Ultrafast Laser Amplifier
Ultrafast Laser Oscillators
Ultrafast Laser Oscillators
Ultrafast oscillators designed to meet a wide range of applications and user requirements, from multi-photon excitation microscopy to time-resolved TeraHertz studies
All Our Ultrafast Laser Oscillators
Chameleon lasers feature the widest tuning range and highest power at any wavelength, expanding the frontiers of Multiphoton Excitation (MPE) microscopy and non-linear optical studies.
HASS-certified for quality and reliability. Addressing the most demanding requirements in two-photon imaging and spectroscopy by delivering industry leading power levels and tunablity. Deepest excitation of all fluorescent probes & label-free modalities. Phase-locked second beam and octave spanning (660 to 1320 nm) tuning range benefit Raman techniques and ultra-fast spectroscopy applications.
Broadly tunable femtosecond and picosecond Ti:Sapphire laser systems for simplicity and flexibility in a well-proven design that delivers a powerful, versatile ultrafast source. Market leader in flexible fs/ps lasers, Mira includes Ultra-Wave optics to enable 690 - 1050 nm tuning with a single optics set. The unique Optima™ control and diagnostics package greatly simplifies daily operation and its patented ß-lock feature provides skip-free ps wavelength tuning
The first femtosecond laser designed for instrumentation and OEM integration, 920 nm and 1064 nm Axon lasers are priced at breakthrough cost to grow applications such as two-photon microscopy, harmonic generation microscopy, and inspection
Powerful fiber lasers delivering up to 18 watt of average power at 1040 and 1070 nm with 140 fs and 55 fs pulses, respectively. Ideal for optogenetics, Two-Photon Polymerization studies, its built-in precompensation ensures optimum pulse duration also with complex microscope set-ups.
Microscopy and Spectroscopy with a Tunable Two-Color Source CARS and SRS microscopy have migrated from physics labs to life-science labs, so APE has responded withan easy-to-use and truly hands-off light source: picoEmerald. In a single-box, picoEmerald provides fully automated temporal- and spatial-overlapping ultra-short pulse trains: 1032 nm from the laser oscillator, plus the OPO Signal beam, and OPO Idler beam. Application: CARS & SRS microscopy, Quantum dots: excitation for single photons and entangled photons
Powerful fiber lasers delivering up to 18 watt of average power at 1040 and 1070 nm with 140 fs and 55 fs pulses, respectively. Ideal for optogenetics, Two-Photon Polymerization studies, its built-in precompensation ensures optimum pulse duration also with complex microscope set-ups.
Continuously expanding series of harmonic generators, many different optical parametric oscillator configurations, pulse pickers, cavity dumpers, compressors, active pulse shaping, laser pulse and CEP stabilization.
NIR / IR OPO pumped at ~0.5 µm or ~ 1 µm. Femtosecond as well as picosecond version for various spectroscopy applications.
Pulse Picker
Changing the repetition rates Single Shot … ~40 MHz
Useful for lifetime measurements (FLIM, TCSPC, …)
Spectral Slicer
Narrows spectral bandwidth of broadband (fs) or narrowband (ps) laser, for various wavelength ranges and minimal bandwidth available
Application: Quantum dots: excitation for single photons and entangled photons
Dispersion compression and management – having shorter pulses on sample site
Application: Microscopy 2 Photon or 3 Photon
Cross sale possibility with Carpe (Microscopy autocorrelator, measure pulse width at laser exit and at sample site)
The CPC-II pule compressor accessory for Vitara is designed to deliver near transform-limited pulses at the target sample. The CPC-II achieves this by introducing continuously variable negative Group
Delay Dispersion (GDD/prechirp) to precisely compensate for normal dispersion of downstream optics
CPC 1040 is a pulse compressor for the 1040 nm output
from the Chameleon Discovery. It will ensure highest peak
power is delivered directly to the sample plane.
CPC 1040 incorporates negative dispersion mirrors that
add a stepwise, variable amount of Group Dispersion Delay
(GDD/pre-chirp) to the laser pulses.
The Synchrolock-AP is used to accurately synchronize two Mira or Vitara lasers together, or to synchronize a Mira or Vitara laser to an external RF source. Operating in the femtosecond or picosecond (Mira only) regime,
the Synchrolock-AP allows smooth wavelength tuning while keeping thelasers synchronized.
