Communications
gk = 2.30, g? = 2.07 were obtained from simulation. Using the
point dipole approximation,[9] we calculated a 4.5-ꢀ separa-
tion between the two copper(ii) atoms, a value in reasonable
agreement with the X-ray structure analysis. Complex 2 is
EPR-silent, indicating that the two copper(ii) atoms are
strongly antiferromagnetically exchange-coupled, due to
optimal magnetic orbital overlap.[5] Complex 3 exhibits a
ferromagnetic coupling between the two copper atoms similar
to that in 1 but with larger zfs parameters (D = 0.080 cmꢀ1,
E = 0.027 cmꢀ1, g1 = 2.04, g2 = 2.06, g3 = 2.12), as is expected
for a complex with a shorter intermetallic separation. (The
1
2
complex [L’(py)Cu]+ exhibits a SCu
mononuclear copper(ii) complex).
=
signal typical for a
The cyclic voltammograms of 1 (Figure 2 inset) and 2 in
CH3CN (0.1m tetrabutylammonium perchlorate (TBAP))
display a reversible one-electron wave in the positive region
of potentials (E1/2 = 0.36 V vs Fc+/Fc, DEp = 0.09 V and E1/2
0.45 V, DEp = 0.09 V for 1 and 2, respectively), attributed to
=
+
Figure 3. a) X-Band EPR spectrum of electrochemically generated 1C
(1 mm in CH3CN, 0.1m TBAP): T=4 K, modulation 0.393 mT/
the oxidation of the m-phenolato moiety into a m-phenoxyl
100 kHz, frequency 9.44 GHz, power 1 mW. Solid lines: experimental,
dotted lines: simulation. b) 115-GHz EPR spectrum 1C+ (5 mm in
CH3CN, 0.1m TBAP) at T=5 K. Solid lines: experimental, dotted lines:
simulation (parameters are given in the text).
radical.[10] This signal is irreversible both for 3 (at Ep
=
a
0.45 V) and [L’(py)Cu]+ (at Epa = 0.14 V), showing that the
radical evolves on the experiment timescale. Complexes 1–3
are thus oxidized in the same potential range, highlighting
that the structure of the complex affects weakly the oxidation
potential of the m-phenolato ligand. However, [L’(py)Cu]+ is
oxidized at a potential 0.3 V lower, which can be explained by
the lower electron density at the oxygen atom of a m-
phenolato ligand compared to that of a phenolate group. In
addition, we have previously shown that species such as 3 do
not retain their dimeric structure upon oxidation: if they are
stable enough to be generated, the phenoxyl radical species
evolve towards the corresponding monomers.[11] Thus, only 1
and 2 could be oxidized to give complexes with bridging
phenoxyl radicals.
Although the DMS = ꢁ 3 transition is weak (its intensity
decreases as the temperature increases), these results dem-
+
onstrate that 2C also exhibits a quartet ground state.
In summary, m-phenoxyl dicopper(ii) complexes in which
the two copper(ii) and the radical spins are ferromagnetically
exchange-coupled could be obtained. Their stability, and thus
their reactivity, is finely tuned by both the nuclearity of the
complex and the nature of coordinating solvent. Since tyrosyl
residues are ubiquitous in metalloenzymes, such species could
be biologically relevant. On the other hand, the chemical
reactivity of these m-phenoxyl dicopper(ii) species which
formally contain “three oxidizing equivalents” constitute a
promising and fascinating area for the studies of new chemical
properties.
+
+
The one-electron-oxidized complexes 1C and 2C exhibit
similar UV/Vis features: p–p* transitions typical of phenoxyl
radicals[12] are observed at 440 nm (3330mꢀ1 cmꢀ1) and 600 nm
+
(560mꢀ1 cmꢀ1) for 1C
(Figure 2), and at 445 nm
(4730mꢀ1 cmꢀ1)[13] and 600 nm (1000mꢀ1 cmꢀ1)[13] for 2C .
+
Received: July 28, 2004
From the decay of the former band, a half-life of 22.3 min
+
+
was obtained for 1C at 298 K, and of less than 20 s for 2C at
290 K.
Keywords: bridging ligands · copper · EPR spectroscopy ·
.
magnetic properties · radicals
The 9.4-GHz EPR spectrum of the electrochemically
+
generated 1C recorded at 4 K (Figure 3) exhibits a DMS = ꢁ 3
transition at g = 8, typical of an S = 32 spin state, whose
intensity is proportional to the reciprocal of the absolute
temperature (Tꢀ1). This quartet thus corresponds to the
ground state.[14] The zfs parameters D = ꢀ0.056 cmꢀ1 and E =
0.015 cmꢀ1 (gk = 2.142, g? = 2.039) were obtained from simu-
lation of both the 9.4-GHz and 115-GHz EPR spectra
(Figure 3). The D value is close to that reported for an
excited S = 32 spin state in a triangular tricopper(ii) complex
(ꢀ53.5 mT),[15] but significantly different from those reported
for organic triradicals (j 0.003–0.008 j cmꢀ1)[16] and mononu-
clear bis(phenoxyl) radical copper(ii) complexes (j 0.4 j
cmꢀ1).[17] The 9.4-GHz EPR spectrum of 2C+ exhibits two
[1] J. Stubbe, W. A. van der Donk, Chem. Rev. 1998, 98, 705; W.
Kaim, Dalton Trans. 2003, 761.
[2] N. Ito, S. E. V. Phillips, C. Stevens, Z. B. Ogel, M. J. McPherson,
J. N. Keen, K. D. S. Yadav, P. J. Knowles, Nature 1991, 350, 87;
J. W. Whittaker in Advances in Protein Chemistry, Vol. 60 (Eds.:
F. M. Richards, D. S. Eisenberg, J. Kuriyan), Academic Press,
Elsevier, 2002, p. 1 – 49.
[3] For reviews see: B. A. Jazdzewski, W. B. Tolman, Coord. Chem.
Rev. 2000, 200–202, 633; S. Itoh, M. Taki, S. Fukuzumi, Coord.
Chem. Rev. 2000, 198, 3; P. Chaudhuri, K. Wieghardt, Prog.
Inorg. Chem. 2001, 50, 151.
[4] Crystal
data:
for
1(ClO4ꢀ)3·0.33H2O·0.66EtOH:
C
40.33H46.67Cl3Cu2N9O15, purple–blue prisms, monoclinic, space
sets of signals, a weak DMS = ꢁ 3 transition at g = 8 and a
group P21/c, a = 21.322(2), b = 10.920(3), c = 23.131(5) ꢀ, a =
1
2
90, b = 115.41(1), g = 908, V= 4864.5(6) ꢀ3, Z = 4, D =
dominating SCu
=
signal (attributed to a degraded complex
containing noninteracting copper(ii) nuclei) at g = 2.
1.544 g.cmꢀ3
,
T= 294 K, F(000) = 2322.60, m = 1.114 mmꢀ1
,
440
ꢀ 2005 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2005, 44, 438 –441