Disclosed is a general PET device (1) with a gradually narrowed head, the device comprising a body (2), a head (3) and a top (4) closely arranged in sequence, wherein the body (2) is composed of a plurality of body module rings (21); the head (3) is composed of N head module rings (31), with N being a natural number and being at least two; the top (4) is composed of a plurality of top PET detection modules (41); each of the body module rings (21) is composed of several body PET detection modules (22) evenly distributed in a circumferential direction thereof, and all the body module rings (21) are closely arranged in an axial direction to form the body (2); in the N head module rings (31), the rings sequentially decreases in size, and are closely arranged in the axial direction in a sequence from the first head module ring (31) to the Nth head module ring (31); and the detection surfaces of the plurality of top PET detection modules (41) are located in the same plane, and all the detection surfaces face the head (3) or the body (2).

The invention relates to a solution for determining events related to photons and charged particles useful in therapies that use methodologies related to hadron therapy. In one aspect of the invention, it relates to a device having a sandwich-type structure of photon-detecting panels (1) and charged particle-detecting panels (2), which can be suitably associated with respective sensors. Also included is a method for detecting photons and charged particles that uses the aforementioned device. Lastly, a specific use of the object of the invention in hadron therapy is described.

A device for the detection of gamma rays presents a high resolution in the three-dimensional position of the impact of the gamma ray within one or more scintillation crystal blocks coupled to an array of photosensors, for the determination of the impact energy of said gamma ray, the determination of the instant in time when said impact occurred, the interaction depth and the determination of the time-of-flight. Advantageously, in said device, the scintillation crystal detection blocks are optically isolated, in such a way that the scintillation light can only exit said blocks via the output region; and the scintillation crystal detection blocks and the array of photosensors are disposed in direct optical coupling.

A device for the detection of gamma rays presents a high resolution in the three-dimensional position of the impact of the gamma ray within one or more scintillation crystal blocks coupled to an array of photosensors, for the determination of the impact energy of said gamma ray, the determination of the instant in time when said impact occurred, the interaction depth and the determination of the time-of-flight. Advantageously, in said device, the scintillation crystal detection blocks are optically isolated, in such a way that the scintillation light can only exit said blocks via the output region; and the scintillation crystal detection blocks and the array of photosensors are disposed in direct optical coupling.

An object of the present invention is to provide a scintillator having a high radiation stopping power, and having a shorter fluorescence decay time compared to conventional scintillators. The above object is achieved by setting the composition of a scintillator to a composition represented by General Formula (1).

Q.sub.xM.sub.yO.sub.3z  (1)

(wherein in General Formula (1), Q includes at least two or more divalent metallic elements; M includes at least Hf; and x, y, and z independently satisfy 0.5≤x≤1.5, 0.5≤y≤1.5, and 0.7≤z≤1.5, respectively).

A method of tailoring the properties of garnet-type scintillators to meet the particular needs of different applications is described. More particularly, codoping scintillators, such as Gd.sub.3Ga.sub.3Al.sub.2O.sub.12, Gd.sub.3Ga.sub.2Al.sub.3O.sub.12, or other rare earth gallium aluminum garnets, with different ions can modify the scintillation light yield, decay time, rise time, energy resolution, proportionality, and/or sensitivity to light exposure. Also provided are the codoped garnet-type scintillators themselves, radiation detectors and related devices comprising the codoped garnet-type scintillators, and methods of using the radiation detectors to detect gamma rays, X-rays, cosmic rays, and particles having an energy of 1 keV or greater.

Particle analyzers having scintillation counters are provided. Particle analyzers of interest include a flow cell for transporting particles in a flow stream, a light source for irradiating a particle in the flow stream at an interrogation point, a particle-modulated light detector for detecting light from the interrogation point, and a scintillation counter for assessing particle radioactivity. In embodiments, the scintillation counter is positioned within the flow cell and configured generate particle radioactivity data that may be associated with a given particle in a plurality of particles. Methods and non-transitory computer readable storage media for practicing the invention are also provided.

Particle analyzers having scintillation counters are provided. Particle analyzers of interest include a flow cell for transporting particles in a flow stream, a light source for irradiating a particle in the flow stream at an interrogation point, a particle-modulated light detector for detecting light from the interrogation point, and a scintillation counter for assessing particle radioactivity. In embodiments, the scintillation counter is positioned within the flow cell and configured generate particle radioactivity data that may be associated with a given particle in a plurality of particles. Methods and non-transitory computer readable storage media for practicing the invention are also provided.

A well image logging tool assembly comprising at least one sensor unit, at least one spatial positioning device, and a cylindrical outer sheath that extends around and contains the sensor unit and the spatial positioning device. The sensor unit includes a solid cylindrical sensor body formed of a gamma ray shielding material and including at least one longitudinal sensor cavity extending through at least one of the top end and the bottom end of the sensor body. A window corresponds to each sensor cavity and extends through the sensor body from the outside surface thereof to the corresponding sensor cavity. A sensor assembly is disposed in each sensor cavity. Each sensor assembly includes a gamma ray radiation sensor and associated photomultiplier tube.

A detector is for electromagnetic radiation. In an embodiment, the detector includes a first, pixelated electrode layer, a second electrode, and a first layer including at least one first perovskite, located between the first, pixelated electrode layer and the second electrode. An embodiment further relates to a method for manufacturing a corresponding detector.