Lidar
PS-M-590: Lidar depends on how optical energy is delivered to the target; 590 nm emission governs absorption, while pulse energy, duration and repetition rate governs peak intensity and heat deposition.
Pulse energy, repetition rate, pulse width
PS-M-590 is a 590 nm Pulsed laser. Used for lidar, laser spectroscopy, sensing, metrology. Picosecond Pulsed Yellow Laser. Key specifications: output / average power 1~600 mW, operating mode Passively Q-switched, rep. rate (khz) 500-1000. View specifications, datasheet and enquiry options from Precisometer.
Specifications
12 specification rows
| Wavelength | 590 nm |
|---|---|
| Output / average power | 1~600 mW |
| Beam / notes | Picosecond Pulsed Yellow Laser |
| Operating mode | Passively Q-switched |
| Rep. rate (kHz) | 500-1000 |
| Power stability (rms, over 4 hours) | <3%, (<2% optional) |
| Beam divergence, full angle (mrad) | <1 |
| Beam diameter at the aperture (1/e2,mm) | ~3.0 |
| Beam height from base plate (mm) | 116 |
| Cooled method | Water cooled |
| Operating temperature (℃) | 15~35 |
| Power supply (220/110VAC) | On request |
| Expected lifetime (hours) | 10000 |
Application context
Typical uses for this laser type, with the selection logic tied to the model record.
PS-M-590: Lidar depends on how optical energy is delivered to the target; 590 nm emission governs absorption, while pulse energy, duration and repetition rate governs peak intensity and heat deposition.
PS-M-590: 590 nm emission sets the excitation and detector-band choice for Laser spectroscopy; linewidth and wavelength stability determine how cleanly weak spectral features can be separated from the laser line. The listed beam characteristic (<1) also controls focusing and collection geometry.
PS-M-590: 590 nm emission determines compatible optics, coatings and detectors for Sensing. The catalogued beam parameter (<1) helps predict how the source will focus and propagate through the instrument.
PS-M-590: 590 nm emission determines compatible optics, coatings and detectors for Metrology. The catalogued beam parameter (<1) helps predict how the source will focus and propagate through the instrument.
System integration
Use these checks to connect PS-M-590 to the surrounding optical, mechanical and control system. Every value shown is taken from this model's own specification record.
Technical FAQ
Cooled method: Water cooled · Operating temperature (℃): 15~35. Provide the stated cooling method and keep the laser-head base thermally coupled; temperature drift moves wavelength, output power and beam pointing.
Beam divergence, full angle (mrad): <1 · Beam diameter at the aperture (1/e2,mm): ~3.0. Size the downstream optics from the stated beam diameter and divergence rather than from the aperture of the housing, and confirm the polarisation state before specifying isolators or polarising optics.
Share wavelength, operating mode, output power or pulse energy, linewidth or pulse width, delivery, control, and safety requirements and we will qualify the matching configuration and lead time.
Model selection
Compare PS-M-590 with the closest available models in the Pulsed Lasers family. Confirm option-dependent values on the final configuration before ordering.
| Selection parameter | PS-M-590 (current) | PS-L-590 | LGS-589.159-PS |
|---|---|---|---|
| Wavelength | 590 nm | 590 nm | 589.159 nm |
| Optical power / pulse energy | 1~600 mW | 1~100 mW | 1-25 W |
| Operating mode / pulse width | Passively Q-switched | <500 | Mode-locked |
| Beam quality | <1 | Confirm for this model | <1.5 |
Compare the PS-M-590 with nearby pulsed lasers across the wavelength range.
Choosing a laser
Which specifications decide the experiment, and which ones cost money without changing the result.
PhotonicsLinewidth, spectral width, RIN, M², and coherence length answer five different questions. Translate each into the units your experiment is designed in — and learn which ones not to pay for.
Open guide
Photoacoustic imagingConnect optical absorption to wavelength, pulse fluence, stress confinement, acoustic bandwidth, repetition rate, and synchronization at the sample.
Open guide
Ultrafast spectroscopyDesign the pump, probe, delay line, monochromator, visible or SWIR camera, synchronization, and transient-signal budget as one experiment.
Open guide