Multiple interactions, such as Compton scattering, inside a PET detector are used to predict an incident photon's direction for identifying true coincidence events versus scatter/random coincidence events by creating a cone shaped shell projection defining a range of possible flight directions for the incident photon. The disclosed techniques can be used as prior information to improve the image reconstruction process. The disclosed techniques can be implemented in a LYSO/SiPM-based layer stacked detector, which can precisely register multiple interactions' 3D position.

Multiple interactions, such as Compton scattering, inside a PET detector are used to predict an incident photon's direction for identifying true coincidence events versus scatter/random coincidence events by creating a cone shaped shell projection defining a range of possible flight directions for the incident photon. The disclosed techniques can be used as prior information to improve the image reconstruction process. The disclosed techniques can be implemented in a LYSO/SiPM-based layer stacked detector, which can precisely register multiple interactions' 3D position.

A data processing apparatus according to an embodiment includes acquisition circuitry and specification circuitry. The acquisition circuitry is configured to acquire a detector signal containing a first component that is based on Cherenkov light and a second component that is based on scintillation light. The specification circuitry is configured to specify timing information about generation of the detector signal by curve fitting to the first component.

In one embodiment, a charged-particle trajectory measurement apparatus for measuring a trajectory of a cosmic ray muon as a charged particle includes: a plurality of detectors, each of which generates a detection signal at the time of detecting a cosmic ray muon; a signal processing circuit that processes the detection signal from the detector; a time calculator that calculates the generation time point of the detection signal from the detector on the basis of the signal outputted from the signal processing circuit; a trajectory calculator that calculates the trajectory of the cosmic ray muon on the basis of the generation time point of the detection signal and the positional information of the detector having detected the cosmic ray muon, wherein the signal processing circuit and each of the detectors are integrally configured by being coupled to each other.

In one embodiment, a charged-particle trajectory measurement apparatus for measuring a trajectory of a cosmic ray muon as a charged particle includes: a plurality of detectors, each of which generates a detection signal at the time of detecting a cosmic ray muon; a signal processing circuit that processes the detection signal from the detector; a time calculator that calculates the generation time point of the detection signal from the detector on the basis of the signal outputted from the signal processing circuit; a trajectory calculator that calculates the trajectory of the cosmic ray muon on the basis of the generation time point of the detection signal and the positional information of the detector having detected the cosmic ray muon, wherein the signal processing circuit and each of the detectors are integrally configured by being coupled to each other.

Multiple interactions, such as Compton scattering, inside a PET detector are used to predict an incident photon's direction for identifying true coincidence events versus scatter/random coincidence events by creating a cone shaped shell projection defining a range of possible flight directions for the incident photon. The disclosed techniques can be used as prior information to improve the image reconstruction process. The disclosed techniques can be implemented in a LYSO/SiPM-based layer stacked detector, which can precisely register multiple interactions' 3D position.

Multiple interactions, such as Compton scattering, inside a PET detector are used to predict an incident photon's direction for identifying true coincidence events versus scatter/random coincidence events by creating a cone shaped shell projection defining a range of possible flight directions for the incident photon. The disclosed techniques can be used as prior information to improve the image reconstruction process. The disclosed techniques can be implemented in a LYSO/SiPM-based layer stacked detector, which can precisely register multiple interactions' 3D position.

A sensor for a coincidence radiation detection device comprises a photomultiplier device to receive incident optical pulses of photons from an associated scintillator device and responsively generate an input electrical signal having corresponding electrical pulses. A charge sensitive amplifier receives the input electrical signal and outputs an amplified electrical signal. An edge-peak detector circuit detects a fast rising edge of the electrical pulses; a beginning of a trailing edge of the electrical pulses; and a peak value of the electrical pulses. A local microcontroller includes: a timing circuit to generate timestamp values for detected pulses in response to a detected pulse edge and to synchronise the timestamp values with a reference clock signal to generate timestamp values for the pulses; an analog to digital converter to record pulse height values of the electrical pulses; and a communications interface to communicate the timestamp values and pulse height values to a memory device.

A sensor for a coincidence radiation detection device comprises a photomultiplier device to receive incident optical pulses of photons from an associated scintillator device and responsively generate an input electrical signal having corresponding electrical pulses. A charge sensitive amplifier receives the input electrical signal and outputs an amplified electrical signal. An edge-peak detector circuit detects a fast rising edge of the electrical pulses; a beginning of a trailing edge of the electrical pulses; and a peak value of the electrical pulses. A local microcontroller includes: a timing circuit to generate timestamp values for detected pulses in response to a detected pulse edge and to synchronise the timestamp values with a reference clock signal to generate timestamp values for the pulses; an analog to digital converter to record pulse height values of the electrical pulses; and a communications interface to communicate the timestamp values and pulse height values to a memory device.

The present disclosure describes a radiation sensing and reporting devices, systems, and methods. The devices and systems are a flexible material that detects the presence of radiation over a surface area and reports the specific location and intensity of the radiation. An article is provided that includes a substrate; a plurality of radiation sensors, each radiation sensor of the plurality of radiation sensors being disposed at a corresponding position on the substrate; and alert circuitry coupled to the plurality of radiation sensors, wherein the alert circuitry indicates, in real time, a localized detection of radiation according to corresponding one or more positions on the substrate of a particular one or more radiation sensors of the plurality of radiation sensors.