The first wide‐view image of multiple structural and phase transformations for MOFs, ranging from crystal state transformations to the extreme limit approaching liquid/glass phase, was presented. The process involves i) an initial crystalline transformation from square‐ layer framework [Co 2 (pybz) 2 (CH 3 COO) 2 ] ⋅ DMF ( Co2 ) to a 3‐fold interpenetrated and ordered vacancies contained framework [Co(pybz) 2 (CH 3 OH) 2 ] ⋅ 2CH 3 OH ( CoM ) due to in situ disassemble‐reassemble, ii) thermal induced departure of a pair of cis ‐form coordinated methanol in CoM leads to amorphous framework a ‐dCoM , iii) glass transition to super‐cooled liquid scl ‐dCoM , iv) obtaining MOF glass g ‐dCoM upon quenching the super‐cooled liquid, and v) re‐crystallization of super‐cooled liquid generates 6‐fold interpenetrated dia ‐ net framework [Co(pybz) 2 ] 6n ( rec ‐dCoM ) under further heating. The access to glass from CoM , provides a new self‐perturbation strategy to create MOF glasses without melting. The wider pore size distribution in amorphous/glassy MOFs than crystalline precursor achieved the first time selective hydrocarbon gas separation by breakthrough experiments, which bring efficient separation of 1 : 99 C 2 H 2 /C 2 H 4 by either a ‐dCoM or g ‐dCoM and produce polymer grade C 2 H 4 with purity≥99.5 % after a single adsorption process. Furthermore, the mixture of 50 : 50 C 3 H 6 /C 3 H 8 can be separated by a ‐dCoM .
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Li et al. (2024) studied this question.
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