Communications
ꢀ
(a(NPNP) = ꢀ27.3(1)8). Both P N bonds (1.715(1) and
1.718(1) ꢀ) are almost equivalent and lie in the range found
for 1Ter (1.709(2) and 1.731(2) ꢀ), which are shorter than the
ꢀ
sum of the covalent radii for a single bond (dcov(N P) = 1.8,
[28]
=
dcov(N P) = 1.6 ꢀ).
Significantly shorter bonds are
ꢀ
observed in the five-membered tetrazaphospholes Mes*
N4P (1.631(4) and 1.664(3) ꢀ).[9b] Comparison of the struc-
tural data of 1Ter (cis isomer) with those of 3Ter (Table 1)
reveal only small differences. Even the P···P distance is almost
ꢀ
identical (1Ter: 2.612(1) vs. 3Ter: 2.6186(8) ꢀ, cf. Srcov(P
P) = 2.22 ꢀ), indicating no significant transannular interac-
tion. It is interesting to note that the compound [P(m-PMes*)]2
of Fluck et al., which is the isovalence-electronic phosphorus
analogue of 3Ter (both N atoms substituted by two P atoms),
ꢀ
shows a strong transannular interaction with a P P distance of
2.166(2) ꢀ and thus must be referred to as a bicyclotetra-
phosphane.[29] This major difference can be attributed to the
fact that tricoordinated P atoms prefer a pyramidal environ-
ment with a lone pair containing a significant amount of
s orbital character, while nitrogen atoms prefer a trigonal
planar environment when delocalization of the lone pair
(occupying a p orbital) is possible.[24] Thus delocalization of
the 6p electrons (N: 2eꢀ, P: 1eꢀ) stabilizes the biradicaloid
and prevents transannular through-space interaction resulting
in the formation of a bicycle.
Figure 2. ORTEP of the molecular structure of 3Ter in the crystal. H
atoms omitted for clarity; ellipsoids are set at 30% probability at
233 K. Selected bond lengths [ꢂ] and angles [8]: N1–C1 1.423(2), N1–
P2 1.715(1), N1–P1 1.718(1), P1···P2 2.6186(8); C1-N1-P2 130.8(1),
C1-N1-P1 129.6(1), P2-N1-P1 99.44(6), N1i-P1-N1 80.48(8), N1-P2-N1i
i
ꢀ
80.64(8), P2-N1-P1 N1 0.0. Symmetry code: (i) ꢀx, y, ꢀz+3/2.
As illustrated in Scheme 3, both synthetic routes with
either [Cp2Ti(btmsa)] or [{Cp2TiCl}2] as reducing agents
afford in good yields (> 80%) 3Ter as orange microcrystalline
solid. Biradicaloid 3Ter is air- and moisture-sensitive but
stable under argon atmosphere over a long period as solid and
in solvents such as thf, diethyl ether, or toluene, even at
ambient temperatures. The orange color of 3Ter vanishes
rapidly when traces of H2O are present. Like 5Hyp and
btmsa-bridged 6Hyp, biradicaloid 3Ter is easily prepared in
bulk and almost indefinitely stable when stored in a sealed
tube. 31P NMR spectroscopy in particular is suitable to follow
the reduction process and to distinguish between 1Ter
Table 1: Selected bond lengths [ꢂ] and angles [8] along with NAO partial
charges [e] for 1Ter, 3Ter, 5Hyp, and 6Hyp.
