2868
S. Salinas et al. / Polyhedron 30 (2011) 2863–2869
Fc, assigned to the oxidation of iridium (III/IV) together with a min-
or contribution from the cyclometallated phenyl fragment of bzq.
An irreversible reduction peak around ꢀ1.4 V, associated with
the reduction of the substituted bipyridine, is also observed. These
results compare well with those reported for similar compounds
[23]. Studies carried out earlier in our group [22a,22b] with an
analogous cyclometallated iridium complex, but containing a more
rigid and conjugated ligand (Scheme 2) also show irreversible oxi-
dation peaks at about 0.96 V, with the reduction of the ligands dis-
placed to ca. ꢀ1.3 V. The unsaturated bridge present in this case in
the substituted bipyridine, favors ligand reduction, due to the high-
er electronic density and delocalization on the complex.
responsible for the vibronic structure observed even at RT on the
emission spectra.
As expected, due to the saturated bridge, the emission of [C1]
and [C2] is very close in energy to that observed for the corre-
sponding bpy analogue, Table 2. In the same table, spectroscopic
data for the phenylpyridine (ppy) analogue is also reported.
The lower lifetime for [C1] and [C2] in regard to [Ir(ppy)2(bpy)]+
and [Ir(bzq)2(bpy)]+ can be understood because of an increase in
non radiative deactivation pathways in the formers, due to the free
rotating substitution on the bpy ligands. It should be mentioned
that the reported value for [Ir(bzq)2(bpy)]+ was measured in
another media than the rest of the series. Additionally, the quan-
tum yield values observed for [C1] and [C2] compare well with
the reported one for [Ir(ppy)2(bpy)]+.
3.3. UV–Vis and photophysical measurement
As a whole, the substitution on the bpy ligands does not change
considerable the energy (color) and the quantum yield of the emis-
sion, but affects the emission lifetime due to non-radiative
processes. Nevertheless, this eventual disadvantage should be
overcome by the advantage of avoiding ordering (that favors deac-
tivation of the excited state) when used in a device, justifying the
testing of these substrates in OLED devices.
The UV–Vis spectra of the cationic complexes [C1] and [C2] in
acetonitrile show three main absorption regions, at 240–270 nm,
300–350 nm and 390–480 nm, Fig. 4. Cyclometallated cationic irid-
ium complexes are reported to show an intense absorption band
about 250 nm in the UV, assigned to spin allowed (p ?
p⁄) transi-
tions on the cyclometallating ligands [2]; bands in the 300–380 nm
range are assigned to spin allowed metal–ligand charge transfer
transitions (1MLCT). Finally, the bands appearing in the proximity
of 420 nm are attributed to spin-forbidden 3MLCT transitions
[14]. It is discussed in literature [15] that this information indicates
an efficient spin–orbital coupling, which favors the emission phos-
phorescence, see below.
Acknowledgment
The financial assistance to this work by FONDECYT, through
project No. 1070799, is gratefully acknowledged.
The emission spectra of complexes [C1] and [C2] are shown in
Fig. 5. Complex [C1] emits at room temperature at kem = 554 nm,
while the maximum for complex [C2] appears at 559 nm. The kmax
values correlate well with those reported for this type of cyclomet-
allated complexes [16]. The vibronic substructure observed can be
related to a contribution of
MLCT processes, as discussed by Dragonetti et al. [17] and He et al.
[18].
References
[1] M.S. Lowry, J.L. Goldsmith, J.D. Slinker, R. Rohl, R.A. Pascal, G.G. Malliaras, S.
Bernhard, Chem. Mater. 17 (2005) 5712.
[2] R. Evans, P. Douglas, C. Winscom, Coord. Chem. Rev. 250 (2006) 2093.
[3] S. Lamansky, D. Djurovic, D. Murphy, F. Abdel-Razzaq, H. Lee, C. Adachi, P.E.
Burrows, S.R. Forrest, M.E. Thompson, J. Am. Chem. Soc. 123 (2001) 4304.
[4] J.D. Slinker, A.A. Gorodetsky, M.S. Lowry, J. Wang, S. Parker, R. Rohl, S.
Bernhard, G.G. Malliaras, J. Am. Chem. Soc. 126 (2004) 2763.
[5] G.A. Crosby, R.J. Watts, D.H.W. Carstens, Science 170 (1970) 1195.
[6] M.K. Nazeeruddin, M. Grätzel, Structure and bonding, Transition Metal
Complexes for Photovoltaic and Light Emitting Applications, vol. 123, 2007,
pp. 113–175.
p ?
p⁄ LC transitions, in addition to the
Table 2 sums up the photophysical data for the complexes
reported in this work. Quantum yields of / = 0.082 and / = 0.071,
and lifetimes of
s = 68 ns and s = 60 ns, were observed for [C1]
[7] F. De Angelis, S. Fantacci, N. Evans, C. Klein, S.M. Zakeeruddin, J. Moser, K.
