G. B. Deacon, C. C. Quitmann, K. MuÈller-Buschbaum, G. Meyer
show that the bonding of the benzoate ligands to the
metal centres is unsymmetrical *for distances and
angles between atoms, see legendto Figs. 1 and2).
The differences between corresponding angles, e. g.
C1±O1±Yb1 andC1±O2±Yb1 *10±12 °) are substantial
but less than those *14±34°) of the marginally more
crowded pentafluorobenzoate [4]. Further, this asym-
metry in coordination foreshadows the intrinsic asym-
metry of bridging tridentate coordination where the
differences between corresponding pairs of Yb±O±C
angles lie in the range of 50±70°. On both dimeric mo-
lecules, the MeCp ligands allow two equally probable
positions for the methyl groups. Not relatedto this is
a disorder of the Yb2 atoms which subsequently re-
sults in a disorder of one of the coordinated MeCp li-
gands in a ratio of one third to two thirds and an
asymmetric coordination of the non-disordered MeCp
ring to the weaker representedYb2 positions *Fig. 2).
All atoms, including the disordered ones, were refined
anisotropically [14] giving a more reasonable result of
the refinement than averagedatomic positions.
The disorder might be explained by a block structure
but not by intergrown individuals. Furthermore, no
evidence of a suitable twinning law was found nor a
possible lower symmetry. The close relation of the
Fig. 1 Dimeric molecule 1 in the structure of [Yb*MeCp)2-
*O2CC6H5)]2. The thermal ellipsoids are scaled to a proba-
bilty density of 50%. The methyl groups C8 and C14 are dis-
ordered in a 1 : 1 ratio. Selected distances/pm and angles/°:
present compoundto YbCp *O2CC6H5) [8] suggests a
2
similar dimeric structure for the latter.
Yb1±O1 218.5*4), Yb1±O2 215.6*4), Yb1±C9 262.3*6), Yb1±C10 259.2*6),
Yb1±C11 255.1*7), Yb1±C15 259.6*7), Yb1±C16 255.8*7), Yb1±C19
262.1*6), C1±O1 125.6*6), C1±O2 121.7*6); Yb1±O1±C1 151.6*4),
Yb1±O2±C1 162.2*4), O1±Yb1±*centroidC9±C13) 105.3*6), O2±Yb1±
*C9±C13) 107.7*6), *C9±C13)±Yb1±*centroidC15±C19) 130.4*6),
O1±Yb1±*C15±C19) 107.1*6), O2±Yb1±*C15±C19) 105.3*6).
This work was supportedby the Australian Research Coun-
cil, the Deutsche Forschungsgemeinschaft, andthe Studien-
stiftung des Deutschen Volkes.
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Newnham, G. N. Pain, T. D. Tuong, D. L. Wilkinson,
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State Inorg. Chem. 1996, 32, 121.
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1990, 29, 4356
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845.
[9] E. C. Baker, Diss. Abstr. B. 1978, 730; E. C. Baker, Ph D
Thesis, University of California, 1977.
[10] G. M. Sheldrick, SHELXS-86, Program for the solution
of crystal structures, GoÈttingen 1986.
[11] G. M. Sheldrick, SHELXL-97, Program for the refine-
ment of crystal structures, GoÈttingen 1997.
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[14] Further information about the crystal structure deter-
mination is deposited at the Cambridge data base and
can be requestedby giving the author names andthe
deposition number CCDC-160132.
Fig. 2 Dimeric molecule 2 in the structure of [Yb*MeCp)2-
*O2CC6H5)]2. The Yb2 atoms as well as one of the Cp rings
are disordered in a 2 : 1 ratio. The individual with the higher
occupation is shown by darker bonds and atoms. Methyl
group C27 is disordered in a 1 : 1 ratio. Selected distances/
pm andangles/ °:
Yb2±O3 225.4*6), Yb2±O4 205.8*6), Yb2'±O3 199*1), Yb2'±O4 235*1),
Yb2±C31 260.4*7), Yb2±C32 266.7*7), Yb2±C35 255.7*7), Yb2±C37
264*2), Yb2'±C29 233*2), Yb2'±C31 259.1*8), Yb2'±C36' 255*2), Yb2'±C34'
269*2), C20±O3 127.1*7), C20±O4 125.6*7); Yb2±O3±C20 139.2*5),
Yb2±O4±C20 152.3*5), Yb2'±O3±C20 148.7*6), Yb2'±O4±C20 156.4*5),
O3±Yb2±*centroidC28±C32) 100.0*7), O4±Yb2±*C28±C32) 105.2*7),
*C28±C32)±Yb2±*centroidC34±C38) 134.7*9), O3±Yb2±*C34±C38)
108.4*8), O4±Yb2±*C34±C38) 104.7*8), O3±Yb2'±*centroidC28±C32)
117*1), O4±Yb2'±*C28±C32) 103*1), *C28±C32)±Yb2'±*centroidC34 '±C38')
129*2), O3±Yb2'±*C34'±C38') 98*2), O4±Yb2'±*C34'±C38') 107*2).
1432
Z. Anorg. Allg. Chem. 2001, 627, 1431±1432