Open Access Article
Antoine
Perennes
a,
Quentin
Sallembien
a,
Weiwei
Fang‡
a,
Stéphane
Grass
b,
Jérôme
Lacour
b,
Laurent
Bouteiller
a and
Matthieu
Raynal
*a
aSorbonne Université, CNRS, Institut Parisien de Chimie Moléculaire, Equipe Chimie des Polymères, 4 Place Jussieu, 75005 Paris, France. E-mail: matthieu.raynal@sorbonne-universite.fr
bDepartment of Organic Chemistry, University of Geneva, Quai Ernest Ansermet 30, 1211 Geneva 4, Switzerland
First published on 10th July 2025
The induction and transmission of chirality across multiple length scales is fundamental to many (bio)chemical processes. For the majority of macromolecular and supramolecular structures adopting a helical configuration, this is harnessed by means of a monomer embedding a stereogenic element, also called a “sergeant” because of its ability to transfer its chirality preference to achiral monomers. Herein, we devise a triarylamine trisamide (TATA) monomer embedding a (thio)urea unit able to interact with a chiral phosphate anion through hydrogen bonding. Thanks to the orthogonal nature of the amide and (thio)urea functions, the anion specifically binds to the (thio)urea unit, thus yielding a supramolecular monomer acting as a “sergeant” i.e. allowing efficient chirality induction in amide-bonded TATA helical copolymers composed of various types of achiral TATA monomers. Unlike covalent “sergeants”, chirality can be induced in situ by binding of the chiral anion to pre-formed coassemblies. In addition, the catalytic performance of TATA coassemblies embedding intrinsically achiral phosphine-functionalized TATA monomers has been evaluated: higher enantioselectivities are reached with the supramolecular versus covalent “sergeant”. Our work may facilitate the design and development of supramolecular “sergeants” as a modular approach to induce chirality in supramolecular helical copolymers and catalysts.
Conventional “sergeants”, i.e. covalent “sergeants”, embed a stereogenic element next to the reactive or interacting groups, for covalent and supramolecular polymers, respectively.6 Given that the nature of the stereogenic group may strongly influence the structure and chiral properties of the polymers, a modular approach for the induction of chirality in these systems is highly desirable. This is quite well-established for covalent helical polymers for which non-covalent or reversible covalent interactions are harnessed between the polymer side chain and chiral “guests” in order to form single handed structures.20 Relevant applications include the possibility to memorize the helical chirality of the polymer backbone21–25 and the development of modular chiroptical sensors26 and asymmetric catalysts.27–30 The strategy is far less developed for supramolecular polymers. This is likely due to the fact that the binding of the chiral inducer must not compete with the formation of assemblies. In other words, orthogonality31 is required between the different types of interactions involved in the assembly process. Chiral solvents are potent chiral inducers for a certain number of supramolecular helical systems.32–34 A few strategies have been devised which involved organic molecules used as chiral additives, yet with different roles. The additive can both bring the chiral information and promote stacking, thus acting as a co-monomer or a template.35–40 Chiral amines,41–43 cations,44,45 or “seeds”46,47 were added to select the handedness of specific helical systems, formed through a mirror-symmetry breaking phenomenon, i.e. supramolecular assemblies and gels that are known to be sensitive to tiny chiral imbalances. Finally, only two studies dealt with supramolecular helical polymers embedding specifically designed receptors or binding sites. Schenning, Meijer and co-workers induced a preferential handedness by combining a chiral acid with π-stacked dimers of a ureidotriazine derivative; limited dynamicity did not allow chirality induction to occur at room temperature.48 Fenniri49 elegantly demonstrated chirality induction in helical rosette nanotubes, thanks to a specific binding of chiral amino acid to crown ether moieties located at the periphery of the nanotubes; chirality induction has an “all-or-none” nature since homochiral nanotubes were obtained provided that most of the binding sites were occupied by the chiral promoter.50 These examples were restricted to homopolymers, i.e. assembly of monomers embedding the receptor site.
