Abstract
We correct an error in figure 6 of our manuscript [Opt. Mater. Exp. 2, 478–489 (2012)] showing the propagation length and confinement width of surface-plasmon-polariton on metal/air interface.
© 2013 Optical Society of America
We correct an error in the calculation of propagation length and mode size of surface plasmon-polariton (SPP) on metal/air interface provided in Fig. 6 of [1]. SPP propagation length (L w) and confinement width (D w) across an interface of a plasmonic material with air may be computed using the Eqs. 1 and 2.
where and , k 0 = ω/c, and ε m is the permittivity of the plasmonic material. δ D and δ m are the 1/e field decay in the dielectric and metal respectively. In Fig. 6 of [1], the propagation length and confinement width or mode size are computed incorrectly. This mistake has been corrected in Figure 1. We regret the error, although it does not alter the results, discussion, or conclusions of the paper.References and links
1. G. Naik, J. Schroeder, X. Ni, A. Kildishev, T. Sands, and A. Boltasseva, “Titanium nitride as a plasmonic material for visible and near-infrared wavelengths optics,” Optical Materials Express 2, 478–489 (2012). [CrossRef]