A radiation detection device according to an embodiment includes a scintillator and a processing circuit. The processing circuit measures transferred energy when scintillation is caused after a gamma ray incident on a scintillator generates Cherenkov light and estimates a Cherenkov angle based on the transferred energy.

An energy sensor is provided including a collimator comprising a plurality of sensor apertures aligned in a plurality of directions configured to allow passage of an energetic particle or photon in a specific direction for respective apertures of the plurality of sensor apertures and at least one energy detector configured to measure the energetic particle or photon including a plurality of detector segments. Respective detector segments of the plurality of detector segments are aligned with the respective sensor apertures and a detector segment which measures the energetic particle or photon is indicative of a directionality of the energetic particle or photon.

A device for generating one or more images of a source distribution of a gamma radiation field in the near and far field can include a detector system that includes several synchronized detectors for detecting radiation, system electronics that registers coincidence events, a data acquisition system that stores the measurement data of the coincidence events, and an analysis unit that performs an image reconstruction, which reconstructs one or more images of the source distribution of the radiation field.

An imaging system includes a detector configured to obtain radiation data from one or more sources and a controller. The controller is configured to define plurality of buffers based on at least one initial condition. The radiation data includes a plurality of events. The controller is configured to receive an individual event of the plurality of events and determine if the individual event falls within a designated current buffer. Each of the plurality of events in the current buffer is corrected for pose and aligned in a common two-dimensional space. The plurality of events in the current buffer are reconstructed into a three-dimensional space, the reconstruction being done once for each of the plurality of buffers. The controller is configured to create a three-dimensional image based in part on the reconstruction in the three-dimensional space.

A method includes obtaining a dark-field signal generated from a dark-field CT scan of an object, wherein the dark-field CT scan is at least a 360 degree scan. The method further includes weighting the dark-field signal. The method further includes performing a cone beam reconstruction of the weighted dark-field signal over the 360 degree scan, thereby generating volumetric image data. For an axial cone-beam CT scan, in one non-limiting instance, the cone-beam reconstruction is a full scan FDK cone beam reconstruction. For a helical cone-beam CT scan, in one non-limiting instance, the dark-field signal is rebinned to wedge geometry and the cone-beam reconstruction is a full scan aperture weighted wedge reconstruction. For a helical cone-beam CT scan, in another non-limiting instance, the dark-field signal is rebinned to wedge geometry and the cone-beam reconstruction is a full scan angular weighted wedge reconstruction.

A system for characterising a beam of charged particles. The system includes a stack comprising an ultra-thin pattern formed from an electrically conductive material; a thin substrate bearing the pattern. The stack forms an emitting electrode able to emit secondary electrons in proximity to a surface of the pattern when the emitting electrode is passed through by the beam of charged particles.

A radiation particle strike detection system is disclosed. The radiation particle strike detection system includes a radiation particle detector and a controller coupled to the radiation particle detector. The radiation particle detector is overlayed on at least one surface of a payload that is sensitive to interaction with radiation particles. The radiation particle detector is configured to undergo a change in state responsive to a radiation particle strike at a location on the radiation particle detector. The controller is configured to 1) monitor a state of the radiation particle detector; 2) detect a radiation particle strike on the radiation particle detector based on a change in state of the radiation particle detector; and 3) determine a location and time of the radiation particle strike on the radiation particle detector based on the change in state of the particle detector.

The present invention provides a radiation imaging apparatus capable of maintaining the quality of an image obtained even when a dose incident on a radiation detector changes suddenly. The present invention is a radiation imaging apparatus including a radiation source, a radiation detector to detect radiation emitted from the radiation source, and a cooling unit to cool the radiation detector; and is characterized in that the radiation detector has a counting circuit to output a number of photons in radiation counted per unit time as a photon counting rate, and the cooling unit controls a coolability of the radiation detector in response to the photon counting rate.

To optimize an image quality and/or a sensitivity, a Compton camera is adaptable. A scatter detector and/or a catcher detector may move closer to and/or further away from a patient and/or each other. This adaptation allows a balancing of the image quality and the sensitivity by altering the geometry.

A radiation particle strike detection system is disclosed. The radiation particle strike detection system includes a radiation particle detector and a controller coupled to the radiation particle detector. The radiation particle detector is overlayed on at least one surface of a payload that is sensitive to interaction with radiation particles. The radiation particle detector is configured to undergo a change in state responsive to a radiation particle strike at a location on the radiation particle detector. The controller is configured to 1) monitor a state of the radiation particle detector; 2) detect a radiation particle strike on the radiation particle detector based on a change in state of the radiation particle detector; and 3) determine a location and time of the radiation particle strike on the radiation particle detector based on the change in state of the particle detector.