Yuan
Xu
ab,
Yatao
Hu
a,
Jiaping
Cao
a,
Dixin
Lin
a,
Qiqi
Zhong
a,
Yi
Wang
*a,
Hongdong
Shi
*c and
Qianling
Zhang
*a
aShenzhen Key Lab of Functional Polymer, College of Chemistry and Environmental Engineering, Shenzhen University, Shenzhen 518060, P. R. China. E-mail: zhql@szu.edu.cn
bCollege of Physics and Optoelectronic Engineering, Shenzhen University, Shenzhen, 518060, P.R. China
cYunnan Key Laboratory of Stem Cell and Regenerative Medicine, College of Rehabilitation, Kunming Medical University, Kunming, 650500, P. R. China. E-mail: shihongdong@kmmu.edu.cn
First published on 28th October 2025
To address the challenges associated with the low cellular uptake efficiency of metal-based anticancer agents and the suboptimal therapeutic efficacy of photodynamic therapy (PDT), a series of polypyridyl ruthenium(II) complexes (Ru–Cn) with tunable carbon chain lengths were rationally designed and synthesized through the incorporation of fatty acid moieties, which confer enhanced lipid solubility and membrane-targeting capabilities. Among these, the octadecanoic acid-modified ruthenium complex (Ru-C18) exhibited superior anticancer activity. Cytotoxicity assays demonstrated that Ru-C18 displayed sub-molar cytotoxic potency under light irradiation. Co-localization studies confirmed its preferential accumulation in lysosomes after cellular internalization. Upon light activation, Ru-C18 efficiently generated singlet oxygen and induced hallmark features of pyroptosis, including plasma membrane blebbing, cellular swelling, and gasdermin-dependent membrane pore formation. Consequently, Ru-C18 significantly suppressed tumor cell proliferation via activation of the pyroptotic pathway. These findings offer new insights into the rational design of highly effective and selectively targeted photodynamic anticancer agents.
Ruthenium complexes, owing to their distinctive chemical properties and favorable biological profiles, exhibit a wider therapeutic window and reduced toxicity compared to platinum-based chemotherapeutic agents.16–19 These complexes selectively target cancer cells to induce apoptosis, inhibit proliferation, and modulate the tumor microenvironment, including the enhancement of immune responses through macrophage inhibition or activation of immune cells.20,21 Critically, these agents disrupt tumor bioenergetics through concurrent targeting of mitochondrial function and oncogenic signaling pathways, thereby enhancing the efficacy of chemotherapy and demonstrating significantly improved therapeutic outcomes against drug-resistant malignancies when compared to conventional platinum-based agents.22–25
Ruthenium(II) complexes utilize their octahedral coordination geometry to function as highly promising photosensitizers in photodynamic therapy (PDT) for anticancer applications.26–29 Upon light irradiation, these complexes generate reactive oxygen species (ROS), inducing cancer cell death via apoptosis, necrosis, or pyroptosis.30–33 The structural versatility of these complexes allows for precise modulation through ligand engineering, thereby improving key properties including photosensitivity, tumor selectivity, and biocompatibility.
