• Photonics Research
  • Vol. 7, Issue 2, 182 (2019)
Maciej Kowalczyk1、*, Tadeusz Martynkien2, Paweł Mergo3, Grzegorz Soboń1, and Jarosław Sotor1
Author Affiliations
  • 1Laser & Fiber Electronics Group, Faculty of Electronics, Wroclaw University of Science and Technology, Wybrzeze Wyspianskiego 27, 50-370 Wroclaw, Poland
  • 2Department of Optics and Photonics, Faculty of Fundamental Problems of Technology, Wroclaw University of Science and Technology, Wybrzeze Wyspianskiego 27, 50-370 Wroclaw, Poland
  • 3Laboratory of Optical Fiber Technology, Maria Curie-Sklodowska University, pl. M. Curie-Sklodowskiej 3, Lublin, Poland
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    DOI: 10.1364/PRJ.7.000182 Cite this Article Set citation alerts
    Maciej Kowalczyk, Tadeusz Martynkien, Paweł Mergo, Grzegorz Soboń, Jarosław Sotor. Ultrabroadband wavelength-swept source based on total mode-locking of an Yb:CaF2 laser[J]. Photonics Research, 2019, 7(2): 182 Copy Citation Text show less
    (a) Schematic of the experimental setup: SESAM, semiconductor saturable absorber mirror; OC, output coupler; λ/2, half-wave plate. (b) Output characteristics of the mode-locked Yb:CaF2 oscillator: autocorrelation trace with a corresponding fit and (inset) optical spectrum. (c) Dispersion of the PCF with indicated pump spectrum and (inset) scanning electron microscope cross-section image of the PCF.
    Fig. 1. (a) Schematic of the experimental setup: SESAM, semiconductor saturable absorber mirror; OC, output coupler; λ/2, half-wave plate. (b) Output characteristics of the mode-locked Yb:CaF2 oscillator: autocorrelation trace with a corresponding fit and (inset) optical spectrum. (c) Dispersion of the PCF with indicated pump spectrum and (inset) scanning electron microscope cross-section image of the PCF.
    Electric field profiles of the cross sections of TEM00 and TEM01 modes (dashed lines) with the resulting normalized intensity of the total electric field (solid lines) at (a), (c) Δφtot=0 and (b), (d) Δφtot=π. The ratio of the mode amplitudes α is equal to (a), (b) 0.2 in the upper row and (c), (d) 0.7 in the lower row. For animation, see Visualization 1 (α=0.7).
    Fig. 2. Electric field profiles of the cross sections of TEM00 and TEM01 modes (dashed lines) with the resulting normalized intensity of the total electric field (solid lines) at (a), (c) Δφtot=0 and (b), (d) Δφtot=π. The ratio of the mode amplitudes α is equal to (a), (b) 0.2 in the upper row and (c), (d) 0.7 in the lower row. For animation, see Visualization 1 (α=0.7).
    Averaged beam profiles at different regimes with corresponding pulse trains and spectra (in logarithmic scale) registered at the PCF output. The set (a) corresponds to the pump laser operating at a stable, pure Gaussian regime; in (b) we started the modulation by exciting the TEM01 mode. The modulation effect is more profound in (c), where the contribution of the higher transverse mode is stronger.
    Fig. 3. Averaged beam profiles at different regimes with corresponding pulse trains and spectra (in logarithmic scale) registered at the PCF output. The set (a) corresponds to the pump laser operating at a stable, pure Gaussian regime; in (b) we started the modulation by exciting the TEM01 mode. The modulation effect is more profound in (c), where the contribution of the higher transverse mode is stronger.
    Pulse trains after the PCF at the modulation frequency of (a) 7 MHz and (b) 21.5 MHz.
    Fig. 4. Pulse trains after the PCF at the modulation frequency of (a) 7 MHz and (b) 21.5 MHz.
    Maciej Kowalczyk, Tadeusz Martynkien, Paweł Mergo, Grzegorz Soboń, Jarosław Sotor. Ultrabroadband wavelength-swept source based on total mode-locking of an Yb:CaF2 laser[J]. Photonics Research, 2019, 7(2): 182
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