γ-Ray, Charged Particle, and Neutron Attenuation Characteristics of Cadmium-Containing 211 MAX Phase Carbides, M <sub>2</sub> CdC (M = Ti, Zr, and Hf)

This study examines the attenuation behavior of γ rays and both charged (proton, α, electron) and uncharged (neutron) particles in cadmium-containing Group 4 MAX phase carbides: Ti<sub>2</sub>CdC, Zr<sub>2</sub>CdC, and Hf<sub>2</sub>CdC. Key parameters such as the linear attenuation coefficient (LAC), atomic cross section (ACS), electronic cross section (ECS), half-value layer (HVL), mean free path (MFP), effective atomic number (<i>Z</i> <sub>eff</sub>), and energy absorption buildup factor (EABF) were evaluated for γ-ray interactions. Among the studied materials, Hf<sub>2</sub>CdC, with a density of 12.67 g/cm<sup>3</sup>, exhibited superior γ-ray shielding performance, reflected in its high LAC and low HVL and MFP. Its effectiveness is comparable to that of conventional shielding materials such as lead (Pb). Notably, Hf<sub>2</sub>CdC demonstrated an HVL of 0.968 cm at 1173 keV, outperforming Pb (0.990 cm) at the same energy. This enhanced performance at γ energies dominated by Compton scattering is primarily attributed to its high density. For charged particles, Ti<sub>2</sub>CdC showed the highest mass stopping power for protons and α particles. However, due to its higher density, Hf<sub>2</sub>CdC resulted in the shortest penetration depths; for example, 10 MeV protons had a penetration range of only 1.77 μm in Hf<sub>2</sub>CdC. Additionally, Hf<sub>2</sub>CdC exhibited a high fast neutron removal cross section (FNRCS) of 0.163 cm<sup>-1</sup>, significantly outperforming common neutron shielding materials such as B<sub>4</sub>C, graphite, and concrete. Furthermore, all three compounds demonstrated excellent thermal neutron absorption due to the presence of cadmium (Cd), with Hf<sub>2</sub>CdC achieving the highest thermal neutron LAC of 43.38 cm<sup>-1</sup>. These results identify Hf<sub>2</sub>CdC as a strong candidate for integrated, multipurpose radiation shielding applications.

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Publication Details

Journal
ACS Omega
Published
2025-10-20
DOI
https://doi.org/10.1021/acsomega.5c04825
Primary Topic
Radiation Shielding Materials Analysis
Type
article
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article

γ-Ray, Charged Particle, and Neutron Attenuation Characteristics of Cadmium-Containing 211 MAX Phase Carbides, M 2 CdC (M = Ti, Zr, and Hf)

Celal Avcıoğlu
ACS Omega
Radiation Shielding Materials Analysis
article

γ-Ray, Charged Particle, and Neutron Attenuation Characteristics of Cadmium-Containing 211 MAX Phase Carbides, M 2 CdC (M = Ti, Zr, and Hf)

Celal Avcıoğlu
article en

Abstract

This study examines the attenuation behavior of γ rays and both charged (proton, α, electron) and uncharged (neutron) particles in cadmium-containing Group 4 MAX phase carbides: Ti<sub>2</sub>CdC, Zr<sub>2</sub>CdC, and Hf<sub>2</sub>CdC. Key parameters such as the linear attenuation coefficient (LAC), atomic cross section (ACS), electronic cross section (ECS), half-value layer (HVL), mean free path (MFP), effective atomic number (<i>Z</i> <sub>eff</sub>), and energy absorption buildup factor (EABF) were evaluated for γ-ray interactions. Among the studied materials, Hf<sub>2</sub>CdC, with a density of 12.67 g/cm<sup>3</sup>, exhibited superior γ-ray shielding performance, reflected in its high LAC and low HVL and MFP. Its effectiveness is comparable to that of conventional shielding materials such as lead (Pb). Notably, Hf<sub>2</sub>CdC demonstrated an HVL of 0.968 cm at 1173 keV, outperforming Pb (0.990 cm) at the same energy. This enhanced performance at γ energies dominated by Compton scattering is primarily attributed to its high density. For charged particles, Ti<sub>2</sub>CdC showed the highest mass stopping power for protons and α particles. However, due to its higher density, Hf<sub>2</sub>CdC resulted in the shortest penetration depths; for example, 10 MeV protons had a penetration range of only 1.77 μm in Hf<sub>2</sub>CdC. Additionally, Hf<sub>2</sub>CdC exhibited a high fast neutron removal cross section (FNRCS) of 0.163 cm<sup>-1</sup>, significantly outperforming common neutron shielding materials such as B<sub>4</sub>C, graphite, and concrete. Furthermore, all three compounds demonstrated excellent thermal neutron absorption due to the presence of cadmium (Cd), with Hf<sub>2</sub>CdC achieving the highest thermal neutron LAC of 43.38 cm<sup>-1</sup>. These results identify Hf<sub>2</sub>CdC as a strong candidate for integrated, multipurpose radiation shielding applications.

ACS OmegaVol. 10(43)
Usak University (TR), Wuxi Institute of Arts & Technology (CN)
Openalex Percentile: Top 76%
Radiation Shielding Materials Analysis
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