In consideration of the octahedral coordination mode of transition metals such as Fe and Zn, the self-assembly of the linear BODIPY-based ligand with these metals always led to the formation of tetrahedral cages through subcomponent self-assembly. The BODIPY-based ligands were prepared from the modification of BODIPY fluorophores with amino groups or 2-formaldehyde pyridines at the β positions and the subsequent self-assembly of the BODIPY-based ligands with other subcomponents and metal ions led to formation of metallacages with high yields. The fluorescence of the metallacages were red-shifted compared to the classic BODIPY fluorophore and the photosensitization property of the metallacages was alternative. In addition, the multi-fluorophore interactions also played an important role in the photophysical/chemical properties of the metallacages.

In 2014, Nitschke and co-workers reported the first BODIPY-based tetrahedral cages and investigated their photophysical properties [63]. Treatment of BODIPY-functionalized diamine ligand 1 with 2 or 3 and metal ions (Fe²⁺ and Zn²⁺) afforded tetrahedral cage 4, 5, and 6 (Fig. 1a), respectively. The cages were well characterized with NMR and mass spectrometry. It should be noted that the NMR spectra of 4-6 were complex due to the presence of stereoisomers. Molecular simulations indicated that 4-6 adopted a classic tetrahedral conformation [64] and that the mesityl groups of BODIPY were randomly pointed in any direction (into the cavities or out of the cavities), which increased the structural complexity of the cages (Fig. 1b). In addition, the formation of cages showed a great influence on absorption and emission by the chromophore. Compared to BODIPY-containing ligand 1, all cages 4-6 exhibited blue-shifted absorptions (approximately 70–100 nm) and recovered fluorescence with fluorescence quantum yields of 0.012, 0.015 and 0.055, respectively. Moreover, the emission of the pyrene subunit of 5 was quenched upon cage formation. Furthermore, the host-guest properties of 4-6 were studied with anionic guests. The combined results from spectrographic data and NMR data revealed that cages 4-6 exhibited strong binding affinity with acetate and azide and moderate binding affinity with fluoride and chloride, whereas they did not respond to bromide, iodide, nitrate, hexafluorophosphate, triflate, perchlorate or tetrafluoroborate. Upon addition of acetate into a solution of cage 4, the absorption maximum was changed from 555 nm to 606 nm (Fig. 1c), and this accompanied by generation of four isosbestic points at 588, 464, 268 and 252 nm. The fluorescence intensity of 4 at 653 nm also showed a 25-fold increase (Fig. 1d). Thus, by taking advantage of this dual-mode recognition, a test-paper strip test was designed. It showed good response to certain anions, and it could be used for anion detection in aqueous media (Fig. 1e). Further experiments indicated that anion recognition was probably due to partial disassembly of cages, and the electrostatic and anion-π interactions between the host and guests also made a great difference. In addition, the cages showed low binding affinity with polycyclic aromatic hydrocarbons (PAHs), such as perylene, naphthalene, and anthracene (Fig. 1f). Considering the multichromophoric character of the host-guest complex (perylene, pyrene and BODIPY as blue, green and red emitters, respectively), white light emission was realized with a fluorescence quantum yield of 0.11 and CIE coordinates of (0.30, 0.36) by fine-tuning the proportion of the guest perylene (Fig. 1g). Moreover, the cages could also be employed as reaction-based sensors for amino acid recognition. The addition of amino acids such as cysteine led to changes in the absorption band as well as the quenching of BODIPY fluorescence, which resulted from amine exchange between the amino acid and the BODIPY-containing ligand (Fig. 1h). The proposed mechanism is that a transient complex [4.amino acid] with more brilliant fluorescence was formed upon the addition of amino acid initially and the subsequent formation of the amino-acid-based mononuclear complexes with almost no fluorescence due to ligand exchange (Fig. 1i). In conclusion, a series of BODIPY-based tetrahedral cages with multiple functionalities were prepared in this work, which laid the foundation for construction of fluorescent SCCs for various applications.

