64results about How to "Small resolution" patented technology

A camera is configured to capture an image of a real world scene as an image signal and to store captured images. The camera includes a screen suitable for displaying a high resolution version of a stored image from a list of stored images when a location within the list is selected. When a browsing mode is selected, the screen displays a scrolling strip of low resolution versions of stored images from the list. A single control allows a user to select the location within the list and also allows a user to select the browsing mode. The camera can allow a user to move between full screen display of stored images and the browsing mode multiple times, with little repetitive finger and/or hand motion, without blocking viewing of the screen, and while allowing the hands to be retained in a convenient picture taking position.

The invention discloses a novel ultra wide angle lens. The novel ultra wide angle lens comprises a lens shell. Pieces of optical glass sequentially arranged from the object space to the image space inside the lens shell include a first lens, a second lens, a third lens, a fourth lens, a diaphragm component, a fifth lens, a sixth lens, a seventh lens and an eighth lens, wherein the first lens is a strawhat-type lens with the negative focal power, the second lens is a biconcave lens or a plane concave lens with the negative focal power, the third lens is a falcate lens or a biconvex lens with the positive focal power, the fourth lens is a falcate lens or a biconvex lens with the positive focal power, the fifth lens is a falcate lens or a biconvex lens with the positive focal power, the sixth lens is a biconvex lens with the positive focal power, the seventh lens is a falcate lens with the negative focal power, the eighth lens is a biconvex lens with the positive focal power, and the eighth lens is connected with a color filter. The visible light wave band and the near-infrared wave band guided in by the lens are focused in the same focal plane, so that the novel ultra wide angle lens can conduct clear imaging in the day and night modes.

Techniques for recovering optical spectral features include receiving a detected time series that represents a temporally varying intensity of an optical signal. The optical signal is formed in response to an interaction between a target optical spectrum and a chirped optical field. The chirped optical field is an optical field that has a monochromatic frequency that varies in time. The target optical spectrum is an optical frequency dependent optical property of a material or device. A phase correction factor is determined based only on one or more properties of the chirped optical field. The detected time series is corrected based on the phase correction factor to produce an output time series that reproduces in time a shape of the target spectrum in frequency. These techniques allow for fast measurement of spectral features and eliminate the need for prior knowledge of the target optical spectrum to adjust the chirp rate.

A construction laser with at least one laser beam (4) defining a plane (3) has a laser unit (6) which is tiltable with respect to a housing (5) around at least one swiveling axis (9a) and includes at least one leveling sensor (10a) which is sensitive to the swiveling axis (9a) for a highly precise orientation to the gravitational field (G), and at least one tilt sensor (11a) which is sensitive to the swiveling axis (9a) for direct measurement of an inclination angle [alpha] relative to the gravitational field (G).

A portable electronic equipment comprises a gaze tracking device configured to track an eye gaze direction of a user in a time interval. The portable electronic equipment comprises a processing device coupled to the gaze tracking device and configured to generate heat map data for the eye gaze direction, generate saliency map data for a field of view of the user, and identify at least one point of interest in the field of view based on both the heat map data and the saliency map data.

A device (100) for processing data, the device (100) comprising a plurality of signal paths (130, 140, 150) each receiving an identical analog input signal (104), at least one signal conditioning unit (101 to 103) in at least one of the plurality of signal paths (130, 140, 150), wherein each signal conditioning unit (101 to 103) is adapted for generating a respective analog intermediate signal (105 to 107) by manipulating a property, particularly an amplitude, of the analog input signal (104), and a plurality of analog to digital converting units (108 to 110) each of which being assigned to a corresponding one of the plurality of signal paths (130, 140, 150) and being supplied with the analog input signal (104) or a respective analog intermediate signal (105 to 107), wherein each of the plurality of analog to digital converting units (108 to 110) is adapted for generating a respective digital intermediate signal (111 to 113) based on the respective analog intermediate signal (105 to 107) or based on the analog input signal (104); a digital signal processing unit (114) supplied with the plurality of digital intermediate signals (111 to 113) and adapted for generating a digital output signal (115) by processing the digital intermediate signals (111 to 113).

A gas concentration detecting apparatus comprises a gas concentration sensor and a gas concentration calculator. The sensor has first to third cells. A gas to be detected is introduced in a chamber and the first cell is responsible for discharging and changing oxygen from and into the chamber. The second cell detects a concentration of a specific gas component of the gas that has passed along the first cell. The third cell detects a concentration of residual oxygen in the gas that remains after discharge of the oxygen through the first cell. The calculator takes in a current acquired from the second cell measured with a voltage applied thereto and calculates the specific gas component concentration based on the current. The calculator includes plural concentration calculating means whose concentration detecting ranges are mutually different in a scale. The specific gas component concentration is calculated every concentration calculating means.

The present invention is intended to prevent the deterioration of resolution due to increase in off-axis aberration resulting from the deviation of a primary electron bean from the optical axis of a scanning electron microscope. A scanning electron microscope is provided with an image shifting deflector system including two deflectors disposed respectively at upper and lower stages. The deflector disposed at the lower stage is a multipole electrostatic deflecting electrode and is disposed in an objective. Even if the distance of image shifting is great, an image of a high resolution can be formed and dimensions can be measured in a high accuracy. The SEM is able to achieving precision inspection at a high throughput when applied to inspection in semiconductor device fabricating processes that process a wafer having a large area and provided with very minute circuit elements.

The invention relates to a method for calibrating the transmitters of ultrasonic flow meters according to the transit time difference method. The object of the invention is to provide a method for calibrating the transmitters of ultrasonic flow meters, said calibration being able to be carried out independently of the other components of the meter, such as the acoustic transducers and the pipe in which the fluid flow being measured occurs. According to the invention, the measurement signals are generated by means of an artificial simulation of the measurement path. This allows the transmitter to be calibrated independently of the remaining components of the measuring apparatus, such as the measuring tube and the acoustic transducers.

