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Imaging of Saddle Point Electron Emission in Slow<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="italic">p</mml:mi><mml:mo>−</mml:mo><mml:mi mathvariant="normal">H</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:math>Collisions

R. DörnerDepartment of Physics, Kansas State University, Manhattan, Kansas 66506H. KhemlicheM. H. PriorC. L. CockeDepartment of Physics, Kansas State University, Manhattan, Kansas 66506J. A. GaryUniversity of Missouri, Rolla, Missouri 65401R. E. OlsonUniversity of Missouri, Rolla, Missouri 65401V. MergelInstitut für Kernphysik, Universität Frankfurt, August Euler Strasse 6, D60486 Frankfurt, GermanyJ. UllrichGesellschaft für Schwerionen Forschung, D64291 Darmstadt, GermanyH. Schmidt‐BöckingInstitut für Kernphysik, Universität Frankfurt, August Euler Strasse 6, D60486 Frankfurt, Germany
1996lv
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Annotatsiya

The two-dimensional velocity distribution of electrons emitted in 5--15 keV $p\ensuremath{-}\mathrm{H}\mathrm{e}$ collisions has been measured for completely determined motion of the nuclei, that is, as a function of the impact parameter and in a well defined scattering plane. The electrons are emitted preferentially in the scattering plane and in the forward direction. The velocity distributions show sharp structures that vary strongly with impact parameter and projectile velocity. The results are compared to classical trajectory calculations.

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