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Titlebook: Coherence in Atomic Collision Physics; For Hans Kleinpoppen H. J. Beyer,K. Blum,R. Hippler Book 1988 Springer Science+Business Media New Yo

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Electron Scattering from Chiral Molecules,) molecules usually exist in two forms, the .- and .-forms, which are mirror images of each other. In living organisms only one of the two alternative enantiomers is found. Apart from a few exceptions, the amino acids occurring in natural proteins belong to the .-species and sugars to the .-species.
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Electron Scattering from Heavy Atoms,ctions now be measured, but the use of high-resolution polarized electron and atom beams enables observables such as the spin polarization, asymmetry functions, and Stokes’ parameters to be determined. Reviews of these developments have been given by Blum and Kleinpoppen,. Hanne,. Slevin,. and Kessl
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Spin Polarization in Electron-Atom Scattering,oss-section measurements. This effort is part of a broad study of coherence in atomic collision physics that has been reviewed by a number of authors in a volume edited by Kleinpoppen and Williams.. The present chapter is part of a review of the progress made since then. Studies of coherence and pol
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Electron Scattering from Chiral Molecules,) molecules usually exist in two forms, the .- and .-forms, which are mirror images of each other. In living organisms only one of the two alternative enantiomers is found. Apart from a few exceptions, the amino acids occurring in natural proteins belong to the .-species and sugars to the .-species.
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Applications of Lasers in Atomic Collision Physics,hniques have now been applied to the study of superelastic scattering and stepwise excitation processes, free-free transitions, photon recoil processes, Rydberg atom collisions, and spin-polarization effects. This chapter is restricted to consideration of two of these applications, namely, stepwise
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Excitation and Ionization in Atomic Collisions, superelastic, and radiative.. In elastic collisions no energy transfer takes place between the kinetic energy of the projectile and the internal energy of either target or projectile. In contrast, in inelastic collisions the projectile transfers part of its kinetic energy into internal energy of on
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