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Published in final edited form as: Inorg Chem. 2020 Jan 23;59(3):2083–2091. doi: 10.1021/acs.inorgchem.9b03572

Coordination-Assisted Reversible Photoswitching of Spiropyran-Based Platinum Macrocycles

Soumalya Bhattacharyya 1,, Manoranjan Maity 2,, Aniket Chowdhury 3, Manik Lal Saha 4, Sumit Kumar Panja 5, Peter J Stang 6, Partha Sarathi Mukherjee 7
PMCID: PMC10615217  NIHMSID: NIHMS1611510  PMID: 31971781

Abstract

Control over the stimuli-responsive behavior of smart molecular systems can influence their capability to execute complex functionalities. Herein, we report the development of a suite of spiropyran-based multi-stimuli-responsive self-assembled platinum(II) macrocycles (57), rendering coordination-assisted enhanced photochromism relative to the corresponding ligands. 5 showed shrinking and swelling during photoreversal, while 6 and 7 are fast and fatigue-free supramolecular photoswitches. 6 turns out to be a better fatigue-resistant photoswitch and can retain an intact photoswitching ability of up to 20 reversible cycles. The switching behavior of the macrocycles can also be precisely controlled by tuning the pH of the medium. Our present strategy for the construction of rapid stimuli-responsive supramolecular architectures via coordination-driven self-assembly represents an efficient route for the development of smart molecular switches.

Graphical Abstract

graphic file with name nihms-1611510-f0001.jpg

INTRODUCTION

Nature has a wide range of species (cephalopods, chameleons, insects, and bacteria) that reversibly change their color or structure in response to various environmental stimuli.1 These living organisms in response to a sudden change in their environment, such as light, heat, or shock, use complex mechanisms involving self-assembled biosupramolecules to accomplish the desired change in their body coloration. When such stimuli-responsive behavior is mimicked in artificial systems, sophisticated architectures with tunable functionality can be achieved.2 A wide array of external stimuli including pH,3 electrochemical potential,4 magnetic field,5 light,6 mechanical shock, and sound wave may be used to induce structural changes in smart molecules. Among them, light is of particular importance because it functions rapidly,7 and the transformations induced by light generally do not produce byproducts even after multiple cycles.8

In a molecular system, the photoresponsive units can be incorporated using various methodologies including covalent attachment, supramolecular interaction, and host–guest chemistry. The covalent attachment approach to design molecular architectures with multiple numbers of photochromic units has several disadvantages: multistep synthesis, a tedious purification process, low final yield, etc. Supramolecular self-assembly using noncovalent metal–ligand bond formation is a great alternative tool to achieve discrete systems decorated with multiple functional moieties.9 Specific numbers of desired photoactive functional groups can be appended in supramolecular coordination architectures by simply attaching suitable functional groups either to the metal acceptors or to the organic donors.10 These architectures have several positive attributes, including simple synthesis, high yield, and kinetic reversibility, that provide the chance of self-repairing the final product.11

Photoinduced reversible transformation of coordination architectures has fascinated researchers because of its precise control over structural isomers during photoirradiation.12 Most of these architectures have extensively used diarylethenes or azobenzenes as the photoactive unit.13 Nevertheless, they have been marred with several shortcomings including slow reversibility and structural fatigue, and oftentimes the change in the signal is not large enough because of the similarity of the two structural forms. Structures derived using other photochromic units, such as chromene, stilbene, and a donor–acceptor Stenhouse adduct,14 have also been characterized with the aforementioned drawbacks and exhibit poor solubility in common solvents, making their synthesis difficult. In contrast, spiropyran is an excellent photochromic unit and has found many applications in data storage,15 smart materials,16 sensors,17 light-harvesting units,18 and biological imaging,19 because of its vast difference in color and absorption profiles between the ring-opened and -closed forms20 as well as its high solubility and drastic change in polarity. Hence, supramolecular photoswitches comprising a spiropyran unit could be of importance in circumventing the aforesaid issues. Most of the spiropyran-based discrete molecular systems have a spiropyran unit in the periphery of the architecture, and they suffer from very fast photoisomerization, leading to a small lifetime of the ring-opened state.21 It is proposed that if the spyropyran moiety is incorporated directly into the backbone of the architecture, upon photoirradiation, not only can the structural change of the whole architecture be achieved but also the time taken for photoisomerization can be precisely controlled. Thus, photoirradiation will lead to a breathing supramolecular photoswitch.