Triarylamine trisamide (TATA) monomers belong to the family of disk-like monomers that stack upon each other in apolar solvents, thanks to hydrogen bonding interactions between their amide functions and aromatic interactions between the TA units.51 Chirality induction was previously achieved, thanks to the integration of covalent “sergeants” in the resulting supramolecular TATA copolymers.11 Herein, we develop a new strategy to induce chirality into TATA coassemblies by devising a supramolecular “sergeant” composed of a chiral phosphate anion bonded to the (thio)urea unit of an achiral TATA monomer (Scheme 1b and c). Despite the fact that both binding of the anion and stacking of the monomer rely on hydrogen bonding interactions, orthogonality between the (thio)urea and amide functions allows efficient control of the helical chirality in supramolecular coassemblies between this supramolecular “sergeant” and various achiral TATA monomers (“soldiers”). The design of the supramolecular “sergeant”, through specific interaction of the chiral inducer with the side chain of the TATA monomer, enables in situ control of the copolymer helicity at room temperature; homochirality being obtained with ca. 35% of “sergeants” in the copolymers. In addition, helical coassemblies embedding an achiral phosphine-functionalized TATA monomer proved to be enantioselective, thanks to the presence of the chiral anion at the remote position of the catalytic centre.
The strategy for chirality induction presented in Scheme 1b is highly modular as in principle any chiral anions with an affinity for (thio)urea function could have been selected. For the purpose of demonstrating the feasibility of the concept, we have selected 3,3′-bis(2,4,6-triisopropyl-phenyl)-1,1′-binaphthyl-2,2′-diyl hydrogen phosphate (abbreviated as TRIP) given its ability to bind strongly to dual hydrogen-bond donors such as (thio)ureas.55,56 Both enantiomers of the tetrabutylammonium salt of TRIP have been prepared in one pot from the commercially available phosphoric acids (see the ESI†).57 These chiral salts proved to be well soluble in toluene and MCH, suitable solvents for enhancing both anion binding to the (thio)urea and polymerization of the TATA monomers through hydrogen bond and aromatic interactions.
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Fig. 1 Characterization of the supramolecular “sergeant”. CD (a) and UV-Vis analyses (b) of the supramolecular “sergeants” formed by mixing TATA TU or TATA p-U (2.9 mM) with (R) or (S)-TRIP·NBu4 (2.9 mM) in toluene (1 : 1 mixture). The spectrum in THF is also shown for the mixture between TATA TU and (S)-TRIP·NBu4. The contribution of the signal coming from the chiral salt is subtracted (see Fig. S2 and S4† for non-subtracted spectra). (c) FT-IR analyses of the “supramolecular sergeant” formed by mixing TATA TU with (R)-TRIP·NBu4 in toluene (1 : 1 mixture, 5.8 mM total concentration). (d) FT-IR analysis of the “supramolecular sergeant” formed by mixing TATA p-U with (R)-TRIP·NBu4 in toluene (1 : 1 mixture, 5.8 mM total concentration). Zoom on the N–H and C O regions. FT-IR spectra for supramolecular stacks with free (thio)urea functions [simul. 1] and (thio)urea functions bonded to (R)-TRIP·NBu4 [simul. 2] have been simulated as indicated in the ESI.† | ||
We next conducted experiments to better apprehend the structure of the adduct formed between TATA TU or TATA p-U and TRIP·NBu4. First, a TATA monomer, named the TATA model, was studied which is similar to TATA TU or TATA p-U but lacks the terminal (thio)urea function (Fig. S6†). This monomer fully assembles into (racemic) helical stacks in toluene, as deduced from its FT-IR spectrum showing characteristic bands for associated amide functions, as well as its ability to form a gel, as a probable result of the formation of entangled fibres. Upon addition of one equivalent of (R)-TRIP·NBu4, the gel is weaker but the viscosity of the solution remains high (Fig. S6a†). In addition, no significant change and induced CD band can be detected from FT-IR and CD analyses, respectively (Fig. S6b and c†). This indicates that the interaction between the chiral anion and the amide functions of TATA assemblies is not very strong; thus TRIP·NBu4 is not a good chain stopper of the supramolecular chains formed by TATA monomers.58 Second, the equimolar mixtures between TATA TU or TATA p-U and (R)-TRIP·NBu4, identical to those characterized by CD, have also been analysed by FT-IR (Fig. 1c and d). The obtained experimental spectra were compared with simulated ones for supramolecular amide-bonded stacks of TATA TU or TATA p-U with (thio)urea functions free or bonded to (R)-TRIP·NBu4, corresponding to simulations 1 and 2, respectively (see Fig. S7 and the ESI† for the procedures). Experimental spectra of the mixtures are closer to simulation 2 since no (or few) free N–H group can be detected (above 3350 cm−1). For TATA p-U, free C
O (1707 cm−1) belonging to the urea functions can be observed which is consistent with urea acting as a dual hydrogen-bond donor of the TRIP anion. The band attributed to amide C
O (maximum at 1640 cm−1) is rather broad for both mixtures, this can be due to the fact that the supramolecular stacks are either short or contain some structural defects, probably because of the steric hindrance generated by the TRIP anion located in the side chain. These experiments support the orthogonality of the interaction of the anion which is selective for the thiourea and urea functions, consistent with previous reports in the literature for which the association constant of the dihydrogen phosphate anion for (thio)urea was two orders of magnitude greater than that for amide.59 Based on these analyses, the assembled two-component aggregate composed of the TATA monomer and the chiral anion embeds the TRIP anion that is non-covalently bonded to the lateral (thio)urea group; it can thus be considered as a supramolecular “sergeant”.
