Picosecond Pulsed Sources
Sub-nanosecond Pulsed LEDs
- Center wavelengths between 245 nm and 600 nm
- Pulse width down to 500 ps
- Adjustable (average) power up to 80 µW
- Repetition rate from single shot up to 40 MHz
- Optional bandpass filter
The pulsed LEDs of the PLS Series are the fastest miniature sub-nanosecond pulsed LED sources commercially available. They combine short pulse widths with high repetition rates in a compact and maintenance free set-up.
Direct emission in the ultraviolet
The LEDs of the PLS Series are the only available compact pulsed light sources that emit directly in the ultraviolet spectral range at wavelengths as short as 245 nm. Eleven different LEDs with central wavelengths between 245 nm and 340 nm allow to choose a peak wavelength according to the needs of the application. Their spectral and timing characteristics are also particularly suitable for biomedical applications, e.g., for the detection of labeled substances as well as naturally fluorescent amino acids like tryptophan or tyrosine.
Pulse widths down to 500 ps
All pulsed LEDs emit picosecond pulses with a full width at half maximum (FWHM) of less than one nanosecond – at some wavelengths even pulse widths down to 500 ps are possible. The pulse width itself cannot be controlled, but does depend on the selected power level of the LED.
Average power of several microwatts
All LED heads are designed to emit an about constant pulse energy at a given intensity setting. Doubling the repetition rate therefore effectively doubles the average output power. The achievable pulse energies of the LEDs in the visible spectrum can reach up to 2 pJ, which corresponds to average output powers up to 80 µW at 40 MHz repetition rate. For the UV LEDs the achievable pulse energy is lower and typically below 1 pJ. At their maximum repetition rate of 10 MHz, this corresponds to average output powers around 1 µW.
Spectral width down to 20 nm
The spectral emission profile of all pulsed LEDs is broader than for pulsed diode lasers. For the UV LEDs the spectral width is smaller than 20 nm, whereas for the LEDs in the visible it may be as large as 50 nm. A further reduction of the spectral width is possible by using suited bandpass filters.
Suitable for time-resolved fluorescence spectrometers
The most important difference between the pulsed LEDs and pulsed diode lasers is the fact that the emission of the LEDs is divergent, not coherent, not polarized and also non-uniform in its intensity distribution. Depending on the LED used, different beam shapes can be seen ranging from near-round to elliptical. Fiber coupling into single mode or multimode optical fibers has therefore only very low efficiency – a notable exception are large area fibers such as liquid light guides. However, for short range interactions, e.g., in a compact time-resolved fluorescence lifetime spectrometer the LEDs of the PLS Series are very useful excitation sources.
All functions of the PLS Series LED heads such as repetition rate and output power are controlled and adjusted by any driver of the PDL Series.
(a) PLS with max. repetition rate of 10 MHz
|Average Power @ 10 MHz|
|without filter||with colored glass filter||with bandpass filter*||Spectral width||Pulse width (typical)|
|PLS 245||245 nm||---||---||0.4 µW||< 30 nm||800 ps|
|PLS 255||255 nm||---||---||1 µW||< 20 nm||800 ps|
|PLS 265||265 nm||---||---||1 µW||< 20 nm||700 ps|
|PLS 270||275 nm||---||---||2 µW||< 20 nm||650 ps|
|PLS 280¹||285 nm||---||1 µW||2 µW||< 20 nm||900 ps|
|PLS 290¹||295 nm||---||1 µW||2 µW||< 20 nm||900 ps|
|PLS 300¹||305 nm||---||0.8 µW||1 µW||< 20 nm||600 ps|
|PLS 310¹||315 nm||---||1 µW||1.1 µW||< 20 nm||600 ps|
|PLS 320¹||325 nm||---||0.5 µW||0.8 µW||< 20 nm||700 ps|
|PLS 340²||345 nm||1 µW||---||---||< 20 nm||500 ps|
|PLS 575²||575 nm||3 µW||---||---||< 20 nm||< 1.3 ns|
Note: An internal security circuit prevents any damage if the these LEDs (PLS 245 to PLS 350 and PLS 575) are operated above 10 MHz.
(b) PLS with max. repetition rate of 40 MHz
|Average power @ 40 MHz||Spectral width (approx.)|
|without filter||with bandpass filter*||without filter||with bandpass filter*||Pulse width (typical)|
|PLS 370³||380 nm||---||8 µW||---||15 nm||600 ps|
|PLS 400²||400 nm||50 µW||---||20 nm||---||800 ps|
|PLS 450||460 nm||80 µW||40 µW||40 nm||30 nm||800 ps|
|PLS 500||500 nm||30 µW||13 µW||45 nm||35 nm||900 ps|
|PLS 600||600 nm||20 µW||12 µW||20 nm||18 nm||950 ps|
* Available as an option
¹ Supplied with a colored glass filter by default, a band-pass filter is available as an option for better performances
² The emission is spectrally clean, no additional filter needed
³ Always supplied with a bandpass filter
All PLS heads are supplied with an integrated lens.
|Length with collimator||66 mm|
|Length with lens and filter||80.5 mm|
All Information given here is reliable to our best knowledge. However, no responsibility is assumed for possible inaccuracies or omissions. Specifications and external appearances are subject to change without notice.
The sub-nanosecond pulsed LEDs of the PLS Series are ideal excitation sources in spectrometer systems that do not require high spatial resolutions. This includes applications such as:
- Time-Resolved Fluorescence
- Time-Resolved Photoluminescence (TRPL)
- Fluorescence Anisotropy (Polarization)
- Biochemical Analysis
- Detection of molecules labeled with Perylene, Coumarin, Fluorescein and Rhodamin dyes
- Detection of naturally fluorescent molecules like tyrosin, tryptophan (intrinisic protein fluorescence)
- Testing of optoelectronic devices such as pin-diodes and PMTs
The following documents are available for download:
Latest 10 publications referencing PLS Series
The following list is an extract of 10 recent publications from our bibliography that either bear reference or are releated to this product in some way. Do you miss your publication? If yes, we will be happy to include it in our bibliography. Please send an e-mail to firstname.lastname@example.org containing the appropriate citation. Thank you very much in advance for your kind co-operation.