Innotech Laser are experts in Huaray DPSS Laser systems
Let us advise you on DPSS-Lasersystems from Huaray Precision Laser Technologies Co., Ltd. In our DPSS-Laser portfolio you will find nanosecond DPSS-Laser, picosecond DPSS-Laser, femtosecond DPSS-Laser, UV-Laser and green Laser.
In a personal consultation, we will work with you to determine which DPSS-Lasersystem is best suited as a beam source for your Laserapplication. Please contact us for data sheets, drawings or further technical information on the DPSS-Laserbeam sources listed.
- Compact design
- Easy integration
- Short pulse widths
- Excellent beam quality
- Long service life
- Huge application range
Product | Wavelength | Power | Repetition rate | Pulse width | Beam quality | Start-up time | Beam ∅ | Cooling | Data sheet |
---|---|---|---|---|---|---|---|---|---|
Poplar-355-3 | 355 nm | >3 W @ 50 kHz | 20-200 kHz | <10 ns @ 50 kHz | M²≤1,2 | <15 min | ≤4 mm | Water | |
Poplar-355-5 | 355 nm | >5 W @ 50 kHz | 20-200 kHz | <10 ns @ 50 kHz | M²≤1,2 | <15 min | ≤4 mm | Water | |
Maple-355-5 | 355 nm | >5 W @ 50 kHz >110 μJ @ 50 kHz | 20-200 kHz | <10 ns @ 50 kHz | M²≤1,2 | <15 min | ≤3.5 mm | Air | |
Cypress-355-10 | 355 nm | >10 W @ 60 kHz >160 μJ @ 60 kHz | 50-200 kHz | <12 ns @ 60 kHz | M²≤1,2 | <15 min | ≤4 mm | Water | |
Cypress-355-15 | 355 nm | >15W @ 50 kHz >300 μJ @ 50 kHz | 50-200 kHz | <15 ns @ 50 kHz | M²≤1,2 | <15 min | ≤4 mm | Water | |
Cypress-355-20 | 355 nm | >20 W @ 60 kHz >300 μJ @ 60 kHz | 50-200 kHz | <20 ns @ 60 kHz | M²≤1,2 | <15 min | ≤3 mm | Water | |
Cypress-355-25 | 355 nm | >25 W @ 60 kHz >410 μJ @ 60 kHz | 50-200 kHz | <20 ns @ 60 kHz | M²≤1,2 | <15 min | ≤3 mm | Water |
- Compact design
- Long service life
- Huge application range
- Infrared, green or UV Laser
- Short pulse widths
- High pulse energy
- Crossover power adjustment possible
Product | Wavelength | Power | Repetition rate | Pulse width | Beam quality | Start-up time | Beam ∅ | Cooling | Data sheet |
---|---|---|---|---|---|---|---|---|---|
Olive-355-10 | 355 nm | >10 W @ 1 MHz >20 µJ | 400 kHz-2 MHz | <10 ps | M²≤1,3 | <30 min | ≤2 mm | Water | |
Olive-355-30 | 355 nm | >30 W @ 800 kHz >75 µJ | 400 kHz-1 MHz | <10 ps | M²≤1,3 | <30 min | ≤2 mm | Water | |
Pine-532-30 | 532 nm | >30 W @ 1 MHz >30 µJ @ 1 MHz | 1 MHz-2 MHz | <10 ps | M²≤1,3 | <30 min | ≤3 mm | Water | |
Olive-1064-20 | 1064 nm | >20 W @ 500 kHz >100 μJ @ 200 kHz | 100 kHz-1 MHz | <10 ps | M²≤1,3 | <30 min | ≤2 mm | Water | |
Olive-1064-40 | 1064 nm | >40 W @ 500 kHz >200 μJ @ 200 kHz | 50 kHz-1 MHz | <10 ps | M²≤1,3 | <30 min | ≤2 mm | Water | |
Pine-1064-50 | 1064 nm | >50 W @ 500 kHz >300 μJ @ 100 kHz | 100 kHz-1 MHz | <10 ps | M²≤1,3 | <30 min | ≤3 mm | Water | |
Olive-1064-100 | 1064 nm | >100 W @ 1 MHz >250 µJ | 400 kHz-1 MHz | <10 ps | M²≤1,3 | <30 min | ≤1.5 mm | Water |
- Compact design
- Long service life
- Huge application range
- Up to 10 μJ pulse energy
- Integrated optical isolator
- <300 fs - 10 ps pulse widths
- Integrated monitoring detector
- Optional SHG unit
Product | Wavelength | Power | Repetition rate | Pulse width | Beam quality | Start-up time | Beam ∅ | Cooling | Data sheet |
HR-IR-50-40 | 1035 nm | >40 W 50 μJ @ 800 kHz | Single shot up to 1MHz | <300 fs - 10 ps | M²≤1,3 | <30 min | ≤3 mm | Water | |
HR-IR-80-60 | 1035 nm | >60 W 80 μJ @ 750 kHz | Single shot up to 1MHz | <300 fs - 10 ps | M²≤1,3 | <30 min | ≤3 mm | Water | |
HR-IR-200-40 | 1035 nm | >40 W 200 μJ @ 750 kHz | Single shot up to 200 kHz | <300 fs - 10 ps | M²≤1,3 | <30 min | ≤3 mm | Water | |
HR-Femto-GN-20-15 | 517 nm | >15 W >20 μJ @ 800 MHz | Single shot up to 800 kHz | <300 fs - 10 ps | M²≤1,3 | <30 min | ≤3 mm | Water | |
HR-Femto-GN-30-20 | 517 nm | >20 W >30 μJ @ 750 MHz | Single shot up to 1 MHz | <300 fs - 10 ps | M²≤1,3 | <30 min | ≤3 mm | Water | |
HR-Femto-GN-75-15 | 517 nm | >15 W >75 μJ @ 750 MHz | Single shot up to 200 kHz | <300 fs - 10 ps | M²≤1,3 | <30 min | ≤3 mm | Water |
These are the biggest advantages and disadvantages of DPSS Lasern
The advantages are a compact Laserunit and a higher efficiency from electrical to optical power. The power density and beam quality are improved by the fact that less heat is introduced by the pump source and the service life is significantly longer. However, the Laserdiodes are quite expensive, which can increase the initial investment.