Inverse Photonic Glasses by Packing Bidisperse Hollow Microspheres with Uniform Cores
Author(s) -
Seunghyun Kim,
Sofia Magkiriadou,
Do Kyung Rhee,
Doo Sung Lee,
Pil J. Yoo,
Vinothan Manoharan,
GiRa Yi
Publication year - 2017
Publication title -
acs applied materials and interfaces
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.535
H-Index - 228
eISSN - 1944-8252
pISSN - 1944-8244
DOI - 10.1021/acsami.7b02098
Subject(s) - materials science , dispersity , structural coloration , photonics , structure factor , shell (structure) , photonic crystal , porosity , inverse , matrix (chemical analysis) , polymer , fabrication , light scattering , filling factor , refractive index , scattering , volume fraction , atomic packing factor , optics , composite material , optoelectronics , polymer chemistry , crystallography , geometry , medicine , chemistry , mathematics , alternative medicine , physics , pathology
A major fabrication challenge is producing disordered photonic materials with an angle-independent structural red color. Theoretical work has shown that such a color can be produced by fabricating inverse photonic glasses with monodisperse, nontouching voids in a silica matrix. Here, we demonstrate a route toward such materials and show that they have an angle-independent red color. We first synthesize monodisperse hollow silica particles with precisely controlled shell thickness and then make glassy colloidal structures by mixing two types of hollow particles with the same core size and different shell thicknesses. We then infiltrate the interstices with index-matched polymers, producing disordered porous materials with uniform, nontouching air voids. This procedure allows us to control the light-scattering form factor and structure factor of these porous materials independently, which is not possible to do in photonic glasses consisting of packed solid particles. The structure factor can be controlled by the shell thickness, which sets the distance between pores, whereas the pore size determines the peak wave vector of the form factor, which can be set below the visible range to keep the main structural color pure. By using a binary mixture of 246 and 268 nm hollow silica particles with 180 nm cores in an index-matched polymer matrix, we achieve angle-independent red color that can be tuned by controlling the shell thickness. Importantly, the width of the reflection peak can be kept constant, even for larger interparticle distances.
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