Liquid-crystal space and wavelength routing switches

Author(s):  
Kuang-Yi Wu ◽  
Jian-Yu Liu
2018 ◽  
Vol 6 (5) ◽  
pp. 380 ◽  
Author(s):  
Zepeng Pan ◽  
Songnian Fu ◽  
Luluzi Lu ◽  
Dongyu Li ◽  
Weijie Chang ◽  
...  

2001 ◽  
Vol 40 (8) ◽  
pp. 1521 ◽  
Author(s):  
Sarun Sumriddetchkajorn

Author(s):  
M. Rodelgo-Lacruz ◽  
C. Lopez-Bravo ◽  
F. J. Gonzalez-Castano ◽  
H. J. Chao

2019 ◽  
Vol 46 (4) ◽  
pp. 126-129 ◽  
Author(s):  
D. S. Goncharov ◽  
E. Yu. Zlokazov ◽  
E. K. Petrova ◽  
N. M. Ponomarev ◽  
R. S. Starikov

Author(s):  
K.J. Ihn ◽  
R. Pindak ◽  
J. A. N. Zasadzinski

A new liquid crystal (called the smectic-A* phase) that combines cholesteric twist and smectic layering was a surprise as smectic phases preclude twist distortions. However, the twist grain boundary (TGB) model of Renn and Lubensky predicted a defect-mediated smectic phase that incorporates cholesteric twist by a lattice of screw dislocations. The TGB model for the liquid crystal analog of the Abrikosov phase of superconductors consists of regularly spaced grain boundaries of screw dislocations, parallel to each other within the grain boundary, but rotated by a fixed angle with respect to adjacent grain boundaries. The dislocations divide the layers into blocks which rotate by a discrete amount, Δθ, given by the ratio of the layer spacing, d, to the distance between grain boundaries, lb; Δθ ≈ d/lb (Fig. 1).


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