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. 2023 May 1;14(21):5734–5742. doi: 10.1039/d2sc06939c

A cross-conjugation approach for high-performance diaryl-hemithioindigo photoswitches †

Max Zitzmann a, Frank Hampel a, Henry Dube a,✉
PMCID: PMC10231315  PMID: 37265733

Abstract

Diaryl-hemithioindigos (diaryl-HTIs) are derivatives of a novel class of highly functionalized indigoid chromophores. In this work a systematic study of the electronic effects on their photoswitching reveals the design principles for achieving an excellent property profile. Two key elements need to be invoked for perfect diaryl-HTI performance, first introduction of strong electron donors and second establishment of cross-conjugation. The resulting photoswitches combine high thermal stability, large extinction coefficients, red-light responsiveness, pronounced photochromism, and strong isomer accumulation in the photostationary states with precise geometry changes. By using the inherent basicity of their strong electron donor moiety, diaryl-HTIs can be rendered into very potent tools for molecular logic applications. We demonstrate a variety of binary logic setups as well as sophisticated three- and four-input keypad locks for sequential logic operations. Three distinct states and up to four different stimuli are invoked for this multi-level molecular information processing. Diaryl-HTIs have thus entered the stage as very capable and promising photoswitch motives for anyone interested in reversible visible- and red-light as well as multi-stimuli responsive molecular behavior.

A new class of diaryl-hemithioindigo is presented as capable reversible photoswitches with enhanced structural elaboration and stimuli-responsive behavior. Multi-state and multi-stimuli addressability enable advanced molecular logic operations.graphic file with name d2sc06939c-ga.jpg

Introduction

Molecular photoswitches are versatile tools for introducing light-responsiveness into nano-scale systems.1–3 Of particular interest are variants that can be operated with visible to red light irradiation while maximizing geometric or electronic changes.4,5 In this regard double bond isomerization is oftentimes used for large geometrical changes and electrocyclization reactions for strong electronic changes. In a few photoswitch motives, both aspects can be combined, for example, in spiropyrans,6–8 Stenhouse dyes,9,10 or the recently discovered hemithioindigo (HTI)-TOND motive.11 Photoinduced double bond isomerization has been utilized for a long time with, e.g., stilbene12–14 and azobenzene chromophores,15 however additional substitutions are needed to shift their absorptions to the visible part of the spectrum.16–22 Indigoid chromophores have gained traction as intrinsically visible light responsive photoswitches for double bond isomerization reactions.23–26 From the different variants such as indigo,27–29 indirubin,30 or thioindigo,31 hemiindigo,32,33 and especially hemithioindigo25 (HTI, see also ref. 34–36 for some recent HTI-photoswitch examples) stand out as especially versatile core structures. HTI-based photoswitches consist of a central isomerizable double bond, which connects a benzothiophenone (a half- or hemithioindigo) fragment to one aromatic residue typically termed the stilbene fragment (Fig. 1a). Since one hydrogen atom remains at the double bond it is threefold substituted in the core chromophore structure. HTIs were employed early on in the photopharmacological or chemical biology context24,37–40 and found their way into supramolecular chemistry,41–44 molecular machine building,45–53 or molecular logic systems.54 However, particularly steep progress has been made since facile fourfold double-bond substitution became synthetically available.55,56 In particular, the combination of sp3-based (alkyl or ether) and aryl-based groups at the stilbene fragment side enabled the discovery of new types of thermal- and photoreactions,11 evidencing the long-debated hula-twist mechanism,57 generating new types of molecular motors,47,48 or establishing the first photogearing process.52

Fig. 1. Diaryl-HTI as a highly functionalized photoswitch motive in comparison to the parent threefold double-bond substituted HTI. (a) The core chromophore of HTI contains a threefold substituted double bond. (b) Diaryl-HTIs contain a fourfold substituted double-bond with two geminal aromatic residues at the stilbene fragment side. Cross-conjugation involving donor/acceptor pairs offers very potent photoswitching properties in combination with well-controlled geometry changes and overall higher degree of functionalization.

