Abstract

The numerical results, Figs. 16 and 18, for the double negative (DNG) metatmaterial Goos-Hänchen examples were incorrect. Corrected numerical results show closer agreement to predictions.

© 2003 Optical Society of America

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References

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  1. R. W. Ziolkowski, “Pulsed and CW Gaussian beam interactions with double negative metamaterial slabs,” Opt. Express 11, 662-681 (2003), <a href="http://www.opticsexpress.org/abstract.cfm?URI=OPEX-11-7-662.">http://www.opticsexpress.org/abstract.cfm?URI=OPEX-11-7-662</a>.
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Figures (2)

Fig. 1.
Fig. 1.

(1.17 MB movie) Electric field intensity distribution for the interaction of a CW Gaussian beam that is incident at 40° in a DPS medium with ε r =9.0 and µ r =+1, i.e., n=+3; to a DNG slab having ε r =-3.0 and µ r =-1, i.e., n=-√3. The negative Goos-Hachen shift of this beam is observed.

Fig. 2.
Fig. 2.

The electric field intensity distribution measured at t=6000Δt at two cells in front of the TF-SF plane for the total internal reflection DNG slab case. The positions of the incident beam center and the specularly-reflected beam center are indicated by the vertical black lines. The theoretical negative Goös-Hachen shift is indicated by the vertical green line.

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