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The coded-aperture gamma camera has significant applications in the fields of space exploration, nuclear security, nuclear industry, and nuclear medicine. The coded-aperture collimator is a key component for modulating gamma rays, and its parameters are important factors to optimize the performance of gamma cameras. In this paper, the impact of collimator thickness on the fully coded field of view and angular resolution was determined through Monte Carlo simulation and experimental verification. By introducing the equivalent thickness, the conventional calculation formulas were modified to improve the calculation accuracy. In addition, the variation in the reconstructed image quality with the collimator thickness was quantitatively evaluated by the contrast-to-noise ratio and normalized mean squared error, thereby establishing the relationship between the gamma-ray transmittance and the imaging quality. The results indicate that for medium- and high-energy gamma rays, the optimal imaging quality is achieved when the gamma-ray transmittance corresponding to collimator thicknesses ranges from 12% to 16%. These research findings provide reference standards for the design of coded-aperture collimators to meet the requirements of different applications.
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http://dx.doi.org/10.1063/5.0239695 | DOI Listing |
Biomed Phys Eng Express
August 2025
Radiological Physics & Advisory Division, Bhabha Atomic Research Centre, Mumbai-400094, Maharashtra, India.
Single photon emission computed tomography (SPECT) is a vital imaging tool for visualizing functional and physiological processes of human body. Periodic quality assurance (QA) ensures imaging accuracy, but high-cost commercial phantoms limit accessibility in resource-constrained settings. To address this, a cost-effective and modular SPECT phantom was developed to evaluate imaging parameters in a single scan.
View Article and Find Full Text PDFWe present a dual focus wavefront tilting metalens, a lens of a few micrometers thick that compensates for incidence angles of ±5° and focuses them to the same target. The metalens comprises an array of SiN nanopillars. We manufactured the metalens using 193 nm deep-ultraviolet scanner lithography, suitable for high-volume manufacturing.
View Article and Find Full Text PDFThis study examines the local transmission of normal and pathological corneal tissues when exposed to coherent collimated near-infrared (NIR) radiation with a wavelength of 1061 nm, highlighting its potential advantages over ultraviolet (UV) radiation for antimicrobial photodynamic therapy (PDT). The proposed measurement method, which employs an original experimental setup with a collimated NIR laser source and a probe fiber for direct layer-by-layer depth profiling, allows for determining the transmission values at specific depths within the cornea. Considering that the affected areas are localized within 1/3 to 1/2 of the corneal thickness, the residual power of the NIR radiation in the posterior part of the affected zone (at a depth of 250-400 µm) does not exceed 20%.
View Article and Find Full Text PDFPhys Med Biol
August 2025
Institute of Biomedical Engineering, Shenzhen Bay Laboratory, Shenzhen, People's Republic of China.
Positron Emission Tomography (PET) benefits from depth-of-interaction (DOI) information to correct parallax errors introduced by thick scintillator crystals, especially in dedicated brain systems where edge-of-field DOI effects are most pronounced. Conventional light-sharing window (LSW) readout is limited to a four-to-one or two-to-one crystal-to-photodetector coupling and cannot decode DOI for central crystals under nine-to-one coupling schemes. This work proposes a novel detector architecture that overcomes these limitations, enabling DOI decoding for all crystals.
View Article and Find Full Text PDFMed Phys
July 2025
Centre for Medical Radiation Physics, University of Wollongong, Wollongong, New South Wales, Australia.
Background: A unique feature of inline MRI-linac prototype systems is the changes to entry surface or skin doses. For the high field (1 T) Australian MRI-linac prototype, a strong surface dose increase is observed. This is a by-product of secondary electron contamination being focused down the MRI bore due to the magnetic field being parallel with the x-ray beam direction.
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