Abstract
The globular and monocationic guest molecule trimethyl‐azaphosphatrane (AZAP, a protonated Verkade superbase) was shown to form a host:guest 1 : 1 complex with the cucurbit[10]uril (CB[10]) macrocycle in water. Molecular dynamics calculations showed that CB[10] adopts an 8‐shape with AZAP occupying the majority of the internal space, CB[10] contracting around AZAP and leaving a significant part of the cavity unoccupied. This residual space was used to co‐include planar and monocationic co‐guest (CG) molecules, affording heteroternary CB[10]⋅AZAP⋅CG complexes potentially opening new perspectives in supramolecular chemistry.
Keywords: azaphosphatrane, CB[10], cucurbituril, host:guest, ternary complexes
An azaphosphatrane (AZAP) forms a host:guest 1 : 1 complex with the cucurbit[10]uril (CB[10]) macrocycle in water and forces CB[10] to adopt an 8‐shape with AZAP occupying the majority of the cavity. The CB[10] contraction leads to a residual space which favors the co‐inclusion of planar and monocationic co‐guest (CG) molecules, affording heteroternary CB[10]⋅AZAP⋅CG complexes.

Introduction
Ternary assemblies of proteins are known to play crucial roles in cells. By assembling in particular oligomers of controlled size and shape, new functions emerged surpassing what could be done based on individual components. For example, ternary complexes of proteins are involved in voltage‐gated potassium channels that are pivotal for channels functions in the brain and in the heart. [1] Heterotrimeric G proteins can function as transducers in signaling pathways, [2] or bind the adenosine A1 receptor as illustrated in the search for non‐opioid analgesic agents. [3] However, artificial heteroternary complexes are still limited to comparatively small molecules and these include for example metal‐ligand cages accommodating two types of guests, [4] molecular Russian dolls, [5] or organic cages with different guest molecules. [6] In this context, the cucurbit[8]uril (CB[8]) macrocycle [7] was shown in 2001 to be able to form heteroternary complexes [8] with a pair of guest molecules combining electron donor and electron acceptor features. [9] This discovery has opened a new domain by enabling to “click” by CB[8], two types of compounds (i. e. peptides, [10] proteins, [11] polymers, [12] dendrimers) [13] each carrying a suitable group for inclusion in CB[8]. Recent developments include molecular switches, [14] host‐enhanced polar‐π interactions (social self‐sorting), [15] dynamic oligomers, [16] bifunctional photoredox catalysts, [17] curcumin delivery in cancer cells, [18] advanced herbicides [19] or dynamic interfacial adhesion. [20] Compared to the more traditional “covalent click” chemistry, this method is endowed with inherent dynamics while permitting to get sufficiently robust links. After the discovery of cucurbit[10]uril, [21] and of its isolation, [22] several studies have demonstrated its unique potential in supramolecular chemistry [23] owing to its large open cavity. During our investigations about new guest molecules of interest for CB[10], [24] we found that trimethyl‐azaphosphatrane (AZAP, a protonated Verkade superbase, [25] Figure 1) could form 1 : 1 complexes with CB[10], the host cavity being left with enough space for other compounds.
Figure 1.

(a) Molecular structures of CB[10], AZAP, and co‐guest (CG1 to CG6) molecules used in this work.
Azaphosphatranes are the conjugated acids, of the well‐known Verkade superbases (pro‐azaphosphatranes). [25] They are the subject of growing interest and were found to act as efficient organocatalysts in various reactions such as ring‐opening polymerization (ROP), Strecker reactions, or for CO2 conversion into cyclic carbonates. [26] The properties of self‐ assembled or covalent cages built from azaphosphatrane units [27] have been also studied and, for example, self‐assembled cages involving azaphosphatrane motifs as sub‐components can recognize and extract anions from water with remarkable selectivity. [28] However only one example of host‐guest complex where an azaphosphatrane plays the role of guest has been described leading to modification of acido/basic properties of the encaged guest. [29] Thus, the supramolecular encapsulation of azaphosphatranes and the properties of the resulting host‐guest complexes have been scarcely studied and could lead to new supramolecular objects with original properties. On the other hand, few heteroternary complexes based on CB[10] have been reported, including a calixarene, [22] a Russian doll, [30] and tetracationic porphyrins. [31] Given the impact of CB[8] on supramolecular coupling by forming heteroternary complexes, we focused on (i) finding plausible reasons to explain the present results, and (ii) deciphering the scope of co‐guests (CG) suitable to form CB[10]⋅AZAP⋅CG heteroternary complexes.
