Both [C4CO](-.) and [C2COC2](-.) are formed in the ion source of a VG ZAB 2
HF mass spectrometer by the respective processes HO- + Me3Si-C=C-C=C-CO-CMe
3 --> [C4CO](-.) + Me3SiOH + Me3C., and Me3Si-C=C-CO-C=C-SiMe3 + SF, + e --
> [C2COC2](-.) + 2Me(3)SiF + SF4. The second synthetic pathway involves a d
ouble desilylation reaction similar to that first reported by Squires. The
two radical anion isomers produce different and characteristic charge rever
sal spectra upon collisional activation. In contrast, following collision i
nduced charge stripping, both radical anions produce neutral C4CO as eviden
ced by the identical neutralisation reionisation (-NR+) spectra. The exclus
ive rearrangement of (C2COC2)-C-13 to (C4CO)-C-13 indicates that C-12-O bon
d formation is not involved in the reaction. Ab initio calculations (at the
RCCSD (T)/aug-cc-pVDZ//B3LYP/6-31G* level of theory) have been used to inv
estigate the reaction coordinates on the potential surfaces for both single
t and tripler rearrangements of neutral C2COC2. Singlet C2COC2 is less stab
le than singlet C4CO by 78.8 kcal mol(-1) and requires only 8.5 kcal mol(-1
) of additional energy to effect conversion to C4CO by a rearrangement sequ
ence involving three C-C ring opening/cyclisation steps. (C) 2000 Elsevier
Science B.V.