A method for measuring and representing the level of local irradiation doses, in at least two dimensions, comprises: a step of positioning N probes S.sub.i sensitive to irradiating radiation, each corresponding to a local zone Z according to a known topology; a step of acquiring, by each of the probes, the level of radiation IS.sub.i detected and periodically recording numerical values IS.sub.i(t); and a step of converting the numerical values IS.sub.i(t) into values DS.sub.i(t) corresponding to the radiation dose applied to each of the Z zones associated with a probe S.sub.i, according to a calibration table. The method further comprises, during the measurement sequence, steps of spatial interpolation calculation of at least one estimated irradiation level value IS.sub.iv(t) of at least one virtual zone Z.sub.iv that is not associated with a probe. A measurement device for implementing this method is also described.

The invention provides a detection system for ionizing radiation, a method of manufacturing a detection system for ionizing radiation, a method of detecting ionizing radiation, a detection chamber for detecting ionizing radiation by liquid scintillation counting, and a method of detecting ionizing radiation by liquid scintillation counting. The detection system for ionizing radiation comprises a detector with a detection surface. The detector is configured to detect ionizing radiation that is incident on the detection surface. An adsorption layer is provided on said detection surface, the adsorption layer being configured to bind target particles, wherein the target particles are radioactive atoms or molecules.

This dosimeter comprises: a transducer material capable, when it is excited by a secondary ionizing radiation, of generating photons or electric charges, an amplifying layer capable, in response to its excitation by the primary ionizing radiation, of generating the secondary ionizing radiation. This amplifying layer comprises a first and a second amplifying sublayer stacked on top of one another. The first and the second amplifying sublayers are composed of at least 70%, by weight, respectively, of at least one first and one second material, the atomic numbers of which are greater than or equal to 29. The atomic number of the first material being less than the atomic number of the second material. The first sublayer is interposed between the second sublayer and the transducer material.

Examples of the present disclosure relate to a particle beam dose profile measurement apparatus comprising a particle detector stack comprising a plurality of scintillator layers. Each scintillator layer of the detector stack is disposed along an axis of the apparatus such that the axis projects through each layer. Each scintillator layer is configured to produce scintillation light indicative of an energy deposition, in that scintillator, of a particle beam incident upon the detector stack along said axis. The apparatus comprises readout circuitry configured to measure the scintillation light of each scintillator layer; and dose profile determination circuitry configured to determine a dose profile of said particle beam within the detector stack. Said determining is based on the measured scintillation light of each scintillator layer, and a quenching correction.

A radiation imaging apparatus including conversion elements acquiring a radiation image and detectors, a readout unit and a controller is provided. In a first operation, the controller causes the readout unit to output a composition signal obtained by composing signals from the detectors, detects irradiation with radiation based on the composition signal, and shifts to a second operation. In the second operation, the controller acquires first signals individually read out from the detectors, decides a signal component, of the composition signal, which is output from a selected detector of the detectors in accordance with a ratio of the first signal from the selected detector to a sum of the first signals, and acquires an integrated dose of radiation incident on the selected detector based on the signal component and the first signal of the selected detector.

Techniques are disclosed for systems and methods to provide a radiation detector module for a radiation detector. A radiation detector module an enclosure, a radiation sensor separated from the enclosure by one or more damping inserts, readout electronics configured to provide radiation detection event signals corresponding to incident ionizing radiation in the radiation sensor, and a cap comprising an internal interface configured to couple to the readout electronics and an external interface configured to couple to a radiation detector, wherein the cap is configured to hermetically seal the radiation sensor within the enclosure. Plated edges of the cap can be soldered to the enclosure to hermetically seal the radiation sensor within the enclosure.

A device for determining an ionizing radiation dose deposited by a medical imaging apparatus during a radiological examination of a patient includes at least one measurement probe comprising at least one optical probe defining two exit ends, the optical probe comprising at least one active section made from a scintillator and intended to emit photons under the effect of incident ionizing radiation and at least two transport sections that are placed on either side of the active section and configured to transport the photons emitted by the active section to the exit ends; at least one detection system comprising at least two photodetectors, each photodetector being connected to one respective exit end of the optical probe to receive and count the photons received from the exit end; and at least one processing module configured to determine the deposited dose on the basis of the measurements carried out by the photodetectors.

A radio-opaque plastic scintillator detector (PSD) for use in various medical applications and methods of making and using the PSD. The method requires coating a plastic scintillator fiber with a radio-opaque material; cutting the scintillator fiber; stripping the end of a plastic fiber optic fiber; cutting the naked end of a plastic fiber optic fiber; inserting a closely fitting guide tube over the naked end and inserting the cut scintillating fiber into the guide tube; coating the detector end of the cable with a light opaque polymer or jacket and adding a connector to the other end.

A device for determining a dose deposited in a scintillator by an ionizing radiation, comprises: a scintillator configured to be irradiated by the ionizing radiation and capable of emitting scintillation photons during interaction with the ionizing radiation; a measurement device comprising a single photodetector, the photodetector being a low-noise photodetector, the determination device being configured in such a way that the photodetector functions in single photon counting mode, the photodetector supplying, at the output of same, a measurement of the total intensity of light received by the photodetector from the scintillator; and an analyzer configured to determine a dose deposited in the scintillator by the ionizing radiation from the total intensity alone of light measured by the photodetector and a predetermined constant dependent only on the scintillator, the light output of the determination device and the type of ionizing radiation.

A device such as a dosimeter for detecting ionizing radiation, for example, X-ray radiation, in hospitals or the like. The device includes scintillator material configured to produce light as a result of radiation interacting with the scintillator material, and photoelectric conversion circuitry optically coupled to the scintillator material and configured to produce electrical signals via photoelectric conversion of light produced by the scintillator material. The device includes a plurality of photoelectric converters optically coupled with the scintillator material at spatially separated locations. The plurality of photoelectric converters thus produce respective electrical signals by photoelectric conversion of light produced by the scintillator material as a result of radiation interacting with the scintillator material. Improved energy linearity is thus facilitated while providing more efficient detection over the whole energy spectrum of radiation detected.