A method of processing a SPECT image of a region of interest is disclosed. The SPECT image was obtained using at least one gamma detector detecting gamma radiation from the region of interest at multiple detector configurations, and the method includes: obtaining data indicative of the detector configurations and their spatial relationships to the region of interest; determining a resolution level for each of a plurality of directions in each point in the image based on the data obtained; and processing the image based on the resolution levels determined.

One embodiment provides a method, including: receiving a dataset associated with a plurality of photon emission events interacting with a detector array of an imaging device; identifying a first subset of the dataset associated with a plurality of unscattered photon emission events from the plurality of photon emission events; identifying a second subset of the dataset associated with at least one scattered photon event from the plurality of photon emission events; determining, for a scattered photon event, a likely location of emission of the scattered photon event using data from the first subset of the dataset associated with the plurality of unscattered photon events; and correcting the dataset by associating the scattered photon event with the determined likely location of emission. Other aspects are described and claimed.

An X-ray sensor (1) having an active detector region including a plurality of detector diodes (2) arranged on a surface region (3) of the X-ray sensor (1), a junction termination (4) surrounding the surface area (3) including the plurality of detector diodes (2), the junction termination (4) including a guard (5) arranged closest to the end of the surface region (3), a field stop (6) arranged outside the guard (2) and a number N of field limiting rings, FLRs (7) arranged between the guard (5) and the field stop (6), wherein each of the FLRs (7) are placed at positions selected so that distances between different FLRs (7) and between the guard and the first FLR lie within an effective area, the effective area being bounded by the lines =(10+1.3(n1)) m and =(5+1.05(n1)) m.

One embodiment provides a method, including: receiving a dataset associated with a plurality of photon emission events interacting with a detector array of an imaging device; identifying a first subset of the dataset associated with a plurality of unscattered photon emission events from the plurality of photon emission events; identifying a second subset of the dataset associated with at least one scattered photon event from the plurality of photon emission events; determining, for a scattered photon event, a likely location of emission of the scattered photon event using data from the first subset of the dataset associated with the plurality of unscattered photon events; and correcting the dataset by associating the scattered photon event with the determined likely location of emission. Other aspects are described and claimed.

Techniques for imaging radioactive emission in a target volume include collecting from each of multiple detectors in a Compton camera, within a coincidence time interval, location and deposited energy from an interaction associated with each high energy particle source event in a target volume, for N source events. A cone of possible locations for each source event is determined based on the locations and deposited energies collected. A SOE algorithm is initiated by selecting a random location on the cone and generating a histogram that indicates, a count of the selected locations that occur inside each voxel of the target volume. N solution locations for the N source events are determined after L iterations by updating the selected location on a corresponding cone based at least in part on values of the counts in the histogram excluding the current source event. A solution is presented on a display device.

An imaging method and device are described for improving the performance of a gamma camera by optimizing a figure of merit that depends upon cost, efficiency, and spatial resolution. In a modular gamma camera comprising a tiled array of gamma detector modules, the performance figure of merit can be optimized by sparsely placing gamma detector modules within the gamma camera, optimizing collimation, and providing means for detector and/or collimator motion. Sparse gamma cameras can be constructed as flat or curved panels, and elliptical or circular rings.

A PET detector array (8) comprising detector pixels acquires PET detection counts along lines of response (LORs). The counts are reconstructed to generate a reconstructed PET image (36, 46). The reconstructing is corrected for missing LORs which are missing due to dead detector pixels of the PET detector array. The correction may be by estimating counts along the missing LORs (60) by interpolating counts along LORs (66) neighboring the missing LORs. The interpolation may be iterative to handle contiguous groups of missing detector pixels. The correction may be by computing a sensitivity matrix having matrix elements corresponding to image elements (80, 82) of the reconstructed PET image. In this case, each matrix element is computed as a summation over all LORs intersecting the corresponding image element excepting the missing LORs. The computed sensitivity matrix is used in the reconstructing.

An imaging system including an imaging device and/or a cooling system is provided. The imaging system may include a control module, an imaging device, and/or a cooling system. The imaging device may include a first portion and a second portion. The cooling system may include a cooling module configured to generate a cooling medium, and/or a cooling medium passage configured to spread the cooling medium. The cooling medium passage may belong to a closed loop. At least part of the cooling system may be located within the imaging device such that the cooling medium may be in direct contact with the at least part of the imaging device.

One embodiment provides an imaging device, including: an enclosure comprising a casing and a radiation lining arranged within the casing to provide a radiation shield, wherein the enclosure comprises a removable portion; a plurality of modular components being in communication with calibration code, wherein the calibration code calibrates the imaging device based upon information of the plurality of modular components; each of the plurality of modular components comprising a plurality of gamma detectors including semiconductor crystals and being removable from the imaging device; the plurality of modular components being arranged such that the plurality of gamma detectors are configured in an array configuration with each of the plurality of gamma detectors having a predetermined spacing from each other gamma detector; a plurality of electronic communication components, wherein the plurality of electronic communication components facilitate communication from each of the gamma detectors using a hierarchical communication technique; and a cooling system.

A method and an apparatus are provided for using a capacitor chain to perform charge sharing and Anger logic to determine, for charge pulses arising from gamma-ray detection, a row position along an array of scintillation-based gamma-ray detectors. Further, high-pass filters configured at the ends of the capacitor chain perform pulse shaping to preserve timing information. To determine the column position for charge pulses, a two-stage summing amplifier configuration is used with weighting amplifiers controlling the relative gain of the second-stage amplifier with respect to respective columns in the array. Each detector element in the array is a silicon photomultiplier (e.g., Geiger-mode avalanched photodiodes biased above breakdown voltage). Position information can be generated by Anger logic on four outputs from the second-stage amplifiers. Energy and timing information can be generated as a sum of the four outputs from the second-stage amplifiers.