Notably, certain metal complexes have been demonstrated to induce gasdermin-mediated pyroptosis, a form of programmed inflammatory cell death.34,35 For instance, the rhenium(I) complex CAIX-Re represents the first light-activated pyroptosis inducer, and triggers antitumor immune responses via pyroptotic mechanisms upon light irradiation.36
Subsequent studies have further demonstrated the capacity of iridium(III), platinum(II), and related metal complexes to photodynamically induce pyroptosis.37–40 A tetrazine-conjugated ruthenium(II) complex facilitates ultrasound-triggered and tumor-selective pyroptosis through a bioorthogonal cell membrane anchoring strategy.41,42
In targeted cancer therapy employing metal complexes, ligand design plays a pivotal role in modulating biological activity. The functionalization of pyridine ligands can substantially enhance the targeting specificity and therapeutic efficacy of polypyridyl ruthenium(II) complexes.43 As the fundamental structural component of biomembrane systems, the phospholipid bilayer allows lipids to maintain membrane homeostasis while creating specialized microenvironments essential for biochemical reactions. Disruption of tumor cell membranes to induce intracellular content leakage constitutes a promising antitumor strategy. Saturated fatty acids with varying carbon chain lengths demonstrate distinct biological activities: short-chain fatty acids, such as butyric acid (C4), induce tumor cell apoptosis through epigenetic regulatory mechanisms; medium-chain fatty acids, including octanoic acid (C8) and lauric acid (C12), exert antitumor and antibacterial effects by destabilizing pathogenic lipid membrane structures; and long-chain fatty acids, such as stearic acid (C18), modulate cholesterol metabolism and aid in the elimination of toxic metal ions.44–46
Leveraging these properties, a library of amphiphilic photosensitizers was constructed by conjugating saturated fatty acids of varying chain lengths to polypyridyl ruthenium(II) complexes (Ru–Cn) (Scheme 1). The experimental results demonstrate that the cellular uptake of Ru–Cn compounds increases significantly with the elongation of the carbon chain, concomitant with a substantial enhancement in cytotoxicity. Notably, Ru-C18 displayed the highest antitumor potency, with a half-maximal inhibitory concentration (IC50) in the submicromolar range (IC50 ≈ 0.3 μM). Notably, upon irradiation at 465 nm, Ru-C18 efficiently generates singlet oxygen, which activates the caspase-1/GSDMD-mediated pyroptosis pathway, characterized by cell swelling and membrane rupture. This ultimately results in extensive tumor cell death. The strategy leverages the biocompatibility and membrane-targeting properties of fatty acids, enabling effective and low-toxicity PDT for cancer treatment, while also offering mechanistic insights into the efficient induction of tumor cell death.
The UV-vis absorption spectra are presented in Fig. 1A. All six Ru(II) complexes exhibited absorption below 325 nm, which can be attributed to the intrinsic vibrations of benzene rings and π → π* transitions within the conjugated double-bond systems. This spectral region corresponds to B-band absorption. These features are closely related to the electronic structure of aromatic rings in organic molecules, indicating that the ligands in the Ru(II) complexes maintain their characteristic aromatic nature. Notably, within the wavelength range of 325 nm to 530 nm, the Ru(II) complexes exhibited strong absorption, with a well-defined absorption maximum at 448 nm. These complexes also demonstrated prominent photophysical and photochemical properties arising from metal-to-ligand charge transfer (MLCT), wherein d-electrons from the ruthenium(II) center are transferred to the π* orbitals of the ligands, thereby facilitating efficient ROS generation upon light irradiation.
Although all complexes exhibit emission at 597 nm (Fig. 1B), Ru-C18 demonstrates significantly enhanced fluorescence intensity. This observation can be primarily attributed to the incorporation of fatty acids, which decreases complex solubility and promotes aggregation. In the aggregated state, molecular free rotation is constrained, thereby substantially suppressing non-radiative transitions and improving radiative efficiency. Additionally, aggregation enhances π–π stacking interactions among molecules, thereby further increasing the fluorescence quantum yield. Through precise modulation of the fatty acid chain length and structural architecture, the solubility and aggregation behavior of the complexes can be finely tuned to optimize fluorescence performance. Notably, although the emission wavelength of these complexes remained around 597 nm, the enhancement in fluorescence intensity was not accompanied by a significant spectral shift. These findings indicate that fatty acid modification primarily influences non-radiative transition processes with minimal impact on the distribution of excited-state energy.
The n-octanol/water partition coefficient, commonly employed as a key parameter for assessing drug hydrophobicity, allows for the calculation of concentration distribution between the two phases by measuring the absorbance of test samples in the aqueous phase against standard curves of varying concentrations. The Ru–Cn complexes exhibited partition coefficients of −1.08, −0.85, −0.79, −0.77, −0.53, and 0.39 (Fig. 1C), respectively, reflecting a gradual increase with the elongation of the carbon chain and corresponding enhancement in lipophilicity. Despite their enhanced hydrophobicity, the complexes remained stable in aqueous solutions without precipitation (Fig. 1D), thereby supporting efficient drug transport and cellular uptake. These findings suggest that extending the carbon chain length simultaneously enhances drug lipophilicity and improves dispersibility in solution, consequently promoting increased bioavailability and therapeutic efficacy.
