Fig. 2 ORTEP drawing of the molecular structure of 3 in the crystal.
Thermal ellipsoids with 50% probability at 200 K (hydrogen atoms and
t
the disordered Bu groups omitted for clarity). Selected bond lengths (s)
and angles (u)]: Ga–Cl1 2.146(1), Ga–Cl2 2.136(1), Ga–N1 1.990(4), P–N1
1.631(4), P–N4 1.664(3), N1–N2 1.374(5), N2–N3 1.286(5), N3–N4
1.355(5) and N4–C1 1.460(5); Cl1–Ga–Cl2 114.28(3), Cl1–Ga–N1
101.9(1), Cl1–Ga–Cl2i 114.28(3), Cl2–Ga–N1 105.00(6), Cl2–Ga–Cl2i
114.56(6), N1–P–N4 88.2(2), Ga–N1–P 129.7(2), Ga–N1–N2 116.1(3), P–
N1–N2 114.3(3), N1–N2–N3 111.8(4), N2–N3–N4 111.5(3), P–N4–N3
114.2(3), P–N4–C1 128.0(3) and N3–N4–C1 117.8(3). Symmetry code: i =
x, K 2 y, z.
Fig. 4 View along the a-axis in the crystal of 3.
typical range found for other GaCl3 adducts, cf. 1.978(3) in 1 and
2.003(5) s in Cl3Ga?NMe2SiMe2NMe2.3,9 The N–P–N angle of
88.2(2)u is rather small compared to the P–N–N (114–115u) and
N–N–N angles (111–112u). In the crystal, all molecules are parallel
to each other and the aryl groups are superimposed (Fig. 4). The
short P–N and N–N bond distances, together with the planarity,
indicate the presence of a strongly delocalized 6p-electron system,
which is supported by MO and NBO calculations (NBO = natural
bond orbital analysis).10
organic solvents (e.g. benzene, CH2Cl2, ether, etc.) when cooled
(T , 25 uC) and stored in the dark. 3 is easily prepared in bulk
and in high yields (>96%).
X-Ray quality crystals were obtained from a saturated CH2Cl2
solution of 3 at 25 uC, and the single crystal X-ray study revealed
an intriguing GaCl3-stabilized 1-(2,4,6-tri-tert-butylphenyl)tetraza-
phosphole. 3 crystallizes in colourless needles in the monoclinic
space group P21/m with two units per cell.§ As depicted in Fig. 2,
the PN4 ring is planar, like in the pentazoles and the triazadipho-
sphols.3,7 The PN4 ring is however slightly distorted, with two
larger N–N bond lengths (d(N1–N2) = 1.374(5) and d(N3–N4) =
1.355(5) s) and one very short N–N distance (d(N2–N3) =
1.286(5) s; cf. N–N distances between 1.307–1.338 s in
phenylpentazole and 1.380(5) s in 1). These N–N distances
between 1.28–1.38 s are substantially shorter than the sum of the
covalent radii (dcov(N–N) = 1.48 and dcov(NLN) = 1.20 s),8 which
indicates partial double bond character for all the N–N bonds,
with the N2–N3 bond being close to having a bond order of two.
Hence, the release of molecular nitrogen seems to be predisposed.
However, upon GaCl3 adduct formation, the ‘‘naked’’ PN4 ring
becomes sandwiched between the large aryl and large GaCl3
moieties, leading to an astonishing kinetic stability for 3 (Fig. 3).
A similar bond situation is found for the two P–N bonds
(1.631(4) and 1.664(3) s) of the PN4 ring, which also lie in the
range between a single and double bond (dcov(N–P) = 1.8 and
dcov(NLP) = 1.6 s). The Ga–N bond length of 1.990(4) s is in the
Adducts such as 3 are typical charge transfer complexes, and the
bond between the GaCl3 and the azaphosphole can be regarded as
a donor–acceptor bond.3 The calculated adduct formation ((gas
phase): Mes*–N4P + GaCl3 A 3) is exergonic (DG298 = 22.1 and
DH298 = 212.7 kcal mol21).{ According to NBO analysis, the
charge transfer is about 0.15e in 3 (cf. 0.16e in 1). The P–N s- and
p-bonds are highly polarized and almost ideally covalent between
the adjacent nitrogen atoms of the ring in 2 and 3.
In summary, 3 represents a GaCl3-stabilized tetrazaphosphole,
with an electronic structure that is related to those of aromatic
hydrocarbons that have (4n + 2) p-electrons and therefore formally
obey the Hu¨ckel rule. 3 can formally be regarded as the [2 + 3]
2
cycloaddition product of Mes*–PLN+ and N3 ions.
Caution: Like pentazoles, tetrazaphospholes and their adducts
are explosives and thermally unstable species; appropriate safety
precautions should be taken.
A. S. thanks Prof. Dr. T. M. Klapo¨tke (LMU Mu¨nchen) for his
generous support. We also wish to thank the Leibniz
Rechenzentrum for a generous allocation of CPU time. This
research was supported by the DFG SCHU 1170/4-1.
Notes and references
{ A solution of TMS–N3 (0.115 g, 1.0 mmol) in benzene (10 mL) was
added dropwise to a stirred solution of Mes*NPCl (0.326 g, 1.0 mmol) in
benzene (10 mL) at 5 uC. To the red solution, GaCl3 (0.194 g, 1.1 mmol) in
benzene (20 mL) was quickly added via syringe, resulting in a colourless
solution. Removal of the solvent in vacuo yielded 3 as fine, colourless,
needle-like crystals, yield 0.498 g, 0.98 mmol, 98%; mp 145–150 uC (dec.).
Anal. calc. % (found): C, 42.52 (42.06); H, 5.75 (5.35); N, 11.02 (10.61).
NMR (CD2Cl2): 1H 1.05 (s, 18 H), 1.37 (s, 9 H) and 7.66 (s, 2 H); 13C{1H}
30.9 (s, C9 (CH3)3), 32.9 (d, 5JPC = 3.8 Hz, C5 (CH3)3), 35.4 (s, C9), 37.0 (s,
C5), 124.8 (s, C3), 127.9 (d, 2JPC = 6.9 Hz, C2), 147.1 (d, 3JPC = 3.1 Hz, C1)
and 154.6 (s, C4) (Fig. 2). 31P{1H} 226.7 (s) (in C6D6: 228.8). 31P MAS
NMR (25 uC, vrot = 15 kHz): diso 223 (s). m/z (%): 332 (0.3) [2]+, 287 (0.8) [2
2 NP]+, 261 (4.0) [Mes*NH2]+, 259 (4.6) [Mes* + Me]+, 258 (7.9) [2 2
N3P]+, 246 (11.9) [Mes*]+, 245 (7.3) [Mes* 2 H]+, 244 (37.8) [Mes* 2 2 H]+,
Fig. 3 Space-filling models of 3 (left: N4P ring in plane, right: 90u out of
plane).
t
228 (1.8), 202 (2.1) [Mes* 2 C3H5]+, 188 (4.4) [Mes* 2 Bu]+, 132 (6.4)
This journal is ß The Royal Society of Chemistry 2006
Chem. Commun., 2006, 1236–1238 | 1237