Herein, we describe the synthesis of spiropyran-functionalized dipyridyl donors (1 and 2) and their use in the construction of supramolecular photoswitches (57), which show metal-coordination-assisted enhanced photochromism (Scheme 1). 6 is a durable, fatigue-free, fast photoswitch where photochromism occurs at the peripheral position, whereas the photochromic macrocycle 5 exhibits shrinking and swelling during photoreversal because of the presence of spiropyran in the backbone. To the best of our knowledge, 5 represents the first example of a discrete supramolecular architecture in which spiropyran is present in the backbone. All of the macrocycles show acidochromism because of the protonation–deprotonation equilibrium of the spiropyran unit.

Scheme 1.

Scheme 1.

Structures of the Building Blocks 1–4 Used in the Synthesis of the Macrocycles

RESULTS AND DISCUSSION

Synthesis and Characterization.

The spiropyran-functionalized dipyridyl building block 1 was synthesized by a palladium-catalyzed Suzuki cross-coupling reaction between dibromospiropyran22 (A) and 4-pyridinylboronic acid (Scheme S1). The other spiropyran-based 120° donor 2 was synthesized following the conventional Sonogashira coupling reaction of N,N-bis(4-pyridyl)-4-iodoaniline (C) with freshly prepared alkyne-functionalized spiropyran (Scheme S2).23 Donors 1 and 2 were fully characterized by multinuclear NMR and electrospray ionization mass spectrometry (ESI-MS) analyses (Figures S1-S6).

Donor 1 was reacted with a 60° organoplatinum(II) acceptor, 2,9-bis[trans-Pt(PEt3)2NO3]phenanthrene (3), in dry dichloromethane at 40 °C for 12 h, and then the solvent was concentrated to a minimum amount, which, upon treatment with cold diethyl ether, afforded pure macrocycle 5 as a precipitate. Donor 2 was separately treated with 3 in similar manner and with cis-protected (tmen)Pt(NO3)2 (4; tmen = N,N,N′,N′-tetramethylethane-1,2-diamine) in an acetone/methanol (1:1) mixture at 50 °C for 12 h, which resulted in the formation of macrocycles 6 and 7, respectively (Schemes 2 and S4-S6). The formation of a single macrocycle in both cases was confirmed by multinuclear NMR (1H, 31P, and 13C) and 2D diffusion-ordered 1H (DOSY) NMR analyses.

Scheme 2.

Scheme 2.

Self-Assembly of the Macrocycles 5–7 from Their Corresponding Building Blocks 1–4

In the 1H NMR spectrum of the macrocycle 6, one of the α-pyridine protons (Ha) exhibited a downfield shift (Δδ = 0.39 ppm) and the other one was upfield-shifted (Δδ = 0.15 ppm) compared to the free ligand (2; Figure 1). These downfield and upfield shifts were observed because of the difference in the electron density generated at the a/a′ and b/b′ positions upon coordination of the pyridine N atom to the Pt(II) metal center. Meanwhile, the singlet peak at 8.48 ppm and the other three peaks at 7.58–7.41 ppm of a 60° platinum acceptor (Figure S7) on the phenanthrene ring were downfield-shifted to a singlet at 8.66 ppm and a multiplet at 7.58–7.53 ppm, respectively. A significant downfield shift of other protons of 2 was observed because of metal–ligand complexation. A quite similar downfield shift in the α-pyridyl protons was observed for macrocycle 7 as well.

Figure 1.

Figure 1.

Stacked 1H NMR spectra of 6 (top), donor 2 (middle) in CDCl3, and 7 (bottom) in CDCl3 + CD3OD (1:1).

