EGAS41 - Swansea University
EGAS41 - Swansea University
EGAS41 - Swansea University
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41 st EGAS CP 66 Gdańsk 2009<br />
Electron collisions with cyclopropane<br />
M. Allan<br />
Department of Chemistry, <strong>University</strong> of Fribourg, chemin du Musée 9, 1700 Fribourg,<br />
Switzerland<br />
E-mail: michael.allan@unifr.ch,<br />
Electron interactions with alkyl groups are important for a number of applications. The<br />
cross sections of the prototype compounds, the alkanes, do not show pronounced resonant<br />
structure, however, only extremely broad humps covering the 2-15 eV region [1]. This is<br />
somewhat surprising, alkanes have many empty orbitals, which could give rise to shape<br />
resonances.<br />
In cyclopropane, however, the high symmetry has the consequence that one virtual<br />
orbital couples only to f-wave and not to lower l waves, thus retarding the ‘leaking out’<br />
of the electron through the centrifugal barrier in the corresponding a ′ 2 shape resonance<br />
at 5.5 eV [1]. As a consequence, this resonance is exceptionally narrow for a shape<br />
resonance in a saturated hydrocarbon (Fig. 1), an effect which could be called ‘symmetryinduced<br />
narrowing’. The present work characterizes this resonance and generally electron<br />
collisions with cyclopropane by measuring the absolute differential cross sections for elastic<br />
scattering and for vibrational excitation. Since the resonance is, in chemical terms, due to<br />
a temporary capture of the incoming electron in a C-C antibonding σ ∗ orbital, it excites<br />
primarily the symmetric ring breathing vibration ν 3 . A representative cross section, drawn<br />
as a function of energy and of scattering angle, is shown in Fig. 1. The calculation of<br />
Čurík and Gianturco [2] are in good agreement with the present measurement.<br />
Cross Section (pm /sr)<br />
2<br />
400<br />
300<br />
200<br />
100<br />
0<br />
5.5 eV<br />
= 180°<br />
2 3<br />
0 5 10 15 20<br />
Electron Energy (eV)<br />
400<br />
300<br />
200<br />
100<br />
0<br />
E i = 5.5 eV<br />
f-wave<br />
2 3<br />
÷2<br />
0 30 60 90 120 150 180<br />
Scattering Angle (deg)<br />
Figure 1: Cross section for exciting the first overtone of the ν 3 symmetric ring breathing vibration,<br />
shown as a function of the incident electron energy (left) and of scattering angle at the<br />
5.5 eV resonance (right).<br />
References<br />
[1] M. Allan, L. Andrić, J. Chem. Phys. 105, 3559 (1996)<br />
[2] R. Čurík, F.A. Gianturco, J. Phys. B: At. Mol. Opt. Phys. 35, 717 and 1235 (2002)<br />
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