Abstract: A charge injection circuit is used to control injection of an electronic charge to be added to a photon-induced charge generated by a detector of a direct integration circuit. The electronic charge can be injected directly to the detector or through a parallel path to the detector.

Abstract: An imaging system is provided. The system includes a receiver to passively receive a millimeter wave (MMW) power level input from a scene and generates an analog output signal. A driver circuit receives the analog output signal and generates a drive output signal based on the amplitude of the analog output signal. A wavelength converter generates a light intensity output is a replica of a portion of the scene associated with the MMW power level input at a different wavelength range than the MMW power level input wavelength range.

Abstract: A system includes a first wearable terminal connected to a measurement device capable of measuring predetermined physical amounts and a second wearable terminal connected to a head-mounted display device, wherein the first wearable terminal includes a distance calculation means for calculating a distance from the second wearable terminal and a predicted value calculation means for calculating a predicted value of the predetermined physical amount at a position of the second wearable terminal based on a measurement value of the predetermined physical amount measured by the measurement device and the calculated distance, and the second wearable terminal includes a display control means for controlling to display the predicted value calculated by the predicted value calculation means on the head-mounted display device.

Abstract: A nuclear reactor fuel integrity monitor includes: a ?-ray detector which detects ?-ray of a specific radionuclide of a subject measurement medium of a nuclear reactor; a sample container which retains the subject measurement medium therein and surrounds the circumference of the ?-ray detector; and a measurement control device which performs a control so that a predetermined amount of the subject measurement medium is introduced into the sample container and calculates a concentration of the specific radionuclide from ?-ray data per each unit time detected by the ?-ray detector and a volume of the subject measurement medium introduced into the sample container.

Abstract: The invention is an imaging apparatus comprising a detector device (12) for determining points of incidence of photons and having an impact surface (13), and an aperture (16) suitable for projecting the photons to the detector device (12) having an inlet surface (17) and an outlet surface facing the impact surface (13), and comprising pinholes (18?, 18?, 22) connecting the inlet surface (17) and the outlet surface. The pinholes (18?, 18?, 22) comprise one or more central pinholes (18?, 22) and one or more peripheral pinholes (18?), and at least one central pinhole (18?, 22) and at least one peripheral pinhole (18?) are formed with focal opening (20?, 20?, 23) depth or focal opening (20?, 20?, 23) sizes different from each other. Furthermore, the invention is an aperture for the imaging apparatus and a method of manufacturing an aperture of an imaging apparatus.

Abstract: A passive radiometric imaging device and a corresponding method for scanning a scene and reconstructing an image of said scene provide an improved image quality. The device comprises a radiometer for detecting radiation and a processing means for subsequently determining pixel values of pixels of the image to be reconstructed. A cost calculation unit calculates costs for the radiation samples of said data sub-set according to a predetermined cost function, said costs indicating the level of noise in the respective radiation sample. An optimization unit determines a pixel value as a label value from a set of label values, a label indicating a radiation sample or a group of radiation samples of the respective data sub-set, by determining an extremum of energy values determined for different radiation samples or different groups of radiation samples of the respective data sub-set by use of an energy function.

Abstract: Embodiments of the present invention provide a method of providing image data for constructing an image of at least a region of a target object, comprising the steps of simultaneously recording, at a detector, a plurality of separable diffraction patterns formed by a respective portion of radiation scattered by the target object; and providing the image data via an iterative process responsive to the detected intensity of radiation.

Abstract: A hand-held portable radiation detection device, such as a radiation isotopic identification device (RIID), is integrated with a personal digital assistant device (PDA), such as a smart phone, to provide with improved data processing capability and user interface. The PDA is configured to receive and process data received from the radiation detection device.

Abstract: An ion implant apparatus and moveable ion beam current sensor are described. Various examples provide moving the ion beam current sensor during an ion implant process such that a distance between the ion beam current sensor and a substrate is maintained during scanning of the ion beam toward the substrate. The ion beam current sensor is disposed on a moveable support configured to move the ion beam current sensor in a first direction corresponding to the scanning of the ion beam while the substrate is moved in a second direction.

