The workhorse of time-of-flight. Two-pin plastic and metal TO56 emitters spanning 15 W to 600 W, in bare, fast-axis-collimated, lens-collimated and spatial-module form factors — including pin-to-pin drop-ins for the ams OSRAM SPLPL90 family already qualified in European rangefinder platforms.
- 15 W – 600 W peak power across 3, 4, 6 and 16 stripe designs
- Pin-to-pin compatible with ams OSRAM SPLPL90_3 (field-proven in volume production)
- Functional equivalents for ROHM RLD90QZW3 / RLD90QZW5 and OSRAM SPLTL90AT03 / SPLUL90AT08
- Low-temperature-drift 180 W part for airborne and long-range scanning
- 28° × 10° bare, 8° × 10° FAC, or 3° × 5° lens-collimated output
Configurations
Expand a group to see the model table. All powers are peak pulse power at 25 °C unless the table states otherwise.
Metal can, 3-pin (TO56)-M
Hermetically sealed TO56 with isolated three-pin header. The default choice for LiDAR modules and industrial rangefinders.
| Model | Peak power | Stripes | Emitting area (microns) | Fast axis | Slow axis | Reference / notes |
|---|---|---|---|---|---|---|
| PLD905-15W-M | 15 W | 3 | 40 × 10 | 28° | 10° | Robot vacuum obstacle-avoidance modules |
| PLD905-25W-M | 25 W | 3 | 70 × 10 | 28° | 10° | Equivalent to ROHM RLD90QZW5 |
| PLD905-30W-M | 30 W | 3 | 68 × 10 | — | — | Compact three-stripe emitter; fast and slow axis data on request |
| PLD905-40W-M | 40 W | 4 | 40 × 18 | 22° | 10° | LiDAR and laser rangefinding |
| PLD905-50W-M | 50 W | 3 | 150 × 10 | 28° | 10° | LiDAR and laser rangefinding |
| PLD905-55W-MB/Z-HC | 55 W | 5 | 60 × 18 | 22° | 10° | Five-stripe high-current variant, 1 – 50 ns pulse width |
| PLD905-70W-M | 70 W | 4 | 90 × 18 | 22° | 10° | Equivalent to ams OSRAM SPLTL90AT03 |
| PLD905AL-70W-M | 70 W | 4 | 90 × 18 | 22° | 10° | Low temperature drift (TC < 0.1 nm/°C), case at negative potential — airborne mapping |
| PLD905-75W-M | 75 W | 3 | 200 × 10 | 28° | 10° | Equivalent to ROHM RLD90QZW3 |
| PLD905-90W-M | 90 W | 4 | 110 × 18 | 22° | 10° | LiDAR and laser rangefinding |
| PLD905-100W-M | 100 W | 3 | 230 × 10 | 28° | 10° | Equivalents: OSRAM SPLUL90AT08, LASER COMPONENTS 905D1S3J09UA |
| PLD905-140W-M | 140 W | 4 | 220 × 18 | 22° | 10° | Long-range scanners |
| PLD905BL-180W-M | 180 W | 6 | 110 × 30 | 22° | 10° | Low temperature drift — airborne mapping and long-range LiDAR |
| PLD905-200W-M | 200 W | 6 | 230 × 240 | 38° | 12° | Equivalent to LASER COMPONENTS 905D2S3JT09X; large emitting area for wide-aperture receivers |
| PLD905-300W-M | 300 W | 9 | 220 × 360 | 40° | 12° | Three-chip vertical stack; equivalent to LASER COMPONENTS 905D3S3JT09X |
| PLD905-600W-MA | 600 W | 16 | 220 × 480 | 22° | 10° | Twelve-stripe stack, 55 A / 80 V drive — the highest-power emitter in the range |
Metal can, 2-pin (TO56)-MP
Two-pin metal header that replaces a plastic package without a footprint change, adding high-temperature solder capability.
| Model | Peak power | Stripes | Emitting area (microns) | Fast axis | Slow axis | Reference / notes |
|---|---|---|---|---|---|---|
| PLD905-15W-MP | 15 W | 3 | 40 × 10 | 28° | 10° | Drop-in for plastic two-pin, high-temperature soldering |
| PLD905-25W-MP | 25 W | 3 | 70 × 10 | 28° | 10° | Drop-in for plastic two-pin |
| PLD905-40W-MP | 40 W | 4 | 40 × 18 | 22° | 10° | Drop-in for plastic two-pin |
| PLD905-50W-MP | 50 W | 3 | 150 × 10 | 28° | 10° | Drop-in for plastic two-pin |
| PLD905-70W-MP | 70 W | 4 | 90 × 18 | 22° | 10° | Drop-in for plastic two-pin |
| PLD905-75W-MP | 75 W | 3 | 200 × 10 | 28° | 10° | Drop-in for plastic two-pin |
| PLD905-90W-MP | 90 W | 4 | 110 × 18 | 22° | 10° | Drop-in for plastic two-pin |
| PLD905-100W-MP | 100 W | 3 | 230 × 10 | 28° | 10° | Drop-in for plastic two-pin |
| PLD905-140W-MP | 140 W | 4 | 220 × 18 | 22° | 10° | Drop-in for plastic two-pin |
| PLD905BL-180W-MP | 180 W | 6 | 110 × 30 | 22° | 10° | Low temperature drift, two-pin metal |
Fast-axis collimated (FAC)-MCL
Cylindrical fast-axis collimating lens integrated in the can. Cuts the fast-axis divergence from 22–28° to 6–8°, which simplifies the receive optics and improves range resolution.
