ABSTRACT
Experiments have assessed various polymer composites for radiation shielding in diverse applications. These composites are lighter and non-toxic when compared to lead (Pb), making them particularly effective in diagnostic imaging for shielding against low-energy photons. This study demonstrates the fabrication of four composites by combining a base material, specifically a high-density polyethylene (HDPE) polymer, with 10% and 20% silicon (Si) and silicon carbide (SiC), respectively. Additionally, 5% molybdenum (Mo) was incorporated into the composites as a heavy metal element. The composites obtained were fabricated into 20 disks with a uniform thickness of 2 mm each. Discs were exposed to radiation from a low-energy X-ray source (32.5-64.5 keV). The chemical and physical properties of composites were assessed. The shielding ability of samples was evaluated by determining the linear and mass attenuation coefficients (µ and µm), radiation protection efficiency (RPE), half-value layer (HVL), and mean free path (MFP). According to our findings, supplementing HDPE with additives improved the attenuation of beams. The µm values showed that composite X-ray shielding characteristics were enhanced with filler concentration for both Si and SiC. Polymer composites with micro-molecule fillers shelter X-rays better than polymers, especially at low energy. The HVL and MFB values of the filler are lower than those of the pure HDPE sample, indicating that less thickness is needed to shield at the appropriate energy. HC-20 blocked 92% of the incident beam at 32.5 keV. This study found that increasing the composite sample thickness or polymer filler percentage could shield against low-energy radiation.
ABSTRACT
Blue emitting nitrogen-doped carbon dots were synthesized using citric acid and urea through the hydrothermal method, and the fluorescence quantum yield was 35.08%. We discovered that N-CDs featured excellent robust fluorescence stability and chemical resistance. For metronidazole detection, our N-CDs exhibited quick response time, high selectivity and sensitivity, and low cytotoxicity. Specifically, our N-CDs could detect metronidazole in the linear range of 0-179 µM, and the LOD was 0.25 µM. Furthermore, metronidazole efficaciously quenches the fluorescence of N-CDs, possibly owing to the inner filter effect. Lastly, we have employed our N-CDs to detect metronidazole in commercial metronidazole tablets with high accuracy. Overall, the newly prepared fluorescence sensor, N-CDs, demonstrated a huge potential to detect metronidazole in a simple, efficient, sensitive, and rapid manner.
ABSTRACT
PURPOSE: Interest in PET imaging using zirconium-89 (Zr) (t1/2=78.41 h)-labeled tracers for the tracking and quantification of monoclonal antibodies (mAbs) is growing, mainly because of its well-matched physical half-life with the biological half-life of intact mAbs. This study aims to evaluate the imaging characteristics of Zr-PET in comparison with those obtained using fluorine-18 fluorodeoxyglucose (F-FDG) PET (gold standard tracer in PET imaging) using a Time-Of-Flight (TOF) PET/computed tomography (CT) scanner. MATERIALS AND METHODS: The system's spatial resolution, sensitivity, scatter fraction (SF), image uniformity, and image quality were measured on a Gemini TOF PET/CT scanner according to the NEMA NU2-2001 protocols. The NEMA 2001 kit was used to carry out these measurements. Timing and energy resolutions were measured using Na and F-FDG point sources only. RESULTS: Spatial resolution in transverse and axial planes measured at 10 mm off access were 4.7 and 4.6 mm for Zr and F-FDG, respectively. At 100 mm, radial, tangential, and axial spatial resolution values were 5.2, 5.1, and 5.2 mm for Zr and 5.1, 4.9, and 5.2 mm for F-FDG, respectively. Sensitivity measured at the center of the field of view was 14.6 and 4.16 cps/kBq for Zr and F-FDG, respectively. SF was 32.6% for Zr in comparison with 31.8% for F-FDG. Image contrast for Zr-PET images was 36.9 and 29.7% for F-FDG for the smallest (10 mm)-sized sphere, and it was 70.6 and 72.8% for Zr and F-FDG, respectively, for the largest (37 mm)-sized sphere. Background variation was 10.3% for Zr and 6.8% for F-FDG for the smallest-sized sphere and 3.4 and 3.8% for Zr and F-FDG, respectively, for the largest-sized sphere. CONCLUSION: In this study, we measured imaging characteristics of Zr on a Gemini TOF PET/CT scanner. Our results show that Zr has lower spatial resolution and noise-equivalent count rate with increased SF and background variation; however, it offered superior sensitivity and improved image contrast in comparison with F-FDG. Zr is an ideal radiotracer for immuno-PET imaging because of its physical half-life, which is well matched with mAbs, in addition to its affinity to be trapped inside the target cell after internalization of the mAbs.