Abstract: An imaging apparatus includes a diffraction grating which diffracts electromagnetic waves from an electromagnetic wave source, a shield grating which shields a part of the electromagnetic waves diffracted by the diffraction grating, a detector which detects an intensity distribution of the electromagnetic waves through the shield grating, and an adjusting unit which adjusts the attitude of at least one of the diffraction grating and the shield grating on the basis of the detection result by the detector, wherein the adjusting unit divides the intensity distribution detected by the detector into a plurality of regions and adjusts the attitude of at least one of the diffraction grating and the shield grating on the basis of the intensity distributions of the plurality of regions.

Abstract: A radiation detector is offered which can suppress generation of sum peaks.

Abstract: A method for a constructing radiation detector includes fabricating a multi-layer structure upon a wafer, the multi-layer structure comprising a plurality of metal layers, a plurality of sacrificial layers, and a plurality of insulating layers, forming a cavity within the multi-layer structure, filling the cavity with a gas that ionizes in response to nuclear radiation, and sealing the gas within the cavity.

Abstract: An electromagnetic wakefield detector placed in close proximity to a design trajectory of a non-relativistic charged particle beam produces an optical signal in response to passage of the charged particle beam without interrupting the charged particle beam. A photon detector receives the optical signal and produces a corresponding output. The wakefield detector may be based on the electro optic effect. Specifically, the detector may measure the effect of the charged particle beam a beam of radiation on the phase of radiation travelling parallel to the beam in a nearby electro optic waveguide. This abstract is provided to comply with rules requiring an abstract that will allow a searcher or other reader to quickly ascertain the subject matter of the technical disclosure. It is submitted with the understanding that it will not be used to interpret or limit the scope or meaning of the claims.

Abstract: A photon detector article includes a photon detector configured to receive a primary waveform, the photon detector includes a multiplication region; a photon absorption region; a punch through voltage range; and a breakdown voltage; a source in electrical communication with the photon detector and configured to provide the primary waveform that includes a first voltage that is: less than a maximum value of the punch through voltage range, or effective to maintain a charge carrier in the absorption region; and a second voltage that is greater than the breakdown voltage; and a reference member in electrical communication with the source and configured to provide a reference waveform in response to receiving the primary waveform.

Abstract: Described is a method and system that facilitates triage of thousands to millions of potential patients within a relatively short period of time by scanning of a substrate of a designated card issued to a victim. The method and the system comprise a plurality of noninvasive self-testing test devices located at a plurality of remote peripheral self-testing sites, and each one of the plurality of noninvasive self-testing test devices facilitates self-testing of the substrate of the designated card. Each of the plurality of noninvasive self-testing test devices provides test results of the scan of the substrate of the designated card, and the potential patients are identified, then subsequently screened and triaged based upon the test results of the scan of the substrate of the designated card.

Abstract: In accordance with some embodiments, an assembly of an ion implanter system is provided. The assembly includes a control unit, a wafer holder and a detecting device. The wafer holder and the detecting device are respectively positioned at two sides of the control unit. The control unit is configured to drive the wafer holder and the detecting device to rotate about at least one rotation axis.

Abstract: In one embodiment, a method for producing a high-purity single crystal of aluminum antimonide (AlSb) includes providing a growing environment with which to grow a crystal, growing a single crystal of AlSb in the growing environment which comprises hydrogen (H2) gas to reduce oxide formation and subsequent incorporation of oxygen impurities in the crystal, and adding a controlled amount of at least one impurity to the growing environment to effectively incorporate at least one dopant into the crystal. In another embodiment, a high energy radiation detector includes a single high-purity crystal of AlSb, a supporting structure for the crystal, and logic for interpreting signals obtained from the crystal which is operable as a radiation detector at a temperature of about 25° C. In one embodiment, a high-purity single crystal of AlSb includes AlSb and at least one dopant selected from a group consisting of selenium (Se), tellurium (Te), and tin (Sn).

