Abstract: A pixel array uses two sets of pixels to provide accurate exposure control. One set of pixels provide continuous output signals for automatic light control (ALC) as the other set integrates and captures an image. ALC pixels allow monitoring of multiple pixels of an array to obtain sample data indicating the amount of light reaching the array, while allowing the other pixels to provide proper image data. A small percentage of the pixels in an array is replaced with ALC pixels and the array has two reset lines for each row; one line controls the reset for the image capture pixels while the other line controls the reset for the ALC pixels. In the columns, at least one extra control signal is used for the sampling of the reset level for the ALC pixels, which happens later than the sampling of the reset level for the image capture pixels.

Abstract: An image sensor controls the gain of a pixel signal on a pixel-by-pixel basis and extends a dynamic range while maintaining a S/N ratio at a favorable level. A column unit in an image sensor is independently detects a level of each pixel signal and independently sets a gain for level of the signal. A photoelectric converting region unit has pixels arranged two-dimensionally with a vertical signal line for each pixel column to output each pixel signal. The column unit is on an output side of the vertical signal line. The column unit for each pixel column has a pixel signal level detecting circuit, a programmable gain control, a sample and hold (S/H) circuit. Gain correction is performed according to a result of a detected level of the pixel signal.

Abstract: A vertical shift register section includes M logic circuits for outputting row selection control signals respectively to M row selection wiring lines and shift register circuits disposed for every two row selection wiring lines. The M logic circuits, when a binning control signal Vbin1 or Vbin2 and an output signal of the shift register circuit both have significant values, output a row selection control signal Vsel so as to close a readout switch. The vertical shift register section, by controlling the timing at which the binning control signals Vbin1 and Vbin2 take significant values, realizes a normal operation mode for successively selecting the two row selection wiring lines and a binning operation mode for simultaneously selecting the two row selection wiring lines. Accordingly, a vertical binning operation is realized by a small vertical shift register.

Abstract: A controlling section, by bringing readout switches of pixels of a certain row out of the M rows into a connected state, causes charges generated in the row to be input to integration circuits, causes first holding circuits to hold voltage values output from the integration circuits, and then brings transfer switches into a connected state to transfer the voltage values to the second holding circuits, and thereafter performs in parallel an operation for causing the voltage values to be sequentially output from the second holding circuits and an operation for, by bringing readout switches of pixels of another row into a connected state, causing charges generated in the row to be input to the integration circuits. Accordingly, a solid-state imaging device and a driving method thereof capable of suppressing variations in output characteristics, while solving the problem due to a delay effect are realized.

Abstract: Optical computing devices containing one or more integrated computational elements may be used to produce two or more detector output signals that are computationally combinable to determine a characteristic of a sample. The devices may comprise a first integrated computational element and a second integrated computational element, each integrated computational element having an optical function associated therewith, and the optical function of the second integrated computational element being at least partially offset in wavelength space relative to that of the first integrated computational element; an optional electromagnetic radiation source; at least one detector configured to receive electromagnetic radiation that has optically interacted with each integrated computational element and produce a first signal and a second signal associated therewith; and a signal processing unit operable for computationally combining the first signal and the second signal to determine a characteristic of a sample.

Abstract: Optical computing devices are disclosed. One exemplary optical computing device includes an electromagnetic radiation source configured to optically interact with a sample and at least two integrated computational elements. The at least two integrated computational elements are configured to produce optically interacted light and further configured to be associated with a characteristic of the sample. The optical computing device further includes a first detector arranged to receive the optically interacted light from the at least two integrated computational elements and thereby generate a first signal corresponding to the characteristic of the sample.

Abstract: Optical computing devices are disclosed. One exemplary optical computing device includes an electromagnetic radiation source configured to optically interact with a sample and at least two integrated computational elements. The at least two integrated computational elements may be configured to produce optically interacted light, and at least one of the at least two integrated computational elements may be configured to be disassociated with a characteristic of the sample. The optical computing device further includes a first detector arranged to receive the optically interacted light from the at least two integrated computational elements and thereby generate a first signal corresponding to the characteristic of the sample.