Fig. 1

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A different possibility is the introduction of two geminal aromatic residues at the stilbene fragment side. This substitution has already shown unique potential for multi-state switching and discovery of yet another unknown photoreaction, the dual single bond rotation (DSBR).58 In the eight-fold sequential switching, photoisomerization and thermal isomerization steps alternate while reversible photoswitching remains to be explored. In this work, we scrutinize the feasibility of reversible photoswitching for diaryl-HTI chromophores using a cross-conjugation approach to optimize the whole property profile. With this approach we achieve strongly red-shifted absorptions enabling red-light responsiveness, pronounced photochromism, high isomer enrichment in the photostationary states (PSS), good quantum yields for both switching processes, and high thermal bistability. These very favorable properties render diaryl-HTIs into particularly promising new photoswitch scaffolds for advanced applications, and we demonstrate a number of molecular logic operations as an example. To this end, the intrinsic basicity of the cross-conjugated and electron-rich aniline group is used to invoke acid/base responsiveness. Thus, another level of chemical stimuli is added and multi-stimuli switching allows the construction of diaryl-HTI based molecular logic operators.

Results and discussion

We investigated 10 different derivatives of diaryl-HTI photoswitches 1–10 bearing combinations of donor, acceptor, or rather neutral substituents at the aromatic para-positions (for all molecular structures investigated see Fig. 2). A systematic approach is followed in which all possible combinations of donor and acceptor substituents are scrutinized. Two different thioindigo-fragments are invoked in this study, one unsubstituted one and a pyridine-variant with the heterocyclic nitrogen next to the sulfur atom. The latter was used to scrutinize the effect of electron deficiency at the thioindigo fragment on the photoswitching properties.

Fig. 2. Diaryl-HTIs 1–10 investigated in this study. (a) Schematic depiction of all structures, only one isomer is shown in each case for clarity; (b) structures of 1, Z-3, 5, E/Z-7, and Z-8 in the crystalline state.

Fig. 2

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Synthesis of diaryl-HTIs follows an established protocol reported earlier by our group (see the Synthesis section of the ESI† for details).56 Starting from commercially available thiosalicylic acids 11 and 12 a substitution reaction with α-bromo-ketones gives the corresponding substituted thioethers 13–16. Basic ring closure leading to ketones 17–20 was followed by subsequent chlorination to yield the chloro-HTI precursor molecules 21–24. The latter can be cross-coupled with aryl-boronic acids to introduce the second aryl residue at the stilbene fragment side of the central double bond. Crystals suitable for X-ray structural analysis were obtained for diaryl-HTI derivatives 1, Z-3, 5, E/Z-7, and Z-8 and for precursor compound 15 (see the ESI† for details on the latter). For derivative 7, both the E and the Z isomer are co-crystallizing and thus allow both isomeric forms to be structurally characterized in detail. The structures in the crystalline state of Z-3 and Z-8 also allowed us to directly assign the corresponding solution spectra to the specific double bond configuration. For derivatives 2, 3, 4, 7, 8, and 9 the double bond configuration in solution was elucidated using NOE-cross-signals in the corresponding NMR spectra (see Fig. S41–S46 in the ESI†).

The thermal behavior of diaryl-HTI derivatives 2–4 and 7–9 was investigated first to establish the relative stability of Z and E isomers as well as the kinetics of thermal isomerization of the metastable states in the dark (see Fig. 3a and the Thermal double bond isomerization section in the ESI†). All derivatives exhibit a greater stability for the Z-configured isomer with the exception of diaryl-HTI 4, for which the E isomer is more stable. The observed stability preference can be well explained by the general trend in which the more electron rich aryl substituent of the diaryl fragment is favored in a trans-relationship to the electron accepting carbonyl function of the thioindigo fragment. This stabilization is most pronounced in the strongest push–pull systems, i.e., diaryl-HTIs 3 and 8, where additionally a matching favorable trans-relationship of the electron-poor aryl substituent of the diaryl fragment to the electron donating sulfur of the thioindigo fragment is present.

Fig. 3. (a) Experimentally determined ΔG‡ values for the thermal double bond isomerization of diaryl-HTIs 2, 3, 7 and 8 in toluene and DMSO solution. (b) Excerpts of the aromatic region of 1H-NMR spectra of HTI 2 after irradiation with different wavelengths (E isomer highlighted in red and Z isomer highlighted in blue). (c) Excerpts of the aromatic region of 1H-NMR spectra of HTI 3 after irradiation with different wavelengths (E isomer highlighted in red and Z isomer highlighted in blue). (d) Molar extinction coefficients of diaryl-HTI 7 in toluene in the PSS measured after irradiation with different wavelengths (best performance for enrichment of the Z isomer at 617 nm (dark blue line) and for the E isomer at 450 nm (light blue line)) and observed color change. (e) Molar extinction coefficients of diaryl-HTI 8 in toluene in the PSS measured after irradiation with different wavelengths (best performance for enrichment of the Z isomer at 617 nm (dark blue line) and for the E isomer at 470 nm (light blue line)) and observed color change.

