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SU‐G‐IeP3‐10: Molecular Imaging with Clinical X‐Ray Sources and Compton Cameras
Author(s) -
Vernekohl D,
Ahmad M,
Chinn G,
Xing L
Publication year - 2016
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 - 10.1118/1.4957059
Subject(s) - imaging phantom , image resolution , physics , optics , monte carlo method , iterative reconstruction , medical imaging , detector , nuclear medicine , molecular imaging , materials science , medical physics , radiology , medicine , statistics , mathematics , microbiology and biotechnology , biology , in vivo
Purpose: The application of Compton cameras (CC) is a novel approach translating XFCT to a practical modality realized with clinical CT systems without the restriction of pencil beams. The dual modality design offers additional information without extra patient dose. The purpose of this work is to investigate the feasibility and efficacy of using CCs for volumetric x‐ray fluorescence (XF) imaging by Monte Carlo (MC) simulations and statistical image reconstruction. Methods: The feasibility of a CC for imaging x‐ray fluorescence emitted from targeted lesions is examined by MC simulations. 3 mm diameter water spheres with various gold concentrations and detector distances are placed inside the lung of an adult human phantom (MIRD) and are irradiated with both fan and cone‐beam geometries. A sandwich design CC composed of Silicon and CdTe is used to image the gold nanoparticle distribution. The detection system comprises four 16×26 cm 2 detector panels placed on the chest of a MIRD phantom. Constraints of energy‐, spatial‐resolution, clinical geometries and Doppler broadening are taken into account. Image reconstruction is performed with a list‐mode MLEM algorithm with cone‐projector on a GPU. Results: The comparison of reconstruction of cone‐ and fan‐beam excitation shows that the spatial resolution is improved by 23% for fan‐beams with significantly decreased processing time. Cone‐beam excitation increases scatter content disturbing quantification of lesions near the body surface. Spatial resolution and detectability limit in the center of the lung is 8.7 mm and 20 fM for 50 nm diameter gold nanoparticles at 20 mGy. Conclusion: The implementation of XFCT with a CC is a feasible method for molecular imaging with high atomic number probes. Given constrains of detector resolutions, Doppler broadening, and limited exposure dose, spatial resolutions comparable with PET and molecular sensitivities in the fM range are realizable with current detector technology.