Perturbation Methods in a Problem of Waveguide Theory
Perturbation Methods in a Problem of Waveguide Theory
David Fox
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2. . , —, sm (mjc + arte ) hr . 2 sm qite 29 This expression is clearly bounded, independent of m. Call this bound B. We have < B 3iii _2q_ s > ; r = m _2q_ + 1 2 < ^^^\2 r / m. 2q m = k-, — 3 m Thus, we have shown that the original sum is less than (k_, + k^ + k^ +k, ) — J. 2 5 4 m as m becomes laree. In order to complete the proof of convergence of u • e (eq^uation (35))^ we must demonstrate the absolute convergence of (36) 1 — e m m m=l Each component of the vector e is a coefficient of the Fourier expansion of the field in the aperture. qjt (37) m. 1_ qir m E cos — y dy y q -qrt Inasmuch as E vanishes for qir < |y| < :n:, equation (37) can be written as (58) e = — / E cos — y dy m qn J y q. ^ -^ 30 2rtq. I Jti ■rti dw dz m m — z - — z e'l + e ^ dz We can convert this to a Line integral in the w-plane using the Schwartz-Christoffel mapping given in equation (29). (59) ^^ = 2^i 1 yq e^+1 + q\/e^+l q. dw \/ 2 w _ i/v 7 Vqe+1+ Ve +1 an m (1-a)^ q C 1-q -w l^V q e +1 + /e +1 dw The path of integration^ C, is illustrated in the following sketch: w- plane I I I TTi+log —5 TTi I q +7ri — r— I L TTI I .
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