Somin Choa,
Youngmin You*b and
Wonwoo Nam*a
aDepartment of Chemistry and Nanoscience, Ewha Womans University, Seoul 120-750, Korea. E-mail: wwnam@ewha.ac.kr; Fax: +82-2-3277-4441; Tel: +82-2-3277-2392
bDepartment of Advanced Materials Engineering for Information and Electronics, Kyung Hee University, Yongin, Gyeonggido 446-701, Korea. E-mail: odds2@khu.ac.kr; Tel: +82-31-201-5273
First published on 28th March 2014
A dual functional molecular dyad, consisting of a cyclometalated Ir(III) complex and rhodamine B, has been synthesized and evaluated for its ability for independent operations of fluorescence staining and photodynamic therapy.
To address this challenge, we designed and synthesized a molecular dyad comprising a biscyclometalated Ir(III) complex and rhodamine B (RhB). In this dyad structure, the former sensitizes 1O2 under two-photon irradiation at 800 nm, while the latter produces strong red fluorescence under one-photon irradiation at 550 nm. Notably, the two photofunctions can be operated in a fully independent manner because the electronic spin selection rule effectively prevents the bidirectional energy transfer between the molecular entities. The unique spin-gated energy transfer has been proved by steady-state and transient photoluminescence studies. Finally, photobiological utility of the dyad has been fully evaluated in vitro. It should be noted that this is the first report on the single molecule containing an Ir(III) complex capable of independent operation of fluorescence imaging and 1O2 sensitization for potential applications in image-guided photodynamic therapy.
The dyad (Irbtp–RhB) was prepared by forming a thiourea linkage between an amine-functionalized Ir(III) complex (Irbtp)12 and rhodamine B isothiocyanate (RhB–NCS) in the presence of triethylamine (Scheme 1). Structures and purity of Irbtp–RhB and its precursors were examined by standard characterization methods, and the spectral identification data fully agreed with the proposed structure (ESI†). UV-vis absorption spectrum of a deaerated acetonitrile solution of 10 μM Irbtp–RhB is a simple superposition of the absorption spectra of the individual components of Irbtp and RhB (Fig. 1), excluding any ground-state interaction between two units. The dyad exhibits strong red fluorescence (λem = 570 nm, photoluminescence lifetime (τobs) = 1.84 ns, photoluminescence quantum yield (ΦPL) = 2.3 ± 0.2%) upon photoexcitation of the RhB moiety (λex = 490–550 nm), whereas weaker phosphorescence from Irbtp (λem = 592 nm, τobs = 1.68 μs, ΦPL = 1.2 ± 0.1%) with a characteristic vibronic progression of Δν = 1340 cm−1 is observed when the photoexcitation beam at λex = 330–450 nm is provided (Fig. 1).12,13 The photoluminescence excitation spectrum (PLE) for the 570 nm emission overlaps exclusively with the absorption band of the RhB unit (Fig. 1b), supporting that the fluorescence emission is due to selective photoexcitation of RhB. The minimal contribution of the Irbtp unit to the PLE spectrum precludes occurrence of singlet–singlet energy transfer from Irbtp to RhB. In addition, spin-restricted energy transfer from the singlet excited state of the RhB unit to the triplet state of the Irbtp unit is also ruled out, because the fluorescence lifetimes for the RhB fluorescence of Irbtp–RhB and RhB–NCS are identical (ESI, Fig. S1†).
Irbtp–RhB shows high ability for photosensitization of 1O2, with a quantum yield (Φ(1O2)) of 43% (λex = 365 nm; abs(365 nm) = 0.17; ESI, Fig. S2†). To identify the 1O2-photosensitizing moiety, Φ(1O2) values were determined with increasing the photoexcitation wavelength (λex) from 350 nm to 550 nm, using 1,3-diphenylisobenzofuran14,15 and methylene blue16 as a 1O2 trap and a reference material (Φ(1O2) = 52%), respectively. As shown in Fig. 1b, the action profile (i.e., Φ(1O2) vs. λex) matches perfectly with the singlet metal-to-ligand charge-transfer (1MLCT) absorption band of Irbtp.12 On the contrary, direct photoexcitation of the RhB moiety produces smaller quantum yields (Φ(1O2) < 9%), because the triplet state formation in RhB is possible only by triplet–triplet energy transfer from the Irbtp unit at a rate constant, kTTET = 2.2 × 105 s−1 (ESI, Fig. S1†).17,18 These results demonstrate that the photoactions of the Irbtp and RhB entities can be performed independently, while intramolecular photoinduced electron transfer from Irbtp to RhB may occur with a positive driving force of 0.56 eV to produce radical ion pair of Irbtp–RhB (i.e., Irbtp˙+–RhB˙−; ESI, Fig. S3†). This decoupling nature also affords significant photostability, as demonstrated by the ΦPL and Φ(1O2) values being unaffected by the continuous exposure to a 550 nm beam for 10 min (ESI, Fig. S4†). Taking the results into consideration, a photophysical scheme of Irbtp–RhB is summarized as Fig. 2. It is noteworthy that the unidirectionality in the energy transfer is the key feature that enables the independent actions of fluorescence and 1O2 photosensitization.
