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63 results about "Optical heterodyne detection" patented technology
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Optical heterodyne detection is a method of extracting information encoded as modulation of the phase, frequency or both of electromagnetic radiation in the wavelength band of visible or infrared light. The light signal is compared with standard or reference light from a "local oscillator" (LO) that would have a fixed offset in frequency and phase from the signal if the latter carried null information. "Heterodyne" signifies more than one frequency, in contrast to the single frequency employed in homodyne detection.
The present invention relates to optical heterodyne detection cavity ringdown spectroscopy. In one aspect the invention relates to an optical system (1) comprising a ring-down cavity cell (3) defining a resonant optical cavity, means for directing coherent light selected from the group consisting of continuous or quasi-continuous light into said optical cavity (8, 9, 10, 11, and 12), means for altering the resonant optical cavity so as to generate a frequency shift of the coherent light in the optical cavity (6, 7), means for coupling said coherent light into the optical cavity and means for decoupling the frequency shifted coherent light out of said optical cavity (5, 6, 7), means for optically combining (10, 11, 12) said decoupled frequency shifted coherent light with another portion of coherent light not in optical communication with the optical cavity and means for optical heterodyne detection (13) of the intensity of said combined light. A method for optical detection is also described as well as methods and apparatus for detecting a parameter of a sample.
A radar apparatus which can simply determine the sign of velocity of an object is provided. Laser light reflected by the object undergoes quadrature optical heterodyne detection performed by mixers, optical detectors, and a π / 2 phase shifter, whereby I and Q component signals are output. A frequency analyzer performs FFT on a complex signal composed of the I component signal (real part) and the Q component signal (imaginary part) to thereby obtain its frequency spectrum. Since the frequency spectrum is calculated without being folded back even in a region where the frequency is negative, the sign of the Doppler frequency fd can be determined. When the Doppler frequency fd is positive, the sign of the velocity of the object is a direction toward the radar apparatus. When the Doppler frequency fd is negative, the sign of the velocity of the object is a direction away from the radar apparatus.
An optical heterodyne detectionsystem includes a tunable optical pre-selector that is adjusted to track the frequency of a swept local oscillatorsignal. The tunable optical pre-selector is adjusted in response to a measure of the frequency of the swept local oscillatorsignal and in response to a measure of a portion of the swept local oscillatorsignal after the portion of the swept local oscillator signal has optically interacted with the optical pre-selector. In an embodiment, at least some portion of the swept local oscillator signal is modulated before it interacts with the optical pre-selector. In an embodiment, the portion of the swept local oscillator signal that interacts with the pre-selector is detected and used in a feedback control circuit to generate a control signal which causes the error between the center frequency of the pre-selector and the frequency of the swept local oscillator signal to be small.
The invention discloses a coherent anti-stokes raman scattering (CARS) optical comb spectrum detection method for improving the precision. The method comprises the steps of: after two femtosecondoptical comb generators as a pumping-detecting light source and a stokes light source of a CARS system pass a CARS spectral measurement system, performing beat frequency and double-optical comboptical heterodyne detection on generated anti-stokes signal light and reference optical combs; eliminating the interference introduced by pumping light by utilizing a polarization dependent balance detection technology at a detecting part so as to realize the quick and real-time CARS optical spectrum detection with high sensitivity and high frequency resolution precision. The method provided by the invention can be used for effectively improving the resolution precision of spectral measurement, realizing the high-precision optical comb imaging within a wide spectral range, effectively inhibiting the environmental noises, eliminating the non-resonant background noise introduced by the pumping light, improving the time and frequency resolution precision and realizing the quick and real-time spectral detection.
A transmitter subsystem generates an optical signal which contains multiple subbands of information. The subbands have different polarizations. For example, in one approach, two or more optical transmitters generate optical signals which have different polarizations. An optical combiner optically combines the optical signals into a composite optical signal for transmission across an optical fiber. In another approach, a single optical transmitter generates an optical signal with multiple subbands. The polarization of the subbands is varied, for example by using a birefringent crystal. In another aspect of the invention, each optical transmitter generates an optical signal containing both a lower optical sideband and an upper optical sideband (i.e., a double sideband optical signal). An optical filter selects the upper optical sideband of one optical signal and the lower optical sideband of another optical signal to produce a composite optical signal.
