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Picosecond

one trillionth of a second.


Showing results: 46 - 48 of 48 items found.

  • Tunable, Ultrafast TI: Sapphire Laser

    SPRITE XT - M Squared Lasers

    Sprite XT is a flexible ultrafast, femtosecond laser source. It delivers stability, reliability and productivity and is equally at home in the lab or as part of an OEM application. Choose your output power (up to multi-Watts), pulse width (femtosecond or picosecond models), wavelength range (fixed wavelength or tunable), and pulse repetition rate (<80 MHz to multi-GHz). All Sprite models are designed for alignment-free and maintenance-free operation and can be controlled from a web browser. It’s ideal for multi-photon excitation (MPE) and FLIM, quantum optics, time resolved spectroscopy, nonlinear optics, pump-probe experiments, microscopy, amplifier seeding, and electro-optic sampling.

  • Photoluminescence Spectrometer

    FLS1000 - Edinburgh Instruments Ltd

    The FLS1000 sets the standard in both steady state and time-resolved photoluminescence spectroscopy for both fundamental research and routine laboratory applications. The system is a modular fluorescence and phosphorescence spectrometer for measuring spectra from the ultraviolet to the mid-infrared spectral range (up to 5,500 nm), and lifetimes spanning from picoseconds to seconds. All of this can be achieved through various upgrade routes, either at the time of order or in the future. Whether you are studying photophysics, photochemistry, biophysics, biochemistry, material or life sciences, the FLS1000 will enable you to reliably and accurately measure luminescence spectra and kinetics using state-of-the-art sources, detectors, acquisition techniques, quality optics and precision mechanics. The large sample chamber will house practically any type of sample accessory.

  • *Pulse Characterization Sensors

    mks Ophir

    Pulse Characterization Sensors provide the ability to see and measure the temporal characteristics of pulsed and CW laser beams. Ophir Fast Photodiode Detectors are designed to convert optical signals into electrical signals which are then measured with third-party instrumentation such as oscilloscopes and spectrum analyzers. Accessories are available to connect to IS6 integrating spheres or fiber optic cables. Attenuating filter accessories are also available to increase their dynamic range. Different models offer silicon, UV enhanced silicon and InGaAs PIN photodiodes, covering a combined spectral range of 193 nm to 1700 nm. Rise times range from 25 picoseconds to 3 nanoseconds. The fast rise times are achieved by an internal reverse bias voltage circuit. Power is supplied by internal batteries and/or an external power supply depending on the model. Detectors should be connected to a 50Ω impedance in order to maintain their nominal rise times. They can be connected to higher impedance loads, but this will result in a significant increase in the rise time. If higher output voltage is required, it is recommended to connect the detector to a trans-impedance amplifier with an Input impedance of 50Ω

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