WinXCom—a program for calculating X-ray attenuation coefficients

Department of Physics, Technical University of Denmark, Building 307, DK-2800 Kongens Lyngby, Denmark
Radiation Physics and Chemistry (Impact Factor: 1.38). 01/2004; 71(3):653-654. DOI: 10.1016/j.radphyschem.2004.04.040
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    ABSTRACT: The mass attenuation coefficients, µ/ρ and effective atomic numbers, Zeff of some carbon steel and stainless steel alloys have been calculated by using Geant4, MCNP simulation codes for different gamma ray energies, 279.1 keV, 661.6 keV, 662 keV, 1115.5 keV, 1173 keV and 1332 keV. The simulation results of Zeff using Geant4 and MCNP codes have been compared with possible available experimental results and theoretical WinXcom, and good agreement has been observed. The simulated µ/ρ and Zeff values using Geant4 and MCNP code signifies that both the simulation process can be followed to determine the gamma ray interaction properties of the alloys for energies wherever analogous experimental results may not be available. This kind of studies can be used for various applications such as for radiation dosimetry, medical and radiation shielding.
    Radiation Physics and Chemistry 01/2015; 106:255-260. · 1.38 Impact Factor
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    ABSTRACT: Gamma ray shielding effectiveness of superconductors with a high mass density has been investigated. We calculated the mass attenuation coefficients, the mean free path (mfp) and the exposure buildup factor (EBF). The gamma ray EBF was computed using the Geometric Progression (G-P) fitting method at energies 0.015–15 MeV, and for penetration depths up to 40 mfp. The fast-neutron shielding effectiveness has been characterized by the effective neutron removal cross-section of the superconductors. It is shown that CaPtSi3, CaIrSi3, and Bi2Sr2Ca1Cu2O8.2 are superior shielding materials for gamma rays and Tl0.6Rb0.4Fe1.67Se2 for fast neutrons. The present work should be useful in various applications of superconductors in fusion engineering and design.
    Radiation Physics and Chemistry 07/2015; 106:175-183. · 1.38 Impact Factor
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