Showing results: 226 - 240 of 1196 items found.
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Transmission Line Pulse Test System -
Impulse Semiconductor Inc.
The Impulse Semiconductor High Current Transmission Line Pulse (TLP) test system is the tool of choice for extracting ESD parameters for transient protection devices in a package, or at wafer level. With accuracy better than 100 milliohms at 40 amps peak current, the Impulse high current TLP is specially tailored to the needs of today's ESD device designers who must accurately measure low values dynamic resistance irrespective of breakdown voltage.
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Laurel Electronics, Inc
The Laureate? time interval meter can display pulse width or time delay between individual pulses to a resolution of 0.2 s. It can also display average pulse width or average time delay between multiple pulses.
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Optilab, LLC.
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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72-190 -
Tenma
A compact and lightweight probe for the analysis and troubleshooting of logic circuits. The probe will recognise high, intermediate and low level pulses in DTL, TTL, HTL and CMOS logic circuits. Works as a pulse detector, pulse stretcher and a pulse memory.
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PL2230 Series -
EKSPLA uab
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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Omega Engineering, Inc
Omega's Non-Contact Level Sensors include Pulse Radar and Ultrasonic Transmitters for liquids, and Pulse Radar Transmitters for solids. Pulse Radar are available in intrinsically safe designs.
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MPA 50 -
CDP Systems Corp.
MPA 50 is a multipass Ti: sapphire amplifier based on a two-mirror confocal design and containing a pulse stretcher, a pulse compressor, a pulse picker, synchronization electronics, and the Faraday isolator.
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Golden Engineering Ltd.
Golden Engineering X-ray generators are based on Pulsed X-ray technology. Pulsed X-rays generate a high intensity X-ray burst (pulse) in a very short period of time (10 to 50 nanoseconds depending on the model). The output dose of each pulse is 3-6 mR measured 12 inches from the front of the X-ray generator. The operator varies the overall dose of each exposure by changing the pulse setting. The pulse rate varies from 10 pulses per second to 25 pulses per second depending on the model. The generators can fire up to 200 pulses before a four-minute rest period.
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S93026B -
Keysight Technologies
S93026B advanced pulsed-RF measurements includes all the capability of S93025B (four internal pulse generators) and adds narrowband-pulse-detection method to extend pulse measurement capability in point-in-pulse and pulse-profile measurements.
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S93025B -
Keysight Technologies
S93025B basic pulsed-RF measurements enables 4 internal pulse generators that can be used to control the internal pulse modulators (N522xB/N524xB Options 021/022), and provides an integrated pulse application that uses the wideband-detection method.
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ADC Corporation
Pulse generation/measurement with basic accuracy of ±0.02% and the minimum pulse width of 50μs, maximum output of 6V/5A
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Minioptic Technology, Inc
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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Coherent Corp.
Measure laser pulse energy over a huge range of wavelengths, repetition rates, pulse energies, and beam diameters.
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PX0105A -
Keysight Technologies
The Keysight PX0105A is suitable for narrow current pulse measurement down to 10 μs pulse width. It supports the Keysight M9602/03A.
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Avoca SPIDER System -
Del Mar Photonics, Inc.
Spectral phase interferometry for direct electric-field reconstruction (SPIDER) is one technique that can recover the spectral phase of an input pulse, without needing any reference pulse. SPIDER interferes two pulses which areseparated in time and in frequency, and the resultantinterferogram is read by a spectrometer.