Abstract

The power transmitted by surface waveguide modes propagating along a semi-infinite dielectric fiber is determined. For a plane wave normally incident on the end of a perfectly circular fiber only the HE<sub>1m</sub> modes are excited. Of these modes the majority of the power is contained in the HE<sub>11</sub> mode. Far above the cutoff conditions for the HE<sub>13</sub> mode, approximately 99.8% of the incident power is contained in the HE<sub>11</sub>, HE<sub>12</sub>, and HE<sub>13</sub> modes.

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  1. E. Snitzer, J. Opt. Soc. Am. 51, 491 (1961).
  2. N. S. Kapany and J. J. Burke, J. Opt. Soc. Am. 51, 1067 (1961).
  3. E. Snitzer, J. Opt. Soc. Am. 49, 1128 (1959).
  4. J. Enoch, J. Opt. Soc. Am. 53, 71 (1963).
  5. G. Biernson and D. Kinsley, IEEE Trans. Microwave Theory Tech. MTT-13, 345 (1965).
  6. G. Goubau, Proc. IRE 40, 865 (1952).
  7. G. N. Watson, Theory of Bessel Functions (Cambridge University Press, London, 1949).

Biernson, G.

G. Biernson and D. Kinsley, IEEE Trans. Microwave Theory Tech. MTT-13, 345 (1965).

Burke, J. J.

N. S. Kapany and J. J. Burke, J. Opt. Soc. Am. 51, 1067 (1961).

Enoch, J.

J. Enoch, J. Opt. Soc. Am. 53, 71 (1963).

Goubau, G.

G. Goubau, Proc. IRE 40, 865 (1952).

Kapany, N. S.

N. S. Kapany and J. J. Burke, J. Opt. Soc. Am. 51, 1067 (1961).

Kinsley, D.

G. Biernson and D. Kinsley, IEEE Trans. Microwave Theory Tech. MTT-13, 345 (1965).

Snitzer, E.

E. Snitzer, J. Opt. Soc. Am. 51, 491 (1961).

E. Snitzer, J. Opt. Soc. Am. 49, 1128 (1959).

Watson, G. N.

G. N. Watson, Theory of Bessel Functions (Cambridge University Press, London, 1949).

Other (7)

E. Snitzer, J. Opt. Soc. Am. 51, 491 (1961).

N. S. Kapany and J. J. Burke, J. Opt. Soc. Am. 51, 1067 (1961).

E. Snitzer, J. Opt. Soc. Am. 49, 1128 (1959).

J. Enoch, J. Opt. Soc. Am. 53, 71 (1963).

G. Biernson and D. Kinsley, IEEE Trans. Microwave Theory Tech. MTT-13, 345 (1965).

G. Goubau, Proc. IRE 40, 865 (1952).

G. N. Watson, Theory of Bessel Functions (Cambridge University Press, London, 1949).

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