Xenon binding has attracted interest due to the potential for xenon separation and emerging applications in magnetic resonance imaging. Compared to their covalent counterparts, assembled hosts that are able to effectively bind xenon are rare. Here, we report a tight yet soft chiral macrocycle dimeric capsule for efficient and adaptive xenon binding in both crystal form and solution. The chiral bisurea-bisthiourea macrocycle can be easily synthesized in multi-gram scale. Through assembly, the flexible macrocycles are locked in a bowl-shaped conformation and buckled to each other, wrapping up a tight, completely sealed yet adjustable cavity suitable for xenon, with a very high affinity for an assembled host. A slow-exchange process and drastic spectral changes are observed in both 1H and 129Xe NMR. With the easy synthesis, modification and reversible characteristics, we believe the robust yet adaptive assembly system may find applications in xenon sequestration and magnetic resonance imaging-based biosensing.
Xenon is a hydrophobic, highly polarizable but rather inert gas. The 129Xe isotope (natural abundance of 26.4%) has a spin of I = 1/2 and its NMR parameters including chemical shift and exchange kinetics are very sensitive to surrounding environments. Meanwhile, application of hyperpolarization (hp) technique can increase the signal by more than 104-fold, thus allowing for very sensitive detection1,2. Consequently, xenon has long been used as an inert probe to determine cavity environments of porous materials and organisms such as proteins3,4,5,6. Promise has also been shown for xenon-based magnetic resonance imaging (MRI)7 and target-specific biosensing when a suitable xenon-trapping host is applied8,9,10,11,12,13.
Even with the important applications, especially recent exciting biosensing applications, our understanding of the host-guest chemistry of xenon is limited and development of efficient xenon receptors is highly desirable. As an inert spherical monoatomic gas, xenon lacks an apparent binding site; van der Waals interaction, specifically London dispersion force, is thought to be the main driving force. This makes xenon binding very challenging. Several macrocycle and cage compounds, including hemicarcerands14,15, cyclodextrins16,17, calixarenes18,19,20,21, cryptophanes22,23,24,25,26,27,28,29,30, cucurbiturils31,32,33,34,35,36,37, and recent porous imine cages38,39,40 have been explored for xenon binding, in solution or solid state. Cryptophanes are shown to be outstanding in terms of high affinity and competence for biosensing applications8,9,13,41,42, though, tedious synthesis and sometimes chiral resolution of the intrinsic enantiomers are required for chirality-sensitive detection43,44,45. On the other hand, assembled hosts have the advantages of reversible formation and easy modular accessibility, however, they are barely explored for xenon binding. In the only few reported examples, earlier Rebek’s rigid, hydrogen-bonded “tennis ball” was found to include xenon on 1H NMR observation46. Recently a cyclic peptide-based columnar assembly was shown able to confine xenon in crystalline form47. Meanwhile, metal-assembled Fe4L648 and Co4L649 cages were recently shown able to encapsulate xenon, with a binding constant of 16 M−1 determined for the former.
Herein we report a stable dimeric assembly of a chiral bisurea-bisthiourea macrocycle and its favorable, adaptive-binding ability toward xenon. The assembly represents a tight, completely sealed yet rather soft capsule and encapsulates xenon with a very high affinity for an assembled host. The adaptive-binding dynamics due to induced fit of the surrounding macrocyclic skeletons is revealed not only in crystal form, but also in solution through the unique spectral features of the dimeric assembly.
Design and synthesis
Recently we have developed a set of chiral tetraamino-bisthiourea macrocycles for substrate-induced assembly asymmetric catalysis50. We envisioned that introducing additional carbonyl groups to the diamine moieties on both sides will lead to a type of bisurea-bisthiourea chiral macrocycle M which incorporates multiple hydrogen bond donors (NH) and acceptors (C=S, C=O) simultaneously, and would favor intra- or intermolecular assembly (Fig. 1). The synthesis of the macrocycle is straightforward. After several simple transformations, the 1 + 1 condensation between bis-amine 1 and bis-isothiocyanate 2 furnished multi-grams of the chiral macrocycle in one batch with an excellent yield of 71% (Fig. 1 and Supplementary Methods).
