Brand: Edinburgh Instruments | Category: Nanotechnology

Picosecond pulsed diode lasers built for time-correlated single photon counting, supplied at fixed wavelengths from 375 nm to 980 nm. Each head includes a built-in spectral filter so no external filtering is needed, and the repetition rate is selectable from 2.5 kHz to 20 MHz. They plug directly into Edinburgh Instruments spectrometers.
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| Model (EPL-) | Nominal Wavelength (nm) | Max. Pulse Width @ 10 MHz (ps) | Typical Average Power @ 20 MHz (mW) |
|---|---|---|---|
| 375 | 375 | 85 | 0.15 |
| 405 | 405 | 75 | 0.11 |
| 445 | 445 | 95 | 0.15 |
| 450 | 450 | 120 | 0.18 |
| 475 | 475 | 90 | 0.15 |
| 485 | 485 | 120 | 0.10 |
| 510 | 510 | 150 | 0.13 |
| 635 | 635 | 85 | 0.07 |
| 655 | 655 | 85 | 0.15 |
| 670 | 670 | 80 | 0.15 |
| 785 | 785 | 85 | 0.12 |
| 800 | 800 | 110 | 0.15 |
| 980 | 975 | 80 | 0.14 |
Manufacturer catalogue checked 2026-09-29.
Each row identifies a separate wavelength model. Typical, maximum and minimum values and the stated repetition-rate conditions are retained in the column headings. Select the exact wavelength, optical output and trigger configuration against the complete current datasheet.
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Pulsed LED sources reaching into the deep ultraviolet from 250 nm, where diode lasers are not available, with sub-nanosecond pulse widths for lifetime measurement. The series runs from 250 nm to 610 nm and shares the housing, trigger interface and mounting of the EPL diode lasers.
Coherent pulse energy sensors measure pulse energies from 10 nJ to 15 J using pyroelectric detectors with large active areas and a high damage threshold. Semiconductor models measure up to 10 kHz, and meterless versions carry USB or RS-232 electronics in the cable.
Picosecond pulsed diode lasers offering higher repetition rate and higher average power than the EPL series, up to 80 MHz. The extra photon flux shortens acquisition on weakly emitting samples, and a high average power option is available on each wavelength.