Results and Discussion
While exploring new guests for CB[10], we found that AZAP could solubilize CB[10] (otherwise scarcely soluble alone in water), and that a titration gradually changing the guest:host ratio (see Supporting Information for details) showed rapid exchange on the NMR timescale in D2O (Figure 2).
Figure 2.

1H NMR titration (300 MHz, 300 K, D2O) of AZAP keeping constant the quantity of CB[10] in the tubes (around 0.41 mg of CB[10] in 500 μL of D2O see experimental section, guest:host ratios on the left). *signal of acetone.
In this series of experiments, the chemical shift of guest methyl protons shifted upfield by 0.40 ppm (Hc) while those corresponding to guest methylene protons also shifted upfield but by 0.42 ppm (Hb) and 0.50 ppm (Ha, Figure 2). 31P NMR spectra of CB[10]⋅AZAP were unusable. Unexpectedly, an excess of host, even apparently insoluble, was required to get the maximum upfield shifts of guest proton signals. In principle, any undissolved CB[10] should not impact the complexation equilibrium between CB[10] and AZAP. However, this is what observed, repeatedly, over time, and host:guest ratios. To try understanding this observation, we have recorded 1H NMR spectra of CB[10] (Figure S1) in D2O (fixed volume) at 500 MHz using a small but precise fraction of acetone as internal standard and increased the total quantity of CB[10] (0.2 to 1.0 mg, Figure S2). As expected, the integrated ratio of signals of CB[10] compared to those of acetone remained about constant enabling to propose a concentration of CB[10] of 5.4 μM in D2O (Figure S3). Despite our efforts, this effect remains unexplained. We suppose a “non‐classical” dissolution/complexation of CB[10] mediated by the presence of CB[10] aggregates. Initial tests aimed at removing the excess of insoluble host by filtration resulted in different spectra presumably due to equilibria displacements. The effect of centrifugation was also checked but identical spectra were obtained without centrifugation. To go further, we performed our experiments using a “standardized” procedure involving an identical concentration of CB[10] for all the titrations of the paper (0.83 mg/mL in D2O). At excess host, integrals suggested formation of a 1 : 1 CB[10]⋅AZAP complex (Figure S4). The binding constant corresponding to this equilibrium could not be determined due to the very low solubility of CB[10] in water. Molecular dynamics calculations considering CB[10] with one included AZAP showed that the 1 : 1 complex is stable for at least 100 ns in water (Figure 3).
Figure 3.

Representative snapshot of the CB[10]⋅AZAP complex from the corresponding molecular dynamics in water (solvent removed for clarity).
The AZAP guest molecule was found to be relatively weakly mobile in the CB[10] cavity that seemed largely accommodating its shape to encircle the guest (mean distance between the barycentre of the host and that of the guest oscillating between ∼2.0 and 3.5 Å, Figure S5 and video S1). The observed, asymmetric 8‐shape of CB[10] was quite stable over all the duration of the dynamics (100 ns), even if AZAP could travel in the host cavity (Figure S6). AZAP seemed entailing CB[10] to contract around it, leaving a small space amenable for further binding. By doing so, AZAP could have preorganized the cavity for subsequent co‐guest accommodation in an allosteric or cooperative manner. However, this is not reflected in 1H NMR spectra that are in line with a preserved high symmetry and suggesting that if the host is contracted, this must be averaged with respect to the NMR timescale.
The free space left available was next used to investigate co‐guest binding with a series of planar cationic compounds.
