Open Access Article
Karolína Salvadori
*abc,
Sabrina Pricl
de,
Aura Tintarub,
Alena Krupková
c,
Václav Eigner
f,
Pavel Matějka
g,
Pavel Lhoták
h and
Olivier Siri
*b
aDepartment of Analytical Chemistry, University of Chemistry and Technology, Prague (UCTP), Technicka 5, 166 28 Prague 6, Czech Republic. E-mail: salvadok@vscht.cz
bAix-Marseille Université, CNRS UMR 7325 Centre Interdisciplinaire de Nanoscience de Marseille (CINaM), Campus de Luminy, Marseille cedex 09 13288, France. E-mail: olivier.siri@univ-amu.fr
cInstitute of Chemical Process Fundamentals of Czech Academy of Sciences v.v.i., Rozvojová 135, Prague 6, 16502, Czech Republic
dMolecular Biology and Nanotechnology Laboratory (MolBNL), Department of Engineering and Architecture (DIA), University of Trieste, Piazzale Europa 1, 34127 Trieste, Italy
eDepartment of General Biophysics, Faculty of Biology and Environmental Protection, University of Lodz, ul. Pomorska 141/143, 90-236 Łódź, Poland
fInstitute of Physics AS CR, v.v.i., Na Slovance 2, 182 21 Prague 8, Czech Republic
gDepartment of Physical Chemistry, University of Chemistry and Technology, Prague (UCTP), Technicka 5, 166 28 Prague 6, Czech Republic
hDepartment of Organic Chemistry, University of Chemistry and Technology, Prague (UCTP), Technicka 5, 166 28 Prague 6, Czech Republic
First published on 28th April 2026
The reaction of tetranitro-tetraminoazacalix[4]arene with a series of aromatic isocyanates leads to the formation of tetraureido-receptors, whose isolation was efficiently achieved (∼80% yield) by organic solvent nanofiltration when conventional chromatographic methods proved ineffective. The receptors exhibit a pronounced tendency to self-aggregate in solution, and the extent and stability of the formed assemblies are strongly modulated by the nature of the aryl substituents. A combined experimental (dilution NMR, DOSY) and theoretical investigation revealed that dimer formation arises from a cooperative interplay between π–π interactions and hydrogen bonding, with aromatic stacking providing the dominant stabilizing contribution. Molecular dynamics simulations highlight significant differences in the stability of selected dimers, rationalizing their distinct aggregation tendencies. X-ray analysis reveals that while π–π stacking remains significant even in the solid state, the ureido motifs preferentially coordinate solvent molecules. Importantly, receptor self-association does not prevent anion recognition. Even in the strongly hydrogen-bond-competitive solvent (DMSO), the receptors efficiently bind anions, exhibiting a selectivity sequence H2PO4− > BzO− > AcO− ≫ Cl−, that cannot be rationalized solely by anion basicity. These findings demonstrate that tetraureido tetranitro-azacalix[4]arene architectures represent substitution-tunable supramolecular systems that combine controlled self-assembly with robust anion complexation ability.
Among the various anion-binding motifs explored to date, ureido groups have attracted considerable attention as versatile supramolecular units, combining strong and highly directional hydrogen bonding with a relatively low propensity for deprotonation.7 Compared with amide-based receptors,8 which often display weaker binding, and with more acidic donors such as thioureas9 and sulfonamides10 that may undergo deprotonation in the presence of basic anions, ureido-based systems provide an optimal balance between binding strength and chemical stability.
Early approaches to receptor design predominantly focused on podand-type systems, including open-chain monoureido structures (Fig. 1, compound A). Despite their structural simplicity, several derivatives were shown to form well-defined intermolecular assemblies governed by complementary N–H⋯O hydrogen bonds and π–π interactions between aromatic units.11,12 In terms of anion-binding properties, various bis(phenyl)urea receptors have been extensively studied. For example, it has been shown that bis(4-nitrophenyl)ureido receptor A binds anions in acetonitrile primarily according to their basicity (KAs): AcO− > BzO− > H2PO4− > NO2− > HSO4− > NO3−.13
The incorporation of additional functional elements to modulate solubility, aggregation propensity, binding affinity, and selectivity represents a natural step in the evolution of ureido-based receptors. On this basis, more complex polyureido architectures have been developed, in which multiple ureido motifs are preorganized through linkers such as m-phenylene units14 or anchored to flexible scaffolds, including tris(2-aminoethyl)amine15–17 and dendrimer-based frameworks18,19 (Fig. 1, B–D).
