Abstract
This study introduces mechanically induced novel phenomena such as standing, leaning, stacking, and interlocking behaviors in naturally twisted optical waveguiding microcrystals on a substrate. The twisted crystal self-assembled from 2,4-dibromo-6-(((2-bromo-5-fluorophenyl)imino)methyl)phenol is flexible and emits orange fluorescence. Crystal’s mechanical flexibility in the perpendicular direction to (001) and (010) planes can be attributed to intermolecular interactions, including C-H···Br, N-H···O, C-H···O, and π···π stacking interactions. Through a systematic process involving step-by-step bending and subsequent optical waveguiding experiments at each bent position, a linear relationship between optical loss and mechanical strain is established. Additionally, the vertical standing and leaning of these crystals at different angles on a flat surface and the vertical stacking of multiple crystals reveal the three-dimensional aspects of organic crystal waveguides, introducing light trajectories in a 3D space. Furthermore, the integration of two axially interlocked twisted crystals enables the coupling of polarization along their long axis. These novel crystal dynamics expand the horizons of crystal behavior and have the potential to revolutionize various applications, rendering these crystals invaluable in the realm of crystal-related science and technology.
Supplementary materials
Title
Supporting Info
Description
1 a) Synthesis of BFIMP (Scheme S1)
b) Preparation of microcrystals of BFIMP.
2 Materials.
3 Instrumental Methods.
4 Figure S1 and S2. 1H-and 13C-NMR spectra of BFIMP.
5 Figure S3. ORTEP view and face-indexed data of BFIMP.
6 Table S1: Crystallographic data of BFIMP.
7 Figure S4. Growth of several orientationally mismatched entwined nanofibres, their cooperative interaction and the associated interfacial strain causing spontaneous twists in growing crystals.
8 Figure S5. EDX analysis of twisted microcrystal.
9 Figure S6. FL lifetime imaging of twisted microcrystals.
10 Figure S7. Optical waveguiding experiments of straight and extreme bent geometry of twisted microcrystal.
11 Figure S8. Rolling operation on twisted microcrystal.
12 Figure S9. Colour coded FESEM images of standing twisted microcrystals on various substrates
13 Figure S10. Polarisation dependent photonic investigations of entwined microcrystal.
14 Figure S11. FESEM images of axially interlocked twisted microcrystals of length 50 µm and 83 µm.
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