Abstract: Optical computing devices are disclosed. One exemplary optical computing device includes an electromagnetic radiation source configured to optically interact with a sample and at least two integrated computational elements. The at least two integrated computational elements are configured to produce optically interacted light and further configured to be associated with a characteristic of the sample. The optical computing device further includes a first detector arranged to receive the optically interacted light from the at least two integrated computational elements and thereby generate a first signal corresponding to the characteristic of the sample.

Abstract: Optical computing devices are disclosed. One exemplary optical computing device includes an electromagnetic radiation source configured to optically interact with a sample and at least two integrated computational elements. The at least two integrated computational elements may be configured to produce optically interacted light, and at least one of the at least two integrated computational elements may be configured to be disassociated with a characteristic of the sample. The optical computing device further includes a first detector arranged to receive the optically interacted light from the at least two integrated computational elements and thereby generate a first signal corresponding to the characteristic of the sample.

Abstract: Optical computing devices are disclosed. One exemplary optical computing device includes an electromagnetic radiation source configured to optically interact with a sample and first and second integrated computational elements arranged in primary and reference channels, respectively. The first and second integrated computational elements produce first and second modified electromagnetic radiations, and a detector is arranged to receive the first and second modified electromagnetic radiations and generate an output signal corresponding to the characteristic of the sample.

Abstract: Optical computing devices are disclosed. One exemplary optical computing device includes an electromagnetic radiation source configured to optically interact with a sample and first and second integrated computational elements arranged in primary and reference channels, respectively. The first and second integrated computational elements produce first and second modified electromagnetic radiations, and a detector is arranged to receive the first and second modified electromagnetic radiations and generate an output signal corresponding to the characteristic of the sample.

Abstract: Optical computing devices are disclosed. One exemplary optical computing device includes an electromagnetic radiation source configured to optically interact with a sample and first and second integrated computational elements arranged in primary and reference channels, respectively, the first and second computational elements are configured to be either positively or negatively correlated to the characteristic of the sample. The first and second integrated computational elements produce first and second modified electromagnetic radiations, and a detector is arranged to receive the first and second modified electromagnetic radiations and generate an output signal corresponding to the characteristic of the sample.

Abstract: An input clamping circuit of a photo detector preamplifier is activated when an input transistor is turned off by an input overload, and the drain voltage of the input transistor is pulled toward ground by a current source. Even with extreme overloads, the operating conditions (Vgs and Id) of the input transistor remain within normal range. During normal operation, the clamping circuit is biased completely off, and has essentially no effect on circuit performance. Since the input FET itself, rather than a separate device, detects the onset of an overload, significantly improved clamping performance is realized without adding additional circuit complexity. The input transistor can be a FET. The preamplifier can be a cascode preamplifier. The clamping circuit can include a clamping FET or other clamping transistor gated by the input transistor drain. In embodiments, the clamping circuit increases current requirements of the preamplifier by no more than 25%.

Abstract: A system for a feedback transimpedance amplifier with sub-40 khz low-frequency cutoff is disclosed and may include amplifying electrical signals received via coupling capacitors utilizing a transimpedance amplifier (TIA) having feedback paths comprising source followers and feedback resistors. Gate terminals of the source followers mey be coupled to output terminals of the TIA. The feedback paths may be coupled prior to the coupling capacitors at inputs of the TIA. Voltages may be level shifted prior to the coupling capacitors to ensure stable bias conditions for the TIA. The TIA may be integrated in a CMOS photonics chip and the source followers may comprise CMOS transistors. The TIA may receive current-mode logic or voltage signals. The electrical signals may be received from a photodetector, which may comprise a silicon germanium photodiode differentially coupled to the TIA. Optical signals for the photodetector in the CMOS photonics chip may be received via optical fibers.

