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. 2026 Aug 17;18(10):1819–1827. doi: 10.1038/s41557-026-02222-6

A protein–foldamer supramolecular synthon for self-assembled hybrid architectures

Johannes Sigl 1, Vasily Morozov 1, Lingfei Wang 1, Janine Sachs 2, Eric Merlet 2, Eric Largy 3, Niklas Geue 4,5, Nicklas Österlund 4,5, Sunbum Kwon 1,2,7, Florian Sanchez 1, Léo Candela 6, Simon Huet 6, Kevin Pagel 4,5, Yann Ferrand 2, Céline Douat 1, Cameron D Mackereth 3, Ivan Huc 1,✉
PMCID: PMC13623658  PMID: 42608459

Abstract

Constructing artificial assemblies that combine proteins and synthetic ligands has been hampered by the lack of protein–ligand interfaces that are sufficiently large and organized to enable precise structural control. Here ribosome display selection is used to identify a protein that binds a helical aromatic foldamer both tightly and selectively through a sizeable surface area. We used this complex as a supramolecular synthon to create well-defined hybrid foldamer–protein architectures. Examples include foldamers that bind two proteins and hold them at a precise distance, proteins that bind two foldamers and crystals in which proteins and foldamers are connected in cyclic or infinite arrays. The modularity of aromatic foldamers brings a further dimension to protein-based assemblies.

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Subject terms: Proteins, Self-assembly


A stable and modular artificial protein–foldamer helical supramolecular synthon enables the assembly of ordered architectures, in which the foldamer dictates protein orientation and spacing on the nanoscale.

Main

Artificial protein assemblies may be constructed by programming protein–protein interaction interfaces using either natural or de novo-designed proteins1–6. Rationally organizing the spatial assembly of proteins using synthetic molecules6, instead of other proteins, is also desirable as illustrated by current efforts in the development of so-called molecular glues7,8, proteolysis targeting chimeras (PROTACs)9,10 and hybrid protein frameworks11–13. However, the co-assembly of proteins and synthetic molecules remains challenging to achieve with high structural precision. It has been limited by the lack of supramolecular synthons with a sufficiently large and organized protein–ligand interface for architectural control. Thus, synthetic macrocycles and molecular tweezers that bind to protein surfaces have been used to organize the packing of proteins in the solid state but their binding modes are variable11,13. Conversely, small molecule ligands that selectively bind protein pockets may not prevent hinge motions, hampering the precise positioning of a large appendage such as another protein. Instead, flexible linkers are generally used, which reduces structural control8. In this Article, we introduce a complex between a synthetic helical aromatic foldamer and a 7-kDa artificial protein identified by ribosome display selection. The complex can serve as a supramolecular synthon for discrete aggregate and lattice construction. As solid-state and solution structures reveal, the binding interface is sizeable (>700 Å2), stable yet dynamic, and well-defined, allowing for the further elaboration of both the foldamer and protein components and for the construction of hybrid assemblies in which proteins are held at precise positions in space by synthetic foldamers.

Developing a supramolecular synthon that combines a protein and a synthetic molecule entailed a judicious choice of both components. Synthetic oligomers that fold—foldamers—provide a variety of medium-sized scaffolds many of which have shown potential to interact with proteins14,15. In particular, aromatic oligoamide foldamers (AOFs) such as the oligoamides of 8-amino-2-quinoline carboxylic acid QXxx (Fig. 1a) adopt particularly stable and predictable conformations and can be tailored to reach sizes that match those of small proteins16. For example, a simple octamer of QLeu remains helically folded at 120 °C in dimethyl sulfoxide17. The surface of AOFs can be decorated with biogenic-like side chains,18 and their main chain can be programmed to form helices of variable diameter as well as sheets19,20. Automated solid-phase synthesis (SPS) enables direct access to sequences in the 5–10-kDa range21. In principle, these combined features make AOFs suitable candidates for recognizing large surface areas of proteins. Efforts have until now focused on AOF design and screening, that is, on the identification of foldamers that bind to a biological protein target by varying helical22 or rod-like23,24 foldamer main chain and side chain components. However, structurally characterized complexes between proteins and helical AOFs are poorly stable (dissociation constant KD in the micromolar range)25 or involve flexible linkers proscribed for the current purpose26. They thus do not constitute reliable supramolecular synthons. By contrast, the approach followed here consisted in identifying a protein that binds a given foldamer from a large library of protein sequence variants, leading to a protein–foldamer complex in which both components are artificial.

Fig. 1. Foldamer building blocks, sequences and display selection results.

