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An elastic metal-organic crystal with a densely catenated backbone.
Meng, Wenjing; Kondo, Shun; Ito, Takuji; Komatsu, Kazuki; Pirillo, Jenny; Hijikata, Yuh; Ikuhara, Yuichi; Aida, Takuzo; Sato, Hiroshi.
Afiliação
  • Meng W; Department of Chemistry and Biotechnology, School of Engineering, The University of Tokyo, Tokyo, Japan.
  • Kondo S; Research Center for Functional Materials, National Institute for Materials Science, Ibaraki, Japan.
  • Ito T; Institute of Engineering Innovation, School of Engineering, The University of Tokyo, Tokyo, Japan.
  • Komatsu K; ELIONIX INC., Tokyo, Japan.
  • Pirillo J; Geochemical Research Center, Graduate School of Science, The University of Tokyo, Tokyo, Japan.
  • Hijikata Y; Institute for Chemical Reaction Design and Discovery (WPI-ICReDD), Hokkaido University, Sapporo, Japan.
  • Ikuhara Y; Institute for Chemical Reaction Design and Discovery (WPI-ICReDD), Hokkaido University, Sapporo, Japan.
  • Aida T; Institute of Engineering Innovation, School of Engineering, The University of Tokyo, Tokyo, Japan.
  • Sato H; Department of Chemistry and Biotechnology, School of Engineering, The University of Tokyo, Tokyo, Japan. aida@macro.t.u-tokyo.ac.jp.
Nature ; 598(7880): 298-303, 2021 10.
Article em En | MEDLINE | ID: mdl-34646002
ABSTRACT
What particular mechanical properties can be expected for materials composed of interlocked backbones has been a long-standing issue in materials science since the first reports on polycatenane and polyrotaxane in the 1970s1-3. Here we report a three-dimensional porous metal-organic crystal, which is exceptional in that its warps and wefts are connected only by catenation. This porous crystal is composed of a tetragonal lattice and dynamically changes its geometry upon guest molecule release, uptake and exchange, and also upon temperature variation even in a low temperature range. We indented4 the crystal along its a/b axes and obtained the Young's moduli of 1.77 ± 0.16 GPa in N,N-dimethylformamide and 1.63 ± 0.13 GPa in tetrahydrofuran, which are the lowest among those reported so far for porous metal-organic crystals5. To our surprise, hydrostatic compression showed that this elastic porous crystal was the most deformable along its c axis, where 5% contraction occurred without structural deterioration upon compression up to 0.88 GPa. The crystal structure obtained at 0.46 GPa showed that the catenated macrocycles move translationally upon contraction. We anticipate our mechanically interlocked molecule-based design to be a starting point for the development of porous materials with exotic mechanical properties. For example, squeezable porous crystals that may address an essential difficulty in realizing both high abilities of guest uptake and release are on the horizon.

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2021 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2021 Tipo de documento: Article