Abstract

We correct typographical errors in four equations showing the integral forms of the equations of motion and the corresponding perturbative approximation. Subsequently presented derivations, results, and conclusions remain unchanged.

© 2017 Optical Society of America

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References

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  1. D. V. Reddy, M. G. Raymer, C. J. McKinstrie, L. Mejling, and K. Rottwitt, “Temporal mode selectivity by frequency conversion in second-order nonlinear optical waveguides,” Opt. Express 21, 13840–13863 (2013).
    [Crossref] [PubMed]

2013 (1)

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Equations (4)

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A r ( L , t ) = A r ( 0 , t β r L ) + i 0 L d z κ ( z , t r ) A s ( z , t r ) ,
A s ( L , t ) = A s ( 0 , t β s L ) + i 0 L d z κ * ( z , t s ) A r ( z , t s ) .
A r ( L , t ) A r ( 0 , t r ) + i 0 L d z κ ( z , t r ) A s ( 0 , t r + β r s z ) ,
A s ( L , t ) A s ( 0 , t s ) + i 0 L d z κ * ( z , t s ) A r ( 0 , t s + β r s z ) .

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