Bis(phthalocyaninato)gadolinium(III) Hexacyanobutadienide(1-), [GdPc
2
]
+
[C
4
(CN)
6
]
-
. An Electron
Transfer Salt with Four Paramagnetic Sites
Durrell K. Rittenberg,
†
Ken-ichi Sugiura,
‡
Yoshiteru Sakata,
‡
Atta M. Arif,
†
and Joel S. Miller*
,†
Department of Chemistry, University of Utah, Salt Lake City, Utah 84112, and Institute for Industrial and Scientific Research,
Osaka University, Osaka 565, Japan
ReceiVed February 13, 2001
Metallophthalocyanines, MPc (H
2
Pc ) phthalocyanine), con-
tinue to be at the forefront of modern chemistry owing to their
unique chemical
1,2
and physical properties
1,3
In particular, rare-
earth phthalocyanines, i.e., LnPc
2
and Ln
2
Pc
3
(Ln ) lanthanide),
have received considerable attention in the past few years due
to their unique electrochromic,
1
spectral,
2
and conducting proper-
ties.
3
Rare-earth phthalocyanines are attractive building blocks for
molecule-based magnets due to the lanthanide, which may possess
up to seven unpaired electrons (i.e., S )
7
/
2
). In their neutral form,
LnPc
2
are characterized as having stable phthalocyaninate(2-)
and radical phthalocyaninate(1-) ligands consisting of (Pc
2-
)-
Ln
+3
(Pc
•-
) in resonance with (Pc
•-
)Ln
3+
(Pc
2-
)
4
or as Ln
4+
(Pc
2-
)
2
for Ln ) Ce.
5
Upon facile reduction to the monoanion the
complex may be described as [Ln
3+
(Pc
2-
)
2
]
-
, which in the case
of [LuPc
2
]
-
was confirmed by NMR.
2a
In contrast, oxidation to
[LnPc
2
]
+
leads to two possible electronic structures, i.e.,
[Pc
2-
Ln
3+
Pc
0
]
+
{in resonance with [Pc
0
Ln
3+
Pc
2-
]
+
} or
[Pc
•-
Ln
3+
Pc
•-
]
+
, as well as systems with tetravalent Ln (i.e.,
Pc
2-
Ln
4+
Pc
2-
). Very few oxidized LnPc
2
species have been
characterized; however, [LuPc
2
]
+
[SbF
6
]
-
is reported to be
diamagnetic;
4c
hence it must be described as [Pc
2-
Lu
3+
Pc
0
]
+
or
[Lu
3+
(Pc
•-
)
2
]
+
with strong antiferromagnetic coupling between
the S )
1
/
2
Pc
•-
units. For spin-containing lanthanide, e.g., Gd
3+
,
the S )
7
/
2
Gd
3+
and S )
1
/
2
Pc
•-
are strongly coupled for GdPc
2
leading to an S ) 3 ground state.
4d
Furthermore, on the basis of
the absence of an EPR signal assignable to Pc
•-
and the presence
of an EPR signal assignable to Gd
3+
, the ground state was reported
to have a [Pc
0
Gd
3+
Pc
2-
]
+
electronic structure,
4b,c
which was
modeled by MO calculations.
6
LnPc
2
with the added feature of possessing spin-bearing ligands
has a structural relationship to S )
1
/
2
[Fe
III
(C
5
Me
5
)
2
]
+
, a key
component in the first organic magnet, [Fe
III
(C
5
Me
5
)
2
]
+
[TCNE]
•-
(TCNE ) tetracyanoethylene) (T
c
) 4.8 K).
7
Hence,
[GdPc
2
]
+
[TCNE]
•-
due to the presence of g ) 2, L ) 0 Gd
3+
,
was targeted for synthesis. Although TCNE was insufficient to
oxidize GdPc
2
,C
4
(CN)
6
8
was reacted with GdPc
2
forming [GdPc
2
]-
[C
4
(CN)
6
], 1. In accord with previous work, GdPc
2
has several
sites that can be oxidized, namely, Pc
•-
, and Pc
2-
, and unlikely,
but observed for other Ln
3+
’s, Gd
3+
. Hence, [GdPc
2
][C
4
(CN)
6
]
is valence ambiguous as it may be formulated in many ways,
e.g., (i) [Gd
3+
Pc
2
]
0
[C
4
(CN)
6
]
0
, (ii) [Gd
3+
(Pc
•-
)
2
]
+
[C
4
(CN)
6
]
•-
, (iii)
[Gd
3+
(Pc
0
)(Pc
2-
)]
+
[C
4
(CN)
6
]
•-
, or their resonance structures.
4d
Herein, we report the crystal and electronic structures of 1.
GdPc
2
4c
and C
4
(CN)
6
8
were prepared by literature methods. 1
was prepared from the reaction of GdPc
2
(24.7.0 mg, 0.0208
mmol) and C
4
(CN)
6
(25.0 mg, 0.122 mmol) each dissolved in 20
mL of PhCl and stirred under nitrogen at room temperature for 4
h. The resulting dark green microcrystalline precipitate was then
collected by vacuum filtration. Single crystals were grown in a
20 mL “H-tube” crystallization cell loaded with 7.1 mg of C
4
-
(CN)
6
in 0.5 mL of CH
2
Cl
2
and 10 mg of GdPc
2
mixed in 0.5
mL of CH
2
Cl
2
in different ends of the tube. Chlorobenzene was
added to the cell very slowly so as not to mix with the starting
materials. The diffusion was completed in 3 weeks, and small
crystals were observed on the wall of the flask: IR (Nujol, cm
-1
)
ν
CN
2185 (m), 2155 (m), 2071 (w).
The presence of isolated [C
4
(CN)
6
]
•-
was confirmed by
characteristic shifts in the ν
CN
absorptions 2185, 2155, and 2071
cm
-1
,
9
while [Gd
3+
Pc
2
]
+
was confirmed by IR spectroscopy with
a characteristic absorptions band at 1319 cm
-1
. The latter
absorption is lower than that of other cationic phthalocyanine
radicals, e.g., [Co
II
Pc
•-
]
+
(1358 cm
-1
), [Ni
II
Pc
•-
]
+
(1356 cm
-1
),
and [H
2
Pc
•
]
+
(1365 cm
-1
), but consistent with the neutral
Ln
III
(Pc
2-
)(Pc
•-
) radicals that range from 1315 to 1320 cm
-1
,
10
suggesting the presence of both Pc
2-
and Pc
•-
.
The structure of [GdPc
2
][C
4
(CN)
6
]‚2PhCl
11
consists of isolated
[GdPc
2
]
+
, [C
4
(CN)
6
]
•-
, and two PhCl solvates, Figure 1. The
Gd-N bond distances average 2.424 Å, and all the bond distances
* Author to whom correspondence should be addressed.
†
University of Utah.
‡
Osaka University.
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10.1021/ic010187a CCC: $20.00 © 2001 American Chemical Society
Published on Web 06/16/2001