Techniques for imaging radioactive emission in a target volume include receiving data indicating a set of one or more known emission energies associated with a high energy particle source and determining a Compton line for each emission energy in the set. A Compton camera collects location and deposited energy from an interaction associated with a single source event from a target volume of a subject. For the single source event, an earliest deposited energy, E.sub.1, and first scattering angle, .sub.1, and a cone of possible locations for the source event are determined. A particular location for the high energy particle source within the target volume without including the single source event, if E.sub.1 is not within a predetermined interval of the Compton line for at least one of known emission energies. A solution is presented on a FILTER display device.

An image processing apparatus for processing a radiation image, includes: a reception unit configured to receive processing information obtained by processing of the radiation image by an external processing apparatus; and a display control unit configured to control displaying at least one of a reception status of the processing information and a determination result of the reception status on a display unit.

A radiation detection device is provided that is wide in visual field, wide in application range of radiation energy, and which is smaller and lighter in weight as compared to other devices. The device includes a detecting element group has a plurality of detecting elements that detect radiation are three-dimensionally arranged. The detecting element group has a structure with a depletion formed by removing the detecting element at any position from a virtual detecting element group in which the detecting elements are laid out on any virtual surface. The depletion is provided at a position at which a difference of detected values between one detecting element and another detecting element arranged along any direction exhibits different values in a case where the radiation having the direction as an incident direction enters and a case where the radiation having an opposite direction of the direction as an incident direction enters.

A system for monitoring radiation treatment images Cherenkov emissions from tissue of a subject. A processor of the system determines densities of a surface layer of the subject from 3D images of the tissue to determine correction factors. The processor uses these factors to correct the Cherenkov images for attenuation of Cherenkov light by tissue, making them proportional to radiation dose. In embodiments, the system obtains reflectance images of the subject, determines second correction factors therefrom, and applies the second correction factors to the Cherenkov emissions images. In embodiments, the corrected images of Cherenkov emissions are compared to dose maps of a treatment plan. A method of correcting Cherenkov emissions images includes determining tissue characteristics from CT or MRI images in a surface volume where Cherenkov is expected, using; imaging Cherenkov emissions; and using the tissue characteristics to correct the images for variations in Cherenkov light propagation through the tissue.

A microwave imaging system and method are disclosed for generating a 3-D map of a body. The system comprises a source of coherent microwave radiation for irradiating the body, at least one microwave detector for detecting at a plurality of locations around the body the amplitude and phase of radiation that has passed through, or has been reflected by, the body, an analyser connected to receive signals from the or each detector and from the source and operative to produce a holographic image indicative at each detection location the phase of the received radiation relative to the phase of radiation received directly from the source at the same location, and a processor for processing the holographic image to calculate in three dimensions the positions of localized physical parameters within the body.

Disclosed herein is a method comprising: directing X-ray in a first wavelength range and X-ray in a second wavelength range are directed to a subject; introducing a contrast agent into the subject; capturing a first image with the X-ray in the first wavelength range and a second image with the X-ray in the second wavelength range; determining a differential image between the first image and second image; wherein strength of interaction between the contrast agent and the X-ray in the first wavelength range and the strength of interaction between the contrast agent and the X-ray in the second wavelength range are different.

Method and apparatus are disclosed for generating a scatter-corrected image from positron emission tomography (PET) or other radioemission imaging data (20) acquired of an object (12) in a field of view (14). A background portion (26B) of the PET imaging data is identified corresponding to a background region (14B) of the FOV that is outside of the object. An outside-FOV activity estimate (40) for at least one spatial region outside of the FOV and into which the object extends is adjusted (e.g. iterative or several randomly selected estimates) to optimize a simulated scatter distribution for the combination of the PET imaging data and the outside FOV activity estimate to match the background portion (26B) of the PET imaging data. The PET imaging data are reconstructed to generate a scatter-corrected PET image of the object in the FOV using the optimized simulated scatter distribution.

A portable gamma ray computed topography (CT) device configured to capture images includes a projector, a collimator, and a detector. The projector includes an isotope encapsulated within a depleted uranium, and the collimator is affixed to the projector eliminating use of a guide tube. The apparatus also includes a crank cable affixed to the isotope, and is configured to extend the isotope out of projector and into the collimator. The apparatus further includes a detector configured to capture multiple shots on order of hundreds of shots to create a three-dimensional (3D) reconstruction from infield gamma ray images.

An X-ray system for acquiring projection measurement data of an examination object comprises: an X-ray emitter arrangement having an X-ray radiation source to emit X-rays; and a photon-counting X-ray detector with at least one detection threshold for spectrally resolved detection of the X-rays. The at least one detection threshold is variable spatially and/or temporally in a same measurement.

The embodiments of the present disclosure provide a method, system, and readable medium for data processing. The method may include: obtaining one or more data processing parameters, the one or more data processing parameters being determined based on a reference detector module; obtaining target data of a target object collected by one or more signal detectors; and processing the target data based on the one or more data processing parameters.