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Industrial Laser

The high-power passive layer inside industrial fiber lasers: isolators to 100 W in-line and 500 W free-space, pump & signal combiners, laser WDMs and hybrids — built to survive the back-reflection that kills lasers.

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The Challenge

Back-reflection is the No.1 killer of fiber lasers — and as cutting and welding systems climb into the multi-kW era, every passive in the optical path becomes a survival-critical part.

Back-Reflection Kills Lasers

Copper and aluminum reflect up to ~90% of 1 µm laser light at room temperature. In cutting and welding, that power travels straight back up the delivery fiber into the amplifier chain — and can burn out the seed and pump diodes in a single bad shot. An output isolator is not an accessory; isolation and power rating must scale together, or the laser dies.

Power Levels Keep Climbing

Industrial systems have moved from hundreds of watts to multi-kW cutting and welding, with laser cleaning and additive manufacturing pulling the same way. Every passive in the path now faces 100 W-class CW loads and 10 kW-class ns pulse peaks — and every absorbed watt becomes heat. Thermal design, not margin, now defines the component.

One Band Is Never Enough

Yb at 1030–1080 nm for cutting and welding, Er at 1550 nm for eye-safe systems, Tm at 1940/1950 nm for medical and plastics processing — each band needs its own magneto-optic and fiber design. Laser OEMs need a supplier who covers all three — and builds to a drawing where the catalog stops.

How We Fit In

Triple-Stone builds the high-power passive layer along the whole fiber-laser chain — from the seed line to the processing head. Here is what actually makes these devices hard, and how far our matrix goes.

Typical high-power Yb-doped fiber laser chain: seed source, isolator, pump and signal combiner, YDF gain stages with pump protectors, cladding power strippers, mode field adapter and a free-space high-power output isolator

A typical multi-stage Yb-doped fiber laser (MOPA) chain: seed → isolator → pump combiner → YDF gain stages → cladding power stripper → free-space output. Triple-Stone supplies the isolators, pump & signal combiner and laser WDMs along this chain — in-line to 100 W, fiber-to-free-space to 500 W.

Walking the chain: the seed passes an isolator into the first pump-and-signal combiner, and a short YDF stage lifts it to drive level. A second isolator protects the stage, and a 650/1064 nm WDM adds a red pilot beam on the same fiber for alignment. The main (N+1)×1 combiner then fuses multiple pump diodes — each behind a pump protector — into the power YDF. Downstream, a cladding power stripper sheds unabsorbed pump light, a mode-field adapter matches the delivery fiber, and a free-space high-power isolator closes the chain at the output window.

Stage-to-stage and output isolation. In a MOPA chain, any reflection from downstream travels back upstream with gain behind it. Our in-line isolators guard seed and pre-amp stages from 300 mW up to 100 W CW, on standard, PM or large-mode-area fiber. At the output, fiber-to-free-space isolators expand the beam to a collimated 7 mm output and hold ≥ 28–30 dB isolation at 60 / 120 / 250 / 500 W — the 500 W version is water-cooled, rated for 50 kW ns pulse peaks, and ships with a specified reverse-power handling for exactly the back-reflected shot it exists to stop. Two things make high-power isolation hard: the magneto-optic crystal has to stay aligned while kilowatts of heat move through it, and the isolator must survive the very reflection it exists to block — hence a 5 W continuous / 20 W short-duration reverse-power rating on the 500 W unit.

Pump and gain-chain passives. Our 50 W pump & signal combiner couples 976 nm pump light into the cladding of LMA double-clad fiber at ≥ 90% efficiency while passing the 1064 nm signal at ≤ 0.5 dB loss — fusing a 105/125 µm multimode pump port onto LMA gain fiber at that efficiency is taper-and-fuse work we run at production scale. Around it: fused PM couplers, polarization beam combiners/splitters, pump & signal WDMs, and high-power PM tap couplers to 100 W for in-line power monitoring.

Pulsed and high-power variants. Nanosecond-pulse versions are rated to 10 kW peak across the line — 50 kW on the 500 W free-space isolator, and 250 kW ps peak on the 1950 nm 100 W unit. High-power circulators cover 760–1940 nm, with LMA / PLMA large-mode-area fiber options to preserve beam quality at power.

Hybrid integration. Laser builders keep shrinking cavities, so we fold functions into one mini package: IWDM (isolator + WDM), WITP (WDM + isolator + tap or band-pass filter) and ITPD (isolator + tap + PD). Fewer splices, fewer failure points — one qualified part instead of three.

Honest about the chain. The cladding power stripper, the pump protectors and the mode-field adapter in the diagram are not our products — the laser builder sources those where they choose. Everything fiber-mated around them is: seed and stage isolators, the pump & signal combiner, laser WDMs and tap couplers, and the free-space output isolator — all qualified on the same LMA fiber types the rest of the chain runs on, from 10/125 up to 50/400 µm core.

Products for This Application

High-Power Isolators

The ace card: in-line isolators from 300 mW to 100 W (1064 / 1550 / 1940 nm), fiber-to-free-space output isolators to 500 W with water cooling — ns pulse peaks to 50 kW, reverse-power handling specified.

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Fiber-Laser Components by Wavelength

Pump & signal combiners, high-power PM tap couplers, PBC / PBS and laser WDMs — organized by working band: 1064, 1550 and 1940/1950 nm.

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High-Power Circulator & Laser WDM

High-power circulators across 760–1940 nm, plus fused, filter and high-power PM filter WDMs spanning 532–1950 nm for pump/signal management.

View details → Laser WDM →
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All products qualified to Telcordia GR-1221 / GR-1073 reliability programs.

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100 W in-line, 500 W free-space, ns pulses to 50 kW — and custom wavelengths, fibers and packages beyond the catalog. Samples ship worldwide.

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+86 137 0968 6019

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