Fig. 1 Crystal structure of 2. The thermal ellipsoids are given at
Fig. 2 Crystal structure of 3. The thermal ellipsoids are given at the
the 50% probability level. Hydrogens are omitted for clarity. Se-
◦
50% probability level. H◦ydrogens are omitted for clarity. Selected bond
˚
lected bond lengths [A] and angles [ ]: Ga1–N1 1.978(2), Ga1–N2
˚
lengths [A] and angles [ ]: I1–Ga1 2.594(2), I2–Ga3 2.565(2), Ga1–N1
1.986(2), Ga1–Ga1¢ 2.430(1), Ga1–I1 2.533(1), N1–C1 1.319(3), N1–C3
1.420(3), N2–C1 1.315(3), N2–C15 1.414(3), C1–C2 1.483(4); N1–Ga1–N2
66.5(1), N1–Ga1–Ga1¢ 120.9(1), N2–Ga1–Ga1¢ 119.4(1), N1–Ga1–I1
107.7(1), N2–Ga1–I1 109.5(1), Ga1¢–Ga1–I1 120.7(1), C1–N1–C3
123.9(2), C3–N1–Ga1 144.8(2), C1–N2–C15 126.9(2), C1–N2–Ga1
91.1(1), C15–N2–Ga1 141.6(2), N2–C1–N1 111.2(2).
1.953(4), Ga1–N2 1.963(4), Ga1–Ga2 2.420(1), Ga2–N3 1.975(4),
Ga2–N4 1.978(4), Ga2–Ga3 2.415(1), Ga3–N5 1.950(4), Ga3–N6
1.976(4); N1–Ga1–N2 66.0(2), N1–Ga1–Ga2 127.9(2), N2–Ga1–Ga2
127.9(2), N1–Ga1–I1 105.5(2), N2–Ga1–I1 107.1(2), Ga2–Ga1–I1
113.32(3), N3–Ga2–N4 65.4(2), N3–Ga2–Ga3 114.0(2), N4–Ga2–Ga3
112.7(1), N3–Ga2–Ga1 114.5(2), N4–Ga2–Ga1 114.9(2), Ga3–Ga2–Ga1
122.2(1), N5–Ga3–N6 66.5(2), N5–Ga3–Ga2 125.7(2), N6–Ga3–Ga2
126.7(2), N5–Ga3–I2 109.1(1), N6–Ga3–I2 109.1(1), Ga2–Ga3–I2
112.1(1), C1–N1–Ga1 93.7(3), C1–N2–Ga1 93.0(3), C18–N3–Ga2 94.8(3),
C18–N4–Ga2 94.1(3), C35–N5–Ga3 93.7(3), C35–N6–Ga3 92.0(3),
N1–C1–N2 107.2(4), N3–C18–N4 105.7(4).
of a molecule 3 consists of a chain of three gallium atoms
˚
˚
with distances of 2.420(1) A and 2.415(1) A. The Ga–Ga–Ga
angle at the central gallium atom is 122.2(1)◦. Each gallium
is bonded to a dicyclohexylneopentylamidinate by its nitrogen
˚
˚
atoms (1.950(4) A–1.978(4) A). The Ga–N bonds of Ga(1) and
˚
Ga(3) are shorter by 0.02 A compared to the central gallium
distorted tetrahedral coordination and typical distance (Ga(1)–
atom’s bond lengths. This is conforming to Bent’s rule.31,32 The
terminal gallium atoms in oxidation state +II complete their
distorted tetrahedral coordination with one iodine, each. The Ga–
I(1) 2.566(2) A). The other Ga(II) in the molecule is bonded to
˚
˚
an NCMe2 group with a Ga(3)–N(7) distance of 2.02(1) A and
angles of 113.7(3)◦ (Ga(2)–Ga(3)–N(7)) and 115.0(4)◦ (C(35)–
Ga(3)–N(7)). The Ga(3)–N(7)–C(52) unit is not linear (Ga(3)–
N(7)–C(52) 133.9(10)◦). It points away from the centre of the
structure, in virtue of C(35)–Ga(3)–N(7)–C(52) 4(1)◦ and Ga(3)–
N(7)–C(52)–C(53) 15(2)◦.