An optical heterodyne detectionsystem includes a tunable optical pre-selector that is adjusted to track the frequency of a swept local oscillatorsignal. The tunable optical pre-selector is adjusted in response to a measure of the frequency of the swept local oscillatorsignal and in response to a measure of a portion of the swept local oscillatorsignal after the portion of the swept local oscillator signal optically interacts with the pre-selector. Additionally, the pre-selector is dithered such that a dither is imparted on the portion of the swept local oscillator signal that interacts with the optical pre-selector.
A radar apparatus which can simply determine the sign of velocity of an object is provided. Laser light reflected by the object undergoes quadrature optical heterodyne detection performed by mixers, optical detectors, and a π / 2 phase shifter, whereby I and Q component signals are output. A frequency analyzer performs FFT on a complex signal composed of the I component signal (real part) and the Q component signal (imaginary part) to thereby obtain its frequency spectrum. Since the frequency spectrum is calculated without being folded back even in a region where the frequency is negative, the sign of the Doppler frequency fd can be determined. When the Doppler frequency fd is positive, the sign of the velocity of the object is a direction toward the radar apparatus. When the Doppler frequency fd is negative, the sign of the velocity of the object is a direction away from the radar apparatus.
In order to solve a problem that a traditional speed measurement and range findingsystem is poor in resisting influence, the invention provides a speed measurement and range findingsystem and method based on laserheterodyne detection. The speed measurement and range findingsystem comprises a laser, an optical path emission assembly, an optical reception assembly, a processor, a beam splitter, a beam combiner and a focal plane array detector; the input terminal of the beam splitter is connected to the output terminal of the laser; in two paths of optical signals which are split by the beam splitter, one path of optical signals is sent to an optical path emission assembly and is projected to a target object to be measured, and the other path of optical signals is sent into the beam combiner; the optical path reception assembly receives echo signals and converges the echo signals on an input terminal of the beam combiner after filtering; the beam combiner is used for performing coherent mixing on one path of optical signals which is split by the beam splitter and the echo signals to obtain a difference frequency signal; the focal plane array detector performs sampling, processing and analog to digital conversion on the difference frequency signal and then transmits the difference frequency signal to a processor; and the processor obtains speed and distance information of the target object to be measured.
The invention discloses a dynamic strain measurement method based on Brillouin phase shift detection. The dynamic strain measurement method comprises the following steps of dividing laser signals into two paths; after one path of signals are subjected to broadbandfrequency shift, generating optical heterodyne to detect local oscillatorlight wave and detection signallight wave, and synchronously injecting the local oscillatorlight wave and the detection signal light wave into a sensor fiber; after spectrum broadening, causing the other path of laser signals and a pulse generator to generate broadband Brillouin pulse pumping light wave, and injecting the broadband Brillouin pulse pumping light wave into the sensor fiber; setting a modulator to drive a voltage waveform to introduce linear chrip so as to obtain broadband laser, which is approximate to a rectangular spectrum, and extending a linear region with the Brillouin phase shift of the sensor fiber; carrying out coherent detection on the local oscillator light wave and the detection signal light wave through coherent demodulation of a beat frequency signal and a radio frequency signal which are generated by photovoltaic conversion so as to obtain the Brillouin phase shift of the detection signal light wave; demodulating information of a strain signal of the sensor fiber. The dynamic strain measurement method has the advantages that the signal to noise ratio is improved, the dynamic strain measurement range is increased and the detection speed is improved. The invention further discloses a dynamic strain measurement device based on the Brillouin phase shift detection.
The invention discloses a wireless digital communication receiving antenna based on microwave optical wave coherent conversion and a method thereof. wherein the communication receiving antenna comprises a laser,a digital signal modulator, a cesium bubble and beam combiner. a photoelectric detector and a digital signal demodulator, wherein the laser is used for generating local oscillation light required in optical heterodyne detection; wherein the digital signal demodulator modulates a digital signal to microwaves, the cesium bulb modulates and converts the microwaves into modulated light waves, the beam combiner superposes local oscillation light and the modulated light waves to generate an optical heterodynesignal, the photoelectric detector receives the optical heterodynesignal, and the digital signal demodulator is used for recovering the optical heterodyne signal to the digital signal. Coherent conversion of microwaves and light waves in the Rydberg atom six-wave mixing processis utilized, phase modulation of a digital signal on the microwaves is converted into phase modulation on the light waves, coherent demodulation is conducted on the modulated light waves through an optical heterodyne demodulation method to recover the digital signal, and therefore digital communication is achieved.