Since BODIPY is a good photosensitizer with excellent capacity for singlet oxygen (¹O₂) generation, Nitschke et al. reported the synthesis of a series of BODIPY-based tetrahedral cages and studied their autocatalytic character through photooxidation-driven ligand exchange [65]. BODIPY-containing cages 13-17 were readily obtained from the reaction of bis(formylpyridyl)-functionalized BODIPY-containing ligand 7 with various diamines 8-12 in CH₃CN (Fig. 2a). After the cages were well characterized with NMR and mass spectrometry, their ¹O₂ generation ability was investigated with the ¹O₂ indicator 1, 3-diphenylisobenzofuran (DPBF) (Fig. 2b). The quantum yields of singlet oxygen generation of 13-15 and 17 are 0.01-0.02 and 0.045, respectively. The relatively high ¹O₂ generation capability of 17 was ascribed to enhanced intersystem crossing (ISC) resulting from the presence of the heavy atom iodine. Moreover, the methylthio groups of cage 15 were oxidized to sulfoxides by ¹O₂ to produce cage 16. In addition, due to the dynamic nature of subcomponent self-assembly, amine exchange occurred through addition of extra diamine, and previous studies revealed that it was easier for electron-rich ligands to displace electron-deficient ligands [66]. Moreover, the Hammett parameters of 8-12 were 0.50, -0.27, 0.0, 0.49 and 0.18, respectively (the more electron-poor aniline showed the larger Hammett parameters) [67]. Therefore, addition of amine ligand 12 into cage 15 led to the rapid release of amine 10 initially due to ligand exchange (Fig. 2c), which was calculated from integration of the NMR spectrum. Then, the release rate gradually declined because equilibrium was reached. However, after an induction period, a large increase in the proportion of 10 released was observed, which was ascribed to ligand exchange between 12 and photooxidation-generated amine ligand 11. Owing to the more electron-deficient character of sulfoxides 11, the incorporation of ligand 12 into the cage occurred more rapidly as the photoreaction proceeded, subsequently resulting in enhanced ¹O₂ generation. Thus, an autocatalytic system based on photooxidation-driven ligand exchange was successfully constructed (Fig. 2d). A control experiment was also conducted, and the results revealed that no second exponential rise was observed in the absence of O₂ and light. Subsequent exposure to O₂ and light also led to a rapid increase in the rate for release of 10, further confirming its autocatalytic character. This research successfully realized the construction of an autocatalytic system based on photooxidation-driven ligand exchange within BODIPY-based tetrahedral cages, which is of great significance for designing artificial supramolecular systems to understand the complexity of nature.

Investigations of excited-state photophysics have played an important role in designing optical materials for artificial photosynthesis and solar energy conversion. In 2017, Nitschke and coworkers synthesized a series of homoleptic and heteroleptic BODIPY-containing cages and studied their excited-state photophysics in depth [68]. The homoleptic BODIPY-containing cages 23 and 24 were readily obtained by a similar method to cage 4. Heteroleptic cages 25 and 26 were prepared through a reaction of diamine 21, diamine 22, 2-formylpyridine and the metal ion (Fe²⁺ or Zn²⁺) in a 3:3:12:4 ratio (Fig. 3a), and NMR and ESI-MS results showed that all seven possible cages were distributed statistically in the mixture. Due to partial disassembly of the cages at low concentrations, the ligands and cages were embedded in a polymer matrix (polymethyl methacrylate, PMMA) to form films for further photophysical studies. The absorption spectra for cages 23 and 24 exhibited narrow and blue-shifted absorption peaks compared to their diamine ligands 21 and 22 (Fig. 3b), respectively, due to suppression of charge-transfer character upon cage formation. In particular, the absorption spectrum of 23 showed a long wavelength tail, probably due to formation of "dim" coupled states with head-to-tail couple interactions, and the higher-energy peak corresponded to "bright" couple states with maximum numbers of head-to-head couple interactions. For cage 24, variation between the "bright" and "dim" states was not distinct due to the disturbedtransition dipole moments resulting from the presence of bulky TIPS groups. In addition, cages 23 and 24 showed almost no emission (QY < 10⁻⁴), which differed from the typical BODIPY chromophore. Transient grating photoluminescence spectroscopy measurements indicated that the fluorescence quenching of the cages was probably attributable to excited-state interchromophore coupling, leading to formation of dark states from bright states. Furthermore, transient absorption (TA) spectroscopy was performed to investigate their photophysics, and the results indicated that the excited states could be classified into three species (Figs. 3c–f). Species I was present from the initial state through a 250 fs lifetime and was indicated primarily by a ground-state bleaching (GSB) peak. Subsequent fast conversion from species I to species II was probably due to conformational flexibility of the cage framework, which led to the dramatic decrease in the peak at 515 nm. Species III, which was derived from the change in the balance of GSB and first-derivative features, showed the longest lifetime, and the conversion from species II to species III was inferred to come from structural changes in the cage geometry. The combined results from transient grating photoluminescence spectroscopy and transient absorption (TA) spectroscopy indicated that dipole frustration of the bright state was dominant and a nonemissive state was subsequently formed (Fig. 3g), which was consistent with the results from the absorption and fluorescence spectra. For the heteroleptic cages 25 and 26, TA spectroscopy was not consistent with a simple combination of cage 23 and cage 24, suggesting that strong chromophore coupling existed in the ground state. In addition, the effect of chromophore coupling was slightly weaker for 26 than for 25, revealing that partial through-bond interactions also participated in excitation energy delocalization. It should be noted that the BODIPY-based cages exhibited distinctive chromophore coupling, which differed substantially from the perylene-based cages reported by Frischmann et al. [69,70], and the small size (3 nm) of the cages played the most important role. Furthermore, the host-guest properties of the cages were investigated, and the results indicated that the cages could bind C₆₀ or C₇₀ with negligible changes in their absorption spectra. TA spectroscopy for the host-guest complexes was significantly different from that of the empty cages (Fig. 4). For example, photoinduced absorption (PIA) beyond 650 nm was observed over hundreds of picoseconds for the host-guest complex, probably due to charge transfer between the cage and C₆₀ or C₇₀, and the charge transfer process depended largely on the pump wavelength. In conclusion, BODIPY-based cages exhibiting excitation energy localization and transfer to guests were successfully constructed, and this will provide guidance for the design of fluorescent supramolecular systems for optical applications.