Structures of the dimeric capsule
High-quality crystals of the dimeric capsule M2 were reproducibly obtained by diffusion of n-hexane to a macrocycle toluene solution. Two forms of crystallographically independent dimeric capsules were observed. As shown by the first form in Fig. 2, the two macrocycles adopt a bowl-shaped conformation and crossly overlay to each other through fourfold intermolecular C=O∙∙∙H–N hydrogen bonds (2.81–2.83 Å). The thiourea moieties lie in the bottom and adopt an unusual syn-anti configuration. The forming of two pairs of parallel intramolecular C=S∙∙∙H–N hydrogen bonds (3.39–3.40 Å) in the meantime helps lock the bowl-shaped macrocyclic conformation, leaving four exo NH sites for intermolecular hydrogen bonding. All the phenyl rings from different macrocycles stack onto each other, which may provide further stabilization.
The buckling of the two bowl-shaped macrocycles produces a completely sealed dimeric capsule (Fig. 2c). The cavity volume was detected to be 72 Å3 for the first form (Fig. 3a). Surprisingly, while the overall interacting motif holds, the second form shows a much smaller cavity (36 Å3; Fig. 3b and Supplementary Table 4). The cavity reduction is due to flattening of the bowl-shaped macrocyclic conformation as reflected by shortened (S=)C---C(=S) and lengthened (C=)O---O(=C) dimensions (Fig. 3b vs 3a), suggesting considerable flexibility of the macrocyclic skeleton. The inter- and intramolecular hydrogen bonding, however, is not significantly affected. The existence of the two forms of dimeric capsules is probably caused by crystal packing effect, as the macrocyclic component has a rather flexible skeleton. In both forms, the solvent molecules were found too large to occupy the cavity.
Dimeric assembly in solution
The formation of dimeric assembly in solution was further studied. 1H NMR in (CDCl2)2/DMSO-d6 (5:1) shows a set of simple signals, consistent with an overall D2-symmetric free macrocycle structure in this competitive solvent system (Fig. 4b). In contrast, in pure (CDCl2)2, the spectrum totally changed to two sets of signals at equal intensity, in line with a reduced C2 macrocycle symmetry (Fig. 4c). The NH signals moved largely to downfield direction, suggesting favorable hydrogen bonding formation. By a combination of 1H, 13C and various 2D NMR (Supplementary Figs. 7–14), a dimeric capsular structure similar to that in crystal can be elucidated with all signals well assigned. The two sets of protons (in blue and purple) can exchange their positions through overturn of the syn-anti thiourea configuration as shown by 2D EXSY NMR (Supplementary Fig. 14; vide infra). As the solvent molecule is too large to fit, most capsules are likely to be empty except those occupied by N2 as indicated by the set of minor N2 inclusion peaks (Fig. 4c). High stability of the assembly was demonstrated by concentration-variable NMR as no essential spectral changes observed until dilution to 0.05 mM (Supplementary Fig. 23). A large dimerization constant of (1.9 ± 0.3) × 104 M−1 was further determined by isothermal titration calorimetry (ITC; Supplementary Fig. 26). The dimeric assembly was also confirmed with high-resolution CSI-MS where a peak at m/z = 2111.5522 corresponding to [M2−H]− dominated (Supplementary Fig. 27).
The macrocycle can congruously form a stable, sealed dimeric capsule in both solid state and solution with a cavity possibly suited for xenon (dw = 4.3 Å, V = 42 Å3). To our delight, through bubbling xenon gas, the original 1H NMR signals of the free dimeric capsule almost disappeared, instead a new group of sharp and well-resolved signals dominated, which can correspond to Xe ⊂ M2 (Fig. 4d). All signals were clearly assigned by a combination of 1H, 13C, and various 2D NMR (Supplementary Figs. 15–22). The upfield shift of NH signals and drastic changes of other proton signals may reflect a shielding effect of large electron cloud of xenon and an induced structural change due to tight inclusion (vide infra). The remarkable spectral difference is distinguished from the usually reported, relatively rigid hosts, suggesting the dimeric capsule is rather soft (as also shown in crystal) and can adaptively include the incoming xenon guest. The 129Xe NMR showed a similar slow exchange process and the signal of the bound xenon appeared at 169.6 ppm, largely upfield-shifted comparing to the free xenon in solution (Δδ = −53.4 ppm; Fig. 5). A binding constant of 99 ± 4 M−1 was determined for xenon by 1H NMR integration (see Supplementary Methods and Supplementary Fig. 15). To the best of our knowledge, this is the highest xenon affinity reported to date for assembled hosts. As compared, a previous only known binding constant of 16 M−1 was reported for a metal-assembled Fe4L6 host48.