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Fig. 2 Proposed mechanism for the photophysical processes of Irbtp–RhB: ISC, intersystem crossing; SRET, spin-restricted energy transfer; TTET, triplet–triplet energy transfer. |
Having understood the photophysical mechanism, photobiological utility of Irbtp–RhB was examined. Irbtp–RhB is cell-permeable when a 10 μM stock solution in DMSO is added to the culture medium of live HeLa cells at 37 °C. The intracellular uptake of Irbtp–RhB may mainly involve passive diffusion, because incubation at 4 °C and treatments of the cells with endocytic inhibitors (50 μM chloroquine or 50 mM NH4Cl)19 and metabolic inhibitors (50 mM 2-deoxy-D-glucose + 5 μM oligomycin)20 do not alter the cellular entry (ESI, Fig. S5†). Bright punctate patterns are localized within the lysosomes of the treated HeLa cells, as seen from the fluorescence images obtained through the excitation (λex = 488 nm) and emission (λem = 551–591 nm) channels adjusted for the RhB fluorescence (Fig. 3a; see ESI, Fig. S6† for more images). Co-staining experiments with 500 nM LysoTracker Red (Molecular Probe) reveal the lysosomal staining capability of Irbtp–RhB (overlap coefficient = 0.99). In addition to the confocal laser-scanning microscopy, Irbtp–RhB is compatible with the standard set-up for fluorescence lifetime-imaging microscopy (Fig. 3b).21
Finally, photoinduced cytotoxicity by intracellular generation of 1O2 has been evaluated. HeLa cells pretreated with different concentrations (0–20 μM, 1 h at 37 °C) of Irbtp–RhB were photoirradiated using a two-photon beam at 800 nm (32 nJ, 80 MHz). The excitation wavelength corresponded to the two-photon absorption of Irbtp, although quantitative evaluations require higher precision of the measurements. Cells that were kept under dark served as controls to estimate dark cytotoxicity of Irbtp–RhB. As shown in Fig. 4a, the 800 nm photoirradiation resulted in vacuolization of the Irbtp–RhB-treated cells. In sharp contrast, neither 561 nm photoirradiation (one-photon) of the treated cells nor 800 nm excitation (two-photon) of untreated cells led to such changes. MTS assays were employed to quantitate the photoinduced cytotoxicity. As shown in Fig. 4b, the 800 nm two-photon photoexcitation significantly attenuates the cell viability value < 30% (10 μM Irbtp–RhB, 15 min photoirradiation). The efficacy of phototoxicity, estimated by the cell viability ratio of the control cells over the photoirradiated cells, reaches as high as 2.72 after 15 min photoirradiation.
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Fig. 4 Photoinduced cell death by Irbtp–RhB. (a) Changes in the cell morphology of HeLa cells under two-photon photoirradiation (80 MHz, 32 nJ) at 800 nm (left and right panels) and one-photon photoirradiation at 561 nm (middle panel). The cells in the left and middle panels were preincubated with 10 μM Irbtp–RhB. See ESI† for the movie clips showing temporal changes of the HeLa cells upon photoirradiation. (b) MTS cell viability data for HeLa cells incubated in the presence and absence of 0.1–20 μM Irbtp–RhB (1 h at 37 °C). The cells were photoirradiated for 5 and 15 min prior to the MTS assay. |
To summarize, we synthesized a molecular dyad comprising a biscyclometalated Ir(III) complex and rhodamine B, and characterized its dual functionality for fluorescence imaging and photodynamic therapy. The unidirectional energy transfer and the ability for selective photoexcitation enable independent operation of the lysosomal staining and the photosensitization of 1O2.
This work was supported by the CRI (2-2012-1794-001-1 to W.N.) and GRL (2010-00353 to W.N.) programs from the NRF of Korea and a grant from Samsung Research Funding Center for Future Technology (SRFC-MA1301-01 to Y.Y.).
Footnote |
† Electronic supplementary information (ESI) available: Experimental details and Fig. S1–S10, plotting photoluminescence decay traces after nanosecond and picosecond laser excitation, determination of Φ(1O2) values, cyclic voltammograms, photostability of ΦPL and Φ(1O2), cellular uptake, subcellular localization of Irbtp–RhB, and copies of 1H and 13C NMR spectra. See DOI: 10.1039/c4ra02354d |
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