The stability of the supramolecular “sergeants” was subsequently probed by CD analyses conducted between 293 K and 393 K (Fig. S8†). These analyses are consistent with the dissociation of the (thio)urea – chiral anion supramolecular couple upon increasing the temperature. This disassembly process is gradual for both TATA p-U and TATA TU. Even though the different assembly behaviour between these two monomers is difficult to assess quantitatively, we noticed that: (i) a higher fraction of the chiral anion is necessary to dissolve TATA p-U, (ii) the intensity of the induced CD signal above 250 nm for TATA p-U is lower than that observed for TATA TU (Fig. 1a, S4 and S8†) and, (iii) the solution containing the supramolecular “sergeant” composed of TATA p-U tends to precipitate over time (Fig. S8†). All these observations suggest that the interaction between TATA TU and TRIP·NBu4 is stronger than that of TATA p-U with the same anion, as a probable result of the higher acidity of the thiourea function.52 The next experiments will be conducted at 293 K, a temperature for which the chiral anion is strongly bound to the (thio)urea function.
:
1 ratio) was selected as the supramolecular “sergeant”. CD analyses of mixtures containing various fractions of the “sergeant” have been performed; the concentration in TATA C8 being set constant to 0.2 mM (Fig. 2a and S9†). Mixtures were prepared sequentially; the solution containing the supramolecular “sergeant” was prepared independently and added to the “soldier”. Comparison of the CD spectra of the mixtures with that obtained for the supramolecular “sergeant” alone shows major differences: CD patterns are different and more strikingly, the intensity of the CD bands is drastically higher for the mixtures (Fig. 2a). The CD signals in the 275–400 nm region for the mixtures with three maxima at λ ≈ 353 nm, λ ≈ 319 nm and λ ≈ 298 nm and a crossover point at ca. 332 nm are characteristic of helical stacks of TATA monomers with a preferred handedness.11,60 In addition, mixtures embedding 40% and 50% of the supramolecular “sergeant” exhibit a CD spectrum which is virtually identical to that of (S)-TATA*, a covalent “sergeant” (Fig. S9†). The molar CD values actually plateau for a fraction of “sergeants” in the mixtures being equal or greater than 40% (Fig. 2c). All these analyses are consistent with the ability of the supramolecular “sergeant”, composed of TATA p-U and (S)-TRIP·NBu4, to coassemble with TATA C8 and impose its preferred handedness, eventually leading to homochiral stacks when at least 40% of sergeants are present in the coassemblies (Fig. 2d, schematic representation of the coassemblies in the upper part of Fig. 2).