As for the planar coordination mode of Pt and Pd as well as the development maturity of Pt or Pd-based SCCs, the M_nL_2n-type BODIPY-based cages was readily obtained via Pt or Pd coordination. The BODIPY-based ligands were prepared from the modification of BODIPY fluorophores with pyridines at the β positions or the meso position. Then the ligands were self-assemblied with Pt or Pd metals, affording the BODIPY-based metallacages with structural complexity. In addition, owing to that the BODIPY fluorophores were usually attached to the peripheries of cages, the photophysical/chemical properties of the metallacages were generally similar to the ligands.

In comparison to monocomponent supramolecular cages, multicomponent emissive cages can combine different fluorescent chromophores into one system, which often exhibit unique properties and functions. In 2017, Zhang et al. reported the syntheses of multicomponent emissive Pt(II) cages based on the chromophores of BODIPY and tetraphenylethene (TPE) [71]. Addition of the TPE-functionalized carboxylate ligand 27, 90° Pt(II) acceptors 31 and dipyridyl ligands 28–30 in a 1:4:2 ratio in acetone/H₂O provided cages 32–34, respectively (Fig. 5a), with yields of more than 90%. All cages were well characterized by NMR spectroscopy, ESI-TOF-MS, UV–visible and fluorescence spectroscopy. The results from molecular stimulations revealed that the cages adopted tetragonal prismatic conformations and the TPE subunits, dipyridyl ligands and 90° Pt(II) acceptors were employed as the faces, pillars, and corners, respectively (Figs. 5b–d). Further spectroscopic experiments indicated that 32 and 33 exhibited main absorption peaks at 282 nm and 318 nm in CH₂Cl₂, respectively, and strong fluorescence at 493 nm, which was attributed to emission from TPE groups. For cage 34, a sharp absorption band at 520 nm was observed in addition to the two broad absorptions at 278 and 319 nm, which were absorptions by BODIPY groups. The fluorescence of 34 also showed two peaks at 472 and 544 nm due to the presence of two different chromophores, TPE and BODIPY. In addition, the fluorescence quantum yields of 32–34 were 0.25, 0.2 and 0.13 in DMSO, respectively, suggesting that the dipyridyl ligands exerted a great influence on the photophysical properties of the cages through coordination-induced emission of TPE subunits. Moreover, the fluorescence quantum yields of the cages varied largely with the solvent (0.02 and 0.13 for 34 in CH₂Cl₂ and DMSO, respectively). Furthermore, the application of cage 33 as a "turn-on" sensor for amino acids was explored. Upon addition of thiol-containing amino acids such as glutathione and cysteine, the fluorescence intensity of 33 showed a remarkable increase at 500 nm and was almost proportional to the concentration of the amino acid (0−80 µmol/L). In addition, the detection limits were very low (0.189 and 0.278 µmol/L for glutathione and cysteine, respectively), and 33 showed no response to other amino acids, indicating that 33 may serve as a good fluorescent sensor for thiol-containing amino acids (Fig. 5e). The combined NMR and mass spectral results revealed the self-destructive mechanism of amino acid sensing, and the cage could be recovered upon addition of 90° Pt(II) acceptors, further confirming the stimuli-responsive properties of the multicomponent emissive cages.

