An elastic metal-organic crystal with a densely catenated backbone

Author(s): Wenjing Meng [sup.1] [sup.8] , Shun Kondo [sup.2] , Takuji Ito [sup.3] , Kazuki Komatsu [sup.4] , Jenny Pirillo [sup.5] , Yuh Hijikata [sup.5] , Yuichi Ikuhara [sup.2] , [...]
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 1970s.sup.1-3. 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 indented.sup.4 the crystal along its a/b axes and obtained the Young's moduli of 1.77 [plus or minus] 0.16 GPa in N,N-dimethylformamide and 1.63 [plus or minus] 0.13 GPa in tetrahydrofuran, which are the lowest among those reported so far for porous metal-organic crystals.sup.5. 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. A rubber-like, metal-organic crystal is reported with a mechanically interlocked catenane backbone, which could allow for easy guest molecule uptake and release.