Abstract: Optical computing devices are disclosed. One exemplary optical computing device includes an electromagnetic radiation source configured to optically interact with a sample and first and second integrated computational elements arranged in primary and reference channels, respectively, the first and second computational elements are configured to be either positively or negatively correlated to the characteristic of the sample. The first and second integrated computational elements produce first and second modified electromagnetic radiations, and a detector is arranged to receive the first and second modified electromagnetic radiations and generate an output signal corresponding to the characteristic of the sample.

Abstract: An RFID sensor comprises an RFID chip, an antenna, and sensing material. The RFID chip is in electrical communication with the antenna and comprises an optical sensor. The sensing material overlies an upper surface of the RFID chip and is configured as a variable light filter that filters light differently depending upon certain properties or conditions of the environment surrounding the RFID sensor. A light source is configured to selectively illuminate the sensing material to facilitate detection of certain properties or conditions of the environment surrounding the RFID sensor.

Abstract: Manufacturing opto-electronic modules (1) includes providing a substrate wafer (PW) on which detecting members (D) are arranged; providing a spacer wafer (SW); providing an optics wafer (OW), the optics wafer comprising transparent portions (t) transparent for light generally detectable by the detecting members and at least one blocking portion (b) for substantially attenuating or blocking incident light generally detectable by the detecting members; and preparing a wafer stack (2) in which the spacer wafer (SW) is arranged between the substrate wafer (PW) and the optics wafer (OW) such that the detecting members (D) are arranged between the substrate wafer and the optics wafer. Emission members (E) for emitting light generally detectable by the detecting members (D) can be arranged on the substrate wafer (PW). Single modules (1) can be obtained by separating the wafer stack (2) into separate modules.

Abstract: Disclosed herein are compounds represented by Formula 1, wherein R1, Ar1, X, Ar2, Ar3, and Het are described herein. Compositions and light-emitting devices related thereto are also disclosed.

Abstract: An opto-electronic module includes a detecting channel comprising a detecting member for detecting light and an emission channel comprising an emission member for emitting light generally detectable by said detecting member. Therein, a radiation distribution characteristic for an emission of light from said emission channel is non rotationally symmetric; and/or a sensitivity distribution characteristic for a detection in said detecting channel of light incident on said detection channel is non rotationally symmetric; and/or a central or main emission direction for an emission of light from said emission channel and a central or main detection direction for a detection of light incident on said detection channel are aligned not parallel to each other; and/or at least a first one of the channels comprises one or more passive optical components.

Abstract: A rotation angle detecting apparatus comprises a shaft portion space formed in a rotation shaft, a bearing holder space, a first condenser lens, a second condenser lens to face the first condenser lens, a detection pattern provided at a focal position of one of the first condenser lens and the second condenser lens, an image sensor provided at a focal position of the other of the first condenser lens and the second condenser lens, and an arithmetic unit for calculating an angle displacement of the rotation shaft. The arithmetic unit carries out a total circumferential scanning, extracts a frequency component, carries out a scanning of a reference designation pattern, and calculates the angle displacement of the rotation shaft based on a phase difference of the frequency component and the number of frequencies corresponding to a change in a position of the reference designation pattern.

Abstract: A process analyses gases emitted during drilling of a borehole using oil based mud. The process comprises (a) using mass spectrometry, analysing the gas recovered during drilling through a hydrocarbon-poor zone at spaced apart locations to provide a mass spectrum for the gas emitted at each of the locations; (b) using mass spectrometry, analysing the gas recovered during drilling through a hydrocarbon-rich zone at one location to provide a mass spectrum for the gas emitted at the location; (c) using spectra from the measurements in (a) to extrapolate and predict a peak in a mass spectrum caused by compounds in the mud at a time when the drilling is proceeding through the hydrocarbon-rich zone; and (d) comparing the spectrum obtained in (b) with the predicted spectrum obtained in (c) to further predict at least one of the quantity and identity of the formation gases emitted from the hydrocarbon-rich zone.

