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:
Not sure which configuration?
Peak power, package, beam divergence, drive conditions and temperature drift — the five decisions that pick the right 905 nm emitter are laid out in our 905 nm selection guide.
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.