NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.Thiel Found 17 matches. 2023BA25 Phys.Lett. B 844, 138080 (2023) M.Bashkanov, D.P.Watts, S.Kay, S.Abt, P.Achenbach, P.Adlarson, F.Afzal, Z.Ahmed, C.S.Akondi, J.R.M.Annand, H.J.Arends, R.Beck, M.Biroth, N.Borisov, A.Braghieri, W.J.Briscoe, F.Cividini, C.Collicott, S.Costanza, A.Denig, E.J.Downie, P.Drexler, S.Fegan, A.Fix, S.Gardner, D.Ghosal, D.I.Glazier, I.Gorodnov, W.Gradl, M.Gunther, D.Gurevich, L.Heijkenskjold, D.Hornidge, G.M.Huber, A.Kaser, V.L.Kashevarov, M.Korolija, B.Krusche, A.Lazarev, K.Livingston, S.Lutterer, I.J.D.MacGregor, D.M.Manley, P.P.Martel, R.Miskimen, E.Mornacchi, C.Mullen, A.Neganov, A.Neiser, M.Ostrick, P.B.Otte, D.Paudyal, P.Pedroni, A.Powell, S.N.Prakhov, V.Sokhoyan, K.Spieker, O.Steffen, I.I.Strakovsky, T.Strub, I.Supek, A.Thiel, M.Thiel, A.Thomas, Yu.A.Usov, S.Wagner, J.Wettig, M.Wolfes, N.Zachariou First measurement of polarisation transfer Cnx, in deuteron photodisintegration NUCLEAR REACTIONS 2H(polarized γ, X), E=370-700 MeV; measured reaction products; deduced the polarisation transfer from a circularly-polarised photon to the final state neutron in deuterium photodisintegration. Cryogenic liquid deuterium target within the Crystal Ball detector at MAMI.
doi: 10.1016/j.physletb.2023.138080
2021KR01 Phys.Rev. C 103, 014607 (2021) P.Kroenert, Y.Wunderlich, F.Afzal, A.Thiel Minimal complete sets for two-pseudoscalar-meson photoproduction
doi: 10.1103/PhysRevC.103.014607
2021ME22 Eur.Phys.J. A 57, 325 (2021) V.Metag, M.Nanova, J.Hartmann, P.Mahlberg, F.Afzal, C.Bartels, D.Bayadilov, R.Beck, M.Becker, E.Blanke, K.-T.Brinkmann, S.Ciupka, V.Crede, M.Dieterle, H.Dutz, D.Elsner, F.Frommberger, A.Gridnev, M.Gottschall, M.Gruner, Ch.Hammann, J.Hannappel, W.Hillert, J.Hoff, Ph.Hoffmeister, Ch.Honisch, T.Jude, H.Kalinowsky, F.Kalischewski, I.Keshelashvili, B.Ketzer, P.Klassen, F.Klein, K.Koop, P.Kroenert, B.Krusche, M.Lang, I.Lopatin, F.Messi, W.Meyer, B.Mitlasoczky, J.Muller, J.Mullers, V.Nikonov, V.Novinsky, R.Novotny, D.Piontek, G.Reicherz, L.Richter, T.Rostomyan, S.Runkel, B.Salisbury, A.Sarantsev, D.Schaab, Ch.Schmidt, H.Schmieden, J.Schultes, T.Seifen, V.Sokhoyan, C.Sowa, K.Spieker, N.Stausberg, A.Thiel, U.Thoma, T.Triffterer, M.Urban, G.Urff, H.van Pee, M.Wagner, D.Walther, Ch.Wendel, D.Werthmuller, U.Wiedner, A.Wilson, A.Winnebeck, L.Witthauer, Y.Wunderlich Observation of a structure in the Mpη invariant mass distribution near 1700 MeV/c2 in the γ p -> p π0 η reaction - The CBELSA/TAPS Collaboration
doi: 10.1140/epja/s10050-021-00634-1
2020WU07 Phys.Rev. C 102, 034605 (2020) Y.Wunderlich, P.Kroenert, F.Afzal, A.Thiel Moravcsik's theorem on complete sets of polarization observables reexamined
doi: 10.1103/PhysRevC.102.034605
