Synthesis and structure description of NCU-1. The light brown plate crystal of NCU-1 crystallizes in the orthorhombic space group, Pna21 (Supplementary Table 1). Each Zn2+ is 5-coordinated and binds to two DTB ligands, two BTC, and one water molecule (Fig. 2a). Viewed from the a axis, rectangular windows with a size of 9.9 Å ×5.8 Å can be observed (Fig. 2b, Supplementary Fig. 1). Owing to the two-fold interpenetration, NCU-1 features numerous small square pockets decorated by multipoint functional sites (Fig. 2c, Supplementary Fig. 2). Each of such small pockets with a size of 3.2 Å is constructed by triazole rings and uncoordinated carboxylate groups that better match with the size/shape of the larger light REE ions (Fig. 2d). The PXRD pattern is consistent with that of the simulated one, indicating the phase purity of NCU-1 (Supplementary Fig. 3). Meanwhile, the chemical stabilities of NCU-1 were investigated upon treatments in various pH values ranging from 1 to 13. The crystallinity of this treated NCU-1 was still retained as evidenced by the PXRD patterns (Supplementary Fig. 4). Furthermore, according to the TG analysis, the NCU-1 showed high thermal stability up to 320°C (Supplementary Fig. 5). These results suggest that NCU-1 with good stability in harsh conditions, which is highly desirable for capturing and separating of REEs from mine tailings.
Sorption isotherm analysis. The adsorption isotherms of Pr3+, Nd3+, Gd3+, and Dy3+ were explored at pH 4.5 as representative models of REE ions due to their abundance in mine tailings collected from Ganzhou city, Jiangxi province, a well-known REEs industry center in China (Supplementary Fig. 6–18, Supplementary Table 5). The results showed that the four Ln3+ were fitted well with the Langmuir adsorption model, and the maximum capacity (qm) of Pr3+, Nd3+, Gd3+, and Dy3+ were calculated to be 420, 310, 140, and 126 mg/g, respectively (Fig. 3a, Supplementary Fig. 19–22, Supplementary Table 3). This greatly exceeds the capacity of most current adsorbents, such as CA@Fe3O4 NPs35, KIT-6-1,3-PDDA36, MFC-O37, and PEI800/ES-1/2.138. Energy dispersive X-ray spectroscopy (EDS) mapping analysis confirms that Pr3+, Nd3+, Gd3+, and Dy3+ were entered the structures of the material with a uniform distribution throughout the samples (Supplementary Fig. 23). In X-ray photoelectron spectroscopy (XPS) (Supplementary Fig. 40, Supplementary Fig. 44), the characteristic peaks of Pr3+ and Nd3+ were clearly found after adsorption of Pr3+ and Nd3+, respectively.
Sorption kinetics analysis. The kinetics of NCU-1 for individual Pr3+, Nd3+, Gd3+, and Dy3+ adsorption were then investigated (Supplementary Fig. 24–31, Supplementary Table 4). The REE ions were rapidly captured by NCU-1, all of which reached equilibrium within 1 h, much shorter than those of the other adsorbents. For example, magnetite@MOF39 and hydroxyl-decorated flexible MOF23, require longer than 2–4 h to reach equilibrium. Additionally, for any sorbents, recyclability is crucial for practical implementation. Significantly, the adsorption processes were fully reversible as reflected by the fact that the loaded REE ions can be washed off by diluted HNO3 at pH 3 with maintained capture efficiency for at least four cycles of sorption /desorption (Supplementary Fig. 32–35). These results indicate that NCU-1 can serve robustly towards high efficient REEs recovery and affirm the judicious choice of the MOF for affording selective trapping REEs.
Selectivity. The selectivity of REE ions is a key parameter for evaluating adsorbents. Thereby, the distribution coefficient (Kd) as a barometer for selectivity was also tested. NCU-1 was dispersed in the mixed solutions containing REE ions and interfering ions with different pH values ranging from 2.0 to 6.0 (Fig. 3b). The Kd of NCU-1 to REEs increases rapidly and reaches the maximum when the pH increases from 2.0 to 4.5, and then decreases to 6.0 (Supplementary Table 2). Compared to transition metal ions and alkaline-earth metal ions, the Kd of NCU-1 to REE ions is 3–4 orders of magnitude higher, suggesting a clear advantage of NCU-1 in selective capture of REE ions. Remarkably, the Kd to various rare-earth ions differs significantly at pH 4.5, which induces that the optimal separation selectivity for REEs can be achieved. Generally, a material is considered an excellent adsorbent if Kd is over 104 mL g-1. Particularly, Kd Gd-La was up to 1.6×104-1.0×106 mL g-1 at pH 4.5. Such high Kd indicates that NCU-1 has an obviously higher affinity toward light REE ions.
Tailings treatment. Encouraged by the excellent performance of NCU-1 for extraction and separation of REE ions, we evaluated the ability of NCU-1 to capture and separate REE ions from mine tailing collected from Ganzhou city. The natural rare-earth tailing sample was filtered through a 0.22 µm filter for ICP-MS analysis. The results show that the concentrations of rare earth elements in the tailing are low about 0.09–0.92 ppm, and the competitive ions concentration of Al (8.15 ppm) is about 10 times compared to those of the REEs (Supplementary Table 5), making the REEs adsorption and separation a great challenging task. Notably, except for competing ions, the NCU-1 could effectively selective capture all REE ions from the nature mine tailing (Fig. 3c), manifesting it is a good platform for adsorption and separation of REEs from mine tailings. As an industrially relevant performance test, experimental breakthrough studies were performed to evaluate the actual separation ability of NCU-1 (Supplementary Fig. 36). The competitive ions occurs first at 10 bed volumes and REE ions occur after 50 bed volumes (Fig. 3d, Supplementary Fig. 37), indicating NCU-1 has an excellent separation effect on REE ions from competitive ions. It is worth noting that compared to heavy REE ions, light REE ions have even higher uptakes and larger breakthrough bed volumes. For instance, the breakthrough bed volume of Pr3+ is 150, which is larger than that of Dy3+ (80) (Supplementary Fig. 38). These results illustrate that NCU-1 is a promising candidate for separation and obtaining high purity REE ions from mine tailing over a single step.
