Angewandte
Communications
Chemie
acetonitrile resulted in the formation of boryldichlorophos-
details, see the Supporting Information): a) the HOMO
exhibits features of the nonbonding lone pair on the
phosphorus atoms, b) the HOMO-7 and the LUMO corre-
spond to the p and p* orbitals of the P=P double bond, and
phine 6. The observed BÀP bond length of 1.952(2) ꢀ in 6 is
close to the sum of the covalent radii of the B and P atoms
[
14]
(
1.98 ꢀ),
which suggests the absence of any pp–pp
interactions. A subsequent reduction of 6 with magnesium
in THF furnished diboryldiphosphene 2 in moderate yield. In
c) the HOMO-1 is predominantly characterized by contribu-
tions from the p-type orbital of the diazaborole moieties.
To better understand the electronic effects of the boryl
substituents in 2, the compound was subjected to UV/Vis
spectroscopy, cyclic voltammetry, and further DFT calcula-
tions. The UV/Vis spectrum of 2 showed two absorption
maxima at 310 nm (e = 5700) and 400 nm (e = 680; Fig-
ure S10), which are slightly blue-shifted relative to the
absorptions of Mes*-substituted diarylphosphene 1 (325,
3
1
the P NMR spectrum of 2 in C D , two magnetically
6
6
equivalent phosphorus nuclei were observed at d 605 ppm,
P
which are comparable, albeit slightly low-field-shifted, to the
resonances of carbon-substituted symmetrical trans-diphos-
[
6a,b,7,15]
phenes (d ꢀ 477–600 ppm).
The electropositive boryl
P
substituents may contribute to the low-field shift of these
resonances, considering that the chemical shifts of symmet-
rical diphosphenes with electropositive silyl substituents
[
6]
460–532 nm), indicating a larger HOMO–LUMO gap of
(
electronegativity of Si: 1.90, Pauling) are further down-
1 relative to that of 2. The cyclic voltammogram of 2 in THF
[
16]
11
n
field-shifted (d 735, 818 ppm). The B NMR spectrum of 2
showed a broad signal at d 30 ppm.
The centrosymmetric molecular structure of 2 was deter-
mined by single-crystal X-ray diffraction analysis (Figure 1).
The observed P=P bond length of 2.0655(17) ꢀ is slightly
(supporting electrolyte: 0.1m [ Bu N][BF ]) showed a rever-
P
4
4
+
sible reduction wave at À2.24 V (vs. Cp Fe/Cp Fe ; Figur-
B
2
2
[20]
es S16 and S17), which is lower than that of 1 (À2.36 V),
suggesting a lower LUMO level in 2 relative to that in 1. A
structural optimization of 1 and 2 at the B3LYP/6-31G(d)
level of theory was able to reproduce the crystallographically
obtained structures, albeit with slightly deviated dihedral
angles. For comparison, diphenyldiphosphene PhP=PPh (7)
longer than those of previously reported carbon-substituted
was calculated as a model compound (for details, see the
Supporting Information). These calculations revealed that the
presence of the boryl substituents in 2 raise the energy levels
of all P=P-related orbitals (n, p, p*) relative to those of 7. Due
to the introduction of three electron-donating tert-butyl
groups on each phenyl substituent in 1 compared to 7, the
change in energy levels of the corresponding orbitals is
consistent with the trends observed by UV/Vis spectroscopy
and cyclic voltammetry.
n
Addition of BuLi to diboryldiphosphene 2 at À358C in
THF afforded the stable adduct 8(thf) , which exhibited two
n
3
1
doublets in the P NMR spectrum at d À192 (P-Li) and d
P
P
n
À127 ppm (P- Bu; Scheme 2). The relatively large coupling
1
constant ( J = 208 Hz) is indicative of direct bonding
PP
Figure 1. Molecular structure of 2 (thermal ellipsoids set at 50%
probability, hydrogen atoms omitted for clarity; asterisks denote atoms
generated by symmetry operation), Selected bond lengths [ꢀ] and
angles [8]: P1–B1 1.936(3), N1–B1 1.418(4), N2–B1 1.424(4), P1–P1*
between two inequivalent phosphorus nuclei. Considering
1
1
7
that the B and Li NMR spectra of 8(thf) showed two
n
distinct broad signals and one sharp singlet signal, respec-
tively, the Li cation should be dissociated from the phosphide
center to form a solvent-separated ion pair. In THF, this
species was found to be stable at room temperature for 9.5 h.
2
.0655(17); P1*-P1-B1 95.83(9), N1-B1-N2 108.3(2), P1-P1-B1-N1 95.8-
(
2).
n
In contrast, treatment of 1 with BuLi at À358C in THF led to
[
17]
[18]
diphosphenes [1.985(3) –2.051(2) ꢀ ]. The two boron-
containing planes are oriented almost perpendicular to the
planar B-P=P-B moiety, exhibiting a dihedral N2-B1-P1-P1*
angle of À83.2(2)8. This structure stands in stark contrast to
the perpendicular and coplanar conformers that were
[5q]
observed for the recently reported diboryldibismuthene.
The B1–P1 bond length of 1.936(3) ꢀ in 2 is similar to the BÀ
P bond length in 6 [1.952(2) ꢀ], indicating a single-bond
character for this bond, due to little overlap between the 2p
and 3p orbitals of the boron and phosphorus atoms, respec-
tively. The observed B1-P1-P1* angle of 95.83(9)8 is relatively
small, but still within the range of the corresponding C-P-P
angles of symmetrical carbon-substituted diphosphenes
[
19]
[18]
[
3
93.22(5)8 -114.9(1)8 ]. DFT calculations at the B3LYP/6-
1G(d) level of theory revealed the following features (for
n
Scheme 2. Addition of BuLi to diboryldiphosphene 1 and 2.
2
ꢀ 2016 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2016, 55, 1 – 6
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