Angewandte
Communications
Chemie
the CC isomer. This excitation is to a higher lying singlet state
(S7), which is dark to one-photon absorption (OPA). The two-
photon absorbing state is of mixed character, with both d-d, as
well as significant MLCT features (see Figure S8). The TPA
maximum is shifted to longer wavelengths for the higher
energy isomers.
Phosphorescence quantum efficiencies (Fem 0.069–0.097)
of the complexes in phosphate-buffered saline (PBS) were
higher under N2 than in air (0.032–0.049; see Table S7).
Phosphorescence lifetimes (t) of the excited states were much
shorter in the presence of O2 (241 ns for 1 and 59 ns for 2)
than in the absence of O2 (389 ns for 1, 109 ns for 2) in PBS
(Figure S9). These results suggest that ground-state 3O2
interacts with the triplet excited states of these complexes.
The lifetimes of 1 and 2 in living A549 human lung cancer
cells were determined to be 404 Æ 23 and 1136 Æ 72 ns,
respectively, by using confocal and phosphorescence lifetime
imaging microscopy (PLIM; Figure 1c,d). These lifetimes,
especially that of 2, are about 19 times longer than for
aqueous solutions (in air), thus suggesting that the complexes
reside in a more hydrophobic and hypoxic environment in
living cells, factors known to enhance the phosphorescence
lifetimes of photosensitizers.[12]
Figure 1. a) Structures of the complexes 1 and 2. b) Absorption and
emission spectra of 1 and 2 in PBS solution (with 2% DMSO),
lex =458 nm. c) PLIM images of living A549 lung cancer cells. d) Life-
times of 1 and 2 in living A549 cells (lex =458 nm, f=0.5 MHz).
À
tion) with Ir O bond lengths of 2.13 to 2.15 ꢀ and an O-Ir-O
twist angle of 87.188. Crystals of 1 could not be obtained, but
DFT calculations gave Ir-S bond lengths of 2.58 and 2.56 ꢀ
for the most stable CC isomer (see Table S3). In addition,
they were highly stable in the cell-culture medium (RPMI-
1640) for 48 hours (see Figure S2).
1O2 generation by 1 and 2 under l = 465 nm (blue) light
irradiation was detected by electron paramagnetic resonance
(EPR) spectroscopy using 2,2,6,6-tetramethylpiperidine
(TEMP) as a spin-trap. The characteristic triplet-of-triplets
for the 2,2,6,6-tetramethylpiperidine-1-oxyl radical was
observed under irradiation. An 1O2 signal was neither
observed in the dark nor in control samples under irradiation
(see Figure S10a). The quantum yields for 1O2 generation
[F(1O2)] by 1 and 2 upon irradiation with l = 465 nm light
were determined as 0.73 and 0.81, respectively (see Table S7).
These values are much higher than those for the well-known
[Ru(bpy)3]2+ [F(1O2) = 0.22].[1b]
The complex 2 has an MLCT absorption at longer
wavelength (l = 475 nm) than that of 1 (l = 445 nm), and
the deep-red phosphorescence of 2 (lmax = 620 nm) is shifted
to longer wavelength compared to that of 1 (lmax = 596 nm;
Figure 1b). TD-DFT calculations (Figures S3 and S4 and
Tables S5 and S6) qualitatively reproduce electronic excita-
tions for both complexes although the primary MLCT
absorption band of 2, compared to 1, is around 0.1 eV
higher, while the phosphorescence emission of 2 is around
0.15 eV higher in energy. The MLCT absorption is blue-
shifted on going from the CC to CN to NN isomers of both
1 and 2. For all three isomers, the excitation character for the
first bright MLCT state is from a d-character orbital to a p*
orbital localized on the phenylquinoline ligand (see Fig-
ure S5). All three isomers of 1 support a bound six-coordinate
triplet state (see Table S4). The stability of these triplets
follows that of the lowest singlet states: CC as the most stable,
CN 6.07 kJmolÀ1 higher, and NN 37.92 kJmolÀ1 higher.
The two-photon luminescence properties of 1 and 2 were
investigated by determining the cross-section d (see Fig-
ure S6). The dithione complex 1 exhibited a slightly stronger
To demonstrate that these IrIII complexes can produce
cellular 1O2 after irradiation with l = 465 nm light or l =
750 nm laser, 2D A549 monolayer lung cancer cells and 3D
A549 tumor spheroids were incubated with the IrIII complexes
and the fluorescence probe 2,7-dichlorodihydro-fluorescein
diacetate (DCFH-DA). Cells treated with only the DCFH-
DA control or the iridium complexes in the dark showed no
enhancement of fluorescence. In contrast, a significant
increase in fluorescence from DCFH-DA was observed
following light irradiation of the cells treated with either
1 or 2 (see Figures S10 and S11). These findings suggest that
1
1 and 2 generate O2 efficiently in cancer cells upon light
irradiation.
PDT in cell experiments was first tested by incubating
monolayer cancer cells with the compounds at various
concentrations for 2 hours. There was no loss of cell viability
after irradiation in the absence of Ir complexes (control +
irradiation; see Figure S12). In the dark, 2 was nontoxic to
both A549 lung cancer and MRC-5 normal lung fibroblasts
(IC50 > 100 mm), while 1 showed moderate toxicity to A549
cells (IC50 = 21.2 mm; see Table S8). The potency of both 1 and
2 towards cancer cells increased markedly upon irradiation,
notably sub-micromolar for A549 cells. The phototoxicity
index (PI) of 2 towards to A549 cancer cells is greater than
two-photon absorption (TPA) at l = 750 nm (d750nm
=
115 GM; 1 GM = 1 ꢁ 10À50 cm4 sÀ1 photonÀ1) relative to that
of the diketonate complex 2 (d750nm = 70 GM). The d values
are encouraging for the possible use of 1 and 2 in two-photon
photodynamic therapy, since red light penetrates more deeply
into tissues than light with shorter wavelengths.[11] The two-
photon excitation process was confirmed by its power
dependence (see Figure S7). A theoretical investigation of
TPA by 1 using a quasi-parity conserving, three-state model
indicated a very large TPA cross-section around 740 nm for
2
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Angew. Chem. Int. Ed. 2017, 56, 1 – 6
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