2019
DOI: 10.1364/oe.27.005478
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Tunable dual-color operation of Yb:fiber laser via mechanical spectral subdivision

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Cited by 34 publications
(10 citation statements)
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“…Non-zero intra-cavity dispersion leads to a difference in repetition rate for the two emitted pulse trains. Based on state-of-the-art fiber lasers, the dual-color/dual-comb approach [19][20][21][22][23][24][25][26][27][28] shows great potential for spectroscopic measurements without the need for active stabilization of the comb parameters [22,23,27]. For instance, Zhao et al described a carbon nanotube modelocked dual-color erbium doped fiber laser [20], which then further evolved into a single-cavity dual-comb and enabled free-running spectroscopy [22].…”
Section: Introductionmentioning
confidence: 99%
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“…Non-zero intra-cavity dispersion leads to a difference in repetition rate for the two emitted pulse trains. Based on state-of-the-art fiber lasers, the dual-color/dual-comb approach [19][20][21][22][23][24][25][26][27][28] shows great potential for spectroscopic measurements without the need for active stabilization of the comb parameters [22,23,27]. For instance, Zhao et al described a carbon nanotube modelocked dual-color erbium doped fiber laser [20], which then further evolved into a single-cavity dual-comb and enabled free-running spectroscopy [22].…”
Section: Introductionmentioning
confidence: 99%
“…In recent work, we have demonstrated the implementation of a mechanical spectral filter to generate a tunable dual-color laser [26]. The method was implemented in a nonlinear polarization evolution (NPE) mode-locked Yb:fiber laser operating at 23 MHz.…”
Section: Introductionmentioning
confidence: 99%
“…[ 12,13 ] Subsequently, similar fiber sources have been demonstrated in various spectral ranges with dual‐comb generation based on polarization‐multiplexing [ 14–16 ] or multiwavelength emission. [ 17–20 ] Despite these advances, the main drawback of soliton mode‐locked lasers based on all‐fiber technology is the limitation of their output power due to excessive nonlinearities, which typically reduces the achievable peak power below the kilowatt level. This in turn prevents their efficient nonlinear frequency conversion to other spectral ranges (e.g., mid‐IR), where many important chemical species have their strongest absorption features.…”
Section: Introductionmentioning
confidence: 99%
“…Historically, the first single-cavity dual-comb mode-locked laser was a 1.55 µm fiber oscillator operating in a bidirectional configuration [7,8]. Subsequently, similar fiber sources have been demonstrated in various spectral ranges with dual-comb generation based on polarizationmultiplexing [9][10][11] or multiwavelength emission [12][13][14][15]. Despite these advances, the main drawback of soliton mode-locked lasers based on all-fiber technology is the limitation of their output power due to excessive nonlinearities, which typically reduces the achievable peak power below the kilowatt level.…”
Section: Introductionmentioning
confidence: 99%
“…The laser source used for this experiment is similar to the system presented in [4], however, the repetition rate of the laser is increased to around 92 MHz. A tuneable mechanical spectral filter [3] allows the all-PM laser to emit two independent pulse trains with different center wavelengths and slightly different repetition rates. As shown in [4], the two pulse trains may run in a different net intracavity dispersion regime each.…”
mentioning
confidence: 99%