2020
DOI: 10.1364/oe.393197
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Fast self-assembly of macroscopic blue phase 3D photonic crystals

Abstract: Blue phase (BP) liquid crystals are materials with unique self-assembling properties. They can be regarded as 3D photonic crystals as they organize in 3D cubic structures with sub-micrometer range periodicity and display selective optical bandgaps. Yet, the obtained BP crystals are usually polycrystalline or micrometer-sized monocrystals. Producing large BP monocrystals has proven to be a challenging and time-consuming endeavor, due to BP crystal growth being notoriously slow and the complex requirements for a… Show more

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Cited by 21 publications
(14 citation statements)
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References 27 publications
(39 reference statements)
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“…Note also that the influence of a CLC periodic structure on the Cherenkov radiation in a CLC is similar to the one in the case of fluorescence in a CLC and, compared to the case of a homogeneous liquid, the additional diffraction Cherenkov cone in CLC (see Chpt.9 in [12]) is very similar to the fluorescence KLs studied above. Finally, it should be mentioned that the fluorescence KLs structure in Blue Phases (BPs) is very similar to the X-rays KLs because in the BP case the fluorescence KL cones are formed around different directions, as it happens in conventional crystals in the X-ray case (it was experimentally observed for BPs, see, for example [16][17][18]), in contrast to the CLC case, where all fluorescence KL cones are formed around the CLC spiral axis.…”
Section: Discussionmentioning
confidence: 99%
“…Note also that the influence of a CLC periodic structure on the Cherenkov radiation in a CLC is similar to the one in the case of fluorescence in a CLC and, compared to the case of a homogeneous liquid, the additional diffraction Cherenkov cone in CLC (see Chpt.9 in [12]) is very similar to the fluorescence KLs studied above. Finally, it should be mentioned that the fluorescence KLs structure in Blue Phases (BPs) is very similar to the X-rays KLs because in the BP case the fluorescence KL cones are formed around different directions, as it happens in conventional crystals in the X-ray case (it was experimentally observed for BPs, see, for example [16][17][18]), in contrast to the CLC case, where all fluorescence KL cones are formed around the CLC spiral axis.…”
Section: Discussionmentioning
confidence: 99%
“…Otón et al prepared large monocrystalline BPLCs with ideal lattice orientation by a simple surface treatment and controlling the amount of precursor materials. [ 127,128 ] Instead of using traditional polyimide as alignment layers, they used Nylon 6 and Nylon 6‐6 polyamide layers. The anchoring energies of polyamide are one or two orders of magnitude lower than that of polyimides.…”
Section: Lattice Orientation Control Of Bplcsmentioning
confidence: 99%
“…To improve the response time of the LC device, manipulation with a driving signal, temperature, thickness of the LC layer or changes to the order of the molecules can be used. Furthermore, special materials have been designed to meet the requirements of fast response time, such as the cholesterics [ 31 ], blue phases [ 32 ] or very fast DFLCs [ 33 , 34 ] mentioned above. An interesting and promising method to speed up the response time is polymerization of the LC host with a monomer to obtain a polymer network LC (PNLC) and polymer-stabilized LC (PSLC) [ 35 , 36 , 37 ].…”
Section: Introductionmentioning
confidence: 99%