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Fig. 4
The experimentally determined geometries of H
2
S
ClF drawn to
scale. The n-pair model of H
2
S, as discussed in the text, is shown for comparison. See
Fig. 1 for key to the colour coding of atoms
···
HCl and H
2
S
···
Fig. 5
The potential energy
V
(
φ
), expressed as a wavenumber, as a function of the angle
φ
for
a
H
2
S
ClF. These have been obtained using ab initio calculations,
by the method discussed in the text. Several vibrational energy levels associated with the
motion in
···
HCl and
b
H
2
S
···
= 0 is high in both molecules, so that in
each case the
v
=0and
v
= 1 vibrational energy levels are negligibly separated and hence
both molecules are pyramidal in the zero-point state and at equilibrium. The values of
φ
e
and the effective values
φ
are also shown. The PE barrier at
φ
φ
0
determined experimentally (see Fig. 4) are in good agreement.
SeeFig.1forkeytothecolourcodingofatoms
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