2021
DOI: 10.1016/j.optmat.2020.110728
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Titania-carbon nanocomposite as a saturable absorber for generation passively ytterbium-mode locked pulses

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Cited by 17 publications
(2 citation statements)
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“…where Δ∅ 0 is the phase shift, K is the wavenumber (2π/λ), I 0 refers to the laser beam intensity at the focusing point, and L ef is the efective length of the propagation light inside the specimen, L eff � 1 − e (− Lα) /α [45].…”
Section: Characterisation Ofmentioning
confidence: 99%
“…where Δ∅ 0 is the phase shift, K is the wavenumber (2π/λ), I 0 refers to the laser beam intensity at the focusing point, and L ef is the efective length of the propagation light inside the specimen, L eff � 1 − e (− Lα) /α [45].…”
Section: Characterisation Ofmentioning
confidence: 99%
“…Saturable absorbers (SAs), one of the passive techniques, are nonlinear optical elements and the most common device to generate mode-locked pulses. There are several kinds of SAs that have been widely studied, such as semiconductor saturable absorber mirrors (SESAMs) [33][34][35] and carbon nanotubes (CNTs) [36][37][38]. SESAMs are widely used in most commercial fiber laser systems.…”
Section: Introductionmentioning
confidence: 99%