Xuanchi
Yu†
ab,
Chenyu
Zhang†
c,
Dongfang
Dong
ab,
Bing
Liu
c,
Dali
Wang
*ad and
Tao
Li
*ab
aSchool of Chemistry and Chemical Engineering, Shanghai Jiao Tong University, Shanghai, 200240, China. E-mail: litao1983@sjtu.edu.cn; energywang@sjtu.edu.cn
bState Key Laboratory of Synergistic Chem-Bio Synthesis, Shanghai Key Laboratory of Electrical Insulation and Thermal Aging, Shanghai Jiao Tong University, Shanghai 200240, China
cDepartment of Oral and Maxillofacial Surgery, The First Affiliated Hospital of Harbin Medical University, Harbin 150001, China
dZhang Jiang Institute for Advanced Study, Shanghai Jiao Tong University, Shanghai 200240, China
First published on 21st July 2025
As a class of universal light-responsive units, most azo compounds require ultraviolet (UV) excitation. Most conventional π → π* redshift strategies, while enabling visible-light excitation, often compromise the thermal stability of the Z-isomer. Herein, we designed a series of ortho-substituted indoleazopyrazoles that simultaneously achieve visible-light responsiveness and exceptional thermal stability. Notably, ester substitution at the ortho position (relative to the azo group) of the indoleazopyrazole exhibits a λmax (π → π*) redshift to 383 nm while maintaining a half-life of up to 4.7 days. Following water-soluble modification, the optimized ester substitution derivative 5-photosurfactant (5-PS) demonstrates visible-light-controlled bioactivity, switching between low toxicity (E-isomer) and high toxicity (Z-isomer) in three human cancer cell lines. Remarkably, the half-maximal inhibitory concentration (IC50) of the E-isomer is approximately threefold higher than that of the Z-rich isomer in HepG2 cells. This strategy achieves the dual enhancement of π → π* redshift and half-life, opening a new avenue for visible-light-controlled targeted anticancer therapy.
Two molecular modification strategies have been employed to design visible-light photoswitches. (1) Separation of the E- and Z-isomers' n → π* absorption bands in the visible-light region. As an elegant approach to integrating visible-light responsiveness with extended half-life, this strategy has seen limited success, with notable examples including ortho-substitutions (–F,30,36 –Cl,37,38 –Br,39,40 –OMe39,41), diazocines29,42,43 and BF2-coordinated azo compounds.31,44,45 Due to inherent constraints on modification sites, the structural influence on n → π* band separation requires further evaluation. (2) Extension of π-conjugation system to lower the HOMO–LUMO gap of E-isomer and redshift the π → π* absorption band. Although this represents a more straightforward design, strategy (2) exhibits inherent drawbacks, as redshifting the λmax (π → π*) of the E-isomer typically shortens the Z-isomer's thermal half-life. For instance, the Fuchter group developed 2-arylazoimidazole with a half-life of 2.95 h, despite the π → π* absorption redshift to 385 nm.46 Similarly, the Tamaoki group reported para-methoxy-substituted phenylazothiazole with a λmax (π → π*) at 385 nm and a t1/2 of 14.8 min.34 Fused-ring incorporation has also been utilized to redshift the absorption maximum, as in the arylazobenzimidazole system, where λmax (π → π*) occurs around 380 nm.47 However, such modification drastically shortens the Z-isomers' thermal half-lives, ranging from minutes to hours. Therefore, it is crucial to design visible-light-responsive azo molecules to address the inverse correlation between the thermal t1/2 and the redshift of λmax (π → π*).
The strategic combination of heteroaryl rings can effectively mitigate this unfavorable effect. From two distinct perspectives, an electron-rich heteroaryl ring contributes to a pronounced redshift of the π → π* transition,33,34,47–50 while the presence of heteroatom-involved intramolecular interactions further stabilizes the Z-isomer, thereby increasing its thermal half-life.46,51 Our interest was to investigate indole-based photoswitches which due to their electron–rich properties extend the π-conjugated system, thereby facilitating a spectral redshift. Meanwhile, indole has been widely investigated as a key structural component in nitrogen-containing heterocyclic drug molecules.52 Therefore, indole-based photoswitches hold significant promise for visible-light-responsive photopharmacology studies. Previously, the König group reported that phenylazoindole achieved 61% E → Z isomerization in acetonitrile (MeCN) and 85% in dimethyl sulfoxide (DMSO) under irradiation at 400 nm.50 However, the Z → E transition relies on thermal relaxation due to the spectral overlap of the tail absorption bands of both isomers. To achieve efficient bidirectional isomerization under visible light while maintaining the half-life, we envisioned the incorporation of an additional heteroaryl moiety. Azopyrazole, known for its long half-life (attributed to potential intramolecular C–H⋯π interaction in the Z-isomer) and multiple twisted configurations, has been widely utilized.20,33,46,51,53 Additionally, pyrazole is frequently employed as a bioisostere to enhance potency and optimize physicochemical properties, including water solubility.52,54,55 Thus, combining pyrazole with azoindole offers the possibility of bidirectional visible-light isomerization, circumvents limitations with Z → E thermal relaxation, and enhances both the system's hydrophilicity and its potential for photopharmacological applications.
