Air-Cooled, Picosecond DPSS Lasers

Laser Model	Output Wavelength	Pulse Energy (mJ)	Pulse per second	Peak power	Pulse Length	Pumping	Cooling
COMPILER	1064 nm	0.3	1000	37 MW	8 ps	Diode	Air
	532 nm	0.18	1000	25 MW	7 ps	Diode	Air
	355 nm	0.1	1000	16 MW	6 ps	Diode	Air
	266 nm	0.07	1000	14 MW	5 ps	Diode	Air
	213 nm	0.05	1000	12 MW	4 ps	Diode	Air
COMPILER UPGRADE	1064 nm	2	1000	250 MW	8 ps	Diode	Air or liquid
	532 nm	1	1000	142 MW	7 ps	Diode	Air or liquid
	355 nm	0.5	1000	80 MW	6 ps	Diode	Air or liquid
	1198 nm	0.3	1000	10 MW	32 ps	Diode	Air or liquid
	599 nm	0.15	1000	5 MW	30 ps	Diode	Air or liquid
	299.5 nm	0.05	1000	2 MW	28 ps	Diode	Air or liquid
Compiler HPRR	1064 nm	0.15	14000	18 MW	8 ps	Diode	Air
	532 nm	0.075	14000	10 MW	7 ps	Diode	Air
	355 nm	0.035	14000	5 MW	6 ps	Diode	Air
	266 nm	0.010	14000	2 MW	5 ps	Diode	Air
UV-VIS-PICO	1064 nm	10	200	100 MW	100 ps	Diode	Air or liquid
	532 nm	5	200	55 MW	90 ps	Diode	Air or liquid
	355 nm	3	200	37 MW	80 ps	Diode	Air or liquid
	266 nm	2	200	26 MW	75 ps	Diode	Air or liquid

While high pulse repetition rates provide higher throughput, the high peak power of laser pulses is imperative for cutting different materials with sharper angle, thus significantly reducing material losses and increasing rate of cutting.

The high peak power is one of the most important features of Passat’s family of picosecond lasers, especially at short UV wavelengths (266 nm – 20 MW, 213 nm – 10 MW).

Picosecond Lasers Articles:

Q-switched lasers: Uses proliferate for high-energy picosecond UV lasers

Materials Processing: Picosecond UV lasers pave the way to new applications

Picosecond Lasers versus Femtosecond Lasers in Micromachining

Air-Cooled, Picosecond DPSS Lasers

COMPILER

COMPILER UPGRADE

Compiler HPRR

UV-VIS-PICO

Picosecond Lasers Articles: