) vs excitation energy. DWIA, RPA, sum rule method transition densities.
doi: 10.1103/PhysRevC.28.2075
1982AU06 Phys.Lett. 114B, 95 (1982) Calculation of Inclusive μ--Capture Rates in Heavy Nuclei ATOMIC PHYSICS, Mesic-Atoms 48Ca, 60Ni, 90Zr, 140Ce, 208Pb; calculated 1s μ- orbit binding energy. Dirac equation, Hartree-Fock charge density, Skyrme interaction. NUCLEAR STRUCTURE 48Ca, 60Ni, 90Zr, 140Ce, 208Pb; calculated muon capture rates. Self-consistent RPA.
doi: 10.1016/0370-2693(82)90122-8
1982AU09 Phys.Lett. 118B, 256 (1982) RPA Calculations of Isovector Spin-Flip Excitations NUCLEAR STRUCTURE 60Ni, 90Zr, 208Pb; calculated Gamow-Teller, M1 resonances, transition strengths, isovector spin-flip excitations. RPA, TDA formalisms, continuum effects.
doi: 10.1016/0370-2693(82)90179-4
1981AU08 Phys.Lett. 106B, 347 (1981) N.Auerbach, A.Klein, Nguyen Van Giai The Giant Dipole Resonance and Its Charge-Exchange Analogs NUCLEAR STRUCTURE 48Ca, 90Zr; calculated GDR, analog energies, isospin dependent dipole strength distributions.
doi: 10.1016/0370-2693(81)90639-0
1980KL02 Phys.Lett. 93B, 1 (1980) Relation of Variable Moment of Inertia (VMI) Concept with the Interacting Boson Model NUCLEAR STRUCTURE 98,100,102Pd; calculated yrast levels; deduced connection between variable moment of inertia, interacting boson models.
doi: 10.1016/0370-2693(80)90082-9
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