The addition of planar and monocationic guest compounds CG1 to CG5 to solutions of the CB[10]⋅AZAP complex (containing a CB[10]/AZAP ratio of 1/0.3, to ensure having a fully complexed AZAP, see experimental part) showed extra‐upfield shifts of AZAP resonances (ΔδHa=−0.01 to −0.10 ppm, ΔδHb=−0.01 to −0.12 ppm, ΔδHc=−0.08 to −0.23 ppm, Figure 4) supporting that no decomplexation of AZAP occurred upon addition of the second guests. For dicationic guests, dimethyl‐viologen or hexamethyl‐N,N‐bisethylene‐1,4,5,8‐naphthalenediimide diammonium, two guests known to include in CB[10] [32] had no impact on the 1H NMR spectrum of the CB[10]⋅AZAP complex, while hexamethyl‐p‐xylylenediammonium (CG6) did (Figure 4 bottom).
Figure 4.

1H NMR spectra (600 MHz, 300 K, D2O) of the CB[10]⋅AZAP 1 : 1 complex (around 0.41 mg of CB[10] in 500 μL, see experimental section) and of heteroternary complexes CB[10]⋅AZAP⋅CG1 to CB[10]⋅AZAP⋅CG6 (*: signal of acetone, vertical dashed line at 2.22 ppm, CB[10] with 0.3 equiv. of AZAP and 0.3 equiv. of CGx to ensure having enough excess host). Bottom, DOSY spectrum corresponding to the CB[10]⋅AZAP⋅CG6 complex.
DOSY NMR of the CB[10]⋅AZAP complex (Figure S7) showed all host and guest signals aligned with a diffusion coefficient D≈2.87×10−10 m2.s−1 corresponding to ∼15 Å of diameter (spherical approximation) so in line with the size of CB[10]. The DOSY spectrum of CB[10]⋅AZAP⋅CG6 (Figure 4, bottom) was in line with (i) double‐guest inclusion (no free guest) and (ii) a size of the CB[10]⋅AZAP⋅CG6 complex close to that of CB[10] (D≈2.82×10−10 m2.s−1, inclusion complexation). DOSY spectra of other ternary complexes CB[10]⋅AZAP⋅CGx (x=1–5, Figures S8 to S12) showed signals deviating from ideal alignment due to rapid exchange of CGx with CB[10]⋅AZAP. [33] Another evidence toward heteroternary complexation is the significant extra‐upfield shift of AZAP signals (Figure 4), in line with favored social self‐sorting (CB[10]⋅AZAP⋅CGx) compared to narcissistic self‐sorting (CB[10]⋅AZAP and CB[10]⋅CGx 2). Controls titrating separately CG2 and CG6 with CB[10] (Figures S13 and S14 respectively) to explore the alternative sequence of guest binding (CB[10]⋅CGx+AZAP⇆CB[10]⋅CGx⋅AZAP) showed that 1 : 1 CB[10]⋅CGx complexes could form but were less favored than corresponding heteroternary complexes and we could not discard the presence of CB[10]⋅(CGx)2 complexes contrary to AZAP which formed exclusively CB[10]⋅AZAP 1 : 1 complexes.
Careful inspections showed that AZAP impacted CGx proton resonances of included CGx with downfield shifts for methyl groups (+0.06 or +0.09 ppm for CG1, CG2 and CG3) suggesting that AZAP may help placing CGx methyl groups near the host carbonyl rims, while aromatic signals are weakly affected (except for CG3, Δδ=+0.07 and +0.11 ppm). Finally, while weak signal‐to‐noise ratios prevented the quantification of complexation induced chemical shift changes for CG4, one signal of CG5 was featured by a +0.18 ppm downfield shift as a result of the simultaneous presence of AZAP in CB[10], compared to signals of CB[10]⋅CG5. Finally, compared to free CG6, the signal corresponding to the aromatic group of the CG6 co‐guest in the CB[10]⋅AZAP⋅CG6 complex shifted upfield by 0.42 ppm while the one corresponding to methyl groups shifted also upfield but by 0.17 ppm. The search for NOE cross‐correlations between included AZAP and CGx was unsuccessful despite the record of 2D NOESY spectra at different mixing times.
