Abstract

Ytterbium-doped fiber lasers (YDFLs) working in the near-infrared (NIR) spectral window and capable of high-power operation are popular in recent years. They have been broadly used in a variety of scientific and industrial research areas, including light bullet generation, optical frequency comb formation, materials fabrication, free-space laser communication, and biomedical diagnostics as well. The growing interest in YDFLs has also been cultivated for the generation of high-power femtosecond (fs) pulses. Unfortunately, the operating wavelengths of fs YDFLs have mostly been confined to two spectral bands, i.e., 970-980 nm through the three-level energy transition and 1030-1100 nm through the quasi three-level energy transition, leading to a spectral gap (990-1020 nm) in between, which is attributed to an intrinsically weak gain in this wavelength range. Here we demonstrate a high-power mode-locked fs YDFL operating at 1010 nm, which is accomplished in a compact and cost-effective package. It exhibits superior performance in terms of both short-term and long-term stability, i.e., <0.3% (peak intensity over 2.4 μs) and <4.0% (average power over 24 hours), respectively. To illustrate the practical applications, it is subsequently employed as a versatile fs laser for high-quality nonlinear imaging of biological samples, including two-photon excited fluorescence microscopy of mouse kidney and brain sections, as well as polarization-sensitive second-harmonic generation microscopy of potato starch granules and mouse tail muscle. It is anticipated that these efforts will largely extend the capability of fs YDFLs which is continuously tunable over 970-1100 nm wavelength range for wideband hyperspectral operations, serving as a promising complement to the gold-standard Ti:sapphire fs lasers.

Highlights

  • High-power ytterbium-doped fiber lasers (YDFLs) have gained popularity in the past decade for their high energy, wideband and reliable operations [1,2]

  • It is anticipated that these efforts will largely extend the capability of fs Ytterbium-doped fiber lasers (YDFLs) which is continuously tunable over 970-1100 nm wavelength range for wideband hyperspectral operations, serving as a promising complement to the gold-standard Ti:sapphire fs lasers

  • This can be attributed to the gain-window shifting as well as the nonlinear effects induced by the high peak power, which can be improved by placing a prechirped stage between the master oscillator and external power booster, e.g., a piece of single-mode fibers (SMFs), which is usually performed for chirped-pulse amplification (CPA) [42]

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Summary

Introduction

High-power ytterbium-doped fiber lasers (YDFLs) have gained popularity in the past decade for their high energy, wideband and reliable operations [1,2]. YDFLs working at 990-1020 nm have rarely been demonstrated, mainly due to the small gain coefficient and the gain competition from the three-level and quasi-three-level bands [1] Bridging this wavelength gap is crucial to achieve a wideband hyperspectral capability, which is essential in applications such as multicolor two-photon excited fluorescence (TPEF) microscopy [15] and hyperspectral coherent Raman scattering microscopy [16,17]. In Amp, another 40-cm YDF (Thorlabs Yb 1200-4/125) serves as the gain medium, which is bidirectionally pumped through two sets of WDMs and LDs. After the power booster, the high-power laser pulses are launched into free space through another fiber collimator with a beam waist diameter of ~4.0 mm. It should be pointed out that the current multiphoton microscope operates in transmission mode with forward detection, while it can be modified to implement epi-detection

Performance of master fiber oscillator
Second-harmonic generation imaging
Conclusions

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