Picosecond
one trillionth of a second.
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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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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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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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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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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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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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Benchtop Femtosecond/Picosecond Lasers and Amplifiers
The systems feature a portable design with user-friendly front panel control knobs for adjustment of output parameters, such as power, pulse width and repetition rate. With wavelength options of 780 nm, 850 nm, 1310 nm, and 1550 nm, pulse widths as low as < 0.3 ps, and GHz low-jitter synchronization signals, these systems provide ideal optical sources for high speed transceiver conformance testing and photodiode characterization.
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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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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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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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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.
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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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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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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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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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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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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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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.
