G01T1/1606

Silicon Photomultiplier Based TOF-PET Detector

A scintillation block detector employs an array of optically air coupled scintillation pixels, the array being wrapped in reflector material and optically coupled to an array of silicon photomultiplier light sensors with common-cathode signal timing pickoff and individual anode signal position and energy determination. The design features afford an optimized combination of photopeak energy event sensitivity and timing, while reducing electronic circuit complexity and power requirements, and easing necessary fabrication methods. Four of these small blocks, or miniblocks, can be combined as optically and electrically separated quadrants of a larger single detector in order to recover detection efficiency that would otherwise be lost due to scattering between them. Events are validated for total energy by summing the contributions from the four quadrants, while the trigger is generated from either the timing signal of the quadrant with the highest energy deposition, the first timing signal derived from the four quadrant time-pickoff signals, or a statistically optimum combination of the individual quadrant event times, so as to maintain good timing for scatter events. This further reduces the number of electronic channels required per unit detector area while avoiding the timing degradation characteristic of excessively large SiPM arrays.

PARTICLE DETECTOR, IMAGE GENERATION DEVICE, AND IMAGE GENERATION METHOD
20200033488 · 2020-01-30 · ·

According to one embodiment, a particle detector is disclosed. The particle detector includes a substrate, and detection regions provided on the substrate and insulated from the substrate. Each of the detection regions includes superconducting strips having a longitudinal direction and configured for detecting a particle, and the superconducting strips are arranged in arrangement directions differing between the detection regions. The numbers of particles detected by the respective detection regions are used to generate accumulated detection number profiles of particles in the arrangement directions of the superconducting strips of the respective detection regions, and each of the accumulated detection number profiles includes a profile obtained by accumulating the numbers of particles detected by the respective superconducting strips along the longitudinal direction.

RADIATION IMAGING SYSTEM
20200018864 · 2020-01-16 · ·

A radiation imaging system includes a radiation-emitting device and a radiation imaging device. The radiation imaging device has an electrical insulation layer having a top surface and a bottom surface, a top electrode on the top surface of the electrical insulation layer, an array of pixel units electrically coupled to the electrical insulation layer, and an array of transistors connected to the array of pixel units.

Synthetic material for detecting ultraviolet radiation and/or X-radiation
10533131 · 2020-01-14 · ·

The invention relates to a material represented by the following formula (I)
(M).sub.8M.sub.6M.sub.6O.sub.24(X,S).sub.2:Mformula (I).
Further, the invention relates to an ultraviolet radiation sensing material, to an X-radiation sensing material, to different uses, to a device and to a method for determining the intensity of ultraviolet radiation.

SUPERCONDUCTING ELEMENT, PARTICLE DETECTION DEVICE, AND PARTICLE DETECTION METHOD
20200011999 · 2020-01-09 · ·

According to one embodiment, a superconducting element used as a pixel for detecting a particle is disclosed. The superconducting element includes at least one superconducting strip. The at least one superconducting strip includes a meandering structure. The meandering structure includes a first portion extending in a first direction and made of a superconducting material, a second portion connected to the first portion, extending in a second direction perpendicular to the first direction, and being conductive, and a third portion connected to the second portion, extending in a direction opposite to the first direction, and made of a superconducting material. A superconducting region of any one of the first portion and the third portion is configured to be divided when the particle is radiated to the first portion.

Silicon photomultiplier based TOF-PET detector

A scintillation block detector employs an array of optically air coupled scintillation pixels, the array being wrapped in reflector material and optically coupled to an array of silicon photomultiplier light sensors with common-cathode signal timing pickoff and individual anode signal position and energy determination. The design features afford an optimized combination of photopeak energy event sensitivity and timing, while reducing electronic circuit complexity and power requirements, and easing necessary fabrication methods. Four of these small blocks, or miniblocks, can be combined as optically and electrically separated quadrants of a larger single detector in order to recover detection efficiency that would otherwise be lost due to scattering between them. Events are validated for total energy by summing the contributions from the four quadrants, while the trigger is generated from either the timing signal of the quadrant with the highest energy deposition, the first timing signal derived from the four quadrant time-pickoff signals, or a statistically optimum combination of the individual quadrant event times, so as to maintain good timing for scatter events. This further reduces the number of electronic channels required per unit detector area while avoiding the timing degradation characteristic of excessively large SiPM arrays.

LITHIUM-CONTAINING THIOSTANNATE SPINELS FOR THERMAL NEUTRON AND ALPHA-PARTICLE DETECTION
20240103186 · 2024-03-28 ·

Lithium-containing thiostannate spinel compounds having the formula Li.sub.2M.sub.1+xSn.sub.3?xS.sub.8, where x is 0 or 1 and M is Mg, Fe, Mn, Ni, Ga, In, or a combination thereof; or the formula Li.sub.1.66CuSn.sub.3.33S.sub.8 are provided. Methods and devices for detecting incident neutrons and alpha-particles using the compounds are also provided. For thermal neutron detection applications, the compounds can be enriched with lithium-6 isotope (.sup.6Li) to enhance their neutron detecting capabilities.

Boundary protection method and system of radiation detection robot

A boundary protection method and system of a radiation detection robot. The boundary protection method comprises: a first laser radar and a second laser radar are arranged diagonally, a first marking rod and a second marking rod are arranged diagonally; a boundary of an interlocking zone is defined by the first laser radar, the second laser radar, the first marking rod and the second marking rod; the object to be detected is placed in the interlocking zone; the radiation detection robot uses rays to detect the object to be detected in the interlocking zone; an early warning zone is provided outside the interlocking zone; wherein when it is detected that a person or object has intruded into the interlocking zone, the radiation detection robot stops emitting rays; and when it is detected that a person or object has intruded into the early warning zone, a warning is issued directly.

DEVICES AND METHODS FOR DETECTING GAMMA RADIATION

A device for detecting gamma radiation has an assembly of scintillating and light-guiding materials, producing scintillation light upon incidence of radiation. At least one photon-detector device includes a detection surface optically coupled to the assembly. The assembly includes at least one photonic crystal slab configured to direct said scintillation light towards the detection surface along an extraction direction. The extraction direction is substantially perpendicular to the detection surface. The photonic crystal slab is arranged substantially perpendicular to the detection surface.

Dual mode detector

A detector system which can be switched between single photon counting and charge integrating mode depending on the application, the photon flux and energy. Although the space for electronics in a pixel or strip detector system is very limited (as each channel is limited by the pixel size), the reconfiguration of the analog chain and the logic/counter in this smart way yields to have a detector system allowing both modes of operation and, therefore, effectively combining the characteristics of an Eiger? single photon counting system and a Jungfrau? charge integrating pixel detector system into one single detector. Depending on the application, the flux and the photon energy, the operator is enabled to switch between single photon counting and charge integrating mode of operation.