130 results about "Phase map" patented technology

A method for three-dimensional shape measurement provides for generating sinusoidal fringe patterns by defocusing binary patterns. A method for three-dimensional shape measurement may include (a) projecting a plurality of binary patterns onto at least one object; (b) projecting three phase-shifted fringe patterns onto the at least one object; (c) capturing images of the at least one object with the binary patterns and the phase-shifted fringe patterns; (d) obtaining codewords from the binary patterns; (e) calculating a wrapped phase map from the phase-shifted fringe patterns; (f) applying the codewords to the wrapped phase map to produce an unwrapped phase map; and (g) computing coordinates using the unwrapped phase map for use in the three-dimensional shape measurement of the at least one object. A system for performing the method is also provided. The high-speed real-time 3D shape measurement may be used in numerous applications including medical science, biometrics, and entertainment.

Embodiments of the invention provide a method of determining one or more characteristics of a target object, comprising determining a first phase map for at least a region of a target object based on radiation directed toward the target object, determining one or more further phase maps for a sub-region of the region of the target object, determining a number of phase wraps for the sub-region based on a plurality of phase maps for the sub-region, and determining a characteristic of the region of the target object based on the number of phase wraps for sub-region and the first phase map. Embodiments of the invention also relate to a method of determining one or more characteristics of a target object, comprising determining a phase map for at least a region of a target object based on one or more diffraction patterns, determining a wavefront at a plane of the object based upon the phase map, and determining a refractive property of the object based on the wavefront.

Disclosed is a three-dimensional imaging method for a Polarimetric Interferometric Synthetic Aperture Radar (Pol-In-SAR) based on the polarimetric data integration, which belongs to the Polarimetric radar Interferometric measurement data processing technology field. The data is read in and two scattering vectors k1 and k2 are structured to each scattering unit; eigenvalue decomposition is performed on the matrix K1 K1-K2 K2 and three eigenvalues are obtained: Lambada1>0, Lambada1>0 and Lambada3=0; values of formula(1) can be respectively calculated so as to determine which condition the value belongs to; if in condition 1, w=w<(1)> can be calculated according to formula (6); if in condition 2, w=w<(2)> can be calculated according to formula (14); and then Phi[s]=arg(wk1k2w)can be calculated. An enhanced complex image can be obtained according to formula 3); the matrix Omega12=> is calculated; and then Phi[m]=arg(w[Omega12]w) can be calculated according to formula 22). The flat-earth effect is removed on the obtained whole phase map (single view or multi-view); and phase unwrapping is performed by using branch-cut algorithm. The invention has wide application range, and the calculating time is smaller than that of the interference optimization method; and the integrated phase quality is better than that of interference optimization method, the phase quality can be always enhanced despite the original signal level, thereby establishing a fine basis for generating accurate digital elevation model (DEM) in the future.

Methods are described for efficient reconstruction of MRI data. In one practice, new reconstruction algorithms for non-uniformly sampled k-space data are presented. In the disclosed algorithms, Iterative Next-Neighbor re-Gridding (INNG) and Block INNG (BINNG), iterative procedures are performed using larger rescaled matrices than the target grid matrix In BINNG algorithm, the sampled k-space region is partitioned into several blocks and the INNG algorithm is applied to each block. In another practice, a novel partial spiral reconstruction (PFSR) uses an estimated phase map from a low-resolution image reconstructed from the central k-space data and performs iterations, similar to the iterative procedures with INNG, with an imposed phase constraint. According to yet another practice, an off-resonance correction is performed on matrices that are smaller than the full image matrix. All these methods reduce the computational costs while rendering high-quality reconstructed images.

A system for generating and utilizing a look-up mechanism consisting of one or more phase difference error maps, tables and/or mathematical models calculates the respective maps, tables and/or models by placing a short baseline or ultra-short baseline antenna array in a known location and known orientation, determining angles of incidence of incoming GNSS satellite signals with respect the antenna array and calculating expected carrier phase differences between respective pairs of antennas, calculating measured carrier phase differences between the respective pairs of antennas, and determining carrier phase difference errors using the expected and measured carrier phase differences. The carrier phase difference errors are then recorded in the look-up mechanism, with the maps and, as appropriate, look-up tables for the respective pairs of antennas being indexed by angles of incidence. Thereafter, the system utilizes the look-up mechanism when determining the unknown orientation of the antenna structure. For respective pairs of antennas, the system enters the look-up mechanism based on angles of incidence determined from a calculated orientation, and uses the retrieved values in the calculation of a corrected orientation, to compensate for phase distortion.