Abstract: A carrier includes attachment holes to which a catalyst attaches, and non-attachment holes to which the catalyst does not attach. An attachment quantity measurement device includes an electromagnetic wave output device that outputs a terahertz wave toward the carrier, an electromagnetic wave detector that detects the terahertz wave which has transmitted through the carrier, a reference value obtainer that obtains, based on a result detected by the electromagnetic wave detector, any one of an absorption rate, a group delay, and a dispersion of the terahertz wave in the non-attachment holes, and an attachment quantity obtainer that obtains, based on the result detected by the electromagnetic wave detector and the result obtained by the reference value obtainer, a weight or a density of the catalyst present in the attachment holes.

Abstract: A material inspection apparatus according to the present embodiment includes a sample mount capable of mounting a sample. A detector detects an ion desorbed from the sample. A voltage generator applies a voltage to the sample. An optical system irradiates a laser beam onto the sample at a tilt angle with respect to a perpendicular direction to an end surface of a tip end of the sample. The tilt angle is equal to or smaller than a Brewster angle.

Abstract: A hand-held portable radiation detection device, such as a radiation isotopic identification device (RIID), is integrated with a personal digital assistant device (PDA), such as a smart phone, to provide with improved data processing capability and user interface. The PDA is configured to receive and process data received from the radiation detection device.

Abstract: A radiographic image capture device of the present invention includes: a radiation detection panel including a photoelectric conversion element that converts radiation into an electrical signal; a signal processing board that is disposed facing towards the radiation detection panel and that performs signal processing on electrical signals obtained by the radiation detection panel; a flexible substrate that includes wiring lines disposed on a base film provided between the radiation detection panel and the signal processing board and including a low wiring density region and a high wiring density region, and electronic component(s) that are electrically connected to the wiring lines; a reinforcement member that is provided at a low wiring density region and that raises the mechanical strength of the wiring lines.

Abstract: A compressive scanning approach for millimeter wave imaging and sensing. A Hadamard mask is positioned to receive millimeter waves from an object to be imaged. A subset of the full set of Hadamard acquisitions is sampled. The subset is used to reconstruct an image representing the object.

Abstract: The techniques described herein provide for correcting for pulse pile-up and/or charge sharing in a radiation scanner (100). It finds particular application with the use of a pixilated radiation detector (116) (e.g., a photon counting detector). A circuit (200), comprising a plurality of comparators (204, 206, 208), is configured to determine the energy spectrum of a pulse produced from a photon strike. If the energy spectrum is greater than the energy range for a pulse produced by a single photon strike given an input spectrum and/or if pulses produced from adjacent pixels have temporal coincidence, pulse pile-up and/or charge sharing may be identified and a correction mechanism/correction factors may be applied to determine an actual number of photons that struck the detector (116).

Abstract: A secondary charged particle detection device for detection of a signal beam is described. The device includes a detector arrangement having at least two detection elements with active detection areas, wherein the active detection areas are separated by a gap (G), a particle optics configured for separating the signal beam into a first portion of the signal beam and into at least one second portion of the signal beam, and configured for focusing the first portion of the signal beam and the at least one second portion of the signal beam. The particle optics includes an aperture plate and at least a first inner aperture openings in the aperture plate, and at least one second radially outer aperture opening in the aperture plate, wherein the first aperture opening has a concave shaped portion, particularly wherein the first aperture opening has a pincushion shape.

Abstract: A detector module (50) for a positron emission tomography (PET) system (10) includes an optical transceiver (66) receiving an optical data stream from a PET processing system (48). The data stream includes a pulse train carrying a command to generate sync/reset pulses. The system (10) further includes synchronization circuitry (70) configured to simultaneously jitter clean the pulse train and one of: 1) count the pulses of the pulse train; and 2) monitor the pulse train for a missing pulse. The synchronization circuitry (70) is further configured to, in response to counting a predetermined number of pulses or detecting the missing pulse, extract a jitter clean pulse from the pulse train to generate a jitter clean sync/reset pulse. The system (10) further includes an internal clock (64) which receives the jitter clean sync/reset pulse.

