Abstract:
The present invention is directed toward realizing a measurement method that enables finding the intensity waveform of optical short-pulse as well as the change in chirp frequency over time at a high resolution. Such a method involves irradiating an optical short-pulse that is to be measured at a delay time .tau. upon a first photoconductor that enters a conductive state when irradiated by light and upon a second photoconductor that enters a conductive state only when irradiated by light while the first photoconductor is in a conductive state. In this way, the autocorrelation waveform of optical short-pulse that is to be measured is found; the result F(.omega.) of a Fourier transform of the autocorrelation waveform of optical short-pulse to be measured is found; and this result is divided by the result of a Fourier transform of the cross-correlated waveform h.sub.12 (.tau.) of the impulse response waveform h.sub.1 (t) of the first photoconductor and the impulse response waveform h.sub.2 (t) of the second photoconductor to find the intensity power spectrum .vertline.I(.omega.).vertline..sup.2 from which the response characteristics of the photoconductors are eliminated, and finding short-pulse waveform from above-described .vertline.I(.omega.).vertline..sup.2 and field power spectrum .vertline.E(.omega.).vertline..sup.2.
Abstract:
Apparatus and a related method for detecting laser pulses and classifying em in accordance with their wavelength, irradiance level, shape and time of occurrence. Each pulse received from a selected field of regard (10) is detected in a high-speed broadband radiometer (12), which generates a corresponding electrical pulse that is used to form a triggering pulse to control a gated camera (24) coupled to a transmission grating spectrometer (22). The gated camera (24) has an inherent delay time before it becomes active after receiving a gating signal (30). To compensate for this delay, light from each laser pulse passes through a fiber image delay line (16) before reaching the transmission grating spectrometer (22). Output data signals from the camera (24) are processed (40) to reduce the effects of background noise and converted (42) to a quantity indicative of wavelength. The electrical pulse from the radiometer (12) is also used to generate additional quantities indicative of pulse shape, as well as to generate, in a thresholding circuit (34), the camera triggering signal and to generate, in another circuit (36), a camera gain control signal.
Abstract:
A method and apparatus for processing signals from light pulses for use in detecting the presence of objects that intrude between a light source and light receiver. Upon the receiver detecting light pulses emitted from the source, the emitted light pulses are modulated responsive to a modulation signal into an electro-optical signal path having successive periods. Each period has main, minimum and maximum pulses with the signal path providing a linear processing area having upper and lower amplitudes. Within the linear processing area an hysteresis range is set with upper and lower detection levels. Detection is disabled for those light pulses having amplitudes which are above or below the respective upper and lower detection levels. The linear processing area has an offset amplitude and the main pulse is controlled to have an amplitude which is a function of the offset amplitude.
Abstract:
A photoconductive photodetector to which a modulation voltage signal having a predetermined frequency is applied receives a signal to be measured (I.sub.I) while adjusting the phase of a modulation signal by a phase shifter. A current-to-voltage conversion unit extracts a DC component of a current signal generated at the photoconductive photodetector in correspondence with the intensity of a predetermined frequency component of the signal to be measured (I.sub.I) as a voltage signal. The maximum value of DC voltage values (V.sub.O) obtained in every setting operation of a phase adjustment value is identified. The maximum value corresponds a case in which the modulation voltage signal and the predetermined frequency component of the signal to be measured (I.sub.I) are in phase. The intensity of the predetermined frequency component of the signal to be measured (I.sub.I) is calculated. As a result, a high-speed phenomenon can be measured with a high precision.
Abstract:
A device and a process for enabling an incident wide bandwidth (greater than about 1 GHz) short duration (less than about 10 microseconds) individual pulse of electromagnetic radiation to be digitally sampled at a sampling rate that is achievable by available digital sampling circuits. The incident pulse is modulated onto an optical signal to form a modulated optical signal and the whole, or successive or randomly selected parts, of the modulated optical signal are replicated using optical time delay means. The resulting plurality of modulated optical signal representations of the whole or parts of the incident pulse can then be digitally sampled at a sampling rate which is reduced in proportion to the number of replications to obtain a complete digital representation of the incident pulse.
Abstract:
Method and apparatus for measuring the time of short events, such as characteristics of a source of short radiation pulses or lifetime of excited states of a sample. The method and apparatus is based on a multi-step photoemission process from an active element target exhibiting superlinear photoemission. A short prompt radiation pulse is used to raise electrons to an excited state, and a following overlapping short probe pulse is used to raise the excited electrons to the vacuum level where they leave the sample, changing its charge state. The number of escaped electrons is measured as a function of the time delay between the prompt and probe pulses to provide the sought after information. Preferably, the charged target is suspended or supported in an electric field, and the voltage needed to restore the charge-changed target to its original position is used.
Abstract:
For the acquisition of data for determining the duration and chirp (frequency modulation) of a single ultrashort laser radiation pulse said pulse is split into two partial pulses which are each conducted through one of two TREACY compressors having different group delay dispersions and then recorded in succession on the same time basis with a streak camera.
Abstract:
System and method for analyzing pulses from an excimer laser by measuring light energy rather than heat energy. The output of the laser is monitored with a photodetector to provide electrical current pulses corresponding to the intensity of the light in individual ones of the laser pulses. The current pulses are integrated to provide voltages corresponding to the light energy of the laser pulses, and the voltages are converted to digital signals. The digital signals are accumulated during the exposure period to determine the total light energy of the pulses during that period and also during a shorter interval of time during the exposure period. The light energy for the interval is divided by the length of the interval to determine the average intensity of the pulses during the interval. Displays are provided for the light energy and the intensity of the pulses, as well as the length of the exposure period.
Abstract:
A technique for the simultaneous measurement, in real time, of the changes in mode size, pulse length, and power of a wavetrain of laser pulses delivered by mode-locked or other pulsed laser systems contemplates directing respective portions of the beam along each of three beam paths. The beam portions along the first and second beam paths are subjected to respective, and different, degrees of focusing, and then passed through respective non-linear elements which generate radiation at the second harmonic. The first harmonic components are removed, and the second harmonic components are passed to respective first and second detectors which generate signals representative of the total second harmonic energy along each of the first and second beam paths. The beam portion along the third beam path is passed to a detector which generates a signal representative of the total energy in the beam pulse. The three signals are combined to give values proportional to peak power, pulse length, and mode size.
Abstract:
An optical signal sampling apparatus for high-speed gating of an optical signal in the form of repetitive waveforms comprises an input optical path for introducing the optical signal to an optical amplifier; the optical amplifier whose gain is adjustable by a gating electrical signal, for amplifying the optical signal; a driving circuit for providing, in response to a sampling signal, the optical amplifier with the gating electrical signal having a series of pulses which are gradually shifted on a time axis with respect to the repetitive waveforms of the optical signal; and an output optical path for introducing an output optical signal from the optical amplifier.