An arrangement for determining an energy spectrum of a beam of radiation or particles is disclosed. The arrangement comprises a plurality of polymeric bodies. Each of the plurality of polymeric bodies includes an optical waveguide. Each of the plurality of polymeric bodies has a scintillator disposed at a respective end of the optical waveguide. The scintillators are arranged relative to each other such that an energy resolution of a particle beam incident on the arrangement can be determined. Furthermore, a particle detector with the arrangement and an evaluation unit for reading out the particle detector are disclosed.

Disclosed herein is a method for image tracking using an X-ray imaging system during an interventional radiology procedure on a human or an animal. The method may comprise acquiring a first image of an object inside a human or an animal with a first X-ray detector of the X-ray imaging system; acquiring a second image of the object with the X-ray imaging system during the interventional radiology procedure, at a time later than acquiring the first image; determining a displacement of the first X-ray detector based on the first image and the second image; moving the first X-ray detector by the displacement, with an actuator of the X-ray imaging system. The X-ray imaging system comprises the first X-ray detector, the second X-ray detector and the actuator. A spatial resolution of the first X-ray detector is higher than a spatial resolution of the second X-ray detector.

Measuring and tracking energy emitted by a radiation source. A system includes an image sensor for sensing electromagnetic radiation and a scintillator. The scintillator absorbs energy emitted by a radiation source and scintillates the absorbed energy. The system is such that the image sensor senses an image frame depicting at least a portion of the scintillator when the radiation source emits the energy. The image frame comprises an indication of where the energy is absorbed by the scintillator.

Systems and methods for determining beam asymmetry in a radiation treatment system using electronic portal imaging devices (EPIDs) without implementation of elaborate and complex EPID calibration procedures. The beam asymmetry is determined based on radiation scattered from different points in the radiation beam and measured with the same region of interest ROI of the EPID.

A radiation diagnostic device according to an aspect of the present invention includes a first detector, a second detector, and processing circuitry. The first detector detects Cherenkov light that is generated when radiation passes. The second detector is disposed to be opposed to the first detector on a side distant from a generation source of the radiation, and detects energy information of the radiation. The processing circuitry specifies Compton scattering events detected by the second detector, and determines an event corresponding to an incident channel among the specified Compton scattering events based on a detection result obtained by the first detector.

A particle detector according to one embodiment includes: superconductive lines, conductive lines, insulating films, a first detection circuit, and a second detection circuit. The superconductive lines extend in a first direction and are arranged in a second direction intersecting the first direction. The conductive lines extend in a third direction different from the first direction and are arranged in a fourth direction intersecting the third direction. The insulating films are each interposed at an intersection point between one of the superconductive lines and one of the conductive lines. The first detection circuit detects a voltage change occurring in the superconductive lines. The second detection circuit detects a current or a voltage generated in the conductive lines when the voltage change occurs.

A method for operating a medical imaging apparatus includes acquiring an intensity distribution of an X-ray radiation by a first X-ray detector assigned to a first radiation source. A scattered radiation distribution of scattered radiation generated at the object is acquired by a second X-ray detector. A spatial distribution for the component of the scattered radiation is estimated based on the scattered radiation distribution acquired by the second X-ray detector. An intensity distribution of the component of the transmitted primary X-ray radiation is determined from the intensity distribution acquired by the first X-ray detector depending on the estimated spatial distribution.

A measurement apparatus for determining a water equivalent path length (WEPL) through an object (100), the measurement apparatus comprising a proton beam source (1) arranged to produce, in use, a beam (2) of protons having a beam shape; a proton detector (3), the proton detector (3) defining a proton detection plane, the proton detector (3) being arranged to measure a spatial profile of protons incident the proton detection plane; and energy deposited inside the detector by protons incident on the proton detection plane the proton detector (3) further arranged to provide a signal indicative of the measured energy with the spatial profile; and a processor (4) coupled to the proton detector (3) so as to process the signal; in which the proton beam source (1) and the proton detector (3) define between them a space for the object (100), and in which the processor (4) is arranged to process the signal so as to fit the spatial profile and deposited energy measured after the proton beam (2) has passed through the object (100) to a distribution having parameters, and from the parameters estimate a water equivalent path length of the object (100).

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

A device and a method for measuring proton beam source position and beamline center are disclosed. The device includes N quadrupole magnets, a laser, a target and a scintillation screen; the target and the scintillation screen are arranged in front of and behind the N-quadrupole lens, respectively; the N-quadrupole lens can be converted to a M-quadrupole lens; the position of proton beam after being focused by the N- or M-quadrupole lens on the scintillation screen is measured; according to the amplification factor and the proton beam position, the offset of the proton beam source from the beamline center, as well as the position of the beamline center on the scintillation screen are calculated; the disclosure can accurately determine the position of the beamline center and the proton beam source by the use of N quadrupole magnets, combined with a scintillation screen.