Introduction

Multi-component self-assembly via reversible bond formation and non-covalent interactions typically affords highly symmetric structures, as commonly seen in nature1,2,3. Over the last four decades, extensive studies of coordination driven self-assembly have demonstrated methods to form a large variety of spheres, octahedra, cubes, tetrahedra and similar regularly shaped architectures consisting of rigid organic ligands and metal ions4,5,6. Recently, to increase complexity and functionality in such coordination-based nano-systems, several strategies that make use of mixtures of ligands have been developed7, including coordination sphere engineering8,9,10,11,12, shape-complementary assembly13,14,15,16, the use of non-symmetric ligands17,18,19, and backbone-centered steric hindrance20. However, multi-component self-assembly forming a C1-symmetric structure is still challenging owing to a large entropic disadvantage21, 22.

The three dimensional structures of biomolecules constructed by weak associating forces, such as hydrogen-bonds, cation-π, anion-π, and CH-π interactions, which are usually considerably weaker than metal–ligand coordination bonds, can often exhibit large structural changes promoted via guest recognition at their binding sites, called induced-fit and allosteric mechanisms23, 24. In many cases, rigid organic substrates will induce reorganization of the flexible binding pocket of an enzyme to increase guest affinity. In a similar way, the cooperative action of guest recognition and structural adaptivity within self-assembled 3D structures constructed by weak associating forces can endow a supramolecular system with additional complexity, providing a chance to afford an unusual low-symmetry structure as a thermodynamic product.

Resorcin[4]arene 1, one of the most classical compounds applied in supramolecular chemistry, is known to assemble into a highly symmetrical hexameric capsule in apolar solents ((1)6, Oh symmetry), comprising eight water molecules which are incorporated via a multitude of hydrogen-bonds (Fig. 1a)25. The resorcin[4]arene hexamer (1)6 features an octahedral cavity (1300 Å3) which was shown to exhibit remarkable catalytic activity for the conversion of small organic substrates with unusual product selectivity and rate acceleration, similar to enzymatic transformations26,27,28. The electron-rich aromatic walls, allowing cation-π interactions, and trapped water molecules which can act as mild Brønsted acids (pKa = 5.5 ~ 6) within the capsule framework were identified as key factors in this system. Our group has previously utilized this hydrogen-bonded hexameric capsule for the encapsulation of luminescent coordination complex salts, forming supramolecular complexes insulated from bulk solvent. As a result, encapsulation-induced emission enhancement (EIEE) behavior was observed for the guest complex29,30,31,32.

Fig. 1: Self-assembly of hydrogen-bonding resorcin[4]arene host.
figure 1

a Formation of a hexameric capsule with eight water molecules. b Symmetry-breaking assembly via host–guest complexation. c Compounds used in this study.

Full size image

Encapsulation of tertiary ammonium cations, which are typical guests for the hexameric capsule, has been mainly studied in solution and in the solid state33. Little is known about the gas phase structures of such host–guest complexes as they easily show fragmentation under usual mass spectrometry measurement conditions such as electrospray ionization34. In contrast, cationic coordination complexes possess larger and more rigid structures as compared to tertiary ammonium cations, which can serve as templates to strongly stabilize discrete resorcin[4]arene oligomers even in the gas-phase34. This observation can be explained by a snug fit of the guest’s large surface area, giving rise to significant stabilization via cation-π and CH–π interactions.

Herein we report the symmetry-breaking behavior of supramolecular complexes forming from a hexameric resorcin[4]arene capsule and luminescent coordination complexes via molecular recognition (Fig. 1b). The coordination complex, carrying sterically demanding substituents, causes a significant structural perturbation of the hydrogen-bonded capsule, away from its typical and thermodynamically most stable solution structure with Oh symmetry, to a defined low-symmetry assembly stabilized by noncovalent host-guest interactions and multiple hydrogen-bond networks. Hence, the C2-symmetric coordination complex combined with the Oh-symmetric hydrogen-bonded resorcin[4]arene capsule leads to a symmetry-breaking phenomenon to afford a C1-symmetric supramolecular complex. Notably, this leads to a rare encapsulation phenomenon, EIEE, for the guest. Furthermore, the symmetry-breaking effect desymmetrizes ED and MD transition moments in the radiative process (emission) of the chiral-at-metal coordination compound within the resorcin[4]arene oligomer, resulting in an increase of the dissymmetry factor glum in the complex’s circularly polarized luminescence (CPL) property.

