In this study, the synthesis of NH
2-MIL-101(Fe) was according to a previous hydrothermal method, combining Fe(Ⅲ)-based precursors with 2-amino-terephthalic acid (H
2ATA). After activation at 70 ℃ for 12 h, B stalks were attached covalently to the NH
2-MIL-101(Fe) surfaces by means of a post-synthetic amidation reaction between the carboxyl groups of 3-(1
H-benzo[
d]imidazol-1-yl)propanoic acid and the amino groups of NH
2-MIL-101(Fe) to achieve B-MIL-101(Fe) (Fig. S1 in Supporting information). The SEM image of NH
2-MIL-101(Fe) presented octahedral and smooth morphologies (
Fig. 2A and Fig. S2A in Supporting information). After being modified with B stalks, the surface morphology of B-MIL-101(Fe) was changed compared with NH
2-MIL-101(Fe) (
Fig. 2B and Fig. S2B in Supporting information). According to dynamic light scattering measurement (
Fig. 2E), the average hydrodynamic diameters of NH
2-MIL-101(Fe) and B-MIL-101(Fe) were 447.8 nm and 514.8 nm, respectively, which was consistent with the crystal size
ca. 400 nm from SME images and exhibited good dispersibility in aqueous solution. In
Fig. 2F, PXRD patterns of the prepared NH
2-MIL-101(Fe) showed the crystal structure is consistent with that reported in the literature, suggesting the successful preparation of NH
2-MIL-101(Fe) [
57,
58]. After modification of B stalks, the prepared B-MIL-101(Fe) presented new characteristic diffraction peaks compared with NH
2-MIL-101(Fe), validating that B stalk was successfully modified onto the surface of NH
2-MIL-101(Fe). FT-IR spectrum of NH
2-MIL-101(Fe) showed that the characteristic peak at 1578 cm
−1 is attributed to the C=N bond of NH
2-Fe-MIL-101 and the characteristic peak at 3368 cm
–1 corresponded to the symmetrical and asymmetrical stretching vibration of amine groups in NH
2-Fe-MIL-101. After covalent functionalization with B stalks, a new absorption peak was found at 3100 cm
–1 (amide Ⅰ band), which was attributed to the stretching vibration of N-H of the secondary amide groups in B-MIL-101(Fe), belonging to the frequency doubling peak of N-H (1550 cm
–1, amide Ⅱ band) bending vibration. Moreover, the characteristic peak at 1280 cm
–1 was assigned to the stretching vibration of C-N (amide Ⅲ band), and the peak at 1655 cm
–1 corresponded to the vibration of N=C in B-MIL-101(Fe), indicating the successful modification of B stalks on NH
2-MIL-101(Fe) (
Fig. 2G). Furthermore, the TGA was used to study the decomposition behaviors and thermal stability of the nanoplatforms. As seen from the TGA curves, the weight loss of NH
2-MIL-101(Fe) and B-MIL-101(Fe) below 100 ℃ was attributed to the physical adsorption of water in both materials, and the decomposition of organic ligands in the structures was between 100 ℃ and 600 ℃. The weight loss of B stalk was about 8.2% in the range of 110 ℃ to 210 ℃ (
Fig. 2H). After OS loading, the TGA curve of B-MIL-101(Fe)-OS showed that the weight loss of OS was 13.3% between 450 ℃ and 570 ℃, due to the decomposition of OS. The TGA curve of
β-CD@B-MIL-101(Fe)-OS demonstrated that the weight loss of
β-CD was 18.6% between 570 ℃ and 900 ℃. Although it is difficult to determine the exact initial decomposition temperature of OS in
β-CD@B-MIL-101(Fe)-OS, the decomposition temperature shift to a higher temperature direction, indicating enhanced thermal stability of OS loaded in the nanoplatforms. The surface zeta potential value of NH
2-MIL-101(Fe) in deionized water changed from +33.98 mV to +20.06 mV after modification of B stalks and eventually turned to +25.14 mV after loading of OS and immobilization of
β-CD on the surface (Fig. S2C in Supporting information). The type Ⅰ N
2 adsorptiondesorption isotherm indicated the micropore nature of B-MIL-101(Fe) and the corresponding Brunauer-Emmett-Teller (BET) surface area and Barett–Joyner–Halenda (BJH) pore size distribution were measured to be 559.0 m
2/g and 1.9 nm (
Fig. 2I), respectively, indicating a great cargo loading capacity of B-MIL-101(Fe). OS with a molecule size of 0.95 nm in length (Fig. S3A in Supporting information) could be easily loaded into B-MIL-101(Fe)
via physical mixing to form B-MIL-101(Fe)-OS (
Fig. 2C) followed by the significant decrease of BET surface (199.1 m
2/g) and pore volume, and a slight effect of pore diameter (Fig. S4 and Table S1 in Supporting information). To overcome the premature release of OS during post-processing,
β-CD as nanovalves were introduced onto the surface of B-MIL-101(Fe)-OS
via hostguest interactions between the B stalk and the cavity of
β-CD to form
β-CD@B-MIL-101(Fe)-OS nanoplatform (
Fig. 2D). According to the published literature,
N-methylbenzimidazole stalks with the p
Ka value of 5.67 that modified covalently on the surfaces of mesoporous silica nanoparticles could be encircled by the
β-CD ring
via supramolecular interactions at pH 7.4, and release the
β-CD ring at pH < 6 due to the protonation of the aromatic amines [
59]. The related host–guest association between
β-CD and 1-methylbenzimidazole was investigated
via 1H NMR spectroscopy of
β-CD, 1-methylbenzimidazole, and the equimolar mixture of
β-CD and 1-methylbenzimidazole in D
2O (Figs. S5 and S6 in Supporting information). As shown in Fig. S6, after the addition of
β-CD, the alkyl protons signals of the benzene ring in 1-methylbenzimidazole displayed an obvious upfield shift in comparison with pure 1-methylbenzimidazole due to the shielding effect of
β-CD, indicating the existence of host–guest interaction between
β-CD and 1-methylbenzimidazole. The stoichiometry of the host–guest binding mode between
β-CD and 1-methylbenzimidazole was 1:1 according to published literature [
59,
60].