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Anion-capped metallohost allows extremely slow guest uptake and on-demand acceleration of guest exchange


The switching of molecular recognition selectivity is important for tuning molecular functions based on host–guest binding. While the switching processes in artificial functional molecules are usually driven by changes of the thermodynamic stabilities, non-equilibrium phenomena also play an important role in biological systems. Thus, here we designed a host–guest system utilizing a non-equilibrium kinetically trapped state for on-demand and time-programmable control of molecular functions. We synthesized a bis(saloph) macrocyclic cobalt(III) metallohost 1(OTf)2, which has anion caps at both sides of the cation-binding site. The anion caps effectively retard the guest uptake/release so that we can easily make a non-equilibrium kinetically trapped state. Indeed, we can obtain a long-lived kinetically trapped state {[1·K]3++La3+} prior to the formation of the thermodynamically more stable state {[1·La]5++K+}. The guest exchange to the more stable state from this kinetically trapped state is significantly accelerated by exchange of TfO anion caps by AcO in an on-demand manner.


The switching of molecular recognition selectivity is important for tuning molecular functions based on host–guest binding1,2,3,4,5. Most of these switching processes are driven by a stimuli-responsive guest uptake/release or guest exchange upon the structural change between two different states. To date, a number of responsive molecular recognition systems has been developed by taking advantage of various kinds of stimuli such as redox reactions6,7,8, acid/base reactions9,10,11, light irradiation12,13,14,15 and metal ion addition16,17, which lead to drastic structural changes in the host scaffold. Such stimuli-responsive systems can also be found in nature, as represented by Na+/K+-ATPase, which pumps Na+ out of a cell with the concomitant transport of K+ into the cell against their concentration gradients with the aid of ATP18,19. The key for regulating the concentrations is the structural changes in the enzyme between the two main states, E1 and E2, which selectively bind Na+ and K+, respectively. In general, the selectivity switching requires reversal of the thermodynamic stabilities, which can be evaluated by the association constants, Ka, in the two different states (Fig. 1a).

Figure 1: Design and concept for kinetically controlled on-demand acceleration of guest uptake/exchange.

(a) Schematic illustration of thermodynamically controlled stimuli-responsive guest exchange in which the association constants for two different of guests are reversed by an external stimulus. (b) Schematic illustration of kinetically controlled stimuli-responsive guest exchange in which the kinetic barrier for the guest exchange is removed by an external stimulus. (c) Design of macrocyclic host 12+ with two capping sites. (d) Concept of the extremely slow guest uptake/exchange by taking advantage of anion caps.

In addition, non-equilibrium phenomena play an important role in biological systems as well as in supramolecular polymer systems20,21,22,23,24,25,26,27,28,29,30. For example, passive transport finely controls ion uptake and release using ion channels and carriers according to their concentration gradients. We could make similar ion uptake/release systems using much simpler artificial host molecules if we can access a suitable non-equilibrium kinetically trapped state (Fig. 1b(i)). Once a kinetically trapped state is generated, removal of the kinetic barrier would initiate the uptake/release of guest ions according to the intrinsic affinity difference of the host molecule (Fig. 1b(ii)). This would enable us to tune the molecular functions in an on-demand and time-programmable manner as seen in biological systems. However, such a guest uptake/release based on a kinetically trapped state has rarely been utilized for controlling molecular functions in artificial systems. As to generating a kinetically trapped state as the first step (Fig. 1b(i)), there have been several host molecules that temporarily bind a kinetically favoured guest prior to the binding with a thermodynamically favoured guest31,32,33,34,35,36,37,38,39,40,41,42,43. Therefore, we envisioned a kinetically trapped host–guest system having the second step in which removal of the kinetic barrier can initiate the guest uptake or exchange (Fig. 1b(ii)).