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Fig. 2 Transfer of chirality of the supramolecular “sergeant” to the “soldier”, TATA C8. (Top) Schematic representation of the copolymerization between the supramolecular “sergeant” and TATA C8. (a) CD analyses of the mixtures containing the supramolecular “sergeant” (1 : 1 mixture of TATA p-U and (S)-TRIP·NBu4) and TATA C8 (0.20 mM) in toluene. The amount of supramolecular “sergeant” in the mixtures is equal to 0.01 mM, 0.02 mM, 0.04 mM, 0.05 mM, 0.13 mM and 0.20 mM corresponding to fractions of supramolecular “sergeant” of 5%, 10%, 15%, 20%, 40%, and 50%, respectively. The fraction of “sergeant” is defined as the ratio of the concentration in TATA p-U to the total concentration in TATA monomers (TATA p-U + TATA C8) in the mixtures. The spectrum of the supramolecular “sergeant” alone composed of TATA p-U and (S)-TRIP·NBu4 (0.2 mM + 0.2 mM) is shown for comparison. (b) UV-Vis spectra corresponding to data in (a). (c) Plot of the molar CD values (Δε) as a function of the fraction of supramolecular “sergeant” in the mixtures. The molar CD values are reported at two different wavelengths after subtracting the contribution of the supramolecular “sergeant” and by considering only the concentration of TATA C8 for the remaining CD signal (Fig. S9†). Δε = θ/(32 982 × [TATA C8] × l), with θ = ellipticity (in mdeg), [TATA C8] = concentration in TATA C8 (in mol L−1), and l = cell pathlength (in cm). (d) Plot of the net helicity as a function of the fraction of supramolecular “sergeant” in the mixtures. The net helicity corresponds to the ratio between Δε of the mixture and Δε max (maximal Δε values measured for the different mixtures). For (c) and (d), the lines are a guide to the eye. | ||
We next tested the scope of this chirality induction process by examining other TATA coassemblies (Fig. 3). This time, the combination of TATA TU and TRIP·NBu4 was selected as the supramolecular “sergeant” and achiral TATA monomers of diverse chemical structures as “soldiers”, including one “soldier” (TATA N C20)61,62 with amide functions connected to their N atoms to the TA core, i.e. inverted connectivity relative to TATA TU. All mixtures contain a fraction of supramolecular “sergeant” of 50%. In all cases, the CD signals of the “sergeants-and-soldiers”-type mixtures are of higher intensity than those of the supramolecular “sergeant” alone (Fig. S10–S13†).
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| Fig. 3 Transfer of chirality of the supramolecular “sergeant” to other “soldiers”. (Top) Schematic representation of the copolymerization between the supramolecular “sergeant” and various “soldiers”. The supramolecular “sergeant” consists of an equimolar mixture between TATA TU and either (S)-TRIP·NBu4 or (R)-TRIP·NBu4 (2.9 mM + 2.9 mM). CD analyses of the “sergeants-and-soldiers”-type mixtures (fs = 50%) containing TATA C8 (a), TATA P (b), TATA PCF3 (c) and TATA N C20 (d) as “soldiers” (2.9 mM). CD spectra have been processed as follows: the contribution of the supramolecular “sergeant” was subtracted from the pristine CD spectra and CD values were converted into molar CD values by considering only the concentration of the “soldier”. The difference in concentrations for the mixtures was also considered. See Fig. S10–S13† for the pristine CD and UV/Vis spectra. | ||
CD spectra are similar regardless of the “soldier” and are characterized by a dominant CD band at λ ≈ 360 nm and two minor bands of opposite intensities with one maximum at λ ≈ 325 nm and one at λ ≈ 295 nm. Two crossover points are thus detected, the first one at λ = 340 nm, which is common to all mixtures, while the position of the second one varies according to the nature of the “soldier”. The different CD signatures for the coassemblies depending on whether TATA p-U/TRIP·NBu4 or TATA TU/TRIP·NBu4 is used as “sergeant” suggest that these two supramolecular “sergeants” induce different conformations in the coassemblies. Anyway, the higher intensity of the CD signals (relative to the “sergeant”) and the fact that enantiomers of TRIP·NBu4 furnish mirror-image CD spectra are consistent with transfer of chirality of the supramolecular “sergeant” to helical TATA coassemblies for all “soldiers” as represented schematically in the upper part of Fig. 3. This includes chirality induction in TATA ligands, TATA P and TATA PCF3, a crucial point for their implementation in asymmetric catalysis (see below). In the case of TATA P, coassembly also occurs in MCH, and additional bands specific to the copolymers are detected in this solvent (Fig. S11†). Monomer TATA N C20, despite having a different connection of its amide functions relative to TATA TU, also coassembles with the supramolecular “sergeant”. The ability of monomers with different amide connectivities to coassemble into the same stacks was previously demonstrated for BTA-based supramolecular polymers.63 Our approach appears quite general and may be applied for the construction of various helically biased TATA copolymers.
