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Picosecond
one trillionth of a second.
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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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Pulse & Delay Generators
The benchtop pulse generators feature a fast risetime and low jitter. Our most popular digital delay pulse series 575 and 577 generators are now available with selectable time references. With up to eight channels of delay and width control, each individual channel's reference can be set either to the trigger or to any other channel. So look below if you require a picosecond pulse generator or nanosecond pulse generator for your application.
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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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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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Fluorescence Microscopes
PicoQuant offers different solutions for time-resolved confocal microscopy. The available systems include single molecule sensitive microscopes with picosecond temporal resolution and super-resolution imaging capabilities as well as upgrade kits for laser scanning microscopes of all major manufacturers that enable time-resolved applications.
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Photoluminescence Spectrometer
FLS1000
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.
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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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High Energy Laser Systems
APL2100 Series
APL2100 series amplifiers are designed to produce up to 1000 mJ picosecond pulses. High pulse energy, excellent pulseto- pulse energy stability, superior beam quality makes APL2100 series picosecond amplifiers well suited for applications like OPCPA pumping, non-linear optics and others.
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Industrial Short-Pulse Lasers
Short-pulsed industrial lasers from nanosecond lasers with up to 1 Joule pulse energy, through picosecond lasers with up to 80 MHz repetition rates, to femtosecond lasers with up to 900 fs pulse widths.
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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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Time to Amplitude Converters and Calibrator
A Time-to-Amplitude Converter (TAC) can achieve exceptional precision by using an analog technique to convert small time intervals to pulse amplitudes. When a timing application demands picosecond precision, a time-to-amplitude converter is a prime candidate. A time-to-amplitude converter is a productive solution for measurements less than 10 μs when time resolutions from 10 ps to 50 ns are required.
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Ultrafast Laser Pulse Measurement
FROG Scan
Our FROG Scan system is versatile, adaptable and easy to use. With our FROG Scan, you can tweak a laser system or measure highly chirped pulses to calculate the amount of dispersion compensation you might need for recompression. Measure a short pulse that has been chirped out to several picoseconds, or measure pulses as short as 12 fs in real-time.
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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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KATANA & PILAS Pulsed Diode Lasers
With external trigger functionality, nano- to picosecond pulse duration, and a wide range of wavelengths, the KATANA & PILAS series are our most versatile offering.
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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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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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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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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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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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Nanosecond Pulsed Lasers
Our nanosecond pulsed lasers feature pulses in the ns range. For picosecond and femtosecond lasers please see Ultrafast Lasers.
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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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*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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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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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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Lasers And LEDs
AGILE features a broadband spectral output from <400 nm to >2000 nm and pulse repetition rates from 10 kHz to 1 MHz, making it the ideal light source for the majority of fluorescence lifetime applications. Using the Time-Correlated Single Photon Counting (TCSPC) technique, fluorescence lifetimes from a few picoseconds to microseconds can be accurately resolved. It is also compatible with Multi-Channel Scaling (MCS) mode for lifetimes up to 10 μs.
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*Tunable Wavelength
*Wide range of OPO and OPA systems*Ultra-broad tuning from 192 to 16 000 nm*Femtosecond, picosecond & nanosecond pulse durations*Narrow bandwidth models
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Fluorometers
Our Fluorometers can accommodate any size work-area, and are available as compact or benchtop models, or as large modular systems, to suit your requirements. In addition, our Fluorometers can be coupled to become modular Fluorometer systems, or supercontinuum white-light laser-powered lifetime Fluorometers!HORIBA’s Fluorometers offer incredibly fast lifetime determinations down to picoseconds, deep UV absorbance and fluorescence excitation from as short as 200 nm in the UV, all the way to near-IR wavelengths of 1000 nm.
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PCI Express Receiver Board
AD12-2000-IRIGB
The AD12-2000-IRIGB is a high performance wideband 0.3-1.8GHz PCIe-bus receiver on a single PCIe Gen3 board, that can continuously digitize a wide portion of the RF spectrum, with a 3.6GSPS 12-bit A/D that can 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. Designed for demanding military, scientific, industrial, communications, safety and electrical power utility applications, the AD12-2000-IRIGB has 60dB of gain adjust range (manual and AGC with programmable loop bandwidth), a wideband noise figure of 9dB, +11dBm 1dB compression point, and 2dB peak-to-peak ripple over the 300MHz to 1.6GB frequency spectrum.
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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.
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PXI FlexRIO Signal Generator
The PXI FlexRIO Signal Generator combines analog I/O and a user-programmable FPGA into a single, customizable instrument. The instrument enables RF signal generation up to 2.9 GHz with 12 bits of resolution. The PXI FlexRIO Signal Generator 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.
