Patent classifications
G01T1/29
IMAGING METHOD USING JOINTLY A PET RECONSTRUCTION AND A COMPTON RECONSTRUCTION, PREFERABLY IN 3D COMPTON
A PET and Compton imaging method implemented by a device including at least two facing PET modules. The device includes a Compton camera arranged outside a plane containing the PET modules for forming a trihedron with the PET modules and producing a Compton view. The acquisition fields of the PET and Compton views having an overlap area covering the object to be imaged. The device allowing the following steps to be carried out: acquisition of a Compton view; location of a dense area and its contour on the Compton view; Computation of the 2D map of the probability of detection of the presence of a source from the Compton view of the Compton camera; Coincidence detection by the PET cameras and association of a response line (LOR); and Segmentation of LORs crossing the dense area by using the detection probability determined by the Compton view.
THREE-DIMENSIONAL TILEABLE GAMMA RAY DETECTOR
For gamma ray detection, 3D tiling is made possible by modules that include a gamma ray detector with at least some electronics extending away from the detector as a side wall, leaving an air or low attenuation gap behind the gamma ray detector. The modules may be stacked to form arrays of any shape in 3D, including stacking to form a Compton detector with a scatter detector separated from the catcher detector by the low attenuation gap where the electronics form at least one side wall between the detectors. The modules may be stacked so that the detectors from the different modules are in different planes and/or not part of a same surface (e.g., same surface provided with just 1D or 2D tiling).
APPARATUS AND METHOD FOR PET DETECTOR
A PET detector and method thereof are provided. The PET detector may include: a crystal array including a plurality of crystal elements arranged in an array and light-splitting structures set on surfaces of the plurality of crystal elements, the light-splitting structures jointly define a light output surface of the crystal array; a semiconductor sensor array, which is set in opposite to the light output surface of the crystal array and is suitable to receive photons from the light output surface, the semiconductor sensor array comprises a plurality of semiconductor sensors arranged in an array.
Timing calibration using internal radiation and external radiation source in time of flight positron emission tomography
A method and system for providing improved timing calibration information for use with apparatuses performing Time of Flight Positron Emission Tomography scans. Relative timing offset, including timing walk, within a set of processing units in the scanner are obtained and corrected using a stationary limited extent positron-emitting source, and timing offset between the set of processing units is calibrated using an internal radiation source, for performing calibration.
Assessment of labeled probes in a subject
Wearable apparatus and method of using same for tracking a labeled probe in a subject are disclosed.
Methods for detecting a position of an energy beam spot and apparatuses for performing the same
A method for detecting a position of an energy beam comprises mapping a first density modulated x-ray signal with a plurality of locations on an energy beam target, thereby generating a model of a background x-ray intensity. The method further comprises forming an x-ray signal time series using subsequent intensity modulated x-ray signals, each resulting from scanning the energy beam along the energy beam target in one of a plurality of directions at one of a plurality of speeds, and determining the position of the energy beam based upon a received x-ray signal strength based on the x-ray signal time series and the model of the background x-ray intensity.
Methods for detecting a position of an energy beam spot and apparatuses for performing the same
A method for detecting a position of an energy beam comprises mapping a first density modulated x-ray signal with a plurality of locations on an energy beam target, thereby generating a model of a background x-ray intensity. The method further comprises forming an x-ray signal time series using subsequent intensity modulated x-ray signals, each resulting from scanning the energy beam along the energy beam target in one of a plurality of directions at one of a plurality of speeds, and determining the position of the energy beam based upon a received x-ray signal strength based on the x-ray signal time series and the model of the background x-ray intensity.
Device for supporting the testing of a brachytherapy applicator and a method for testing of such a brachytherapy applicator prior to the use of the brachytherapy applicator in brachytherapy radiation treatments
The invention relates to a device for supporting the testing of a brachytherapy applicator prior to the use of the brachytherapy applicator in brachytherapy radiation treatments. The invention also relates to a method for testing of a brachytherapy applicator prior to the use of the brachytherapy applicator in brachytherapy radiation treatments.
Device for supporting the testing of a brachytherapy applicator and a method for testing of such a brachytherapy applicator prior to the use of the brachytherapy applicator in brachytherapy radiation treatments
The invention relates to a device for supporting the testing of a brachytherapy applicator prior to the use of the brachytherapy applicator in brachytherapy radiation treatments. The invention also relates to a method for testing of a brachytherapy applicator prior to the use of the brachytherapy applicator in brachytherapy radiation treatments.
CHARGED-PARTICLE TRAJECTORY MEASUREMENT APPARATUS AND CHARGED-PARTICLE TRAJECTORY MEASUREMENT METHOD
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.