2019AK10 Eur.Phys.J. A 55, 202 (2019) C.S.Akondi, K.Bantawa, D.M.Manley, S.Abt, P.Achenbach, F.Afzal, P.Aguar-Bartolome, Z.Ahmed, J.R.M.Annand, H.J.Arends, M.Bashkanov, R.Beck, M.Biroth, N.Borisov, A.Braghieri, W.J.Briscoe, F.Cividini, C.Collicott, S.Costanza, A.Denig, M.Dieterle, E.J.Downie, P.Drexler, M.I.Ferretti-Bondy, S.Gardner, D.I.Glazier, I.Gorodnov, W.Gradl, M.Gunther, D.Gurevich, S.Kay, L.Heijkenskjold, D.Hornidge, G.M.Huber, M.Kaser, V.L.Kashevarov, M.Korolija, B.Krusche, A.Lazarev, K.Livingston, S.Lutterer, J.C.McGeorge, I.J.D.MacGregor, P.P.Martel, D.G.Middleton, R.Miskimen, E.Mornacchi, A.Mushkarenkov, C.Mullen, A.Neganov, A.Neiser, M.Oberle, M.Ostrick, P.B.Otte, B.Oussena, D.Paudyal, P.Pedroni, A.Powell, S.N.Prakhov, G.Ron, T.Rostomyan, A.Sarty, C.Sfienti, V.Sokhoyan, K.Spieker, O.Steffen, I.I.Strakovsky, Th.Strub, I.Supek, A.Thiel, M.Thiel, A.Thomas, M.Unverzagt, Yu.A.Usov, N.K.Walford, D.P.Watts, S.Wagner, D.Werthmuller, J.Wettig, L.Witthauer, M.Wolfes Experimental study of the γp → K0Σ+, γn → K0Λ, and γn → K0Σ0 reactions at the Mainz Microtron
doi: 10.1140/epja/i2019-12924-x
2019BA02 Phys.Lett. B 789, 7 (2019) M.Bashkanov, S.Kay, D.P.Watts, C.Mullen, S.Abt, P.Achenbach, P.Adlarson, F.Afzal, Z.Ahmed, C.S.Akondi, J.R.M.Annand, H.J.Arends, R.Beck, M.Biroth, N.Borisov, A.Braghieri, W.J.Briscoe, F.Cividini, C.Collicott, S.Costanza, A.Denig, E.J.Downie, P.Drexler, S.Garni, D.I.Glazier, I.Gorodnov, W.Gradl, M.Gunther, D.Gurevich, L.Heijkenskjold, D.Hornidge, G.M.Huber, A.Kaser, V.L.Kashevarov, M.Korolija, B.Krusche, A.Lazarev, K.Livingston, S.Lutterer, I.J.D.MacGregor, R.Macrae, D.M.Manley, P.P.Martel, R.Miskimen, E.Mornacchi, A.Neganov, A.Neiser, M.Ostrick, P.B.Otte, D.Paudyal, P.Pedroni, A.Powell, S.N.Prakhov, G.Ron, T.Rostomyan, A.Sarty, C.Sfienti, V.Sokhoyan, K.Spieker, O.Steffen, I.I.Strakovsky, T.Strub, I.Supek, A.Thiel, M.Thiel, A.Thomas, Yu.A.Usov, S.Wagner, N.K.Walford, D.Werthmuller, J.Wettig, M.Wolfes, L.A.Zana Deuteron photodisintegration by polarized photons in the region of the d*(2380) NUCLEAR REACTIONS 2H(polarized γ, np), E=420-620 MeV; measured reaction products; deduced beam-spin asymmetry for deuteron photodisintegration.
doi: 10.1016/j.physletb.2018.12.026
2017DI10 Phys.Lett. B 770, 523 (2017) M.Dieterle, L.Witthauer, F.Cividini, S.Abt, P.Achenbach, P.Adlarson, F.Afzal, Z.Ahmed, C.S.Akondi, J.R.M.Annand, H.J.Arends, M.Bashkanov, R.Beck, M.Biroth, N.S.Borisov, A.Braghieri, W.J.Briscoe, S.Costanza, C.Collicott, A.Denig, E.J.Downie, P.Drexler, M.I.Ferretti-Bondy, S.Gardner, S.Garni, D.I.Glazier, D.Glowa, W.Gradl, M.Gunther, G.M.Gurevich, D.Hamilton, D.Hornidge, G.M.Huber, A.Kaser, V.L.Kashevarov, S.Kay, I.Keshelashvili, R.Kondratiev, M.Korolija, B.Krusche, A.B.Lazarev, J.M.Linturi, V.Lisin, K.Livingston, S.Lutterer, I.J.D.MacGregor, J.Mancell, D.M.Manley, P.P.Martel, V.Metag, W.Meyer, R.Miskimen, E.Mornacchi, A.Mushkarenkov, A.B.Neganov, A.Neiser, M.Oberle, M.Ostrick, P.B.Otte, D.Paudyal, P.Pedroni, A.Polonski, S.N.Prakhov, A.Rajabi, G.Reicherz, G.Ron, T.Rostomyan, A.Sarty, C.Sfienti, M.H.Sikora, V.Sokhoyan, K.Spieker, O.Steffen, I.I.Strakovsky, Th.Strub, I.Supek, A.Thiel, M.Thiel, A.Thomas, M.Unverzagt, Yu.A.Usov, S.Wagner, N.K.Walford, D.P.Watts, D.Werthmuller, J.Wettig, M.Wolfes, L.Zana First measurement of the polarization observable E and helicity-dependent cross sections in single π0 photoproduction from quasi-free nucleons NUCLEAR REACTIONS 2H(γ, π0), E=400-1450 MeV; measured reaction products; deduced σ.
