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Power stability, linewidth, beam quality

MSL-FN-588588 nm yellow CW laser

588 nm

The MSL-FN-588 is a 588 nm continuous-wave solid-state laser. Light is amplified in a solid gain medium inside an optical resonator. The resonator feeds light back through that medium to build the laser beam. The pump arrangement and cooling determine how energy is supplied and waste heat is removed. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.

Specifications

MSL-FN-588

24 specification rows

Output / average power1~200 mW
Beam / notesLaser
Operating modeCW
Transverse modeTEM00
Longitudinal modeSingle
Spectral line width (nm)<1MHz
Noise of amplitude (rms, 20Hz-20MHz)<1%, <0.5%
Warm-up time (minutes)<5
Pointing stability over temperature (urad/°C)<8
Frequency shift (MHz) (over ±2°C and 8hrs) (optional)<±200
Operating temperature (°C)10-35
Power supply (100-240VAC)PSU-H-FDA
Expected lifetime (hours)>10000
Wavelength (nm)588±2
Power stability (rms, 4 hours ±3°C)<3%, <2%, <1%
Coherent length (m)>50
M²<1.2
Beam diameter at the aperture (1/e2, mm)<2.5
Beam divergence, full angle (mrad)<1.2
Polarization ratio>100:1, Horizontal (Vertical optional)
Pointing stability (urad) (over 2 hours after warm-up and ±3°C)<50
Frequency shift with temp (MHz/°C) (optional)<200
Beam height from base plate (mm)27.4
Laser head consumption (W)15 (typical), <25 (40°C)

What do you need?

Tell us the output power, beam quality and beam delivery you need, and we'll reply with the matching configuration and lead time.

Model selection

Nearby series comparison

Compare MSL-FN-588 with the closest available models in the CW Lasers family.

Selection parameterMSL-FN-588 (current)MSL-W-588MLL-U-588
Wavelength588 nm588 nm588 nm
Optical power / pulse energy1~200 mW200-500 mW1~200 mW
Operating mode / pulse widthCWCWCW
Beam quality<1.2<1.5<1.2