0 - 20Hz Lasers
10Hz Pulsed Nd:YAG Lasers with Stable and Telescopic Resonators
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. Telescopic resonators produce low-divergence output beams that are spatially smooth in the near field suiting them to a host of pump source applications.
GENERAL FEATURES
| APPLICATIONS INCLUDE
|
| Model | LPY | LPY | LPY |
704-10 | 706-10 | 764-10 | |
| Repetition Rate (Hz) | 0-10 | 0-10 | 0-10 |
| Output Energy (mJ) | |||
| 1064nm | 420 | 650 | 1250 |
| 532nm | 210 | 325 | 675 |
| 355nm | 80 | 100 | 200 |
| 266nm | 50 | 70 | 120 |
10Hz Gaussian Coupled Pulsed Nd:YAG Lasers
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 | LPY |
704G-10 | 706G-10 | 707G-10 | 764G-10 | 776G-10 | 787G-10 | |
| Repetition Rate (Hz) | 0-10 | 0-10 | 0-10 | 0-10 | 0-10 | 0-10 |
| Output Energy (mJ) | ||||||
| 1064nm | 400 | 650 | 850 | 1250 | 1600 | 2000 |
| 532nm | 200 | 325 | 425 | 625 | 800 | 1000 |
| 355nm | 80 | 110 | 150 | 225 | 320 | 400 |
| 266nm | 50 | 75 | 95 | 125 | 160 | 195 |
10Hz Pulsed Nd:YAG Lasers with Stable and Telescopic Resonators
High Energy laser systems with industry leading spatial homogeneity - ideally suited to applications such as Ti:S pumping, Dye laser pumping and deflashing.
The LPY600 Series models are single rod oscillators or oscillator-amplifiers. Telescopic resonators produce low-divergence output beams that are spatially smooth in the near field suiting them to a host of pump source applications.
GENERAL FEATURES
| APPLICATIONS INCLUDE
|
| Model | LPY | LPY |
664-10 | 674-10 | |
| Repetition Rate (Hz) | 0-10 | 0-10 |
| Output Energy (mJ) | ||
| 1064nm | 850 | 1000 |
| 532nm | 425 | 500 |
| 355nm | 130 | 160 |
| 266nm | 95 | 110 |
10Hz Gaussian Coupled Pulsed Nd:YAG Lasers
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 LPY600 Series models are single rod oscillators or oscillator-amplifiers. Gaussian resonators produce very low-divergence, single transverse mode output beams.
GENERAL FEATURES
| APPLICATIONS INCLUDE
|
| Model | LPY |
674G-10 | |
| Repetition Rate (Hz) | 0-10 |
| Output Energy (mJ) | |
| 1064nm | 1000 |
| 532nm | 500 |
| 355nm | 250 |
| 266nm | 110 |
20Hz Pulsed Nd:YAG Lasers with Stable and Telescopic Resonators
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. Telescopic resonators produce low-divergence output beams that are spatially smooth in the near field suiting them to a host of pump source applications.
GENERAL FEATURES
| APPLICATIONS INCLUDE
|
| Model | LPY | LPY | LPY |
704-20 | 706-20 | 764-20 | |
| Repetition Rate (Hz) | 0-20 | 0-20 | 0-20 |
| Output Energy (mJ) | |||
| 1064nm | 380 | 600 | 1000 |
| 532nm | 190 | 300 | 500 |
| 355nm | 70 | 85 | 140 |
| 266nm | 45 | 65 | 90 |
20Hz Gaussian Coupled Pulsed Nd:YAG Lasers
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 | LPY |
704G-20 | 706G-20 | 707G-20 | 764G-20 | 776G-20 | 787G-20 | |
| Repetition Rate (Hz) | 0-20 | 0-20 | 0-20 | 0-20 | 0-20 | 0-20 |
| Output Energy (mJ) | ||||||
| 1064nm | 380 | 600 | 800 | 1000 | 1400 | 1800 |
| 532nm | 190 | 300 | 400 | 500 | 700 | 900 |
| 355nm | 70 | 90 | 130 | 140 | 280 | 380 |
| 266nm | 45 | 65 | 75 | 90 | 140 | 180 |
20Hz Pulsed Nd:YAG Lasers with Stable and Telescopic Resonators
High Energy laser systems with industry leading spatial homogeneity - ideally suited to applications such as Ti:S pumping, Dye laser pumping and deflashing.
The LPY600 Series models are single rod oscillators or oscillator-amplifiers. Telescopic resonators produce low-divergence output beams that are spatially smooth in the near field suiting them to a host of pump source applications.
GENERAL FEATURES
| APPLICATIONS INCLUDE
|
| Model | LPY | LPY |
| 664-20 | 674-20 | |
| Repetition Rate (Hz) | 0-20 | 0-20 |
| Output Energy (mJ) | ||
| 1064nm | 800 | 850 |
| 532nm | 400 | 425 |
| 355nm | 110 | 130 |
| 266nm | 75 | 80 |
20Hz Gaussian Coupled Pulsed Nd:YAG Lasers
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 LPY600 Series models are single rod oscillators or oscillator-amplifiers. Gaussian resonators produce very low-divergence, single transverse mode output beams.
GENERAL FEATURES
| APPLICATIONS INCLUDE
|
| Model | LPY |
674G-20 | |
| Repetition Rate (Hz) | 0-20 |
| Output Energy (mJ) | |
| 1064nm | 850 |
| 532nm | 425 |
| 355nm | 150 |
| 266nm | 80 |
Click here for full specification on this range or view the PDF files in the more information panel.