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| Fig. 4 Chirality induction in pre-formed TATA copolymers. (Top) Schematic representation of the formation of helically biased TATA copolymers by addition of the chiral anion to pre-formed TATA coassemblies. *The thiourea functions in the racemic stacks are not free (see Fig. S15†). (a) CD spectra of “sergeants-and-soldiers”-type mixtures obtained by adding (S)-TRIP·NBu4 (0–100% relative to TATA TU, 0–2.9 mM) to pre-formed coassemblies between TATA P (2.9 mM) and TATA TU (2.9 mM) in toluene. (b) Plot of the CD signal (λ = 363.0 nm) as a function of the percentage of (S)-TRIP·NBu4 added to the mixtures (relative to TATA TU). | ||
We examined in more detail the dynamic induction of chirality in pre-formed stacks of TATA P and TATA TU. Incremental quantities of (S)-TRIP·NBu4 were added to equimolar mixtures of TATA P and TATA TU. CD (Fig. 4a) and FT-IR (Fig. S15†) analyses of the corresponding solutions were performed. CD spectra (Fig. 4a) exhibit a nonlinear increase of the intensity of the CD bands relative to the percentage of (S)-TRIP·NBu4 added to the mixtures. This is particularly obvious for the CD band at λ = 363.0 nm (Fig. 4b). This trend can be explained by considering two extreme states for the TATA copolymers. In the first state, there is no (or very low) chirality transfer to TATA P, i.e. the amount of supramolecular “sergeant” formed is not sufficient to induce a preferred handedness in the copolymers. In the second state, the quantity of “sergeants” is sufficient to bias the helicity of the copolymers. The nonlinear increase of the CD signal is an attribute of the “sergeants-and-soldiers” effect, as further corroborated by the fact that a linear evolution of the CD signal is observed when a molecular thiourea model is mixed with (S)-TRIP·NBu4 (Fig. S5†). FT-IR analyses of the mixtures (Fig. S15†) are also consistent with two main states for the coassemblies since two types of FT-IR spectra with small but significant shifts of the N–H and C
O stretching frequencies are observed for mixtures with low and high amounts of (S)-TRIP·NBu4. FT-IR analyses bring the additional information that at least part of the thiourea functions are bonded to each other in the initial TATA copolymers (see the notes in the captions of Fig. 4 and S15†). It thus appears that binding of the TRIP anion with the thiourea competes with the ability of thiourea functions to bind together. If we consider that all anions are bonded to thiourea, full chirality induction is achieved for a fraction of supramolecular “sergeants” in the coassemblies of ca. 35% ([(S)-TRIP·NBu4]/(TATA TU + TATA P) for the plateau in Fig. 4b). This is consistent with the quantity of supramolecular “sergeants” required to fully bias the sense of rotation of the TATA copolymers embedding TATA C8 as the “soldier” (Fig. 2).
The copper-catalyzed hydrosilylation of 4-nitroacetophenone has been selected as a benchmark reaction64 to test whether chirality induction into the TATA copolymers can be transferred to the copper atoms, centers of the asymmetric catalytic reaction. Initial tests help to identify TATA PCF3 as a more efficient ligand than TATA P; the presence of the CF3 groups on the aryl rings connected to the phosphorus atom was also beneficial in the case of BTA-based helical catalysts (Table S1†).54 Supramolecular and covalent “sergeants” were thus evaluated with TATA PCF3 for the catalytic reaction. The fraction of “sergeant” in the mixtures of 50% ensures full induction of chirality, as probed above by CD measurements (Fig. 4). (R)-TRIP·NBu4, on its own, does not induce selectivity in the reaction (Table 1, entry 1). Limited conversion in this case can infer competitive binding of the TRIP anion to the copper atoms. The supramolecular “sergeant” composed of TATA TU and TRIP led to no conversion (entries 2 and3). This can be explained by the well-established strong interaction between copper(I) and sulfur, i.e. thiophilicity which prevents coordination of the substrate to the copper center.65 We were pleased to see that full conversion was achieved when urea-functionalized TATA monomers were present in the catalytic mixtures. More interestingly, TATA p-U displayed significant enantioselectivities since both enantiomers of 4-nitroacetophenol were obtained with ca. 30% enantiomeric excess (ee) depending on the configuration of the TRIP anion (entries 6 and 7). The same mixture was poorly active and selective in THF (entries 8 and 9), further corroborating that chirality induction occurs within TATA copolymers. In contrast, TATA m-U showed no selectivity: this suggests either non-optimal coassembly between TATA PCF3 and TATA m-U or an unfavorable geometry preventing transfer of chirality to the copper atom (entries 4 and 5).