Results

Encapsulation of Ir complexes

The host–guest complex (1)6⊃([2]Cl) was obtained via the following process regarding the self-assembly of (1)6 and encapsulation of [2]Cl (Supplementary Fig. 2). First, simple mixing of CDCl3 solutions of (1a)6 and [2a]Cl in a 1: 1 ratio at room temperature showed upfield shifts of aromatic protons in the 1H NMR spectrum of [2a]+, as compared with that of free [2a]Cl in CDCl3 (Fig. 2b–d). The doublet signal at 9.12 ppm, assigned to the 3,3’-protons on the 2,2’-bipyridine moiety in [2a]Cl, is sensitive to the presence of a chloride ion owing to a strong chelating hydrogen-bond formed with the anion35. The resorcin[4]arene capsule initially expels the chloride ion from the complex cation because of the stronger hydrogen-bonding nature of phenolic protons in the hexameric capsule (1a)631, leading to a significant upfield shift of the doublet peak in [2a]+ after mixing the solution of (1a)6 and [2a]Cl (Fig. 2d). During heating the mixture at 50 °C, partial dissociation of 1a from the assembly is likely to form a portal in the hydrogen-bonded hexameric capsule and encapsulation of [2a]+ within the resorcin[4]arene capsule proceeds to afford the host–guest complex (1a)6⊃([2a]Cl)31. The 1H NMR spectrum recorded after heating for 1 h clearly showed that a singlet peak of tBu substituents in [2a]+ appeared at −0.61 ppm owing to the shielding effect from the host, suggesting that the Ir complex was trapped inside the resorcin[4]arene capsule (Fig. 2e). Very interestingly, the host–guest complex (1a)6⊃([2a]Cl) showed severe signal splitting in the 1H NMR spectrum. This is probably caused by a strong template effect from [2a]+ which can effectively suppress some molecular dynamics, such as self-assembly and encapsulation equilibria in (1a)6⊃([2a]Cl), rapid rotation of [2a]+ within the resorcin[4]arene capsule, and hydrogen-bond recombination of the capsule on the NMR time scale. A variable temperature (VT) NMR study revealed that the molecular dynamics were still slow even at elevated temperature on the NMR time scale (Supplementary Fig. 5). Diffusion-ordered NMR spectroscopy (DOSY) showed a single band at diffusion coefficient D(host-guest)=3.6 ± 0.4 × 10−10 m2 s−1 and significant reduction with respect to the diffusion coefficient of free [2a]+ (D(free Ir)=7.0 ± 0.5 × 10−10 m2 s−1, D(host-guest)/D(free Ir) ≈ 0.50), suggesting that the solution mainly contained a single supramolecular species and the Ir complex was strongly trapped within the resorcin[4]arene capsule via multiple cation-π interactions and ion-pair formation within the cavity (Fig. 2f and Supplementary Fig. 6).

Fig. 2: Symmetry-breaking assembly consisting of resorcin[4]arene and cationic Ir complex.
figure 2

a Schematic representation of the assembly. 1H NMR spectra (500 MHz, CDCl3, RT) of b resorcin[4]arene hexameric capsule (1a)6, c Ir complex [2a]Cl, d a mixture of (1a)6 and [2a]Cl, e the mixture after heating at 50 °C for 1 h, and f partial 1H DOSY spectrum of the host–guest complex showing the diffusion coefficient (D) around 3.6 ± 0.4 × 10−10 m2 s−1. The signals marked with beige filled circles indicate the encapsulated Ir complex.