Herein, through heteroaryl incorporation and ortho modifications, we developed a series of indoleazopyrazoles as visible-light-responsive photoswitches, exhibiting excellent bidirectional isomerization efficiency and extended thermal half-lives of several days, thereby overcoming the deficiency of Z → E photoisomerization in phenylazoindole systems that rely on thermal recovery. Notably, compound 5 demonstrated excellent photoswitching properties (λmax (π → π*): 383 nm; half-life: 4.7 d; bidirectional isomerization ratio: 86.0%/96.2%), successfully achieving a dual enhancement of redshift and half-life (Scheme 1). In addition, given the favourable biological activities of indole and pyrazole rings, the water-soluble derivative 5-PS was evaluated as a potential drug scaffold for photocontrolled anticancer experiments. Interestingly, after visible-light irradiation, the Z-rich 5-PS exhibited significant cytotoxicity in the HepG2 cell line (IC50 = 46.3 ± 3.2 μM), in contrast to E-5-PS, which showed markedly lower activity (IC50 > 140.2 μM).
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Scheme 1 (a) Modification strategies for indoleazopyrazoles. (b) Correlation between λmax (π → π*) and half-life (previous work: ref. 34 – purple dots and dotted line; ref. 46 – yellow dots and dotted line; ref. 47 – green dots and dotted line). (c) Photocontrolled cytotoxicity of 5-PS to HepG2 cells (data represent three independent experiments as mean ± SD (n = 3)). |
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Fig. 1 Synthesis and chemical structures of indoleazopyrazole/indazoles 1–13 and X-ray single-crystal structures of 5; see SI for details. |
The photoswitching ability of indoleazopyrazole/indazoles was determined by UV-visible absorption spectroscopy in MeCN at 25 °C (Fig. S1–S3). E-1 and E-2 exhibited a strong π → π* band around 360 nm, while the n → π* band was observed around 400 nm as a tail of the π → π* transition. Z-1 and Z-2 exhibited significantly reduced absorption between 360 nm and 400 nm, enabling E → Z isomerization of 73.5% and 85.7%, respectively, under 400 nm irradiation (Table 1). Furthermore, both compounds achieved nearly quantitative Z → E isomerization under 549 nm irradiation. The quantum yield (QY) for E → Z isomerization (π → π* excitation) of 2 in MeCN was 0.44, substantially higher than that of azobenzene (0.10–0.15) (Fig. 2a). The π → π* absorption bands exhibited a significant redshift (∼20 nm) upon incorporation of more conjugated 5-pyrazole and indazole. However, the E → Z isomerization ratio under 400-nm irradiation remained largely unchanged, prompting the selection of compound 2 as the core structure for further study. Subsequently, we focused on modifications to the pyrazole ring. Notably, the designed ester substitution at the ortho position of the azo group resulted in a substantial redshift (∼20 nm) in λmax (π → π*) of E-5, resulting in 86.0% Z-isomer at 400PSS (Fig. 2b). Despite the significantly reduced n → π* transition intensity of Z-5 due to symmetry–forbidden transitions, 96.2% Z → E isomerization was achieved under 549 nm irradiation through weak tail absorption. Furthermore, the QYE→Z of 5 was 0.43, exceeding that of other fused-ring systems, including azobenzimidazole47 (0.22 and 0.17) and arylazoindazole49 (0.16 and 0.11).
