This invention provides a scan method, scan system and radiation scan controller, and relates to the field of radiation. Wherein, the scan method of this invention comprises: obtaining detection data of an object to be inspected under radiation scanning using a detector; adjusting an accelerator output beam dose rate and/or an output electron beam energy level of a radiation emission device according to the detection data. With this method, working conditions of the accelerator of the radiation emission device may be adjusted according to the detection data detected by the detector, so that for a region having a larger mass thickness, a higher output beam dose rate or a higher electron beam output energy level is adopted to guarantee satisfied imaging technical indexes, for a region having a smaller mass thickness, a lower output beam dose rate or a lower electron beam output energy level is adopted to reduce the environmental dose level while guaranteeing satisfied imaging technical indexes.

The invention relates to a hybrid medical PET-SPECT/MR imaging device comprising at least one scintillating crystal and at least one module for detecting radiation which contains at least one matrix of photodetectors and an electronics section, such that said module has a mechanical structure, the external, internal or both surfaces of which are divided into at least two sections, of which at least one is coated in graphene, and the rest in non-ferromagnetic conductive material, or all the sections are coated in graphene, and such that the coating forms a Faraday cage. The invention also relates to a shielding against radiofrequency for a medical imaging device, comprising a graphene coating, which is continuous or in bands, on all the faces of the mechanical structure of the detection module of the device, or a graphene coating, continuous or in bands, on at least one face, combined with a coating of non-ferromagnetic conductive materials on the remaining faces, and said shielding forming a Faraday cage.

Methods, devices and computer-readable mediums for clock synchronization are provided. The methods include receiving a synchronizing clock in a unit clock cycle of a measuring clock, calibrating position information of a rising edge of the synchronizing clock in the unit clock cycle, determining a phase difference between the measuring clock and the synchronizing clock in the unit clock cycle based on the calibrated position information, and compensating a photon time in the unit clock cycle with the determined phase difference as a time compensation value.

A radiographic capturing apparatus includes the following. A wireless communication circuit or a wireless communication device establishes wireless communication with an external unit. A power supply circuit feeds electrical power to the wireless communication circuit or the wireless communication device and is switchable between a low-load mode and a high-load mode. The power supply circuit is able to feed a current having a larger value in the high-load mode than in the low-load mode. A power supply efficiency of the power supply circuit in the high-load mode is lower than that in the low-load mode when a current having a small value as in the low-load mode is fed in the high-load mode. A switcher switches a load mode of the power supply circuit based on the detected or obtained load state. A built-in power supply feeds electrical power to the power supply circuit.

An apparatus comprising a radiation source, coincident positron emission detectors configured to detect coincident positron annihilation emissions originating within a coordinate system, and a controller coupled to the radiation source and the coincident positron emission detectors, the controller configured to identify coincident positron annihilation emission paths intersecting one or more volumes in the coordinate system and align the radiation source along an identified coincident positron annihilation emission path.

In capturing an image of a grid by an image detector, a measurement pixel that is not in the position of a specific point having a maximum or minimum value of an output signal is referred to as a first measurement pixel, and a measurement pixel that is in the position of the specific point is referred to as a second measurement pixel. The disposition of the first and second measurement pixels are determined so as to satisfy the following condition: fG/fN≠odd number, wherein fG is a grid frequency and fN is a Nyquist frequency of pixels; and in shifting the grid C times by one pixel, the number of the first measurement pixels is larger than that of the second measurement pixels at any time in the range of a cycle C of a repetition pattern appearing in the image.

Provided is a preview image generating section configured to generate preview image during radiography for the purpose of providing a radiation tomography apparatus that allows suppression of unnecessary imaging time by displaying a condition of an image during the radiography in the process of diagnosis. An operator can recognize from the preview image how a subject appears in the image in a radiation tomography apparatus also during the radiography. This allows stopping the radiography before a diagnostic image having a suitable level of clearness for diagnosis is generated. As a result, a shorter imaging time is achieved, and burden to the subject can be suppressed.

An X-ray detector assembly for an imaging system is provided. The X-ray detector assembly includes a block for mounting to a rotating disc, the block including two opposing end surfaces, two opposing side surfaces and at least one mounting surface, and at least two detector chips, each detector chip including an X-ray detecting surface and an opposing block-facing surface, two opposing end surfaces and two opposing side surfaces, and each detector chip having a flexible bus mounted to the opposing block-facing surface of the detector chip adjacent to a side surface of the detector chip. The at least one mounting surface of the block receives the at least two detector chips in side-by-side disposition, with the buses of the at least two detector chips extending along a side surface of the block.

A method and apparatus are provided for positron emission imaging to calibrate energy measurements of a pixilated gamma-ray detector using energy calibration based on a calibration with a distribution energy signature (i.e., having more spectral features than just a single full-energy peak). The energy calibration can be performed using a deep learning (DL) network or a physics-based model. Using the DL network, a calibration spectrum is applied to either generate the measured-signal values of known energy values (e.g., spectral peaks for spectra of various radioactive isotopes) or the parameters of an energy-calibration function/model.

An energy sensor is provided including a collimator comprising a plurality of sensor apertures aligned in a plurality of directions configured to allow passage of an energetic particle or photon in a specific direction for respective apertures of the plurality of sensor apertures and at least one energy detector configured to measure the energetic particle or photon including a plurality of detector segments. Respective detector segments of the plurality of detector segments are aligned with the respective sensor apertures and a detector segment which measures the energetic particle or photon is indicative of a directionality of the energetic particle or photon.