We designed a host molecule [LCo2(CH3NH2)4](OTf)2 (=1(OTf)2) containing an 18-crown-6-like cavity suitable for cation recognition44,45. The molecule has two octahedral cobalt(III) centres and four axially coordinating methylamine molecules as anchors, which would contribute to holding anionic species at the capping sites (Fig. 1c). The anion caps are expected to block the guest from entering and exiting the cavity, and work as a removable kinetic barrier (Fig. 1d). In this paper, we report an ion recognition system that shows an extremely slow uptake of guest cations due to the blocking effect of the anion caps. This enables us to obtain a kinetically trapped state, from which on-demand acceleration of the guest exchange is triggered by the anion cap exchange.


Synthesis of anion-capped metallohost

The metallohost 1(OTf)2 was synthesized by the complexation of the bis(saloph) macrocyclic host44,45 (H2saloph=N,N′-disalicylidene-o-phenylenediamine) with cobalt(II) acetate under aerobic conditions in the presence of methylamine (Supplementary Fig. 1). Each of the two saloph moieties accommodates a low-spin diamagnetic cobalt(III) ion, to which two methylamine molecules coordinate to form an octahedral geometry. A crystallographic analysis revealed its molecular structure in which the central O6 cavity remains vacant as similarly observed in the nickel(II) analogue44,45. The four methylamine molecules coordinate to the octahedral cobalt(III) centres to form the capping sites as expected, but the triflate counteranions were not located at the capping sites (Supplementary Fig. 15).

Guest recognition behaviour

We were initially skeptical about the idea that the dicationic metallohost 12+ would bind cationic guests because electrostatic repulsion between the positive charges was expected. However, 12+ showed an excellent binding affinity towards cationic guests. For example, the addition of 1 equiv of NaOTf to the metallohost 1(OTf)2 in CD3OD resulted in complete conversion to the inclusion complex [1·Na]3+ (Fig. 2a and Supplementary Fig. 2). It is noteworthy that the 1H NMR signals for the inclusion complex were separately observed from those for the free metallohost 12+. This indicated that the complexation/decomplexation process is slow on the NMR timescale. This slow guest exchange would be due to the anion caps as we had expected. Indeed, the X-ray crystallographic analysis of the Na+ complex (Fig. 2b) clearly showed that the counteranions are located at the capping sites. The Na+ ion was located in the central O6 site, and the two triflate anions at the capping sites coordinate to the guest Na+ ion from both sides of the macrocycle. In addition, the anions are hydrogen-bonded to the methylamine molecules as the anchors. The strong interaction between these triflate counteranions and guest Na+ ion is probably one of the important factors for the unexpectedly strong cation-binding affinity to overcome the electrostatic repulsion between the positive charges.

Figure 2: Na+ encapsulation by anion-capped metallohost.

(a) 1H NMR spectral changes of 1(OTf)2 upon the addition of NaOTf in CD3OD (400 MHz, [1(OTf)2]=1.0 mM). (b) X-ray crystal structure of [1·Na(OTf)2](OTf). Hydrogen atoms are omitted for clarity except for those of the NH2 groups. The solvent molecules and one triflate anion are also omitted.

Thermodynamics and kinetics of cation recognition

While the metallohost 1(OTf)2 did not interact with the smaller ions (Mg2+, Li+), it strongly recognized metal ions having radii of >1.26 Å (Supplementary Figs 3–11). In particular, the association constants for metal ions having ionic radii of 1.3 Å (Ca2+, La3+, Na+ and K+) were greater than 106 M−1 (Table 1, equations (1) and (2)).

Table 1 Association constants and kinetic data for the complexation between 12+ or 18-crown-6 and guest cations.

The binding strengths seem to be mainly governed by the size-fit principle rather than the electrostatic interactions, although the binding strengths might be influenced by some other factors such as the charge of the guest ions. Even multivalent metal ions, such as Ca2+ or La3+, were strongly bound to the dicationic metallohost 1(OTf)2 in spite of the expected electrostatic repulsion. This unexpectedly strong binding can be ascribed to the interaction with the anion caps as observed for the Na+ complex (for the X-ray crystal structures of the K+ and Ca2+ complexes, see Supplementary Figs 17 and 18).