A further conceptual step involves macrocyclic platforms,20 where preorganization improves recognition efficiency by minimizing the entropic penalty of binding, and an appropriate degree of structural rigidity ensures high binding affinity while simultaneously suppressing non-specific interactions.
Within macrocyclic receptors, the ureido motif can fulfil different structural roles: they may constitute integral components of macrocyclic frameworks (like glycoluril in bambusuril21), serve as a bridging element embedded within the macrocyclic backbones (e.g. E,22 F
23), or function as an appended binding site on preorganized scaffolds (e.g. G,24 H
25). These distinct design strategies enable precise control over the cavity size, shape, or spatial orientation of the binding sites, rendering ureido-containing macrocycles particularly attractive for advanced host–guest chemistry. However, while multivalent ureido architectures offer enhanced recognition capability, they are inherently susceptible to pronounced self-aggregation.26 This often-overlooked phenomenon can complicate both purification and the reliable interpretation of binding data. Despite these challenges, the practical and conceptual importance of developing new, effective ureido-based anion receptors remains undeniable (Fig. 2).
![]() | ||
| Fig. 2 Examples of macrocyclic receptors featuring ureido motif as a bridging element (E, F), or appended unit (G, H). | ||
Our recent work27 described a series of acyclic and macrocyclic anion receptors containing 4-tert-butylphenylureido motifs and demonstrated that modulation of the electron-density distribution of the supporting scaffold strongly influences interactions with basic anions, leading either to undesired deprotonation (in acyclic systems) or to anion complexation (in macrocyclic receptors). Building on these findings, the present study reports a new family of tetraureido derivatives preorganized on a tetranitro-azacalix[4]arene platform, with particular emphasis on elucidating the relationship between the nature of the aryl substituent and the resulting supramolecular properties, including both host–host aggregation and host–guest anion recognition.
The crude reaction mixtures containing isocyanate decomposition by-products (mainly symmetric ureas 7) were initially purified by preparative thin-layer chromatography (prep-TLC) on silica gel, affording isolated yields of approximately 70% for several derivatives. However, for some tetraureido derivatives (6C and 6E), chromatographic purification proved inefficient. This difficulty can be attributed to the limited solubility of these compounds in common solvents. To overcome these limitations, organic solvent nanofiltration (OSN) using a regenerated cellulose membrane29 was employed. This alternative purification strategy exploits the molecular size difference between the target receptors and impurities. For 6C (Fig. S13), dissolution of the crude reaction mixture in DMF diluted with MeOH to decrease viscosity (and to disrupt hydrogen bonding between product and impurities) allowed filtration through the membrane. The progress of the separation was followed by checking the color of the filtrate. Here, 5–6 filtration cycles were sufficient to obtain pure 6C, recovered from the retentate in approximately 80% yield.
Following the purification, the structures of receptors 6A–E were confirmed by a combination of nuclear magnetic resonance (NMR) spectroscopy and high-resolution mass spectrometry (HRMS) techniques. The choice of solvent played a key role in the NMR analysis (Fig. S23), and highly competitive DMSO-d6 was employed to gain well-resolved spectra. In the 1H NMR records, all receptors 6 displayed characteristic signals corresponding to the macrocyclic platform, including the bridging NH protons (∼9.5 ppm) and 4 singlets assigned to the aromatic C–H protons of azacalix[4]arene (∼9.1; 8.7; 7.1 and 5.5 ppm). In addition, two singlets corresponding to the ureido NH protons and the anticipated aromatic signals of the substituents were observed. The spectral patterns are consistent with the expected C2 symmetry of the products.
Despite this overall similarity, noticeable differences were observed among derivatives 6A–E. Particularly, in concentrated solutions, the aromatic signals appeared broadened and poorly resolved (Fig. 3a and Fig. S24), suggesting a dynamic process in solution. Upon heating to higher temperatures (Fig. S13b), these features gradually changed, with the aromatic C–H bond signals sharpening, while the ureido NH signals showed noticeable shifts. These observations pointed to a temperature-dependent equilibrium, likely associated with intermolecular interactions. To further investigate this behavior, concentration-dependent 1H NMR experiments were conducted to evaluate the potential self-aggregation of these compounds. With the exception of receptor 6A, bearing a strong electron-donating substituent, dilution-induced upfield shifts of the ureido NH signals, consistent with partial dissociation of self-aggregated species (Fig. S26–S29), were observed. Analysis of the dilution data using Bindfit software30 afforded corresponding equilibrium constants K following the order 6C ≫ 6E > 6D > 6B (Table S1), clearly indicating substituent-dependent aggregation strength.