˚
˚
I-distances (2.594(1) A–2.565(1) A) are in the typical range. The
amidinate groups binding to them have the same bite angle as in 2
within the standard deviation (66.3(2)◦). The NCN-angles deviate
significantly from the ideal 120◦ for a triple coordinated carbon
(NCN 107.5(4)◦ (avg)). This is in line with the acute NGaN angles
in the planar four membered GaN2C rings. The amidinate bonded
to the central Ga(2) (oxidation state +I) differs slightly, since the
bite angle with 65.3(2)◦ and the NCN-angle with 105.7(4)◦ are a
bit sharper, even.
We were able to obtain 3 cocrystallized with n-hexane (3a,
colourless, triclinic crystals, space group P1), toluene (3b, colour-
less, triclinic crystals, space group P1) and thf (3c, colourless,
monoclinic crystals, space group P21/n). The structures of 3a and
3b do not differ very much from 3, but 3c does. While the torsion
angle I1–Ga1–Ga3–I2 in 3, 3a and 3b is approximately 125–126◦,
in 3c it is -88◦. There is no close contact between the solvent
molecules and the compound. A possible answer for this twist will
be given in the Quantum chemical calculations section.
5 was crystallized from n-hexane as colourless, monoclinic rods
in space group P 21/c (Fig. 4). Molecules of 5 contain a chain of
three gallium atoms which form almost the same angle like in 3
(121.3(1)◦). The Ga–Ga-distances are slightly elongated compared
˚
˚
to 3 (Ga(1)–Ga(2) 2.457(2) A and Ga(2)–Ga(3) 2.463(2) A), which
is in the line with Bent’s rule.31,32 Each of the gallium atoms
is chelated by one dicyclohexylneopentylamidinate, with Ga–N-
¯
¯
˚
˚
distances of 2.006(7) A to 2.029(6) A, which is slightly longer
than in 3. Due to this elongation the bite angles have to decrease
to 64.9(2)◦ to 65.1(2)◦. The distorted tetrahedral coordination
sphere at Ga(1) at the one side of the chain is completed by a
˚
hydride (H(1)) (Ga(1)–H(1) 1.54(6) A). Ga(3) at the other side of
the chain is surrounded in a distorted tetrahedral manner by an
˚
amidinate, Ga(2) and an ethyl group (Ga(3)–C(52) 1.988(9) A).
4 was obtained by crystallization from thf as colourless,
monoclinic rods, space group Cc (Fig. 3). The unit cell contains
three molecules of thf per molecule 4. The Ga3-unit forms an
This ethyl group points away from the molecule in a way, that the
ethyl carbons, Ga(3) and the linking carbon of the amidinate rest
are coplanar (torsion angle C(53)–C(52)–Ga(3)–C(35) -0.5(7)◦).
6 was crystallized from toluene as colourless, monoclinic plates
in space group C 2/c (Fig. 5). It is composed by a gallium atom
in oxidation state +III distorted tetrahedral coordinated by two
iodine atoms and chelated by one dicyclohexylneopentylamid-
◦
˚
angle of 124.5(1) , with distances of Ga(1)–Ga(2) 2.417(2) A
˚
and Ga(2)–Ga(3) 2.436(2) A. All gallium atoms are chelated
by dicyclohexylneopentylamidinates, with Ga–N distances o◦f
◦
˚
˚
1.939(8) A–1.984(7) A and bite angles of 66.6(3) (Ga(1)), 65.9(3)
(Ga(2)) and 68.2(3)◦ (Ga(3)). Ga(1) carries an iodine atom in
˚
˚
inate (Ga(1)–I(1) 2.508(1) A, Ga(1)–I(2) 2.491(1) A, Ga(1)–N
This journal is
The Royal Society of Chemistry 2011
Dalton Trans., 2011, 40, 5591–5598 | 5595
©