E-isomer λmaxa | Z-isomer λmaxa | Photoisomerizationb | t 1/2 (h)c | ||
---|---|---|---|---|---|
π → π* (nm) | n → π* (nm) | E → Z (%) 400 nm | Z → E (%) 549 nm | ||
a The λmax was taken from UV-visible absorption spectra measured in MeCN. b The isomer compositions were determined by 1H NMR in CD3CN. c The half-lives were determined in DMSO at 25 °C or various temperatures. d The isomer compositions of 4 could not be accurately measured due to rapid thermal Z → E isomerization. e Irradiation wavelength: 495 nm. f The λmax was taken from UV-visible absorption spectra measured in H2O with 1.0‰ Et3N. g The isomer composition was determined by 1H NMR in D2O. h The half-life was measured in H2O with 1.0‰ Et3N at 37 °C. i The half-life was measured in DMSO at 37 °C. | |||||
1 | 365 | 442 | 73.5 | 100.0 | 15.6 |
2 | 363 | 441 | 85.7 | 100.0 | 55.3 |
3 | 381 | 460 | 81.6 | 100.0 | 3.2 |
4 | 387 | 456 | >65.9d | 100.0 | 0.5 |
5 | 383 | 433 | 86.0 | 96.2 | 112.2 |
6 | 389 | 447 | 91.1 | 98.0 | 20.5 |
7 | 365 | 440 | 81.3 | 100.0 | 14.5 |
8 | 367 | 443 | 78.5 | 96.2 | 7.4 |
9 | 370 | 444 | 87.5 | 99.0 | 14.9 |
10 | 362 | 427 | 87.1 | 96.2 | 106.9 |
11 | 394 | 429 | 94.1 | 37.0e | 204.5 |
12 | 395 | 448 | 90.8 | 79.4 | 6.8 |
13 | 352 | 426 | 65.4 | 88.5e | 206.7 |
5-PS | 371 | 440 | 73.2g | 100.0g | 6.7h (26.1i) |
We subsequently investigated the structure–property relationship by introducing an electron-donating group (–OMe) at the 4-, 5-, 6- and 7-positions of indole. Among the derivatives, only E-6 (λmax = 389 nm) exhibited a 26-nm redshift compared to E-2, along with significant broadening of both the π → π* and n → π* absorption bands (Fig. 2c). As a result, the E ↔ Z isomerization efficiency (>90%) was significantly improved under 400 nm and 549 nm irradiation. Given the substantial spectral modulation observed with 4-position substitution on indole, we further investigated electron-withdrawing group (EWG) substitutions, including –F and –NO2 (molecules 10 and 11). Compared to E-2, λmax (π → π*) of ortho-fluorinated E-10 remained largely unchanged, enabling efficient bidirectional isomerization under visible-light irradiation (E → Z400nm: 87.1%; Z → E549nm: 96.2%). With increased electron-withdrawing strength and steric hindrance, E-11 exhibited a redshifted λmax (π → π*) to 394 nm, accompanied by a reduction in n → π* absorption intensity of Z-11. Consequently, although the E → Z isomerization reached 94.1%, the reverse Z → E isomerization under 495 nm irradiation was limited to 37.0%. The effect of other ortho-substitution of the NN bond was investigated by designing derivative 12, which features an acetyl group at the 2-position of indole. Similar to compound 11, the electron-withdrawing acetyl substitution induced a redshift in λmax (π → π*) of the E-isomer to 395 nm, leading to spectral overlap with the n → π* band of Z-12. Based on previous work,56 we recognized that substitution of an EWG at the N-position of indole causes a blueshift in λmax (π → π*) of the E-isomer owing to an increased HOMO–LUMO gap. Consequently, the E → Z isomerization efficiency of E-13 under 400 nm irradiation decreased to 65.4%.
The thermal Z → E isomerization of indoleazopyrazole/indazoles was determined in DMSO and followed first-order kinetics (Fig. S21–S30 and Tables S6–S15). Z-1 exhibited a t1/2 of approximately 15.6 h, while Z-2 displayed an extended t1/2 of 55.3 h (2.3 d), attributed to the exceptional properties of the 4-pyrazole unit. With increasing conjugation (compounds 3 and 4), t1/2 decreased significantly (3.2 h and 0.5 h, respectively). Notably, the introduction of the ester substitution at the ortho position (relative to the azo group) significantly extended the thermal half-life of Z-5 to 112.2 h (4.7 d), despite a further redshift of the π → π* absorption of E-5 (Fig. 2d). Methoxy substitution (EDG) at different positions reduced the thermal stability of Z-isomers. However, introducing an EWG (–F and –NO2) at the 4-position increased the half-life of the Z-isomer by approximately two-to fourfold compared to Z-2. Ketocarbonyl substitution led to substantial variations in half-lives. The half-life decreased to 6.8 h with substitution at the 2-position of indole (Z-12), whereas substitution at the N-position of indole significantly enhanced thermal stability (Z-13:
206.7 h/8.6 d). Combined with spectral analysis, only compounds 5 and 11 exhibited a notable increase in half-life while simultaneously achieving a redshift of λmax (π → π*) (Fig. 2d).
