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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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