Based on these results, receptor 6C was selected for further investigation of its aggregation behavior. Due to the strong absorption and fluorescence arising from the naphthyl moieties, dynamic light scattering (DLS) measurements were not feasible. Instead, concentration-dependent diffusion-ordered spectroscopy (DOSY) NMR experiments31 were carried out. As shown in Fig. 3b, increasing the concentration of 6C leads to slower diffusion, whereas the solvent diffusion remains unchanged. The appearance of new signals at more negative log
D values at higher concentration indicates the formation of larger species. Then, the values of the hydrodynamic radii Rh for the molecular species in solution were estimated using the Stokes–Einstein equation (eqn (1)):
![]() | (1) |
D = −9.5) in diluted solution and Rh ≈ 0.9–1.1 nm (log
D = −9.9 to −10) at higher concentration are consistent with the formation of small self-associate aggregates.
To gain molecular-level insight into the distinct aggregation behavior of 6C and the less-aggregating receptor 6B, molecular dynamics (MD) simulations were performed on their dimeric assemblies in explicit DMSO (Fig. S30), where solvent effects and molecular flexibility play a dominant role. The structural stability of the dimers was evaluated by monitoring several descriptors along the trajectories, including the total number of intradimer hydrogen-bond (HB)contacts, the fraction of native contacts (Q), the center-of-mass distance between monomers (dCOM–COM), and π–π stacking parameters (Fig. 4).
The evolution of intradimer HB contacts provides an initial measure of interfacial cohesion (Fig. 4a). The 6C dimer maintains a consistently high number of HB contacts throughout the 500 ns simulation, with only limited fluctuations. These persistent HBs likely contribute to the overall structural integrity of the assembly, helping to orient the aromatic platforms in a favorable geometry for aggregation. In contrast, 6B shows a gradual decline in intradimer HBs over time, indicative of reduced internal stabilization.
Analysis of the native contacts fraction (Q) further highlights the divergent stability profile of the two systems (Fig. 4b). For 6C, Q remains high and nearly constant (∼0.93), indicating preservation of the initial inter-residue contacts defining the dimer interface. This stability suggests minimal conformational drift and supports a compact, native-like organization across the entire trajectory. Conversely, 6B exhibits a continuous and marked decline in Q (from ∼0.95 to ∼0.75), reflecting progressive disruption of the interface and structural rearrangement. The observed behavior is likely caused by internal strain and steric hindrance from the bulky tert-butyl groups, which impede maintenance of a stable dimer.
The evolution of the center-of-mass distance (dCOM–COM) between monomers provides a direct measure of supramolecular association (Fig. 4c). In the case of 6C, dCOM–COM remains remarkably stable at approximately 4.0 Å, indicating that the two macrocycles remain tightly associated. In contrast, 6B displays a pronounced and progressive increase in dCOM–COM, ultimately exceeding 6.0 Å. This behavior is consistent with partial separation of the monomers and gradual loss of compact dimer organization.
The analysis of π–π stacking geometries provide insight into the aromatic interactions stabilizing the dimers (Fig. 4d). The 6C dimer exhibits a narrow and well-defined distribution of interplanar distances (3.5–4.5 Å) and angles (<30° or >150°), consistent with a persistent face-to-face stacking arrangement. This ideal geometry is maintained throughout the simulation and is likely a key contributor to the overall rigidity and cohesion of the 6C assembly. On the other hand, 6B displays a broader and more scattered distribution of stacking parameters. Although the initial geometry briefly falls within the optimal range, the stacking progressively deteriorates over time, with interplanar distances increasing and angles becoming highly variable. This pattern reflects a gradual loss of π–π overlap, most likely due to steric hindrance imposed by the tert-butyl substituents, which interfere with close aromatic alignment. The resulting differences appear to be rooted in both electronic and steric effects: while the planar, extended aromatic surface of 6C facilitates effective stacking and compact assembly, the bulkier architecture of 6B disrupts optimal packing, leading to dynamic instability and impaired supramolecular integrity.
