We have re-examined the
B-N distance potential of CH
3CN-BF
3 usin
g MP2, DFT, and hi
gh-accuracymulticoefficient methods (MCG3 and MC-QCISD). In addition, we have solved a 1-D Schr&
ouml;din
ger equationfor nuclear motion alon
g the B-N stretchin
g coordinate, there
by o
btainin
g vi
brational ener
gy levels, wavefunctions, and vi
brationally avera
ged B-N distances. For the
gas-phase, MCG3//MP2/au
g-cc-pVTZ potential,we find an avera
ge B-N distance of 1.95 &Arin
g;, which is 0.13 &Arin
g; lon
ger than the correspondin
g equili
briumvalue. In turn, this provides solid evidence that the lon
g-standin
g discrepancy
between the experimental (
R(B-N) = 2.01 &Arin
g;) and theoretical (
R(B-N) = 1.8 &Arin
g; or
R(B-N) = 2.2-2.3 &Arin
g;) distances may
be
genuine, stemmin
gfrom lar
ge amplitude vi
brational motion in the B-N stretchin
g coordinate. Furthermore, we have examinedthe effects of low-dielectric media (
![](/ima<font color=)
ges/
gifchars/epsilon.
gif" BORDER=0 > = 1.1-5.0) on the structure of CH
3CN-BF
3 by calculatin
g solvationfree ener
gies (PCM/B97-2/au
g-cc-pVTZ) and addin
g them to the
gas-phase, MCG3 potential. These calculationsdemonstrate that the inner re
gion of the potential is sta
bilized to a
greater extent
by these media, andcorrespondin
gly, the equili
brium and avera
ge B-N distances decrease with increasin
g dielectric constant.We find that the crystallo
graphic structural result (
R(B-N) = 1.63 &Arin
g;) is nearly reproduced with a dielectricconstant of only 5.0, and also predict si
gnificant structural chan
ges for
![](/ima<font color=)
ges/
gifchars/epsilon.
gif" BORDER=0 > values of 1.1-1.5, consistent withresults from matrix-isolation-IR experiments.