Fundamentals of optical waveguides

By K. Okamoto. 2000

1,083 citations recorded by the source corpus.

View Paper: https://www.semanticscholar.org/paper/27c50fa300c55ca2ecd924753ea07c225cd28cde

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Citations in the corpus

Fiber to the Home Using a PON Infrastructure (2006, methodology): “ture ranges experienced at the passive-node location [29].”
Theory of coupled optical PT-symmetric structures. (2007, methodology): “In retrospect, we could have arrived at this same formalism by projecting the evolution equations on the PT-symmetric base functions u2,1 * − as opposed to u1,2 * used in conventional CMT [6,7].”
Optical generation and distribution of continuously tunable millimeter-wave signals using an optical phase modulator (2005, unknown): “1) Dispersion Effect: When fiber chromatic dispersion is taken into consideration, the propagation constant β(ω) of the fiber for an optical sideband at ωo ± nωe can be approximately represented by a Taylor series around the center angular frequency ωo [10]”
Space-division multiplexing: the next frontier in optical communication (2014, methodology): “For example, the coupling coefficient for the degenerate LP11 mode is given by [11]”
Generation and distribution of a wide-band continuously tunable millimeter-wave signal with an optical external modulation technique (2005, background): “By expand the propagation constant of the fiber for each optical sideband to a Taylor series around the angular frequency of the optical carrier [ 19 ], i.e.,”
Ultrafast laser written active devices (2009, background): “This is a consequence of the round-trip phase criterion associated with a DFB laser in which the phase shift of one round-trip must be an integer multiple of 2π [84–86].”
Pulse Propagation in a Short Nonlinear Graded-Index Multimode Optical Fiber (2012, methodology): “where is the group index at the center of the core, is the speed of light in vacuum, and is defined as [13], [16]”
Wavelength tunable fiber lens based on multimode interference (2004, methodology): “Applying the separation of variables and solving Maxwell equations inside the MMF for linearly polarized modes, can be written as follows [7]:”