Abstract: A vehicle detection device includes: an antenna configured to sense electromagnetic waves; an image generation unit configured to generate a radio wave image; a road surface region detection unit configured to detect a road surface region in the radio wave image; a symmetry axis setting unit configured to set a first symmetry axis at a part of the boundary of the road surface region; a road surface reflection region setting unit configured to set a horizontal central line at a center of the radio wave image and set a road surface reflection region between the central line and the first symmetry axis; and a vehicle detection unit configured to compare the waveform of pixel outputs in the road surface reflection region with the waveform of pixel outputs in the road surface region and to detect the road surface reflection region as a vehicle.

Abstract: An optical sensing module including a lens and a sensing device is provided. The lens has an optical axis. The sensing device is disposed under the lens, wherein the sensing device is to receive an object beam passing the lens. The optical axis of the lens deviates from a geometric center of the sensing device. An optical sensing module including a prism film, a sensing device and a lens is further provided. The prism film has a plurality of prisms. The sensing device is disposed under the prism film, wherein the sensing device is to receive an object beam sequentially passing the prism film and the lens. The lens is disposed between the prism film and the sensing device.

Abstract: A system and method for determining a probability of the location of an illicit radiation source within an environment based on directional detectors. An embodiment includes a plurality of directional radiation detectors distributed about the environment and integrated with a processing unit adapted to determine the probability of the source location based on the radiation count data received from the plurality of detectors. The processing unit is further adapted to output information indicative of the location of the radiation source within the environment.

Abstract: Apparatus and a method for intercepting a rocket body during boost phase. A sensor is arranged to detect thermal emission in a range that is characteristic of a firing rocket body. The image detected by the sensor is applied to an analog-to-digital converter for digitization and application to a computer that includes a routine for separating the modulated photon energy of the detected image from the substantially unmodulated photon energy that characterizes rocket body emissions. The unmodulated photon energy, signature of the rocket body, may be utilized by a fire control system for tracking, targeting and aiming munitions at the firing rocket body.

Abstract: A system for analyzing an electron beam including a circular electron beam diagnostic sensor adapted to receive the electron beam, the circular electron beam diagnostic sensor having a central axis; an annular sensor structure operatively connected to the circular electron beam diagnostic sensor, wherein the sensor structure receives the electron beam; a system for sweeping the electron beam radially outward from the central axis of the circular electron beam diagnostic sensor to the annular sensor structure wherein the electron beam is intercepted by the annular sensor structure; and a device for measuring the electron beam that is intercepted by the annular sensor structure.

Abstract: A radiation imaging apparatus, comprising a sensor array in which a plurality of sensors are arranged, each includes a first holding unit for holding a first signal obtained with a first sensitivity and a second holding unit for holding a second signal obtained with a second sensitivity, a row selecting unit for selecting each sensor on a row basis, a signal readout unit for reading out a signal from each of the selected sensors, and a control unit configured to perform first control to control the sensor array so as to make the first holding units hold the first signals and make the second holding units hold the second signals, and perform second control to control the row selecting unit so as to make the signal readout unit read out the first and the second signals.

Abstract: An instrument for assaying radiation includes a flat panel detector having a first side opposed to a second side. A collimated aperture covers at least a portion of the first side of the flat panel detector. At least one of a display screen or a radiation shield may cover at least a portion of the second side of the flat panel detector.

Abstract: An antenna array includes a plurality of antenna elements. The antenna elements include layers of dielectric material; an antenna inlaid in a top layer of the dielectric material so a surface of the antenna is substantially parallel to an outer surface of the top layer of dielectric material; and a conductive balun, coupled to the antenna, and embedded in one or more layers of the dielectric material. The antenna array is operative to receive signals from V to W frequency band transmissions generated by a heat source.

Abstract: A radioactive waste body inspection device according to an embodiment includes a surface contamination inspecting unit configured to conduct a surface contamination inspection of a radioactive waste body while acquiring concavo-convex information on the radioactive waste body, and a dose rate inspecting unit configured to conduct a dose rate inspection of the radioactive waste body in consideration of the concavo-convex information.

