Abstract

We report a correction to the numerical procedure, in which the source vector lacked a factor 1/2 and the integration in Eq. (19) was incorrect. The errors are inconsequential for the main results.

© 2013 OSA

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  1. J. Mäkitalo, S. Suuriniemi, and M. Kauranen, “Boundary element method for surface nonlinear optics of nanoparticles,” Opt. Express19, 23386–23399 (2011)
    [CrossRef] [PubMed]
  2. C. Forestiere, A. Capretti, and G. Miano, “Surface Integral Method for the Second Harmonic Generation in Metal Nanoparticles,” arXiv:1301.1880 [physics.optics] (2013)

2011

Capretti, A.

C. Forestiere, A. Capretti, and G. Miano, “Surface Integral Method for the Second Harmonic Generation in Metal Nanoparticles,” arXiv:1301.1880 [physics.optics] (2013)

Forestiere, C.

C. Forestiere, A. Capretti, and G. Miano, “Surface Integral Method for the Second Harmonic Generation in Metal Nanoparticles,” arXiv:1301.1880 [physics.optics] (2013)

Kauranen, M.

Mäkitalo, J.

Miano, G.

C. Forestiere, A. Capretti, and G. Miano, “Surface Integral Method for the Second Harmonic Generation in Metal Nanoparticles,” arXiv:1301.1880 [physics.optics] (2013)

Suuriniemi, S.

Opt. Express

Other

C. Forestiere, A. Capretti, and G. Miano, “Surface Integral Method for the Second Harmonic Generation in Metal Nanoparticles,” arXiv:1301.1880 [physics.optics] (2013)

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Equations (5)

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𝒦 l f ( r ) = V l [ G l ( r , r ) ] × f ( r ) d S = 1 2 f ( r ) × n l + 𝒦 l f ( r ) ,
𝒦 l f ( r ) = lim a 0 V l D ( r , a ) [ G l ( r , r ) ] × f ( r ) d S
( 𝒟 1 J 1 S + 𝒦 1 M 1 S 𝒟 2 J 2 S 𝒦 2 M 2 S ) tan = 1 2 ε S P n S , ( 𝒦 1 J 1 S + 1 η 1 2 𝒟 1 M 1 S + 𝒦 2 J 2 S 1 η 2 2 𝒟 2 M 2 S ) tan = i 1 2 Ω P S × n .
S P n S = l = 1 N p l f l .
b m n 2 = 1 ε l p l S m S l f m n × f l d S ,

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