Separation mechanism. The FT-IR and XPS were applied to evaluate the structure-performance relationship of NCU-1 in the effective capture of REE ions. The results show that the high adsorption toward REE ions of NCU-1 is ascribed to the strong coordination ability between the REE ions and carboxyl groups, lattice water molecules, and triazolium nitrogen atoms in the host (Supplementary Fig. 39–51). To elucidate the origin of the observed high selectivity of the NCU-1 for REE ions, the first principle calculations were carried out between metal ions and the NCU-1 configurations. In addition, Al3+, Dy3+, and Pr3+ were selected as the representative interfering ions, heavy REEs ions, and light REE ions, respectively. Figure 4a-c show the differential charge density (DCD) maps of NCU-1 configurations after adsorption Al3+, Dy3+, and Pr3+, respectively. Obviously, charge redistribution occurs at metal ions and NCU-1, and the negatively charged regions (yellow) with excess electrons accumulate around the O atoms and N atoms, which is beneficial to the adsorption of metal ions40,41. The Bader charge analysis42 shows that the charges on Al3+ ion in the NCU-1 configuration are + 2.09 e, while + 2.17 e for Dy3+, and increase to + 2.31 e for Pr3+. Generally, the larger the Bader charge, the stronger the binding strength between the host and guests43. Therefore, the order of the binding strength of NCU-1 with the three ions is as follows: Al3+< Dy3+< Pr3+. It suggests that the selectivity of NCU-1 for light REE ions is higher than those of heavy REE ions and interfering ions, due to the more electrons obtained from the host. Moreover, the density functional theory (DFT) calculation clearly reveals that the primary adsorption sites of metal ions are located at the REE nanotraps (Fig. 4d-f). As for Pr3+, two oxygen atoms of the carboxyl group and one water molecule were calculated to coordinate with Pr3+ with the bond distances of 1.79 Å, 2.73 Å, and 1.94 Å, respectively (Supplementary Fig. 52). The calculated distance of Pr3+···N in NCU-1 is 3.30 Å. In the case of Nd3+, it is coordinated to the two oxygen atoms of the carboxyl group and one water molecular with the bond distances of 1.66 Å, 2.76 Å, and 1.86 Å, respectively, and the Nd3+···N bond distance is about 3.27 Å (Supplementary Fig. 53). While as for Al3+, only the coordination bonds between the carboxyl and water molecular oxygen and Al3+ were calculated (Supplementary Fig. 54). The adsorption energies (Eads) of NCU-1 with different metal ions were also calculated to discriminate the adhesion level. The calculated adsorption energy for Al3+, Dy3+, and Pr3+ are − 1.66 eV, -2.58 eV and − 3.29 eV, respectively. It decreases when the size of the adsorbed ions increases, which is fully consistent with our experimental observations. This is partly because the larger Pr3+ (r = 0.99 Å) sterically “matches” better to the nanotraps size/shape than Dy3+ (r = 0.91 Å) and Al3+ (r = 0.50 Å).5,17 Light REE ions within a larger size radius enter the REE nanotraps and coordinate with O and N atoms in them to form a stable rare earth-like hydrated ion structure44. However, competing ions and heavy rare earth ions with a large difference in pore size from NCU-1 have poor binding ability to coordinate with O, which makes the ions easily escape from the pores and achieve high-selectivity separation of light RREs. Therefore, the suitable sizes of the nanotraps and the uncoordinated carboxyl groups and N atoms in nanotraps play a decisive role in the light/heavy REE separation.
Binary REE ions separation. Since the affinity of NCU-1 to REE ions exhibits a unique periodic trend with significant differences, the individual REE can be separated from other REEs by the adsorption method (Fig. 3b). As a proof of concept, a series of experiments (6 combinations in total) were conducted to determine its application on individual REE separations. Consequently, NCU-1 was dispersed into binary mixtures of REE ions (M1 and M2) in a 1:1 molar ratio. As shown in Fig. 5, larger Ln3+ is selectively adsorbed by NCU-1, and smaller Ln3+ almost remained in the solution, indicating that this system successfully separated light/heavy REE mixtures. For a mixtures that contained Nd3+ and Dy3+, the separation factor (SF) reached up to 67, which exceeded those of many materials, for example, TriNOx3- (SFNd:Dy= 8.45 ± 1.62) 4, Zn-BTC (SFNd:Dy= 30.23) 44, TRPO (SFNd:Dy < 5) 11. Especially interesting is the separation factor of 73 observed for Eu3+ over Lu3+, a value that is extremely high than that of the crystallization extraction method recently developed by Wang et al3. Impressively, the case of Pr/Lu, obtains a high separation factor of 579, which is one of the highest single-step separation factors known for REEs separations45. Mixtures that contained Nd: Er also gave an extremely large separation factor of SFNd: Er =273. Generally, NCU-1 demonstrates a clear and high preference for larger-sized REE ions in the solid adsorption process, and the selectivity increases with the ionic radii difference. High-purity individual rare-earth ions can be obtained through one-step adsorption in this work, which has made a breakthrough process in the separation of REEs.