As expected based on the structures of the host–guest complexes having anion caps, the guest uptake and release were extremely slow. For example, the uptake of better guests, such as K+, Na+ and Ca2+, was slow on the NMR timescale (Table 1). Nevertheless, the guest uptake was completed and reached equilibrium within 5 min after mixing the guests with 1(OTf)2. In stark contrast, the complexation with La(OTf)3 was exceptionally slow (Supplementary Fig. 13). It took 120 h for complete encapsulation after the addition of 2 equiv of La(OTf)3. The half-life of the guest uptake was roughly estimated to be 10 h from the time course analysis of the 1H NMR spectra. Thus, the guest inclusion by 1(OTf)2 was much slower than that by simple crown ethers (within milliseconds to seconds)46,47,48. The retarded guest inclusion should mainly be attributed to the effect of the anion caps, although there are differences in the charge and the host structures that could also affect the guest uptake rates.

On-demand acceleration of guest exchange

We expected that this exceptionally slow uptake of La3+ is due to the capping effect of the triflate anions. We thus expected that the guest uptake rates can be tuned by changing the counteranions because the capping effect might depend on the sizes and basicity of the anions. It was inferred that it would be easy to understand the effect of counteranions if we could start with the metallohost having non-coordinating anion such as BPh4. However, it was difficult to obtain pure sample of 1(BPh4)2. Thus, 3 equiv of Bu4NX (X=AcO, F, Cl, Br, BF4, PF6, BPh4) was added to the mixture of 1(OTf)2 and La(OTf)3 and the uptake rates were compared with the blank experiment. As we expected, acetate ion (AcO) significantly accelerated the cation uptake, while other anions (F, Cl, Br, BF4, PF6, BPh4) did not. This acceleration was also observed when La(OAc)3 was used as the La3+ source. The uptake of La3+ was completed within 5 min after the addition of 2 equiv of La(OAc)3 (Supplementary Figs 12 and 14). The uptake rate kin of La(OAc)3 was estimated to be ≥30 M−1s−1, which was at least 100 times faster than that of La(OTf)3. Clearly, the counteranions played a critical role in the exceptionally slow uptake of La(OTf)3.

As already described, the guest uptake/release by 12+ is exceptionally slow, and this would allow us to obtain kinetically trapped states as depicted in Fig. 1b(i). In order to use this system for kinetically controlled switching, it is necessary to accelerate it by removing or lowering the kinetic barrier (Fig. 1b(ii)). Since the counteranions (TfO and AcO) significantly affect the guest uptake/release rates of 12+, we expected that exchanges of the anion caps would lower the barrier and trigger the guest uptake/release. Thus, we made an on-demand guest exchange system driven by the anion cap replacement.

We chose K+ and La3+ as the guests to obtain a kinetically trapped state because La(OTf)3 was more strongly bound (Ka=2.4 × 106 M−1) than KOTf (Ka=1.1 × 106 M−1), but more slowly taken up (kin≈10−2 M−1s−1) than KOTf (kin=1.9 × 107 M−1s−1). As expected from the thermodynamic and kinetic data, we successfully generated the kinetically trapped state {[1·K]3++La3+} when KOTf (1 equiv) and La(OTf)3 (2 equiv) were added to the metallohost 1(OTf)2 at once (Figs 3a(i) and 4(i)). The kinetically formed K+ complex would be converted to the thermodynamically more stable La3+ complex according to the difference in the association constants. However, this guest exchange was found to be very slow; the K+ complex was still dominant even after 14 days (Figs 3a(i), b(i) and and Supplementary Fig. 20). It should be noted that the reverse reaction from [1·La]5+ to [1·K]3+ did not take place at all when KOTf was added to the La3+ complex (Fig. 4(iii) and Supplementary Fig. 23). Since both of the two states, {[1·K]3++La3+} and {[1·La]5++K+}, were observable, the thermodynamically less stable state, {[1·K]3++La3+}, is thought to be a very stable kinetically trapped state.