Full size image

Symmetry analysis of the host-guest complex

The molecular symmetry of the resorcin[4]arene capsule drastically reduced from Oh to C1 symmetry by encapsulation of the large guest [2a]+, judging from the severe peak splitting and the single diffusion coefficient of the host–guest complex in the 1H DOSY spectrum. The symmetry lowering of self-assembled molecular hosts has typically been observed in host–guest systems using rigid coordination-driven metallocages, when guest molecules are tightly bound and the motions of guests are restricted within the cages36,37,38. Thus, this is indeed a rare NMR observation for the desymmetrization of an otherwise rather flexible resorcin[4]arene hydrogen-bonded system39.

For symmetry analysis of the host–guest complex (1a)6⊃([2a]Cl), 1H–13C heteronuclear single quantum correlation (HSQC) spectroscopic analysis was utilized for the assignments of the NMR signals in this host–guest system (Fig. 3). The HSQC spectrum clearly discriminates the cross peaks derived from the host and the guest complex, clarifying the structural aspects of the assembly. The aromatic proton of free 1a at 6.2 ppm splits into 24 signals observed at around 5 to 7 ppm in the 1H NMR spectra (100 to 110 ppm for the corresponding carbon atoms in the 13C NMR spectra), indicating that all resorcin[4]arene units are fixed in non-equivalent environments around the guest on the NMR time scale (Supplementary Fig. 11).

Fig. 3: 1H–13C heteronuclear single quantum correlation (HSQC) spectrum (1H: 800 MHz, CDCl3, 298 K) of the mixture of [2a]Cl and (1a)6⊃([2a]Cl).
figure 3

The cross peaks marked with black and encircled numbers are assigned to the protons of free [2a]+ and entrapped [2a]+, respectively. The upfield (<0) and downfield shifts (>0) in the 1H NMR spectrum caused by the host–guest formation are shown as Δδ in parentheses.

Full size image

Signals 1–7 assigned to the pyridine protons of [2a]+ are considerably shifted to the upfield region (Δδ = −0.8 ~ −3.5 ppm) and, in contrast, protons 8–11 at the phenyl moieties show a downfield shift (Δδ = 0.25 ~ 0.7 ppm) on host–guest formation. As guest signals typically show upfield shifts upon encapsulation, owing to the shielding effect from the hosts, this HSQC spectrum suggests that the pyridine moieties of entrapped [2a]+ were located within the hexameric capsule, while the phenyl moieties were not covered by the capsule. More interestingly, protons 1, 2 and 4–8 are clearly split into two peaks, suggesting that two ppy ligands and two pyridine moieties in the bpy ligand in [2a]+ are located in an asymmetric environment generated by the distorted hexameric capsule to lower the molecular symmetry of the host–guest complex on the NMR time scale. Therefore, this HSQC result clearly indicates that the host–guest complexation of hexameric capsule (1)6 with Oh symmetry and [2a]Cl with C2 symmetry leads symmetry-breaking to afford a C1-symmetric compound as the thermodynamic product.

Coordination-driven supramolecular architectures were previously shown to undergo dynamic transformations via guest binding, as seen in induced-fit molecular recognition mechanisms23, 24. Such biomimetic functions belong to important challenges in supramolecular chemistry40, 41. Although individual association forces in the system studied herein are weaker and less directional than typical coordination bonds, our results show that the cooperation of multiple weak interactions can control the structure and symmetry of the final product, in particular, achieving the formation of an unusual C1-symmetric assembly.

Solution structure of the distorted hexameric capsule

To gain further structural information about the symmetry-breaking assembly, we carried out several 2D NMR experiments for determining the relative orientation between the host and the guest molecules. A VT-HSQC measurement at 50 °C showed significant broadening of the peaks of the resorcin[4]arene molecules around 5.7 and 6.3 ppm, while other peaks were still sharp and slightly shifted (Supplementary Fig. 12). This suggests that two resorcin[4]arene units in the distorted hexameric capsule are relatively flexible, as compared with the other four resorcin[4]arene units. Furthermore, the Rotating-frame Overhauser Effect Spectroscopy (ROESY) spectrum showed that the flexible resorcin[4]arene units correlate to guest protons 8 to 11. Therefore, it was concluded that the flexibility of the host originates from weaker interactions of the host’s electron-rich aromatic moieties with the guest.

