Y.Feng et al./ Inorganic Chemistry Communications 6 (2003) 466–468
467
UV–Vis [kmax(toluene)/nm (10À3e=dm3 molÀ1 cmÀ1)]:
338(9), 420(28), 437(117), 518(1), 570(4), 611(3). 1H
NMR (toluene-d8, )50 °C) d : 9.08 (s, 8H, pyrrole-H),
8.28 (m, 8H, o-H), 7.83 (m, 12H, m,p-H), )6.47 (s, 1H,
GaH).
Single crystals of 1 suitable for X-ray analysis were
obtained by slow evaporation of a solution of the
compound in toluene at )20 °C during a few weeks.
2.2. X-ray structural study of 1
The intensity data of the compound was collected on
Nonius Kappa CCD with Mo-Ka radiation
a
ꢀ
Fig. 1. Electronic absorption spectrum of Ga(TPP)H (solid line) and
Ga(TPP)Cl (dashed line) in toluene.
(k ¼ 0:71073 A) at 293 K. The structure was solved by
direct methods and refined by full-matrix least-squares
based on F 2 using the SHELXL-97 program. All non-
hydrogen atoms were refined anisotropically, while all
hydrogen atoms except M–H were assigned to calcu-
lated positions.
Crystal structure analysis data for 1: [GaC44H28
N4ÞH], Mr ¼ 683:46, tetragonal, I4, a ¼ 13:370ð2Þ, b ¼
ꢀ
ꢀ3
13:370ð2Þ, c ¼ 9:750ð2Þ A, V ¼ 1742:9ð5Þ A , Z ¼ 2,
l ¼ 0:827 mmÀ1, GOF ¼ 1:155, F ð000Þ ¼ 704, R1 ¼
0:0645, wR2 ¼ 0:1731, 118 parameters, 1528 reflections
[I > 2rðIÞ].
3. Results and discussion
The presence of hydride ligand in the compound was
confirmed by the IR spectrum. The Ga–H IR stretch
occurs at 1864 cmÀ1, which locates in the typical region
Fig. 2. ORTEP view of the compound 1 showing the 50% probability
thermal motion ellipsoid. Hydrogen atoms have been omitted for
ꢀ
clarity. Selected bond distances (A): Ga–N 2.035(4), Ga–H 1.48(4),
for other terminal gallium hydrides (ca. 1850–1900 cmÀ1
)
[17,18]. The high-field hydride signal (d: )6.47 ppm) in
the 1H NMR spectrum gives further support for the
existence of hydride. Unlike Ga(TPP)Cl, which shows a
‘‘normal’’ porphyrin electronic spectrum, 1 shows elec-
tronic absorption spectrum belonging to the hyperclass
[19]. The Soret band is split into two bands (labeled band
I and band II), which appear between 338 and 437 nm.
The B(1,0) blue-shifted band is observed at 420 nm, and
the three Q bands are located at 518, 570 and 611 nm.
Band I may be attributed to 4Pz ! egðpꢀÞ transition,
while band II is assigned as a p ! pꢀ electronic transi-
tion. For comparison, the electronic absorption spectra
of [Ga(TPP)Cl] and 1 are shown in Fig. 1.
The molecular structure of 1 is shown in Fig. 2 with
important bond lengths and angles in figure caption. A
crystallographic 4-fold axis passes through Ga and is
perpendicular to the porphyrin plane relating the four
equal parts of the molecule. As observed for Fe(TPP)Cl
[20] and Ga(TPP)Cl [16], the gallium and hydrogen at-
oms are statistically disordered up and down the por-
phyrin macrocyclic plane. The coordination polyhedron
of the metallic atom is a square pyramid and the metal
N–C(1) 1.381(6), N–C(4) 1.378(6), C(1)–C(2) 1.434(7), C(2)–C(3)
1.341(7), C(3)–C(4) 1.446(6), C(4)–C(5) 1.386(7).
ꢀ
little longer than that in Ga(TPP)Cl (0.317(1) A) [16].
ꢀ
The Ga–H distance is 1.48(4) A, which is at the medium
of previously reported terminal Ga–H bonds (ca. 1.4–1.6
ꢀ
A) [21,22]. The bond distances and angles in the por-
phyrinic group are statistically equal to those usually
found.
References
[1] (a) A.J. Downs, Chemistry of Aluminum, Gallium, Indium and
Thallium, Blackie, Glasgow, 1993;
(b) A.J. Downs, C.R. Pulham, Chem. Soc. Rev. (1994) 175, and
references therein.
[2] N.N. Greenwood, A. Storr, M.G.H. Wallbridge, Inorg. Chem. 2
(1963) 1036.
[3] J.L. Atwood, S.G. Bott, F.M. Elms, C. Jones, C.L. Raston, Inorg.
Chem. 30 (1991) 3792.
[4] P.C. Andrews, M.G. Gardiner, C.L. Raston, V.-A. Tolhurst,
Inorg. Chim. Acta 259 (1997) 249.
ꢀ
atom lies 0.46(1) A from the porphyrin plane, which is a