Abstract

Ultrafast mid-infrared (mid-IR) lasers with a high pulse repetition rate are in great demand in various fields, including attosecond science and strong-field physics. Due to the lack of suitable mid-IR laser gain medium, optical parametric amplifiers (OPAs) are used to generate an ultrafast mid-IR laser. However, the efficiency of OPA is sensitive to phase mismatches induced by wavelength and temperature deviations from the preset points, which thus limits the pulse duration and the average power of the mid-IR laser. Here, we exploited a noncollinear phase-matching configuration to achieve simultaneously wavelength- and temperature-insensitive mid-IR OPA with a LiGaS2 crystal. The noncollinearity can cancel the first-order dependence of phase matching on both wavelength and temperature. Benefitting from the thermal property of the LiGaS2 crystal, some collinear phase-matching solutions derived from the first-order and even third-order wavelength insensitivity have comparatively large temperature bandwidths and can be regarded as approximate solutions with simultaneous wavelength and temperature insensitivity. These simultaneously wavelength- and temperature-insensitive phase-matching designs are verified through numerical simulations in order to generate few-cycle, high-power mid-IR pulses.

Highlights

  • Academic Editors: Tongyu Dai andMid-infrared lasers are important for the fields of research, industry, and medicine

  • Ultrafast intense mid-IR lasers are in great demand in attosecond science due to the λ2 -scaling law in the high-order harmonic generation (HHG) process [1]

  • We focus on the semiconductor LiGaS2 crystal, which has been popular in recent years because it has a high transparency from 0.32 to 11.6 μm, covering both the near-IR pump source around 1 μm and the mid-IR

Read more

Summary

Introduction

Academic Editors: Tongyu Dai andMid-infrared (mid-IR) lasers are important for the fields of research, industry, and medicine. Ultrafast intense mid-IR lasers are in great demand in attosecond science due to the λ2 -scaling law in the high-order harmonic generation (HHG) process (cutoff frequency ∝ λ2 , pulse duration ∝ λ−2 ) [1]. Mid-IR laser-driven HHG can generate shorter attosecond pulses with wavelengths accessible in both soft and hard X-ray regions [2]. Nonlinear optical parametric amplification (OPA) has become the popular route for generating mid-IR lasers [4,5]. Different from laser amplifiers, OPA has to satisfy the phase-matching (PM) condition for efficient energy transfer from the pump to signal. The perfect PM condition is usually satisfied within a limited range of wavelengths and temperatures, as the refractive index depends on both the wavelength and temperature. The practical demands for ultrashort pulses and high repetition rates require a PM condition with both a large wavelength and temperature tolerance

Objectives
Results
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call