To complement the structural insights, component-wise decomposition of the binding free energies was performed using the Molecular Mechanics/Poisson-Boltzmann Surface Area (MM/PBSA) approach (Fig. 5a).32 In both systems, the van der Waals term (ΔEvdW) dominates the stabilizing contributions. Notably, 6C exhibits a significantly stronger ΔEvdW, consistent with tight aromatic stacking. The electrostatic interaction energy (ΔEele) is slightly more favorable in 6B; but insufficient to compensate for the weaker ΔEvdW contribution. As a result, the overall non-covalent interaction profile remains clearly more favorable for 6C. The internal energy term (ΔEint), which includes bond, angle, and dihedral contributions, is also slightly more stabilizing in 6C. This suggests that 6C maintains a more favorable internal geometry upon dimerization, with less conformational strain compared to 6B. The lower ΔEint contribution observed in 6B may ultimately reflect suboptimal alignment of the monomeric units and internal distortion required to maintain contact. As expected, the polar solvation free energy (ΔGPB) introduces a positive penalty in both dimers, as polar groups become partially buried. Nevertheless, this cost is better compensated in 6C due to stronger non-covalent stabilization. The nonpolar solvation energy (ΔGNP) is minor in magnitude but still more favorable in 6C, consistent with a greater solvent-excluded surface upon dimerization.
Fig. 5b compares the overall binding enthalpy (ΔH) and free energy (ΔG) for the 6C and 6B dimers. While both dimers experience an entropic penalty associated with reduced configurational freedom, 6C retains a substantially more favorable free energy of binding (ΔG = −16.3 ± 1.3 kcal mol−1), confirming its superior thermodynamic stability. For 6B, the weaker enthalpic stabilization is compounded by the entropic penalty, resulting in a significantly less favorable ΔG (−1.1 ± 1.6 kcal mol−1). Although MM/PBSA estimates should be interpreted in a comparative rather than absolute sense, the energetic trends are consistent with both the structural descriptors and experimental data, and support the conclusion that 6C forms a persistent, compact dimer in solution, whereas 6B lacks the capacity to sustain stable supramolecular association under comparable conditions.
Taken together, the MD simulations provide a coherent picture of the marked difference in supramolecular stability between the two systems. Receptor 6C forms a persistent π–π stacked dimer stabilized by intradimer hydrogen bonding and a compact, complementary interface. By contrast, 6B, although initially dimeric, undergoes progressive disassembly over time. These divergent behaviors stem from a combination of electronic and steric factors: the planar, extended aromatic core of 6C favors efficient stacking and tight molecular packing, whereas the bulkier substituents in 6B hinder optimal interfacial alignment, ultimately compromising dimer stability. These computational findings are consistent with experimental results from dilution NMR and binding assays, offering a molecular-level rationale for the differential behavior observed for these two macrocyclic receptors in DMSO solution.
Alongside the investigation of host–host interactions of 6C in solution, we aimed to examine its solid-state structure by X-ray diffraction analysis. Although intermolecular packing in the crystal does not necessarily mirror behavior in solution, owing to the fundamentally different physical environments of the two phases, the solid-state analysis provides complementary structural insight and may help contextualize the observed intermolecular interactions. Initial crystallization attempts from DMSO and various other solvents and their mixtures, including acetone, acetonitrile, and ethyl acetate, did not yield crystals of sufficient quality. Slow evaporation from a DMF/hexane mixture ultimately proved successful, affording single crystals suitable for diffraction studies.
The macrocycle 6C crystallized in a monoclinic crystal system, space group P21/n, forming a 1
:
5 solvate with DMF molecules. As shown in Fig. 6a and b, the azacalix[4]arene skeleton adopts the expected 1,3-alternate conformation in the solid state. Two nitro-substituted aromatic moieties are extremely flattened with the corresponding interplanar angles (Φ) of 155.30° and 145.95° (towards the main plane of the molecule defined by the four nitrogen bridging atoms). The remaining urea-bearing subunits are nearly perpendicular to the main plane (Φ = 80.82° and 81.88°), resulting in their slight tilt towards the cavity. The structure is fixed by a quadruple intramolecular hydrogen bond between the oxygen of the nitro group and the proximal N–H bond of the bridging nitrogen with corresponding N–H⋯O distances ranging from 1.910 to 2.062 Å (Fig. 6b).
The crystal packing of 6C is characterized by a large number of non-covalent interactions, which cannot be listed in a simple way. However, some general conclusions can be drawn. First of all, urea groups are practically excluded from intermolecular HB interactions, since each of these groups is involved in complexation of solvent molecules through the interaction of both NH bonds with the DMF carbonyl oxygen (Fig. 6c). Depending on the specific bonded partners, the NH⋯O
C distances range from 1.935 to 2.454 Å. The molecules of 6C are linked to each other by several different types of aromatic interactions.33,34 Fig. 6d shows the dimeric motif based on π–π interactions between the naphthyl and tetraamine fragments. Both aromatic systems adopt a practically coplanar arrangement with at least six C⋯C close contacts (from 3.360 to 3.527 Å), corresponding to the typical interplanar distances in aromatic interactions (3.5 Å). The importance of naphthyl groups in the packing of 6C can be demonstrated on the π–π interactions between these aromatic units. Fig. 6e shows a dimeric motif based on at least four close contacts (3.340 to 3.540 Å) between carbon atoms of the naphthalene moieties. In addition, another type of π–π interactions can be observed between the coplanar naphthyl and dinitro fragments of the macrocycle (Fig. 6f).
