2020
DOI: 10.1007/s00340-020-07489-2
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Compact mode-locked Er-doped fiber laser for broadband cavity-enhanced spectroscopy

Abstract: We report the design and characteristics of a simple and compact mode-locked Er-doped fiber laser and its application to broadband cavity-enhanced spectroscopy. The graphene mode-locked polarization maintaining oscillator consumes less than 5 W of power. It is thermally stabilized, enclosed in a 3D printed box, and equipped with three actuators that control the repetition rate: fast and slow fiber stretchers, and metal-coated fiber section. This allows wide tuning of the repetition rate and its stabilization t… Show more

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Cited by 16 publications
(13 citation statements)
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References 32 publications
(39 reference statements)
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“…3(a), is caused by the etalon fringes remaining after the baseline correction procedure and by uncertainties in the frequency scale calibration. Nevertheless, the relative amplitude of the residuum is lower than what was observed in previous CF-VS demonstrations employing the rotating diffraction grating and active stabilization using either an Er-doper fiber laser [31] or a mid-infrared optical parametric oscillator [28]. The improvement is brought partly by the lack of high-speed active stabilization whose gain depended on the amplitude of the signal (and thus distorted the absorption lines), and partly by the silicon etalon used for frequency calibration, which has a better fringe contrast than the CaF 2 etalon used in the previous works.…”
Section: Co 2 Detection At Non-adiabatic Scanning Speedscontrasting
confidence: 59%
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“…3(a), is caused by the etalon fringes remaining after the baseline correction procedure and by uncertainties in the frequency scale calibration. Nevertheless, the relative amplitude of the residuum is lower than what was observed in previous CF-VS demonstrations employing the rotating diffraction grating and active stabilization using either an Er-doper fiber laser [31] or a mid-infrared optical parametric oscillator [28]. The improvement is brought partly by the lack of high-speed active stabilization whose gain depended on the amplitude of the signal (and thus distorted the absorption lines), and partly by the silicon etalon used for frequency calibration, which has a better fringe contrast than the CaF 2 etalon used in the previous works.…”
Section: Co 2 Detection At Non-adiabatic Scanning Speedscontrasting
confidence: 59%
“…We record spectra of CO 2 covering 1.7 THz of bandwidth at 1575 nm, and of CH 4 , covering 2.7 THz at 1650 nm. The noise equivalent absorption at 1575 nm is 5 × 10 −9 cm −1 Hz −1/2 , which is better than in previous demonstrations of the technique in the same spectral region, using a spectrometer with the galvo scanner and the same Er-doped fiber laser [31] or a commercial comb source [29], or using a Czerny-Turner spectrometer with scanned mirror and a CCD camera [36]. Moreover, the demonstrated absorption sensitivity is comparable to that of other robust cavity-enhanced techniques, e.g.…”
Section: Discussionmentioning
confidence: 64%
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“…Controlling the external environment of the laser is the former, specifically placing the laser in a thermotank or a well-controlled room. However, it must be carefully controlled to ensured that the exterior remains unchanged [10][11][12][13]. Additionally, a phase-locking system can stabilize the pulse source parameters, and excellent performance can be obtained [14][15][16].…”
Section: Introductionmentioning
confidence: 99%