Communication
Organometallics, Vol. 28, No. 23, 2009 6647
Scheme 1. Synthesis of Lu(GaMe
4
)
3
(1): (a) [Amide] f [Gallate]
route albeit being hampered by the comparable solubility of
2
0
Transformation; (b) GaMe Adduct Formation
3
colorless crystalline 1 and (Me GaNMe ) .
2 2 2
Very pure Lu(GaMe ) , in almost quantitative yield, could
3
4
be obtained by adding a slight excess of GaMe to a suspen-
3
8
sion of polymeric [LuMe ] in hexane (Scheme 1, b). The
3
n
nearly stoichiometric use of expensive trimethylgallium and
the avoidance of undesired gallium-containing byproducts
are clearly favorable attributes. However, the applicability of
this synthesis approach is so far limited to the smaller rare-
8
earth metal centers.
Homoleptic tris(tetramethylgallate) complex 1 is soluble
in hydrocarbon and aromatic solvents. In the absence of
excess GaMe , precipitation of [LnMe ] (accompanied by
3
3 n
the release of GaMe ) immediately occurs in hexane or
3
toluene solutions of Lu(GaMe ) at ambient temperature.
4
3
-
(PNP = N[2-P(CHMe ) -4-methylphenyl] ) were reported
to support monomeric, base-free dimethylscandium com-
2 2 2
Even at -35 °C metal alkyl separation is observed within a
day. This clearly reflects the weak interaction of the
21
1
2-14
plexes.
Trofimenko’s tris(pyrazolyl)borate ligands (Tp
vide a uniquely stabilizing ligand environment for low-
strongly basic lanthanide methyl groups with the compara-
tively weak Lewis acid trimethylgallium.
Single crystals of the homoleptic lutetium tetramethyl-
R,R’ 15
)
pro-
coordinate complexes (L)LnR , as shown by Piers, Takats,
2
gallate were grown from a saturated hexane/GaMe solution
3
tBu,Me
16
)Ln(CH SiMe ) (Ln = Sc, Y) and
and us for (Tp
tBu,Me
(Tp
sent a study of homoleptic lutetium tris(tetramethylgallate),
emphasizing its propensity to act as a [LuMe ] synthon.
3
Utilizing the weak coordination of GaMe in the Lu(GaMe )
3
22
at -35 °C. The X-ray crystallographic structure determi-
2
3 2
17
)Ln(Me)(AlMe ) (Ln = Y, Lu). Herein we pre-
4
nation revealed the 2:1 inclusion complex [{Lu(GaMe ) }
4
3 2
3
(GaMe )] (1 ). As shown in Figure 1, GaMe has been
3 crystal 3
trapped in the crystal lattice, sandwiched between two
molecules of homoleptic Lu(GaMe ) . For homoleptic tetra-
methylaluminates inclusion of Al Me in the crystalline
4
4
3
tBu,Me
moiety and superbulky [Tp
dimethyl lutetium complex has been isolated.
], a monomeric base-free
2
6
lattice has been reported; however, no interaction with
neighboring Ln(AlMe ) molecules was observed (Ln = Y,
7a
Nd).
7
Like the homologous aluminate compound, Lu(Ga-
c
4
3
Me ) (1) was obtained by the original GaMe -mediated
4
3
3
1
8
[NMe ] f [GaMe ] ligand exchange reaction. Accordingly,
2 4
treatment of a suspension of [Lu(NMe ) (LiCl) ] in hexane
with excess GaMe (>6 equiv) yielded 1, (Me GaNMe ) ,
2
and LiCl (Scheme 1, a). While the ligand transformation is
clearly driven by the thermodynamic stability of the alky-
lated gallium amide byproduct, its separation from the
desired Lu(GaMe ) is delicate. The decreased volatility of
Me GaNMe ) compared with the corresponding amino-
2 2 2
aluminum compound prevents the separation in vacuo (10
Torr). Fractional crystallization was found to be a viable
The GaMe moiety is planar (sum of angles about Ga7
3
2
3
3
359.98°) and weakly coordinated to two terminal methyl
groups of neighboring tetramethylgallate ligands, with a
1
9
3
2 2
˚
Ga7 C3 distance of 3.225(3) A and a Ga7 C16 distance
3
3 3
3 3 3
˚
of 3.217(3) A. The Ga7 H separations range from 2.70
3
3 3
˚
to 3.44 A. Similar weak contacts between GaMe molecules
3
4
3
were previously found in the solid-state structures of
trimethylgallium, causing the formation of infinite GaMe3
(
-
2
23
2
shorter than in gaseous GaMe (1.967(2) A), showing that
D networks. The Ga7-C bonds are only marginally
˚
3
the intermolecular interactions do not strongly distort the
2
4
structure of the sandwiched GaMe3. The Lu-C(μ-Me)
(
12) Conroy, K. D.; Piers, W. E.; Parvez, M. J. Organomet. Chem.