Abstract: An ion mobility spectrometer has an inlet for an analyte substance opening into an ionization region that produces ions of the substance. Parallel grid electrodes extend laterally across the ion flow path and apply an electric field to the ions that is switchable between a relatively low magnitude alternating field that varies in magnitude over multiple periods and an asymmetric alternating field of sufficiently high magnitude to cause differential mobility effects. A collector collects the passed ions, and an indication of the nature of the analyte substance is produced from the collected ions passed during both the low and high field intervals. Also disclosed is the application of a substantially alternating field between the electrodes, which field varies between a low value and a higher value over a time exceeding that of the alternating period.

Abstract: The present invention relates to a method for the quantitative determination of an impurity present in a peptide product, wherein the impurity cannot be separated from other impurities or the main product. The method particularly involves the use of high resolution mass spectrometry (MS) detection with or without high performance liquid chromatography (HPLC). The method can be used for the investigation of the quality of peptides and proteins, particularly of pharmaceutical peptides and proteins.

Abstract: Industrial fluids can be monitored by employing differential ion mobility spectrometer to sample the industrial fluids. This process may also include controlling an industrial device or an industrial process using the results of the output from the field asymmetric ion mobility spectrometer. The process may also include employing a device to condition the sample prior to introducing the sample into field asymmetric ion mobility spectrometer.

Abstract: Systems and methods disclosed provide for methods of managing polarity switching in an ion mobility spectrometer, and provide for management of the repelling grid voltage, the gating grid voltage, and the fixed grid voltage during polarity switching. Systems and methods also provide for the management of the effect of dielectric relaxation in an insulator proximal to the collector, and provide for a preamplifier coupled to the collector including a switch, and a method of managing the collector output including the switch. Systems and methods consistent with the current disclosure further provide for a method of normalizing ion mobility data by determining fitting coefficients associated with a plurality of measurement data sets, and subtracting the curves determined by the fitting coefficients from the data acquired by the ion mobility spectrometer.

Abstract: A mass spectrometry method of the present invention is a method for conducting mass spectrometry in such a manner that an ion that is produced from a sample is introduced into a mass spectrometer by using DART or DESI, wherein the mass spectrometer has an ion introduction part for introducing the ion thereinto and the ion introduction part is heated at a predetermined timing.

Abstract: There is provided a transfer device (30) that transfers ionized substances in a first direction. The transfer device (30) includes a drift tube (50) and the drift tube (50) includes electrode plates (71) and (72) constructing an outer wall and a plurality of ring electrodes (60, 61, 62) disposed inside the tube. The ring electrodes (60) forms a first AC electric field for linear driving that causes the ionized substances to travel in the first direction that is the axial direction. The electrode plates (71) and (72) form an asymmetric second AC electric field that deflects the direction of travel of the ionized substances.

Abstract: A mass spectrometer system is provided that is configurable for operation in both a Kinetic Energy Discrimination (KED) and Dynamic Reaction Cell (DRC). A pressurized or collision cell included in the mass spectrometer encloses a quadrupole and is coupled to a source of both inert and reactive gas. To operate in the KED mode, the collision cell can be filled with a quantity of the inert gas and an energy barrier formed between the collision cell and a downstream mass analyzer. Interferer ions collided with the inert gas can lose on average more energy relative to analyte ions of the same mass to charge ratio and can thus be trapped by the energy barrier in greater proportions. To operate instead in the DRC mode, the collision cell can be filled with a quantity of gas that is reactive with the interferer ions only. Mass filtering of the product ions can then transmit proportionally more of the analyte ions to the downstream mass analyzer. A mode controller coordinates the two modes of operation.

Abstract: A curved ion guide (2) includes four curved rod electrodes (201-204) arranged around a curved central axis (O), two deflecting auxiliary electrodes (205, 206) which are located on a plane P on which the curved central axis (O) lies and which face each other across the axis (O), and two focusing auxiliary electrodes (207, 208) which are located on a curved surface orthogonal to the plane P and including the axis (O) and which face each other across the axis (O). Ions are focused by the effect of an electric field created by radio-frequency voltages applied to the curved rod electrodes, and a deflecting electric field having the effect of curving ions along the axis (O) is created by direct-current voltages applied to the deflecting auxiliary electrodes.