Fig. 1

a, Monomer building blocks for AOFs with their respective letter code used in this study. Asp, aspartate-like side chain; Sul, sulfonate side chain; Pho, phosphonate-containing side chain; Orn, ornithine-like side chain; Dap, diaminopropionic acid-like side chain; Leu, leucine-like side chain; Phe, phenylalanine-like side chain; Hyd, hydroxy side chain; Dol, diol-containing side chain; Deg, diethylene glycol-containing side chain; Bio, biotin-containing terminal unit; PEG, diethylene glycol-containing terminal unit. Colours indicate the chemical nature of the side chains: orange, acidic; blue, basic; black, hydrophobic; green, polar neutral. Bold bonds define the inner rim of helical oligomers. b, AOF sequences synthesized, written left to right in the N- to C-terminal direction. In 4, the unit D is a diacid, resulting in a symmetrical sequence with two C termini. c, Crystal structure of the dodecaamide 1b, shown from side and top view. The right-handed conformation is shown. The crystal also contains the left-handed helix. The bond order and hydrogen atoms are omitted for clarity. d, Crystal structure of the selected Nanofitin C10 at 1.4 Å (Supplementary Fig. 2) shown at the same scale as the structure of 1b in c. Residues highlighted in pink, including five aromatic residues, are at positions randomized in the selection process. The coiled-coil extension was omitted for clarity. e, BLI sensorgrams of P-1a (blue curves) and M-1a (red curves) used as ligands on SA biosensors, against Nanofitin C10 (analyte) in a serial dilution from 250 nM to 62.5 nM in phosphate-buffered saline with 0.05% Tween 20 (PBST) revealing a dissociation constant (KD) of 92 nM for P-1a•C10. f, Circular dichroism (CD) spectra of C10 recorded in ten steps heating the sample from 5 °C to 95 °C (top). Molar ellipticity (θ) recorded at 222 nm heating from 5 °C to 95 °C, then cooling back to 5 °C, showing complete CD signal recovery (bottom).

Source data

To identify a protein that would tightly bind a foldamer, we turned to display selection methods, which brought their own challenges. Antibodies and nanobodies are typical proteins amenable to display selection. They have flexible loops that can create cavities, and successful examples of display selection of nanobodies against small molecules have been reported7,27. However, their complex structure, relatively large size and moderate stability are not ideal to serve as supramolecular synthons. Smaller proteins based on non-immunoglobulin scaffolds would fare better in this respect. Many such proteins have been used in display selection to bind to other protein targets28,29. Yet examples of display selection against small synthetic molecules are rare; they typically involve loop binding regions rather than flat interfaces, and the structures of the complexes remain unknown30,31. We opted for the selection of Nanofitins32,33, which are based on the scaffold of Sac7d, a 66-residue cysteine-free protein stable over a broad range of temperature and pH34. Sac7d naturally binds to dsDNA, whose size is similar to that of (QXxx)n helices. Binding is mediated by the slightly concave surface of an incomplete five-stranded β-barrel within which up to 14 residues have been randomly mutated for display selection. At their C-terminus, an α-helix caps the β-barrel and points away from the binding interface, thus providing a handle for fusion with other proteins. Furthermore, Nanofitin–protein complexes are amenable to X-ray crystallographic analysis35–37.

Selection of a foldamer-binding protein

Biotinylated AOF 1a (Fig. 1b), a QXxx dodecaamide five-turn helix, was chosen as the selection target because its chemically diverse side chain decoration potentially offers a variety of protein-binding epitopes, as highlighted by the X-ray crystallographic structure of its analogue 1b (Fig. 1c)38. Furthermore, the protein-binding capabilities of 1a have been demonstrated in yeast lysate pull-down assays38. Nanofitin selection was performed in four rounds of ribosome display, as previously described32, using biotinylated 1a as a bait. The enrichment of naive libraries towards binders was monitored by enzyme-linked immunosorbent assay (ELISA) using the DNA pools collected after each round (Supplementary Fig. 1). Subsequent cloning and sequencing led to the identification of clone C10. Foldamer 1a exists as a mixture of right-handed (P) and left-handed (M) diastereomeric helical conformers that do not interconvert and in which the chiral biotin has no effect on the proportion of P and M helices, which are thus present in identical amounts. The diastereoisomers can be separated by reversed-phase high-performance liquid chromatography (RP-HPLC) on a chiral stationary phase38. C10 was recombinantly expressed and its affinity for P-1a and M-1a was assessed in parallel biolayer interferometry (BLI) assays. C10 was found to bind to P-1a with a KD of 91.7 nM while no binding to M-1a was detected, hinting at a structurally well-defined interaction (Fig. 1e). We thus synthesized analogue 1c whose N-terminal chiral C* camphanyl group quantitatively biases helix handedness to the P conformation39. Initial attempts to crystallize C10 alone or in complex with 1b or 1c were unsuccessful. Yet by C-terminal fusion of the coiled-coil talin dimerization domain40 (PDB 2QDQ) to C10, a high-resolution 1.4-Å X-ray crystallographic structure was obtained showing that the C10 apo-protein adopts the same tertiary fold as wild-type parent Sac7d (Fig. 1d, Supplementary Fig. 2 and Supplementary Table 1). The structure also showed that aromatic residues selected at randomly mutated positions (H22, F24, H26, Y33, H42) promote C10 dimerization in the solid state. Weak dimerization was also suspected in solution at concentrations required for NMR characterization (see below) and observed during size exclusion chromatography (SEC). Variable-temperature circular dichroism (CD) measurements highlighted the high thermostability of C10, showing a decrease of CD band intensity but no melting transition between 5 °C and 95 °C as well as complete CD signal recovery upon cooling (Fig. 1f), which boded well for its use in a supramolecular synthon.