The invention discloses a light field matching heterodyne detection device and method based on an array detector, and belongs to the field of laserheterodyne detection, especially continuous heterodyne detection capable of utilizing the array detector for carrying out light field matching correction on signal light and local oscillator light. The signal-to-noise ratio of heterodyne detection can be improved. A light signal is received through the array detector, weighted stacking is carried out on receiving signals of all units of the array detector, and finally a total intermediate frequencysignal obtained after stacking is output. In the target detection process, firstly, the signal light reflected back by a target is independently received, then the local oscillator light is independently received, weighting coefficients of all the detection units in the array detector are calculated according to detected light field distribution of the signal light and the local oscillator light, then the signal light and the local oscillator light are received at the same time, weighted stacking is carried out on detection signals output by the detection units according to the calculated weighing coefficients, and finally a composite signal obtained after stacking is output. Therefore, the effect of improving the signal-to-noise ratio of heterodyne detection and the effect of easy and convenient operation are achieved.
The invention relates to a long-distance optical fiber Bragg grating sensing method and device based on self-heterodyne detection. A single frequency light beam sent from a wavelength adjustable narrow line widthlaser is split into two parts of light beam with the same intensity after passing through a triport optical fiber coupler, one part of the light beam passes through a scrambler and is used as an intrinsic light, and the other part of the light beam passes through a light pulse modulation module and is modulated into a pulse detection light; and the detection pulse light passes through an optical isolator, enters a segment of a long-distance transmission optical fiber, and then enters a sensing optical fibergrating array through a far-end light circulator; and the signal reflected from the optical fibergrating shifts frequency of the returned reflection sensing signal through a frequency shift module and then enters a four-port optical coupler together with the intrinsic light, and the generated coherent light signal enters a balance photoelectric detector through the other two ports of the optical coupler and is converted to an electrical signal. The electrical signal received and converted by a signal collection analysis and control module is collected and analyzed to obtain the time domain track of the sensing signal, and the peak power is the power of the coherent signal.
The embodiment of the invention discloses an optical heterodyne method cavity ring down spectral measurement device and method. The measurement device comprises a laserlight source for generating a laser beam, a modulation optical path mechanism, a passive resonant cavity for receiving the laser beam modulated by the modulation optical path mechanism and performing interference superposition on the laser beam, an optical heterodyne detection mechanism for receiving the laser beam subject to the interference superposition and generating an electrical signal, a data processing mechanism for receiving the electrical signal and determining a relationship between the electrical signal and a preset threshold, and if the electrical signal is greater than the preset threshold, the data processingmechanism sends an instruction of turning off the laser light source, collecting and drawing a ring down curve via a data collection circuit, and calculating the concentration of trace substance to be measured. By adoption of the measurement device and method, the measurement accuracy can be improved, the operation is simple, and the cost is low.
A branch portion 101 branches an inputted electrical signal into an in-phase signal and an opposite phase signal which have an opposite relation as to a phase. A first FM laser 104 converts the in-phase signal into an optical frequency-modulated signal (a first optical signal) having a center wavelength λ1 and then outputs the resultant signal. A second FM laser 105 converts the opposite phase signal into an optical frequency-modulated signal (a second signal) having a center wavelength λ2 and then outputs the resultant signal. The two optical signals are combined and then inputted into an optical-electrical converting portion 106. The optical-electrical converting portion 106 subjects the inputted optical signals to optical heterodyne detection by its square-law detection characteristic, and outputs a beat signal between the two optical signals which is a wide-band FM signal at a frequency corresponding to a wavelength difference Δλ(=|λ1−λ2|) between the first optical signal and the second optical signal. It is thus possible to increase frequency deviation of the outputted FM signal and thus greatly improve a CNR.
Provided is an SAIT distance imaging speckle effect suppression method. The bandwidth of linear frequency-modulation pulse signals emitted by a laser device is expanded to N (N is larger than or equal to 2) times of the bandwidth needed by resolution ratio design, and optical heterodyne detection is carried out on echo signals and local oscillator signals to obtain light current data needed for imaging. When data processing is carried out, imaging data obtained after bandwidth expanding are divided into N parts in the distance direction, distance dechirping and orientation focusing imaging are carried out on the data, and ultimately N relatively independent data are produced. Incoherent superposition average is conducted on the N relatively independent target images, and finally images are output. Compared with speckle suppression after uniformization, average strength and contrast of the images are improved to some extent. The method plays a certain role in reducing the speckle effect in an SAIT.