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Collisional alignment and orientation of atomic outer shells. III. Spin-resolved excitation
Institution:1. Department of Chemical Engineering, Konkuk University, Seoul, 05029, Republic of Korea;2. Department of Applied Physics, Delhi Technological University, Bawana Road, New Delhi, 110 042, India;3. Department of Physics, Koneru Lakshmaiah Educational Foundation, Hyderabad, 500043, Telangana, India;1. Institute of Physics, Johannes Gutenberg University, Staudingerweg 7, 55128 Mainz, Germany;2. Jülich Centre for Neutron Science, Forschungszentrum Jülich GmbH, Outstation at MLZ, Lichtenbergstrasse 1, 85747 Garching, Germany;1. Accelerator Science and Technology Centre, ASTeC, STFC Daresbury Laboratory, Warrington WA4 4AD, UK;2. Aix Marseille Universite, IUSTI, UMR 7343 CNRS, Polytech Marseille, France;3. Budker Institute of Nuclear Physics SB RAS, 630090 Novosibirsk, Russia;4. CERN, Geneva, Switzerland;5. Cockcroft Institute, Warrington WA4 4AD, UK;6. Czech Technical University, Zikova 1903/4, 166 36 Praha 6, Czech Republic;7. DESY, Notkestrasse 85, 22607 Hamburg, Germany;8. Fermilab, Batavia, IL 60510, USA;9. Heinrich-Heine-University of Düsseldorf, Moorenstrae 5, 40225 Düsseldorf, Germany;10. GoLP/Instituto de Plasmas e Fusão Nuclear, Instituto Superior Técnico, Universidade de Lisboa, Lisbon, Portugal;11. Blackett Laboratory, Imperial College London, London SW7 2BW, UK;12. John Adams Institute for Accelerator Science, Oxford, UK;13. Karlsruhe Institute of Technology, Germany;14. Lancaster University, Lancaster LA1 4YR, UK;15. Los Alamos National Laboratory, New Mexico, USA;p. Ludwig-Maximilians-Universität, 80539 Munich, Germany;q. Max Planck Institute for Nuclear Physics, Saupfercheckweg 1, Heidelberg 69117, Germany;r. Max Planck Institute for Physics, Föhringer Ring 6, 80805 München, Germany;s. Max Planck Institute for Plasma Physics, Wendelsteinstr. 1, 17491 Greifswald, Germany;t. Northern Illinois University, 1425 W Lincoln Hwy, DeKalb, IL 60115, USA;u. Novosibirsk State University, 630090 Novosibirsk, Russia;v. PSI, 5232 Villigen, Switzerland;w. Shanghai Jiao Tong University, Shanghai 200240, China;x. SLAC National Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025-7015, USA;y. STFC Rutherford Appleton Laboratory, Didcot OX11 0QX, UK;z. Swiss Plasma Center, EPFL, 1015 Lausanne, Switzerland;11. Technische Universität München (TUM), Arcisstrasse 21, D-80333 Munich, Germany;12. TRIUMF, 4004 Wesbrook Mall, Vancouver, BC V6T 2A3, Canada;13. Tsinghua University of Beijing, 100084, China;14. UCL, Gower Street, London WC1E 6BT, UK;15. University of Liverpool, Liverpool L69 7ZE, UK;16. University of Manchester, Manchester M13 9PL, UK;17. University of Oslo, 0316 Oslo, Norway;18. University of Oxford, Oxford OX1 2JD, UK;19. University of Strathclyde, 16 Richmond Street, Glasgow G1 1XQ, UK;110. University of Victoria, 3800 Finnerty Rd, Victoria, Canada;1. State Key Laboratory of Estuarine and Coastal Research, East China Normal University, 3663 Zhongshan North Road, Shanghai, 200062, China;2. School of Geographic and Oceanographic Sciences, Nanjing University, 163 Xianlin Ave., Nanjing, 210023, China;3. Department of Earth Sciences, Freie Universität Berlin, Malteserstr. 74-100, 12249, Berlin, Germany;4. Leibniz Laboratory for Radiometric Dating and Stable Isotope Research, Christian Albrechts Universität, Max-Eyth-Str. 11, 24118, Kiel, Germany
Abstract:The review generalizes the formalism of the first part of this series N. Andersen, J.W. Gallagher and I.V. Hertel, Phys. Rep. 165 (1988) 1–188] on electron-atom collisions to cases where the spin polarization of the electron is investigated at least once, i.e., before and/or after the collision. In addition, the target atom may be spin polarized. The preparation of initially polarized beams and/or the analysis of photon and spin polarization in the final state significantly increase the number of cases where a “perfect scattering experiment” can be performed. The connection between the scattering amplitudes and the generalized Stokes and STU parameters is analyzed. Favorable scattering geometries for perfect experiments and possibilities for consistency checks are pointed out. Recommendations are made about directions of future work.
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