doi: 10.1016/j.physletb.2017.04.079
2017TH01 Eur.Phys.J. A 53, 8 (2017) A.Thiel, for the CBELSA/TAPS Collaboration Double-polarization observable G in neutral-pion photoproduction off the proton NUCLEAR REACTIONS 1H(polarized γ, π0), E=617-1325 MeV[electron end-point energy E0=3.2 GeV in bremsstrahlung γ production]; measured Eγ, Iγ(θ) (from π0 decay to 2 γ) from linearly polarized γ on logintudinally polarized protons, beam asymmetry; deduced double-polarization observable G vs Eγ and vs θ. Compared with values predicted by different models and from partial wave analysis.
doi: 10.1140/epja/i2017-12194-8
2017WU08 Eur.Phys.J. A 53, 86 (2017) Y.Wunderlich, F.Afzal, A.Thiel, R.Beck Determining the dominant partial wave contributions from angular distributions of single- and double-polarization observables in pseudoscalar meson photoproduction using PWA
doi: 10.1140/epja/i2017-12255-0
2016AN18 Eur.Phys.J. A 52, 284 (2016) A.V.Anisovich, R.Beck, M.Doring, M.Gottschall, J.Hartmann, V.Kashevarov, E.Klempt, Ulf-G.Meissner, V.Nikonov, M.Ostrick, D.Ronchen, A.Sarantsev, I.Strakovsky, A.Thiel, L.Tiator, U.Thoma, R.Workman, Y.Wunderlich The impact of new polarization data from Bonn, Mainz and Jefferson Laboratory on γp → πN multipoles NUCLEAR REACTIONS 1H(γ, π0), (γ, π+), E=147-219, 650-2200 MeV; analyzed published σ(θ), beam asymmetry, double polarization data; calculated σ(θ), beam asymmetry, double polarization using PWA (Partial-Wave Analysis) BnGa code, Juelich-Bonn DCC (Dynamical CC) model, MAID and SAID models; deduced photoproduction multipoles, partial waves real, imaginary parts, parameters.
doi: 10.1140/epja/i2016-16284-9
1991BO12 J.Phys.(London) G17, 691 (1991) C.Borchert, W.Greiner, A.Thiel, W.Scheid Inelastic Excitation and Nucleon Transfer in the Scattering of 17O on 13C NUCLEAR REACTIONS, ICPND 13C(17O, 17O), (17O, 17O'), E(cm)=18.29 MeV; analyzed σ(θ), σ(E). Coupled-channels model.
doi: 10.1088/0954-3899/17/5/015
1991TH02 Phys.Rev. C43, 1480 (1991) Reaction Calculations for 17O + 12C Including Fusion within the Molecular Particle-Core Model NUCLEAR REACTIONS, ICPND 12C(17O, 17O), (17O, 17O'), E=50 MeV; calculated σ(θ). 12C(17O, X), E(cm)=7-14 MeV; calculated fusion σ(E).
doi: 10.1103/PhysRevC.43.1480
1989TH07 J.Phys.(London) G15, 1833 (1989) A.Thiel, W.Greiner, J.Y.Park, W.Scheid Structures Due to the Nuclear Landau-Zener Effect in the 17O + 12C Scattering within Molecular Particle-Core Model NUCLEAR REACTIONS, ICPND 12C(17O, 17O), (17O, 17O'), E=50, 62 MeV; calculated σ(θ). 12C(17O, 17O'), E(cm)=8-28 MeV; calculated σ(E). Molecular particle-core model.
doi: 10.1088/0954-3899/15/12/009
1988TH02 J.Phys.(London) G14, L85 (1988) Nuclear Landau-Zener Effect in 17O + 12C Scattering within the Molecular Particle-Core Model NUCLEAR REACTIONS 12C(17O, 17O), (17O, 17O'), E(cm) ≤ 28 MeV; calculated σ(θ). 12C(17O, 17O'), E(cm) ≈ 8-20 MeV; calculated σ(E). Coupled-channels method.
doi: 10.1088/0305-4616/14/5/004
1987TH04 Phys.Rev. C36, 647 (1987) A.Thiel, W.Greiner, J.Y.Park, W.Scheid Inelastic Excitation and Neutron Transfer in the 13C - 13C Scattering with the Molecular Particle-Core Model NUCLEAR REACTIONS 13C(13C, 13C), (13C, 13C'), (13C, 12C), E(cm) ≤ 30 MeV; calculated σ(E, θ). Molecular particle-core model.
doi: 10.1103/PhysRevC.36.647
1986MA58 Nucl.Phys. A460, 324 (1986) R-Matrix Formalism with Physical Boundary Conditions for Heavy-Ion Scattering and Application to 24Mg on 24Mg NUCLEAR REACTIONS 24Mg(24Mg, 24Mg), (24Mg, 24Mg'), E(cm)=46 MeV; calculated σ(θ). R-matrix formalism.
doi: 10.1016/0375-9474(86)90129-6
1984TH02 Phys.Rev. C29, 864 (1984) Nuclear Molecular Barrier Resonances in the Scattering of 28Si on 28Si Studied by Coupled Channel Calculations NUCLEAR REACTIONS 28Si(28Si, 28Si), (28Si, 28Si'), E(cm)=40-75 MeV; analyzed σ(θ=90°, E); deduced nuclear molecular resonance evidence.
doi: 10.1103/PhysRevC.29.864
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