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2021-07-13 18:33:55
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Femtosecond ultrafast lasers are one of the most powerful research tools developed by laser science in the past three decades, with their rapid development and the expansion and deepening of femtosecond ultrafast laser-related applications mutually reinforcing and promoting each other.
With the further expansion and deepening of femtosecond ultrafast spectroscopy and nonlinear optical microscopy imaging related applications, some important experimental studies in recent years require the simultaneous use of multiple femtosecond ultrafast light fields at different wavelengths (i.e., multicolor femtosecond ultrafast light fields). In terms of ultra-intensity, how to obtain a stable and clean seed source in ultra-intense and ultra-short laser systems, and how to achieve accurate and efficient measurement of parameters such as temporal width and contrast of femtosecond laser pulses, are crucial for the long-term development of ultra-intense and ultra-short femtosecond lasers themselves and their applications.
Given the ultrafast response characteristics of femtosecond laser pulse Four-Wave, it can serve as an ultrafast optical switch or ultrafast filter for ultrafast modulation of incident femtosecond laser pulses, opening up new avenues for obtaining stable and clean seed sources in ultra-intense and ultra-short laser systems. Femtosecond Four-Wave can also be used to obtain multicolor femtosecond lasers and to achieve accurate and efficient measurement of important parameters such as temporal width and temporal contrast of femtosecond laser pulses.
In summary, the development of femtosecond Four-Wave technology brings new insights to femtosecond laser-related technological research. The following text will outline the applications of four femtosecond Four-Wave techniques in femtosecond laser research: cascaded Four-Wave (CFWM), cross-polarization wave generation (XPW), self-diffraction (SD), and transient grating (TG), for reader reference.
Application Background: The output wavelength range of common solid-state lasers is usually limited to certain regions. For example, titanium sapphire's emission wavelength range is 700 nm-900 nm, chromium-doped forsterite's emission wavelength range is 1200 nm-1360 nm, and chromium-doped garnet's emission wavelength range is 1360 nm-1570 nm.
However, in fields such as multicolor nonlinear optical microscopy imaging and multidimensional ultrafast spectroscopy research, multiple femtosecond laser pulses with different central wavelengths are often required, making frequency conversion of laser pulses to obtain suitable wavelengths a very important task. The CFWM process is a collection of multiple non-degenerate femtosecond Four-Wave. Two femtosecond light beams with different central wavelengths, crossing and overlapping at a certain angle in a third-order nonlinear material, can simultaneously obtain multiple spatially separated and tunable central wavelength femtosecond laser pulses. Based on the output light of currently commercialized 25 fs titanium sapphire amplifiers, CFWM can be used to obtain femtosecond laser pulses with energy exceeding hundreds of microjoules, with a spectral range covering ultraviolet to near-infrared.
Application Advantages: The device used is simple and compact, and to some extent, it is equivalent to multiple NOPAs working simultaneously, making it simple and economical [1].