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oxoborane featuring a five-membered ring skeleton. The sum of the
bond angles around the boron atom is 359.991 indicating the
trigonal-planar geometry. The B1–O1–Al1 angle (169.44(18)1) in 5
is similar to the value of 169.2(1)1 reported in Ia.7 The B1–O1 bond
length of 1.304(3) Å is ca. 3.5% shorter than the corresponding
B1–O1 single bond in 3, and comparable to that observed in Ia
(1.304(2) Å) but slightly shorter than that in IbꢀB(C6F5)3 (1.311(3) Å).9
The O1–Al1 bond length is 1.7073(16) Å which is slightly shorter
than that in Ia (1.720(1) Å). The B1–N1 bond length (1.480(3) Å) is
longer than B1–N2 (1.437(3) Å), presumably owing to the steric
repulsion between the bulky Dipp group on the N1 atom and the
OAlCl3 moiety on the B atom. The C1–N3 bond (1.319(3) Å) in 5 is
longer than the corresponding C–N bond (1.291(7) Å) in 3. Mean-
while, the C1–N1 bond (1.345(3) Å) in 5 is 0.05 Å shorter than the
corresponding C–N bond (1.401(6) Å) in 3, which indicates that the
cationic charge induced by the coordination of hydrogen on the N3
atom delocalizes over the N1–C1–N3 fragment.
Fig. 4 Selected molecular orbitals of 50 and 6.
Cowley et al. also theoretically supported that the boron–oxygen
functionality of Ia retains considerable double bond character. Thus,
because their calculation results revealed that the B–O distance
(1.316 Å) of the optimized Ia was only increased by 1.9% with
respect to that (1.292 Å) of the Lewis acid-free model compound
LBQO (L = b-diketiminate) which displayed BQO p-bonding in the
HOMO ꢁ 6, they concluded that the B–O bond in Ia has double
bond character. We also performed natural bond order (NBO)
analysis for 50 at the M052X level of theory using the 6-311G(d,p)
basis set, which showed that the B–O s bond is formed by the sp1.71
hybrid orbital of the boron and the sp0.44 hybrid orbital of the oxygen
atom, respectively. The characteristic donor–acceptor interaction
was found between the lone pair orbital on the O atom and the
p-orbital on the B atom, which gives rise to a stabilization energy
of 80.15 kcal molꢁ1 (see Table S2 in the ESI†). Concomitant with
a high occupancy (0.43 e) in the p-orbital on the B atom, the
Wiberg bond index (WBI) value of 1.07 for the B–O moiety was
confirmed. These computational studies supported the partial
BQO double-bond property.
In summary, we synthesized a novel type of oxoborane derivative
5 with a 1,2,4,3-triazaborole skeleton, via the oxydrilic hydrogen
transfer promoted by the coordination of AlCl3 to the corresponding
borinic acid 3. X-ray diffraction analysis of 5 revealed the
presence of the B–O unit coordinating to AlCl3, and computa-
tional study supported the partial BQO double-bond character.
Investigation of the reactivity and synthesis of other analogues
featuring BQX bonds is underway in our laboratory.
In the solid-state IR spectrum of 5, a characteristic peak was
observed at 1636 cmꢁ1 which is assigned to a B–O stretch based
on theoretical calculation (see the ESI,† Fig. S4),18 and the value
is larger than the corresponding stretch (1467 cmꢁ1) of VI
which Yamashita et al. reported,14 indicating the somehow
stronger B–O bond of 5 than that of VI.
The bonding properties and the electronic structure of 5 were
further explored theoretically using ab initio calculations at the
B3LYP level of theory with the 6-31G(d) basis set. The structural
optimization on 5 well reproduced the experimental geometry and
the structural parameters. We also performed the calculations on
the model compound 6 which features the B–O moiety without the
coordination of AlCl3. The resulting optimized structures (50 and 6)
are summarized in Fig. 3. The N–B–N angle of 101.511 in 50 is wider
than the corresponding angle in 6 (97.951). Shortening of both the
B–N bonds when AlCl3 is coordinated to the oxoborane 6 indicates
the enhanced B–N pbonding character, probably attributed to the
decrease of electron-donation of the lone pair on the O atom to the
p-orbital of the B atom. The calculated B–O distance (1.297 Å) in 50 is
only 0.033 Å longer than that in the free oxoborane 6. The p-bonding
interaction on the B–O unit in 50 was found in HOMO ꢁ 12 where
the nitrogen 2p orbitals, the CQN p orbital, and chlorine lone pairs
were involved (Fig. 4, left). In contrast, HOMO ꢁ 2 of 6 exhibits the
BQO p-bonding orbital in which participation of other p-orbitals on
the five-membered ring was not observed (Fig. 4, right). Note that
We are grateful to Nanyang Technological University and
Agency for Science, Technology, and Research, Singapore (A*STAR)
(PSF-SERC: 1321202066), for financial support.
Notes and references
1 (a) M. Ito, N. Tokitoh and R. Okazaki, Tetrahedron Lett., 1997,
38, 4451; (b) M. Ito, N. Tokitoh and R. Okazaki, Phosphorus, Sulfur
Silicon Relat. Elem., 1997, 124, 533; (c) P. Paetzold, S. Neyses and
L. Geret, Z. Anorg. Allg. Chem., 1995, 621, 732; (d) M. Groteklaes and
P. Paetzold, Chem. Ber., 1988, 121, 809.
2 For transient heavier analogues, see: (a) M. Ito, N. Tokitoh,
T. Kawashima and R. Okazaki, Tetrahedron Lett., 1999, 40, 5557;
(b) M. Ito, N. Tokitoh and R. Okazaki, Chem. Commun., 1998, 2495;
(c) H. Suzuki, N. Tokitoh, S. Nagase and R. Okazaki, J. Am. Chem.
Soc., 1994, 116, 11578; (d) H. W. Kroto, Chem. Soc. Rev., 1982,
11, 435; (e) T. A. Cooper, M. A. King, H. W. Kroto and R. J. Suffolk,
J. Chem. Soc., Chem. Commun., 1981, 353; ( f ) C. Kirby, H. W. Kroto and
M. J. Taylor, J. Chem. Soc., Chem. Commun., 1978, 19; (g) R. W. Kirk and
P. L. Timms, Chem. Commun., 1967, 18.
Fig. 3 Selected bond lengths [Å] and angles [1] for the optimized struc-
tures 50 and 6.
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