Picosecond
one trillionth of a second.
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*Picosecond Lasers
A revolutionary laser technology due to its much shortened pulse duration of just 1012 seconds.
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Picosecond Laser
SIRIUS
SIRIUS is a compact, high energy hybrid ultrafast laser which produces <10 ps pulse duration with energy exceeding 60 µJ and > 5 W of average power.
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Picosecond-Diode Lasers for Spectroscopy
Designed and manufactured by Becker & Hickl – bh delivers prominent picosecond diode lasers with wavelengths from the NUV to the NIR. All bh pulsed diode lasers work with simple +12V power supply or pull their power from the USB port of a PC or Notebook Computer. Other features are high repetition rate, short pulse width, unprecedented timing and power stability, and extremely low electrical noise level.
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Differential Picosecond Pulse Generators
PicoSource PG900 Series
The fast-transition pulse can stimulate a transmission path, device or network with a broad spectrum signal in a single instant. Such a pulse is very useful for many of the high-speed broadband measurements that we need to make; for instance in time-domain reflectometry, semiconductor test, gigabit interconnect and port test and in radar.
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12-Channel VME Picosecond Resolution Time-Interval Measurement Module
V660
The V660 is a 12-channel time-to-digital converter used to record the time of occurrence of twelve independent electrical pulse inputs, each independently timestamped and buffered in FIFO memory.
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Turn Key Laser and LED Sources with Picosecond Pulse and Repetition Rate up to 100 MHz
DeltaDiode
DeltaDiodes utilize laser diode and LED technology to generate short optical pulses over a very wide range of repetition rates and wavelengths. Optical pulses as short as 50ps can be generated at repetition rates up to 100MHz.
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Picosecond Lasers
PL2250 Series
Featuring up to 100 mJ pulse energy and less than 30 ps (20 ps optional) pulse duration, PL2250 series picosecond mode-locked Nd:YAG lasers set new standard in high pulse energy picosecond lasers. Innovative and cost effective design allows to improve laser reliability, while reducing running and maintenance costs.
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Picosecond Laser
ANTARES
ANTARES is an advanced picosecond laser producing high average power at high repetition rates up to 80 MHz with narrow linewidth in a very compact and robust format.
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Picosecond Lasers
High single pulse energy: over 100 μJ@100kHzTotal pulse controlBurst modeVariable rep rate: single shot to 2MHzOption to 8MHzPEC: power or pulse energy controlPulse width <15ps, optional 20-100psZero leakageExcellent beam quality (M²<1.3)Exceptional beam pointing stabilityCompact industrial grade ps laserLow maintenance
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Photon Counting Detector - Single Photon Detection with Picosecond Accuracy
PPD
The PPD Series is a range of miniaturized single-photon counting detectors containing all the electronics necessary to detect single photons with picosecond accuracy.
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PCI Express A/d Board
AD14-500x4-IRIG
The AD14-500x4-IRIG is a high performance wideband 4-channel 14-bit data single PCIe Gen3 board, that can continuously digitize four wideband signals, with four high linearity A/Ds. A second board version AD14-500x4-K7US-IRIG-B has all of the above features and can additionally be synchronized with stability of better than +/- 100 picoseconds with respect to an IRIG-B 1PPS signal and global time codes from a satellite receiver or local site time reference, allowing simultaneous synchronized acquisition of data at multiple locations anywhere in the world.
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Pulsed Lasers and LEDs
PicoQuant's compact and reliable turn-key diode laser solutions work in picosecond pulsed, modulated, or fast-switched (nsec to µsec) operation mode. The laser systems typically consist of a common driver unit and exchangeable heads. Specialized lasers are also available as stand-alone units.
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Picosecond Laser
PIXEA
The PIXEA is a high-quality laser system for OEM and R&D applications generating ultra-short optical pulses by using gain-switched laser diode technologies. The laser features high-quality picosecond laser pulses with no satellite pulses and minimize pulse tail. The PIXEA series offer a large variety of centered wavelengths between 375 nm and 2 um. The pulse duration down to 20 ps is optimized for each wavelength. The system is based in two modules or one module, the laser head and the dedicated Control Unit including the GUI software. Different optical output options are available, including free space collimating optics and fiber coupled.
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PXI FlexRIO IF Transceiver
The PXI FlexRIO IF Transceiver combines analog I/O and a user-programmable FPGA into a single, customizable instrument. The instrument enables direct RF acquisition up to 6 GHz. You can use the instrument in a dual-channel mode at 3.2 GS/s or in a single-channel interleaved mode at 6.4 GS/s. The PXI FlexRIO IF Transceiver uses FPGAs from Xilinx alongside LabVIEW and Vivado programming options for custom algorithm implementation and real-time signal processing. Using this instrument with NI-TClk, you can synchronize modules in one or more PXI chassis at up to picosecond‐level accuracy for high‐channel‐count applications.
