Technical data:
Wavelength | 355 nm |
Spatial mode | TEM00 |
Beam divergence (full angle) | < 2.5 mrad |
Ellipticity | < 2:1 |
Beam diameter | 400 ± 150 μm (at laser aperture) |
Peak power | 180 kW @ 20 Hz |
Pulse energy | > 300 μJ @ 20 Hz |
Pulse repetition rate | 1 – 80 Hz [5 – 40 Hz, with closed loop control for pulse energy] |
Pulse width (FWHM) | < 1.7 ns |
Polarisation orientation and purity | > 100:1, vertical |
Long term pulse energy stability (6 Stunden) | < ± 5 % |
Pulse-to-pulse stability | < 3 % rms |
Optical output | Free beam |
Laser class | 3B / IIIb |
Residual 532nm emission | < 0.5 mW @ 1064 nm (Class 3R) < 0.1 mW @ 532 nm (Class 2) |
Electrical power consumption | < 90 W |
Line voltage | 100 – 240 V AC (50-60 Hz) or 24 V DC |
RS 232, USB
Warm-up time | < 15 min |
Operating temperature | 18 – 38 °C |
Laser head size | 217 x 65 x 45 mm |
- SMA-connectors for fibers with a diameter ≥ 400 μm
- Synchronization module (rise time < 2 ns)
- Manual shutter or electrical beam blocker
- Manual or electrically driven wavelength switch 532 nm / 1064 nm
- Upgrade to 1 kHz pulse frequency (on request)
- External telescope (i.e. M=5)
- Heat sink with fan (recommended for pulse frequencies > 50 Hz)
- Manual or electrical Attenuator
- Stand-alone system (incl. key-switch, heat-sink and manual shutter; CDRH compliant)
The well-established high-power product series
The first firmly established product development of CryLaS GmbH is the High-Power Series. With comparatively low repetition rates of about 20 Hz to 100 Hz, the pulse energies here are much higher than those of the Q lasers developed later. The latter have more compact dimensions, both for the controller and the laser head, but unlike the High-Power series, they are not optimized by closed-loop control. NLO optics (conversion crystals) are installed in an airtight capsule, which convert the initially generated 1064 nm fundamental to frequency multiples, so that wavelengths from DUV to IR are available with these lasers:
- 213 nm
- 266 nm
- 355 nm
- 532 nm
- 1064 nm
A photodiode monitors the relative laser energy at the beam output during operation and passes this data to a closed loop control system. The diode currents are evaluated and ultimately serve as the basis for fast-acting temperature adjustments within the laser head. These always keep the noise of the laser power as low as possible in the optimum. Since heat is generated in the laser (when pumping the resonator), the closed loop serves to counteract this.
The 355 nm lasers of the High-Power model series are based on frequency conversion and combination. The microchip, consisting of an Nd:YAG as well as a Cr.YAG crystal bonded to it, is pumped with an 808 nm laser diode. The resulting fundamental wave of 1064 nm is guided into conversion crystals sealed off from the air and finally frequency tripled, resulting in an emission wavelength of 355 nm. Depending on the pump time, lasers with three different pulse energies from 70 µJ to 300 µJ can be realized. Since the wavelength is well absorbed by biological materials without destroying them extensively, lasers at 355 nm are well suited for cutting or dividing biological samples, such as cell structures. Therefore, the 355-HP series is mainly used in mass spectroscopy and microdissection. Their high pulse energy puts them in direct competition with the 337.1 nm nitrogen (N2) lasers also commonly used in these applications.
The passive Q-switching of the CryLaS lasers saves acquisition costs and also makes the lasers very compact. Similar to the MOPA and Q series, the HP lasers are diode-pumped microchip lasers. The compact, rugged and air-sealed housing gives the laser a long service life and makes it insensitive to outdoor influences. By storing all relevant data about the laser, it is possible to perform remote maintenance and adjust the lasers in the field to the environmental conditions or perform repairs. The lasers can also be adapted to any application by means of adaptable options. It is possible to attenuate the laser energy by optical filters, to couple the light in fibers, to integrate a wavelength switch to a higher conversion level or to widen the laser beam. Years of field testing have made the lasers suitable not only for scientific applications, but also for industrial applications and 24/7 operation.
Conclusion:
- Max. repetition rate: 80 Hz – 100 Hz
- High output energy in a compact housing: 70 µJ – 600 µJ
- Average power of 7 mW up to 12 mW
- Peak power of 50 kW up to 350 kW