| Entry | “Sergeant” or “chiral inducer” | Conversion | ee ± 2 (%) |
|---|---|---|---|
| a In THF. | |||
| 1 | (R)-TRIP·NBu4 | 50% | +2 |
| 2 | TATA TU + (S)-TRIP·NBu4 | 0% | n.d. |
| 3 | TATA TU + (R)-TRIP·NBu4 | 0% | n.d. |
| 4 | TATA m-U + (S)-TRIP·NBu4 | 84% | 0 |
| 5 | TATA m-U + (R)-TRIP·NBu4 | 99% | 0 |
| 6 | TATA p-U + (S)-TRIP·NBu4 | 99% | −35 |
| 7 | TATA p-U + (R)-TRIP·NBu4 | 98% | +30 |
| 8a | TATA p-U + (S)-TRIP·NBu4 | 40% | +5 |
| 9a | TATA p-U + (R)-TRIP·NBu4 | 13% | −5 |
| 10 | (S)-TATA* | 92% | −8 |
| 11 | (R)-TATA* | 95% | +9 |
The couple TATA p-U/TRIP thus constitutes the best tested supramolecular “sergeant” for the hydrosilylation reaction. Its selectivity is significantly higher than the one provided by TATA*, a covalent “sergeant” (8–9% ee, entries 10 and 11). It was previously found with BTA-based helical catalysts that the main difference in the displayed selectivities was related to the ability of the “sergeant” to intercalate efficiently into the stacks formed by the ligand.17,66 Herein, CD analyses suggest that both TATA p-U/TRIP and TATA* coassemble with the TATA “soldier” (Fig. S9†). Two possible pathways for chirality induction in catalytic TATA copolymers can thus be envisaged: (i) the anticipated induction of chirality “through bond” that allows to provide a chiral environment to the catalytic copper centre through a four-level induction of chirality from the chiral anion to the copper centre through the main chain of the supramolecular copolymer (as represented by the four red arrows in Fig. 5, left); the difference in selectivities between TATA p-U/TRIP and TATA* may arise from a different conformation induced to TATA PCF3 by the “sergeants”, (ii) an alternative induction of chirality through space because of the local proximity between the TRIP anion and the copper atom at the periphery of the TATA copolymers (Fig. 5, right); this mechanism may allow a better stereodiscrimination of the transition states explaining the superiority of TATA p-U/TRIP over TATA*.67 These pathways can actually constitute two limited structures; it can also be envisaged as contribution of both pathways for biasing the stereochemical outcome of the reaction with the supramolecular “sergeant”. Even though the overall enantioselectivities are significantly lower than those obtained with BTA-based helical catalysts13,17,18,66,68 under similar conditions, there is arguably room for further optimization notably through the screening of chiral anions of varied chemical natures,69–71 a strategy not accessible with conventional “sergeants”.
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| Fig. 5 Possible modes of chirality induction in supramolecular helical TATA catalysts embedding a supramolecular “sergeant”. S: substrate, P: product. | ||
Footnotes |
| † Electronic supplementary information (ESI) available: Supplementary chart (Chart S1), figures (Fig. S1–S58), table (Table S1), general methods, preparation protocols of the solutions for spectroscopic analyses and catalysis, synthetic procedures for the preparation of the monomers, selected chiral GC traces, and NMR spectra of the synthesized molecules. See DOI: https://doi.org/10.1039/d5sc02159f |
| ‡ Current address: College of Chemical Engineering, Nanjing Forestry University, 159 Longpan Road, 210037, Nanjing, China. |
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