Abstract: A miner's personal gas alarm can be mounted in a helmet powered by a rechargeable battery for a light or be self-contained. A visual indicator will generate an alarm when the concentration of gas detected by the gas sensor triggers an alarm condition. An audio alarm can also be generated by the alarm condition. The gas sensor is a non-dispersive infrared (“NDIR”) gas sensor. When the gas sensor detects methane, the alarm condition is triggered by either an abnormally high rate of increase of methane concentration level or by an elevated concentration of methane that is above approximately 500 ppm and substantially below a lower explosion limit of methane (e.g., approximately 10,000 ppm), and the gas sensor is recalibrated whenever the sample concentration of methane falls below an ambient threshold level of methane.

Abstract: A CT system includes a rotatable gantry having an opening for receiving an object to be scanned, an x-ray source configured to project x-rays through the opening, and a detector assembly positioned to receive the x-rays. The detector assembly includes a plurality of readout chips positioned within a cooling zone and configured to receive electrical signals from a plurality of diode arrays, and a fan positioned to blow air into the cooling zone. An air temperature within the cooling zone is controlled independent of a speed of the fan.

Abstract: A transmission X-ray analyzer for detecting a transmission X-ray image of a sample that moves relatively in a predetermined scanning direction includes; a time delay and integration (TDI) sensor including a plurality of stages of line sensors including the plurality of two-dimensionally arranged image pickup devices arranged in a direction perpendicular to the predetermined scanning direction, being configured to transfer charge accumulated in one line sensor to an adjacent subsequent line sensor; a shield unit for shielding a part of the image of light entering the TDI sensor by moving back and forth in the predetermined scanning direction, the shield unit being disposed between the TDI sensor and the sample; and a shield unit position control unit for controlling a position of the shield unit so as to shield a predetermined number of stages of line sensors among the plurality of stages of line sensors.

Abstract: An apparatus for ultrasensitive long-wave imaging cameras is provided. In one embodiment, the apparatus includes a filter configured to allow high frequencies of interest to pass through the filter. The apparatus also includes an antenna that is configured to receive the high frequencies of interest. The apparatus further includes a plurality of bolometers that are configured to measure data regarding the high frequencies of interest.

Abstract: The image obtaining unit obtains a radiation image from the radiation detector, the radiation field area detection unit detects a radiation field area from the radiation image. The analysis area setting unit detects a direct radiation area, a superabsorbent body area, and a high noise area as the areas where a periodic pattern is unlikely to present and sets an analysis area by excluding these areas. The frequency analysis unit performs a frequency analysis only on the analysis area and detects a frequency component of the periodic pattern arising from a grid. The filtering processing unit removes the frequency component of the periodic pattern arising from the grid from the radiation image.

Abstract: An apparatus, method, computer-readable medium, and system for adjusting data acquisition parameters during a scan performed by a Positron Emission Tomography (PET) scanner. The method includes obtaining, during the scan, a current temperature of a detector of the PET scanner, and adjusting, based on the current temperature, the data acquisition parameters used by the PET scanner during the scan.

Abstract: The invention provides a switchable photomultiplier switchable between a detecting state and a non-detecting state including a cathode upon which incident radiation is arranged to impinge. The photomultiplier also includes a series of dynodes arranged to amplify a current created at the cathode upon detection of photoradiation. The invention also provides a detection system arranged to detect radiation-emitting material in an object. The system includes a detector switchable between a detecting state in which the detector is arranged to detect radiation and a non-detecting state in which the detector is arranged to not detect radiation. The system further includes a controller arranged to control switching of the detector between the states such that the detector is switched to the non-detecting state whilst an external radiation source is irradiating the object.

Abstract: A computation apparatus that calculates information of a subject includes: a calculation unit configured to calculate a spatial distribution of a first first-order phase value, a spatial distribution of a second first-order phase value, and a spatial distribution of a first-order measurement target value, by using the subject data; a calculation unit configured to calculate an error correction function including the first first-order phase value and the second first-order phase value as variables, by using information of the spatial distribution of the first first-order phase value, information of the spatial distribution of the second first-order phase value, and information of the spatial distribution of the first-order measurement target value; and a calculation unit configured to calculate information of a spatial distribution of a second-order measurement target value, corresponding to a spatial distribution obtained by correcting the spatial distribution of the first-order measurement target value.