The existence of two sets of position-exchangeable protons in the macrocyclic skeleton provides a unique probe for exploring the adaptive xenon binding dynamics. As intracapsular, simultaneous overturn of the many locked syn-anti configurated thiourea motifs seems unlikely, the position exchange is probably accomplished through a disassembly-reassembly pathway, i.e., once disassembled the conformation of the free macrocycle can be readily converted (Fig. 6a). Accordingly, the position-exchange rate can reflect the assembly-disassembly dynamics. The influence of xenon binding can thus be probed by comparing the temperature-variable 1H NMR before and after xenon inclusion (Fig. 6b, c). Upon temperature increasing, the two sets of signals started to coalesce and Xe ⊂ M2 showed an obviously higher coalescence temperature Tc and accordingly a higher activation energy ΔG‡ than M2 (17.4 ± 0.1 vs 16.4 ± 0.2 kcal mol−1; Supplementary Figs. 24 and 25 and Supplementary Table 6). This suggests upon xenon inclusion, the dimeric assembly becomes more kinetically stable; in other words, xenon binding could have induced a tighter capsular structure by fitting the soft macrocyclic skeletons. It is worth noting that even at elevated temperatures (up to 373 K), the assembly was still kept intact, once again showing its high thermodynamic stability.
Structures of Xe ⊂ M2
Two different high-quality crystals of Xe ⊂ M2 were independently obtained by diffusion of n-hexane to a macrocycle solution in chloroform or toluene saturated with xenon (Supplementary Tables 2–5). The first crystal crystallized in orthorhombic system as the free dimeric capsule with similar cell parameters (vide supra). As shown by the first form of the two crystallographically independent complexes (Fig. 7), the xenon was completely sealed in the cavity with a perfect packing coefficient of 52%51. In order to fit xenon, the cavity volume was expanded to 81 Å3. The xenon atom shows multiple contacts with the surrounding macrocyclic skeletons, including with the four endo nitrogen (3.83–3.87 Å; the sum of van der Waals radii of nitrogen and xenon is 3.71 Å52) and four carbon atoms (3.98–4.01 Å; the sum of van der Waals radii of carbon and xenon is 3.86 Å52) from the thiourea groups, and with the interior carbon (3.86–4.02 Å) and hydrogen atoms (3.23–3.42 Å; the sum of van der Waals radii of hydrogen and xenon is 3.36 Å52) from four diagonal phenyl rings (Fig. 7a). These contacts, especially that with polar nitrogen atoms, are different to those rigid aromatic faces or sole C–H sites in the usually reported xenon hosts. The second form showed an overall similar structure with a cavity of 69 Å3 and xenon packing coefficient of 61% (Supplementary Tables 4 and 5). The cavity size is largely expanded comparing to that free form of 36 Å3 (vide supra), reflecting the adaptive ability of this tight yet soft capsule. Again, the adaptation is accomplished through the adjust of the bowl-shaped macrocyclic conformation, rather than the change of hydrogen bonding distances.
The second crystal crystallized in a different monoclinic system, but exhibited a similar capsular structure and xenon binding motif (Supplementary Tables 4 and 5). The contacts of xenon to the relevant thiourea nitrogen atoms are even shorter (3.69–3.82 Å). It is worth noting that, even both crystals were grown under 1 atm xenon pressure, the averaged xenon occupancy in the cavity reaches 0.85 and 0.94 respectively, suggesting favored binding53. The sealed but reversible assembly capsule system could thus have potentials for sequestration and separation of xenon (see Supplementary Note 1 for detailed discussion).