Abstract: When an SIM measurement for ions originating from a target component separated by a chromatograph is performed, the measurement is performed while the mass-resolving power is switched among a plurality of levels of resolving power, with the mass-to-charge ratio fixed at a target value (S2), and an extracted ion chromatogram is created based on each of data obtained corresponding to respective mass-resolving powers (S3). After the extracted ion chromatograms are obtained, an S/N ratio is calculated for a peak of the target component on each of the chromatograms (S4), and a mass-resolving power which yields the highest S/N ratio is selected (S5). The selected mass-resolving power is set as the mass-resolving power in the subsequent measurements of the same target component in the same kind of sample (S6), and the quantitative determination of the target component is performed using the extracted ion chromatogram obtained with the selected mass-resolving power (S7).

Abstract: Various aspects are directed to systems and methods for assessing neural activity of a neural region having multiple subfields. In certain embodiments, a method includes evoking a cellular electrical response in at least one subfield due to neural activity in the neural region, capturing image data of the electrical response at a level sufficiently detailed in space and time to differentiate between polarization-based events of two respective portions of the subfield, and then assessing neural activity by correlating space and time information, from the captured data, for the two respective portions of the sub-field. Other more specific aspects of the invention involve different preparation and neural stimulation approaches which can vary depending on the application.

Abstract: An object of the present invention is to provide a method and apparatus for measuring a potential on a surface of a sample using a charged particle beam while restraining a change in the potential on the sample induced by the charged particle beam application, or detecting a compensation value for a change in a condition for the apparatus caused by the sample being electrically charged. In order to achieve the above object, the present invention provides a method and apparatus for applying a voltage to a sample so that a charged particle beam does not reach the sample (hereinafter, this may be referred to as “mirror state”) in a state in which the charged particle beam is applied toward the sample, and detecting information relating to a potential on the sample using signals obtained by that voltage application.

Abstract: There is implemented a scanning electron microscope or a charged-particle beam apparatus. The scanning electron microscope or the charged-particle beam apparatus is provided with a function capable of managing utilization states of a micro scale with ease. The utilization states include a radiation position and the number of utilizations. A map corresponding to the layout of cells on the micro cells is created. The apparatus user selects a cell on the micro scale as a cell to be actually used from cells displayed on the map. On the actual display, the number of utilizations is not displayed simply as numerical data. Instead, cells are displayed on the map in different colors each indicating a utilization state. In addition, the utilization states of the micro scale are classified properly into categories and each of the colors is assigned to one of the categories.

Abstract: With a scanning electron microscope (SEM) adopting a commonly available exhaust system such as a turbo-molecular pump, an ion pump, or a rotary pump, and so forth, there is realized an apparatus capable of safely executing observation, or adsorption of a target substance that is high in rarity. Further, there is realized a safe SEM low in the risk of an electrical discharge by providing the apparatus with a probe, a means for replacing an atmosphere in a specimen chamber, with a predetermined gas, and a means for forming an image by detection of an ion current, and detection of an absorption current. Further, there is provided a means for controlling the polarity of a voltage applied to the probe. Still further, there is provided a control means for controlling a value of the voltage applied to the probe according to a degree of vacuum.

Abstract: There is provided an apparatus which can accurately carry out focusing of an optical microscope mounted on a charged particle beam apparatus while restraining an increase in an apparatus cost and a reduction in a throughput. An approximate polynomial is formed based on a focus map of the optical microscope which is previously measured, and a control amount which adds a difference between a piece of wafer height information at that occasion and a piece of wafer height information in actual observation to the approximate polynomial is inputted as a focus control value of the optical microscope.

