524
M. Canlıca et al. / Polyhedron 30 (2011) 522–528
(CHCl3) kmax/nm (log
e
/dmꢀ3 molꢀ1 cmꢀ1): 664 (4.67), 325 (4.73).
and 325 nm for 6 and 7, respectively. Typical of ball-type phthalo-
cyanines, the intensity of the B-bands is high relative to the Q-band
when compared to the monomer, and this may be due to intramo-
lecular interactions between the Pc rings [30]. For example a CoPc
tetra substituted at the non-peripheral positions with 3,4-(methyl-
IR (KBr) (m
max/cmꢀ1): 3054 (ArACH), 1579 (C@C), 1245 (CAOAC).
Anal. Calc. for C164H88N16O8Co2: C, 77.90; H, 3.51; N, 8.86%. Found:
C, 78.57; H, 3.10; N, 9.03%. MALDI-TOF-MS m/z Calc.: 2528.42.
Found: [M+H2O]+: 2546.51, [Mꢀ11H]+: 2517.6.
endioxy)-phenoxy substituents gave a log
e value for the Q-band of
5.39 compared to 4.75 for the B-band [31], whereas complex 7
3. Results and discussion
shows a log
e value of 4.67 for the Q-band compared to 4.73 for
the B band.
3.1. Syntheses and characterization
The aggregation behavior of a Pc is depicted as a coplanar asso-
ciation of rings, progressing from the monomer to a dimer and to
higher order complexes, which are dependent on concentration,
the nature of the solvent and substituents, metal ions and temper-
ature [32]. Aggregation in MPcs is typified by broadened or split Q-
band, with the high energy band being due to the aggregate and
the low energy band due to the monomer. As expected for ball-
type structures, complexes 6 and 7 have broad spectra [12–
25,33]. A band near 620 nm in ball-type phthalocyanines has been
associated with exciton coupling between the two Pc rings [33]. A
strong intermolecular interaction between the Pc rings in ball-type
Pc complexes is expected to result in a splitting of the molecular
orbitals and hence a lowering of the symmetry, resulting in the
splitting of the Q-band. The spectra of complexes 6 and 7 in chlo-
roform shows bands in the 600 nm region, which could be a com-
bination of vibronic bands and the band due to exciton coupling
between the two rings. There is no clear splitting in the Q-band
of both complexes, suggesting that the interactions are not very
strong. The broadening is larger for 7, showing more intermolecu-
lar interactions and possibly aggregation. The peripherally substi-
tuted complex 7 is expected to show more aggregation than the
non-peripherally substituted complex 6 [28].
The substituted phthalonitriles were synthesized according to
the synthetic route shown in Scheme 1. New binuclear, ball-type
Co(II)Pcs (6 and 7) were prepared by the reaction of compound 4
or 5 with CoCl2. The structure and purity of the CoPc derivatives
were confirmed by UV–Vis, IR, mass spectroscopies and elemental
analyses. Complexes 6 and 7 are soluble in DMSO, THF and CHCl3,
and are partially soluble in most other organic solvents.
The IR spectra of 6 and 7 show no C„N vibrational peak (2233
or 2232 cmꢀ1) which was observed in the IR spectra of compounds
4 and 5. This confirms the formation of the desired CoPc deriva-
tives. The remaining IR spectra are very similar for compounds
4–7. The IR spectra of 4–7 showed ArAOAAr vibrational band
bands between 1235 and 1255 cmꢀ1. The 1H NMR spectrum of 5
shows a characteristic sharp singlet at 7.79 ppm, which is assigned
to the peripherally positioned proton on the CNAArAH moiety. In
both 1H NMR spectra of 4 and 5 the total number of protons inte-
grates to 22.
Elemental analysis results are also consistent with the proposed
structures of 4–7. The purified ball-type phthalocyanines were fur-
ther characterized by mass spectra. The deprotonated molecular
ion peaks were observed at m/z 2523.0 (for 6) and 2546.51 and
2517.6 (for 7), which concur with the theoretical calculated molec-
ular ions (See Supplementary materials, Fig. 1). These results con-
firm that the complexes have been synthesized successfully.
The UV–Vis spectra of 6 and 7 in CHCl3 are in accordance with
the trend found in the literature, Fig. 1. The phthalocyanines show
typical electronic spectra with two main absorption bands in the
UV region (320–350 nm, the B-bands) and the visible region
(600–700 nm, the Q-band). The characteristic Q-band transition
of metallophthalocyanines with D4h symmetry is observed as a sin-
gle band of high intensity in the visible region. Complexes 6 and 7
have Q-band absorption maxima at 688 and 664 nm in chloroform,
3.2. Voltammetric studies
The electrochemistry of ball-type phthalocyanine complexes
containing electroactive central metals is characterized by the for-
mation of mixed valance species [12]. Multi-electron processes are
known in the cyclic voltammetry of these complexes. The observa-
tion of one-electron processes in homo-dinuclear ball-type MPc
complexes is attributed to a strong interaction between the rings,
resulting in the splitting of the cyclic voltammetry peaks and the
formation of mixed redox processes. The transfer of two electrons
in each redox step suggests that there is no considerable interac-
tion between the two Pc rings, and that the two rings are reduced
and oxidized at the same potentials.
Complex 6 (Fig. 2) exhibited five redox processes, which are not
reversible in some cases. The lack of reversibility of redox couples
is typical behavior of ball-type MPc complexes and has been asso-
ciated with interactions between the Co2Pc2 units [12,34]. The
reported electrochemistry of ball-type phthalocyanines is charac-
terized by weak and often irreversible cyclic voltammograms
[12,25]. The cyclic voltammograms observed in Figs. 2 and 3 are
typical [12,25] of ball-type phthalocyanines.
respectively, as is shown in Fig. 1. It is well known that
a substitu-
tion results in red shifting of the spectra in MPcs [28,29], this is due
to the electron density enhancement caused by the substitution at
the non-peripheral position. The B-bands were observed at 323
5
4
Redox couple III in Fig. 2 is reversible, with a peak to peak sep-
aration (DE) of 80 mV (DE = 85 mV for ferrocene standard). Pro-
3
6
cesses I, I0, II and IV are not clearly reversible. The reversibility or
relative intensities of the peaks could not be improved by changing
the scanning direction or using a narrow potential window. Process
II is only clearly observed on the square wave voltammogram at
ꢀ0.46 V, Table 1, whereas process I is irreversible and is not ob-
served on the square wave voltammogram, Fig. 2b, this is due to
the extreme sensitivity of this technique to the reversibility of a
couple and the chemical stability of the redox products. Using
the known redox behavior of monomers and ball-type CoPc com-
plexes, where the first reduction occurs on the central metal, pro-
cess II is assigned to (CoIIPcꢀ2)2/[(CoIPcꢀ2)2]2ꢀ. The assignment is
2
1
0
7
320
420
520
620
720
Wavelength / nm
Fig. 1. Absorption spectra of complexes 6 and 7 (4 ꢁ 10ꢀ5 mol dmꢀ3) in CHCl3.