008, 693, 834.
13) Scott, J.; Fan, H.; Wicker, B. F.; Fout, A. R.; Baik, M.-H.;
Mindiola, D. J. J. Am. Chem. Soc. 2008, 130, 14439.
bond lengths of the Lu(GaMe4)3 moieties (2.465(2)-
2
(
2
(
˚
.493(2) A) are slightly longer than those observed for Lu-
˚
AlMe ) (2.455(2)-2.471(2) A), while the Lu Ga dis-
-
4 3
3 3 3
(
14) Another [PNP ] ligand was employed to stabilize a monomeric
unsolvated scandium diethyl complex, [N(SiMe CH PiPr ]ScEt
Fryzuk, M. D.; Giesbrecht, G.; Rettig, S. J. Organometallics 1996, 15,
329.
15) Trofimenko, S. Scorpionates: The Coordination Chemistry of
Polypyrazolylborate Ligands; Imperial College Press: London, 1999.
16) (a) Blackwell, J.; Lehr, C.; Sun, Y.; Piers, W. E.; Pearce-
Batchilder, S. D.; Zaworotko, M. J.; Young, V. G. Jr. Can. J. Chem.
997, 75, 702. (b) Cheng, J.; Saliu, K.; Kiel, G. Y.; Ferguson, M. J.;
McDonald, R.; Takats, J. Angew. Chem. Int. Ed. 2008, 47, 4910.
17) (a) Zimmermann, M.; Takats, J.; Kiel, G.; T o€ rnroos, K. W.;
˚
tances (2.9883(3)-3.0018(3) A) are marginally shortened
2
2
2
)
2
2
:
3
(
3 n 4 3
(21) The formation of insoluble [LnMe ] from Lu(GaMe ) is
further observed in the solid state shortly after the mother liquor is
taken off the crystalline material. The previously clear crystals become
(
opaque and brittle within minutes. Crystals of Lu(GaMe
ever, be stored under their mother liquor with some drops of added
GaMe
at -35 °C for weeks.
(22) Compound 1crystal ((C12
crystallizes from a hexane/GaMe
4 3
) can, how-
1
3
(
H
36Ga
3
Lu)
2
ꢀ(C
˚
3 9 r
H Ga), M = 1243.90)
Anwander, R. Chem. Commun. 2008, 612. (b) Litlabø, R.; Zimmermann,
M.; Saliu, K.; Takats, J.; T €o rnroos, K. W.; Anwander, R. Angew. Chem. Int.
Ed. 2008, 47, 9560.
3
mixture in the triclinic space group
˚
˚
P1 with a = 7.2253(2) A, b = 17.3978(5) A, c = 18.6916(6) A, R =
77.626(1)°, β = 86.399(1)°, γ = 85.495(1)°, V = 2285.39(12) A , and
dcalc = 1.808 g cm for Z = 2. Data were collected at 100(2) K on a
3
˚
-
3
(
18) Evans, W. J.; Anwander, R.; Doedens, R. J.; Ziller, J. W. Angew.
Chem., Int. Ed. Engl. 1994, 33, 1641.
19) (a) Coates, G. E. J. Chem. Soc. 1951, 2003. (b) Beachley, O. T.;
Bruker-AXS 2K CCD system. The structure was solved by direct
methods, and least-squares refinement of the model based on 13 491
(all data) and 12 272 reflections (I > 2.0σ(I)) converged to a final wR2 =
0.0477 and R1 = 0.0193, respectively.
(23) (a) Mitzel, N. W.; Lustig, C.; Berger, R. J. F.; Runeberg, N.
Angew. Chem. Int. Ed. 2002, 41, 2519. (b) Boese, R.; Downs, A. J.; Greene,
T. M.; Hall, A. W.; Morrison, C. A.; Parson, S. Organometallics 2003, 22,
2450.
(
Coates, G. E.; Kohnstam, G. J. Chem. Soc. 1965, 3248. (c) Schauer, S. J.;
Lake, C. H.; Watkins, C. L.; Krannich, L. K.; Powell, D. H. J. Organomet.
Chem. 1997, 549, 31.
(
20) The GaMe
proceed as smoothly as with the more Lewis acidic AlMe
of GaMe has to be used to avoid incomplete ligand exchange, as
evidenced earlier crystallographically with Nd(NMe (GaMe and
La(NMe (GaMe (GaMe ), ref 18.
3
-mediated [NMe
2
] f [GaMe
4
] exchange does not
3
; a large excess
3
2
)
3
3
)
3
(24) McGrady, G. S.; Turner, J. F. C.; Ibberson, R. M.; Prager, M.
Organometallics 2000, 19, 4398.
2
)
2
3
)
2
4