Abstract
Metallic photonic crystals with strong light harvesting capabilities for SERS and photodetectors.
Highlights
Metallic photonic crystals (MPCs), as arti cial ordered nanostructures, have already attracted extensive attention due to their great potential in metamaterials,[1] extraordinary optical transmission (EOT),[2] optical sensors,[3] solar energy conversion[4] and molecular detection.[5]
We propose a general strategy for the controllable fabrication of MPCs with inverse opal structure consisting of plasmonic metals (Ag and Cu) and transition metals (Ni and Co), respectively, which exhibit characteristic optical properties compared with dielectric photonic crystals
We have fabricated a series of MPCs with highly uniform inverse opal structure consisting of plasmonic metals (Ag and Cu) and transition metals (Ni and Co), respectively, by a self-assembly and electrochemical deposition method
Summary
Metallic photonic crystals (MPCs), as arti cial ordered nanostructures, have already attracted extensive attention due to their great potential in metamaterials,[1] extraordinary optical transmission (EOT),[2] optical sensors,[3] solar energy conversion[4] and molecular detection.[5]. The effect of the MPC structure on performance is a signi cant issue to explore To solve these problems, we propose a general strategy for the controllable fabrication of MPCs with inverse opal structure consisting of plasmonic metals (Ag and Cu) and transition metals (Ni and Co), respectively, which exhibit characteristic optical properties compared with dielectric photonic crystals. The photonic band gap is quite broad because of the enhanced optical penetration depth in the MPCs, compared with the skin depth of the pure metals These optical properties could be controlled by changing the diameter of the MPCs, illustrating that it is bene cial for applications in SERS and photodetectors. A remarkable rise in photocurrent was observed, when the light was switched on, in Ag and Cu MPCs which exhibited a signi cant rise in a linear model on optical power density, completely reversed compared with semiconductors
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