title: The geometric modulation transfer function of a transmission imaging system that uses a SPECT scintillation camera and parallel hole collimation.
abstract: An analytic expression has been derived to calculate the geometric modulation transfer function of a transmission imaging system that uses parallel hole collimation for both the source and the SPECT camera. This expression describes the resolution of the transmission imaging system and replaces the need to use computer intensive Monte Carlo simulations for the system design. The geometric modulation transfer function, denoted as MTFg(rho) = [A2sc(Ssc rho)**A2cc(Scc rho)]D(rho), where ** denotes two-dimensional convolution; Asc(rho) and Acc(rho) are the Fourier transforms (FT) of the aperture functions for the parallel hole source collimator (SC) and the camera collimator (CC) holes, respectively; D(rho) is the FT of the camera response; and ssc and scc are scaling constants that depend on the respective collimator dimensions, the system dimensions, the object distance above camera collimator and whether MTFg(rho) is calculated for the object or image plane. The theoretical MTFg(rho) was verified with Monte Carlo simulations and experimental results. The formalism shows that the system resolution is characterized by the camera resolution and a combination of the resolutions of the source and camera collimators. This expression can be used to optimize the design of transmission imaging systems to be used in nuclear medicine.
authors.affiliation: Department of Nuclear Medicine and Magnetic Resonance, St. Joseph's Health Center, Lawson Research Institute, London, Ontario, Canada.
authors.forename: B J
authors.initials: BJ
authors.lastname: Kemp
authors.forename: F S
authors.initials: FS
authors.lastname: Prato
authors.forename: R L
authors.initials: RL
authors.lastname: Nicholson
mesh_terms: D005583:Fourier Analysis; D006801:Humans; D008433:Mathematics; D008962:Models, Theoretical; D009010:Monte Carlo Method; D015899:Tomography, Emission-Computed, Single-Photon / Q000295:instrumentation* / Q000379:methods*