2005 58th Gaseous Electronics Conference
Sunday–Thursday, October 16–20, 2005;
San Jose, California
Session QW1: Electron and Positron Collisions
10:00 AM–12:00 PM,
Wednesday, October 19, 2005
Doubletree Hotel
Room: Pine
Chair: Murtadha A. Khakoo, California State University-Fullerton
Abstract ID: BAPS.2005.GEC.QW1.2
Abstract: QW1.00002 : Ionization of Simple Molecules by Ion or Electron Impact in a Reaction Microscope*
10:30 AM–11:00 AM
Preview Abstract
Abstract
Author:
Christina Dimopoulou
(Max-Planck-Institut f{\"u}r Kernphysik, Heidelberg, Germany)
We have studied single ionization of simple molecules by fast
charged
particle impact in a reaction microscope. By measuring the
momenta of the
emitted electron and the recoil ionic fragment in coincidence,
channel-selective low-energy electron spectra have been recorded.
For
non-dissociative ionization of H$_{2}$ by 6 MeV protons, the
electron energy
distribution agrees well with a CDW-EIS prediction [1] except for
E$_{e}$
$<$ 1 eV where an significant enhancement is observed. It is due
to the
autoionization of rovibrational levels of Rydberg states of
H$_{2}$, which
occurs by converting vibrational energy into kinetic energy of
the emitted
electron. First fully differential cross sections have been
obtained bearing
the ``signature'' of this molecular mechanism, which lies beyond the
Born-Oppenheimer approximation [2]. \newline
Recently, considerable interest has been raised by the
observation of
two-center interference effects in the electron emission from
H$_{2}$, in
analogy to Young's double-slit experiment [3]. They are predicted
to be more
pronounced if one could fix the orientation of the molecular axis
at the
instant of the collision [4]. For dissociative ionization of
H$_{2}$ by 6
MeV protons we had access to this information. Molecular-frame
angular
distributions of the emitted electrons have been compared to the
CDW-EIS
calculation [5]. \newline
Argon dimers as well as atomic Ar, both present in the same
gas-jet, are
ionized by 1keV electron impact in a kinematically complete
experiment
carried out in an upgraded reaction microscope. The obtained
electron
spectra for Ar$_{2}$ and Ar are compared directly in order to
identify
interference structures, which are expected to be much more
visible than for
H$_{2}$ since the interatomic distance of Ar$_{2}$ is comparable
to the de
Broglie wavelength of the emitted electron.
\newline
\newline
[1] M.E. Galassi \textit{et al.,} Phys. Rev. A \textbf{66},
052705 (2002)\newline
[2] C. Dimopoulou \textit{et al.,} Phys. Rev. Lett. \textbf{93},
123203 (2004)\newline
[3] N. Stoltherfoht \textit{et al}., Phys. Rev. Lett.
\textbf{87}, 023201 (2001)\newline
[4] G. Laurent \textit{et al.}, J. Phys. B \textbf{35}, L495
(2002)\newline
[5] C. Dimopoulou \textit{et al.,} J. Phys. B \textbf{38}, 593 (2005)
*Coauthors: R. Moshammer, A. Dorn, D. Fischer, P.D. Fainstein, M. D{\"u}rr, C. H{\"o}hr and J. Ullrich
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2005.GEC.QW1.2