Chinese Optics Letters, Volume. 19, Issue 8, 081301(2021)

Near-infrared lasing and tunable upconversion from femtosecond laser inscribed Nd,Gd:CaF2 waveguides Editors' Pick

Ruonan Li1, Lifei Sun1, Yangjian Cai1、*, Yingying Ren1、**, Hongliang Liu2, Mark D. Mackenzie3, and Ajoy K. Kar3
Author Affiliations
  • 1Center of Light Manipulations and Applications & Shandong Provincial Key Laboratory of Optics and Photonic Device, School of Physics and Electronics, Shandong Normal University, Jinan 250014, China
  • 2Institute of Modern Optics, Nankai University, Tianjin 300350, China
  • 3Institute of Photonics and Quantum Sciences, Heriot-Watt University, Edinburgh EH14 4AS, UK
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    Figures & Tables(6)
    (a) Microscopic image of the end-facet of the Nd,Gd:CaF2 sample with 16 cladding WGs deeply embedded beneath the surface. (b)–(e) The cross sections of WG1–WG4.
    (a) Mode intensity distributions from the fabricated cladding WGs at 633 nm under TM polarization. (b) Propagation losses of WGs obtained under both TM and TE polarizations.
    (a) The room temperature µ-PL emission spectra of Nd3+ ions obtained from the WG area (blue), the filament (green), and the bulk of Nd,Gd:CaF2 crystals (red). The inset of (a) shows the cross section of WG1. The spatial two-dimensional (2D) distributions of (b) intensity, (c) peak shift, and (d) FWHM of 867 nm emission line obtained from the WG cross section. 1D distributions of (e) the emitted intensity, (f) energy shift, and (g) FWHM corresponding to the regions indicated by dashed lines in the inset of (a).
    cw WG laser output power as a function of the input pump power with (a) 9% and (b) 70% output coupler. (c) Spectrum of WG laser at 1059.91 nm. The inset shows the spatial intensity distribution of the output laser with a single-mode profile.
    Photographs of visible UC luminescence generated from (a) WG1 and (b) the bulk. UC spectra obtained from WG1 under (c) TE and (d) TM polarizations with varying excitation powers.
    (a) UC spectra from WG1 obtained with a rotating half-wave plate. Luminescence intensities of emission lines centered at (b) 485 nm and (c) 585 nm as a function of the angles of the polarizer. The intensity ratios of (d) I485/I585 and (e) I585/I485 as a function of the angles of the polarizer.
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    Ruonan Li, Lifei Sun, Yangjian Cai, Yingying Ren, Hongliang Liu, Mark D. Mackenzie, Ajoy K. Kar, "Near-infrared lasing and tunable upconversion from femtosecond laser inscribed Nd,Gd:CaF2 waveguides," Chin. Opt. Lett. 19, 081301 (2021)

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    Paper Information

    Category: Integrated Optics

    Received: Oct. 5, 2020

    Accepted: Dec. 30, 2020

    Published Online: Apr. 27, 2021

    The Author Email: Yangjian Cai (yangjiancai@sdnu.edu.cn), Yingying Ren (ryywly@sdnu.edu.cn)

    DOI:10.3788/COL202119.081301

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