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- W2054953204 abstract "At a collision energy E=0.1 eV we see a large polarization effect ${mathit{Q}}_{mathrm{ion}}^{mathrm{*}{mathit{M}}_{mathit{j}}mathrm{*}=0,1}$/${mathit{Q}}_{mathrm{ion}}^{{mathit{M}}_{mathit{j}}mathrm{*}=3}$=2.5, decreasing to 1.4 for Eensuremath{ge}1 eV. A two-state basis is used for the autoionization width of the ensuremath{pi} and ensuremath{sigma} orientations of the (2p${)}^{mathrm{ensuremath{-}}1}$ core hole, resulting in a preference for the ensuremath{Omega}=0,1 molecular states as seen at 0.1 eV. The energy dependence is due to the decrease of ``locking'' of J to the internuclear axis with increasing angular velocity ensuremath{varphi}ifmmode dot{}else .{}fi{}, leading to the semiclassical criterion ${ensuremath{omega}}_{mathrm{prec}=4mathrm{ensuremath{varphi}}mathrm{ifmmode dot{}else .{}fi{}}}$ for the transition from a space-fixed to a body-fixed description of J." @default.
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- W2054953204 title "Polarization effects in the ionization cross section for collisions of<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant=normal>Ne</mml:mi></mml:mrow><mml:mrow><mml:mo>/</mml:mo><mml:mi mathvariant=normal>e</mml:mi><mml:mi mathvariant=normal>m</mml:mi><mml:mi mathvariant=normal>p</mml:mi><mml:mi mathvariant=normal>h</mml:mi><mml:mo>></mml:mo><mml:mn /></mml:mrow></mml:msup></mml:mrow></mml:math>{(2<i>p</i><mml…" @default.
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