Abstract:
A patient (14), at rest, is injected with a first isotope tracer. After a first uptake period, the patient is stressed and injected with a second isotope tracer. After a second isotope tracer uptake period, first and second isotope imaging data are concurrently detected by data acquiring devices (16). The first and second isotope imaging data are reconstructed into a first or rest state image, a second or stressed state image, and optionally a combined first and second isotope image. The image with the better image statistics is segmented to generate segmentation parameters, which segmentation parameters are applied to both the first or rest and second or stressed state images. In this manner, an image whose image statistics may be too weak for accurate segmentation is accurately segmented by generating two inherently aligned images and applying the same segmentation parameters to both.
Abstract:
When reconstructing low-collimation nuclear scan data (18) (e.g., SPECT) into a nuclear image volume (19), a spatial frequency-dependent (SFD) filter function is applied in Fourier space to the reconstructed image (19) to improve image resolution given a predefined number of reconstruction iterations and/or to reduce the number of reconstruction iterations required to achieve a predetermined level of image resolution. Size of an object to be imaged is determined, and the SFD filter function is determined or generated based on signal power spectrum (and/or modulated transfer function) data, object size, and desired image quality (or number of reconstruction iterations). The SFD filter function amplifies higher-energy components (e.g., corresponding to a lesion or tumor, or the like) of the spatial frequency spectrum to improve viability in a low collimated nuclear image (19) using fewer reconstruction iterations.
Abstract:
A detector arrangement providing imaging information at the edge of the scintillator is provided. The detector arrangement provides complete information and improved spatial resolution. SiPMs can be used in place of PMTs in order to provide the geometrical coverage of the scintillator and improved spatial resolution. With such detector arrangements, the spatial resolution can be under 2 mm. Furthermore, the overall thickness of the detector can be substantially reduced and depth of interaction resolution is also improved.
Abstract:
The present invention is directed to a Gd 2 O 2 S: M fluorescent ceramic material with a very short afterglow, wherein M represents at least one element selected from the group Pr, Tb, Yb, Dy, Sm and/or Ho and the Gd 2 O 2 S: M fluorescent ceramic material comprises further: europium of ≤ 1 wt. ppm based on Gd 2 O 2 S, and cerium of ≥ 0.1 wt. ppm to ≤ 100 wt. ppm based on Gd 2 O 2 S, wherein the content of cerium is in excess of the content of europium with a ratio of europium to cerium of 1 : l0 to l : 150.
Abstract:
A radiation imaging device suitable for SPECT or other nuclear imaging includes a detector (22) which receives radiation. A fan beam-slit collimator (20) is positioned adjacent a radiation receiving face (32) of the detector, intermediate the detector and a radiation source (12, 18). The collimator includes a plurality of slats (30) having a common focus. A body (44) adjacent the slats defines one or more elongate slits (46). The slit is arranged such that radiation passes through the slit and between the slats to the detector face. The body is at least substantially impermeable to the radiation. The fan beam-slit collimator (20) enables higher resolution or efficiency to be achieved from the detector.
Abstract:
The invention relates to an X-ray detector with detector elements (1) arranged in a layer. The detector elements (1) contain a scintillator element (2) for the conversion of X-rays (X) into photons (v), a photodiode (5) for detection of the photons (v), and a processing circuit (4) for the processing of electric signals generated by the photodiode (5). In order to protect the electronics (4) from X-rays a shielding (3) of variable effective thickness (dl, d2) is disposed in front of the electronics (4). This shielding (3) can in particular be L-shaped. By reduction of the effective thickness of the shielding (3) to a necessary minimum the volume of the scintillator unit (2) can be maximized.
Abstract:
A nuclear imaging system includes a scanner (8), such as a PET scanner. A patient is injected with a [ 13 N]ammonia radioisotope tracer which is contaminated with a small percent of 18 F contamination. The scanner receives radiation from the injected tracer and a reconstruction processor (28) reconstructs the detected radiation into image representations. A warning generator (12) generates warnings to the clinician concerning the effects of the 18 F contamination. A calibration processor (16) generates an estimated decay curve based on a time since the end of the proton bombardment which created the tracer and a priori information about the tracer. An activity meter (42) measures radiation emitted from a sample of the tracer and a dose calibrator (44) determines a decay curve from the measured radiation. Either the detected radiation is corrected in accordance with one of the decay curves during reconstruction or a correction processor (50) corrects reconstructed images in accordance with one or both of the decay curves. A display (14) displays uncorrected reconstructed images and the decay curve and/or the corrected images.
Abstract:
In a medical system, at least one medically operative member (10, 12, 100) is configured to interact with or acquire data from a subject (74) disposed in an examination region. An array of photosensors (70, 170) is disposed on the at least one medically operative member. The array of photosensors is arranged to view the examination region. A position-determining member (82, 82a, 82b) is configured to determine a position of at least one optically detectable marker (72, 172) disposed with the subject in the examination region based on light from the at least one optically detectable marker sensed by the array of photosensors.
Abstract:
In a disclosed imaging method, the instantaneous speed or data acquisition dwell times of a detector head (14, 16) is optimized as a function of position along a path (P) of the detector head around a subject (S, SS, SXL). The optimization is respective to an expected radioactive emission profile (EPROI) of a region of interest (H, HS, HXL) that is less than the entire subject. The detector head is traversed along the path using the optimized instantaneous speed or data acquisition dwell times (40). During the traversing, imaging data are acquired using the detector head. The acquired imaging data are reconstructed to generate a reconstructed image of at least the region of interest. A gamma camera (10) configured to perform the foregoing imaging method is also disclosed.
Abstract:
The present invention is directed to a Gd 2 O 2 S: M fluorescent ceramic material with a very short afterglow, wherein M represents at least one element selected from the group Pr, Tb, Yb, Dy, Sm and/or Ho and the Gd 2 O 2 S: M fluorescent ceramic material comprises further: europium of = 1 wt. ppm based on Gd 2 O 2 S, and cerium of = 0.1 wt. ppm to = 100 wt. ppm based on Gd 2 O 2 S, wherein the content of cerium is in excess of the content of europium with a ratio of europium to cerium of 1 : l0 to l : 150.
Abstract translation:本发明涉及具有非常短的余辉的Gd 2 O 2 S 2 M荧光陶瓷材料,其中M表示选自Pr, Tb,Yb,Dy,Sm和/或Ho和Gd 2 O 2 S 2 M荧光陶瓷材料进一步包括:铕= 1wt。 基于Gd 2 O 2 S的ppm和= 0.1重量%的铈。 ppm至= 100重量% ppm,基于Gd 2 O 2 S,其中铈的含量超过铕的含量,铕与铈的比例为1:10至1: 150。