Fig. 3

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In general, all derivatives show sizable Gibbs free energies of activation ΔG‡ for the thermal double bond isomerizations, giving rise to corresponding half-lives of the metastable states in the several hours to years range at ambient temperatures (Fig. 3e). The kinetics vary by about four orders in magnitude in terms of rate or by 5.5 kcal mol−1 in terms of ΔG‡ (Table 1). The fastest isomerization is seen for diaryl-HTI 7, giving rise to several hours persistence of the metastable state in solution. The highest barrier and thus slowest isomerization is observed for diaryl-HTI 2 with up to several years persistence of the metastable state. No clear trend is seen with respect to the particular electronic nature of the diaryl substituents. However, noticeably smaller ΔG‡ values are obtained for pyridine-thioindigo variants 7, 8, and 9 as compared to 2, 3, and 4. Interestingly, solvent polarity dependence in this series is typically opposite to the parent HTI derivatives with higher ΔG‡ values observed in the more polar solvent DMSO. Scrutiny of the thermal behavior of diaryl-HTIs 2–4 and 7–9 thus establishes favorable slow kinetics for the spontaneous thermal double bond isomerization in the dark, guaranteeing full photocontrol over their switching on a convenient time scale of hours (pyridine-thioindigo derivatives 7, 8, and 9) to years (diaryl 2, 3, and 4).

Quantified properties of diaryl-HTIs 1–10.

Diaryl-HTI ΔGE→Z‡ [kcal mol−1] ΔG [kcal mol−1] (at T) t eq. 23 °C d Isomer % in PSS (at LED nm) λ max [nm] and εmax [L mol−1 cm−1] of Z/E isomers' lowest energy absorption band Δλmax [nm] and Δεmax [L mol−1 cm−1] of E and Z isomers Φ Z to E/ΦE to Z
1 — — — — 509; 14 200a —
526; 16 800b
2 25.7a 0.2 (50 °C)a 12 da 76% E (450 nm)a 473; 19 300a 45; 4200a 3%a
96% Z (617 nm)a 518; 15 100a
28.3b 0.3 (100 °C)b 3 ab 75% E (470 nm)b 490; 22 900b 48; 8800b 11%a
97% Z (617 nm)b 538; 14 100b
3 23.2a 1.0 (40 °C)a 4 ha 75% E (450 nm)a 496; 21 100a 27; 7700a 3%a
97% Z (617 nm)a 523; 13 400a
27.7b 1.6 (90 °C)b 1 ab 77% E (470 nm)b 493; 21 800b 46; 6000b 3%a
96% Z (617 nm)b 539; 15 800b
4 27.8b 0.5 (90 °C)b 1 ab 49% Z (490 nm)c 444; 6300c 6; 580c 11%c
69% E (420 nm)c 438; 6800c
55% Z (490 nm)b 447; 5600b 7; 940b 6%c
64% E (420 nm)b 440; 6600b
5 — — — — 440; 5200a —
440; 5600b
6 — — — — 517; 14 800a —
486; 16 800b
7 23.9a 0.3 (40 °C)a 14 ha 75% E (450 nm)a 480; 20 800a 45; 7800a 6%a
97% Z (617 nm)a 525; 13 000a
22.8b 0.3 (30 °C)b 2 hb 79% E (470 nm)b 496; 21 200b 49; 6600b 5%a
94% Z (617 nm)b 545; 14 600b
8 24.0a 0.9 (30 °C)a 16 ha 83% E (470 nm)a 486; 21 100a 46; 7300a 4%a
98% Z (625 nm)a 532; 13 800a
24.5b 0.9 (40 °C)b 38 hb 78% E (470 nm)b 499; 20 400b 56; 7600b 4%a
96% Z (650 nm)b 555; 12 800b
9 25.6b 0.4 (60 °C)b 16 db 49% E (490 nm)a 426; 4700a 0; 1180a 5%a
71% Z (435 nm)a 426; 5800a
52% E (505 nm)b 424; 5100b 0; 1290b 3%a
69% Z (420 nm)b 424; 6400b
10 — — — — 426; 4900a —
422; 4500b
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a

In toluene-d8.

b

In DMSO-d6.

c

In benzene-d6.

d

Linearly extrapolated to 23 °C.