In conclusion, a chiral bisurea-bisthiourea macrocycle was efficiently synthesized. This macrocycle can form stable dimeric capsular assembly in both solid state and solution. The capsule possesses a tight, sealed cavity, and effectively binds xenon. Different from other rigid hosts, the capsule is rather soft and can adaptively include xenon through induced fit of the surrounding macrocyclic skeletons. Multiple contacts including several unusual contacts to polar nitrogen atoms are engaged. The adaptive binding dynamic was demonstrated not only in crystal, but also in solution by taking the unique spectral features of the dimeric assembly. These knowledges should have advanced our current understanding on the host–guest chemistry of xenon. The sealed but reversible assembly could also have potentials for developing host materials toward xenon sequestration and separation. With the easy synthesis, modification, robust yet adjustable assembly features, further optimization of the xenon affinity, and 129Xe NMR related parameters should be feasible toward biosensing applications. The enantiopure form of the chiral assembly could also have advantages on chirality-sensitive detection.
The X-ray crystallographic coordinates for structures reported in this study have been deposited at the Cambridge Crystallographic Data Centre (CCDC), under deposition numbers 2006631-2006633. These data can be obtained free of charge from The Cambridge Crystallographic Data Centre via www.ccdc.cam.ac.uk/data_request/cif. Supplementary methods for synthesis and characterization, crystallography, NMR, ITC studies, and additional data supporting the findings of this study are available in Supplementary Information file.
Walker, T. G. & Happer, W. Spin-exchange optical pumping of noble-gas nuclei. Rev. Mod. Phys. 69, 629–642 (1997).
Meersmann, T. & Brunner, E. Hyperpolarized Xenon-129 Magnetic Resonance: Concepts, Production, Techniques and Applications. (RSC, Cambridge, 2015).
Dybowski, C. & Bansal, N. NMR spectroscopy of xenon in confined spaces: clathrates, intercalates, and zeolites. Annu. Rev. Phys. Chem. 42, 433–464 (1991).
Goodson, B. M. Nuclear magnetic resonance of laser-polarized noble gases in molecules, materials, and organisms. J. Magn. Reson. 155, 157–216 (2002).
Rubin, S. M., Lee, S. Y., Ruiz, E. J., Pines, A. & Wemmer, D. E. Detection and characterization of xenon-binding sites in proteins by Xe-129 NMR spectroscopy. J. Mol. Biol. 322, 425–440 (2002).
Weiland, E., Springuel-Huet, M., Nossov, A. & Gédéon, A. 129Xenon NMR: review of recent insights into porous materials. Micropor. Mesopor. Mater. 225, 41–65 (2016).
Albert, M. S. et al. Biological magnetic resonance imaging using laser-polarized 129Xe. Nature 370, 199–201 (1994).
Spence, M. M. et al. Functionalized xenon as a biosensor. Proc. Natl Acad. Sci. USA 98, 10654–10657 (2001).
Schröder, L., Lowery, T. J., Hilty, C., Wemmer, D. E. & Pines, A. Molecular imaging using a targeted magnetic resonance hyperpolarized biosensor. Science 314, 446–449 (2006).
Berthault, P., Huber, G. & Desvaux, H. Biosensing using laser-polarized xenon NMR/MRI. Prog. Nucl. Magn. Reson. Spectrosc. 55, 35–60 (2009).
Schröder, L. Xenon for NMR biosensing – inert but alert. Phys. Med. 29, 3–16 (2013).
Palaniappan, K. K., Francis, M. B., Pines, A. & Wemmer, D. E. Molecular sensing using hyperpolarized xenon NMR spectroscopy. Isr. J. Chem. 54, 104–112 (2014).
Wang, Y. & Dmochowski, I. J. An expanded palette of xenon-129 NMR biosensors. Acc. Chem. Res. 49, 2179–2187 (2016).
Cram, D. J., Tanner, M. E. & Knobler, C. B. Guest release and capture by hemicarcerands introduces the phenomenon of constrictive binding. J. Am. Chem. Soc. 113, 7717–7727 (1991).
Robbins, T. A., Knobler, C. B., Bellew, D. R. & Cram, D. J. A highly adaptive and strongly binding hemicarcerand. J. Am. Chem. Soc. 116, 111–122 (1994).
Bartik, K., Luhmer, M., Heyes, S. J., Ottinger, R. & Reisse, J. Probing molecular cavities in α-cyclodextrin solutions by xenon NMR. J. Magn. Reson. Ser. B 109, 164–168 (1995).