Kalyanasundaram, H.J. Bolink, M. Gratzel, M. Nazeeruddin, Inorg. Chem. 46
(2007) 5989.
[8] S. Bernhard, J.A. Barron, P.L. Houston, H.D. Abruña, J.L. Ruglovksy, X. Gao, G.G.
Malliaras, J. Am. Chem. Soc. 124 (2002) 45.
and [C2], respectively. Ir (III) complexes typically exhibit high
phosphorescence quantum yields (/ = 0.1–0.9) and excited state
lifetimes in the nanosecond order [19]. The origin of the phospho-
rescence is attributed to a 3MLCT excited state, but with electron-
withdrawing ligands, which decrease the energy of the 3p p⁄
–
[9] M. Lowry, W. Hudson, R. Pascal, S. Bemhard, J. Am. Chem. Soc. 126 (2004)
14129.
states, emission may be considered to be a mixture of both MLCT
and IL [20,21]. The quantum yield for the emission of iridium com-
plexes can be modulated by introducing ligands having strong
ligand field stabilization energy [6]. It is noteworthy that the emis-
sion appears very close in position to the corresponding to
[Ir(bzq)2(bpy)]+, i.e. to the analogous complex with 2,20-bipyridine
(bpy) instead of substitued bpy, Table 2.
[10] A. Juris, S. Campagna, I. Bidd, J.M. Lehn, R. Ziessel, Inorg. Chem. 27 (1998) 4007.
[11] J. Caspar, Th Meyer, J. Am. Chem. Soc. 105 (1983) 5583.
[12] (a) R. Spencer, G. Weber, Ann. NY Acad. Sci. 158 (1969) 331.
(b) R. Spencer, G. Weber G, J. Chem. Phys. 52 (1970) 1654.
(c) E. Gratton, D. Jameson, R.D. Hall, Ann. Rev. Biophys. Bioeng. 13 (1984) 105.
(d) J.R. Alcala, E. Gratton, F.G. Prendergast, Biophys. J. 51 (1987) 587.
(e) D. Jameson, E. Gratton, R. Hall, Appl. Spectroc. Rev. 20 (1984) 55.
[13] F. Angel, B. Loeb, Inorg. Chem. Acta.; in preparation.
[14] E. Baranoff, S. Fantacci, F. De Angelis, X. Zhang, R. Scopelliti, M. Grätzel, M.K.
Nazeeruddin, Inorg. Chem. 50 (2011) 451.
[15] M. Xu, R. Zhou, G. Wang, Q. Xiao, W. Du, G. Che, Inorg. Chim. Acta 361 (2008)
2407.
[16] D.L. Davies, M.P. Lowe, K.S. Ryder, K. Singh, S. Singh, Dalton Trans. 40 (2011)
1028.
4. Conclusions
The objective of this study was to analyze the photophysical
properties of new iridium cyclometallated complexes, in order to
infer their potentiality as materials of iTMC type to be used in
OLED devices. The complexes were designed to possess a bulky
substitution on the bpy ligand, in order to avoid ordering, when
eventually used in an OLED device [8]. At the same time, the sub-
stituents were chosen to possess saturated chains, which should
‘‘disconnect’’ electronically bpy with the substituent.
[17] C. Dragonetti, L. Falciola, P. Mussini, S. Righetto, D. Roberto, R. Ugo, A. Valore,
Inorg. Chem. 46 (2007) 21.
[18] L. He, L. Duan, J. Qiao, R. Wang, P. Wei, L. Wang, Y. Qiu, Adv. Funct. Mater 18
(2008) 2123.
[19] M.K. Nazeeruddin, R. Humphrey-Baker, D. Berner, Rivier, L. Zuppiroli, M.
Graetzel, J. Am. Chem. Soc. 125 (2003) 8790.
[20] F.M. Hwang, H.Y. Chen, P.S. Chen, C.S. Liu, Y. Chi, C.F. Shu, F.L. Wu, P.T. Chou,
S.M. Peng, H. Lee, Inrog. Chem. 44 (2005) 1344.
[21] Md.K. Nazzeruddin, R. Wegh, Z. Zhou, C. Klein, Q. Wang, F. De Angelis, S.
Fantacci, M. Grätzel, Inorg. Chem. 45 (2006) 9245.
[22] (a) M. Fritzsche, S. Salinas, B. Loeb, Umpublised results.;
(b) M. Fritzsche, B. Loeb, XII Encuentro de Química Inorgánica, Página 76,
Enero, 2009, Antofagasta Chile, Unpublised results.
[23] S. Lamansky, P. Djurovich, D. Murphy, F. Abdel-Razzaq, H. Lee, C. Adachi, P.
Burrows, S. Forrest, M. Thompson, J. Am. Chem. Soc. 123 (2001) 4304.
According to literature information on similar compounds,
the substitution on the bipyridine ligands is not responsible for
the photochemical characteristics of these complexes, but rather
the cyclometallated ligand [24]. This latter ligand would also be