NMR complex structure elucidation

A partial assignment of the NMR spectra of [13C,15N]-labelled C10 was performed (Supplementary Fig. 3). The backbone amide signals of some residues were broadened and a few were missing. These were primarily residues from the region randomized during display selection. The broadening of these signals suggests that some aggregation involving this region of the protein surface takes place at micromolar concentrations (Supplementary Fig. 3). By contrast, the spectra of solutions of the 1c•C10 complex were sharp and its structure could be determined, allowing for an assessment of the nature of the binding mode in solution. Compared with usual ligands in protein–ligand complexes, the large size of the foldamer ligand necessitated the use of a modified structure determination process (see Methods for details). To assist further in identifying protein, foldamer and intermolecular cross-peaks, we used [13C,15N]-labelled C10 combined with unlabelled foldamer 1c at natural isotope abundance. This isotope labelling scheme allowed for the collection of edited or filtered NMR spectra so that signals of the protein only, of the foldamer only or of both the foldamer and protein are observed (Supplementary Figs. 4–6 and Supplementary Table 2). The resulting ensemble of 20 structures was calculated using restrained molecular dynamics in AMBER with 114 dihedral angle restraints and 737 distance restraints distributed throughout the complex (Supplementary Fig. 7 and Supplementary Tables 3 and 4).

The NMR structure of the 1c•C10 complex revealed the architecture of the 1:1 assembly (Fig. 2a). The C-terminal aromatic cross-section of 1c covers a large area of the protein β-sheet region (~830 Å2, Fig. 2a), where most of the residues that were randomized during the selection process are located, while the N-terminus of the helix protrudes away from the protein. The interaction between the extended aromatic C-terminal region of 1c with the flat C10 surface is somewhat reminiscent of G-quadruplex DNA–protein structures41. The upright binding mode of the foldamer helix on C10 differs from side-on helix orientations previously observed in more labile aromatic helical foldamer–protein complexes25. In atomic detail, the 1c•C10 binding interface primarily consists of (1) face-to-face π-stacking between the QDol11 quinoline ring and H42 and T-shaped π–π interaction between QAsp12 and H26; (2) hydrophobic contacts between the two solvent-exposed terminal quinoline rings and residues V31 and L44, between the side chain of QDol11 and Y33 and between QOrn9 and F24; (3) hydrogen bonding of Y33 to the main chain QDol11–QAsp12 amide carbonyl and between T40 and the side chain of QDol11; and (4) charge-reinforced hydrogen bonding of both Y8 and H42 to the C-terminal carboxylate of the foldamer and of H26 to the side chain carboxylate of QAsp12 (Fig. 2b–d). Interactions thus mainly involve residues located at the positions randomized during selection with the notable exception of Y8 and K9. The ensemble of 20 NMR structures determined for the 1c•C10 complex shows limited variation in the relative position of the foldamer and protein, with an overall all-heavy atom RMSD of 1.7 ± 0.2 Å (Fig. 2a and Supplementary Table 3). Furthermore, molecular dynamics simulations of the complex confirm that the foldamer position and orientation on the C10 surface are essentially stable (Supplementary Video 1). The simulations also highlight the structural integrity of the complex in terms of residue fluctuations and hydrogen bond frequencies (Supplementary Figs. 8 and 9). Taken together, the solution structure data of 1c•C10 validate the potential of this complex as a supramolecular synthon. Furthermore, the structure confirmed the location of the α-helix of C10 away from the foldamer-binding region and thus its potential use as a handle to fuse C10 with other proteins without altering foldamer binding.

Fig. 2. Nuclear magnetic resonance (NMR) structure elucidation reveals the protein–foldamer complex binding epitope.

Fig. 2

a, NMR structure of the 1c•C10 complex showing the aligned ensemble of 20 models. Structure statistics can be found in Supplementary Table 3. b, Schematic diagram of intermolecular contacts between C10 and the last four quinoline monomers of 1c in the binding epitope identified with protein–ligand interaction profiler50. Hydrogen bonds are shown as pink dashed lines and hydrophobic contacts as black solid lines. c–e, Three close-up structure views from different directions of important foldamer–protein contacts with annotated foldamer units and protein side chains. Hydrogen bonds are shown as pink dashed lines, and hydrophobic contacts as black dashed lines. f, Time course of CD spectrum of pentameric sequence 2a after addition of C10 at 30 µM, tris-buffered saline (TBS) pH 7.4, 25 °C. Note that the biotin moiety of 2a does not bias foldamer helix handedness as seen in the flat curve for 2a alone. g, BLI sensorgrams (blue solid lines) of C10 in solution and 2a loaded on SA-biosensors and global fitting using a 1:1 binding model (black dashed lines). Kinetic experiments were performed in PBST at pH 7.4 with a serial dilution of C10 from 500 nM to 15.6 nM.

Source data

Foldamer helix truncation

Large parts of the foldamer are not in contact with C10 in the complex, suggesting that a truncated version of 1 might bind equally well. We thus prepared pentaamide 2a which comprises the five C-terminal units of 1. For such short sequences, the equilibrium between P and M helices is expected to take place over the course of hours42. Indeed, upon mixing 2a and C10, CD bands above 300 nm where only the foldamer absorbs were found to slowly emerge (Fig. 2f), indicating foldamer helix handedness bias upon binding to the protein. The emergence of the CD band occurred faster at 60 °C owing to enhanced helix dynamics, confirming that binding still takes place at such high temperatures. The positive band at 380 nm confirmed that the P helix is the favoured binding conformation39. BLI measurements with biotinylated 2a confirmed that it binds as well as P-1a. Note that helix handedness bias of 2a is expected to remain marginal during the few minutes required for BLI measurements. We also prepared shorter foldamers having the last four, three or only two C-terminal units of 1a. BLI and CD assays showed that strong binding was retained with four residues but worsened below that number (Supplementary Fig. 10). Altogether, these results support that foldamer–C10 interactions are limited to those revealed by the NMR structure and that C10 and a pentaamide foldamer helix provide a robust supramolecular synthon for the elaboration of more complex architectures with controlled spatial organization.