The 31P NMR spectrum supported the formation of one product because only a single peak was observed for both the macrocycles 5 and 6. For 6, a peak at 13.83 ppm is significantly upfield-shifted in comparison with the 60° platinum acceptor 3 (18.50 ppm). This change, as well as a decrease in the coupling of the flanking 195Pt satellites [ΔJ(Pt,P) ≈ −265 Hz], was consistent with electron back-donation from the Pt(II) ion. The macrocycle 5 also showed a similar upfield shift from 18.50 to 12.93 ppm with ΔJ(Pt,P) ≈−290 Hz (Figure 2). Single vertical traces in the 2D 1H DOSY NMR spectra for all of the three macrocycles also confirmed the formation of a single product in these complexation reactions (Figures S11, S14, and S16).

Figure 2.

Figure 2.

31P NMR spectra of acceptor 3 (b), 6 (c) in CDCl3, and 5 (a) in CD2Cl2.

Metal ligand coordination was clearly evident from the multinuclear NMR analysis, but it could not indicate the composition of the macrocycles. The stoichiometry of the building blocks and the formation of bis(spirospyran)-functionalized macrocycles (57) were established by ESI-MS analysis.

In the MS spectrum of 5, peaks corresponding to the [5 – 2NO3]2+ (m/z 1531.8307), [5 – 3NO3]3+(m/z 1000.9058), and [5 – 4NO3]4+ (m/z 734.9351) fragments were observed. For 6, the signal for the [6 – 3NO3]3+ (m/z 1077.78) fragment along with [6 – 2NO3]2+ (m/z 1647.68) was found in the spectrum. The isotopic patterns of these peaks were well resolved and matched properly with the simulated patterns (Figures 3 and S17-S22). Similarly, for 7, the m/z 592.57 and 1901.64 peaks corresponding to the [7 – 3NO3]3+ and [7 – NO3]+ fragments, respectively, were present in the MS spectrum and were in good agreement with the calculated values (Figures S21 and S22). All of these signals and their well-resolved isotopic patterns support the formation of [2 + 2] macrocycles.

Figure 3.

Figure 3.

Partial ESI-MS spectra of 5 (a) and 6 (b). Experimental isotopic patterns of their corresponding [M – 3NO3]3+ charge fragments (inset).

Single crystals suitable for X-ray diffraction could not be obtained after many attempts. To gain further insight into the structures of the macrocycles and building blocks, their geometries were optimized using the PM6 method, where ethyl groups of the phosphine ligands were modeled as H atoms. 1 has a bite angle of ~134° in the close form which reduces to ~125° in the open form. A bite angle closer to 120° supports formation of the [2 + 2] macrocyle (5). Compound 5 has an oval-shaped structure with a coplanar geometry. 6 is found to be planar with a rhomboid shape, whereas 7 has a bent structure due to the presence of the 90° platinum(II) building block (Figure 4).

Figure 4.

Figure 4.

Optimized structures of the macrocycles 5 (a), 6 (b), and 7 (c) and ring-closed (d) and ring-opened (e) isomers of donor 1. Color code: C, gray; N, blue; O, red; P, orange; Pt, dark blue. H atoms omitted for clarity.

Photochromism.

The photoisomerization behavior was investigated using 365 nm irradiation with dimethyl sulfoxide (DMSO) as the solvent. When the spiropyran transforms to its ring-opened form upon light irradiation, it becomes more polar in comparison to its ring-closed form because of the generation of charge-separated species (Scheme 3). The use of a polar solvent like DMSO can not only stabilize the more polar open structure but also increase the solubility of the complex.

Scheme 3.

Scheme 3.

Partial Schematic Representation of the Photochromism of Macrocycle 6

The photochromism was monitored by UV–vis spectroscopy. When donor 1 was exposed to light irradiation (365 and 254 nm), no color change was observed even after 15 min of exposure. Donor 2 also showed similar results (Figures S29 and S30). In contrast, the DMSO solution of 5 gave an intense blue coloration from an almost colorless solution upon irradiation for 2 min with 365 nm light. The absorbance of the band at 347 nm decreased, and a new peak was observed at 632 nm. This is attributed to the formation of an open merocyanine structure of spiropyran, which was facilitated by metal–ligand coordination. The blue solution returned to its initial state within 5 min of exposure to visible light. The peak at 632 nm vanished, and the absorption profile was like that of the initial (Figure 5a) form. In the case of 6, the absorption maximum at 328 nm was lowered, and the peak corresponding to the open form appeared at 623 nm with intense-blue coloration. The reversibility was very fast in this case; within 2 min, the blue merocyanine form changed to its initial ring-closed colorless spiropyran form (Figure 5b). Very similar photochromic behavior was observed for 7 as well, where the color change was observed in 2 min and at 621 nm an intense band appeared in the UV–vis spectrum (Figure S31a).