A 1H–1H Nuclear Overhauser Effect Spectroscopy (NOESY) experiment revealed that the sharp signal at –0.61 ppm in the 1H NMR spectrum, assigned to the tBu groups in [2a]+, gives eight cross-peaks with rigid 1a (Supplementary Fig. 8). It suggests that two resorcin[4]arene units cover the tBu groups and fix their orientation owing to effective CH–π interactions. The signal at 5.4 ppm of 1a shows two cross-peaks with guest protons 3 and 8 in the ROESY spectrum, implying that the pyridine moieties in the guest are recognized by the concave cavities of the resorcin[4]arene molecules, probably because the electron-rich aromatic walls of the host effectively capture the electron-deficient pyridyl units (Supplementary Fig. 9).

We propose that these different binding modes concertedly serve to form an asymmetric cavity in the distorted hexameric capsule. A partial structure of such a binding motif could be visualized by a single crystal X-ray analysis of Ru complex analogue [3a]Cl2 with 1c (Supplementary Fig. 32). A molecular model was built based on the X-ray structure of (1c)3⊃[3a]2+ and 2D NMR results of (1a)6⊃([2a]Cl), implying that the distorted hexameric capsule formed an open structure around the guest (Supplementary Fig. 16). As the capsule structure of resorcin[4]arene hexamer (1a)6 is stabilized by multiple hydrogen-bonds with the eight contained water molecules, the distorted hexameric capsule structure of (1a)6⊃([2a]Cl) should also be supported by the incorporation of several water molecules42.

The effect of ligand bulkiness and counter anions

In this symmetry-breaking assembly, steric bulkiness of the Ir complex salt plays a crucial role in forming the remarkably low-symmetric structure. When the sterically less demanding Ir complex [2b]Cl was used as a guest instead, containing methyl (Me) substituents on the bpy ligand instead of tertiary butyl (tBu) groups as in [2a]Cl, the 1H NMR study revealed that encapsulation of [2b]Cl within the resorcin[4]arene hydrogen-bonded capsule proceeded to give a more common type of host–guest complex, showing a higher averaged symmetry due to the larger mobility of the smaller guest inside the cavity (Supplementary Fig. 22). On the other hand, an Ir complex having even larger substituents (phenyl groups) on the bpy units, [2c]Cl, did not yield any host–guest complex in solution, as judged from a 1H NMR study (Supplementary Fig. 25). This can be rationalized with the increased size of the Ir complex which is too large to be encapsulated within the hexameric capsule and the shape of [2c]+ does not template any other resorcin[4]arene oligomer. Therefore, these results demonstrate that this symmetry-breaking assembly is a size- and shape-specific molecular recognition phenomenon in solution.

In addition, an anion-dependent behavior was observed distinctly. When the counter anion Cl– was replaced with NO3–, host–guest complexation also proceeded, as confirmed by NMR studies (Supplementary Fig. 17). Notably, the proton signals in 1a are severely broadened and the molecular symmetry of the guest stays C2 on the NMR time scale after encapsulation. It implies that the NO3– anion weakens the hydrogen-bond network in the capsule and thus increases the flexibility of 1a, producing a symmetric cavity. On the other hand, large anions (PF6–, BF4–, ClO4–, and OTf–) did not show host–guest formation (Supplementary Fig. 21). The typical hexameric capsule can accommodate a cationic guest molecule as its ion-pair through hydrogen-bonds between weakly acidic H2O molecules in the capsule framework and hydrogen-bond accepting anions31, 33. Thus, the anions also participate in the self-assembly process and are able to control the flexibility of the supramolecular structure43. Recently, it has also been reported that hydrogen-bonds between a resorcin[4]arene capsule and Cl anions afforded an anion-sealed capsule to produce a larger internal cavity in weakly anion-solvating solvents, such as THF and benzene, while not being stabilized by ammonium cations in chloroform44. For our system, we propose that the formation of an enlarged capsule, capturing a Cl anion in the hydrogen-bonding network, is likewise possible owing to the template effect of the rather large Ir complex guest. Apparently, this process is favored over ion-pair formation of the guest salt within the neutral hexameric capsule. Although the solution structure of this symmetry-breaking assembly still remains uncertain, these results definitely reveal that the cooperative effect among the guest cation, Cl anion, and hydrogen-bonded hosts plays a crucial role to form this remarkable assembly.