Abstract: An electron beam device includes a first electron biprism between an acceleration tube and irradiation lens systems, and an electron biprism in the image forming lens system. The first electron biprism splits the electron beam into first and second electron beams, radiated to differently positioned first and second regions on objective plane of an objective lens system having a specimen perpendicular to an optical axis. The first and second electron beams are superposed on the observation plane by the electron biprism of the image forming lens system. The superposed region of those electron beams is observed or recorded. Optical action of the irradiation lens system controls each current density of the first and second electron beams on the objective plane of the objective lens system having the specimen, and distance on electron optics between the first electron biprism and the objective plane of the objective lens system having the specimen.

Abstract: A radiation detector outputs an analog pulse for incident radiation, and a signal processing portion is furnished with a wave height measuring function of converting the analog pulse inputted therein to a digital form and then measuring a peak wave height of the analog pulse and a wave height spectrum measuring function of measuring a wave height spectrum on the basis of measured wave height data, computes a dose rate and mean energy on the basis of measured wave height spectral data, and outputs computation results. The signal processing portion computes the dose rate and the mean energy on the basis of the wave height spectral data in a same wave height range on a same time axis. It thus becomes possible to provide accurate information based on which to determine whether a rise in dose rate is contributed by natural radon and thoron or contributed by a reactor facility.

Abstract: In at least one embodiment, a sensing apparatus is provided. The sensing apparatus comprises a substrate, a thermopile, and a readout circuit. The thermopile includes an absorber positioned above the substrate for receiving thermal energy and for generating an electrical output indicative of the thermal energy. The readout circuit is positioned below the absorber and includes at least one first switch positioned therein for being electrically coupled to the thermopile to provide a bypass in the event the thermopile is damaged.

Abstract: A photonic crystal, which is a periodically arranged structure made of free-standing columns, has a base material of at least one metal or a metal alloy. Intermediate spaces between the columns allow passage of a gas to be analyzed. The photonic crystal has predefined imperfections, by which at least one resonator is formed, the resonant frequency of which is in a frequency range which is absorbed by a gas component to be detected. A heating unit heats at least some of the columns and at least one detector element extracts the energy present in the resonator in the heated state under the action of the gas to be analyzed. The device may have extremely small dimensions and very low energy consumption.

Abstract: A terahertz-wave element includes a waveguide (2, 4, 5) that includes an electro-optic crystal and allows light to propagate therethrough, and a coupling member (7) that causes a terahertz wave to enter the waveguide (2, 4, 5). The propagation state of the light propagating through the waveguide (2, 4, 5) changes as the terahertz wave enters the waveguide (2, 4, 5) via the coupling member (7).

Abstract: According to the present invention, a measurement device includes an electromagnetic wave detector, a phase measurement unit and a deriving unit. The electromagnetic wave detector detects an electromagnetic wave having a frequency equal to or more than 0.02 THz and equal to or less than 12 THz having traveled inside an object to be measured, which is an aggregation of particles. The phase measurement unit measures a change in phase of the electromagnetic wave generated by the travel inside the object to be measured based on a detection result by the electromagnetic wave detector. The deriving unit derives hardness or porosity of the object to be measured based on a measurement result by the phase measurement unit.

Abstract: An infrared sensor device includes a plurality of infrared sensors that is provided in a plurality of divided areas in which an infrared-receiving area is radially divided in one plane; a detector that detects presence or absence of movement of an object in the infrared-receiving area for each of the divided areas based on an output of the infrared sensor; and a determiner that determines whether the object is in a detection area in a predetermined distance range from the infrared sensor, based on an arrangement pattern of the divided areas in which the movement of the object is detected, in an alignment of the divided areas in the infrared-receiving areas.

Abstract: A flat lens with multiple focal lengths has a lens segment. The lens segment is flat and has multiple convex lenses. The convex lenses are mounted on one of the surfaces of the lens segment, and have multiple focal lengths. With the different focal lengths of the convex lenses, multiple distances of detection of a sensor behind the lens segment can be extended to different lengths, and further increase the range of detection. Besides, with different distances of detection, the accuracy of detection would be enhanced effectively, and the erroneous estimate on a volume of the object would reduce effectively. Furthermore, because a shape of the lens segment is flat, the lens as described is more innovative and aesthetically appealing, and is relatively easier to match the building's design or decoration.

