“…A golden rule to design jumping crystals (Figure , top), based on the summarization of occasional phenomenon, as we have recognized, is trying to generate force through stimulating lattice deformation, ,, which is usually triggered by reactions (thermal decomposition of ammonium salts, photoinduced cis–trans isomerization of azos, photoswitchable ring opening and closing of diarylethenes, [2+2] photocycloaddition of olefins or [4+4] photocycloaddition of anthracenes, for example), ,,− conformational transition, ,, packing mode transition, − and molecular machine rotation (rotaxanes-containing or amphidynamic crystals). , Due to the not all-inclusive stimulation, the inhomogeneity caused by varying degrees of lattice deformation on different regions of a crystal provides the motive power for jumping. Nevertheless, there are some issues unsolved in the aforementioned design concept: (1) Specific functional groups and/or molecular backbones are always required, at the expense of time-consuming, complicated molecular design, and synthesis.…”