Fluorescence quantum yields were determined using [Ru(bpy)3]2+ as a reference standard, resulting in values of 0.45, 0.68, 0.77, 0.76, 0.75, and 0.75 for Ru(II) complexes (Table S1). Time-correlated single-photon counting (TCSPC) analysis of these complexes (Fig. S13) revealed average fluorescence lifetimes (τ) of 441.11 ns, 497.94 ns, 499.52 ns, 505.96 ns, 500.50 ns, and 497.13 ns at specific wavelengths. The molecular polarity of fatty acids exerts a significant influence on the photophysical properties of ruthenium complexes. Elongation of the carbon chain decreases molecular polarity, thereby modulating the excited-state behavior of the complexes. Within the conjugated system, benzene rings facilitate electronic delocalization through π–π stacking interactions, leading to prolonged excited-state lifetimes and enhanced fluorescence efficiency. A synergistic interaction between fatty acids and benzene rings further contributes to the optimization of optical performance. All spectral data are summarized in Table S1.
Confocal microscopy revealed notable differences in the cellular uptake of the Ru(II) complexes. Under identical experimental conditions, significant variations in uptake efficiency were observed among the six Ru(II) complexes during the same incubation period (Fig. 2). In the first two experimental groups, minimal or no red fluorescence signals were detected, indicating a limited capacity for cellular internalization. For Ru-C14 and Ru-C18, red fluorescence exhibited rapid and distinct localization on the cell membrane within 1 minute, suggesting a significantly enhanced uptake efficiency. Flow cytometry further confirmed that cellular internalization increased progressively with increasing carbon chain length under consistent time and concentration conditions (Fig. S14). Moreover, the uptake of the same complex showed a positive correlation with incubation time at equivalent concentrations (Fig. S15). These findings indicate that elongation of the fatty acid carbon chain enhances drug–membrane binding interactions, thereby substantially improving cellular uptake efficiency.
Flow cytometry analysis of cellular drug uptake revealed significant differences in internalization efficiency among the six Ru(II) complexes within the same time frame. Cellular uptake efficiency was markedly reduced at 4 °C compared to that of the control group, underscoring the impact of temperature on cellular metabolic activity. Low temperature reduces membrane fluidity and protein mobility, thereby inhibiting endocytic processes. It also reduces cellular metabolic rates and diminishes energy supply, thereby collectively impairing drug uptake and transport. These factors contribute to the significantly reduced internalization efficiency observed under cold conditions. Unexpectedly, endocytosis inhibitors such as amiloride and the clathrin-mediated inhibitor chlorpromazine (CPZ) did not exert a significant inhibitory effect on cellular drug uptake across various experimental conditions. In contrast, the caveolin-mediated inhibitor methyl-β-cyclodextrin (mβCD) markedly suppressed Ru-C18 internalization, highlighting the predominant involvement of caveolin-dependent pathways (Fig. S16). These findings suggest that the cellular uptake of polypyridyl Ru(II) complexes is not only dependent on energy availability but also involves caveolin-mediated endocytic pathways.
The singlet oxygen generation capacity of Ru–Cn complexes was quantified by monitoring the fading reaction of N,N-dimethyl-4-nitrosoaniline (RNO) in the presence of L-histidine (Fig. 3). Upon excitation of the photosensitizer at specific wavelengths, molecular oxygen is converted into singlet oxygen (1O2). The histidine radical formed through the reaction between singlet oxygen and L-histidine consumes RNO in the solution, resulting in a decrease in its concentration. Changes in the UV absorbance of RNO at λ = 440 nm were monitored to quantify the amount of singlet oxygen produced. A gradual decrease in the absorbance of RNO at 440 nm was observed with increasing illumination time. Using [Ru(bpy)3]2+ as a reference standard (Φ(1O2) = 0.22), the singlet oxygen quantum yields of the ruthenium complexes were calculated, yielding values of 0.08, 0.24, 0.23, 0.22, 0.22, and 0.15, as presented in Table S2. Compared to the reference ruthenium compound, these complexes exhibited a significant enhancement in singlet oxygen quantum yield.
Fig. S17 displays the time-dependent absorbance changes of various Ru complexes over a 30-minute period, represented by distinct colored lines. These data indicate that all complexes exhibit a progressive increase in absorbance, suggesting ongoing chemical reactions or molecular interactions that influence their optical properties. Differences in reaction rates are reflected in the varying slopes of the curves. Ru-C12 and Ru-C14 display steeper slopes, indicating more rapid increases in absorbance, which may be attributed to their distinct structural or electronic features.