Figure 3: Time course analysis of guest exchange from [1·K]3+ to [1·La]5+.

(a) Changes of the imine signals in the 1H NMR spectra (blue circle: K+ complex and yellow triangle: La3+ complex) in the absence/presence of tetrabutylammonium acetate (1.0 mM, CD3OD, 25 °C). (b) Plots of mole fractions of [1·La]5+ versus time after addition of K+ and La3+.

Figure 4: Guest recognition and exchange behaviours of 1(OTf)2.

When KOTf and La(OTf)3 were added to the metallohost 1(OTf)2 at once, the kinetically trapped state {[1·K]3++La3+} was generated (i). While the conversion from the kinetically formed K+ complex to the thermodynamically more stable La3+ complex was exceptionally slow (ii, iii), the guest exchange was significantly accelerated by the addition of tetrabutylammonium acetate (iv).

Interestingly, the addition of acetate ion markedly changed this situation. When 3 equiv of Bu4NOAc was present from the beginning, the exchange of K+ with La3+ took place much faster (Figs 3a(ii), b(ii) and and Supplementary Fig. 21). The reaction was accelerated by 75 times, which was estimated from the initial rates. Obviously, the addition of Bu4NOAc drastically accelerated the guest exchange. It is noteworthy that we can accelerate this metal exchange at any stage of the reaction. For example, when 3 equiv of Bu4NOAc was added after 120 h, [1·La]5+ started to immediately increase after the addition (Fig. 3b(iii) and Supplementary Fig. 22). Since almost no metal exchange had occurred before the addition, the acetate ion acted as a trigger to initiate the guest exchange reaction from the kinetically trapped state.

In the X-ray crystal structure (Fig. 5), the complex cation [1·La]5+ has three acetate and two triflate counteranions, among which only the three acetate ions coordinated to the La3+. This clearly demonstrates the complete binding selectivity of [1·La]5+ for acetate ion over triflate ion. The higher coordination ability of the acetate ions to La3+ probably contributes to the acceleration of the exchange of K+ with La3+ in the metallohost 1(OTf)2 (Fig. 4).

Figure 5: X-ray crystal structure of [1·La(OAc)3](OTf)2.

Hydrogen atoms are omitted for clarity except for those of the NH2 groups. The solvent molecules and two triflate anions are also omitted.


We synthesized a dicationic cobalt(III) metallohost 1(OTf)2 that has capping sites to hold the anion caps. The guest ion (Na+, K+, Rb+, Cs+, Ca2+ or La3+) was encapsulated in the O6 cavity of 1(OTf)2 in such a way that the two counteranions capped the guest cation. Uptake of La(OTf)3 by 1(OTf)2 was exceptionally slow (half-life 10 h) probably due to the capping effect of the triflate ion. This anion-capped structure enabled us to construct a host–guest system in which the guest exchange is accelerated in a time-programmable and on-demand manner. We believe that these results will open the way for the development of new functional materials in which the desired function is triggered by guest recognition not only by chemical stimuli but also by physical stimuli such as light or heat.


Materials and methods

Reagents and solvents were purchased from commercial sources and used without further purification. 1H NMR spectra were recorded on a JEOL JNM-ECS 400 (400 MHz). Chemical shifts in CD3OD were referenced with respect to the solvent residual peak (3.31 p.p.m.). Electrospray ionization time of flight (ESI-TOF) mass spectra were recorded on a Bruker Daltonics micrOTOF II spectrometer.