Encapsulation-Induced Emission Enhancement (EIEE)

The photoluminescent properties of the Ir complex guests, originating from metal-to-ligand charge transfer (3MLCT) and triplet ligand-to-ligand charge transfer (3LLCT) excited states (Supplementary Fig. 50)45, are significantly modulated after encapsulation within the hydrogen-bonded capsule as compared with their free forms in solution, owing to drastic changes of local environments around the guests by formation of highly aggregated structures46. The emission spectrum of encapsulated [2a]Cl (λem = 564 nm) shows a large blue shift (Δλem = −19 nm) from that of free [2a]Cl (λem = 583 nm) after mixing of 1a (60 μM, 6 eq.) and heating the mixture at 50 °C for 1 min (Fig. 4). In addition to the blue shift of the emission, higher emission quantum yields (Φ) and longer emission lifetimes (τave) were observed, rising from 40% and 510 ns to 63% and 1020 ns, respectively. Further addition of 1a (300 μM, 30 eq.) into the solution of [2a]Cl enhances the photoluminescent properties (λem = 562 nm, Φ = 73%, τave = 1090 ns) of (1a)6⊃([2a]Cl) even further, because the supramolecular structure is formed via two coupled equilibrium processes (self-assembly of 1a and encapsulation of [2a]Cl), and therefore a high concentration of 1a favors the formation of the host–guest complex. The non-radiative rate constants (knr) of the photoluminescence were significantly reduced by addition of 1a, indicating that the tight host–guest complex formation effectively suppressed the molecular dynamics of [2a]+ and showed EIEE behavior. It is noted that this EIEE behavior was also observed with guests [2a]NO3 and [2b]Cl (Supplementary Fig. 37 and 39), which were also entrapped within the symmetric hexameric capsule (1a)6, while the photoluminescent properties of [2a]PF6 and [2c]Cl were not significantly altered since they cannot fit inside the cavity of the resorcin[4]arene oligomer (Supplementary Fig. 38 and 40).

Fig. 4: Normalized emission spectra of [2a]Cl (10 μM) with various amounts of resorcin[4]arene monomer 1a (0, 60, 300 μM).
figure 4

The solutions containing [2a]Cl and 1a were heated at 50 °C for 1 min before the measurements (λex = 400 nm).

Full size image

Symmetry-breaking triggers modulation of chiroptical properties

Although these host–guest complexes showed an EIEE behavior, the symmetry-breaking effect in (1a)6⊃([2a]Cl) was not observed clearly in the luminescent properties as discussed above. Therefore, we next investigated symmetry-dependent photophysical properties of the Ir complexes. The chiral-at-metal Ir complexes are obtained as a 1:1 racemic mixture of Δ- and Λ-stereoisomers in a typical synthetic manner. The optical resolution of the mixture can give enantiopure complexes showing CD and CPL properties, which directly reflect the structural information in the molecular system47.