Following the analysis of host-host interaction, the anion-binding properties of receptors 6 were investigated. UV–Vis spectroscopy was used to distinguish between hydrogen-bond-assisted complexation and receptor deprotonation. Only moderate spectral changes were observed upon addition of basic anions (Fig. S31a–S37a), whereas DBU (1,8-diazabicycloundec-7-ene) induced pronounced absorbance changes (Fig. S31b–S33b and S36b–S37b). This contrast indicates that anion recognition proceeds via complexation rather than receptor deprotonation.
UV–Vis spectroscopy was suitable to distinguish receptor deprotonation from anion binding, but showed only a weak response to anions, limiting further insight into binding interactions. Therefore, 1H NMR spectroscopy was employed to probe anion binding preferences (Fig. 7a). As expected, large and diffuse anions such as I−, ClO4− and PF6− exhibited negligible interaction with ureido binding sites, as evidenced by the absence of chemical-shift changes in the ureido NH signals. This lack of interaction can be attributed to their low charge density and poor hydrogen-bond-accepting ability.
Slightly stronger, yet still moderate, interactions were observed for stabilised non-basic anions (Cl−, HSO4− and NO3−). Saturation in titration experiments required either a high anion excess or elevated concentrations. Regarding the complex stoichiometry, continuous variation analysis35,36 was used. For chloride, Job plot (Fig. S48–S52) showed maxima near 0.2 for all receptors, consistent with multiple independent binding events and an apparent 1
:
4 receptor–anion ratio. This is supported by the unchanged diagnostic signals of the macrocyclic platform (C–H between nitro groups) throughout the titrations (Fig. 7c and Fig. S38–S42), indicating that chloride binding does not induce significant changes in scaffold geometry. Overall, non-basic anions exhibiting weak interactions without significant advantages coming from the macrocyclic skeleton.
In contrast, basic anions induced pronounced spectral changes (Fig. 7a, c and Fig. S43–S47), indicating complexation-driven response of the receptor. Significant shifts were observed in both the ureido NH and macrocyclic C–H signals, consistent with conformational adaptation of the azacalixarene scaffold. Signal broadening in some cases prevented precise assignment, but the overall spectral characteristics indicate a cooperative and geometrically demanding binding process compared to non-basic anions. Job plot analysis revealed maxima between 0.33 and 0.5 depending on the receptor substituent and the anion (Fig. S48–S52), suggesting deviations from simple independent-site binding. For 6A and 6B, which exhibit minimal aggregation and reduced hydrogen-bond donating ability, consistent maxima at ∼0.33 were observed for all basic anions, corresponding to a 1
:
2 (receptor-to-anion) stoichiometry. In contrast, 6C–6E displayed shifted or broadened maxima, likely reflecting multiple coexisting equilibria and higher-order binding modes.
Given this complexity, the raw NMR data were primarily presented graphically (Fig. 7b and Fig. S53), analysing the percentage of CIS values and the shapes of the binding isotherms for qualitative comparison. To compare selectivity, receptors 6B and 6C were examined under identical conditions (1.2 mM receptor concentration, comparable anion equivalents). Fig. 7b (Fig. S53) reveals the selectivity sequence H2PO4− > BzO− > AcO− ≫ Cl−, indicating that factors beyond simple basicity contribute to anion coordination. A possible rationale for the observed affinity increase lies in the propensity of H2PO4− to dimerize within a well-preorganized supramolecular complex/assembly.37 Notably, the differences among individual anions were more pronounced for 6C.
To examine substituent effects, benzoate was chosen as a representative guest. Although it is strongly bound, benzoate is not the most tightly coordinated anion, thereby allowing the influence of individual substituents to be clearly distinguished (Fig. 8). Receptor 6E, (–CF3 substituent) exhibited the highest binding efficiency, consistent with the positive influence of electron-withdrawing groups on hydrogen-bond donation and, hence, binding strength. Receptors 6C and 6D reached approximately 85% of the CIS value upon addition of four equivalents of benzoate. However, it should be noted that their titration profiles differ, as receptor 6C forms significantly stronger and more stable self-aggregates. The weakest binding was observed for receptors bearing electron-donating groups (tert-butyl or –OMe), in agreement with expectations based on their reduced hydrogen-bond donating ability.