Binding multiple proteins on the same foldamer

To test the generality and robustness of the supramolecular synthon upon modifications of the foldamer remote from the binding site, variants 3 and 4 were designed and synthesized (Fig. 1b), each presenting two binding epitopes through different modes of symmetric multimerization. Variant 4 consists of a long C2-symmetrical 31-mer single helix with two identical halves linked at their N termini by a central diacid unit D. Each half of 4 thus possesses a C-terminal C10-binding pentaamide elongated at its N terminus by a B* chiral unit, a number of hydrophilic QOrn and QDeg residues and a P residue, all assembled during SPS (Supplementary Fig. 11). The B* chiral control unit quantitatively biases helix handedness to the P conformation43, and the benzylic amine of the P unit facilitates the post-SPS assembly of 4 by fragment condensation on the diacid of unit D activated as a bis-N-hydroxysuccinimide ester25. The complexation of 4 with C10 was analysed by SEC. It resulted in a decrease of the retention time, indicating the formation of a presumably dumbbell-shaped ternary complex (Fig. 3a,b). The complex was also analysed in the gas phase using native nano-electrospray ionization mass spectrometry (nESI-MS). The 4•(C10)2 complex was found to be the dominant species, and its fragmentation into C10+4•C10 could be monitored by tandem mass spectrometry (MSMS, Fig. 3c). Analogues of 4 having longer or shorter helices are thus expected to rigidly hold in space two C10 molecules (and any protein fused to C10) at a distance and twist angle precisely defined by the number of AOF residues.

Fig. 3. Binding multiple proteins on the same foldamer.

Fig. 3

a, Energy-minimized model of the C2-symmetrical 4•(C10)2 complex. b, Size-exclusion chromatograms showing the formation of foldamer protein complexes as indicated by the lower elution volume for 4•(C10)2 and (P-3•C10)2 compared with the protein alone. The split peak for (P-3•C10)2 was assigned to the presence of some (P-3)2•C10. c,d, Native mass spectrometry (MS) spectra of 1:2 and 1:1 mixtures of 4/C10 and P-3/C10, respectively, at 100 µM in 200 mM ammonium acetate pH 6.8 (top), detecting the formation of 4•(C10)2 and (P-3•C10)2. The complexes were subjected to MSMS and collisional activation (bottom). Dashed arrows in the MSMS spectra indicate the dissociation produced from the m/z-selected precursor ions. e, Collision cross-section in the gas phase (TWCCSN2→He) of the C10+5, 4•(C10)2+9 and (P-3•C10)2+9 ions measured by ion mobility mass spectrometry. f, Asymmetric unit of the crystal structure of (P-3•C10)2 at 1.84 Å resolution containing two protein chains bridged by the foldamer duplex (P-3)2. A pseudo (non-crystallographic) C2 axis is indicated. g, Two different views of the C4-symmetrical higher order assembly observed in the (P-3•C10)2 X-ray crystallographic structure. The cyclic 8+8 aggregate comprised of four (P-3•C10)2 complexes is stabilized by inter-duplex π-π contacts between QOMe units and side chain-mediated charge-reinforced hydrogen bonds.

Source data

Variant 3 uses an N-terminal extension of the pentaamide binding epitope with four 7-amino-8-methoxy quinoline carboxylic acid QOMe residues that code for a wider aromatic helix diameter, which in turn promotes dimerization into stable antiparallel double helices in water44. The resulting duplex of sequence 3 binds two copies of C10, and the 2+2 quaternary complex can also be traced by SEC, showing an elution volume smaller than that of the protein or foldamer alone, yet larger than that of 4•(C10)2, reflecting the effect of foldamer length on elution time (Fig. 3b). In the gas phase, the (P-3•C10)2 complex was also observed by native nESI-MS (Fig. 3d) to be the dominant species. Its main fragmentation in MSMS was through a loss of a C10 unit and the formation of (P-3)2•C10, and not through the disruption of the (P-3)2 double helix highlighting its robustness. Furthermore, ion mobility measurements gave access to the collision cross-sections of C10, (P-3•C10)2 and 4•(C10)2 showing a trend consistent with the SEC data (Fig. 3e). Note that helix handedness control was not implemented in 3 and that, given its length, its helical conformation is kinetically locked (no CD band emerges upon adding C10 to 3). In solutions of racemic (3)2 duplexes, only the P helices thus bind to C10. We successfully crystallized and solved the structure of the (P-3•C10)2 complex, thus resolving the racemic (3)2 duplexes by crystallization. The structure at 1.84 Å resolution confirmed the expected dumbbell geometry, with two C10 molecules spatially separated upon binding to the opposite sides of double helical (3)2 (Fig. 3f, Supplementary Video 2 and Supplementary Table 1). The asymmetric unit (ASU) contains two independent foldamer–C10 interfaces which show highly conserved interactions essentially identical to those of the NMR structure (Supplementary Figs. 12 and 13, Supplementary Table 5), highlighting again the robustness of the supramolecular synthon.

