Metallaborane compounds, in particular the earlier transition metals, present interesting challenges to the well-established cluster electron-counting rules. 1À4 Although the electron-counting rules suggest a wide variety of target metallaborane compositions, they provided no direct information on their synthesis. The answer to overcoming the inherent instability of the MÀB bond network relative to a mixture of boranes and metal complexes is to lower all free energy barriers in the preparative pathway. The successful approach of Fehlner utilized the formation of metalÀ polyborohydrides either from metathesis of metal halogen bonds with metal borohydrides or by MÀX, BÀH bond metathesis with neutral boranes. 5 The H 2 elimination from the metalÀ polyborohydride leads to metallaboranes in preference to borane elimination that produces metal hydrides. This approach has been successful for metallaboranes containing a variety of group 6À9 metals having a pentamethylcyclopentadienyl ligand. 6 In the same way, we applied the above approach, with some modifications, to group 5 metals and discovered a number of interesting metallaborane compounds having novel cage geometries and unusual structural features of interest. 7,8 Interestingly, these results as well as the existence of higher nuclearity closorhenaboranes 9 and hydrogen-rich nido-ruthenaboranes, 10 led us to revisit the Ta system that yielded hypoelectronic tantalaborane [(Cp*Ta)(Cp*TaCl)B 9 H 16 ], 2. Reported here is the synthesis and structural characterization of tantalaborane 2.
' RESULTS AND DISCUSSIONAs previously reported, the reaction of 1 with monoborane reagents (LiBH 4 and BH 3 3 thf) resulted in [(Cp*Ta) 2 (B 2 H 6 ) 2 ], [(Cp*TaCl) 2 B 5 H 11 ], and [(Cp*Ta) 2 B 5 H 11 ] (Scheme 1). 7 Minor product 2, with an R f higher than [(Cp*TaCl) 2 B 5 H 11 ], was enhanced by using excess [BH 3 3 thf] and reduced temperature and time. Although compound 2 is produced in a mixture, these compounds can be separated by preparative thin-layer chromatography (TLC), allowing the characterization of pure materials. The FAB mass spectrum gave a molecular ion peak corresponding to C 20 H 46 B 9 Cl 1 Ta 2 , while the IR spectrum displayed bands at 2506 and 2484 cm À1 , characteristic of terminal BÀH stretches. The 11 B NMR spectrum of 2 displays seven signals in the ratio 1:1:1:2:1:2:1, distributed over an unusually large chemical shift range of ca. 100 ppm. Besides the BH terminal protons, three BÀHÀB and four TaÀHÀB protons with an equal intensity were observed. Furthermore, 1 H and 13 C NMR spectra imply two inequivalent Cp* ligands. The variable-temperature 1 H{ 11 B} and 11 B{ 1 H} NMR study revealed no fluxional behavior associated with TaÀHÀB or BÀHÀB bonding.In order to confirm the spectroscopic assignments and determine the crystal structure of 2, an X-ray analysis was undertaken. Crystals suitable for X-ray diffraction studies were grown by cooling a concentrated hexane solution to À10°C. The crystal structure of 2 corresponds to discrete molecules of [(Cp*Ta)...