Dual Head Laser (1)
For Particle Image Velocimetry (PIV) applications
All DS, DSH and DM Series Lasers can be combined as dual head lasers where the pulses can be fully overlapped to double the pulse energy or fully interleaved to double the prf.
Nd: YLF Laser (1)
For high pulse energy and KHz rep rates, we have built a large number of 1053nm, 527nm, 351nm and 211nm lasers for a various applications ranging from FPD repair to remote Raman detection systems.
DC UV SeriesNd: YLF Laser
4th Harmonic Laser (1)
All DS, DX, RX and SN Series lasers can be built as 4th harmonic lasers to provide outputs from 10mW to 6W @ 263nm or 266nm
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DS Series4th Harmonic Laser
Narrow Linewidth Ti:Sapphire Laser (1)
With only a 0.1cm-1 linewidth, power outputs up to 1.5W and wavelength tunability in the fundamental from 700nm to 960nm along with its harmonics for wavelengths as short as 193nm, we have built a large number of these lasers for applications ranging from radioactive ion beam (RIB) to resonance Raman spectroscopy at major Universities all over the world
Radioactive ion beam (RIB)
The Resonance Ionization Laser Ion Source (RILIS) is a powerful tool for efficient and selective production of radioactive ion beams at Isotope Separator On Line (ISOL) facilities. To avoid isobaric background, highly selective stepwise resonant ionization is applied, using up to three different laser wavelengths. Due to their advantages in terms of stability and reliability, an all solid-state titanium:sapphire (Ti:Sa) system is used at the majority of on-line facilities worldwide.
Tu Series TEM00 tunable Ti:Sapphire laser’s pulse width is perfectly matched to the lifetime of many fluorophores (i.e., ~10ns). With its Broad Tuning Range of ~700 to 900nm over the “Blood window”, High prf up to 10KHz and high average power of >1W, this makes the Tu laser a valuable tool for cell visualization and other novel biomed imaging applications, such as photoacoustics (PA).
OH Radical Concentration Measurement
Laser Induced Fluorescence (LIF)
CARS – freq domain spectroscopy with the narrower linewidths of our TU laser
Time Resolved Spectroscopy
Planar Laser Induced Fluorescence (PLIF) – with twin pulse mode
TU SeriesNarrow Linewidth Ti:Sapphire Laser
Optical Parametric Oscillator (OPO) Laser (1)
With our novel intracavity OPO technology, we have built a large number of these OPO lasers producing 1.5um to 3.4um outputs and power from 0.5W to 10W with pulse widths of ~10 to 15ns for applications such as eye safe illumination, defense range finding and biophotonic research.
Photonics Industries novel intracavity OPO Series ns lasers can also provide mJs of pulse energy pulsed at kHz rep rates at any fixed wavelength selectable from the following wavelength ranges:
- 3.4um to 2.2um
- 2um to 1.5um (e.g., 1.7um)
- 1um to 750nm
- 666nm to 255nm
all with a TEM00 spatial mode profile. Such lasers are applicable to medical techniques such as photoacoustic (PA) ultrasound medical imaging, photoacoustic tomography, 3D photoacoustic microscopy, UV surface excitation microscopy, laser surgery, etc.
OPOHigh Repetition Rate OPO Diode Pumped Laser
Single Longitudinal Mode (SLM) and Narrow Linewidth (NL) (1)
SLM and NL options are available for many of DS, DC series lasers mentioned above: SLM with linewidth <100MHz or narrow linewidth(NL) ~3GHz in the fundamental.
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SLM and NLSingle Longitudinal Mode (SLM) and Narrow Linewidth (NL)