F. Thomas et al.
Scheme 2. Possible formulations for the chelated and two-electron oxi-
ꢀ
dized bis(di-tert-butyl-phenol)–dipyrrin ligand: (a) closed shell, M–L
and (b) diradical, M–LDꢀ.
Figure 3. Vis/NIR spectra of 1 (solid lines) and 1+ (dotted lines) in
CH2Cl2 solution. T=298 K. Insert: b-HOMO!b-LUMO transition
which contributes to the NIR band of 1 (lclcd =1270 nm, f=0.072). Pre-
dicted transitions are shown by vertical bars (1, black bars; 1+, grey
bars).
Notably, the monoanionic ligand in 1+ may exist as either a
diradical, LDꢀ, or as a closed shell, Loxꢀ (Scheme 2). Although
the crystal structure supports both forms, the DFT-based en-
ergetic analysis of 1+ predicts that the closed-shell singlet
state (S=0) is approximately 12 kcalmolꢀ1 lower in energy
than the triplet state (S=1). Broken-symmetry optimiza-
tions for 1+ collapsed to a singlet state in all cases, suggest-
ing that the closed-shell form, Loxꢀ, form is lower in energy
than the antiferromagnetically coupled diradical state, LDꢀ.
The structure of 2+ (Figure 1) contrasts sharply with the
previously described compounds because the metal ion
exists in a square pyramidal geometry containing an axially
are thus assigned as ligand-to-ligand charge-transfer (LLCT)
transitions. A TD-DFT calculation on 2 (triplet state) pre-
dicts a low-energy transition at 940 nm, which is in good
agreement with the broad experimental feature at approxi-
mately 1000 nm. The low-energy transition for 2 involves or-
bitals delocalized over the ligand-radical framework with a
small Co contribution (see the Supporting Information, Fig-
ure S14).
ꢀ
The cyclic-voltammetry curves of 1 and 2 in CH2Cl2 (with
coordinated water molecule with a Co O3 bond distance of
1
0.1m TBAP) display a reversible reduction wave at E1/2
=
2.252 ꢂ. The discrimination between a (+2) and (+3) oxi-
dation level of the Co ion is therefore not possible solely on
the basis of the geometry at the metal center. Further ex-
amination of the bond lengths within the ligand framework
ꢀ0.48 and ꢀ0.61 versus Fc/Fc+, respectively; this wave is as-
signed to the L 2ꢀ/L3ꢀ redox couple. The potentials required
C
for the formation of the ligand radical in 1 and 2 are thus
much lower in comparison to M2+–(di-tert-butyl-salen), M2+
–TPP, and M2+–OEP complexes.[4,5,13,14] This result could be
rationalized by considering the additional negative charge of
the deprotonated bis(di-tert-butyl-phenol)–dipyrrin ligand
(ꢀ3 instead of ꢀ2 in its initial nonradical form), which coun-
teracts the electron deficiency common to oxidized radical
complexes. When scanning towards positive potentials a re-
versible one-electron redox process is observed at E1/22 = +
0.03 V versus Fc/Fc+ for 1, whereas two reversible waves
are observed for 2 at E1/22 =ꢀ0.01 V and E1/23 = +0.58 V.
The former is attributed to a second ligand-centered redox
process, as demonstrated below.[17]
shows an overall distribution very similar to the one ob-
+
ꢀ
ꢀ
served for 1 , although the C1 O1 and C20 O2 bond
lengths (1.285 and 1.297 ꢂ, respectively) are intermediate
between those of 2 and 1+. The EPR spectrum of 2+ at
100 K displays a major anisotropic (S=1= ) signal at gk =
2
2.005 and g? =2.258 with cobalt hyperfine structure
(Ak(Co) =10.4 mT and A?(Co) =2.0 mT), which is comparable
to other Co2+ complexes involving a closed-shell ligand.[18,19]
In agreement with the experimental data, DFT calculations
ꢀ
of 2+ predict that the singlet state (S=1/2) of Co2+–Lox is
lower in energy by approximately 11 kcalmolꢀ1.
The Vis/NIR spectra are dominated by intense transitions
at 432 (18480), 760 (16050), and 904 nm (10540 Mꢀ1cmꢀ1)
for 1+ (Figure 3), and 508 (13 750) and 864 nm
(17410 Mꢀ1cmꢀ1) for 2+. In both cases the UV/Vis bands
shift to higher energy upon oxidation to the cations 1+ and
2+. TD-DFT calculations on the closed-shell singlet state
(S=0) for 1+ predicts three bands in the 600–950 nm range,
thus matching the experiment data, in which there was a
shift to higher energy upon oxidation (Figure 3). The pre-
dicted transitions are assigned as delocalized LLCT bands
(see the Supporting Information, Figure S13). TD-DFT cal-
culations on the oxidized 5-coordinate Co complex, Co2+
The cations 1+ and 2+ were generated chemically by oxi-
dation with AgSbF6 (E8=0.65 V) in CH2Cl2 and crystallized
by slow diffusion of pentane into the solution. The metal ion
exists in a square-planar geometry in 1+, similar to 1, sug-
gesting that the Ni atom remains in the +2 oxidation state,
and indicating that the ligand is two-electron oxidized.
ꢀ
ꢀ
ꢀ
When comparing the C C, C N, and C O bond lengths of
1+ with the corresponding values measured for 1, a trend
similar to that obtained on going from the nonoxidized L3ꢀ
derivatives[10,11] to 1 is observed. The C1 O1, C20 O2, C2
ꢀ
ꢀ
ꢀ
ꢀ
ꢀ
ꢀ
C5, C21 C34, C17 C17, and C36 C37 bonds have thus a
more marked double-bond character. In addition, the bond
lengths within the rings of each half of the ligand are very
similar, thus showing that the ligand is highly conjugated.
ꢀ
–Lox (2+), also predicts three bands in the 600–950 nm
range. The predicted bands for 2+ are similar to those pre-
dicted for 1+, thus providing further evidence that the
14592
ꢁ 2012 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Eur. J. 2012, 18, 14590 – 14593