Abstract: An X-ray detector includes a light receiver configured to generate charges of a quantity corresponding to energy of a photon, a comparison device including a plurality of comparators, each of the comparators being configured to compare a voltage signal corresponding to the quantity of the generated charges with a respective threshold voltage and output a result of the comparison as a pulse signal, a counter device including a plurality of counters, each of the counters being configured to count a pulse of a certain state, and a synchronous control circuit configured to receive as input the pulse signals output from each of the comparators and to output the pulse of the certain state to one of the counters corresponding to a highest threshold voltage of the threshold voltages which is less than a peak value of the voltage signal.

Abstract: The present disclosure relates to a method and a system for generating low-energy electrons in a biological material. The biological material is held in position by a support. Laser beam pulses are directed by a focusing mechanism toward a region of interest within the biological material. This generates filaments of low-energy electrons within the region of interest. The method and system may be used for radiotherapy, radiochemistry, sterilization, nanoparticle coating, nanoparticle generation, and like uses.

Abstract: The invention relates to a detection apparatus for detecting photons, such as used in radiographic imaging systems. A detection unit (14) generates detection signal pulses having a detection signal pulse height being indicative of the energy of the detected photons (13), wherein a detection values generation unit (16) generates energy-resolved detection values depending on the detection signal pulses. A signal pulse generation unit (15) generates artificial signal pulses having a predefined artificial signal pulse height and a predefined generated rate. The detection values generation unit (16) determines an observed rate being the rate of the artificial signal pulses having an artificial signal pulse height being larger than a predefined threshold as observed by the detection values generation unit (16) and determines an offset of the detection signal pulses depending on the determined observed rate.

Abstract: The present invention relates to an x-ray detector comprising a sensor unit (200, 300) for detecting incident x-ray radiation comprising a number of sensor elements (230, 311-314), a counting channel (240) per sensor element for obtaining a count signal by counting photons or charge pulses generated in response to the incident x-ray radiation since a beginning of a measurement interval, an integrating channel (250) per sensor element for obtaining an integration signal representing the total energy of radiation detected since the beginning of the measurement interval, and a processing unit (260) for estimating, from the integration signals of the sensor elements (321), count signals of sensor elements (311, 312) whose counting channel has been saturated during the measurement interval.

Abstract: The present invention relates to a low-resistance MCP with an expanded dynamic range and excellent environment resistance, in comparison with the conventional technology. The MCP has a double structure composed of hollow first cladding glasses whose inner wall surfaces function as channel walls, and a second cladding glass having an acid resistance lower than that of the first cladding glasses.

Abstract: An inspection apparatus by an electron beam comprises: an electron-optical device 70 having an electron-optical system for irradiating the object with a primary electron beam from an electron beam source, and a detector for detecting the secondary electron image projected by the electron-optical systems; a stage system 50 for holding and moving the object relative to the electron-optical system; a mini-environment chamber 20 for supplying a clean gas to the object to prevent dust from contacting the object; a working chamber 31 for accommodating the stage device, the working chamber being controllable so as to have a vacuum atmosphere; at least two loading chambers 41, 42 disposed between the mini-environment chamber and the working chamber, adapted to be independently controllable so as to have a vacuum atmosphere; and a loader 60 for transferring the object to the stage system through the loading chambers.

Abstract: An imaging device capable of obtaining image data with a small amount of X-ray irradiation is provided. The imaging device obtains an image using X-rays and includes a scintillator and a plurality of pixel circuits arranged in a matrix and overlapping with the scintillator. The use of a transistor with an extremely small off-state current in the pixel circuits enables leakage of electrical charges from a charge accumulation portion to be reduced as much as possible, and an accumulation operation to be performed substantially at the same time in all of the pixel circuits. The accumulation operation is synchronized with X-ray irradiation, so that the amount of X-ray irradiation can be reduced.

Abstract: The present invention provides, at low cost, a multilayer radiation detector whose position relative to a beam axis can be verified. The radiation detector includes a plurality of sensors that react to radiation and are stacked in parallel inlayers in a traveling direction of the radiation. The sensors are each sectioned into a central region including the center of the sensor and another region surrounding the central region. The radiation detector independently measures signals measured by the central regions and signals measured by the other regions. Thus, the position of the radiation detector can be verified.