A first method to compute a phase map within an optical proximity correction simulation kernel utilizes simulated wavefront information from randomly generated data. A second method uses measured data from optical tools. A phase map is created by analytically embedding a randomly generated two-dimensional array of complex numbers of wavefront information, and performing an inverse Fourier Transform on the resultant array. A filtering function requires the amplitude of each element of the array to be multiplied by a Gaussian function. A power law is then applied to the array. The elements of the array are shuffled, and converted from the phasor form to real/imaginary form. A two-dimensional Fast Fourier Transform is applied. The array is then unshuffled, and converted back to phasor form.

A patterned sapphire substrate is measured from a fine phase map and a coarser height map of the sample. The boundaries of the PSS features are identified by finding the locations of minimum contrast in the modulation map of the substrate and are used to produce a height map of the substrate base and a phase map of center regions of the features. A fringe-order map of the features with respect to the base is used to identify the most prevalent fringe order of pixels in the center-regions of the features. That fringe order is adopted as the correct offset between corresponding pixels in the phase map of the center regions of the features and the base of the substrate. A complete map of the substrate is thus obtained by combining the phase map of the features with the height map of the substrate with an offset equal to the fringe order produced by the invention.

The invention discloses a phase error correction method for an out-of-focus phenomenon of a fringe projection three-dimensional measuring system. The method comprises: a computer generates a phase-shifted fringe image and the image is collected by a camera; for the collected image, a background image I' and a phase phi' containing an error are calculated and edge extraction is carried out on the background image I'; a point spread function (PSF) of each edge pixel is calculated after edge map obtaining; a phase gradient direction and a phase density of each to-be-processed pixel are calculatedby using gradient filtering and neighborhood averaging methods in the phase map phi'; and then for the to-be-processed pixels, phase errors delta phi caused by the out of focus of the camera are calculated pixel by pixel, so that a finally corrected phase phi is obtained and the phi meets a formula: phi=phi'-delta phi. The corrected phase information can be converted into three-dimensional information of a to-be-measured object by a phase-height mapping relationship.

A correlation method of real part and imaginary part in interference phase map includes using isoline window in size of m x n to carry out correlation operation for real part and imaginary part data of two complex maps for deriving out correlation coefficient C1, utilizing the same manner to drive out C2 by carrying out correlation operation for real part of the first complex map data and for imaginary part of the second complex map data, deriving out arc tangent for obtaining interference phase map by utilizing ratio of C1 and C2; using two accurate complex maps to generate interference phase map being free from coherent speckle noise.

Interferometric methods and apparatus by which the map between pixel positions and corresponding part locations are determined in situ. The part under test, which is assumed to be a rigid body, is precisely moved from a base position to at least one other position in one to six degrees of freedom in three-dimensional space. Then, the actual displacements are obtained. The base position is defined as the position with the smallest fringe density. Measurements for the base and all subsequent positions are stored. After having collected at least one measurement for each degree of freedom under consideration, the part coordinates are calculated using the differences of the various phase maps with respect to the base position. The part coordinates are then correlated with the pixel coordinates and stored.

The present invention provides an image area cutting method of the Duffing vibration generator phase map. 1. Selecting a typical Duffing vibration generator normalized equation. 2. Inserting an A/D converter in front of the typical Duffing vibration generator, inserting an area cutter in back. 3. Inputting the signals having noise to be detected into the A/D converter. 4. A quarter to a tenth of a circle of the signals to be detected is used as the converting circle of the A/D converter and is used together with a Duffing vibration generator equation to figure out the step length. 5. The result is calculated out by the Duffing vibration generator by using a fourth order Runge-Kutta algorithm and is sent to the area cutter. 6. The result is judged by the area cutter which then outputs the detected signals carrying the information of the data to be detected. In the present invention the identifying problem of two-dimensional chaos vibration generator phase map is transformed into a problem of one-dimensional detecting, and the problem that the phase map analyzing method can not be directly used for detecting the communication signals currently is solved.

In general, one embodiment of the invention relates to a method for detecting data bits and estimating the channel reliability of each carrier. The detection method comprises (i) computing a complex phase difference between a current symbol and a previous symbol, (ii) separating a real value component (R) from a corresponding imaginary value component (I) forming the complex phase difference, (iii) determining at least one boundary constraint line of a complex phase map for a selected demodulation scheme, and computing an arithmetic combination of the real value component and the corresponding imaginary value component to detect whether a series of bits falls within a selected region of the complex phase map defined by the at least one boundary constraint line. Over N symbols propagating over a carrier, including the current symbol and the previous symbol, the channel estimation counts a number of symbols (less than N but greater than a threshold) that fall within an estimated area of the complex phase map. The estimated area is bound by boundary constraint lines based on a parameterized real value component.

