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Achromatic polarization and focusing op-tics were employed, and the far-field collimation improvedusing photonic-crystal fiber as described previously [13].The reflectance was obtained by simultaneously recordingthe input beam spectrum

Achromatic polarization and focusing op-tics were employed, and the far-field collimation improvedusing photonic-crystal fiber as described previously [13].The reflectance was obtained by simultaneously recordingthe input beam spectrum

It is completelysuppressed for opposite circular polarizations, and at theselow powers exhibits negligible nonlinearities for the op-posite spin polaritons, confirming the absence of excitonbleaching.

the X0 recombination time, given that the two holes have op-.

Fur-thermore such miniaturization enables integrated devices op-erating under plausible conditions for applications.

However almost any other op-tical property involves extra interactions of polaritons, such as the relaxationof polaritons to produce photoluminescence or nonlinear optical absorptionand emission.

However almost any other op-tical property involves extra interactions of polaritons, such as the relaxationof polaritons to produce photoluminescence or nonlinear optical absorptionand emission.

predicting atomic-scale confinement of op-tical fields (6, 20). This optical confinementexplains atomic resolution in tip-based exper-iments (3, 5) and approaches the quantum limitderived previously (4), V Rd2QR,

In summary, theNPoMs made of thicker PANI shells (>15 nm) provide excellent colorperformance with high fidelity, in reasonable agreement with the op-timal predictions of the numerical simulation.

A R T I C L E Op e n A c c e s s.