The photochemical and photophysical properties of all diaryl-HTIs in the series 1–10 were quantified subsequently (see Fig. 3b–e and 4 for selected examples and the UV/Vis spectroscopic measurements, NMR irradiation experiments, and Quantum yield determination sections in the ESI† for more details). For reasons of simplicity, we refer to hypsochromic and bathochromic species in the following instead of Z and E isomers, as the former allows working out more precisely the structure-related trends. Hypsochromic species possess a trans-relationship of the thioindigo-fragments' carbonyl to the most electron-rich aromatic residue of the diaryl fragment, while the bathochromic species possess a corresponding cis-relationship.

Fig. 4. (a) Comparison of molar extinction coefficients of diaryl-HTIs 1–5 (solid line: Z isomers, dashed line: E isomers); (b) comparison of molar extinction coefficients of diaryl-HTIs 6–10 (solid line: Z isomers, dashed line: E isomers); (c) comparison of molar extinction coefficients of diaryl-HTIs 2 and 3 with their pyridine substituted counterparts 7 and 8 (solid line: Z isomers, dashed line: E isomers); (d) solvatochromism of diaryl-HTIs 3 and 8 in toluene and DMSO (solid line: Z isomers in toluene solution, dashed line: Z isomers in DMSO solution, dotted line: E isomers in toluene solution, short dotted line: E isomers in DMSO solution).

Fig. 4

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Molar extinction coefficients show pronounced absorption in the visible region of the electromagnetic spectrum for all derivatives ranging from 5000 M−1 cm−1 to 22 000 M−1 cm−1 (Fig. 4). Extinction coefficients are largest for dimethyl-aniline substituted variants. The combination of cross-conjugated donor–acceptor pairs gives rise to the most red-shifted absorptions, and non-symmetrically substituted diaryl-HTIs 3 and 8 exhibit absorptions beyond 650 nm for the bathochromic species. When comparing the influence of systematic electronic variations in the series, a consistent behavior is observed. The most hypsochromic absorption and rather low extinction coefficients are present in twofold acceptor substituted diaryl-HTIs 5 and 10, followed by slightly more redshifted derivatives 4 and 9 (see Fig. 4a and b). Substitution by dimethyl-aniline gives rise to significant redshifted absorptions and much stronger extinction coefficients as seen for diaryl-HTIs 2 and 7. The former is an accumulative effect as seen in the further redshifted absorptions of twofold dimethyl-aniline substituted diaryl-HTIs 1 and 6. Cross-conjugation of a strong donor–acceptor combination in diaryl-HTIs 3 and 8 leads to the largest achievable absorption redshift in the series, however not by a large margin (Fig. 4a–c). The effect of nitrogen-substitution at the thioindigo-fragment is also small as derivatives of the series 1–5 show essentially the same absorptions as their counterparts in the series 6–10 with the latter being a bit more redshifted (Fig. 4a–c).

Solvatochromism is absent for all derivatives lacking a dimethyl-aniline substituent, i.e., diaryl-HTIs 4, 5, 9, and 10 (Fig. 4d). The presence of a dimethyl-aniline substituent gives rise to pronounced solvatochromism with absorption red-shifts up to 20 nm in more polar DMSO as compared to toluene solutions. Again, a slightly larger solvatochromism and thus the largest effect overall is observed for cross-conjugated derivatives 3 and 8.

Strong photochromism is observed for diaryl-HTIs 2, 3, 7, and 8, with maxima differences between the hypsochromic and the bathochromic species reaching beyond 50 nm (Fig. 3c, d and 4c). As described above, the hypsochromic species bear the most electron rich aromatic residue of the diaryl fragment in a trans-relationship to the carbonyl function of the thioindigo fragment. Correspondingly, the bathochromic species shows a cis-relationship between these groups. This behavior is consistent with the parent HTIs, where the single aromatic substituent of the stilbene fragment serves the role of the most electron rich substituent. Because of their pronounced photochromism, photoswitching of diaryl-HTIs 2, 3, 7, and 8 is very effective. Isomer enrichment up to 83% of the bathochromic species as well as up to 98% of the hypsochromic species in the photostationary state (PSS) is possible using blue and red-light irradiation, respectively (see Fig. 3b–e, Table 1 and the ESI†). The polarity of the solvent (e.g., toluene versus DMSO) does not influence the proficient photoisomerization strongly, which establishes robust operation of diaryl-HTIs under different conditions.

