• Photonics Research
  • Vol. 9, Issue 3, 357 (2021)
Yongguang Zhao1、2、*, Li Wang2, Weidong Chen2, Pavel Loiko3, Xavier Mateos4, Xiaodong Xu1, Ying Liu1, Deyuan Shen1, Zhengping Wang5, Xinguang Xu5, Uwe Griebner1, and Valentin Petrov1
Author Affiliations
  • 1Jiangsu Key Laboratory of Advanced Laser Materials and Devices, School of Physics and Electronic Engineering, Jiangsu Normal University, Xuzhou 221116, China
  • 2Max Born Institute for Nonlinear Optics and Short Pulse Spectroscopy, 12489 Berlin, Germany
  • 3Centre de Recherche sur les Ions, les Matériaux et la Photonique (CIMAP), UMR 6252 CEA-CNRS-ENSICAEN, Université de Caen, Caen 14050, France
  • 4Universitat Rovira i Virgili (URV), Física i Cristal·lografia de Materials i Nanomaterials (FiCMA-FiCNA), Marcel.li Domingo 1, 43007 Tarragona, Spain
  • 5State Key Laboratory of Crystal Materials and Institute of Crystal Materials, Shandong University, Jinan 250100, China
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    DOI: 10.1364/PRJ.413276 Cite this Article Set citation alerts
    Yongguang Zhao, Li Wang, Weidong Chen, Pavel Loiko, Xavier Mateos, Xiaodong Xu, Ying Liu, Deyuan Shen, Zhengping Wang, Xinguang Xu, Uwe Griebner, Valentin Petrov. Structured laser beams: toward 2-μm femtosecond laser vortices[J]. Photonics Research, 2021, 9(3): 357 Copy Citation Text show less
    Schematic of the passively mode-locked femtosecond TEM00 and HG10 laser using collinear and off-axis pumping (BM, bending mirror; L, lens; CM1–CM3, chirped mirrors; OC, output coupler).
    Fig. 1. Schematic of the passively mode-locked femtosecond TEM00 and HG10 laser using collinear and off-axis pumping (BM, bending mirror; L, lens; CM1–CM3, chirped mirrors; OC, output coupler).
    (a) Optical spectra and (b), (c) interferometric autocorrelation traces of the mode-locked Tm:LuYO3 ceramic laser operating in TEM00 and HG10 modes. Insets of (b) and (c) show the corresponding far-field beam patterns (fs, femtosecond).
    Fig. 2. (a) Optical spectra and (b), (c) interferometric autocorrelation traces of the mode-locked Tm:LuYO3 ceramic laser operating in TEM00 and HG10 modes. Insets of (b) and (c) show the corresponding far-field beam patterns (fs, femtosecond).
    (a) Schematic of the SCL mode converter, and the recorded far-field (b), (e) HG10 and (c), (d), (f), (g) LG0,±1 beam patterns as the mode-locked laser operated in the first (middle row) and second (bottom row) femtosecond regimes (l, topological charge).
    Fig. 3. (a) Schematic of the SCL mode converter, and the recorded far-field (b), (e) HG10 and (c), (d), (f), (g) LG0,±1 beam patterns as the mode-locked laser operated in the first (middle row) and second (bottom row) femtosecond regimes (l, topological charge).
    (a) Optical spectrum of the generated LG0,+1 modes and the corresponding interferometric autocorrelation traces in the (b) first and (c) second femtosecond regimes; (d) and (e) are the RF spectra of the femtosecond (112 fs) LG0,+1 beam in different span ranges. The inset in (c) shows the noncollinear autocorrelation trace recorded on a long time scale (RBW, resolution bandwidth).
    Fig. 4. (a) Optical spectrum of the generated LG0,+1 modes and the corresponding interferometric autocorrelation traces in the (b) first and (c) second femtosecond regimes; (d) and (e) are the RF spectra of the femtosecond (112 fs) LG0,+1 beam in different span ranges. The inset in (c) shows the noncollinear autocorrelation trace recorded on a long time scale (RBW, resolution bandwidth).
    Yongguang Zhao, Li Wang, Weidong Chen, Pavel Loiko, Xavier Mateos, Xiaodong Xu, Ying Liu, Deyuan Shen, Zhengping Wang, Xinguang Xu, Uwe Griebner, Valentin Petrov. Structured laser beams: toward 2-μm femtosecond laser vortices[J]. Photonics Research, 2021, 9(3): 357
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