The X-ray crystallographic structure of C10 bound to the foldamer was also compared with that of the apo-C10, showing that the main chains are essentially superimposable, an illustration of the robustness of the Nanofitin scaffold, while surface side chains, including those involved in foldamer recognition, may have different orientations (Supplementary Fig. 12). Future developments may exploit the use of longer helical segments to adjust protein–protein distance–foldamer length spontaneously doubles upon duplex formation, and the fact that heteromeric foldamer double helices form selectively when complementary strands are used44.

In the solid state, the (P-3•C10)2 complexes form a higher-order tetrameric [(P-3•C10)2]4 assembly organized in a fourfold cyclic arrangement (Fig. 3g and Supplementary Video 3). The assembly is held together by face-to-face contacts between QOMe residues belonging to different duplexes and an extensive array of inter-duplex charge-reinforced hydrogen bonds (Supplementary Fig. 14). In solution, the 8+8 aggregate was not detected by electron microscopy, and SEC retention volume shifts seem to be too small for an ~80-kDa object. It was also not visible in native nESI-MS spectra measured from micromolar solutions (Fig. 3d). We concluded that the assembly forms only at the mM concentration of the crystallization drops and possibly represents a minor component in solution, even at these higher concentrations, that would only be stabilized in the solid state. It nevertheless represents a starting point for designing stable foldamer assemblies able to bind multiple—here eight—proteins.

Binding multiple foldamers on a protein dimer

We next investigated modifications on C10 to explore how to spatially organize the supramolecular synthon via multimerization of the protein. Coil coiling of α-helices is arguably the best understood aggregation pattern and the easiest to design1,2,45. Implementation of a coiled coil on C10 is straightforward, thanks to its C-terminal α-helix that points away from the foldamer-binding region. We opted again for a simple fusion with the antiparallel coiled-coil domain of talin mentioned above, albeit with some design improvements. In the first design, two consecutive glycine residues (G66&67) present at the junction between C10 and the coiled coil were responsible for a local disruption of α-helix that kinked the structure (Supplementary Fig. 1). In this second design, these two glycine residues were replaced by alanine residues to better promote α-helicity. Crystallization efforts with this coil-extended C10 construct (C10CE) in complex with the initial target sequence, for example, 1b or 1c, repeatedly yielded crystals of the foldamer alone, presumably owing to its lower solubility. Therefore, pentamer 2b (Fig. 1b) was synthesized, carrying a solubilizing PEG termination as well as two phosphonate-containing QPho residues that were expected to improve solubility with respect to the original carboxylate QAsp units. Native nESI-MS showed the formation of the 2b•C10CE complex along with the (2b•C10CE)2 dimer. The proportions also seen in the spectrum of C10CE alone suggested some lability of the coiled-coil dimerization in the gas phase. The (2b•C10CE)2 dimer was found to fragment via coiled-coil dissociation (Supplementary Figs. 15, 16).

Diffraction quality crystals of the C10CE in complex with 2b were eventually obtained, and the X-ray crystallographic structure was elucidated (Fig. 4, Supplementary Fig. 17 and Supplementary Table 1). In the ASU, two coiled-coil protein dimers are in complex with two molecules of 2b through their C-terminal cross-section, providing further evidence that this robust, cognate interaction is highly conserved (Fig. 4b, Supplementary Fig. 13 and Supplementary Table 5). In addition, the two C10 domains establish contacts with the N-terminal cross-section of the 2b helices (Fig. 4b). This interaction only concerns the N-terminal quinoline ring and its short PEG chain, which involve hydrophobic contacts with Y33, H22 and T40 and a charge-reinforced hydrogen bond between H42 and a phosphonate side chain. We presume that they are weaker than the cognate foldamer–C10 recognition and only occur at the mM concentration of crystallization drops at substoichiometric amounts of foldamer. There is thus little risk that such non-cognate interactions would compete with the 91.7-nM cognate C10–foldamer recognition. The 4+2 cyclic assembly—four proteins and two foldamers—mediated by the non-cognate interactions was not detected by native nESI-MS from micromolar solutions (Supplementary Fig. 15). It is possibly a crystallization artefact—it crystallizes although it represents a minor component in solution. It may also be the result of a substoichiometric amount of foldamer. Nevertheless, the outcome is an X-shaped, figure-of-8, discrete macrocyclic assembly between two foldamers and two C10CE coiled-coil dimers (Fig. 4a, Supplementary Video 4). At the centre of the cyclic structure, favourable contacts between the two coiled coils are mediated by hydrogen bonds between multiple Glu, Lys and Arg residues that may be amenable to optimization (Fig. 4c). Altogether, the structure validates, and goes beyond, the initial design principles, and it suggests directions for further developments.

Fig. 4. Binding multiple foldamers by protein dimerization.

