The (c) over tilde state of CH2 is found to be bent at the highest lev
els of theory used in this work, but the energy difference between the
linear and bent geometries is only about 10 cm(-1). Improving the bas
is set or correlation treatment favors the linear geometry over the be
nt, thus it is impossible to definitively determine if the (c) over ti
lde state has a barrier in its bending potential. If there is a barrie
r, it is clear that it will be so small that the (c) over tilde state
will be quasilinear.