To investigate the effect of substituent modifications on half-life enhancement, the NCI of Z-5/10, along with the minimum energy structures and the transition states (TSs) of Z-2/5/11/13 were analyzed.57,58 As shown in Fig. 3b, Z-5 exhibited a nearly T-shaped conformation, with the H atom at the 2-position of indole oriented towards the pyrazole, forming a C–H⋯π interaction. Furthermore, NCI analysis revealed that the O(sp3) of the ester group formed an attractive interaction with the nitrogen atom of the NN bond, further stabilizing Z-5. In Z-10, the fluorine atom interacted with the carbon at the 4-position of the pyrazole ring. Despite increased distortion of the T-configuration, the H atom at the 5-position of pyrazole remained attracted to the indole plane via a C–H⋯π interaction, thereby contributing to enhanced conformational stability of Z-10. To understand the thermal Z → E isomerization of 2, 5, 11 and 13, we investigated the isomerization process and demonstrated that the inversion process involves a lower energy barrier than the rotation process, indicating that it is the energetically favored pathway (Fig. 3c). Furthermore, the introduction of the ester group on the pyrazole ring induced a conformational deviation in TS-5 compared to TS-2/11/13, with the N
N bond preferentially adopting an orientation of approximately 180° relative to the pyrazole ring, possibly due to the electron-withdrawing interaction of the ester group. Theoretical free energy barriers (ΔGcalc.‡) were obtained by calculating the Gibbs free energies of Z-isomers (ΔGZ‡) and TSs (ΔGTS‡), while experimental free energy barriers (ΔGexp.‡) were determined by the Arrhenius and Eyring plots of the Z → E thermal isomerization kinetics in DMSO solution at different temperatures. Compared to 2, both ΔGcalc.‡ and ΔGexp.‡ increased for 5 (ΔGcalc.‡: 121.1 kJ mol−1vs. 122.3 kJ mol−1 and ΔGexp.‡: 104.2 kJ mol−1vs. 105.9 kJ mol−1), correlating with the observed twofold increase in the half-life of Z-5. Moreover, the ΔG‡ values were significantly higher in Z-11 and Z-13, resulting in markedly prolonged half-lives for the thermal Z → E isomerization.
Based on the experimental findings and DFT calculations, we proposed a scenario in which spectral redshift—achieved either by stabilizing the HOMO to reduce the HOMO–LUMO gap or by introducing new excitation bands (e.g., CT transition) through ortho modifications—might also enhance the thermal half-life of the Z-isomers, thereby enabling the simultaneous dual enhancement of spectral redshift and thermal half-life.
The photocontrolled anticancer potential of 5-PSin vitro was systematically evaluated against three human cancer cell lines (HepG2, MDA-MB-231 and HeLa) using MTT assays. Control experiments confirmed that neither the presence of 1‰ Et3N nor 400-nm LED irradiation alone affected cell proliferation. The E-isomer of 5-PS demonstrated mild cytotoxicity. In HepG2 cells, cytotoxic effects became apparent at an E-5-PS concentration of 60 μM. In MDA-MB-231 and HeLa cells, a gradual decrease in viability was observed only at concentrations above 100 μM, exhibiting varying IC50(E-5-PS) values: HepG2, >140.2 μM; MDA-MB-231, >500.4 μM; HeLa, >150.1 μM (Fig. 4c and S32). Conversely, the 400 nm PSS group (Z-rich isomer of 5-PS) exhibited significant antiproliferative activity. In HepG2 cells, cell survival declined significantly at 10 μM, with only ∼10% viability remaining at 100 μM. Similar trends were observed in MDA-MB-231 cells and HeLa cells, where the Z-rich isomer exhibited higher cytotoxicity even at low concentrations, with only ∼40% viability at 100 μM. These findings contrasted sharply with the dark group, in which E-5-PS exhibited negligible toxicity at concentrations below 100 μM (Fig. S32 and Tables S16–S18). The IC50 values of Z-rich isomers were generally 3- to 10-fold lower than those of E-5-PS (HepG2, ≈46.3 μM; MDA-MB-231, ≈55.6 μM; HeLa, ≈83.2 μM). At 50 μM, E-5-PS showed no significant toxicity in any of the three cell lines, whereas only ∼50% of the cells remained viable in the 400 nm PSS group (Fig. 4d). This significant light-controlled therapeutic window highlights the potential for precise spatiotemporal control of anticancer activity.
To preliminarily investigate the underlying causes of the high toxicity of the Z-isomer, we examined the aggregation behavior and reactive oxygen species (ROS) production before and after light irradiation. Transmission electron microscopy characterization revealed that 5-PS was well dispersed in solution before irradiation, whereas microspheres of various sizes formed after light exposure (Fig. S45–46). We hypothesized that the enhanced toxicity may result from the aggregates being more readily adsorbed onto cell membranes while exhibiting reduced susceptibility to metabolic degradation and elimination. Moreover, no significant ROS production was detected after irradiation (Fig. S47), thereby preliminarily ruling out ROS-mediated enhancement of cytotoxicity.
CCDC 2424490, 2424491, 2424493 and 2424494 contain the supplementary crystallographic data for this paper.61–64
Supplementary information is available and includes experimental procedures, characterization data of the compounds (NMR, MS, UV-vis, single-crystal) and computational data. See DOI: https://doi.org/10.1039/d5sc03275j.
Footnote |
† X. Yu and C. Zhang contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2025 |