Fig. 4

a, Crystal structure of the coil-extended C10 (C10CE) in complex with pentaamide 2b. The ASU is shown from two perspectives, illustrating the cyclic arrangement of two foldamers and four C10CE proteins in the solid state. b, Detailed view of the foldamer packed between two C10 molecules, with the cognate-binding epitope highlighted in teal on one protein and non-cognate interactions in purple on the opposite chain. c, Highlights of Glu, Lys and Arg inter-coiled-coil interactions, connecting two protein dimers. Residues marked with a star were reconstituted from the crystal structure and energy minimized.

Binding multiple proteins with multiple foldamers in one system

Based on the established principles of enforced multimerization around the foldamer–C10 supramolecular synthon, we lastly combined the rigid homochiral divalent single helix of 4 with the head-to-tail coiled-coil-mediated dimer of C10CE. Crystallization trials quickly yielded diffraction quality crystals and revealed a structure of high symmetry, with the ASU containing one protein monomer and half of the C2-symmetrical 4 (Fig. 5, Supplementary Table 1). This structure provided yet one more illustration of the conservation of C10–foldamer interactions (Supplementary Fig. 1–3, Supplementary Table 5). Through application of the symmetry operations, a 1D polymeric zig-zag-like network that extends in a sort of flat ribbon is built (Fig. 5a). The ribbon consists mainly of cognate foldamer–C10-binding interfaces and the α-helical coiled coiling included in the design, along with C10–C10 contacts associated with crystal packing. The coincidence of the symmetry elements of the building blocks with the crystallographic rotational axes can be interpreted as an enforcement of global symmetry by predisposed local symmetries46. Here the C2 symmetry axis of the foldamer and the C2 symmetry axis of the C10 coiled-coil dimer are perpendicular, hence the formation of a flat assembly, but they do not intersect, giving rise to a polymeric structure rather than a macrocycle. This assembly is the direct outcome of the distance and angular twist between the protein-binding epitopes of 4 encoded in the number of QXxx residues and of the distance and angular twist between the foldamer-binding epitopes of the C10 coiled-coil dimer encoded by the length of the α-helices. In the gas phase, the 1D polymer was not observed by native nESI-MS (Supplementary Fig. 16).

Fig. 5. Crystal structure of the coiled-coil-mediated C10CE dimer in complex with the C2 symmetrical foldamer 4 (4•(C10CE)2) at 2.53 Å.

Fig. 5

a, Continuous ribbon built of protein dimers connected to the C2-symmetrical foldamer 4. The ASU (highlighted in gold) contains one protein monomer and one-half of 4. The imposed local C2 axes of the complex coincide with crystallographic symmetry axes, giving rise to a highly ordered assembly in the space group I4122. b–d, Orthoscopic views of the crystal lattice along different directions: along (010) (b), along (110) (c) and along (001) (d). In all cases, the unit cell is shown in black. Proteins are shown as blue ribbons and foldamers as red sticks.

While the crystal lattice appears to be tightly packed when viewed down its c-axis (Fig. 5d), it is in fact highly porous, with the foldamer spacing the proteins ~4.3 nm apart, while the coiled-coil domain keeps the foldamers ~8 nm apart (Fig. 5a–c). Computational analysis of the pores showed that the resulting channels in a and b directions reach a bottleneck radius of 15.5 Å and that the largest cavities can accommodate theoretical spheres with a diameter of ~5 nm (Supplementary Fig. 18)47, a value comparable to that of other highly porous frameworks11. A typical way to assess solvent content in protein crystal structures is through the Matthews coefficient, which describes the unit cell volume per protein mass (but does not tell anything about pore size). The mean Matthews coefficient of Protein Data Bank (PDB) protein structures is 2.67 Å3 Da−1 (ref. 48) to be compared with 3.51 Å3 Da−1 for the porous lattice mentioned above11 and 5.13 Å3 Da−1 for the structure of 4•(C10CE)2. This contrasts with the low porosity of the structure obtained with the pentaamide helix 2b•(C10CE)2 (Fig. 4), which has a calculated maximum bottleneck size of 8.6 Å, and reflects the benefit of the space between proteins imposed by 4. Considering that the length of the foldamer is freely adjustable (within synthetic limits), spacing within such lattices is, in principle, tunable, highlighting the relevance of protein–synthetic foldamer assemblies in the context of porous solid design.

In summary, in contrast to smaller molecules or peptides, aromatic foldamers constitute large and rigid-enough synthetic molecules to allow for successful display selection of protein binders and the generation of a well-defined and robust binding interface. It appears that the foldamer aromatic cross-section acted as a hot spot—one such protein–foldamer contact had been observed before with carbonic anhydrase II (ref. 49), and this feature may be exploited in future studies to target proteins with flat surfaces. The identification of C10 also suggests that targets other than aromatic foldamers may be amenable to the selection of protein binders, to bridge further the synthetic and protein chemical spaces. In turn, both the foldamer and protein can be further designed without altering their binding interactions so as to produce discrete or extended aggregates and lattices combining both biogenic and synthetic components. Extensions of this work will take advantage of the inherent modularity and synthetic accessibility of foldamers, of the diversity of protein scaffolds amenable to display selection such as the Nanofitin described in our study29 and of the advanced computational approaches to design protein structures and interaction1–3. These extensions include the design, either structure-guided or using ab initio protein design tools, of foldamer–protein nanocages and porous 3D lattices in which the foldamers may bring functional groups not available to proteins. They also included the use of foldamers to bring together or, on the contrary, to keep at a well-defined distance, naturally occurring proteins that have been tagged with foldamer-binding domains to alter their biological functions.