As a result of the simple planar coordination mode for Pd as well as the developmental maturity of Pd-based SCCs, a variety of Pd-based SCCs, especially M_nL_2n-type supramolecules, have been constructed in the past few decades and have displayed wide-ranging applications in host-guest chemistry and catalysis. In 2018, Lützen and Käseborn et al. reported the synthesis of a rotaxane-like Pd₆L₁₂ metallosupramolecular architecture with structural complexity based on the BODIPY chromophore [72]. BODIPY-containing ligand 38 was readily prepared in four steps (Fig. 6a). By reacting ligand 38 with [Pd(CH₃CN)₄](BF₄)₂ in a molar ratio of 2:1 in acetonitrile-d₃/dichloromethane-d₂ (5:1), an unexpected feature was observed in its NMR spectrum in which the pyridine resonances were split into three sets of signals, suggesting structural complexity. Even though the ESI-MS spectrum indicated exclusive formation of a Pd₆L₁₂ supramolecular assembly, the combined ¹H NMR, ¹⁹F NMR and 2D NMR results revealed that the complex obtained was not like previously reported Pd₆L₁₂ supramolecular architectures. Furthermore, a single crystal of the complex was grown in DMF/benzene, and X-ray diffraction results indicated that complex 39 adopted a rotaxane-like cage-in-ring arrangement (Figs. 6b and c). The giant complex consisted of two parts, a typical Pd₂L₄ cage with a Pd–Pd distance of 23.6 Å and a crown-like Pd₄L₈ macrocycle with neighbouring Pd–Pd distances of 27.9 and 28.0 Å. For the cage-like Pd₂L₄ part of the complex, the ligands exhibited a C-shaped conformation in which the BODIPY moieties and the long alkoxy chains were pointed outwards and inwards from the cage, respectively. In the macrocyclic Pd₄L₈ part of the complex, the ligands adopted a W-shaped conformation, and the BODIPY moieties and the long alkoxy chains were pointed inwards and outwards from the complex, respectively, completely unlike those in the Pd₂L₄ part. Therefore, a distinctive rotaxane-like complex 39 was formed, and the BODIPY-containing ligands in the complex were mechanically interpenetrated without being catenated. One ligand with a different conformation in one entity was uncommon in previously reported SCCs, and this arrangement led to significant π-stacking interactions between the BODIPY moieties and ligand skeletons, which further enhanced the stability of the complex. In addition, the NMR and MS experiments indicated extremely fast formation of the Pd₆L₁₂ complex (within 5–10 min), which also suggested the excellent stability of the complex. Furthermore, spectroscopic experiments were conducted, and the results revealed that the absorption spectra of the ligands showed negligible changes upon coordination, while the fluorescence was partially quenched. This research provided successful construction of a rotaxane-like Pd₆L₁₂ metallosupramolecular architecture with structural complexity resulting from π-stacking interactions between the BODIPY-containing ligands, offering the possibility of constructing more complex and sophisticated SCCs through weak interactions such as π-π and van der Waals interactions.

Construction of fluorescent SCCs with high fluorescence quantum yields is still challenging because of fluorescence quenching resulting from the "heavy-atom effect". In 2019, Casini and coworkers reported the construction of a series of highly emissive BODIPY-based supramolecular cages and investigated their utility in cell imaging [73]. Treatment of BODIPY-functionalized dipyridyl ligands 40 or 41 with [Pd(CH₃CN)₄](BF₄)₂ or Pd(NO₃)₂ in DMSO at room temperature afforded BODIPY-containing cages 42 and 43, respectively (the counter anions were different due to the Pd precursors) (Fig. 7a). The cages were well characterized with NMR and mass spectrometry. Spectroscopic experiments indicated that the cages showed two main absorption bands at 290 and 520 nm with relatively high fluorescence quantum yields of 0.5–0.7. Notably, the amide and azido group linkers reduced the conjugation between the BODIPY chromophore and the Pd metal and enabled efficient emission from the cages. Furthermore, the stabilities of the cages in biological systems were studied, and the results from UV–visible absorption spectra showed that all cages were completely stable in water, whereas 42·BF and 42·NO showed moderate stability for 24 h in PBS buffer. However, the absorption intensity for cage 43·NO showed a large decrease in PBS buffer, suggesting instability resulting from poor solubility in physiological media. In addition, NMR titration results indicated that 42·BF and 42·NO disassembled into ligands upon addition of physiologically relevant concentrations of glutathione. Moreover, the slight downfield shifts of ¹H NMR signals corresponding to the pyridines and the upfield shifts for ¹⁹⁵Pt NMR signals upon addition of cisplatin both proved efficient encapsulation of 2 equiv. of cisplatin into the cages 42·BF and 42·NO. Furthermore, the antiproliferative effects of the cages were studied (Fig. 7b), and cage 42 showed no toxicity against human A375 cells and an EC50 of more than 50 mmol/L; however, host-guest complexes of the cages with cisplatin exhibited antiproliferative effects similar to those of cisplatin. Using the highly emissive character of the BODIPY-containing cages, uptake and cellular localization studies of the cages were conducted with confocal fluorescence microscopy imaging. The results indicated that the 42·BF and 42·NO cages mainly accumulated in intracellular vesicles. In addition, the cells showed no uptake of the cages at low temperature (4 ℃), demonstrating that energy-independent endocytic transport was the main pathway for cell uptake.