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Peer-reviewedCC BY-NC-NDJournal of Isotopes

Simulation of Shielding Performance of Ta-10W Alloy and Lead in CT Lateral Scattered Radiation Fields

  1. 1China Southwest Architectural Design and Research Institute Corp. Ltd. General Contracting Engineering Co., Ltd., Chengdu 610000, China

Abstract

Shielding performances of Ta-10W alloy and Pb in CT lateral-scattered radiation fields were compared using NIST XCOM data and MCNP6 models of a tungsten-target source,a PMMA phantom,and flat shielding plates. The air-kerma ratio \begin{document}$B_k was used to characterize transmission. As the tube voltage increased from 80 to 140 kVp,the mean energy of the 90° scattered spectrum increased from 47.01 to 57.95 keV,and the air−kerma contribution from 67.4–88.0 keV increased from 2.40% to 19.14%. For the sameB_k $\end{document} as 2.5 mm Pb,the equivalent Ta-10W thicknesses were 2.01,1.50,1.37,and 1.33 mm at 80,100,120,and 140 kVp,respectively,corresponding to thickness reductions of 19.56%–46.98%. At 100–140 kVp,the areal density was reduced by 10.67%–21.08%. The mass attenuation coefficient of Ta-10W at 80 keV was about 3.15 times that of Pb. The advantage is attributed to enhanced attenuation above the Ta/W K edges and below the Pb K edge,providing a numerical reference for thin local shielding in CT rooms.

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BibTeX
@article{teng2026simulation,
  title = {{Simulation of Shielding Performance of Ta-10W Alloy and Lead in CT Lateral Scattered Radiation Fields}},
  author = {Na TENG},
  journal = {Journal of Isotopes},
  year = {2026},
  month = oct,
  doi = {10.7538/tws.2026.youxian.059},
  url = {https://doi.org/10.7538/tws.2026.youxian.059},
  note = {CC BY-NC-ND},
}
RIS
TY  - JOUR
TI  - Simulation of Shielding Performance of Ta-10W Alloy and Lead in CT Lateral Scattered Radiation Fields
AU  - Na TENG
PY  - 2026
DA  - 2026/10/26
JO  - Journal of Isotopes
DO  - 10.7538/tws.2026.youxian.059
UR  - https://doi.org/10.7538/tws.2026.youxian.059
AB  - Shielding performances of Ta-10W alloy and Pb in CT lateral-scattered radiation fields were compared using NIST XCOM data and MCNP6 models of a tungsten-target source,a PMMA phantom,and flat shielding plates. The air-kerma ratio \begin{document}$B_k was used to characterize transmission. As the tube voltage increased from 80 to 140 kVp,the mean energy of the 90° scattered spectrum increased from 47.01 to 57.95 keV,and the air−kerma contribution from 67.4–88.0 keV increased from 2.40% to 19.14%. For the sameB_k $\end{document} as 2.5 mm Pb,the equivalent Ta-10W thicknesses were 2.01,1.50,1.37,and 1.33 mm at 80,100,120,and 140 kVp,respectively,corresponding to thickness reductions of 19.56%–46.98%. At 100–140 kVp,the areal density was reduced by 10.67%–21.08%. The mass attenuation coefficient of Ta-10W at 80 keV was about 3.15 times that of Pb. The advantage is attributed to enhanced attenuation above the Ta/W K edges and below the Pb K edge,providing a numerical reference for thin local shielding in CT rooms.
SN  - 1000-7512
ER  -