Patent classifications
G01T1/1641
CRYSTAL ARRAY, DETECTOR, MEDICAL DETECTION DEVICE AND METHOD OF MANUFACTURING CRYSTAL ARRAY
A crystal array, a detector, a medical detection device and a method for manufacturing a crystal array are provided. The crystal array includes a plurality of crystals arranged in an array, each of the crystals having a light incident surface, a light exit surface, and a connection surface connecting the light incident surface to the light exit surface, where the connection surface of at least one of two adjacent crystals includes a rough surface and a smooth surface connected to the rough surface, and the rough surface and the smooth surface are arranged along a length direction of the crystal.
HIGH RESOLUTION DEPTH-ENCODING PET DETECTOR WITH PRISMATOID LIGHT GUIDE ARRAY
Provided is are a particle detection device and method of fabrication thereof. The particle detection device includes a scintillator array that includes a plurality of scintillator crystals; a plurality of detectors provided on a bottom end of the scintillator array; and a plurality of prismatoids provided on a top end of the scintillator array. Prismatoids of the plurality of prismatoids are configured to redirect particles between top ends of crystals of the scintillator array. Bottom ends of a first group of crystals of the scintillator array are configured to direct particles to a first detector of the plurality of detectors and bottom ends of a second group of crystals of the scintillator array are configured to direct particles to a second detector substantially adjacent to the first detector.
SYSTEM AND METHOD OF USING TEMPORAL MEASUREMENTS OF LOCALIZED RADIATION TO ESTIMATE THE MAGNITUDE, LOCATION, AND VOLUME OF RADIOACTIVE MATERIAL IN THE BODY
A system and method for the measurement of radiation emitted from the body, for example, is presented. In one example, radiation sensors (e.g., gamma radiation sensors) may be used to measure activity proximate an injection site as a function of time. With that data, a function describing an amount of radioactive material in tissue proximate the injection site as a function of time may be estimated where an amount of radioactive material in the tissue at a time t is known. When an array of sensors is employed, the amount of radioactive material in the tissue proximate the injection site may be determined directly by the system. With an estimated function of radioactive material proximate the injection site as a function of time known, an estimated arterial input function may be determined, allowing for calculation of a correction factor that may be applied by a clinician during nuclear medical imaging.
Direct photon conversion detector
In the present invention a direct X-ray conversion layer comprises a material having a perovskite crystal structure. This is preferable since this enables constructing an X-ray detector with edge-on illuminated detector elements.
PROTON COMPUTED TOMOGRAPHY USING MULTICHANNEL GAS DETECTION TECHNOLOGY
A Proton Computed Tomography (pCT) system utilizing proton beams for construction of 3-dimensional density maps of both test phantoms and living tissue. PCT is a much sought-after modality for treatment planning and validation at proton therapy treatment centers, as it would allow in situ imaging with the same beam that is used for the treatment. A pCT system according to the present invention includes gaseous detectors for tracking and energy reconstruction, a shutter system to extend dynamic range features while maintaining good energy resolution, and a method for determining proton energy from a forward-search algorithm utilizing segmentation of energy detector ionization signal readout. The gaseous detectors are Gas Electron Multiplier (GEM) based gaseous detectors.
Motion detection for nuclear medicine imaging
A patient bed for a medical treatment system is equipped with a plurality of flexible photodetector pads arranged on top surface of the patient bed, where the flexible photodetector pads generate an electrical signal from ambient lighting. A monitoring circuit monitors the electrical signal generated by the plurality of flexible photodetector pads while a patient on the patient bed, where any change in the voltage level of the electrical signal from the plurality of flexible photodetector pads represents a movement of the patient.
Motion Detection for Nuclear Medicine Imaging
A patient bed for a medical treatment system is equipped with a plurality of flexible photodetector pads arranged on top surface of the patient bed, where the flexible photodetector pads generate an electrical signal from ambient lighting. A monitoring circuit monitors the electrical signal generated by the plurality of flexible photodetector pads while a patient on the patient bed, where any change in the voltage level of the electrical signal from the plurality of flexible photodetector pads represents a movement of the patient.
DIRECT PHOTON CONVERSION DETECTOR
In the present invention a direct X-ray conversion layer comprises a material having a perovskite crystal structure. This is preferable since this enables constructing an X-ray detector with edge-on illuminated detector elements.
Model-based scatter correction for non-parallel-hole collimators
Model-based scatter correction is used in SPECT with a non-parallel-hole collimator. Model-based scatter correction uses scatter kernels based on simulation to model the scatter for a given system and patient. For non-parallel-hole collimators, the measured sensitivity and measured vector maps are used in the modeling of scatter. The measured sensitivity is used to normalize the scatter kernels simulated for a parallel-hole collimator rather than attempting to simulate scatter with the complicated arrangement of holes. The measured vector maps are used to accurately project the model-based scatter sources into a data or emissions space.
Model-based Scatter Correction for Non-parallel-hole Collimators
Model-based scatter correction is used in SPECT with a non-parallel-hole collimator. Model-based scatter correction uses scatter kernels based on simulation to model the scatter for a given system and patient. For non-parallel-hole collimators, the measured sensitivity and measured vector maps are used in the modeling of scatter. The measured sensitivity is used to normalize the scatter kernels simulated for a parallel-hole collimator rather than attempting to simulate scatter with the complicated arrangement of holes. The measured vector maps are used to accurately project the model-based scatter sources into a data or emissions space.