Exceptional enhancement of localization effect in a one-dimensional multilayer system with destructive weak disorder strength: erratum

Junying Huang; Luwei Zhou

doi:10.1364/OL.39.002390

Abstract

In an earlier Letter [Opt. Lett. 36, 1305 (2011)], we report that the photon localization effect in a system with weak disorder strength, but in a destructive interference resonance region, is stronger than that in a completely disordered system. We reveal that the only reason for this peculiar phenomenon is that the certain weak disorder system confines the resonances between the wave and layers in the destructive interference resonance region. However, there are some errors in the published article, which are corrected here.

In [1], Eq. (1) is misprinted as

t_{e} = \frac{1 - γ^{2}}{1 - γ^{2}} \exp (I δ),

whereas the correct form is

t_{e} = \frac{1 - γ^{2}}{1 - γ^{2} \exp (I δ)} .

Equation (2) is misprinted as

r_{e} = \frac{γ [1 - \exp (I δ)]}{1 - γ^{2}} \exp (I δ),

whereas the correct form is

r_{e} = \frac{γ [1 - \exp (I δ)]}{1 - γ^{2} \exp (I δ)} .

In the fourth line of page 1306, the correct form for “ $[- π]$ , $π$ ” is “ $[- π, π]$ .”

Reference

1. J. Huang and L. Zhou, Opt. Lett. 36, 1305 (2011). [CrossRef]

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Equations (4)

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t_{e} = \frac{1 - γ^{2}}{1 - γ^{2}} \exp (I δ),

t_{e} = \frac{1 - γ^{2}}{1 - γ^{2} \exp (I δ)} .

r_{e} = \frac{γ [1 - \exp (I δ)]}{1 - γ^{2}} \exp (I δ),

r_{e} = \frac{γ [1 - \exp (I δ)]}{1 - γ^{2} \exp (I δ)} .

Abstract

Reference

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Equations (4)

Optics Letters