The addition of CG2 was also tested to see whether CG2 could promote AZAP capture in conditions where AZAP is only partially complexed in CB[10]. CG2 was added in a solution containing CB[10] and AZAP in a 1 : 1 ratio (corresponding to ∼75 % of complexed AZAP, Figure S15) and the 1H NMR spectra showed an upfield shift of AZAP signals with 0.5 and 1 equiv. of CG2 (Figure S15) confirming the suspected cooperativity. However, when more than 2 equiv. of CG2 were added, both sets of NMR signals corresponding to AZAP and CG2 shifted downfield as a consequence of a competition between formation of CB[10]⋅AZAP⋅CG2 and CB[10]⋅(CG2)n (n=1 or 2).
Next, considering the CB[10]⋅AZAP complex as a “soluble modified host” (when a CB[10]:AZAP ratio of 1:0.3 is used), we first checked the stoichiometry of the CB[10]⋅AZAP⋅CG2 complex by a Job Plot (Figure S16) confirming formation of a “1 : 1 complex” between CB[10]⋅AZAP and CG2. Then we performed 1H NMR titrations considering increasing amounts of co‐guest molecules (Figures S17‐S22, Table 1, for a representative example see Figure 5). Fitting experimental points considering complexation induced AZAP chemical shift changes according to a 1 : 1 binding model afforded binding constants K a associated to the following equilibria: CB[10]⋅AZAP+CGx↔CB[10]⋅AZAP⋅CGx (Figure 5 inset and Table 1).
Table 1.
Binding constants for co‐guests CG1 to CG5 toward the CB[10]⋅AZAP complex, maximum observed Δδ and mean distances from MD simulations.
|
CGx |
K a [M−1][a] |
Δδmax [ppm][b] |
d AZAP‐CGx |
d Host‐AZAP |
d Host‐CGx |
|---|---|---|---|---|---|
|
CG1 |
6800 |
0.23 |
7.1±0.3 Å |
2.9±0.2 Å |
4.5±0.3 Å |
|
CG2 |
25100 |
0.30 |
7.0±0.3 Å |
3.0±0.2 Å |
4.1±0.3 Å |
|
CG3 |
25000 |
0.43 |
6.5±0.6 Å |
3.0±0.3 Å |
3.8±0.5 Å |
|
CG4 |
1500 |
0.45 |
6.5±0.5 Å |
2.9±0.2 Å |
3.8±0.5 Å |
|
CG5 |
13600 |
0.49 |
6.2±0.6 Å |
2.7±0.4 Å |
3.7±0.4 |
[a] determined using the BINDFIT program; [34] error: ±11 %. [b] experimental values from signals of protons Hc, see Figure 2.
Figure 5.

1H NMR titration of the CB[10]⋅AZAP 1 : 1 complex (around 0.41 mg of CB[10] in 500 μL of D2O, see experimental section) with CG2 (500 MHz, 300 K).
Among them and assuming co‐guests sit axially against AZAP inside CB[10], the least sterically demanding co‐guests laterally CG2, CG3 and CG5 bind with a ∼104 M−1 affinity, the difference between CG4 and CG5 being especially striking (a factor of nearly 10 times) explained solely by the position of the methyl group on the co‐guest (1‐ versus 2‐quinoline). Another control mixing separately prepared solutions of CB[10]⋅AZAP and CB[10]⋅CG3 afforded a new 1H NMR spectrum (Figure S23) different from those of the initial complexes and in line with CB[10]⋅AZAP⋅CG3. Finally, a large excess of CG2 did not result in AZAP expulsion (heteroternary complex dislocation). Attempts to grow single crystals of the complexes resulted in small single crystals and those large enough for analyses by X‐ray diffraction enabled to observe a unit cell with the host only, presumably due to high guests disordering in the host cavity. Even if these structures should be considered with extreme caution due to the high levels of disordering, the host appear flattened (roughly resembling the shape shown on Figure 3 though without methylene inversion) when crystallized from a solution of CB[10] and AZAP, but almost circular when CG2 was added before solvent evaporation (Figure S24).