The enantiopure Ir complexes Δ-[2]Cl and Λ-[2]Cl were obtained by auxiliary-mediated asymmetric synthesis according to established methods (Supplementary Fig. 1)48, 49. The CD spectra of Δ- and Λ-[2]Cl clearly showed mirror image spectra irrespective of their counter anions, indicating that the enantiopure Ir complexes possessed opposite metal-centered configuration (Supplementary Fig. 45). Upon addition of 1a into the solution containing Δ- or Λ-[2a]Cl, respectively, gradual spectral changes were observed in the CD spectra of the Cl salts (Fig. 5a), while those of the PF6 salts did not change significantly (Supplementary Fig. 48a). As the PF6 salt is not encapsulated within the capsule as confirmed by NMR studies, the spectral change in Fig. 5a unambiguously originates from the formation of the host–guest structure. In particular, the cotton effect around 420 nm, which derives from the chiral Ir complex, gradually blue shifts upon addition of 1a. These results therefore indicate that encapsulation within the hydrogen-bonded capsule can slightly alter the chiroptical property of the chiral guests. Since resorcin[4]arene absorbs light only in high energy UV region (<320 nm), chiral information transfer on the capsule might be observed due to the encapsulation of a chiral guest50. However, it should be noted that these results are still indirect evidence of the symmetry-breaking effect upon the host–guest assembly, because the CD spectra of smaller chiral Ir complex Δ- and Λ-[2b]Cl were also altered upon addition of 1a into the solution (Supplementary Fig. 49a).

Fig. 5: Chiroptical properties of the complexes.
figure 5

a Circular dichroism (CD) spectra (10 μM, CHCl3, RT) of Δ- and Λ-[2a]Cl in the presence of resorcin[4]arene 1a (0, 30, 60, 120 μM). b Normalized circularly polarized luminescence (CPL) spectra (50 μM, CHCl3, RT) of enantiomerically pure Ir complex [2a]Cl (50 μM) with resorcin[4]arene monomer 1a (0, 300, 600 μM), which was obtained from division of the 2ΔI curve by the maximum of the emission intensity. All samples solutions containing [2a]Cl and 1a were heated at 50 °C for 1 min before the measurements.

Full size image

Stronger evidence of the symmetry-breaking clearly derives from the circularly polarized luminescence (CPL) studies. CPL analysis allows to probe specifically the chiral Ir complexes47, since the resorcin[4]arene hydrogen-bonded capsule are not emissive. Comparison between free and encapsulated complexes in hexameric hosts provides a unique perspective on how the symmetry-breaking affects the chiroptical properties of the system. The Δ- and Λ-configured complexes [2a]Cl in degassed CHCl3 upon excitation at 350 nm clearly show right- and left-handed CPL effects (λmax = 580 nm), respectively, with a dissymmetry factor glum = 2 × 10−4 (Fig. 5b). After addition of resorcin[4]arene 1a into the solution and heating at 50 °C for 1 min, EIEE effects in the CPL properties are observed as a consequence of the host–guest formation as well as changes in the chirality-independent luminescent properties, including blue shift of the emission peak (λmax = 530 nm) and enhancement of the emission intensity in the CPL spectra (Supplementary Fig. 46). Surprisingly, the dissymmetry factor glum of the CPL increases fourfold (8 × 10−4) by the symmetry-breaking host–guest formation event (Fig. 5b). According to the physical theory, the glum value is related to the ED and MD transitions moments in the radiative process (emission) as follows:

$${g}_{{{{{{\rm{lum}}}}}}}=4|{{{{{\boldsymbol{\mu }}}}}}||{{{{{\boldsymbol{m}}}}}}|\cos \theta /({|{{{{{\boldsymbol{\mu }}}}}}|}^{2}+{|{{{{{\boldsymbol{m}}}}}}|}^{2})$$
(1)