The fluorescent probe 2′,7′-dichlorodihydrofluorescein diacetate (DCFH-DA) functions through hydrolysis to generate the non-fluorescent compound dichlorodihydrofluorescein (DCFH), which subsequently accumulates within cells. Upon exposure to photosensitizers or reactive oxygen species (ROS) generators, DCFH undergoes oxidation to form fluorescent 2′,7′-dichlorofluorescein (DCF), which emits green fluorescence and enables quantitative detection of ROS. Under dark conditions, no significant ROS production was observed following drug internalization. Upon exposure to 465 nm light, the Ru(II) complex generated ROS, which oxidized DCFH to fluorescent dichlorofluorescein (DCF). Pronounced green fluorescence was observed in cells treated with Ru-C12, Ru-C14, and Ru-C18 under 465 nm illumination (Fig. S18), indicating significant intracellular ROS generation. Conversely, the Ru, Ru-C4, and Ru-C8 groups exhibited no detectable fluorescence. This absence can likely be attributed to low cellular uptake efficiency under short-term incubation with low drug concentrations. Although Ru-C18 generated slightly lower levels of ROS compared to Ru-C14, its extended fatty acid chain and increased lipophilicity contributed to enhanced membrane penetration.
HeLa and Hep-G2 cells were utilized to evaluate the anticancer efficacy of Ru–Cn (Fig. 4A, and Table S3). Under dark conditions, all ruthenium complexes exhibited minimal cytotoxicity against both HeLa and Hep-G2 cells (IC50 > 50 μM). However, a significant time-dependent increase in cytotoxic activity was observed upon visible light irradiation. The cytotoxic effect was notably enhanced with increasing alkyl chain length. Following 0.5 h of irradiation, the IC50 values of Ru-C12 to Ru-C18 for both cell lines decreased to sub-micromolar concentrations, ranging from 0.28 to 1.81 μM. Upon complete photoactivation for 2 h, Ru-C14 and Ru-C18, which possess long alkyl chains, demonstrated the highest cytotoxic activity among all tested complexes (Hep-G2: 0.29 ± 0.02 μM; HeLa: 0.28 ± 0.02 μM). Prolonging the irradiation time to 2 hours resulted in a 1.3- to 8.2-fold enhancement in the cytotoxic activity of each complex. Notably, Ru-C18 exhibited the most pronounced increase in cytotoxicity in Hep-G2 cells (IC50: 0.51 ± 0.04 μM at 0.5 h vs. 0.29 ± 0.02 μM at 2 h).
These results indicate that the alkyl chain structure exerts a significant influence on intracellular ROS production by modulating transmembrane efficiency, thereby enhancing cytotoxicity and demonstrating superior PDT efficacy. In subsequent co-localization experiments, the subcellular distribution of Ru-C18 was examined as a representative model. Lyso-Tracker® Green (LTG) and Mito-Tracker® Green (MTG), which are widely utilized fluorescent probes for labeling lysosomes and mitochondria, were employed. These probes specifically bind to acidic compartments and depend on the mitochondrial membrane potential to achieve accurate organelle localization. As shown in Fig. 4B, following 1 hour of incubation, a clear overlap was observed between the drug's fluorescence signal and that of the lysosomal probe, indicating specific accumulation of Ru-C18 within lysosomes. The colocalization coefficient between Ru-C18 and the lysosomal probe was determined to be 0.91, while that with the mitochondrial probe was 0.14, as quantitatively analyzed using ImageJ software.
To more intuitively illustrate the differential therapeutic effects, live/dead cell staining reagents were utilized to evaluate the treatment efficacy of six Ru(II) complexes. Calcein acetoxymethyl ester (calcein-AM) generates green fluorescence in viable cells following intracellular esterase-mediated hydrolysis, whereas propidium iodide (PI) stains cells with compromised membrane integrity, emitting red fluorescence.
Fig. S19 displays widespread green fluorescence in the Ru and Ru-C4 groups, indicating minimal therapeutic effectiveness at comparable concentrations. In contrast, the Ru-C8, Ru-C12, Ru-C14, and Ru-C18 groups exhibit pronounced red fluorescence, which suggests significant membrane disruption and structural degradation. This membrane rupture is consistent with the pyroptotic morphology, as confirmed by confocal microscopy of Hep-G2 cells treated with Ru-C18 (Fig. 5). Under continuous irradiation at a 2% confocal laser power and a wavelength of 465 nm for 30 minutes, observable changes in the cell morphology were recorded. Following the binding of the drugs to the cell membrane, bubble formation was observed on the membrane surface upon light exposure, leading to progressive cell swelling and eventual rupture, culminating in cell death. These findings suggest that light-induced swelling and pyroptosis represent the primary mechanisms through which Ru complexes exert their cytotoxic effects on cancer cells.