A measuring apparatus includes a shape maintaining member that maintains a shape of at least a part of a subject, an element that receives an acoustic wave through the shape maintaining member and converts the acoustic wave into a first electric signal, the acoustic wave being generated in the subject when the subject is irradiated with light, and a processing unit that generates image data using the first electric signal. The processing unit determines, on the basis of the first electric signal, a first time from when the acoustic wave is generated in the subject to when the acoustic wave reaches a reception surface of the element. The processing unit converts the first electric signal into a second electric signal using a difference between the first time and a second time in which the acoustic wave travels from a virtual detection region set near a subject-side surface of the shape maintaining member to the reception surface of the element, the second electric signal being assumed to have been obtained by receiving the acoustic wave at the virtual detection region.

A phase locked loop including a flying-adder divider circuit configured to receive phases of a periodic signal from a frequency generator and output a feedback signal to a phase detector, and a method of generating a periodic signal using such a flying-adder circuit, are disclosed. The flying-adder divider circuit generally includes a flying-adder and one or two divide-by-N dividers. The flying-adder receives K phases of the periodic signal, where K is an integer of at least 2, and generates a divided periodic signal from the K phases. The phase locked loop may include flying-adder divider circuits inside and/or outside the loop.

A camera module compresses image data and produces a thumbnail image of this image data in FIFO order (First In First Out) by several lines of the image so as to enable transmission of the image data to the host module while significantly decreasing the size of the frame buffer memory. This can be achieved by, for example, an electronic device, including: a camera module, which transmits the data acquired by photographing; and a host module, which receives the data; wherein the camera module alternately transmits a compressed small portion including the data made by compressing the small portion of the image data for one frame and a sub small portion including the data with the resolution of the small portion reduced.

A method for forming a regularly repeating pattern on to a substrate comprising the steps of: applying a resist on a surface of a substrate to be processed; imprinting on the applied resist a pattern formed by exposing it to a beam of ultra violet (‘UV’) light, which has been caused to pass through a suitable mask delineating the pattern and then trough a focusing lens on to the resist, so as to cause chemical changes in the resist which makes it more or less soluble in a suitable developer solution; the imprinting step being carried out: in a repetitive series of discrete exposure steps using a mask held stationery with respect to the beam and the lens that represents only a small area of the total area of the substrate and using a single short pulse of UV radiation at each step to illuminate the mask, the radiation pulse having such an energy density at the substrate that it is below the threshold value for ablation of the resist; and the series of discrete exposure steps being repeated over the full area of the surface of a substrate, to give a full structure comprising a plurality of pixels, by moving the substrate in a direction parallel to one axis of the structure to be formed on the substrate and activating the pulsed mask illumination light source at the instant that the substrate has moved over a distance equivalent to a complete number of periods of the repeating pattern on the substrate; treating the exposed resist with a developer to cause either exposed regions (for positive resists) or unexposed regions (for negative resists) to be dissolved and subsequently washed away by the developer solution to reveal the pattern formed by the remaining resist; treating the substrate with a suitable chemical etching solution, reactive plasma or abrasive particles that removes the substrate in resist free areas; and removing remaining resist from the substrate with a suitable solvent to leave a finished patterned substrate.

The invention further comprises a scanning exposure tool for carrying out the method as aforesaid.

An interactive input system comprises at least one imaging device having a field of view looking into a region of interest. At least one radiation source emits radiation into the region of interest. A bezel at least partially surrounds the region of interest. The bezel comprises a multi-angle reflecting structure to reflect emitted radiation from the at least one radiation source towards the at least one imaging device.

The invention prevents the display unevenness of a high-resolution liquid crystal display device that results from the presence of regions where an alignment film is not applied. The invention provides a liquid crystal display device including: a TFT substrate having scan lines, video signal lines, and pixels formed by the intersecting scan lines and video signal lines; a counter substrate; and a liquid crystal layer placed between the TFT substrate and the counter substrate. Each of the pixels includes a TFT, a pixel electrode, a common electrode, and a through-hole and an opening that are used to connect the TFT and the pixel electrode. Connective ITO is formed in and around the through-hole at the same time as the common electrode is formed. A step d is formed at an edge portion of the connective ITO and covered with an alignment film.

A method for imaging an object using a microscope includes obtaining axial response data, the axial response data representative of a relationship between a separation between a top surface of the object and an objective lens of the microscope and an intensity of light reflected by the top surface of the object; positioning the object at a distance from the objective lens that is within a linear region of the axial response data; sequentially illuminating the object with a plurality of periodic patterns; obtaining a plurality of images of the object, each image resulting from the illumination of the object with a corresponding one of the plurality of periodic patterns; determining a reconstructed image of the object based on the plurality of images of the object; and, based on variations in the intensity of the reconstructed image, determining a topographic profile of the top surface of the object.

The invention discloses an image acquisition method and device, a mobile terminal and a storage medium, and particularly relates to the field of electronic equipment. The method comprises the steps: controlling a driving motor to drive an image acquisition module to move from a first position to a preset second position in a frame gap of image acquisition under the condition of identifying that the first position of the image acquisition module is not in the preset second position; receiving an angular velocity signal, the acquired next frame of image and the first position of the image acquisition module in the acquisition time period of the next frame of image acquired by the image acquisition module; when the first position of the image acquisition module does not return to the preset second position, cutting the acquired next frame of image according to the first position, the preset second position, the angular velocity signal and a preset electronic anti-shake algorithm; and under the condition that the first position returns to the preset second position, based on the angular velocity signal and the first position of the image acquisition module, controlling the driving motor to execute the optical anti-shake operation.