Figure 5.

Figure 5.

Reversible photochromic behavior of 5 (a) and 6 (b) in DMSO. λex = 365 nm and visible light.

Upon examination of the optimized structure, 5 showed shrinkage upon going from a closed form to an open form after light irradiation, and the distance between the two spiro C atoms of the opposite spiropyrans was found to decrease by 1 Å (Figure S23). This is due to the structural change of the spiropyran backbone of 1 in 5 during photoisomerization. For 5, we observed that the open form stays for 5 min, which is greater in comparison to 6 and 7. This can be attributed to the fact that the bite angle of donor 1 changes from 134° to 125° after ring opening (Figure 4). Thus, it may be assumed that more electron density can be transferred through coordination to a metal ion as the angle gets closer to 120°, making the open form more stable.

Because the macrocycles showed fast reversible photoisomerization, it was important to verify the extent of the photoswitching ability because for practical applications it is crucial to have good photoreversibility. Thus, DMSO solutions of these macrocycles were repeatedly exposed to UV and visible light, and their absorption spectra were recorded. 6 showed excellent photostability over a period of 20 cycles, with a negligible amount of lowering of the absorption intensity for the open form, whereas 5 started to degrade after 5 cycles (Figure 6). This is due to the positional difference of the spiropyran in the macrocycles. For 6, the spiropyran unit is in the periphery, and so during photoisomerization it does not disturb the geometry of the macrocycle, which avoids any sort of photofatigue. In contrast, the spiropyran unit is present in the backbone in 5, and hence the macrocycle swells and shrinks during photoisomerization, which may rupture the self-assembly after a few cycles because of variable bite angles of the closed and open forms of donor 1. 7 was found to be a good reversible photoswitch for up to 10 cycles (Figure S31b).

Figure 6.

Figure 6.

Reversible photochromic cycles of 6 (a) and 5 (b) under UV- (365 nm) and visible-light exposure.

Because of the short lifetime of the open forms, attempts to obtain NMR data were unsuccessful. Time-dependent density functional theory (TD-DFT) was performed to get a better understanding of the photochromism. For 5, the UV–vis band for the open form was found to be very close to the experimental results, suggesting that a well-controlled photoinduced transformation has been successfully achieved (Figure 7). Because the open merocyanine form is more polar as a result of charge separation, any group that can draw electron density toward itself from the spiro ring would favor photoisomerization. In the case of both donors (1 and 2), aryl moieties are attached to the spiro ring, which increases the electron density over the spiro ring and restricts photochromism. However, when it coordinates to the Pt(II) metal ions, the electron density gets transferred to the acceptor from the pyridyl rings, which is evident from the downfield shift of the pyridyl protons in 1H NMR. Thus, it escalates the ring opening, and photochromism occurs at ambient conditions upon coordination. This was also shown via electron density mapping in our previous report.24 The Pt(II) metal ion being a heavy atom can act as an intramolecular photosensitizer which also may accelerate the photoswitching.25 N-methylation of donor 2 was performed (Scheme S7) to partially reduce the electron density over the spiropyran, and its photochromism was studied (Figure S34). We did not observe any photochromism of the N-methylated pyridinium salt (8) at ambient conditions, which also strengthens the hypothesis of metal-ion-coordination-assisted photochromism.

Figure 7.

Figure 7.

Comparison of the experimental and theoretical (TD-DFT) UV–vis spectra for the photochromic behavior of 5.