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| Fig. 5 Time-lapse confocal microscopy images showing morphological changes in Hep-G2 cells treated with Ru-C18 under irradiation with 465 nm light (scale bar: 10 μm). | ||
The activation of caspase-1 represents a key biochemical marker of pyroptosis and plays a central role in the canonical inflammasome signaling pathway. To evaluate intracellular caspase-1 activity, a caspase-1 activity assay kit was employed. This assay utilizes the substrate Ac-YVAD-pNA (acetyl-Tyr-Val-Ala-Asp p-nitroanilide), which is specifically cleaved by caspase-1 to release the yellow chromogenic product p-nitroaniline (pNA). The enzymatic activity of caspase-1 can be quantitatively determined by measuring the absorbance at 405 nm. As illustrated in Fig. S20, upon irradiation at 465 nm, the caspase-1 activity in HepG2 cells treated with Ru-18 was markedly elevated compared to that in the PBS control group, indicating that Ru-18 induces increased caspase-1 activation in response to light exposure. Under dark conditions, the Ru-18 treatment group exhibited negligible levels of caspase-1 activity. These findings highlight the critical role of Ru-18 in promoting caspase-1 activation under specific photonic conditions and confirm that light exposure is essential for the modulation of pyroptotic pathways through the Ru-18 complex. Furthermore, the results demonstrate that Ru-C18 effectively generates 1O2 upon excitation with 465 nm light, thereby inducing pyroptotic cell death in tumor cells.
The 1H NMR spectra were acquired using a Bruker AV-500M spectrometer, UV-visible absorption spectra using a Shimadzu UV-2600, fluorescence spectra using a JASCO FP-6500 fluorimeter, and confocal images using a Zeiss LSM 880 confocal microscope. For blue light excitation, a Beijing Princes Technology Co., Ltd PL-LED100F 465 nm-laser served as the light source.
| I = I0 × (1 − 10−Aλ) |
Under room temperature conditions, fluorescence lifetime detection was conducted using Time-Correlated Single Photon Counting (TCSPC) spectroscopy. At a specific concentration, an excitation wavelength of 465 nm and an emission wavelength of 600 nm were set with a time range of 10 μs. The decay curve of fluorescence intensity under specific wavelengths was obtained. The fluorescence lifetime of the complex was calculated by fitting, weighting and using the formula.
| R(t) = B1e(−t/τ1) + B2e(−t/τ2) + B3e(−t/τ3) + B4e(−t/τ4) |
Po/w measurementlog Ko/w = log Aoctanol/Awater |
Under similar culture conditions, different endocytosis inhibitors, including chlorpromazine (CPZ, 20 μg mL−1), amiloride (AMI, 2 mM), and methyl-β-cyclodextrin (m-β-CD, 5 mM), were used to pretreat the cells for 30 minutes. After pretreatment, Ru-C18 (25 μM) was added and the cells were incubated at 37 °C for 4 hours. One group of cells was incubated at 4 °C for 4 hours, while the control cells underwent no treatment. After the incubation, the culture medium was removed, and the cells were washed 2–3 times with PBS and HBSS, collected by trypsinase digestion, and assessed for drug uptake efficiency using a flow cytometer (BD FACS Calibur) to determine the uptake pathway under different inhibition conditions.
Hep-G2 and HeLa cells were separately seeded at 6 × 103 cells per well in a 96-well plate with a volume of 100 μL per well. The outer wells received the same volume of sterile PBS. The cells were incubated in a 37 °C, 5% CO2 incubator for 24 hours. Different drug concentrations were added using a two-fold dilution method, with 3 to 5 parallel groups for each concentration. The cells were then incubated for 0.5 h, 1 h, and 2 h, followed by dark treatment or exposure to a 465 nm light source (10 mW cm−2, 30 minutes). After overnight incubation, MTT (25 μL per well, 5 mg mL−1) was added and incubated for 2 to 4 hours. The medium was then removed, and 150 μL of DMSO was added to each well for dissolution. After shaking, the absorbance at 490 nm for each well was measured. The IC50 value was calculated using GraphPad Prism software.
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