where μ is the transition ED moment, m is the transition MD moment, and θ is the angle between μ and m51. As the free Ir complexes possess C2 molecular symmetry, two phenylpyridinato ligands at the Ir metal center and two pyridine moieties in the bipyridine ligand are equivalent. On the other hand, after the symmetry-breaking assembly, the molecular symmetry in the supramolecular system lowers to point group C1, leading to desymmetrization of the chemical environment of the organic ligands (Fig. 2a). Therefore, after vibrational relaxation of the excited state structure upon sensing the asymmetric environment originated from symmetry-breaking assembly, the vectors of the transition ED moment (μ) and the transition MD moment (m) in the host–guest assembly should differ from those of the free Ir complex (Supplementary Fig. 51). In fact, the dissymmetry factor glum of the CPL properties of chiral [2a]NO3 and [2b]Cl did not change significantly upon addition of 1a, although the EIEE effect in the CPL spectra of chiral Ir complex salts, that is the blue shift of the emission peak and increase of the emission intensity in the CPL spectra, was observed similarly to the case of [2a]Cl with 1a (Supplementary Fig. 47 and 49). This is probably because these two Ir complex salts gave host–guest complexes without forming the symmetry-breaking assembly, supported by matching observations in the NMR studies. Thus, these CPL results are a clear evidence of the symmetry-breaking in the supramolecular assembly with guest [2a]Cl52. A careful design of the supramolecular system allows to couple the EIEE effect with an enhancement of the chiroptical properties, providing a new strategy for tuning the efficiency of CPL emitting materials.

This study showed the formation of C1-symmetric supramolecular coordination complexes insulated by resorcin[4]arene oligomers in solution. Although resorcin[4]arenes typically form symmetric hydrogen-bonded capsules, encapsulation of shape-specific coordination complexes caused a structural change of the symmetric host frameworks to afford a distorted hexameric capsule in solution, creating asymmetric environments inside the oligomer, where the organic ligands of the guests are located in nonequivalent positions. The structures of the symmetry-breaking assemblies in this supramolecular system were elucidated by extensive 2D NMR spectroscopic analyses. CD and CPL measurements in solution revealed that the encapsulated chiral metal complexes are strongly affected by the surrounding asymmetric environment. The synergistic effect of weak interactions between the components is a key to construct these C1-symmetric assemblies, because the combination of multiple weak interactions can provide enough enthalpic gain to overcome the large entropy loss of C1-symmetric products in the multi-component self-assembly. As the distribution of the weak binding forces is basically controllable by a tuning of reaction conditions, thus, the present strategy might provide a useful methodology to bring more complexity and flexibility into self-assembled nano systems. The preparation of relatively large anisotropic, yet defined supramolecular architectures based on chiral components bears potential to develop new applications in areas such as molecular chiroptical materials, selective luminescent diagnostics and homogeneous enantioselective photocatalysis.

Methods

The 1H and DOSY NMR spectra were obtained on a 500 MHz Varian NMR System 500PS spectrometer. 2D NMR measurements were conducted by using a Bruker Avance III 800 spectrometer. Chemical shifts are reported as values in p.p.m. relative to tetramethylsilane (δ = 0) in deuterated solvents. Electrospray ionization (ESI), tandem mass, and ion mobility spectrometry were performed on a Bruker ESI timsTOF mass spectrometer. UV/Vis absorption spectra, emission spectra, emission lifetime decay profiles, and emission quantum yields were obtained on a Jasco V-560 spectrophotometer, Jasco FP-6500 spectrofluorometer, a Hamamatsu Photonic Absolute PL Quantum Yield Measurement System C9920-02 integrating sphere and a PMA-12 multichannel photodetector (excitation wavelength = 420 nm), and a Hamamatsu C11200 streak camera as a photodetector by exciting at 355 nm using a nanosecond Q-switched Nd:YAG laser (Continuum Minilite), respectively. The CD spectra were collected on a Jasco J-75W CD spectrometer. The CPL spectra were recorded on a JASCO CPL-300 spectrophotometer, equipped with a 150 W Xenon lamp and a PMT detector. All CPL measurements were carried out at room temperature, whose spectra correspond to an average of 10 scans with a fixed excitation bandwidth of 25 nm, a fixed emission bandwidth of 15 nm and an integration time of 1 s. All photophysical measurements were performed under deaerated conditions after N2 bubbling for 30 min.