We thus decided to investigate the heteroternary complexes by molecular dynamics in water. Heteroternary complexes with CG1 to CG5 were found to be quite stable over 100 ns in water (snapshots for the CB[10]⋅AZAP⋅CG5 complex in Figure 6 and Figure S25). With co‐guest molecules, AZAP was found to be largely mobile in CB[10] but co‐guests could either stay inside the complex or be expulsed before being included again (this was observed for CG3 and CG5). Nevertheless, in the latter case, heteroternary complexes were stable for the last 50 ns of MD trajectories. Calculations of distances between the barycentres of CB[10], AZAP, and CGx showed that the two different guests considered remained facing each other's inside CB[10] (see Supporting Information and Table 1), AZAP being systematically slightly offset (∼3 Å) to the center of CB[10], as CGx (∼4 Å). Consistently, distances between AZAP and CGx remained in the 6.3–7.3 Å window, in line with stable co‐inclusion for the 2nd half of the MD trajectories (Figures S26 to S30). Attempts to quantify CB[10] deformation by measuring the 5 distances between opposite carbon atoms of the equatorial plane for CB[10]⋅AZAP⋅CG1 to CB[10]⋅AZAP⋅CG5 (Figure S31) showed large macrocycle contraction and expansion cycles seemingly not impacting its faculty to accommodate two of such dissimilar guest compounds. The dynamical behavior was similar for the five considered heteroternary complexes, that for CG5 summarizing well the trends (video S2). In this case, AZAP was found to be highly mobile, translating and rotating in all directions in the CB[10] cavity. Simultaneously, CG5 was found to adjust its position with respect to AZAP, with its main axis almost always staying parallel to the C 10 axis of the host, CG5 being able to rotate around this axis.
Figure 6.
Snapshot of the CB[10]⋅AZAP⋅CG5 complex from the corresponding molecular dynamics trajectory in water (hydrogen atoms removed for clarity, see text and video S2; the yellow disk delineated by a yellow dashed line denotes the AZAP location, the structure of CB[10] is found to be very flexible with these two included guests, see Figure S25).
As a consequence, CB[10] was observed to continuously adjust its shape toward the two guests, the cause‐consequence relationship remaining difficult to firmly establish. Even if dynamic, the averaged rounded shape of CB[10] is in agreement with the shape of the host determined from the preliminary X‐ray structure. These results of host and guests dynamics in heteroternary complexes are also in line with NMR results since signals of both host and guests remain sharp and “simple” (no symmetry break), suggesting unhindered rotation. Finally, both kinds of guests experiencing a more hydrophobic environment in CB[10] should have the signals of their protons shifted upfield which is indeed observed for signals of AZAP protons (Figures 2, 4, 5) and CGx protons (i. e. Figure S15). If we consider the inclusion of AZAP followed by CGx, the former seems pre‐organizing the cavity for subsequent binding in a manner reminding an allosteric binding. However, because of the ambiguity about CB[10]⋅CGx complexes stoichiometry (singly or doubly accommodated guests in some cases), weak binding requiring excess guest, and fast exchange with free CGx, we could not investigate the equally important alternative pathway of guest inclusion (CB[10] binding CGx followed by AZAP). The question of a mechanism more relevant to induced fit (IF) or conformational selection (CS) remains open. [35] In either case, the space for co‐guest inclusion (induced by AZAP) resembles a half‐cavity of nor‐seco‐CB[10], [36] and contrasts with what reported for others CB[10] heteroternary complexes for which π‐stacking, [31] or strong guest‐guest interactions involving electron donor/acceptor features [30] directed the assembly. The flexibility of CB[10] could thus be an important factor in the stabilization of the reported heteroternary complexes. Globally, the observed social, instead of narcissistic self‐sorting could be explained by the preferred 1 : 1 host:guest ratio at excess host with AZAP resulting in formation of a CB[10]⋅AZAP inclusion complex featured by residual space left in the host cavity. We surmise that mixed guest pairs are favored owing to better fillings of the cavity space compared to a mixture of CB[10]⋅AZAP with residual internal space together with homoternary complexes featuring identical guest pairs (i. e. CB[10]⋅CGx⋅CGx) not able to fill, as well, the host cavity.