Song, Y.-Q. et al. Selective enhancement of NMR signals for α-cyclodextrin with laser-polarized xenon. Angew. Chem. Int. Ed. Engl. 36, 2368–2370 (1997).
Brouwer, E. B., Enright, G. D. & Ripmeester, J. A. Solid-state NMR and diffraction studies of p-tert-butylcalixarene·nitrobenzene·xenon. Chem. Commun. 939–940 (1997).
Enright, G. D., Udachin, K. A., Moudrakovski, I. L. & Ripmeester, J. A. Thermally programmable gas storage and release in single crystals of an organic van der waals host. J. Am. Chem. Soc. 125, 9896–9897 (2003).
Fukutomi, J., Adachi, Y., Kaneko, A., Kimura, A. & Fujiwara, H. Inclusion complex formation of thiacalixarene and Xe in aqueous solution studied by hyperpolarized 129Xe NMR. J. Incl. Phenom. Macrocycl. Chem. 58, 115–122 (2007).
Ananchenko, G. S., Moudrakovski, I. L., Coleman, A. W. & Ripmeester, J. A. A channel-free soft-walled capsular calixarene solid for gas adsorption. Angew. Chem. Int. Ed. 47, 5616–5618 (2008).
Bartik, K., Luhmer, M., Dutasta, J.-P., Collet, A. & Reisse, J. 129Xe and 1H NMR study of the reversible trapping of xenon by cryptophane-A in organic solution. J. Am. Chem. Soc. 120, 784–791 (1998).
Luhmer, M. et al. Study of xenon binding in cryptophane-A using laser-induced NMR polarization enhancement. J. Am. Chem. Soc. 121, 3502–3512 (1999).
Brotin, T., Lesage, A., Emsley, L. & Collet, A. 129Xe NMR spectroscopy of deuterium-labeled cryptophane-A xenon complexes: investigation of host-guest complexation dynamics. J. Am. Chem. Soc. 122, 1171–1174 (2000).
Huber, G. et al. Water soluble cryptophanes showing unprecedented affinity for xenon: candidates as NMR-based biosensors. J. Am. Chem. Soc. 128, 6239–6246 (2006).
Hill, P. A., Wei, Q., Eckenhoff, R. G. & Dmochowski, I. J. Thermodynamics of xenon binding to cryptophane in water and human plasma. J. Am. Chem. Soc. 129, 9262–9263 (2007).
Fogarty, H. A. et al. A cryptophane core optimized for xenon encapsulation. J. Am. Chem. Soc. 129, 10332–10333 (2007).
Fairchild, R. M. et al. A water-soluble Xe@cryptophane-111 complex exhibits very high thermodynamic stability and a peculiar 129Xe NMR chemical shift. J. Am. Chem. Soc. 132, 15505–15507 (2010).
Taratula, O., Hill, P. A., Khan, N. S., Carroll, P. J. & Dmochowski, I. J. Crystallographic observation of ‘induced fit’ in a cryptophane host–guest model system. Nat. Commun. 1, 148 (2010).
Joseph, A. I., Lapidus, S. H., Kane, C. M. & Holman, K. T. Extreme confinement of xenon by cryptophane-111 in the solid state. Angew. Chem. Int. Ed. 54, 1471–1475 (2015).
Haouaj, M. E., Luhmer, M., Ko, Y. H., Kim, K. & Bartik, K. NMR study of the reversible complexation of xenon by cucurbituril. J. Chem. Soc. Perkin Trans. 2, 804–807 (2001).
Miyahara, Y., Abe, K. & Inazu, T. “Molecular” molecular sieves: lid-free decamethylcucurbituril absorbs and desorbs gases selectively. Angew. Chem. Int. Ed. 41, 3020–3023 (2002).
Kim, B. S. et al. Water soluble cucurbituril derivative as a potential Xe carrier for 129Xe NMR-based biosensors. Chem. Commun. 2756–2758 (2008).
Huber, G. et al. Interaction of xenon with cucurbituril in water. ChemPhysChem 12, 1053–1055 (2011).
Wang, Y. & Dmochowski, I. J. Cucurbituril is an ultrasensitive 129Xe NMR contrast agent. Chem. Commun. 51, 8982–8985 (2015).
He, S. et al. Cavitation energies can outperform dispersion interactions. Nat. Chem. 10, 1252–1257 (2018).
