2016
DOI: 10.1088/1361-6463/aa4f47
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High power, widely tunable dual-wavelength 2 μm laser based on intracavity KTP optical parametric oscillator

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Cited by 4 publications
(2 citation statements)
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“…The experimental setup is shown in figure 1. The experimental scheme of the dualwavelength 2 µm pump source is similar to our previous work and described in detail in [11,12]. A dichroic mirror coated for high reflection at 1.06 µm and antireflection at 1.9-2.5 µm is used to filter out the fundamental laser.…”
Section: Experiments and Setupmentioning
confidence: 99%
“…The experimental setup is shown in figure 1. The experimental scheme of the dualwavelength 2 µm pump source is similar to our previous work and described in detail in [11,12]. A dichroic mirror coated for high reflection at 1.06 µm and antireflection at 1.9-2.5 µm is used to filter out the fundamental laser.…”
Section: Experiments and Setupmentioning
confidence: 99%
“…Tunable sources near 2 μm are also of interest due to their utility in applications such as speckle-imaging [2][3], eye-safe differential absorption lidar [4][5], range finding [6], coherent Doppler wind lidar [7], and terahertz (THz) difference-frequency-generation (DFG) [8]. Wavelength generation in the 2-μm region has been achieved using Ho 3+ -doped, Tm 3+ -doped, or Tm 3+ :Ho 3+ co-doped fiber lasers [9][10], mode-locked Tm:CaYAlO4 (Tm:CYA) laser [11], near-degenerate optical parametric oscillators (OPOs) [12], and, more recently, intracavity OPOs in two-crystal walkoff compensation scheme [13]. Laser sources at ~2 μm and beyond are also necessary for pumping long-wave mid-infrared (mid-IR) OPOs and DFG sources based on non-oxide nonlinear materials such as ZnGeP2, AgGaS2, AgGaSe2 and quasi-phase-matched orientationpatterned gallium arsenide (OP-GaAs) [12,[14][15][16][17].…”
Section: Introductionmentioning
confidence: 99%