Methods

Detailed methods are provided in the Supplementary Information.

Foldamer synthesis

All foldamers were obtained by manual or automated solid-phase-supported synthesis from Fmoc-amino acid monomers—Fmoc-QXxx-OH, Fmoc-QOMe-OH, Fmoc-P-OH and Fmoc-B*-OH—bearing suitable acid-labile side chain-protecting groups, for example, Boc for QOrn, QDap and QOMe (Fig. 1a). The monomers used in this study are not commercially available and were synthesized following well-established protocols. In general, the carboxylic acid function of the monomers was activated as its acid chloride by applying in situ Appel’s conditions in the presence of triphenylphosphine and trichloroacetonitrile. Coupling reactions to the free amine of an oligomer were performed in the presence of 2,4,6-collidine as a base. Subsequent deprotection of the main chain amine, that is, Fmoc removal, was carried out with 2% DBU (1,8-diazabicyclo[5.4.0]undec-7-ene) in N-methyl-2-pyrrolidone. Removal of the silyl ether protection of QDol was carried out on-resin with 1 M tetrabutylammonium fluoride in THF. Cleavage from the solid support was performed using a mixture of TFA, triisopropylsilane and H2O (95:2.5:2.5; v/v/v) for Wang resin, thereby leading to the deprotection of the other side chains, or with 1% TFA in dichloromethane for SASRIN resin, leaving the other side chain-protecting groups intact. Fragment condensation en route to the C2-symmetrical helical foldamer 4 was performed in DMF with the di-N-hydroxysuccinimide active ester of pyridine-2,6-dicarboxylic acid D and diisopropylethyamine as a base. All foldamer sequences were purified by RP-HPLC.

Nanofitin selection

The combinatorial library of Nanofitins for ribosome display was assembled by two successive overlapping PCRs from degenerate oligonucleotides encoding NNS triplets (N=A, C, T or G and S=C or G). Finally, a PCR step added the 5′- and 3′-flanking regions necessary for ribosome display. The PCR-amplified library was transcribed, and the selection was performed in four rounds at 4 °C against 15 pmol of the immobilized biotinylated foldamer 1a. Amplified DNA material from the last round was cloned between BamHI and HindIII restriction sites of a plasmid derived from pQE-30 (Qiagen), and the ligation mixture was transformed into Escherichia coli DH5α LacIq strains (Invitrogen). Expression of the Nanofitin clones was induced by the addition of isopropyl β-D-1-thiogalactopyranoside (IPTG). The selection target 1a was immobilized on streptavidin (SA) MaxiSorp plates, and crude E. coli extracts were applied to wells with and without immobilized antigen for 1 h. Detection was carried out by the addition of an RGS–His antibody HRP conjugate (Qiagen), followed by the addition of o-phenylenediamine dihydrochloride substrate (Sigma-Aldrich) solution. Absorbance at 450 nm was measured using a Varioskan enzyme-linked immunosorbent assay plate reader (Thermo Scientific), revealing Nanofitin C10 as a binder with a strong signal-to-background ratio.

Nanofitin expression and purification

Nanofitin C10 and the coil-extended versions were expressed recombinantly in E. coli BL21(DE3) as N-terminally His-tagged or MBP-His-tagged fusion proteins. Plasmids (pET-28a(+), pMAL-c5E) were purchased ready to use as lyophilized solids (GenScript). For unlabelled proteins, cultures were grown in LB. For the expression of the [13C,15N]-isotope-labelled C10, M9 minimal medium supplemented with d-glucose-13C6, 15NH4Cl, and trace element solutions was used. Overexpression was induced with IPTG. Purification was carried out by Ni-NTA IMAC. Tag removal was achieved by cleavage with HRV-3C protease overnight. Final purification was carried out by SEC.

Reporting summary

Further information on research design is available in the Nature Portfolio Reporting Summary linked to this article.

Online content

Any methods, additional references, Nature Portfolio reporting summaries, source data, extended data, supplementary information, acknowledgements, peer review information; details of author contributions and competing interests; and statements of data and code availability are available at https://doi.org/10.1038/s41557-026-02222-6.

Supplementary information

Supplementary Information (12.8MB, pdf)

Supplementary Sections 1–5, including Supplementary Figs. 1–18, Supplementary Tables 1–5, legends of Supplementary Videos 1–4 and Supplementary References.

Reporting Summary (80.5KB, pdf)
Supplementary Video 1 (44.1MB, mp4)

Supplementary video—MD simulation of the 1c•C10 complex.

Supplementary Video 2 (1.4MB, mp4)

Supplementary video—animated view of the (P-3•C10)2 complex.

Supplementary Video 3 (5.1MB, mp4)

Supplementary video—animated view of the 8+8 assembly of four (P-3•C10)2 complexes.

Supplementary Video 4 (3.1MB, mp4)

Supplementary video—animated view of the cyclic X-shape assembly of two foldamers P-2b and two C10 coiled-coil dimers.

Source data

Source Data Fig. 1 (492.8KB, xlsx)

Statistical source data for Fig. 1e,f (BLI and CD raw data).

Source Data Fig. 2 (234.9KB, xlsx)

Statistical source data for Fig. 2f,g (CD and BLI raw data).

