1620 Organometallics, Vol. 19, No. 9, 2000
Communications
dihedral angle is 19.9(2)°,5 these atoms are essentially
coplanar (along with O) in anions 2. Notably, the
geometry about oxygen is trigonal planar (the sums of
the angles are 360.0 and 359.9° for 2-OC6F 5 and
2-OCH 3, respectively) in contrast to the trigonal-
pyramidal ground-state structures found for the related
alkyloxonium salts [R3O]+[A]-. The energy surface
connecting these two geometries is soft;11 presumably,
bulky groups about O will favor planar geometries.12
Alternatively, the bite angle of 1 may require that O
assumes an sp2 hybridization in order to form strong σ
bonds to the two boron atoms.
The stoichiometric reactivity of compounds 2 with 1
or 2 equiv of Cp2ZrMe2 was investigated to assay the
stability of the resulting ion pairs. Clean reactions were
observed in each case, although in the case of 2-F , it is
clear that F- transfer to zirconium is facile (eq 3). This
F igu r e 1. ORTEP diagram for the anionic portion of
2-OC6F 5. The F atoms on the B-C6F5 rings and the OC6F5
ring have been removed for clarity. Selected bond distances
(in Å; values in brackets are the analogous values for
2-OCH3): B(1)-C(1), 1.600(10) [1.614(2)]; B(2)-C(6), 1.572-
(10) [1.622(2)]; B(1)-O(1), 1.693(8) [1.568(2)]; B(2)-O(1),
1.644(9) [1.562(2)]; O(1)-C(7), 1.386(8) [1.4485(19)]. Se-
lected bond angles (in deg): B(1)-O(1)-B(2), 115.4(5)
[117.72(12)]; B(1)-O(1)-C(7), 120.8(5) [121.27(13)]; B(2)-
O(1)-C(7), 123.8(5) [120.93(13)]; B(1)-C(1)-C(6), 115.4-
(6) [113.27(14)]; B(2)-C(6)-C(1), 116.8(6) [112.77(14)].
is particularly indicated by the highly characteristic 19
F
NMR spectral fingerprint for the [1‚Me]- anion,6 which
forms when free diborane 1 is liberated after the F-
transfer event. The presence of the dimeric µ-F cation2,13
is evidenced by a signal in the 19F NMR spectrum at
-90.4 ppm.
nance is observed between 0 and 9 ppm, the region
expected for four-coordinate boron centers with a formal
-0.5 charge. For 2-OC6F 5, evidence for fluxionality is
apparent in the room-temperature 19F spectrum. Vari-
able-temperature experiments show that this process
is associated with restricted rotation of the boron C6F5
rings, since the patterns present for the backbone
fluorines and those associated with the OC6F5 group
indicate that the C2v symmetry of the anion is main-
tained at all temperatures. Presumably, the hindered
rotation of the -C6F5 substituents on boron is due to
In contrast, the µ-OR anions are stable in the presence
of both [(Cp2ZrMe)2(µ-Me)]+ 14 (eq 4a) and [Cp2Zr(S)Me]+
(eq 4b) in C6D5Br, with no OR- transfer to Zr15 observ-
able over time periods on the order of days in each case.
the bulkier character of the pentafluorophenoxide group
-
in comparison to F- or OCH3
.
This stability appears to be thermodynamic in nature.
Gentle heating (60 °C) of solutions of the ion pair
3-OCH3 resulted in decomposition of the dimeric cation
through loss of methane,16 but 19F NMR spectroscopy
showed that the anion remained intact throughout.
Similarly, heating solutions of the monomeric ion pair
4-OCH3 gives no evidence for decomposition at 40 °C.
The molecular structure of the anion in 2-OC6F 5 is
shown in Figure 1 along with selected metrical param-
eters; in brackets, the analogous data for 2-OCH3 are
given for comparison.10 Confirming the solution struc-
tural assignments, in both of these compounds, OR is
bound to both borane centers in a symmetrical fashion.
Unlike the free diborane, in which the B-C-C-B
(11) (a) Lambert, J . B. Top. Stereochem. 1971, 6, 19. (b) Rauk, A.;
Andose, J . D.; Frick, W. G.; Tang, R.; Mislow, K. J . Am. Chem. Soc.
1971, 93, 6507.
(12) A related compound with less bulky groups at boron, [(µ-CH3-
CO2)(BF2)2(µ-OCH3)], crystallizes with two molecules in the unit cell,
one of which is planar at the µ-OCH3 oxygen and the other pyrami-
dal: Binder, H.; Matheis, W.; Deiseroth, H.-J .; Fu-Son, H. Z. Natur-
forsch., B 1983, 38, 554.
(10) Crystal data for 2-OC6F 5: C57H19B2Cl3F29O, 0.20 × 0.19 × 0.06
mm, triclinic, P1h, a ) 12.2241(15) Å, b ) 12.8975(16) Å, c ) 18.801(2)
Å, R ) 80.166(2)°, â ) 72.091(2)°, γ ) 70.812(2)°, V ) 2655.9(6) Å3, Z
) 2, FW ) 1398.69, Dcalcd ) 1.749 g cm-3, θ range for data collection
1.68-25.00°, Mo KR radiation, λ ) 0.710 73 Å, T ) 160(2) K, 15 208
measured reflections, 8865 unique, 3565 reflections with Inet > 2.0σ-
(Inet), µ ) 0.319 mm-1, min/max transmission 0.939 and 0.981, final R
indices R1 ) 0.0812 and wR2 ) 0.2135, GOF ) 0.969, 36 restraints,
848 parameters. Crystal data for 2-OCH3: C51H20B2Cl2F24O, 0.60 ×
0.35 × 0.35 mm, monoclinic, P21/n, a ) 13.5900(2) Å, b ) 19.3540(2)
Å, c ) 18.5439(2) Å, â ) 101.517(2)°, V ) 4779.23(10) Å3, Z ) 4, FW
) 1197.19, Dcalcd ) 1.664 g cm-3, θ range for data collection 2.00-
29.11°, Mo KR radiation, λ ) 0.710 73 Å, T ) 160(2) K, 39 886
measured reflections, 11 847 unique, 8912 reflections with Inet > 2.0σ-
(Inet), µ ) 0.271 mm-1, final R indices R1 ) 0.0446 and wR2 ) 0.1158,
GOF ) 1.061, 15 restraints, 733 parameters. The restraints were
applied to geometry and anisotropic displacement parameters of atoms
in disordered solvent molecules, to aid their refinement. There were
no restraints on the cations and anions.
(13) Yang, X.; Stern, C. L.; Marks, T. J . J . Am. Chem. Soc. 1994,
116, 10015.
(14) (a) Bochmann, M.; Lancaster, S. L. Angew. Chem., Int. Ed. Engl.
1994, 33, 1634. (b) Yang, X.; Stern, C. L.; Marks, T. J . Organometallics
1991, 10, 840. (c) Beck, S.; Prosenc, M.-H.; Brintzinger, H. H.; Goretzki,
R.; Herfert, N.; Fink, G. J . Mol. Catal. 1996, 111, 67. (d) Ko¨hler, K.;
Piers, W. E.; Xin, S.; Feng, Y.; Bravakis, A. M.; J arvis, A. P.; Collins,
S.; Clegg, W.; Yap, G. P. A.; Marder, T. B. Organometallics 1998, 17,
3557.
(15) Siedle, A. R.; Newmark, R. A.; Lamanna, W. M.; Schroepfer, J .
N. Polyhedron 1990, 9, 301.
(16) Bochmann, M.; Cuenca, T.; Hardey, D. T. J . Organomet. Chem.
1994, 484, C10.