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222 results about "Fresnel zone" patented technology

A Fresnel zone (/freɪˈnɛl/ fray-NEL), named after physicist Augustin-Jean Fresnel, is one of a series of confocal prolate ellipsoidal regions of space between and around a transmitter and a receiver. Transmitted radio, sound, or light waves can follow slightly different paths before reaching a receiver, especially if there are obstructions or reflecting objects between the two. The waves can arrive at slightly different times and will be slightly out of phase due to the different path lengths. Depending on the magnitude of the phase shift, the waves can interfere constructively and destructively. The size of the calculated Fresnel zone at any particular distance from the transmitter and receiver can help to predict whether obstructions or discontinuities along the path will cause significant interference.

Focusable and steerable micro-miniature x-ray apparatus

A micro-miniature x-ray apparatus comprises: a first chip subassembly including a source of x-rays including both Bremsstrahlung photons and characteristic x-rays; a second chip subassembly including a filter for transmitting the characteristic x-rays and blocking the Bremsstrahlung photons; a third chip subassembly including a movable element for focusing or collimating the transmitted characteristic x-rays into a beam and means for controlling the position of the focusing element. In one embodiment, the controlling means include a micro-electromechanical system (MEMS). In another embodiment, the position of the movable element determines how the x-ray beam is steered to the focal area. In still another embodiment, the x-ray source includes a field emitter electron source and a target responsive to the electrons for generating x-rays. In this case, the x-ray beam is also steered by selectively energizing the anode segments. In yet another embodiment, the movable element includes a Fresnel zone plate; in still another embodiment it includes an array of poly-capillaries. Advantageously, our x-ray source, including its focusing, collimating and steering components, can be fabricated small enough to be mounted at the end of a catheter. In addition, in some embodiments it can also fabricated sufficiently inexpensively to be disposable after each use.
Owner:LUCENT TECH INC

Spectral-domain optical coherence tomography imaging system based on Fresnel spectrometer

The invention relates to a spectral-domain optical coherence tomography imaging system based on a Fresnel spectrometer, which is characterized by comprising a Michelson interferometer, the Fresnel spectrometer and a Fourier transformation module. The Michelson interferometer sends coherent light which is formed by superposing sample light returned from various layers of a sample with reference light into the Fresnel spectrometer, the coherent light is emitted onto a Fresnel zone plate parallelly through a collimating lens and an expanded beam lens respectively, and is expanded at the same interval according to the wave number and then projected to a linear array CCDs (charge coupled devices) by the Fresnel zone plate, frequency spectrum data of the coherent light are read by the linear array CCDs and sent to the Fourier transformation module, and then recovered into information of spatial position of the sample by means of discrete Fourier transformation through the Fourier transformation module. The spectral-domain optical coherence tomography imaging system based on the Fresnel spectrometer can be applied to not only spectral-domain optical coherence tomography imaging but also spectral analysis having requirements for wavelength-wave number conversion and resampling for imaging or detecting and required to be expanded uniformly according to the wave number, and especially can be applied to the biomedical imaging process.
Owner:TSINGHUA UNIV

Three-dimensional dip angle domain stationary phase pre-stack time migration method and system

The invention discloses a three-dimensional dip angle domain stationary phase pre-stack time migration method and system. The method comprises the steps that pre-stack seismic data are read, and a migration speed field and a stretching and removing parameter are determined; according to the migration speed field and the stretching and removing parameter, two dip angle channel sets corresponding to dip angles in the directions parallel to and perpendicular to a measuring line respectively are generated through a selected imaging line; based on the two dip angle channel sets on the selected imaging line, Fresnel zones in the two dip angle directions are picked up, and the Fresnel zones of all imaging points on a quasi imaging block are obtained through interpolation; through the obtained Fresnel zones of all the imaging points, three-dimensional stationary phase pre-stack time migration is carried out, and migration results corresponding to different migration distances are obtained; the migration results of three-dimensional stationary phase pre-stack time migration are collected, and a three-dimensional imaging data body is formed; the three-dimensional imaging data body is converted into a profile image of an underground reflection structure. According to the method and system, the problem that when a high dip angle structure exists, the signal to noise ratio of the migration image obtained through an existing migration imaging technology is low is effectively solved.
Owner:INST OF GEOLOGY & GEOPHYSICS CHINESE ACAD OF SCI

Scattered wave pre-stack imaging method for identifying small-fault throw breakpoints

The invention relates to a scattered wave pre-stack imaging method for identifying small-fault throw breakpoints, which is applied to processing of seismic reflection information in seismic exploration and is of a seismic imaging method of a micro-small fault for identifying the underground geological structure. According to the method, scattered waves of the breakpoints of the fault are utilized for independent imaging of the breakpoints with the fault throw of less than 1/4 wavelength, which are difficult to identify by conventional reflected wave migration. According to the method, the existing seismic reflection information is utilized, and the independent imaging of the small breakpoints is realized by pressing the energy of transmitted waves in pre-stack migration calculation and utilizing the polarity inversion characteristic of the scattered waves of the breakpoints. Pre-stack time migration is taken as the basis, an angle gather is generated by migration of single-shot information, and a Fresnel zone corresponding to an inphase axis of reflected waves is excised so as to eliminate the transmitted waves. According to the method, the small fault and breakpoints of the underground structure can be indicated in a fine manner, migration and plugging of underground oil gas can be better known, and the method further has an important application value for exploration and development of oil gas resources. The ability to identify the underground deep fissures and fault of the seismic exploration method is significantly improved.
Owner:INST OF GEOLOGY & GEOPHYSICS CHINESE ACAD OF SCI

Wavelength scanning confocal micro-displacement measurement device and method

The invention provides a wavelength scanning confocal micro-displacement measurement device and a method. In a confocal microscope optical path system, a wavelength tunable laser is used for carrying out illumination; a Fresnel zone plate is used for carrying out focus point illumination; according to the axial color difference focal shift characteristic, axial scanning of focus light spots is achieved through wavelength scanning; a confocal pinhole photoelectric detection unit is used for detecting confocal axial optical chromatography response output; for the disperse wavelength lambda<n> = lambda<min> + (n-)deltalambda, n = 1, 2, ..., 11, obtaining the axial optical chromatography displacement-intensity response, wherein the lambda<min> is the wavelength lower limit, the wavelength upper limit is lambda<max> = lambda<min> + 10deltalambda, and the deltalambda is the wavelength stepping interval; peak value positions of the optical chromatography response curves form a linear calibration relation searching table of illumination wavelengths and axial displacement; and fine wavelength scanning is executed for each characteristic point of a to-be-measured sample for once, and actual displacement of each point is calculated according to the peak value of each response curve and the searching table. Thus, measurement of micro-displacement or relative height is finished, and the method is suitable for precise measurement of micro displacement, film thickness, nano steps and the like.
Owner:XI AN JIAOTONG UNIV
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