Synthesis of [LCo2(CH3NH2)4](OTf)2 (1(OTf)2)

A solution of macrocyclic ligand H4L (149 mg, 0.201 mmol)44,45 in chloroform (40 ml) was mixed with a solution of cobalt(II) acetate tetrahydrate (108 mg, 0.434 mmol) in methanol (12 ml), a solution of tetrabutylammonium trifluoromethanesulfonate (783 mg, 2.00 mmol) in methanol (12 ml) and then methylamine (40% in methanol, 2.0 ml). The resulting solution was stirred under air for 12 h. After the solution was concentrated to dryness, the residue was dissolved in acetonitrile and diethyl ether was added. The precipitated crude product was collected and dissolved in a small amount of methanol containing methylamine (40% in methanol, 1.0 ml). The solution was left for 3 h and then diethyl ether was added to give precipitates, which were collected by filtration. After repeating the purification by reprecipitation, the product was collected by filtration to give 1(OTf)2 (150 mg, 0.125 mmol, 62%) as a reddish brown powder. 1H NMR (400 MHz, CD3OD) δ 8.80 (s, 4H), 8.34–8.29 (m, 4H), 7.61–7.56 (m, 4H), 7.51 (dd, J=7.8, 1.4 Hz, 4H), 7.35 (dd, J=7.8, 1.4 Hz, 4H), 6.72 (t, J=7.8 Hz, 4H), 1.64 (s, 12H). ESI-MS m/z 1047.1 [1+OTf]+. Anal. Calcd for C46H44Co2F6N8O12S2·3MeOH·2H2O: C, 44.28; H, 4.55; N, 8.43. Found: C, 44.42; H, 4.81; N, 8.76.

X-ray crystallography

Intensity data were collected on a Rigaku Mercury diffractometer (with Mo Kα radiation, λ=0.71073 Å) or a Bruker SMART APEX II diffractometer (with Cu Kα radiation, λ=1.54178 Å). The data were corrected for Lorentz and polarization factors and for absorption by semi-empirical methods based on symmetry-equivalent and repeated reflections. The structures were solved by direct methods (SHELXS 97 (ref. 49) or SHELXT50) and refined by full-matrix least squares on F2 using SHELXL 2014 (ref. 51) (Supplementary Tables 1-3 and Supplementary Figs 15-19).

Data availability

Crystallographic data in this paper can be obtained free of charge via (or from the Cambridge Crystallographic Data Centre, 12 Union Road, Cambridge CB2 1EZ, UK). The deposit numbers are 1525963 ([1·K(OTf)2](OTf)), 1525964 ([1·La(OAc)3](OTf)2), 1525965 ([1·Na(OTf)2](OTf)), 1525966 ([1·Ca(OTf)2](OTf)2) and 1525967 (1(OTf)2). All other data are available in this article and in the Supplementary Information file.

Additional information

How to cite this article: Sakata, Y. et al. Anion-capped metallohost allows extremely slow guest uptake and on-demand acceleration of guest exchange. Nat. Commun. 8, 16005 doi: 10.1038/ncomms16005 (2017).

Publisher’s note: Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.


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This work was supported in part by JSPS KAKENHI (Grant Number JP16H06510 (Coordination Asymmetry) and JP26288022), the Noguchi Institute and Kanazawa University CHOZEN Project. We thank Dr Kenji Yoza (Bruker AXS KK) for the X-ray data collection for [1·K(OTf)2](OTf), [1·Ca(OTf)2](OTf)2 and [1·La(OAc)3](OTf)2.

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S.A. initiated the project and Y.S. designed the research; C.M. carried out all the experiments under the guidance of Y.S. and S.A. All authors contributed to analysing and interpreting the data, and Y.S. and S.A. co-wrote the manuscript.

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Correspondence to Shigehisa Akine.

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Sakata, Y., Murata, C. & Akine, S. Anion-capped metallohost allows extremely slow guest uptake and on-demand acceleration of guest exchange. Nat Commun 8, 16005 (2017).

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