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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.
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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.
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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.
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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.
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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.
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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.
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41
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50449104100
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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.
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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.
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