Structure and Photoluminescence Tuning Features of Mn2+- and Ln3+-Activated Zn-Based Heterometal–Organic Frameworks (MOFs) with a Single 5-Methylisophthalic Acid Ligand
2011-10-17T00:00:00Z (GMT) by
In attempts to investigate whether the photoluminescence properties of the Zn-based heterometal–organic frameworks (MOFs) could be tuned by doping different Ln3+ (Ln = Sm, Eu, Tb) and Mn2+ ions, seven novel 3D homo- and hetero-MOFs with a rich variety of network topologies, namely, [Zn(mip)]n (Zn–Zn), [Zn2Mn(OH)2(mip)2]n (Zn–Mn), [Mn2Mn(OH)2(mip)2]n (Mn–Mn), [ZnSm(OH)(mip)2]n (Zn–Sm), [ZnEu(OH)(mip)2]n (Zn–Eu1), [Zn5Eu(OH)(H2O)3(mip)6·(H2O)]n (Zn–Eu2), and [Zn5Tb(OH)(H2O)3(mip)6]n (Zn–Tb), (mip = 5-methylisophthalate dianion), have been synthesized hydrothermally based on a single 5-methylisophthalic acid ligand. All compounds are fully structurally characterized by elemental analysis, FT-IR spectroscopy, TG-DTA analysis, single-crystal X-ray diffraction, and X-ray powder diffraction (XRPD) techniques. The various connectivity modes of the mip linkers generate four types of different structures. Type I (Zn–Zn) is a 3D homo-MOF with helical channels composed of Zn2(COO)4 SBUs (second building units). Type II (Zn–Mn and Mn–Mn) displays a nest-like 3D homo- or hetero-MOF featuring window-shaped helical channels composed of Zn4Mn2(OH)4(COO)8 or Mn4Mn2(OH)4(COO)8 SBUs. Type III (Zn–Sm and Zn–Eu1) presents a complicated corbeil-like 3D hetero-MOF with irregular helical channels composed of (SmZnO)2(COO)8 or (EuZnO)2(COO)8 heterometallic SBUs. Type IV (Zn–Eu2 and Zn–Tb) contains a heterometallic SBU Zn5Eu(OH)(COO)12 or Zn5Tb(OH)(COO)12, which results in a 3D hetero-MOF featuring irregular channels impregnated by parts of the free and coordinated water molecules. Photoluminescence properties indicate that all of the compounds exhibit photoluminescence in the solid state at room temperature. Compared with a broad emission band at ca. 475 nm (λex = 380 nm) for Zn–Zn, compound Zn–Mn exhibits a remarkably intense emission band centered at 737 nm (λex = 320 nm) due to the characteristic emission of Mn2+. In addition, the fluorescence intensity of compound Zn–Mn is stronger than that of Mn–Mn as a result of Zn2+ behaving as an activator for the Mn2+ emission. Compound Zn–Sm displays a typical Sm3+ emission spectrum, and the peak at 596 nm is the strongest one (λex = 310 nm). Both Zn–Eu1 and Zn–Eu2 give the characteristic emission transitions of the Eu3+ ions (λex = 310 nm). Thanks to the ambient different crystal-field strengths, crystal field symmetries, and coordinated bonds of the Eu3+ ions in compounds Zn–Eu1 and Zn–Eu2, the spectrum of the former compound is dominated by the 5D0 → 7F2 transition (612 nm), while the emission of the 5D0 → 7F4 transition (699 nm) for the latter one is the most intense. Compound Zn–Tb emits the characteristic Tb3+ ion spectrum dominated by the 5D4 → 7F5 (544 nm) transition. Upon addition of the different activated ions, the luminescence lifetimes of the compounds are also changed from the nanosecond (Zn–Zn) to the microsecond (Zn–Mn, Mn–Mn, and Zn–Sm) and millisecond (Zn–Eu1, Zn–Eu2, and Zn–Tb) magnitude orders. The structure and photoluminescent property correlations suggest that the presence of Mn2+ and Ln3+ ions can activate the Zn-based hetero-MOFs to emit the tunable photoluminescence.