Utah State University

Raymond P DeVito

Timothy Edwin Doyle

A radiation detection, localization, and identification system uses a searching algorithm to identify hypothetical solutions to Compton scatter data. Model based representations of the physical data collection yield the location of radiation sources when suppressed correlations of source location are identified in processed event data. The system's detector is an array of radiation detectors networked to act as a single detection system. This network has wide area of view and high sensitivity to radiation sources since no collimation is required.

Suppressed correlation method for identifying radioactive sources

A neutron source illuminates suspect material leading to emission of gamma rays characteristic of the isotopes present. The system measures Compton scattering of emitted gamma rays using detectors with three dimension event localization capability. Detection does not require full energy deposition. A spatial correlation of projection vectors is computed by a reconstruction that searches for solutions that generate spatial correlation. Identification and location for contraband material is determined from solutions that generate spatial correlation.

Identification and localization of explosives and other material

A radiation detection, localization, and identification system uses a searching algorithm to identify hypothetical solutions to Compton scatter data. Model based representations of the physical data collection yield the identity and location of radiation sources when correct associations of gamma ray energies and locations are made with detected data events. The system's detector is an array of radiation detectors networked to act as a single detection system. This network has wide area of view and high sensitivity to radiation sources since no collimation is required.

Identification and localization of radioisotopes using likelihood estimation

A method for improving single photon emission computed tomography by controlling acquisition parameters specific to the imaging goals and specific to the individual case under study. Data acquisition is modulated by scanning to adapt to the particular signal to noise characteristics of each object. A preliminary acquisition quickly scans the object of interest. The preliminary data is analyzed to optimize the secondary scan. The secondary scan is then acquired with optimized sampling of the object based on its own particular image characteristics. The system is able to learn, incorporating site specific data into a triaging set.

Optimized case specific SPECT sampling

A radiation detection, localization, and identification system uses a searching algorithm to identify geometric correlation of hypothetical solutions to Compton Imaging. Geometric correlation of correct associations of gamma ray energies with each detected event yields the identity and location of radiation sources. The system's detector is an array of radiation detectors networked to act as a single detection system. This network has wide area of view and high sensitivity to radiation sources since no collimation is required.

Identification and localization of radioisotopes

An ionization detector having a grid of electrodes disposed perpendicular to an oscillating voltage. Charge released from an ionization event oscillates in the detector medium at the same frequency as the applied oscillating voltage. The electrode grid is configured to measure induced oscillating charge from the oscillating ionization charge in the detector. The detector signal is obtained from readout of the induced oscillating charge on the electrodes. Signal processing electronics processes the measured signal from the oscillating induced charge to derive energy and position information of the ionization event. A bias voltage is applied across the detector to further sweep the ionization charge from the active detection volume.

Radiation detector

A radioisotope identification and localization device having at least one radiation detector with three dimensional event localization that utilizes a spatial correlation of projection vectors arising from Compton scattering of gamma ray emissions. Source identification and location is supplied by a reconstruction that searches for solutions with radioactive material of unknown type. Detection, identification and localization does not require full energy deposition. Identification and location of known or unknown radioactive material somewhere in a large active area of interrogation is achieved.

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Lansing, UT, United States of America

Raymond P DeVito