The co
mpounds (
tBuCO
2)
3M
2(
mages/entities/
mgr.gif">-O
2CCO
2)M
2(O
2C
tBu)
3 (M
4OXA), where M = Mo or W, are shownby analysis of powder X-ray diffraction data to have extended lattice structures wherein oxygen ato
msfro
m the oxalate
and pivalate lig
ands of one M
4OXA
molecule are linked to
metal ato
ms of neighboring
molecules. Ra
man, resonance Ra
man, electronic absorption (2-325 K in 2-MeTHF),
and e
mission spectraare reported, together with corresponding spectra of the
mages/entities/
mgr.gif">-O
213C
13CO
2 isotopo
mers. To aid in the assign
ment,the Ra
man spectra of K
2C
2O
4·H
2O
and K
213C
2O
4·H
2O have also been recorded. The visible region of theelectronic spectra is do
minated by intense, fully allowed MLCT transitions, M
2 mages/gifchars/delta.gif" BORDER=0 > to oxalate
mages/gifchars/pi.gif" BORDER=0 >*, which showpronounced ther
mochro
mis
m and extensive vibronic progressions associated with the oxalate lig
and atlow te
mperatures. With excitation into these charge-transfer b
ands, strong resonance enhance
ment is seenfor Ra
man b
ands assigned to the oxalate
mages/gifchars/nu.gif" BORDER=0 >
1(a
g)
and, to a lesser extent,
mages/gifchars/nu.gif" BORDER=0 >
2(a
g)
modes. Electronic structurecalculations for the
model co
mpounds (HCO
2)
3M
2(
mages/entities/
mgr.gif">-O
2CCO
2)M
2(O
2CH)
3, e
mploying density functional theory(gradient corrected
and ti
me-dependent) with the Gaussian 98
and ADF 2000 packages, predict the planaroxalate
D2h configuration to be favored, which
maxi
mizes M
2 mages/gifchars/delta.gif" BORDER=0 > to oxalate
mages/gifchars/pi.gif" BORDER=0 >* back-bonding,
and indicatelow barriers (<8 kcal
mol
-1) to rotation about the oxalate C-C bonds.