Picosecond laser
Picosecond laser-non-frequency doubling
Real photos | Wavelength | Pulse Width | Power | Introduction | Features |
![]() | 6-20ps | 6-200mW | The nonlinear technology is used to realize the saturable absorber effect. The long-term stability of the output laser pulse is extremely high. It can work in high and low temperature environments and provide an excellent seed source solution for ultrafast laser processing. |
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![]() | 6-20ps | 1-50W | The nonlinear technology is used to realize the saturable absorber effect. The high-power laser pulse is output stably for a long time through amplification. It can work in high and low temperature environments and is suitable for precision machining. |
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Picosecond laser-frequency doubling
Real photos | Wavelength | Pulse Width | Power | Introduction | Features |
![]() | <20ps@1064nm <50ps@1064nm | 1-40W | Adopt solid state amplification solution to achieve high repetition rate and high power output, suitable for precision detection |
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Picosecond laser-frequency tripling
Real photos | Wavelength | Pulse Width | Power | Introduction | Features |
![]() | <20ps@1064nm <50ps@1064nm | 1-8W | Adopt solid state amplification solution to achieve high repetition rate and high power output, suitable for precision detection |
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Picosecond laser-Frequency quadrupling
Real photos | Wavelength | Pulse Width | Power | Introduction | Features |
![]() | 266nm | <20ps@1064nm <50ps@1064nm | 1-5W | Adopt solid state amplification solution to achieve high repetition rate and high power output, suitable for precision detection |
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