Abstract:
A control system and apparatus for use with an ultra-fast laser is provided. In another aspect of the present invention, the apparatus includes a laser, pulse shaper, detection device and control system. A multiphoton intrapulse interference method is used to characterize the spectral phase of laser pulses and to compensate for any distortions in an additional aspect of the present invention. In another aspect of the present invention, a system employs multiphoton intrapulse interference phase scan. Furthermore, another aspect of the present invention locates a pulse shaper and/or MIIPS unit between a spectral dispersion point in a laser oscillator and an output of a laser amplifier.
Abstract:
A photon detecting apparatus for use in a quantum encryption receiver apparatus or the like, wherein a plurality of photon detectors are used to improve the response speed of the photon detecting apparatus. There are included wavelength branching means (12) for branching a wavelength-multiplexed incident photon pulse sequence for each of wavelengths; a plurality of photon detectors (13-1, ···, 13-n) for detecting the photons as branched by the wavelength branching means (12); bias applying means (14) for applying gate pulses, as bias voltages, to the respective ones of the plurality of photon detectors (13-1, ···, 13-n) in conformity with the timings at which the output lights of the wavelength branching means (12) are incident on the plurality of photon detectors (13-1, ···, 13-n); and data processing means (15) for converting the detection signals from the plurality of photon detectors (13-1, ···, 13-n) to time series signals.
Abstract:
A system for emitting and detecting terahertz frequency electromagnetic pulses. The system comprises a single transceiver device, which may be an electro-optic crystal or photoconductive antenna, for both emitting and detecting the pulses. A related method comprises using a single transceiver device to both emit and detect electromagnetic terahertz frequency pulses. The transceiver device is excited by a pump pulse to emit a terahertz output pulse, which is modulated with a chopper. An object reflects the terahertz pulse and the reflected pulse is detected in the transceiver using a probe pulse. A lock-in amplifier set to the same frequency of the chopper is used to reduce noise in the signal detected by the transceiver. An image of the object may be created using the intensity or the timing of the peak amplitude of the terahertz pulses reflected from the object.
Abstract:
La présente invention se rapporte à une méthode et un dispositif pour la caractérisation d'impulsions optiques isolées ou au sein d'un train d'impulsions. La méthode et le dispositif sont utilisables pour caractériser des impulsions courtes et ultracourtes. La méthode comprend une étape de création de deux images de spectres décalés, à partir de la même impulsion ou du même train d'impulsions. À partir d'un signal de battement entre deux fréquences superposées des deux spectres, la méthode de l'invention permet de reconstruire la phase spectrale de l'impulsion. Dans sa forme préférée, le dispositif de l'invention comprend un prisme de Wollaston (3) et un polariseur (6), pour créer deux faisceaux interférant après avoir parcouru le même chemin optique depuis le lieu de séparation du faisceau en deux parties.
Abstract:
In a photoelectric signal conversion device comprising a substrate (4), formed thereon a thin film (3) that functions as a light detection portion (5), and a pair of electrodes (2) provided thereon across the light detection portion, the thin film constituting the light detection portion is made of a solid state phase transition material, and the pair of electrodes are made of a superconductive material, whereby the light detection portion can respond to optical signals on the order of psec, and the device can follow ON-OFF signals of terahertz.
Abstract:
A system (100) that measures a segment of a waveform by isolating the segment by virtue of gating (10). A waveform anomaly may be gated. The gated waveform is supplied to a plurality of frequency information extractors (16, 18, 20), which yield information regarding the frequency content of the gated waveform at individual frequencies (f0, f1, …, fn). Distortion introduced into the gated waveform may be measured by applying the same gating function to a reference waveform. The system may measure or gate an incoming waveform at time intervals dictated by a clock signal recovered from the incoming waveform. A segment of the waveform to be measured may be circulated through a fiber loop, with a fraction of the circulated signal split off for presentation to a measurement system with each circulation. The point in time at which the waveform crosses a threshold may be determined by straddle sampling.
Abstract:
Le procédé selon l'invention consiste à effectuer :
un filtrage optique linéaire du signal (S) dont on veut mesurer l'amplitude des impulsions grâce à une interaction acoustique entre le signal optique (S) et un faisceau acoustique colinéaire ou quasi-colinéaire, un mélange dans un élément électrooptique à réponse non linéaire (4) des faisceaux optiques diffractés par le faisceau acoustique, suivi d'au moins un détecteur de l'intensité lumineuse issue du mélangeur (4), ou au moins une détection-intégration du carré de l'intensité optique diffractée par le faisceau acoustique.
Abstract:
An optical autocorrelator comprises an optical waveguide (40) of semiconductor material which exhibits two photon absorption at a wavelength at which the autocorrelator is intended to operate. Reflecting means (46) are provided at a part of the waveguide which is remote to an end (42) in which an optical pulse (44) is input for reflecting the optical pulse such as to generate counter-propagating optical pulses in the waveguide. A plurality of electrodes (481-48N) are disposed along the waveguide for measuring a two photon absorption photocurrent (i1-in) generated in the waveguide by the counter-propagating optical pulses.
Abstract:
A method of determining accurately and expeditiously the frequency of a coherent signal from an incoming electrical signal is disclosed. The method comprises the steps of: generating a time sequence of sampled data signals from the incoming electrical signal, detecting the coherent signal in the time sequence of sampled data signals and generating a frequency estimate thereof; and determining the frequency of the detected coherent signal based on a function of the frequency estimate and a time segment of sampled data signals associated with the coherent signal. A system for performing the same is also disclosed.