DPSS Lasers for Research & Life Sciences

261 nm – 1064 nm · TEM₀₀ Beam Quality · Ultra-Low Noise · 14 Wavelengths

AIMPICO's diode-pumped solid-state (DPSS) lasers complement our diode laser lineup by providing access to wavelengths and performance characteristics that direct diode lasers alone cannot achieve. By using a diode laser to pump a solid-state gain medium — typically a crystal such as Nd:YAG or Nd:YVO₄ — and then frequency-converting the output, DPSS lasers produce highly stable, low-noise beams at wavelengths from the deep UV through the near-infrared that are critical for scientific and life science applications.

How DPSS Lasers Work

In a DPSS laser, a semiconductor diode laser (usually emitting at 808 nm) pumps energy into a laser crystal. The crystal amplifies light at its characteristic wavelength — for example, 1064 nm for Nd:YAG. That infrared beam is then passed through a nonlinear crystal that converts it to a shorter, visible wavelength through frequency doubling (second harmonic generation) or sum-frequency mixing.

This multi-stage architecture gives DPSS lasers several advantages over direct diode emission:

Superior Beam Quality

DPSS lasers naturally produce a TEM₀₀ Gaussian beam with near-perfect spatial coherence — ideal for confocal microscopy and other applications requiring a diffraction-limited focus.

Excellent Noise Performance

Well-designed DPSS cavities deliver extremely low RMS noise (typically <0.5%), essential for quantitative fluorescence measurements where signal-to-noise ratio directly impacts data quality.

Wavelength Accessibility

Through frequency doubling, tripling, and quadrupling, DPSS lasers reach wavelengths across a broad range — from deep UV at 261 nm to the 1064 nm fundamental — covering lines where high-quality direct diode sources are limited or unavailable.

Available Wavelengths

WavelengthGeneration MethodCommon Applications
261 nmFifth-harmonic generationDeep UV spectroscopy, photochemistry, semiconductor inspection
266 nmFourth-harmonic of 1064 nmDeep UV fluorescence, material inspection, micromachining
320 nmHarmonic generationUV curing, UV Raman spectroscopy
349 nmThird-harmonic generationUV fluorescence excitation, micro-processing
355 nmThird-harmonic of 1064 nmUV Raman, micromachining, UV-excited fluorescence
360 nmHarmonic generationUV fluorescence, photobiology
457 nmFrequency-doubled / intracavityCFP excitation, forensics, display
473 nmFrequency-doubled Nd:YAGOptogenetics (ChR2), blue laser displays, holography
532 nmFrequency-doubled Nd:YAG / Nd:YVO₄GFP, YFP, Raman spectroscopy, holography, alignment
561 nmFrequency-doubled Nd:YAGmCherry, tdTomato, PE, RFP, confocal microscopy
589 nmSum-frequency or Raman-shiftedSodium D-line spectroscopy, guide star, yellow laser displays
1030 nmYb-doped gain mediumNIR imaging, materials processing, optical sensing
1064 nmNd:YAG / Nd:YVO₄ fundamentalOptical trapping, NIR imaging, LIDAR, materials processing

Contact our applications team to discuss wavelength selection, power levels, and beam specifications for your application.

Applications

Confocal Microscopy
TEM₀₀ output focuses to a tight, diffraction-limited spot for high-resolution optical sectioning
Flow Cytometry
Stable, low-noise excitation for consistent fluorescence signal detection across large cell populations
Optogenetics
473 nm for ChR2 activation, 561 nm for inhibitory opsins
Super-Resolution Imaging
Clean beam profiles for SIM and STED microscopy techniques
TIRF Microscopy
Precise beam pointing and low noise enable single-molecule imaging near the coverslip surface
Raman Spectroscopy
532 nm excitation for high signal-to-noise Raman measurements
Holography
532 nm and 473 nm for holographic recording and display
UV Processing
Deep UV lines (261–360 nm) for micromachining, inspection, and photochemistry
Calcium Imaging
Reliable excitation of calcium indicators for real-time monitoring of neural activity
Laser Displays
Visible DPSS lines (473 nm, 532 nm, 589 nm) for vivid colour production

DPSS vs. Direct Diode: Choosing the Right Source

Choose a Diode Laser when…

  • You need fast modulation (microsecond switching)
  • The most compact form factor is required
  • Your target wavelength is directly available from a diode (e.g. 405 nm, 488 nm, 635 nm)
Learn about Diode Lasers →

Choose a DPSS Laser when…

  • You need the highest beam quality at green or yellow-green wavelengths
  • The lowest possible intensity noise is required for quantitative measurements
  • A perfectly Gaussian beam is needed for diffraction-limited focusing
Talk to an applications engineer →

In many multi-laser systems — such as flow cytometers or multi-channel microscopes — a combination of both diode and DPSS sources provides the best overall performance.

Engineering for Reliability

DPSS lasers require careful thermal management to maintain stable output. AIMPICO addresses this with precision temperature control of both the pump diode and the laser crystal, ensuring consistent wavelength and power output even in variable laboratory environments. Our DPSS lasers are designed for continuous operation and are backed by comprehensive performance specifications and warranty support.

Ready to Get Started?

Whether you're specifying lasers for a new instrument platform or upgrading an existing system, AIMPICO's DPSS lasers deliver the beam quality and stability your research demands.