Abstract: A method and system is disclosed for acquiring image data of a subject. The image data can be collected with an imaging system in a selected manner and/or motion. More than one projection may be combined to generate and create a selected view of the subject.

Abstract: A cerebral infarction treatment support system (100) includes a detection device (10), a display (30), and an image controller (20), and the image controller (20) includes a receiver (21) configured to receive at least one of first information (41) generated by the detection device (10) or second information (42) related to a susceptibility gene generated based on the first information (41), and a video output (22) configured to output at least one of the received first information (41) or second information (42) to the display (30).

Abstract: A radon gas sensor comprising: a diffusion chamber; a photodiode positioned inside the diffusion chamber; and a photomultiplier positioned inside the diffusion chamber; wherein a scintillating material is provided on at least a part of an inner surface of the diffusion chamber. The photomultiplier detects more alpha particles, but cannot distinguish the energies of different alpha particles. On the other hand, the photodiode can distinguish different decays because the magnitude of the signal generated by the photodiode is proportional to the kinetic energy of the alpha particle striking it. Thus, the photodiode produces spectral data. The spectral data is used to estimate the amount of Polonium that is adhering to aerosols. This is used to apply a correction factor to the data to provide a better estimate of the true Radon concentration in the chamber. This can be combined with the count data of the photomultiplier for overall improved data.

Abstract: A method is provided for count loss correction based on detector dead time in a radiation diagnosis apparatus. The method includes acquiring scan data from a scan of a patient performed using the radiation diagnosis apparatus; determining, from the acquired scan data, a first count rate occurring in a first energy window spanning a first energy range; determining, from the acquired scan data, a second count rate occurring in a second window spanning a second energy range, the second energy range being different from the first energy range; calculating a particular count loss correction factor based on the determined first count rate and the determined second count rate; and reconstructing an image based on the acquired scan data and the calculated particular count loss correction factor.

Abstract: A radiative cooling device that is in a state in which a radiative surface is colored is provided. A radiative cooling device CP includes an infrared radiative layer A that radiates infrared light IR from a radiative surface H, a light reflective layer B that is disposed on the side opposite to the radiative surface H with respect to the infrared radiative layer A, and a color portion X. The infrared radiative layer A is a resin material layer J that has a thickness adjusted so as to emit a heat radiation energy greater than an absorbed solar energy in a wavelength range from 8 ?m to 14 ?m, and the color portion X contains a colorant that absorbs light in the visible range.

Abstract: A device for detecting monocrystalline substrate defects, wherein a normal to the surface of the substrate is tilted by a tilt angle being contained in an angle plane, perpendicular to the surface, the device includes a detector, an illumination light source having a light beam, and arranged in a first position and/or a second position, an excitation light source illuminating the substrate and producing an emission of photoluminescence light by the substrate, imaging means imaging the substrate according to a detector field of view producing at least one image of the substrate, and processing means detecting crystalline defects using the substrate image, each illumination light source and the imaging means are arranged in a dark-field configuration, and in the first position, the illuminating light beam is parallel or quasi-parallel to the angle plane, and in the second position, the illuminating light beam is parallel or quasi-parallel to a perpendicular plane.

Abstract: A method of detecting fluorescence from bacteria suitable for determining the presence of faeces or other fluorophores, the method comprising the steps of: illuminating a target with fluorescence excitation light having an excitation wavelength and monitoring for the emission of fluorescence light from the target at wavelengths longer than the excitation wavelength.

Abstract: There is described a terahertz modulation system. The terahertz modulation system generally has a terahertz signal emitter emitting a terahertz signal along a path; a modulation unit having a substrate and an electromechanical transducer actuatably mounted to said substrate, said electromechanical transducer having a terahertz interacting surface in said path receiving said terahertz signal and moving in back-and-forth sequences between first and second positions relative to said path upon actuation with a modulation signal, said moving modulating at least a portion of said terahertz signal; and a terahertz signal detector downstream from said modulation unit along said path, said terahertz signal detector synchronously measuring said modulated portion of said terahertz signal using said modulation signal, and generating a differential signal indicative thereof.

Abstract: In a method for regulating a position of an X-ray focus on the anode of an X-ray source of a scan unit of an X-ray imaging system, a combined actual position of the X-ray focus is determined by a combination of a measured position of the X-ray focus and a model-based position of the X-ray focus, which is determined based on a measured value of a deflection current. On the basis of the combined actual position and a target position, a manipulated variable is determined. On the basis of the determined manipulated variable, a regulation is performed to correct a deviation of the position of the X-ray focus from the target position.

Abstract: A photon counting circuit, a radiographic imaging apparatus, and a threshold setting method are provided, in which the photon counting circuit is capable of sufficiently reducing a difference between a target threshold value and a threshold value set for a pixel even if each pixel of a photon counting detector is divided into a plurality of subpixels. In the photon counting circuit for counting, for each pixel, electrical charges generated depending on photon energy of radiation applied to an object, a pixel is divided into a plurality of subpixels. When N is a natural number, a threshold value of each of the subpixels is selected from among top N discrete values of a plurality of discrete values arranged in order of proximity to a target threshold value corresponding to the photon energy so as to minimize a difference between the target threshold value and an average of the threshold values of the respective subpixels included in the pixel.

