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Volumn 78, Issue 8, 2008, Pages

Reflection and diffraction at the end of a cylindrical dielectric nanowire: Exact analytical solution

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EID: 50449085559     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.78.085318     Document Type: Article
Times cited : (14)

References (42)
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    • Here and in the following we omit the factor exp (-iωt) for brevity. Note that even and odd waves for which the θ -dependence is given by cos (nθ) and sin (nθ), respectively, can be considered as a superposition of two waves with amplitudes proportional to e-inθ and einθ.
    • Here and in the following we omit the factor exp (-iωt) for brevity. Note that even and odd waves for which the θ -dependence is given by cos (nθ) and sin (nθ), respectively, can be considered as a superposition of two waves with amplitudes proportional to e-inθ and einθ.
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    • One can show that the Fourier-transformed amplitudes given by Eq. 28 tend to zero when |β| →∞. Then, according to the Jordan's lemma, the integral about the semicircle is equal to zero if z<0.
    • One can show that the Fourier-transformed amplitudes given by Eq. 28 tend to zero when |β| →∞. Then, according to the Jordan's lemma, the integral about the semicircle is equal to zero if z<0.
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    • The quantity qj2 = kj2 - β2 changes its sign twice when one moves from one edge of the cut to another around the branch point. This means that its argument acquires a shift of 2π. Correspondingly, the quantity qj acquires a factor exp (iπ) =-1.
    • The quantity qj2 = kj2 - β2 changes its sign twice when one moves from one edge of the cut to another around the branch point. This means that its argument acquires a shift of 2π. Correspondingly, the quantity qj acquires a factor exp (iπ) =-1.
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    • The validity of such a deformation of the integration path C can be proved in much the same way as it was done for the path C- in Sec. 3.
    • The validity of such a deformation of the integration path C can be proved in much the same way as it was done for the path C- in Sec. 3.


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