UN laser à fibre uses rare-earth-doped glass fiber as the gain medium, and ytterbium-doped fiber is one of the core components in high-power ytterbium-doped fiber laser systems. As the output power of lasers à fibre increases, various stability “killers” like Transverse Mode Instability (TMI), Stimulated Raman Scattering (SRS), and thermal damage have emerged as challenges.

Recently, Zhao Juyun, the Product Director of Kepin Fiber Laser, shared online insights on “Cutting-Edge Technologies and Innovative Applications of High-Power Fiber Lasers,” detailing how to combat the stability “killers” in lasers à fibre. Let’s review the main points discussed.

Fiber Laser Principle and Structure

UN laser à fibre primarily consists of three components: the pump source, the gain medium (active fiber), and the resonator cavity.

Resonator Cavity Fiber Laser Principle: The pump semiconductor laser’s power is injected into the ytterbium-doped double-clad fiber (YDF) via fiber gratings (HR for high-reflectivity, OC for low-reflectivity). The ytterbium-doped fiber absorbs the pump light, leading to a population inversion, and generates spontaneous radiation. This radiation is then amplified by stimulated emission in the cavity formed by the fiber gratings, creating laser output, which is subsequently guided out through the output optical cable.

Amplifier Structure Fiber Laser Principle: Similar to the resonator cavity, the difference lies in the seed laser from the previous stage, reducing the power requirements for individual components, thus enabling higher power output.

Transverse Mode Instability (TMI) Effect in Fiber Lasers

Transverse Mode Instability (TMI) occurs when high-power lasers à fibre reach a specific threshold. As the output power increases or after a certain amount of time, the output mode switches from a steady fundamental mode to an unstable high-order mode. This leads to beam quality degradation and limits the increase in output power. In severe cases, it can undermine the effectiveness of a laser à fibre, rendering it less effective than advertised.

Principle and Experimental Data on Mode Instability

After mode instability occurs, power between the fundamental and high-order modes continues to couple, maintaining constant total power. When mechanisms like bend filtering are present, the fundamental mode has a smaller loss, and the higher-order modes experience more significant bending losses, resulting in the high-order modes being filtered out, and the output shows fundamental mode jitter in the time domain.

Factors Influencing Mode Instability

Unlike traditional high-energy lasers, mode instability is caused by thermal effects and the coupling between the fiber modes. Therefore, the factors influencing mode instability not only relate to waste heat but also to the fiber’s mode characteristics. The main influencing factors are:

Fiber Doping Characteristics: Doping concentration and the radius of the doping region.

Darkening Effects: Impacts on signal light power, signal strength noise, and signal initial high-order mode ratio.

Pump Characteristics: Pump power, wavelength, and intensity modulation.

Pump Method: Forward pumping, backward pumping, side pumping, and bidirectional pumping.

Fiber Material: Fiber core diameter, cladding diameter, and numerical aperture.

Fiber Mode Influencing Factors: High-order mode losses, system cooling ability, and fiber polarization properties.

Methods to Suppress Mode Instability

To counteract mode instability, measures focus on improving thermal management and mode control capabilities.

Enhancing Thermal Management: By adjusting the fiber core-cladding ratio, changing the semiconductor pump wavelength, increasing signal injection power, and optimizing the pump light direction, the gain saturation can be improved, reducing thermal damage.

Improving Mode Control: Increasing bending loss (by reducing the bending radius, decreasing fiber core numerical aperture, and optimizing fiber winding methods) can help suppress higher-order modes and improve output stability.

Stimulated Raman Scattering (SRS) in Fiber Lasers

Stimulated Raman Scattering (SRS) occurs when a laser photon interacts with the medium, causing a shift to longer wavelengths. SRS is a major nonlinear effect that limits the increase in laser à fibre power. For ytterbium-doped fibers, the SRS effect depends on core diameter, fiber length, doping concentration, and pump method.

Methods to Suppress Stimulated Raman Scattering

Core Diameter Impact: As pump power increases, SRS occurs at higher pump power levels. Increasing the fiber core diameter significantly raises the SRS power threshold.

Fiber Length Impact: SRS decreases as fiber length increases. By reducing fiber length, the output power can be increased.

Doping Concentration Impact: As doping concentration increases, the threshold for SRS decreases, resulting in lower output laser power. In high-power fiber lasers, low-doping concentration fibers are selected to mitigate SRS effects.

Future Developments in Fiber Laser Technology

Thanks to advancements in Large Mode Area (LMA) gain fiber technology, high-power, high-brightness semiconductor pump sources, and high-power pump coupling technology, lasers à fibre are expected to continue developing towards higher power levels and better beam quality.