Finally, despite the varying Job plot outcomes, quantitative analysis of titration data was attempted using classical 1
:
2 host–guest binding models38 (Table 1). While this approach adequately described the data for receptors 6A and 6B, lower quality fits were obtained for the remaining receptors. For the receptors 6B–6E, self-aggregation is present, and the observed behavior reflects a competition/interplay between host–host and host–guest interactions. The results indicate that the binding constants derived for 6B–6E should be regarded as effective parameters rather than precise thermodynamic descriptors. Nevertheless, the trends correlate with ureido hydrogen-bond donating ability and provide a meaningful comparison of relative binding efficiencies across the receptor series.
:
1) and (apparent) overall association constants β, which were determined by 1H NMR in DMSO-d6 with a series of receptors 6 and TBABzO
| Receptor | KAs (1 : 1)a |
βb |
|---|---|---|
a Error, when estimated, was <30%.b β values were calculated for 1 : 2 stoichiometry using a statistical model, where: β = KAs (1 : 1) × KAs (1 : 2), and KAs (1 : 2) = KAs (1 : 1)/4.c Represents the case in which no detectable self-aggregation occurs, and therefore its behavior can be described as a host–guest association process. |
||
6A c |
2530 | 1.60 × 106 |
| 6B | 2520 | 1.59 × 106 |
| 6C | 4000 | 4.00 × 106 |
| 6D | 6490 | 1.05 × 107 |
| 6E | 8400 | 1.76 × 107 |
:
2 DMF
:
MeOH (v
:
v) solvent ratio. The initial volume of 10–15 mL was reduced to approx. 1/10 and the retentate was diluted by fresh solvent mixture. This cycle was repeated until there was no detectable impurity in the filtrate (5–6 times).All prepared compounds were characterized by multinuclear NMR (1H NMR, 13C NMR, and 19F NMR), IR spectroscopy, and high-resolution mass spectrometry (HRMS). Detailed spectroscopic data and copies of the spectra are provided in the SI.
:
ACN (9
:
1 (v
:
v)). Compound 3 was obtained as a white solid (0.85 g, 82%) and was used immediately in the next step due to its instability.
Stepwise synthesis: The synthesis was initiated by dissolving the acyclic precursor 4 (0.125 g, 0.25 mmol) and compound 3 (0.066 g, 0.23 mmol) in dry acetonitrile (100 mL). Then, the oxygen was removed from the solution by a stream of argon, after which N,N-diisopropylethylamine (185 μL, 1.06 mmol) was added dropwise under stirring. The reaction mixture was stirred at ambient temperature for 3 h and subsequently heated to reflux overnight. After completion of the reaction, the solvent was removed under reduced pressure, and the resulting solid residue was repeatedly washed with cold EtOH (100 mL). Compound 5 was obtained as a brown powder (0.13 g, 87% yield). 1H NMR (400 MHz, DMSO-d6) δ: 8.99 (s, 2H, ArH); 8.88 (s, 4H, NH); 6.52 (s, 2H, ArH); 6.06 (s, 2H, ArH); 5.69 (s, 2H, ArH); 5.00 (brs, 8H, NH2) ppm.
:
EA (3
:
1 (v : v), total volume 2 mL) or in dry DMF (0.5 mL). To the stirred solution, the appropriate isocyanate (2 equiv. per free NH2 group) was added dropwise. The reaction mixture was stirred at ambient temperature for 3 days. To quench any remaining isocyanate, MeOH (5 mL) was added, and the mixture was stirred for an additional 20 min. After completion, the solvent was removed under reduced pressure, and the resulting solid residue was purified by preparative thin-layer chromatography on silica gel, with the eluent selected according to the properties of the by-products.
:
MeOH; 20
:
1 (v
:
v)). The product 6A was obtained as an ochreous powder (82 mg, 73%), m. p. >300 °C. 1H NMR (400 MHz, DMSO-d6) δ: 9.53 (s, 4H, NH); 9.10 (s, 2H, ArH); 8.75 (s, 4H, NH); 8.69 (s, 2H, ArH); 8.13 (s, 4H, NH); 7.27 (d, 8H, ArH, J = 8.7 Hz); 7.02 (s, 2H, ArH); 6.77 (d, 8H, ArH; J = 9.2 Hz); 5.41 (s, 2H, ArH); 3.67 (s, 12H, –OCH3) ppm. 13C{1H} NMR (100 MHz, DMSO-d6) δ: 154.6; 152.4; 148.5; 136.6; 132.2; 128.6; 128.1; 124.9; 122.1; 120.3; 113.9; 95.3; 55.1 ppm. IR (ATR) 3323; 3205; 3090; 3044; 3004; 2952; 2935; 2908; 2835; 1693; 1623; 1567; 1506 cm−1. HRMS ESI+: (C56H48N16O16 + H)+ m/z calcd [M + H]+ 1201.3507; found 1201.3511; (C56H48N16O16 + NH4)+ m/z calcd [M + NH4]+ 1218.3773; found 1218.3771.