Quantum yield measurements of diaryl-HTIs 2–4 and 7–9 established good photoisomerization efficiencies in both switching directions with values ranging from 3% up to 11% (see Table 1 and the Quantum yield determination section in the ESI†). Only small effects of nitrogen-substitution at the thioindigo-fragment are seen, which somewhat improve the Z to E photoisomerization and diminish the E to Z photoisomerization. All quantum yields measured are in the mid-range of measured quantum yields for HTI photoswitches and are sizable enough to allow for timely isomer conversions even under lower light conditions. It has to be mentioned at this point that fourfold double bond substitution in HTI photoswitches typically leads to significantly diminished quantum yields as compared to the parent threefold-double bond substituted variants.47,48,57,58 Additionally, quantum yields for Z to E and E to Z photoisomerizations are oftentimes very different, which hampers proper isomer accumulation in the PSS in many cases. For diaryl-HTI derivatives, both Z to E and E to Z photoisomerization reactions possess comparable quantum yields, which enable high isomer accumulation in the PSS with similar pacing because of their substantial photochromism.

A theoretical description of diaryl-HTIs 3 and 8 was undertaken to elucidate the character of the photoinduced electronic transition (see the Theoretical description section in the ESI†). In both cases this is essentially a π–π* transition at the central double bond as judged by the molecular orbitals shown in Fig. S39 and S40 in the ESI.† Theory also correctly predicts more stable Z isomers with absolute energy differences in good agreement with the experimental ΔGE–Z values obtained at elevated temperatures (theoretical values are ΔGE–Z(3) = 1.1 kcal mol−1 and ΔGE–Z(8) = 1.4 kcal mol−1 and experimental ones are ΔGE–Z(3) = 1.0 kcal mol−1 at 40 °C and ΔGE–Z(8) = 0.9 kcal mol−1 at 30 °C).

In order to demonstrate the value of the expanded structural space, functionality, and high-performance of diaryl-HTI photoswitches we explored an application that makes direct use of their defining characteristics. To this end we use the basicity of the electron-rich aniline moiety, which is needed for proper photoswitching, to introduce two more independent chemical stimuli, i.e., acid and base. Upon protonation of either isomer of diaryl-HTI 3 with trifluoroacetic acid (TFA) a third state, the protonated Z isomer Z-3H+, is obtained with a distinct absorption spectrum (Fig. 5a and b). At the same time photoisomerization of Z-3H+ is prohibited, which establishes acid-gating of the photoswitching property. Upon addition of triethylamine (TEA) unprotonated 3 is recovered and photoswitching is enabled again rendering the three-state/four-stimuli switching process between Z-3, E-3, and Z-3H+ fully reversible. Since the absorptions of the three states are significantly different, an advanced molecular logic system (see ref. 59–61 for examples of earlier molecular logic systems based on photoswitches) can be setup with diaryl-HTI 3. By thresholding absorption intensity at different wavelengths as output signals, a variety of binary logic gates such as AND, SAND, NOT, or Identity, as well as a binary multiplier can be constructed (see Fig. 5c–e, for specific examples and the Molecular logic application section of the ESI† for more details). In addition, application of diaryl-HTI 3 as a molecular sequential logic system is possible with a heightened level of selectivity. A three-input system (input A = TFA addition, input B = TEA addition, input C = 470 nm light) with one true input combination (one out of six possible, i.e. ABC) as well as a system with two true input combinations (two out of six, i.e. ACB and CAB) can be setup as shown in the Molecular logic application section of the ESI.† A more sophisticated four-input system can also be established with diaryl-HTI 3, which offers a heightened level of performance as the sequence of four different inputs (input A = TFA addition, input B = TEA addition, input C = 470 nm light, and input D = 617 nm light) is distinguished with three true input combinations (ABDC, ADBC, and DABC) out of 24 possible (Fig. 5f). With these applications diaryl-HTIs already show their potential as versatile multi-responsive molecular building blocks offering a range of optimal switching properties within a functionally expanded structure.

