Abstract
Hetero-opals were synthesized by successive crystallization of one opal film on top of the other film using monodisperse PS beads of a different diameter. As such, the transmission spectrum of a hetero-opal shows two main minima following the difference of the Bragg resonance frequencies of its constituents. Strong spatial and frequency anisotropy of the reflectance spectrum of hetero-opals was a straightforward consequence of this mismatch of the Bragg resonances.
| Original language | English |
|---|---|
| Pages (from-to) | 1029-1035 |
| Journal | Journal of Applied Physics |
| Volume | 95 |
| Issue number | 3 |
| DOIs | |
| Publication status | Published - 1 Feb 2004 |
| Externally published | Yes |
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