:
EA). The residue was purified by prep-TLC (eluent DCM
:
MeOH; 10
:
1 (v
:
v)). The product 6B was obtained as an orange-brown powder (72.6 mg, 70%). 1H NMR (400 MHz, DMSO-d6) δ: 9.53 (s, 4H, NH); 9.09 (s, 2H, ArH); 8.87 (s, 4H, NH); 8.67 (s, 2H, ArH); 8.18 (s, 4H, NH); 7.30 (d, 8H, ArH, J = 8.7 Hz); 7.20 (d, 8H, ArH, J = 8.8 Hz); 7.02 (s, 2H, ArH); 5.42 (s, 2H, ArH); 1.21 (s, 36H, CH3) ppm. Spectrum is in accordance with the literature.27
:
MeOH 40
:
1 (v
:
v)) or OSN (as described above). The product 6C was obtained as a brown powder in a yield depending on the purification procedure used: 38% (prep-TLC; silica) vs. 82% (OSN), m. p. 282–285 °C. 1H NMR (400 MHz, DMSO-d6) δ: 9.66 (s, 4H, NH); 9.13 (s, 2H, ArH); 9.06 (s, 4H, NH); 8.79 (s, 2H, ArH); 8.63 (s, 4H, NH), 8.02–7.80 (m, 16H, ArH); 7.62–7.30 (m, 12H, ArH); 7.13 (s, 2H, ArH), 5.56 (s, 2H, ArH) ppm. 13C{1H} NMR (100 MHz, DMSO-d6) δ: 153.2; 148.5; 139.1; 136.3; 128.3; 126.4; 125.9; 125.8; 125.7; 125.5; 125.2; 124.1; 123.3; 122.1; 120.0; 118.6; 118.5; 113.7; 95.3 ppm. IR (ATR) 3316; 3093; 3054; 3016; 2955; 2925; 2853; 1681; 1627; 1567; 1527; 1504 cm−1. HRMS ESI+: (C68H48N16O12 + H)+ m/z calcd [M + H]+ 1281.3710; found 1281.3690; (C68H48N16O12 + Na)+ m/z calcd [M + Na]+ 1303.3530; found 1303.3504.
:
EA). The residue was purified by prep-TLC (eluent EA
:
PE; 1
:
1 (v
:
v)). The product 6D was obtained as a brownish powder (71 mg, 74%), m. p. ∼300 °C. 1H NMR (400 MHz, DMSO-d6) δ: 9.54 (s, 4H, NH); 9.10 (s, 2H, ArH); 9.04 (s, 4H, NH); 8.71 (s, 2H, ArH) 8.29 (s, 4H, NH); 7.38 (d, 8H, ArH, J = 7.7 Hz); 7.21 (m, 8H, ArH); 7.07 (s, 2H, ArH); 6.92 (t, 4H, ArH, J = 7.3 Hz); 5.46 (s, 2H, ArH) ppm. 13C{1H} NMR (100 MHz, DMSO-d6) δ: 152.3; 148.5; 139.3; 136.4; 128.7; 128.1; 125.0; 122.5; 122.0; 118.4; 118.2; 113.7; 95.3 ppm. IR (ATR) 3315; 3200; 3134; 3089; 3038; 2985; 2930; 1698; 1625; 1598; 1567; 1531 cm−1. HRMS ESI+: (C52H40N16O12 + Na)+ m/z calcd [M + Na]+ 1103.2903; found 1103.2896.
