METHOD AND APPARATUS TO USE A BROAD-SPECTRUM ENERGY SOURCE TO CORRECT A NONLINEAR ENERGY RESPONSE OF A GAMMA-RAY DETECTOR

    公开(公告)号:US20210247530A1

    公开(公告)日:2021-08-12

    申请号:US16788741

    申请日:2020-02-12

    Abstract: A method and apparatus are provided for nonlinear energy correction of a gamma-ray detector using a calibration spectrum acquired from the background radiation of lutetium isotope 176 (Lu-176) present in scintillators in the gamma-ray detector. Further, by periodically acquiring Lu-176 spectra using the background radiation from the scintillators, the nonlinear energy correction can be monitored to detect when changes in the gamma-ray detector cause the detector to go out of calibration, and then use a newly acquired Lu-176 spectrum to update the calibration of the nonlinear energy correction as needed. The detector calibration is performed by comparing a reference histogram to a calibration histogram generated using the nonlinear energy correction, and adjusting the parameters of the nonlinear energy correction until the two histograms match. Alternatively, the detector calibration is performed by comparing reference and calibration values for specific spectral features, rather than for the whole Lu-176 spectrum.

    TIME-WALK CORRECTION USING MULTIPLE ENERGY MEASUREMENTS

    公开(公告)号:US20240210575A1

    公开(公告)日:2024-06-27

    申请号:US18086966

    申请日:2022-12-22

    CPC classification number: G01T1/2006 G01T1/15 G01T1/1644 H03K3/021

    Abstract: An apparatus and method are provided to correct for time-walk errors during photon detections (e.g., detecting gamma rays). A time-walk correction is determined using measurements of energy (or charge) that apply different time windows, enabling corrections accounting for variations in the ratio between fast and slow components in the detected pulse. For example, one time window can be used to integrate the leading end of the pulse, thereby predominantly measuring the fast component, while a second window is used to integrate a trailing end of the pulse to predominantly measure the slow component. Alternatively or additionally, low-pass and high-pass filters may select the slow and fast components, respectively. The time-walk correction is a function of multiple measurements representing different components (e.g., fast and slow) of the pulse shape.

    METHOD AND APPARATUS TO USE A BROAD-SPECTRUM ENERGY SOURCE TO CORRECT A NONLINEAR ENERGY RESPONSE OF A GAMMA-RAY DETECTOR

    公开(公告)号:US20200379133A1

    公开(公告)日:2020-12-03

    申请号:US16738828

    申请日:2020-01-09

    Abstract: 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.

    METHOD AND APPARATUS TO USE A SINGLE ENERGY SOURCE TO DETERMINE ENERGY CORRECTION FOR A GAMMA DETECTOR

    公开(公告)号:US20200249369A1

    公开(公告)日:2020-08-06

    申请号:US16269380

    申请日:2019-02-06

    Abstract: A method and apparatus are provided for positron emission imaging to calibrate energy measurements of a pixilated gamma-ray detector using energy sharing events between channels of the detector. Due to conservation of energy, when the energy of a single gamma ray shared among multiple channels, the sum of measured energies across the respective channel must equal the original energy of the incident gamma ray. Further, the fractions of the original energy distributed to the respective channels can span the entire range of zero to the original energy. Thus, a single gamma-ray source (e.g., cesium isotope 137) can be used to continuously calibrate the nonlinear energy response of the detector over an entire range of interest.

    PET RECONSTRUCTION FOR ADJUSTABLE PET SYSTEM

    公开(公告)号:US20240122558A1

    公开(公告)日:2024-04-18

    申请号:US17963737

    申请日:2022-10-11

    CPC classification number: A61B6/037 A61B6/4258 A61B6/481

    Abstract: A PET scanner includes gamma-ray detector rings that form a bore through which an imaging subject is translated, a length of the bore defining an axial length of the PET scanner, the gamma-ray detector rings being movable along the axial length, the gamma-ray detector rings including gamma-ray detector modules therein, and processing circuitry configured to receive PET data associated with a plurality of transaxial slices of the imaging subject, the PET data including a first set of spatial information and timing information corresponding to a first data acquisition period for the gamma-ray detector modules in a first axial position and a second set of spatial information and timing information corresponding to a second data acquisition period for the gamma-ray detector modules in a second axial position, and reconstruct a PET image based on the first set of spatial and timing information and the second set of spatial and timing information.

    PCCT ENERGY CALIBRATION FROM X-RAY TUBE SPECTRA USING A NEURAL NETWORK

    公开(公告)号:US20240230934A1

    公开(公告)日:2024-07-11

    申请号:US18152856

    申请日:2023-01-11

    CPC classification number: G01T7/005 G06N3/08

    Abstract: An apparatus for calibrating a detector, including acquiring an energy spectrum obtained from a scan using an X-ray tube as a source of radiation, estimating calibration parameters, such as a gain and an offset, for each of several channels of the detector by applying the acquired first energy spectrum to inputs of a trained neural network that outputs the calibration parameters, and calibrating each of the plurality of channels using the estimation parameters. The neural network is trained to produce target output calibration parameters, using two or more measurements selected from isotope peak positions, K-edge absorption features, or K-edge emission peaks.

    SUMMING CIRCUIT FOR POSITRON EMISSION TOMOGRAPHY DIAGNOSTIC APPARATUS

    公开(公告)号:US20220397688A1

    公开(公告)日:2022-12-15

    申请号:US17345823

    申请日:2021-06-11

    Abstract: A circuit for receiving signals from a photodetector array arranged to detect signals generated by a crystal includes a plurality of summing circuits having weighting circuits, the summing circuits being configured to produce outputs corresponding to a total energy of the signals, a position of the signals in a first dimension of the photodetector array, a position of the signals in a second dimension of the photodetector array, and a radius of a charge distribution of the signals.

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