1Ter[a]
3Ter[b]
5Hyp[c]
6Hyp
d(N–P)
1.720(2)[c]
2.612(1)
80.93(8)[c]
98.83(8)
ꢀ5.4(1)
+1.32
1.716(1)[c]
2.6186(8)
80.56(8)[c]
99.44(6)
0.0
1.585(2)[c]
2.53(6)
106.9(1)[c]
88.0(2)
4.28(4)
1.29
1.734(3)[c]
2.442(1)
83.5(1)
89.5(1)[c]
27.8(1)
ꢀ1.49
d(P···E)[b]
a(NPN)
a(PNE)[b]
a(NPNE)[b]
q(P)
(d(31P) = 227.4 ppm (cis
isomer), 264.1 ppm (trans
+0.83
isomer)),[20] and 3Ter (d(31P) = 289.8 ppm). The characteristic
deshielding of the P atoms in central P2N2 unit indicates a P,N
p-bonding system. The resonance signals lie in the range
q(N)
ꢀ1.18
ꢀ1.03
ꢀ1.55
+1.16
Sq(NPNE)[b]
+0.28
ꢀ0.41
ꢀ1.22
ꢀ0.67
[a] Taken from reference [20]. [b] E=P for 1Ter, 3Ter, 6Hyp; E=Li for
5Hyp. [c] Averaged values are presented.
ꢀ
typical for cyclic p-delocalized P,N aromatics (cf. Ter N4P:
d(31P) = 217.2 ppm,[9d] Mes* N4P: d(31P) = 226.7 ppm,[9b]
ꢀ
31
[9a]
ꢀ
(Me3Si)2N N3P2: d( P) = 292.1/317.2 ppm), which is con-
siderably more deshielded compared to the compound [Li-
Computations of the electronic structure, and also MO
and NAO analyses (NAO = natural atomic orbital)[24b,c,30]
support the assumption that 3Ter may be regarded as a
biradicaloid with six delocalized p electrons (Figure 3).[24c]
NAO/MO analyses indicate an electron-rich 6p-electronic
system with a pp orbital occupation of 1.65 for the N (2pp) and
1.26e for the P atoms (3pp).[24b,c] The overall charge of the
P2N2 ring amounts to ꢀ0.41e (Table 1). Full optimization at
the UB3LYP/6-31G(d,p) level of theory shows a singlet
ground state with a planar N2P2 ring and no P···P bond. The
singlet state of 3Ter is 22.6 kcalmolꢀ1 lower in energy than the
triplet state (UB3LYP/6-311 + G(d,p)//6-31G(d,p)).[24b,c] UHF
and CASSCF(2,2)/6-31G(d) calculations indicate open-shell
character. The two dominant contributions to the CI wave
2ꢀ
(dme)]+2 [Me3Si C(m-P)]2
(d[31P] = 200.3) from Niecke
ꢀ
et al.[25] The presence of aromaticity is supported by the
calculated NICS(0)[24b,26] value of ꢀ6 ppm (cf. ꢀ7 ppm for
2ꢀ [25]
[Li(dme)]+2 [Me3Si C(m-P)]2
,
and + 5 ppm in 4p elec-
ꢀ
tronic, antiaromatic [TerN(m-Si)]2.[27]
Biradicaloid 3Ter crystallizes as orange crystals from
toluene (or Et2O) without solvent molecules in the mono-
clinic space group C2/c and with four units per cell. The
phenyl rings on the amino nitrogen are twisted to each other,
with a dihedral angle of 27.638 forming a pocket with four aryl
groups (in the 2 and 6 position) in which the N2P2 ring is very
well sterically protected (Figure 2). Thus, the molecular
structure shows, in contrast to P4(tBuN)4, a monomer
consisting of a planar, Cs-symmetric four-membered P2N2
ring (a(P1NP2) = 99.44(6)8, a(N1P1N1’) = 80.48(8)8, and
a(N1P2N1’) = 80.64(8)8). For comparison a butterfly con-
formation is found for 1Ter (a(NPNP) = ꢀ5.3(1)8) and 6Hyp
2
2
2
function for the 1A state are F(1A) = 0.93 j p1 p2 p3 > ꢀ0.35 j
2
2
2
p1 p2 p4 > (Figure 3 left, HOMO = p3, LUMO = p4).[24c] This
corresponds to an occupation of the nonbonding p3 orbital
with 1.7 electrons and thus species 3 possesses considerably
ꢀ 2011 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2011, 50, 8974 –8978