Cross-flow resonators
Over 1,500 low-consumption, clean-running laser machining powerhouses sold. 0 replacements needed.
The best laser in the world is only as good as its access to reliable, uninterrupted, productivity-fueling power.
That’s why we’ve developed our own series of cross-flow resonators optimized specifically for Mitsubishi laser machines. But what’s so special about them?
Our cross-flow resonators deliver a unique pulse that results in a sharper beam, leads to cleaner parts, and contributes to a best-in-industry 90% lower gas consumption—all so your maintenance and downtime costs remain as low as possible.
That’s partly why, with more than 1,500 Mitsubishi laser machines sold and not a single replacement required, our cross-flow resonators remain the most reliable on the market.
90% EASIER RESOURCE MANAGEMENT
- Imagine if, after operating a laser machine for one month, you got almost all of your resource budget back in your pockets. What would you do with it?
Our cross-flow resonators consume far fewer materials to keep a Mitsubishi laser up and running, with no negative impact on work quality, cutting power, or production speed.
NO INTERRUPTIONS, NO SURPRISES
- With more than 1,500 Mitsubishi laser machines sold and not a single replacement required, they’re the most reliable on the market.
LESS DOWNTIME REQUIRED
- Powering your laser machines with one of our cross-flow resonators results in sharper beams with less waste, meaning you can spend less time cleaning your machine and more time running it.
| Model | 20CF3 | 20XF | 32XP | 30CF-R | 35CF-R | 40CF-R | 45CF-R | 60XF |
| Rated CW Power (W) | 2000 | 2000 | 2700 | 3000 | 3500 | 4000 | 4500 | 6000 |
| Beam mode | Low-order mode (TEM o1* main component) | Low-order mode (TEM o1* main component) | Low-order mode (TEM o1* main component) | Low-order mode (TEM o1* main component) | Low-order mode (TEM o1* main component) | Low-order mode (TEM o1* main component) | Low-order mode (TEM o1* main component) | Low-order mode (TEM o1* main component) |
| Beam output diameter: in (mm) | ~ 0.83 (21) | ~ 0.83 (21) | ~ 0.83 (21) | ~ 1.02 (26) | ~ 1.02 (26) | ~ 1.02 (26) | ~ 1.02 (26) | ~ 1.06 (27) |
| Power stability (%) | Less than +/-1% of rated power | Less than +/-1% of rated power | Less than +/-1% of rated power | Less than +/-1% of rated power | Less than +/-1% of rated power | Less than +/-1% of rated power | Less than +/-1% of rated power | Less than +/-1% of rated power |
| Gas sealing time: hr | 24 | 24 | 24 | 24 | 24 | 24 | 24 | 24 |
| Laser gas consumption rate: l/hr (liter/hour) | 1 | 1 | 1 | 3 | 3 | 3 | 3 | 3 |
| Overall dimensions: W x D x H in (mm) |
98.43 x 31.5 x 71.3 (2,500 x 800 x 1,810) |
80.3 x 17.7 x 63.8 (2,040 x 450 x 1,620) | 80.3 x 17.7 x 63.8 (2,040 x 450 x 1,620) | 98.43 x 31.5 x 71.3 (2,500 x 800 x 1,810) | 98.43 x 31.5 x 71.3 (2,500 x 800 x 1,810) | 98.43 x 31.5 x 71.3 (2,500 x 800 x 1,810) | 98.43 x 31.5 x 71.3 (2,500 x 800 x 1,810) |
98.43 x 31.5 x 71.3 (2,500 x 800 x 1,810) |
| Mass: lb (kg) |
2,650 (1,200) |
2,650 (1,200) | 2,650 (1,200) | 4,850 (2,200) | 4,850 (2,200) | 4,850 (2,200) | 4,850 (2,200) |
6,615 (3,000) |
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