The structural isomers (open form) of the photochromic macrocycles were easily converted to their original conformations (closed form) in the absence of light. To arrest the ring-opened merocyanine (MC) forms, dilute (2 N) HNO3 (a DMSO solution) was added to the DMSO solutions of the macrocycles. No change was observed in room light, but after irradiation with 365 nm UV light for 2 min, the colorless solutions became intense yellow. As soon as the spiro ring opened, the negatively charged O captured the proton from the medium and formed a protonated merocyanine (MCH+) with yellow coloration. When the proton was removed by the addition of a dilute solution of base (triethylamine), the yellow solution turned blue (MC form), and upon subsequent exposure to visible light, the initial spiro (SP) form of the molecule was regenerated (Scheme S8). This acid chromism was confirmed by a UV–vis study, which showed a new band at 447 nm for 6 upon irradiation of 365 nm light for 2 min in the presence of dilute acid. When an equivalent amount of base was added to the medium, the band for the MC form at 625 nm (6) regenerated and then vanished upon further exposure to visible light (Figure 8). In a similar way, new bands at 452 and 449 nm were observed for the MCH+ form for 5 and 7, respectively (Figures S35 and S36). The time to go back to the initial colorless form is 3 times more for 5 compared to that for 6 and 7. This also stems from the positional difference of spiropyran in the macrocycles. Because the open protonated form is stable enough, we tried to explore the 1H NMR of the merocyanine form as well. Upon treatment with dilute HNO3 and UV light (365 nm), significant displacement of the proton peaks was observed and was reversibly restored when neutralized with a base (Figure S37 and S38. Thus, these platinum(II) macrocycles are not only photoresponsive but also acidochromic.

Figure 8.

Figure 8.

Acidochromic behavior of the solution of 6 and its reversibility.

CONCLUSION

In conclusion, two spiropyran-based dipyridyl ligands (1 and 2) were employed to construct three [2 + 2] self-assembled platinum(II) macrocycles (57) in an efficient manner via the directional coordination self-assembly approach. In 1, the spiropyran unit is in the backbone, whereas in 2, the spiropyran resides on the periphery, which dictated the nature of the photochromism in the final macrocycles. Essentially nonphotochromic ligands gave rise to fast and reversible phtochromic macrocycles upon metal–ligand coordination. 5 is the first example of a discrete coordination architecture as a photoswitch where spiropyran resides in the backbone of the architecture, and it showed photoinduced structural changes during photoreversal, having efficient photoswitching ability for up to 5 cycles. On the other hand, 6 is an excellent fatigue-free supramolecular photoswitch showing efficient reversibility for up to 20 reversible cycles. 7 also showed comparable photochromic behavior, which reconfirms the idea of coordination-driven enhanced photochromism. This work fulfills the requirement of fast supramolecular photoswitches and could pave the way for the development of new smart materials.

Supplementary Material

Supporting Info

ACKNOWLEDGMENTS

P.S.M. and S.B. thank the CSIR (New Delhi, India) for financial support. M.M. and S.K.P. are grateful to Dr. D. S. Kothari and for a national postdoctoral fellowship, respectively.

Footnotes

Supporting Information

The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acs.inorgchem.9b03572.

Experimental procedures, multinuclear NMR (1H, 31P, 13C, DOSY, and COSY), MS, and UV–vis spectra, and the DFT and TD-DFT results (PDF)

Complete contact information is available at: https://pubs.acs.org/10.1021/acs.inorgchem.9b03572

The authors declare no competing financial interest.

Contributor Information

Soumalya Bhattacharyya, Department of Inorganic and Physical Chemistry, Indian Institute of Science, Bangalore 560012, India.

Manoranjan Maity, Department of Inorganic and Physical Chemistry, Indian Institute of Science, Bangalore 560012, India.

Aniket Chowdhury, Department of Inorganic and Physical Chemistry, Indian Institute of Science, Bangalore 560012, India; Department of Industrial Chemistry, Mizoram University, Aizawl 796004, India.

Manik Lal Saha, Department of Chemistry, University of Utah, Salt Lake City, Utah 84112, United States.

Sumit Kumar Panja, Department of Inorganic and Physical Chemistry, Indian Institute of Science, Bangalore 560012, India.

Peter J. Stang, Department of Chemistry, University of Utah, Salt Lake City, Utah 84112, United States.

Partha Sarathi Mukherjee, Department of Inorganic and Physical Chemistry, Indian Institute of Science, Bangalore 560012, India.

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