Abstract: The device includes: a scintillator 200 configured to emit fluorescence by irradiation of radiation, and a photodetector 40 configured to detect the fluorescence emitted from the scintillator 200 as an electrical signal, wherein the scintillator 200 includes a columnar section 20 which is disposed at a rear side of the photodetector 40 in a travel direction of the radiation and at the same time is formed by a group of columnar crystals 20A obtained through columnar growth of crystals of a fluorescent material, and a first non-columnar section 23 which is provided at the photodetector 40 side of the columnar section 20.

Abstract: A radiological image conversion panel 2 is provided with a phosphor 18 containing a fluorescent material that emits fluorescence by radiation exposure, in which the phosphor includes, a columnar section 34 formed by a group of columnar crystals which are obtained through columnar growth of crystals of the fluorescent material, and a non-columnar section 36, the columnar section and the non-columnar section are integrally formed to overlap in a crystal growth direction of the columnar crystals, and a thickness of the non-columnar section along the crystal growth direction is non-uniform in a region of at least a part of the non-columnar section.

Abstract: The X-ray image detection apparatus 1 includes: a scintillator panel 10 including a phosphor 200 that is formed on a support 101 and emits fluorescence by irradiation of radiation; and a photodetector 40 that detects the fluorescence emitted by the phosphor as an electric signal, wherein the phosphor 200 includes a columnar section 20 formed by growing crystals of a fluorescent material in a columnar shape, and a non-columnar section 25 provided between the columnar section 20 and the support 101 and has a porosity lower than that of the columnar section 20, and the scintillator panel 10 is disposed at the rear side of the photodetector 40 in a radiation travelling direction, and in the phosphor 200, the non-columnar section 25 is disposed at a side opposite to the photodetector side.

Abstract: A Positron Emission Tomography (PET) detector assembly includes a cold plate having a first side and an opposite second side, the cold plate being fabricated from a thermally conductive and electrically non-conductive material, a plurality of PET detector units coupled to the first side of the cold plate, and a readout electronics section coupled to the second side of the cold plate. A radio frequency (RF) body coil assembly and a dual-modality imaging system are also described herein.

Abstract: The present invention provides a radiation detecting element and a radiographic imaging device that may reliably detect radiation even when a region where radiation is irradiated is set narrowly. Namely, in the radiation detecting element and the radiographic imaging device of the present invention, plural pixels including radiographic imaging pixels and plural radiation detection pixels are disposed in a matrix in a detection region that detects radiation.

Abstract: A gamma ray detector apparatus comprises a solid state detector that includes a plurality of anode pixels and at least one cathode. The solid state detector is configured for receiving gamma rays during an interaction and inducing a signal in an anode pixel and in a cathode. An anode pixel readout circuit is coupled to the plurality of anode pixels and is configured to read out and process the induced signal in the anode pixel and provide triggering and addressing information. A waveform sampling circuit is coupled to the at least one cathode and configured to read out and process the induced signal in the cathode and determine energy of the interaction, timing of the interaction, and depth of interaction.

Abstract: Embodiments of systems, methods and non-transitory computer readable media for imaging are presented. Preliminary image data corresponding to a first FOV of a subject at a first resolution is acquired using an imaging system including one or more radiation sources and at least one hybrid detector, specifically using at least one section of the hybrid detector having the first resolution. The target ROI is identified using the preliminary image data. Further, the subject is positioned to align the target ROI along a designated axis. Additionally, parameters associated with the sources, the hybrid detector and/or an imaging system gantry are configured for acquiring target image data at a second resolution greater than the first resolution using at least one section of the hybrid detector having the second resolution. Further, one or more images corresponding to at least the target ROI are reconstructed using the target and/or the preliminary image data.