| Model | Peak power | Stripes | Emitting area (microns) | Fast axis | Slow axis | Notes |
|---|---|---|---|---|---|---|
| PLD905-25W-MCL | 25 W | 3 | 70 × 10 | 8° | 10° | FAC barrel; other wavelengths quoted on request |
| PLD905-40W-MCL | 40 W | 4 | 40 × 18 | 6° | 10° | FAC barrel |
| PLD905-50W-MCL | 50 W | 3 | 150 × 10 | 8° | 10° | FAC barrel |
| PLD905-55W-MCL | 55 W | 5 | 60 × 18 | 22° | 10° | Five-stripe FAC variant of the 55 W emitter |
| PLD905-70W-MCL | 70 W | 4 | 90 × 18 | 6° | 10° | FAC barrel |
| PLD905-75W-MCL | 75 W | 3 | 200 × 10 | 8° | 10° | FAC barrel |
| PLD905-90W-MCL | 90 W | 4 | 110 × 18 | 6° | 10° | FAC barrel |
| PLD905-100W-MCL | 100 W | 3 | 230 × 10 | 8° | 10° | FAC barrel |
| PLD905-140W-MCL | 140 W | 4 | 220 × 18 | 6° | 10° | FAC barrel |
| PLD905BL-180W-MCL | 180 W | 6 | 110 × 30 | 8° | 10° | Low temperature drift with FAC |
Collimating pin (MZ) — isolated header-MZ
Same emitter as the -M parts, with a collimating pin and a header that is not electrically live. Because the case carries no potential, the diode can be mounted straight onto a metal housing without an insulating pad — which removes a thermal interface from the stack.
| Model | Peak power | Stripes | Emitting area (microns) | Fast axis | Slow axis | Notes |
|---|---|---|---|---|---|---|
| PLD905-40W-MZ | 40 W | 4 | 40 × 18 | — | — | Collimating pin, isolated header; 1 – 50 ns pulse width |
| PLD905-70W-MZ | 70 W | 4 | 90 × 18 | — | — | Collimating pin, isolated header |
| PLD905-90W-MZ | 90 W | 4 | 110 × 18 | 26° | 10° | Collimating pin, isolated header |
| PLD905-140W-MZ | 140 W | 4 | 220 × 18 | — | — | Collimating pin, isolated header; 1 – 50 ns pulse width |
| PLD905BL-180W-MZ | 180 W | 6 | 110 × 30 | — | — | Six-stripe low-drift emitter, collimating pin, isolated header |
Lens collimated (aspheric) — confirmed at enquiry-MZS / -MSAvailability on enquiry
Aspheric collimating lens giving a 3° × 5° beam at a lower cost than a FAC stack — the tightest beam we have shipped in a standard TO56 can. These configurations sit outside the current price list, so stock and tooling status is confirmed at enquiry: tell us the peak power and the beam you need and we will come back with availability and a lead time.
| Model | Peak power | Stripes | Emitting area (microns) | Fast axis | Slow axis | Notes |
|---|---|---|---|---|---|---|
| PLD905-70W-MZS | 70 W | 4 | 90 × 18 | 3° | 5° | Aspheric lens, small divergence, cost optimised |
| PLD905-75W-MS | 75 W | 3 | 200 × 10 | 3° | 5° | Aspheric lens |
| PLD905-90W-MZS | 90 W | 4 | 110 × 18 | 3° | 5° | Aspheric lens |
| PLD905-100W-MS | 100 W | 3 | 230 × 10 | 3° | 5° | Aspheric lens |
| PLD905-140W-MZS | 140 W | 4 | 220 × 18 | 3° | 5° | Aspheric lens |
| PLD905BL-180W-MZS | 180 W | 6 | 220 × 18 | 3° | 5° | Aspheric lens, low temperature drift |
Plastic package, 2-pin-P
Cost-optimised plastic package with silver lead frame — the format used in every handheld rangefinder and golf laser on the market.
| Model | Peak power | Stripes | Emitting area (microns) | Fast axis | Slow axis | Reference |
|---|---|---|---|---|---|---|
| PLD905-15W-P | 15 W | 3 | 40 × 10 | 28° | 10° | — |
| PLD905-25W-P | 25 W | 3 | 70 × 10 | 28° | 10° | Equivalent to ams OSRAM SPLPL90 (silver lead frame) |
| PLD905-50W-P | 50 W | 3 | 150 × 10 | 28° | 10° | — |
| PLD905-75W-P | 75 W | 3 | 200 × 10 | 28° | 10° | Equivalent to ams OSRAM SPLPL90_3 (silver lead frame) — field proven |
| PLD905-90W-P(银) | 90 W | 4 | 110 × 18 | — | — | Silver lead frame |
Product views
Typical applications
Where this family is usually designed in:
Send us the specification you need to hit.
Wavelength, peak power, package and annual volume is usually enough for us to quote — and to say whether a sample is available from stock.