Abstract: A metrology system includes a light beam metrology apparatus configured to sense one or more aspects of an amplified light beam and to make adjustments to the amplified light beam based on the sensed one or more aspects; a target metrology apparatus configured to measure one or more properties of a modified target after a target has interacted with the amplified light beam, and to determine a moment when the modified target achieves a reference calibration state; and a control apparatus configured to: receive the reference calibration state and the moment at which the reference calibration state is achieved from the target metrology apparatus; determine a light beam calibration state of the amplified light beam based on the received reference calibration state and the moment at which the reference calibration state is achieved; and provide the light beam calibration state to the light beam metrology apparatus.

Abstract: Methods and systems are provided for contrast-to-noise evaluation in medical imaging systems. In one embodiment, a method includes positioning a phantom having a variable width cross-section within a gantry of a computed tomography (CT) system so that the variable width cross-section is perpendicular to a central axis of the CT system, adjusting the phantom within the gantry of the CT system to a first imaging configuration having a first position and a first translation within the gantry, acquiring a first set of measurements from the phantom in the first imaging configuration, and calculating a contrast-to-noise ratio (CNR) of the CT system based on at least the first set of measurements and a first material density of an imaged slice of the phantom in the first imaging configuration.

Abstract: Provided is a new and improved method for examining the penetration of fragments in ballistic gelatin through the use of state-of-the art computed tomography (CT) equipment and analytical software. The inventive method can be used for fragment penetration testing as a key performance parameter (KPP). Ballistic gel containing multiple fragments are obtained, placed in a container, positioned in a CT chamber, and scanned. The scan is imported into a Volume graphics software program. A surface determination is made, which is used by one or more algorithms to isolate potential fragmentation within the gel block. The number of fragments, depth of penetration, and fragment mass are then calculated.

Abstract: Systems and methods of profiling a charged-particle beam are disclosed. The method of profiling a charged-particle beam may comprise activating a charged-particle source to generate the charged-particle beam along a primary optical axis, modifying the charged-particle beam by adjusting an interaction between the charged-particle beam and a standing optical wave, detecting charged particles from the modified charged-particle beam after the interaction with the standing optical wave, and determining a profile of the charged-particle beam based on the detected charged particles. Alternatively, the method may include activating an optical source, modifying the optical beam by adjusting an interaction between the optical beam and a charged-particle beam, detecting an optical signal from the modified optical beam, and determining a characteristic of the charged-particle beam based on the detected optical signal.

Abstract: Aspects of the present disclosure may include a method and/or a system for identifying an ion chain having a plurality of trapped ions, selecting at least two non-consecutive trapped ions in the ion chain for implementing a qubit, applying at least a first Raman beam to shuttle at least one neighbor ion of the at least two non-consecutive trapped ions from a ground state to a metastable state, and applying at least a second Raman beam to one or more of the at least two non-consecutive trapped ions, after shuttling the at least one neighbor ion to the metastable state, to transition from a first manifold to a second manifold.

Abstract: The laminated glass of the present invention has a T/R rate (A) of larger than 1, the T/R rate (A) being calculated from the following formula (1): T/R rate (A)=log 10(TA/100)/log 10(RA/100)??(1) wherein an average transmittance at a wavelength of 900 to 1300 nm through one face is represented by TA, and a maximum reflectance at a wavelength of 900 to 1300 nm at an incident angle of 60° on the other face is represented by RA.

Abstract: A device and a spectrometer for quantitatively detecting carbon 14 isotope by a dual-wavelength method. Two mid-infrared lasers with different wavelengths are locked in an optical cavity of a sample chamber, to ensure the two lasers are collinear. The cavity length of the optical cavity is adjusted by a cavity length adjusting unit, to tune the mode frequency of the optical cavity, and then tune the frequencies of the two mid-infrared lasers, so that the frequencies of the two mid-infrared lasers match with different energy levels of the target isotope molecule simultaneously. After the frequencies of the mid-infrared lasers match with the energy levels of the target isotope molecule simultaneously, the target isotope molecule is excited by two mid-infrared lasers simultaneously, and the optical cavity output signal of the second mid-infrared laser passing through the optical cavity is detected.

Abstract: Multicolor analysis is enabled while suppressing increase in size.

Abstract: An X-ray detection system is described having a solid-state detector module including a plurality of detector tiles at a first side thereof for directly detecting X-ray radiation. The detector module has a plurality of interstitial areas separating adjacent tiles of the detector module, and at least one actuator for inducing motion of the detector module to a plurality of detection positions along a trajectory with respect to a stationary reference frame while the detector module is operated in an exposure mode. The spatial extent of the trajectory in the stationary reference frame is at least as large as the largest interstitial area, and the detector module is adapted for acquiring a plurality of frames in the exposure mode at a frame acquisition rate at least a factor of 100 faster than the inverse of a predetermined exposure time for the exposure mode.

Abstract: The present disclosure provides a gamma camera imaging method and a gamma camera imaging device. The method includes: selecting, from energy spectrums captured by a gamma camera on one or more radioactive materials, one or more energy ranges of each radioactive material among the one or more radioactive materials as one or more monitored energy regions of the radioactive material; performing image reconstruction on the monitored energy regions of each radioactive material among the one or more radioactive materials; performing normalization on images obtained through the image reconstruction; and performing superimposing on the normalized images to form a composite image.