1977
DOI: 10.1109/jqe.1977.1069328
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Coupled wave analysis of DFB and DBR lasers

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Cited by 214 publications
(57 citation statements)
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“…For a given device with a corrugation only on one side of the active material, like our DFB laser fabricated through nanograting transfer, the decrease in threshold fluence with increased pump spot size can be explained via coupled-wave theory [23][24][25][26]. For a tooth-shaped onedimensional grating one obtains the coupled-wave equations…”
Section: Discussionmentioning
confidence: 99%
“…For a given device with a corrugation only on one side of the active material, like our DFB laser fabricated through nanograting transfer, the decrease in threshold fluence with increased pump spot size can be explained via coupled-wave theory [23][24][25][26]. For a tooth-shaped onedimensional grating one obtains the coupled-wave equations…”
Section: Discussionmentioning
confidence: 99%
“…For given Bragg order and reference (Bragg) wavelength nm, the total length of the period of the grating is given by (1) For given duty cycle , the effective index of the reference waveguide is obtained by averaging the dielectric function along (2) It varies between the effective indexes of the constituent slab waveguides for and for . Hence, the grating period is correspondingly changed between nm and nm.…”
Section: Benchmark Examplementioning
confidence: 99%
“…The complex valued total coupling coefficient is composed of terms due to the direct and indirect interactions of the two oppositely going waves with the grating [2], [5]. The indirect interaction gives also rise to a modification of both the real and imaginary parts of the relative propagation coefficient via the self-radiation coupling coefficient given in the Appendix (5) Due to the fact that there is no gain and loss in the waveguide sections, the corresponding modal gain-loss function is omitted in (5).…”
Section: A Coupled-mode Theorymentioning
confidence: 99%
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