Publications by authors named "Hsing-Chih Liang"

A diode-pumped Kerr-lens mode-locked laser generating 25 fs pulses at 1080 nm is demonstrated with an Yb-doped compositional mixed calcium aluminate crystal. The Yb:Ca(Gd,Y)AlO laser, which operates at a repetition rate of 65.6 MHz via soft-aperture Kerr-lens mode-locking, is pumped by a spatially single-mode, fiber-coupled diode laser.

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For accurate measurement of carboxyhemoglobin level in the blood, a compact dual-wavelength laser at 555 and 579.5 nm with conversion efficiency up to 27.5% is originally developed by using Nd:YVO/KGW/LBO laser with intracavity stimulated Raman scattering (SRS), second harmonic generation (SHG), and sum frequency generation (SFG).

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We develop a compact high-frequency actively Q-switched Nd:YVO/YVO Raman laser at 1525 nm. The mode size stability and the mode overlapping are numerically analyzed to craft the resonator. Experimental results reveal that the compact cavity and the cavity dumping effect lead to the considerable narrowing of the pulse width.

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  • * Using these equations, we successfully created a solid-state laser that produces a stable pulse train at a low repetition rate of 18 MHz by designing the cavity for a specific trajectory.
  • * By fine-tuning the mirrors in the same setup, we can also achieve lower pulse repetition rates of 12 and 9 MHz, showing a practical method for obtaining low repetition rates in lasers.
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We report on the continuous-wave (CW) and, for what we believe to be the first time, passively mode-locked (ML) laser operation of an Yb-doped YSr(PO) crystal. Utilizing a 976-nm spatially single-mode, fiber-coupled laser diode as pump source, the Yb:YSr(PO) laser delivers a maximum CW output power of 333 mW at 1045.8 nm with an optical efficiency of 55.

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Two compact laser sources at 707 and 714 nm are realized efficiently by using a diode-pumped a-cut Nd:YVO laser with intracavity stimulated Raman scattering and sum-frequency generation (SFG). The fundamental wave at 1342 nm is generated by the F → I transition in Nd:YVO crystal. The Raman Stokes waves at 1496 and 1526 nm were obtained by placing the c-axis of the Nd:YVO crystal along the Ng and Nm axes of an Np-cut KGW crystal, respectively.

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A low-threshold continuous wave dual-wavelength mid-infrared laser is demonstrated by using an intracavity optical parametric oscillator (OPO) with a dual-wavelength pump wave. To realize a high-quality dual-wavelength pump wave, a composite Nd:YVO/Nd:GdVO gain medium is applied for a linear polarized state and synchronization output. With the quasi-phase-matching OPO process, it is found that the dual-wavelength pump wave shares equal signal wave oscillation and leads to a lower OPO threshold.

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A compact efficient continuous wave (CW) laser with selectable two wavelengths at 671 and 714 nm is developed. The laser cavity comprises an Nd-doped and an undoped YVO crystal to generate the fundamental wave at 1342 nm and the first-Stokes Raman wave at 1525 nm, respectively. A single LBO crystal with the cut angle in the XZ plane is designed to achieve the selectable phase-matching via the thermal tuning for the second harmonic generation (SHG) of 1342 nm and the sum frequency generation (SFG) of 1342 and 1525 nm.

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  • * A unique Np-cut KGW crystal is used to selectively produce either a yellow 579 nm laser or an orange 589 nm laser, enhancing versatility.
  • * The design features a compact resonator that boosts efficiency, with the orange laser achieving output energies up to 0.08 mJ and peak powers of 50 kW, while the yellow laser can reach 0.10 mJ and 80 kW peak power.
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  • * It was found that the focal length of the thermal lens for one polarization is negative (ranging from -1.1 to -0.5) as pump power increases, while for the other polarization, it is positive (ranging from 1.2 to 0.9 m) with a different range of pump power.
  • * The sensitivity factors for thermal lensing were calculated, resulting in -0.54 for the negative focal length polarization and 0.1 for the positive focal length polarization.
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We propose a theoretical model to generate the resonant geometric modes localized on ray periodic trajectories with orbital angular momentum. Based on the numerical analysis, we realize resonant geometric modes in the off-axis pumped degenerate cavity ${\rm Nd}{:}{{\rm YVO}_4}$Nd:YVO lasers with an external mode converter. The experimental results reveal that laser output modes display the planar geometric modes when the off-axis displacement is sufficiently large, and the cavity length is set to satisfy the degenerate conditions.

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  • A novel mode-locked laser scheme is created using a reflected Fabry-Perot (FP) cavity, resulting in stable continuous-wave operation with a repetition rate of 48 MHz and average output power of 2.6 W.
  • The pulse width of the laser can be adjusted by changing the optical thickness of the FP cavity, ranging from 0.8 to 2.6 ns.
  • The study highlights the importance of the reflected FP cavity in generating optical pulses with narrow spectral linewidths, offering a promising approach for future laser technologies.
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A continuous-wave (cw) self-mode-locked Tm:YAG laser at 2015 nm is successfully demonstrated by suppressing the self-pulsing behavior. By using rate equations to simulate the laser temporal dynamic, the theoretical analysis indicates that the reabsorption-induced self-pulsing for the Tm:YAG laser can be suppressed with sufficient pump power. It is experimentally confirmed that at absorbed powers higher than 6 W, the self-pulsing can be eliminated and a cw self-mode-locked pulse is generated instead of the Q-switched mode locking.

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A synchronously dual self-mode-locked (SML) operation at 946 and 1064 nm is experimentally accomplished by using a compact coupling scheme to obtain the optical beating frequency up to 35.2 THz. The SML emissions at 946 and 1064 nm are established by a monolithic Nd:YAG cavity and a Nd:YVO crystal in a flat-flat cavity, respectively.

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  • * Our numerical analysis confirms these dynamics are due to the total mode locking of different transverse electromagnetic modes and higher-order modes that exhibit significant astigmatism.
  • * The behaviors we found are comparable to what's seen in Ti:sapphire lasers that utilize soft-aperture Kerr-lens mode locking.
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