2003
DOI: 10.1038/nmat979
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Exploring for 3D photonic bandgap structures in the 11 f.c.c. space groups

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Cited by 88 publications
(77 citation statements)
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“…[17] Moreover, controlling their architecture and interaction has led to open, simple cubic, and diamond networks, [71] which are known to be useful candidates for photonic applications. [72][73][74][75] As the spacing and characteristics of individual domains can be tuned in a reliable manner, it is possible to propose new and previously inaccessible structures, as well as create complex and hierarchical morphologies. [76][77][78][79][80][81][82][83] Finally, the solvent selectivity is important to the kinds of morphologies that will assemble, and has been found to dramatically affect the nature of self-assembled structures allowing for a wide variety of tunable micellar structures.…”
Section: Computational Design Of Functional Nanostructuresmentioning
confidence: 99%
“…[17] Moreover, controlling their architecture and interaction has led to open, simple cubic, and diamond networks, [71] which are known to be useful candidates for photonic applications. [72][73][74][75] As the spacing and characteristics of individual domains can be tuned in a reliable manner, it is possible to propose new and previously inaccessible structures, as well as create complex and hierarchical morphologies. [76][77][78][79][80][81][82][83] Finally, the solvent selectivity is important to the kinds of morphologies that will assemble, and has been found to dramatically affect the nature of self-assembled structures allowing for a wide variety of tunable micellar structures.…”
Section: Computational Design Of Functional Nanostructuresmentioning
confidence: 99%
“…Unfortunately, calculations and band structure modelling have revealed a complete photonic band gap that forms only under very strict structural and dielectric conditions. [18][19][20] Regardless of the type of lattice structure, the high-dielectric component of the photonic crystal needs to have a refractive index exceeding 2 (assuming that air is the low-dielectric component), while being optically transparent in and around the band gap wavelength region; for example, for an optimized diamond lattice the minimum refractive index is 2.0 in order to open a complete band gap, whereas for a close-packed face-centred cubic lattice of air spheres (inverse opal) the surrounding high-dielectric needs to have a refractive index of at least 2.8. 19,20 Interestingly, complete band gaps are absent in biological photonic crystals, despite millions of years of optimization.…”
Section: Photonic Structures In Biology and Technologymentioning
confidence: 99%
“…For certain large area applications, simpler techniques could be more suitable. Spontaneous self-assembly of colloids [375], synthetic opals [379][380][381][382][383][384], inverted opals [379,[385][386][387] and block copolymers [218,219,221,378,[388][389][390][391][392][393][394][395][396][397][398][399][400][401][402], on the other hand, allows the preparation of small enough structures. Although self-assembly leads to a well-defined local order and offers a potentially low-cost method for the production of photonic crystals, it is nontrivial to achieve perfectly ordered structures over the macroscopic length scale combining carefully engineered defects.…”
Section: Optical Properties Of Self-assembled Polymer Systemsmentioning
confidence: 99%
“…In the purely layered geometry, it is not possible to achieve a complete photonic bandgap, which would stop the light propagation in all directions. Therefore, higher dimensional block copolymer structures have been pursued [374,377,393,398,400,402]. Even 2D materials consisting of self-assembled cylinders do not allow a complete bandgap [399] and in this respect 3D network-like structures are currently being studied in detail [402].…”
Section: Optical Properties Of Self-assembled Polymer Systemsmentioning
confidence: 99%