| Literature DB >> 29695794 |
Sujing Wang1,2, Takashi Kitao3,4,5,6, Nathalie Guillou2, Mohammad Wahiduzzaman7, Charlotte Martineau-Corcos2,8, Farid Nouar1,2, Antoine Tissot1,2, Laurent Binet9, Naseem Ramsahye7, Sabine Devautour-Vinot7, Susumu Kitagawa3,10, Shu Seki11, Yusuke Tsutsui11, Valérie Briois12, Nathalie Steunou2, Guillaume Maurin7, Takashi Uemura13,14,15,16, Christian Serre17,18.
Abstract
Porous titanium oxide materials are attractive for energy-related applications. However, many suffer from poor stability and crystallinity. Here we present a robust nanoporous metal-organic framework (MOF), comprising a Ti12O15 oxocluster and a tetracarboxylate ligand, achieved through a scalable synthesis. This material undergoes an unusual irreversible thermally induced phase transformation that generates a highly crystalline porous product with an infinite inorganic moiety of a very high condensation degree. Preliminary photophysical experiments indicate that the product after phase transformation exhibits photoconductive behavior, highlighting the impact of inorganic unit dimensionality on the alteration of physical properties. Introduction of a conductive polymer into its pores leads to a significant increase of the charge separation lifetime under irradiation. Additionally, the inorganic unit of this Ti-MOF can be easily modified via doping with other metal elements. The combined advantages of this compound make it a promising functional scaffold for practical applications.Entities:
Year: 2018 PMID: 29695794 PMCID: PMC5916937 DOI: 10.1038/s41467-018-04034-w
Source DB: PubMed Journal: Nat Commun ISSN: 2041-1723 Impact factor: 14.919
Fig. 1Structural transformation of and modification to MIL-177 MOFs. A thermally induced structural transformation of the discrete Ti12O15 cluster SBUs linked by bridging formates in MIL-177-LT structure (left) to 1D infinite (Ti6O9)n nanowires in MIL-177-HT structure (middle) is observed with an increase of the condensation degree from 1.25 to 1.5. Introduction of conductive polythiophene into the pores of MIL-177-HT gives rise to a perfectly alternating donor–acceptor architecture for photoconduction application (right top). Other metal species can be doped into the inorganic unit of MIL-177 to introduce modification to its properties (right bottom)
Fig. 2Structural characterization and detail of MIL-177-LT. a SEM image of MIL-177-LT particles with a hexagonal rod morphology and a uniform size distribution. b Final Rietveld plot of MIL-177-LT structure. c Comparison of the PXRD patterns obtained from experimental data, theoretically derived minimum energy structure and refined structure model of MIL-177-LT. d A Ti12O15 cluster SBU with 12 carboxylate groups from mdip linkers (in gray) and terminal formate groups (in red). e Adjacent Ti12O15 cluster SBUs with terminal and bridging formates (in red) connected by mdip linkers (in gray). f Nano-sized channels with a free diameter of 1.1 nm when viewed along the c-axis. g Small channels of 0.3 nm windows when viewed along the b-axis. h Overall pore shape of MIL-177-LT framework. i bnn topological network of MIL-177-LT
Fig. 3Chemical stability test results of MIL-177-LT. a PXRD patterns and b nitrogen adsorption isotherms of MIL-177-LT samples before and after chemical treatment in various acids
Fig. 4Structural characterization and detail of MIL-177-HT. a PXRD comparison between MIL-177-LT and HT compounds. b. Final Rietveld plot of MIL-177-HT structure. c Comparison of the PXRD patterns obtained from experimental data, theoretically derived minimum energy structure and refined structure model of MIL-177-HT. d Adjacent infinite ultrathin (Ti6O9)n nanowires with a thickness of ca. 1 nm connected by mdip linkers (in gray). e Channels between the (Ti6O9)n nanowires array running along the c-axis with a diameter of ca. 0.9 nm. f Small channels of 0.3 nm windows retained when viewed along the b-axis of the MIL-177-HT crystal structure
Fig. 5Physical properties of MIL-177 and related composites. a Total and partial PDOS of MIL-177-HT calculated at the PBEsol level to determine the contribution of the different orbitals. b Conductive transients observed by FP-TRMC upon excitation at 266 nm with a UV laser (MIL-177-HT in blue, MIL-177-LT in green and MIL-125 in orange); c Conductive transients observed by FP-TRMC under 355 nm near-UV irradiation (MIL-177-HT⊃PTh in red, MIL-177-HT in blue, and neat PTh in light green); d Conductive transients observed by FP-TRMC under 355 nm near-UV irradiation showing the extremely long lifetime of MIL-177-HT⊃PTh (>1 ms, in red) with MIL-177-LT⊃PTh in purple and MIL-103(La)⊃PTh in black for comparison