Truxal, A. E., Cao, L., Isaacs, L., Wemmer, D. E. & Pines, A. Directly functionalized cucurbituril as a biosensor for the selective detection of protein interactions by 129Xe HyperCEST NMR. Chem. Eur. J. 25, 6108–6112 (2019).
Chen, L. et al. Separation of rare gases and chiral molecules by selective binding in porous organic cages. Nat. Mater. 13, 954–960 (2014).
Komulainen, S. et al. Inside information on xenon adsorption in porous organic cages by NMR. Chem. Sci. 8, 5721–5727 (2017).
Egleston, B. D. et al. Controlling gas selectivity in molecular porous liquids by tuning the cage window size. Angew. Chem. Int. Ed. 59, 7362–7366 (2020).
Brotin, T. & Dutasta, J.-P. Cryptophanes and their complexes – present and future. Chem. Rev. 109, 88–130 (2009).
El-Ayle, G. & Holman, K. T. in Comprehensive Supramolecular Chemistry II (ed. Atwood, J. L.) (Elsevier Ltd: Amsterdam, Netherlands, 2017).
Huber, J. G. et al. NMR study of optically active monosubstituted cryptophanes and their interaction with xenon. J. Phys. Chem. A 108, 9608–9615 (2004).
Ruiz, E. J., Sears, D. N., Pines, A. & Jameson, C. J. Diastereomeric Xe chemical shifts in tethered cryptophane cages. J. Am. Chem. Soc. 128, 16980–16988 (2006).
Taratula, O. et al. Synthesis of enantiopure, trisubstituted cryptophane-A derivatives. Org. Lett. 14, 3580–3583 (2012).
Branda, N., Grotzfeld, R. M., Valdés, C. & Rebek, J. Jr. Control of self-assembly and reversible encapsulation of xenon in a self-assembling dimer by acid–base chemistry. J. Am. Chem. Soc. 117, 85–88 (1995).
Pizzi, A. et al. Tight xenon confinement in a crystalline sandwich-like hydrogen bonded dimeric capsule of a cyclic peptide. Angew. Chem. Int. Ed. 58, 14472–14476 (2019).
Roukala, J. et al. Encapsulation of xenon by a self-assembled Fe4L6 metallosupramolecular cage. J. Am. Chem. Soc. 137, 2464–2467 (2015).
Du, K., Zemerov, S. D., Parra, S. H., Kikkawa, J. M. & Dmochowski, I. J. Paramagnetic organocobalt capsule revealing xenon host-guest chemistry. Inorg. Chem. 59, 13831–13844 (2020).
Guo, H. et al. Substrate-induced dimerization assembly of chiral macrocycle catalysts toward cooperative asymmetric catalysis. Angew. Chem. Int. Ed. 59, 2623–2627 (2020).
Mecozzi, S. & Rebek, J. Jr. The 55% solution: a formula for molecular recognition in the liquid state. Chem. Eur. J. 4, 1016–1022 (1998).
Bondi, A. van der Waals Volumes and Radii. J. Phys. Chem. 68, 441–451 (1964).
Kane, C. M., Banisafar, A., Dougherty, T. P., Barbour, L. J. & Holman, K. T. Enclathration and confinement of small gases by the intrinsically 0D porous molecular solid, Me,H,SiMe2. J. Am. Chem. Soc. 138, 4377–4392 (2016).
Guex, N. & Peitsch, M. C. SWISS-MODEL and the Swiss-Pdb viewer: an environment for comparative protein modeling. Electrophoresis 18, 2714–2723 (1997). Information for the software, see: https://spdbv.vital-it.ch.
Financial supports from National Natural Science Foundation of China (21871276 and 21521002) and Chinese Academy of Sciences (QYZDJ-SSW-SLH023) are gratefully acknowledged. We thank Dr. Junfeng Xiang (NMR), Dr. Xiang Hao and Mrs. Tongling Liang (crystallography) from ICCAS for helpful discussion.
The authors declare no competing interests.
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Nie, SX., Guo, H., Huang, TY. et al. Xenon binding by a tight yet adaptive chiral soft capsule. Nat Commun 11, 6257 (2020). https://doi.org/10.1038/s41467-020-20081-8