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Use of a magnetic field to increase the spatial resolution of positron emission tomography
Author(s) -
Hammer Bruce E.,
Christensen Nelson L.,
Heil Brian G.
Publication year - 1994
Publication title -
medical physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.473
H-Index - 180
eISSN - 2473-4209
pISSN - 0094-2405
DOI - 10.1118/1.597178
Subject(s) - positron emission tomography , positron , full width at half maximum , image resolution , positron emission , physics , magnetic field , resolution (logic) , range (aeronautics) , detector , nuclear medicine , annihilation , optics , tomography , materials science , nuclear magnetic resonance , nuclear physics , electron , medicine , quantum mechanics , artificial intelligence , computer science , composite material
Detector geometry, spatial sampling, and more fundamentally, positron range and noncollinearity of annihilation photon emission define Positron Emission Tomography (PET) spatial resolution. In this paper, a strong magnetic field is used to constrain positron travel transverse to the field. Measurement of the spread function from a 500 μm diameter 68 Ga impregnated resin bead shows a squeezing of the full width at half maximum (FWHM) by a factor of 1.0, 1.22, 1.42, and 2.05, at 0, 4.0, 5.0, and 9.4 Tesla, respectively. The full width at tenth maximum (FWTM) decreases by a factor of 1.0, 1.73, 2.09, and 3.20, at 0, 4.0, 5.0, and 9.0 Tesla, respectively. Acquiring a PET image in a magnetic field should significantly reduce resolution loss due to positron range.