Fig. 5. (a) Schematic representation of the multi-stimuli responsiveness of diaryl-HTI 3 towards 470 nm and 617 nm light as well as acid and base addition. Protonation with TFA (2000 equiv.) leads to the protonated Z isomer (Z-3H+) and subsequent deprotonation with TEA (2000 equiv.) to Z-3; (b) UV/Vis absorption spectra of Z-3, E-3, and Z-3H+ in toluene solution with indicated output readouts at 580 nm, 500 nm, 480 nm, and 328 nm (vertical dashed lines) and threshold limits (horizontal solid black lines); (c) truth table for four two-bit logic gates (NOR, SAND, NOT, and Identity) using TFA (2000 equiv.) and 617 nm light as orthogonal inputs; (d) experimental absorption outputs at 580 nm for a NOR gate (threshold level shown as horizonal dashed lines) starting from E-3; (e) experimental absorption outputs at 500 nm for a NOT gate (threshold level shown as horizonal dashed line) starting from E-3; (f) experimental absorption outputs at 580 nm for a keypad lock with three true outputs (threshold level shown as horizonal dashed line) starting from Z-3H+ and using four different inputs (TFA (input A), TEA (input B), 470 nm light (input C), and 617 nm light (input D)).

Fig. 5

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Conclusion

In summary, a systematic study of diaryl-HTI photoswitching is presented optimizing the photochemical responses for these structurally expanded and visible-light responsive chromophores. It is revealed that the implementation of strong electron donation is key for achieving very good performance. Introduction of an additional pronounced cross-conjugation allows further improvement of the properties resulting in highly capable photoswitches responsive to blue and red-light irradiation. The introduction of a nitrogen atom within the thioindigo fragment does not lead to deterioration of this favorable behavior. As a result, the high thermal stability of metastable states across different solvent polarities is combined with efficient photoswitching, pronounced photochromism, and high isomer enrichment in the photostationary states. Acid and base can be used as further chemical stimuli to reversibly access a third protonated state of diaryl-HTI 3 with distinct spectral characteristics. Upon protonation photoisomerization capability is stalled, which establishes reversible acid gating of the photoresponse as well as multi-state and multi-stimuli responsiveness. The use of diaryl-HTIs in different molecular logic systems directly showcases the enabling effects of the diaryl-substitution for advanced switching applications. A variety of binary logic as well as sequential logic operations can be realized with these new chromophores, including expanded keypad locks that distinguish the sequences of up to four different inputs. Diaryl-HTIs are therefore very promising and highly functionalized multi-responsive photoswitches offering multi-addressability in combination with an outstanding property profile.

Data availability

All relevant data have been included in ESI.† Crystal structural data have been deposited at the CCDC https://www.ccdc.cam.ac.uk. All original data underlying this work are available from the corresponding author upon request.

Author contributions

M. Z. and H. D. conceived the study. M. Z. conducted the synthesis, full analysis including quantifying photochemical and photophysical properties, quantum chemical calculations, and molecular logic application experiments, F. H. provided X-ray analysis of the structures in the crystalline state, H. D. coordinated the study, helped in the analysis, and wrote the manuscript. All authors discussed and commented on the manuscript.

Conflicts of interest

The authors declare no conflict of interest.

Supplementary Material

SC-014-D2SC06939C-s001
SC-014-D2SC06939C-s002
SC-014-D2SC06939C-s003

Acknowledgments

H. Dube thanks the Deutsche Forschungsgemeinschaft (DFG) for an Emmy Noether fellowship (DU 1414/1-2). This project has also received funding from the European Research Council (ERC) under the European Union's Horizon 2020 research and innovation programme (PHOTOMECH, grant agreement no. 101001794).

†

Electronic supplementary information (ESI) available. CCDC 2227014–2227018 and 2227451. For ESI and crystallographic data in CIF or other electronic format see DOI: https://doi.org/10.1039/d2sc06939c

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

SC-014-D2SC06939C-s001
SC-014-D2SC06939C-s001.xlsx (84.2KB, xlsx)
SC-014-D2SC06939C-s002
SC-014-D2SC06939C-s002.pdf (10.5MB, pdf)
SC-014-D2SC06939C-s003
SC-014-D2SC06939C-s003.cif (1.4MB, cif)

Data Availability Statement

All relevant data have been included in ESI.† Crystal structural data have been deposited at the CCDC https://www.ccdc.cam.ac.uk. All original data underlying this work are available from the corresponding author upon request.

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