:
EA). The residue was purified by prep-TLC (eluent DCM
:
MeOH; 40
:
1 (v
:
v)). The product 6E was obtained as a dark reddish-brown powder (20 mg, 18%), m. p. >300 °C. NMR – due to strong self-aggregation ability and splitting caused by –CF3, the 1H, 13C and 19F spectra were not clearly resolved Fig. S18–S20. 1H (400 MHz, DMSO-d6) δ: 9.49 (s, 4H, NH); 9.42 (s, 4H, NH); 9.09 (s, 2H, ArH); 8.97 (s, 2H, ArH); 8.20 (s, 4H, NH); 7.62–7.16 (m, ArH, 16H); 6.93 (s, 2H, ArH); 5.20 (s, 2H, ArH) ppm. 19F NMR (376 MHz, DMSO-d6) δ: −60.33 ppm. IR (ATR) 3294; 3206; 3117; 3059; 3012; 2928; 2854; 1707; 1605; 1567; 1512 cm−1. HRMS ESI+: (C56H36F12N16O12Na)+ m/z calcd [M + Na]+ 1375.2399; found 1375.2402.
:
1) and overall association constants β with their errors were evaluated using the freeware program Bindfit30 for 1
:
2 stoichiometry (receptor 6: anion) using a statistical model. All raw data and calculation details for the individual binding events are provided in the SI.
Bonded and nonbonded parameters for the receptors were assigned using the general AMBER force field for organic molecules (GAFF),44 following the standard AmberTools 202543 parametrization workflow. Partial atomic charges were assigned using the AM1-BCC scheme as implemented in the antechamber module of AmberTools 2025, and any missing parameters were generated within the GAFF framework. All simulations were conducted under periodic boundary conditions.
After energy minimization, the systems were equilibrated in two stages: (i) NVT equilibration at 298 K using a Langevin thermostat45 (collision frequency 2.5 ps−1), followed by (ii) NPT equilibration at 1 atm using a Berendsen barostat46 to adjust the box volume. Production MD simulations were carried out for 500 ns for each system. No predefined production window was excluded from analysis, as the objective was to monitor the full-time evolution of dimer stability. All structural descriptors and energetic analyses were therefore performed over the entire 500 ns trajectories. A time step of 2 fs was used, and all covalent bonds involving hydrogens were constrained via the SHAKE algorithm.47 Long-range electrostatics were treated with the particle mesh Ewald method,48 with a real-space cutoff of 10 Å.
Appropriate counterions were added when required to maintain electroneutrality.
Analysis of the trajectories focused on structural descriptors relevant to supramolecular association. The total number of intradimer hydrogen-bond (HB) contacts was computed using standard geometric criteria (donor–acceptor distance ≤3.5 Å and H–D–A angle ≥135°), without predefining specific donor–acceptor pairs. The native-contact fraction (Q) was calculated by monitoring intermonomer heavy-atom contacts within a cutoff distance of 4.5 Å, relative to the initial dimer structure. The center-of-mass distance (dCOM–COM) between the macrocycles was evaluated along the trajectories to quantify association stability. π–π stacking parameters (interplanar distance and angle between the aromatic platforms) were obtained by least-squares plane fitting.
To estimate the thermodynamic stability of the dimers, an MM/PBSA approach32 was applied using a single-trajectory protocol. Snapshots were extracted every 10 ps from the full 500 ns trajectories, resulting in 50
000 frames for each system. The binding enthalpy (ΔH) was computed as the sum of van der Waals (ΔEvdW), electrostatic (ΔEele), internal (ΔEint), polar solvation (ΔGPB), and nonpolar solvation (ΔGNP) contributions. Entropic contributions (TΔS) were evaluated by quasi-harmonic analysis49 of the covariance matrix of atomic fluctuations. The free energy of binding was then computed as ΔG = ΔH − TΔS. Reported uncertainties correspond to standard deviations over the sampled frames.
All trajectory and structural analyses were performed with AmberTools 2025 and in-house Python scripts on the Leonardo supercomputer (CINECA, Bologna, Italy) and on in-house CPU/GPU hybrid cluster. Graphs were produced using GraphPad Prism (version 10 for macOS, GraphPad Software, Boston, Massachusetts USA, https://www.graphpad.com). Visual inspection and rendering of representative structures were carried out with UCSF Chimera.50
517 independent reflections (θmax = 73.5°), 1310 parameters and 528 restrains. The hydrogen atoms were placed in calculated positions refined with riding constraints. One naphthyl group and one ureido group were found to be disordered over two positions. In both cases the atomic positions of second positions were found in difference electron density maps and refined with restrained geometry and ADPs. In both cases the occupancies were refined with sum constrained to 1, resulting in occupancy ratios of 537(4)
:
463(4) for naphthyl and 918(3)
:
82(3) for ureido group. The residual electron density maps were visualized in MCE.54 The molecular graphics were created using Diamond 3.0.55 The structure was deposited into Cambridge Structural Database under number CCDC 2538630. For numbering schemes and disorder descriptions see SI.
CCDC 2538630 contains the supplementary crystallographic data for this paper.56
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