Research · Publication & note
Porous Silicon Microcavities Based Photonic Barcodes
Advanced Materials · Journal article · 2 May 2011
Article summary
Here, we show that the photoluminescence emission of a single porous silicon colloid is strongly coupled to the whispering-gallery modes of the microcavity defined by the colloid itself, resulting in a unique photoluminescence spectrum with a high quantum yield. This spectrum depends on the colloid size and porosity, and constitutes a fingerprint of the particle. The authors propose a photonic encoding procedure in which a unique barcode can be assigned to each colloid through its photoluminescence spectrum.
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Figures

From F. Ramiro-Manzano et al., Advanced Materials 23, 3022-3025 (2011), DOI 10.1002/adma.201100986. © 2011 Wiley-VCH Verlag GmbH & Co. KGaA. Reused by the authors under Wiley's contributor reuse terms.

From F. Ramiro-Manzano et al., Advanced Materials 23, 3022-3025 (2011), DOI 10.1002/adma.201100986. © 2011 Wiley-VCH Verlag GmbH & Co. KGaA. Reused by the authors under Wiley's contributor reuse terms.

From F. Ramiro-Manzano et al., Advanced Materials 23, 3022-3025 (2011), DOI 10.1002/adma.201100986. © 2011 Wiley-VCH Verlag GmbH & Co. KGaA. Reused by the authors under Wiley's contributor reuse terms.
Research fields
Bottom-up
Porous silicon microspheres are produced as luminescent, high-index colloids with a radial pore distribution and smooth outer boundary. Each particle therefore forms its own microcavity rather than requiring a patterned mirror stack.
Simulations & fits
Mie-mode assignments link transmission minima to the resonances that enhance the broad porous-silicon photoluminescence. The resulting sequence of narrow emission peaks constitutes a particle-specific optical barcode governed by diameter and effective refractive index.
Characterization
Single-particle transmission and photoluminescence are correlated with optical microscopy and compositional analysis. Measuring the same sphere in both channels shows directly that its luminescence maxima coincide with cavity modes rather than with unrelated spectral structure.
