• Chinese Optics Letters
  • Vol. 17, Issue 9, 091402 (2019)
Wei Huang1, Yulong Cui1, Zhiyue Zhou1, Zhixian Li1, Yubin Chen4, and Zefeng Wang1、2、3、*
Author Affiliations
  • 1College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha 410073, China
  • 2State Key Laboratory of Pulsed Power Laser Technology, Changsha 410073, China
  • 3Hunan Provincial Key Laboratory of High Energy Laser Technology, Changsha 410073, China
  • 4Luoyang Electronic Equipment Test Center of China, Key Laboratory of Electro-Optical Countermeasures Test & Evaluation Technology, Luoyang 471003, China
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    DOI: 10.3788/COL201917.091402 Cite this Article Set citation alerts
    Wei Huang, Yulong Cui, Zhiyue Zhou, Zhixian Li, Yubin Chen, Zefeng Wang. Towards all-fiber structure pulsed mid-infrared laser by gas-filled hollow-core fibers[J]. Chinese Optics Letters, 2019, 17(9): 091402 Copy Citation Text show less
    (a) Taper formation by heating and stretching an SMF. The light gray section represents the fiber cladding, and the dark gray section represents the fiber core, in which both are not to scale. (b) Schematic diagram of the tapered SMF inserted into the HCF.
    Fig. 1. (a) Taper formation by heating and stretching an SMF. The light gray section represents the fiber cladding, and the dark gray section represents the fiber core, in which both are not to scale. (b) Schematic diagram of the tapered SMF inserted into the HCF.
    Schematic of the experimental setup based on coupling between the tapered solid-core fiber and HCF. AOM, acousto-optical modulator; EDFA, erbium-doped fiber amplifier; PM, power meter; XYZ, manual 3D translation stage; W, uncoated sapphire window; L, plano-convex lens; M, mirror on flipper mount; IBF, infrared bandpass filter. Inserts: the measured transmission loss spectrum (red curve and black curve represent fiber loss from 3000 to 3300 nm and from 1500 to 1600 nm, respectively) and the scanning cross-section of the HCF.
    Fig. 2. Schematic of the experimental setup based on coupling between the tapered solid-core fiber and HCF. AOM, acousto-optical modulator; EDFA, erbium-doped fiber amplifier; PM, power meter; XYZ, manual 3D translation stage; W, uncoated sapphire window; L, plano-convex lens; M, mirror on flipper mount; IBF, infrared bandpass filter. Inserts: the measured transmission loss spectrum (red curve and black curve represent fiber loss from 3000 to 3300 nm and from 1500 to 1600 nm, respectively) and the scanning cross-section of the HCF.
    (a) Measured spectrum of the mid-infrared laser from acetylene-filled HCF lasers taken at 3.5 mbar with 2 m length of HCF. P(3)–P(25) displayed in upper right corner represent corresponding odd pump lines. (b) The simplified molecular energy-level diagram of acetylene for 3 μm emissions when pumped at 1.5 μm absorption band, and the right table displays the odd P branch absorption lines of acetylene molecules used in experiments and the corresponding measured laser wavelengths using the OSA.
    Fig. 3. (a) Measured spectrum of the mid-infrared laser from acetylene-filled HCF lasers taken at 3.5 mbar with 2 m length of HCF. P(3)P(25) displayed in upper right corner represent corresponding odd pump lines. (b) The simplified molecular energy-level diagram of acetylene for 3 μm emissions when pumped at 1.5μm absorption band, and the right table displays the odd P branch absorption lines of acetylene molecules used in experiments and the corresponding measured laser wavelengths using the OSA.
    Measured laser pulse energy with respect to absorbed pump pulse energy for a 2 m long HCF filled with various pressures of acetylene gas when pumped with (a) P(11) and (b) P(13) absorption lines, respectively.
    Fig. 4. Measured laser pulse energy with respect to absorbed pump pulse energy for a 2 m long HCF filled with various pressures of acetylene gas when pumped with (a) P(11) and (b) P(13) absorption lines, respectively.
    Wei Huang, Yulong Cui, Zhiyue Zhou, Zhixian Li, Yubin Chen, Zefeng Wang. Towards all-fiber structure pulsed mid-infrared laser by gas-filled hollow-core fibers[J]. Chinese Optics Letters, 2019, 17(9): 091402
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