Conclusions
In conclusion, we found that the azaphosphatrane AZAP could behave as a new monocationic guest for CB[10]. Beyond CB[10] solubilization and formation of a 1 : 1 CB[10]⋅AZAP complex, some residual space inside the complex was found to be available and relevant for co‐guest inclusion. A small screening of planar (aromatic) guests converged toward monocationic co‐guests able to include in the 1 : 1 CB[10]⋅AZAP complex to afford heteroternary 1 : 1 : 1 host:guest:guest complexes with possibilities for planar dicationic co‐guests opened by CG6. These new heteroternary complexes could be used for the construction of advanced oligomeric structures or open new avenues toward new heteroguest pairs amenable for example, to supramolecular click binding with CB[10].
Experimental Section
Chemical compounds: CB[10] was prepared according to a previous paper. [37] AZAP was prepared according to the literature. [38] N,N,N‐trimethyl‐benzenaminium iodide CG1 was purchased from TCI and used without further purification. The synthesis of co‐guests CG2 to CG6 is described in Supporting Information.
NMR titration of CB[10]⋅AZAP: for each NMR tube, an amount of around 0.41 mg of CB[10] was precisely weighted and a precise volume of a 3 mM solution of AZAP was added to afford the selected CB[10]:AZAP ratio (between 1 : 8 to 1:0.125, Figure 2). The total volume (around 500 μL, depending on the weighted CB[10]) was adjusted with D2O to target 0.5 mM solutions of CB[10] (considering complete CB[10] solubility in D2O aided by the guest, even if CB[10] presents a very low solubility in D2O). Experimental results show that excess CB[10], even scarcely soluble without guest, plays a role in the titration.
NMR titration of CB[10]⋅AZAP⋅CGx: for each titration (CG1‐CG6), an amount of around 0.41 mg of CB[10] was weighted and a precise volume of a 3 mM solution of AZAP was added to afford the CB[10]:AZAP ratio 1:0.3. The total volume (∼500 μL, depending of weighted CB[10]) was adjusted with D2O to prepare a targeted 0.5 mM solution of CB[10]. Then corresponding volumes of stock solutions of CGx were added for the titrations shown on Figures S17–S22 of co‐guests CG1‐CG6, respectively.
Conflict of interest
The authors declare no conflict of interest.
1.
Supporting information
As a service to our authors and readers, this journal provides supporting information supplied by the authors. Such materials are peer reviewed and may be re‐organized for online delivery, but are not copy‐edited or typeset. Technical support issues arising from supporting information (other than missing files) should be addressed to the authors.
Supporting Information
Supporting Information
Supporting Information
Acknowledgements
CNRS and Aix Marseille Université are acknowledged for continuous support. This work received support from the French government under the France 2030 investment plan, as part of the Initiative d′Excellence d′Aix‐Marseille Université ‐ A*MIDEX. Dr. Michel Giorgi (Spectropole, Marseille) is gratefully acknowledged for two preliminary crystal structures of CB[10]. Dr. Yann Ferrand and Dr. Brice Kauffmann (IECB, Bordeaux) are gratefully acknowledged for one preliminary crystal structure of CB[10] crystallized from a solution of CB[10], AZAP and CG2.
C. Li, A.-D. Manick, Y. Zhao, F. Liu, B. Chatelet, R. Rosas, D. Siri, D. Gigmes, V. Monnier, L. Charles, J. Broggi, S. Liu, A. Martinez, A. Kermagoret, D. Bardelang, Chem. Eur. J. 2022, 28, e202201656.
Contributor Information
Prof. Simin Liu, Email: liusimin@wust.edu.cn.
Prof. Alexandre Martinez, Email: alexandre.martinez@univ-amu.fr.
Dr. Anthony Kermagoret, Email: anthony.kermagoret@univ-amu.fr.
Dr. David Bardelang, Email: david.bardelang@univ-amu.fr.
Data Availability Statement
The data that support the findings of this study are available from the corresponding author upon reasonable request.
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Data Availability Statement
The data that support the findings of this study are available from the corresponding author upon reasonable request.

