Levin et al., 1995 - Google Patents
A Monte Carlo correction for the effect of Compton scattering in 3-D PET brain imagingLevin et al., 1995
View PDF- Document ID
- 1894941834193117403
- Author
- Levin C
- Dahlbom M
- Hoffman E
- Publication year
- Publication venue
- IEEE transactions on nuclear science
External Links
Snippet
A Monte Carlo simulation has been developed to simulate and correct for the effect of Compton scatter in 3-D acquired PET brain scans. The method utilizes the 3-D reconstructed image volume as the source intensity distribution for a photon-tracking Monte Carlo …
- 230000000694 effects 0 title abstract description 16
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
- G01T1/00—Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
- G01T1/16—Measuring radiation intensity
- G01T1/161—Application in the field of nuclear medicine, e.g. in vivo counting
- G01T1/164—Scintigraphy
- G01T1/1641—Static instruments for imaging the distribution of radioactivity in one or two dimensions using one or several scintillating elements; Radio-isotope cameras
- G01T1/1647—Processing of scintigraphic data
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
- G01T1/00—Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
- G01T1/16—Measuring radiation intensity
- G01T1/161—Application in the field of nuclear medicine, e.g. in vivo counting
- G01T1/164—Scintigraphy
- G01T1/1641—Static instruments for imaging the distribution of radioactivity in one or two dimensions using one or several scintillating elements; Radio-isotope cameras
- G01T1/1648—Ancillary equipment for scintillation cameras, e.g. reference markers, devices for removing motion artifacts, calibration devices
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
- G01T1/00—Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
- G01T1/29—Measurement performed on radiation beams, e.g. position or section of the beam; Measurement of spatial distribution of radiation
- G01T1/2914—Measurement of spatial distribution of radiation
- G01T1/2985—In depth localisation, e.g. using positron emitters; Tomographic imaging (longitudinal and transverse section imaging; apparatus for radiation diagnosis sequentially in different planes, steroscopic radiation diagnosis)
-
- G—PHYSICS
- G06—COMPUTING; CALCULATING; COUNTING
- G06T—IMAGE DATA PROCESSING OR GENERATION, IN GENERAL
- G06T11/00—2D [Two Dimensional] image generation
- G06T11/003—Reconstruction from projections, e.g. tomography
- G06T11/005—Specific pre-processing for tomographic reconstruction, e.g. calibration, source positioning, rebinning, scatter correction, retrospective gating
-
- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61B—DIAGNOSIS; SURGERY; IDENTIFICATION
- A61B6/00—Apparatus for radiation diagnosis, e.g. combined with radiation therapy equipment
- A61B6/02—Devices for diagnosis sequentially in different planes; Stereoscopic radiation diagnosis
- A61B6/03—Computerised tomographs
- A61B6/037—Emission tomography
-
- G—PHYSICS
- G06—COMPUTING; CALCULATING; COUNTING
- G06T—IMAGE DATA PROCESSING OR GENERATION, IN GENERAL
- G06T2207/00—Indexing scheme for image analysis or image enhancement
- G06T2207/10—Image acquisition modality
- G06T2207/10072—Tomographic images
- G06T2207/10104—Positron emission tomography [PET]
-
- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61B—DIAGNOSIS; SURGERY; IDENTIFICATION
- A61B6/00—Apparatus for radiation diagnosis, e.g. combined with radiation therapy equipment
- A61B6/58—Testing, adjusting or calibrating devices for radiation diagnosis
- A61B6/582—Calibration
-
- G—PHYSICS
- G06—COMPUTING; CALCULATING; COUNTING
- G06T—IMAGE DATA PROCESSING OR GENERATION, IN GENERAL
- G06T2207/00—Indexing scheme for image analysis or image enhancement
- G06T2207/30—Subject of image; Context of image processing
- G06T2207/30004—Biomedical image processing
-
- G—PHYSICS
- G06—COMPUTING; CALCULATING; COUNTING
- G06T—IMAGE DATA PROCESSING OR GENERATION, IN GENERAL
- G06T2207/00—Indexing scheme for image analysis or image enhancement
- G06T2207/10—Image acquisition modality
- G06T2207/10072—Tomographic images
- G06T2207/10084—Hybrid tomography; Concurrent acquisition with multiple different tomographic modalities
-
- G—PHYSICS
- G06—COMPUTING; CALCULATING; COUNTING
- G06F—ELECTRICAL DIGITAL DATA PROCESSING
- G06F17/00—Digital computing or data processing equipment or methods, specially adapted for specific functions
- G06F17/10—Complex mathematical operations
-
- G—PHYSICS
- G06—COMPUTING; CALCULATING; COUNTING
- G06T—IMAGE DATA PROCESSING OR GENERATION, IN GENERAL
- G06T7/00—Image analysis
Similar Documents
Publication | Publication Date | Title |
---|---|---|
Levin et al. | A Monte Carlo correction for the effect of Compton scattering in 3-D PET brain imaging | |
Zaidi et al. | Scatter modelling and compensation in emission tomography | |
Ollinger | Model-based scatter correction for fully 3D PET | |
Zaidi | Comparative evaluation of scatter correction techniques in 3D positron emission tomography | |
Alessio et al. | Application and evaluation of a measured spatially variant system model for PET image reconstruction | |
Tong et al. | Image reconstruction for PET/CT scanners: past achievements and future challenges | |
Cherry et al. | Effects of scatter on model parameter estimates in 3D PET studies of the human brain | |
Song et al. | Fast modelling of the collimator–detector response in Monte Carlo simulation of SPECT imaging using the angular response function | |
Beekman et al. | Improved SPECT quantitation using fully three-dimensional iterative spatially variant scatter response compensation | |
Holdsworth et al. | Performance analysis of an improved 3-D PET Monte Carlo simulation and scatter correction | |
Zaidi et al. | Strategies for attenuation compensation in neurological PET studies | |
JP2021512312A (en) | Scattering correction for positron emission tomography (PET) | |
Zubal et al. | High resolution anthropomorphic phantom for Monte Carlo analysis of internal radiation sources | |
Zaidi et al. | Scatter correction strategies in emission tomography | |
Hamill et al. | Energy‐based scatter estimation in clinical PET | |
De Jong et al. | Efficient simulation of SPECT down‐scatter including photon interactions with crystal and lead | |
Levin et al. | Removal of the effect of Compton scattering in 3-D whole body positron emission tomography by Monte Carlo | |
Gustafsson et al. | Evaluation of attenuation corrections using Monte Carlo simulated lung SPECT | |
Hamill | Phantom evaluation of energy-based scatter estimation in an SiPM PET scanner | |
Zaidi | Reconstruction-based estimation of the scatter component in positron emission tomography | |
Ma et al. | Analytical modeling of PET imaging with correlated functional and structural images | |
Levin et al. | A Monte Carlo correction for Compton scattering effects in 3D PET brain imaging | |
Wu et al. | Scatter correction for 3D PET using beam stoppers combined with dual-energy window acquisition: a feasibility study | |
Trindade et al. | Clear-PEM: Monte Carlo performance and image reconstruction studies | |
Smith et al. | Evaluation of projection pixel-dependent and pixel-independent scatter correction in SPECT |