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3.4.4
Alkoxides of Yttrium, Lanthanides, and Actinides
3.4.4.1 Yttrium and lanthanum alkoxides
A number of yttrium and lanthanum alkoxides have been investigated by 1 Hand
13 C spectral studies 18 , 21 by the research groups of Evans 160 , 161 , 164 , 346 , 552 and Bradley
et al . 345 , 349 - 349c in an attempt to provide preliminary evidence for the structures of
these derivatives. Although the spectral patterns are generally more complex, the data
are interpretable in terms of X-ray crystallographically established structures of typical
compounds of each series. For example, the 1 H NMR spectrum (in C 6 D 6 )ofY 3 ( 3 -
OBu t )( 3 -Cl)( 2 -OBu t ) 3 (OBu t ) 4 (THF) 2 exhibits several broad overlapping resonances
in the υ 1.1 - 2.1 region attributable to the t -butoxide ligands. 160 In THF-d 8 ,these
peaks split into six sharp well-resolved signals with relative intensities of 1:2:1:2:1:1.
The 13 C f 1 Hg NMRspectrumofthecomplexinTHF-d 8 also showed six chemi-
cally nonequivalent OBu t
groups, consistent with the solid-state structure 160
of the
derivative.
The 1 H NMR spectrum of La 3 (OBu t ) 9 (thf) 2 in aromatic solvents shows broad
resonances characteristic of fluxional behaviour. 160 In THF-d 8 , the resonance due
to OBu t groups sharpens. Using the structure - shift correlations developed for
Y 3 (OBu t ) 8 Cl(thf) 2 , the lanthanum complex contains two equivalent 3 -OBu t groups,
three 2 -OBu t groups in a ratio of 1:2, and four terminal OBu t groups. Even at
500 MHz, the terminal OBu t peaks are not fully resolved, so the number of distinct
environments is indeterminate. The 13 C NMR pattern is consistent with 1 H NMR data.
At room temperature, the 1 Hand 13 C NMR studies on tris- tert -alkoxides of yttrium
and lanthanum 345 reveal that the complexes are fluxional and require low temperatures
to slow down the exchange between distinguishable alkoxo ligands. Even at around
43 Ž C 1 H NMR spectra of the trinuclear complexes [M 3 (OBu t ) 9 (HOBu t ) 2 ](MD Y,
La) exhibit a complex pattern, each having five major peaks with intensities in the ratio
2:2:2:1:4, appearing from lower to higher fields. For interpretation of such complex
spectral data, the knowledge gained from the X-ray crystallographically characterized
lanthanum complex 345 proved invaluable. The 1 H NMR spectral data of these and some
alkoxide complexes of Y and La are listed in Table 2.20.
The 1 Hand 13 C NMR spectra 346 of [(Ph 3 CO) 2 La( 2 -OCPh 3 ) 2 La(OCPh 3 ) 2 ] show
two types of phenyl resonances, consistent with terminal and bridging groups in the
dimer.
3.4.4.2 Thorium and uranium alkoxides
At room temperature the 1 H NMR spectrum of [Th(OBu t ) 4 (py) 2 ] reveals that the
molecule is fluxional 406 and low-temperature (75 Ž C) spectra in toluene-d 8 failed
to freeze out a limiting structure. In benzene-d 6 the room temperature 1 HNMR
spectrum 406 of [Th 2 (OBu t ) 8 (HOBu t )] shows only one broad signal due to OBu t groups
at υ 1.54 and a broad peak at υ 3.22 for alcoholic OH protons in the intensity ratio
80:1, consistent with these assignments.
In an interesting 1 H NMR experiment the reaction of Th 2 (OBu t ) 8 (HOBu t ) with
pyridine has been studied 406
which supports the stepwise changes as illustrated in
scheme 2.4:
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