High Energy laser systems with industry leading spatial homogeneity - ideally suited to applications such as Ti:S pumping, Dye laser pumping and deflashing.
The LPY700 Series models feature twin rod oscillator design with birefringence compensation leading to high beam homogeneity and conversion efficiencies. For industrial applications that require high pulse energy at higher frequencies particularly at 532nm at the UV wavelengths these lasers offer superior long term stability and spatial homogeneity.
All systems feature a birefringence compensating twin-rod oscillator, with the option of either single or twin-rod amplifier. This ensures that the highest beam quality and efficiency is obtained.
GENERAL FEATURES
| APPLICATIONS INCLUDE
|
Model | LPY | LPY | LPY | LPY | LPY |
704-50 | 742-50 | 704-30 | 706-30 | 764-30 | |
Repetition Rate (Hz) | 50 | 50 | 30 | 30 | 30 |
Output Energy (mJ) | |||||
1064nm | 300 | 450 | 380 | 550 | 900 |
532nm | 150 | 225 | 190 | 225 | 450 |
355nm | 40 | 80 | 50 | 80 | 150 |
266nm | 20 | 35 | 45 | 60 | 80 |
High Energy, single transverse mode, low divergence laser systems ideally suited to applications requiring a low M-squared, such as LIBS and OPO pumping.
The LPY700 Series models feature twin rod oscillator design with birefringence compensation leading to high beam homogeneity and conversion efficiencies. Gaussian resonators produce very low-divergence, single transverse mode output beams.
GENERAL FEATURES
| APPLICATIONS INCLUDE
|
Model | LPY | LPY | LPY | LPY | LPY |
704G-30 | 706G-30 | 764G-30 | 774G-30 | 787G-30 | |
Repetition Rate (Hz) | 0-30 | 0-30 | 0-30 | 0-30 | 0-30 |
Output Energy (mJ) | |||||
1064nm | 380 | 550 | 900 | 1200 | 1500 |
532nm | 190 | 225 | 450 | 600 | 750 |
355nm | 50 | 80 | 150 | 260 | 300 |
266nm | 45 | 60 | 80 | 120 | 150 |
Click here for full specification on this range or view the PDF files in the more information panel.