Source Data Fig. 3 (10.3MB, xlsx)

Statistical source data for Fig. 3b–e (SEC, native MS and collision cross-section).

Acknowledgements

The synchrotron data were collected at beamlines P13 and P14 operated by EMBL Hamburg at the PETRA III storage ring (DESY, Hamburg, Germany). We would like to thank D. von Stetten, G. Grebnev, I. Bento and S. Storm (all from European Molecular Biology Laboratory, Hamburg) for the assistance in using the beamlines. We thank M. Loos, I. Alonso and M. Vançon (all of the Department of Pharmacy, Ludwig-Maximilians-Universität München) for helping with the synthesis of short oligomers as well as the Max Planck Institute for Biochemistry for granting access to their crystal broad screening facility. We thank the Core Facility BioSupraMol, Freie Universität Berlin, for instrument time and support. This work benefited from the facilities and expertise of the Biophysical and Structural Chemistry platform (BPCS) at IECB, CNRS UMS3033, Inserm US001 and Bordeaux University. We thank Axelle Grélard and Estelle Morvan (both from BPCS) for access to the NMR spectrometers and technical assistance.

Author contributions

I.H. and J. Sigl conceived the project. V.M., C.D.M., C.D. and S.H. developed the methodology. J. Sigl, V.M., L.W., J. Sachs, E.M., E.L., N.G., N.Ö., S.K., F.S., L.C., S.H., C.D. and C.D.M. carried out the investigation. I.H., Y.F. and C.D.M. acquired funding for the study. The project was supervised by I.H., Y.F., C.D.M., S.H. and K.P. J. Sigl, C.D.M., C.D. and I.H. wrote the original draft of the paper. All authors reviewed and edited the paper.

Peer review

Peer review information

Nature Chemistry thanks the anonymous reviewers for their contribution to the peer review of this work.

Funding

This study was funded by the Free State of Bavaria under the Excellence Strategy of the Federal Government and the Länder through the ONE MUNICH Project Munich Multiscale Biofabrication (I.H.) and by CNRS-LMU IRP Foldsfun (Y.F. and I.H.). A Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) Walter Benjamin grant (559720072) was awarded to N.G. A Wenner-Gren Foundation fellowship was awarded to N.Ö.Open access funding provided by Ludwig-Maximilians-Universität München.

Data availability

X-ray crystallographic structures have been deposited at the PDB under 9QDO, 9QT7, 9QOG and 9QNU. The ensemble of 20 structures calculated for the 1c•C10 complex has been deposited at the PDB under accession 9T0O. The chemical shift assignments for the unbound C10 and 1c•C10 complex were deposited in the BMRB (https://bmrb.io/) under accession numbers 53300 and 53317, respectively. The raw data that served to create the graphs in Figs. 1, 2 and 3 as well as BLI data have been deposited at Open Data LMU under https://data.ub.uni-muenchen.de/701/1/C10_BLI-raw_Data.zip (https://doi.org/10.5282/ubm/data.818). All other data are available in the article or the Supplementary Information. Source data are provided with this paper.

Competing interests

L.C. and S.H. are employees of Affilogic. The other authors declare that they have no competing interests.

Footnotes

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

Supplementary information

The online version contains supplementary material available at https://doi.org/10.1038/s41557-026-02222-6.

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Supplementary Information (12.8MB, pdf)

Supplementary Sections 1–5, including Supplementary Figs. 1–18, Supplementary Tables 1–5, legends of Supplementary Videos 1–4 and Supplementary References.

Reporting Summary (80.5KB, pdf)
Supplementary Video 1 (44.1MB, mp4)

Supplementary video—MD simulation of the 1c•C10 complex.

Supplementary Video 2 (1.4MB, mp4)

Supplementary video—animated view of the (P-3•C10)2 complex.

Supplementary Video 3 (5.1MB, mp4)

Supplementary video—animated view of the 8+8 assembly of four (P-3•C10)2 complexes.

Supplementary Video 4 (3.1MB, mp4)

Supplementary video—animated view of the cyclic X-shape assembly of two foldamers P-2b and two C10 coiled-coil dimers.

Source Data Fig. 1 (492.8KB, xlsx)

Statistical source data for Fig. 1e,f (BLI and CD raw data).

Source Data Fig. 2 (234.9KB, xlsx)

Statistical source data for Fig. 2f,g (CD and BLI raw data).

Source Data Fig. 3 (10.3MB, xlsx)

Statistical source data for Fig. 3b–e (SEC, native MS and collision cross-section).

Data Availability Statement

X-ray crystallographic structures have been deposited at the PDB under 9QDO, 9QT7, 9QOG and 9QNU. The ensemble of 20 structures calculated for the 1c•C10 complex has been deposited at the PDB under accession 9T0O. The chemical shift assignments for the unbound C10 and 1c•C10 complex were deposited in the BMRB (https://bmrb.io/) under accession numbers 53300 and 53317, respectively. The raw data that served to create the graphs in Figs. 1, 2 and 3 as well as BLI data have been deposited at Open Data LMU under https://data.ub.uni-muenchen.de/701/1/C10_BLI-raw_Data.zip (https://doi.org/10.5282/ubm/data.818). All other data are available in the article or the Supplementary Information. Source data are provided with this paper.


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