Recently, room-temperature crystal structures of SO
2F
- in its K
+ and Rb
+ salts were published in
Z. Anorg. Allg.Chem. 1999,
625, 385 and claimed to represent the first reliable
geometries for SO
2F
-. However, their almostidentical S-O and S-F bond len
gths and O-S-O and O-S-F bond an
gles are in sharp contrast to the resultsfrom theoretical calculations. To clarify this discrepancy, the new [(CH
3)
2N]
3SO
+ and the known [N(CH
3)
4+],[(CH
3)
2N]
3S
+, and K
+ salts of SO
2F
- were prepared and their crystal structures studied at low temperatures.Furthermore, the results from previous RHF and MP2 calculations were confirmed at the RHF, B3LYP, andCCSD(T) levels of theory usin
g different basis sets. It is shown that all the SO
2F
- salts studied so far exhibitvaryin
g de
grees of oxy
gen/fluorine and, in some cases, oxy
gen-site disorders, with [(CH
3)
2N]
3SO
+SO
2F
- at 113K showin
g the least disorder with
r(S-F) -
r(S-O) = 17 pm and
ges/entities/an
g.
gif">(O-S-O) -
ges/entities/an
g.
gif">(F-S-O) = 6
ges/entities/de
g.
gif">. Refinementof the disorder occupancy factors and extrapolation of the observed bond distances for zero disorder resulted ina
geometry very close to that predicted by theory. The correctness of the theoretical predictions for SO
2F
- isfurther supported by the
good a
greement between the calculated and the experimentally observed vibrationalfrequencies and their comparison with those of isoelectronic ClO
2F. A normal coordinate analysis of SO
2F
-confirms the weakness of the S-F bond with a stretchin
g force constant of only 1.63 mdyn/&Arin
g; and shows thatthere is no hi
ghly characteristic S-F stretchin
g mode. The S-F stretch stron
gly couples with the SO
2 deformationmodes and is concentrated in the two lowest a' frequencies.