• 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
  • show less
    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

    Abstract

    We present an ultrabroadband, high-speed wavelength-swept source based on a self-modulated femtosecond oscillator. Photonic crystal fiber was pumped by a mode-locked Yb:CaF2 laser, resulting in a strong spectral broadening from 485 to 1800 nm. The pump laser cavity could be realigned in order to achieve total mode-locking of the longitudinal and transverse TEM00 and TEM01 electromagnetic modes. This led to spatial oscillations of the output beam, which induced modulation of the coupling efficiency to the fiber. Due to the fact that nonlinear spectral broadening was intensity dependent, this mechanism introduced wavelength sweeping at the fiber output. The sweeping rate could be adjusted between 7 and 21.5 MHz by changing the geometry of the pump cavity. By controlling the ratio of the transverse mode amplitudes, we were able to tune the sweeping bandwidth, eventually covering both the 1300 nm and 1700 nm bioimaging transparency windows. When compared with previously demonstrated wavelength-swept sources, our concept offers much broader tunability and higher speed. Moreover, it does not require an additional intensity modulator.
    E(t)=Epulse(t){H00(x,y)+αH01(x,y)exp[i(Δωt+Δφ)]}.(1)

    View in Article

    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
    Download Citation