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Chromatic Dispersion Emulator
CS-CDE
The ClearSpectrum™-CDE is a chromatic dispersion emulator suited for test and measurement. This 1U half 19-inch rack-mountable module is designed to emulate tens of thousands of picoseconds per nanometer in a compact unit while maintaining very low insertion loss. It is a passive, ready-to-use emulator which can be cascaded several times to achieve higher levels of dispersion.
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Fluorescence Spectrometers
PicoQuant offers several fluorescence spectrometers that range from compact table-top spectrometers for teaching or daily routine work to modular high-end spectrometers with exact timing down to a few picoseconds. Samples can be liquids in standard cuvettes, solid samples or even semiconductor wafers for in-line quality control.
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Picosecond Lasers
PL2230 Series
The first commercial fully diode pumped high pulse energy mode-locked laser, producing 28 ps pulses with up to 140 mJ pulse energy.
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Test Instrument
Is a programmable laser that produces picosecond pulses with pulse generator integrated. It functions as a seed pulse generator for Master Oscillator Power Amplifiers (MOPA).
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Lasers for Micromachining
fs/ps
With thousands of femtosecond and picosecond lasers deployed in demanding manufacturing applications, Spectra-Physics delivers highest reliability for dependable multi-year operation to advance micromachining production applications.
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TCSPC Lifetime Fluorometer
DeltaPro
The DeltaPro has taken the complexity of time correlated single photon counting (TCSPC) and made it simple and affordable. Any lab can exploit the power of fluorescence dynamics using TCSPC. This system enables the seamless measurement of luminescence lifetimes from picoseconds to 1 second, using our DeltaHub timing electronics.
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Pulse Characterization Sensors
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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Hybrid Picosecond Photon Detectors
HPPD Series
technology.The HPPD is our latest development in TCSPC detector technology that combines the benefits of conventional PMT design (wide spectral response and large active area)with the advantages of solid state APD technology (good detection efficiency, negligible after-pulsing and exceptional temporal resolution). Hybrid detectors are becoming thefirst choice for FLIM and short lifetime determination.
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OEM, Embedded, and Custom Electronics
Picosecond timingPrecision analog and mixed signal processingDigital delay and pulse generationHigh speed photonics and fiberoptic timing distributionAerospace instrumentation and simulation
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Autocorrelator: 10fs-100ps, Any Repetition Rate
UVisIR'sreal-time long scanning autocorrelator measures laser pulses from femtosecond to picosecond. It is easy-to-use, real-time, dispersion-free, high-sensitivity and background-free! Long scanning range: 10fs-100ps. Real-time, dispersion-free and background-free scanning. High sensitivity: High-voltage(-1000VDC) PMT embeded! (Diode version is also available!). Broadband wavelength range: 500-1700nm.
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Tunable, Ultrafast TI: Sapphire Laser
SPRITE XT
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.
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AXIe High-Speed Digitizer/DAQ, 10-bit, 10 GS/s, DC to 2.5 GHz BW
M9710A
Based on the AXIe standard, the M9710A is a unique 10-bit high-speed digitizer, capturing signals from DC up to 2.5 GHz at 5 GS/s. It provides excellent measurement accuracy and high dynamic range across four phase-coherent channels within a single card. Optimized response allows few hundred picoseconds pulse analysis. Moreover, an interleaving option allows acquisition at 10 GS/s on two combined channels, keeping excellent measurement fidelity.
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SFG Spectrometer
Ideal laser spectroscopy tool for in-situ investigation of surfaces and interfaces. SFG spectrometer operates from 4300 to 625 cm-1 and provides < 6 cm-1 spectral resolution. The heart of the system is a picosecond Nd:YAG laser generating 25 ps pulses that pump an OPG/DFG delivering from 260 to 20 µJ per pulse across the IR range
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Autocorrelators
Opticala Autocorrelators are devices for measuring the intensity or field autocorrelation function of light, mostly used for determining the pulse width of picosecond or femtosecond pulses, to which an electronic apparatus such as oscillascope would be too slow. The basic principle of operation of an autocorrelator for a pulse width measurement is to check the correlation of the temporal pulse trace with itself.
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OEM Femtosecond/Picosecond Laser and Amplifier Modules
They provide output wavelength options at 780 nm, 925 nm, 1030 nm, 1064 nm and 1550 nm and can be used as stand-alone systems with a user-provided 5 V DC power supply or integrated into higher power laser platforms. The high quality ultrafast pulse streams are perfect seed sources for chirped pulse amplifier systems used in diverse applications, such as high precision microelectronics micromachining, laser eye surgery and nonlinear spectroscopy.
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Harmonic Generators
Our harmonic Generators include Doubler, Tripler, and Quadrupler for doubling, tripling, and quadrupling laser frequency in the wavelength range 680-1300nm. The second harmonic, third harmonic, and fourth harmonic generation up-convert the laser frequency to a wavelength range 190-650nm. These harmonic generators greatly expanded the application of wavelength range for femtosecond and picosecond lasers available for both amplifiers and oscillators.