The present invention adopts standard raster specimen, using LSCM scanning moire method to obtain scanning moire image, to proceed four steps phase shift processing to originality image though moire phase shift technology to obtain phase shift moire image, according to moire phase shift theory to obtain phase map, after unpackaging to obtain originality phase map, according to phase and displacement field relation to obtain scanning perturbed field, thereby reaching correction target. Compared with current method, the present invention can directly measure scan line perturbed field resulted from scanning control unit distortion phenomena through scanning moire and moire phase shift technology , with high precision, simple operation, and real time and all field measurement.

The invention provides a super-lens microstructure generation method. The method includes the following steps of generating phase maps, calculating phase distribution and generating microstructures. The invention further relates to a micro biphoton microscopy system based on the super-lens. A super-surface lens is introduced into the field of biphoton microscopy, medium numerical aperture focusingis achieved under full field of view, the structure of a microscope is greatly simplified, the weight of the overall equipment is largely reduced, and lighter load animal experiments can be achieved.The reliability of in vivo biphoton microscopy experimental data is improved, and the method has high scientific value for micro biphoton, especially in vivo microscopic imaging; the influence of a backpack type micro microscope system on observed objects (such as mice) is further reduced. According to the system, from simulation design to processing to experiments, a super-surface lens is introduced into the biphoton microscopy imaging system, and a new generation of imaging equipment is provided for brain imaging of living animals. The progress in brain and Neuroscience research is promoted.

The invention discloses a novel four-order neural network hyperchaotic circuit. First, second, third and fourth operational amplifiers A1, A2, A3 and A4 construct a linear inverting integrator; the output ends of the first, second, third and fourth operational amplifiers are chaotic signal output ends X1, X2, X3 and X4 respectively; a fifth operational amplifier A5 constructs a nonlinear inverting limiting amplifier; sixth and seventh operational amplifiers A6 and A7 construct a linear inverting amplifier; an inverting integrator A1 is connected with a limiting amplifier A5 and an amplifier A3 respectively; an inverting integrator A2 is connected with an integrator A3 and an amplifier A7 respectively; an inverting integrator A3 is connected with an amplifier A6; and an inverting integrator A4 is connected with an integrator A2 and an integrator A7 respectively. Due to the adoption of the four-order neural network hyperchaotic circuit, various waveforms, phase maps and chaotic evolvement curves can be output, and a hyperchaotic secret communication system can be constructed.

A modified projection on convex sets (POCS) algorithm and method for partial k-space reconstruction using low resolution phase maps for scaling full sets of reconstructed k-space data. The algorithm can be used with partial k-space trajectories in which the trajectories share a common point such as the origin of k-space, including variable-density spiral trajectories, projection reconstruction trajectories with a semicircle region acquisition, and projection reconstruction trajectories with every other spike acquired.

A coherent radiation imaging system that produces digital images with a reduced amount of speckle. Radiation from a long coherence length source is used to form an image of a sample. The output coherent wave is temporally divided into a plurality of wavelets. The spatial phase of each wavelet is then modulated a known and different amount. Each phase modulated wavelet illuminates the sample and is perturbed by its interaction with the sample. A spatial phase map of each perturbed wavelet is then created and converted to a sample image with an image reconstruction program. The plurality of sample images thus formed is statistically averaged to form a final averaged image. The high frequency speckle that is not optically resolvable tends to average to zero with continual statistical averaging, leaving only the optically resolvable lower frequency phase information.

This invention relates to a method of detecting outdoors water substance impediment base on polarization information, the process is: fix polarizationlum filter at camera front; pick three pieces different polarization physic images in identity region; count the polarization degree chart, polarization phase map and phase similarity measure chart of this region, and at the phase similarity measure chart verdict whether water substance impediment existing; if existing, then through self-adapting threshold partition algorithm to line out possible range of water substance impediment, at last combine polarization degree chart to definite true water substance impediment region. This device by detecting polarization characteristic of water-reflected light, could detect rounded water surface region, especially possess favorable identify effect to state of water surface existing reflection .This invention adopt relatively simple image segmentation algorithm, small calculated amount, quickly, high accuracy rating, and wide detecting celerity, wide applicability.

A system (10) and method generate one or more MR data sets of an imaging volume (16) using an MR scanner (14). The imaging volume (16) includes one or more of a region of interest (ROI), the ROI including a metal element, and a local receive coil (18) of the MR scanner (14). At least one of an attenuation, confidence or density map accounting for the metal element is generated and the location of the local receive coil (18) within the imaging volume (16) is determined. The generating includes identification of the metal element within the ROI based on a phase map of the ROI generated from the MR data sets. The determining includes registering a known sensitivity profile of the local receive coil (18) to a sensitivity map of the local receive coil (18) generated from the MR data sets.