Linear Attenuation Coefficient Values Research Articles

Simulation on Image Reconstruction of Concrete with Rebars by Filtered Back Projection Algorithm using PHITS and MATLAB Program

This paper describes simulation on image reconstruction of concrete with rebars by filtered back projection algorithm using PHITS and MATLAB program. In PHITS simulation, a source of Cs-137 and NaI (Tl) detector were used. Concrete block with one rebar was carried out with PHITS simulation. The sample of another concrete block with two rebars with different diameters was also conducted. Linear attenuation coefficient values of the concrete were calculated. These phantoms were rotated with 2.8125 degree intervals over 0 to 180° in PHITS simulation. The objects were scanned with the parallel beam method and the projection data were obtained. The data was built into the image using filtered back projection (FBP) algorithm. The ‘spline’ interpolation and ‘Hamming’ filter functions were chosen for the clearest image in image reconstruction. The results indicated that the reconstructed images of the concrete containing one rebar and two rebars can be observed clearly in MATLAB.

MATXCOM—an x-ray/gamma-ray attenuation calculator for arbitrary materials based on EPICS2023 evaluated photon data library

A program called MATXCOM was developed for the calculation of x-ray/gamma-ray interaction cross-sections, the mass attenuation coefficient (MAC), linear attenuation coefficient (LAC), half and tenth value layers (HVL and TVL), mean free path (MFP), total atomic and electronic cross-sections (ACS and ECS), effective atomic number (Zeff), effective electron density (Neff), effective conductivity (Ceff), and energy absorption and exposure buildup factors (EABF and EBF) for arbitrary materials based on the EPICS2023 evaluated photon data library (EPDL). MATXCOM was implemented as a stand-alone program written in Fortran featuring a streamlined input/output interface. This design allows it to be easily integrated into scripts or wrapper functions, making it adaptable for use in large computational projects.

Investigation of the radiation shielding efficiency of Bi2O3-doped borosilicate glasses

Abstract In the present work, new borosilicate glasses were prepared to examine their radiation shielding characteristics, focusing on the role of increased Bi2O3 concentration on different radiation shielding parameters as determined by the Phy-X software. At 0.296 MeV, the mass attenuation coefficient was found to be 0.105 cm2/g for the free-Bi2O3 glass, and it increased to 0.266 cm2/g for the sample with 15 mol% Bi2O3. The linear attenuation coefficient (LAC) was investigated in the 0.0395–1.460 MeV energy range. The LAC was very high at the low energy range and a large LAC value variation was found between the free-Bi2O3 glass sample and those containing Bi2O3, which confirmed that Bi2O3 had a significant impact on the prepared glasses’ radiation shielding properties. The glasses’ effective atomic number (Zeff) was also examined, with the results showing an almost constant Zeff for the free-Bi2O3 glass sample, while the introduction of Bi2O3 caused a notable increase. At 0.0395 MeV, the Zeff value of sample Bi0B70 (free-Bi2O3) was 8.20, while it increased to 55.09, 66.08, and 70.98 with the addition of 5, 10, and 15 mol% Bi2O3.

A detailed study on the physical, mechanical, structural and gamma ray shielding properties of Al2O3–Na2O–SiO2–B2O3–Bi2O3glass system

The density, boron–boron separation, and molar volume of 4Al2O3–12Na2O-(18-x)SiO2-(64-x) B2O3-(2+2x)Bi2O3 (where x = 2, 4, 6 and 8 mol%) are increasing with the addition of Bi2O3. The addition of Bi2O3 results in an open network structure. The elastic moduli decrease from 34.711 to 29.875 GPa for Young modulus (E); 20.395 to 15.843 GPa for bulk modulus (B); from 15.257 to 13.494 GPa for shear modulus (G) and 40.738 to 33.836 GPa for longitudinal (L) respectively with increased Bi2O3 concentration. FTIR spectrainvestigation found BO3, BO4, SiO4, and BiO6 structural units to be present. The glasses' highest mass attenuation coefficient (MAC) is at 0.0395 MeV, the lowest energy value. It gradually decreases as energy increases. There is a decrease in the linear attenuation coefficient (LAC) values with energy. Sample Bi18 has the highest MAC and LAC values due to its high concentration of Bi2O3. Across the entire energy range, sample Bi18 has the highest effective atomic number, and the lowest half value layer and mean free path values across all energy values. The transmission factor (TF) values for Bi6 indicate that the required thickness for blocking 90% of the radiation must be greater than the thickness necessaryfor the attenuation of 50%. Bi18 has the lowest TF compared to other glass samples. The radiation protection efficiency values for Bi18 are highest, confirming their full protection ability. Bi18's is the best choice for radiation shielding.

Fabrication and characterization of rubcrete-iron composite for mixed radiation shielding

Mixed radiation environments need unique shielding materials that can effectively attenuate photons and neutrons simultaneously. Most ordinary shielding materials can only shield one form of radiation effectively. In this work, a novel composite material was fabricated in our laboratories and characterized for photon and neutron shielding. Waste materials were used as partial substitutes for aggregates in concrete, which is a sustainable practice in the building industry at present. The main components of the composite material are iron filings, rubber, and concrete. Concrete samples were mixed with iron filings at varying percentages (0%, 10%, 20%, and 30%) and a fixed 5% crumb rubber content. The material’s photon and neutron shielding characteristics were evaluated through experimental and simulation methods. Gamma-ray attenuation measurements were experimentally carried out using a NaI(TI) spectrometer and a Cs-137 0.662 MeV energy source. In contrast, GEANT4, PHY-X/PSD, and NIST-XCOM codes were used to simulate photon and neutron cross-sections. The findings indicate that an increase in iron filings results in enhanced radiation attenuation, reflected by a higher linear attenuation coefficient (μ). The linear attenuation coefficient values range from (0.1590 ± 0.0004) to (0.2045 ± 0.0003) cm−1 for samples with no crumb rubber and from (0.1521 ± 0.0002) to (0.1920 ± 0.0004) cm−1 for samples with 5% crumb rubber. Half Value Layer (HVL) decreases with an increase in iron content and is slightly higher in samples with crumb rubber. The HVL results from simulations and measurements agree. This study optimizes the potential of concrete as a radiation-shielding material while promoting sustainable construction and environmental practices.

Exploring the diverse modifiers influence on the structural, physical, and mechanical properties of a zinc oxide-based boro-tellurite glass system for enhancing radiation shielding performance

This work is meant to fabricate zinc boro-tellurite (ZnO–TeO2–B2O3) glass systems with various modifiers, including MoO3, Bi2O3, and PbO, using the melt quench technique. Four glass samples were produced, each comprising 20 % of a specific modifier from the total weight percent of the neat glass system. Each glass sample is given a code: TBZn, TBZMo, TBZBi, and TBZPb. The XRD results showed an amorphous nature for all glass samples. The FTIR results showed the functional groups for borate and tellurite oxide. The mechanical properties were reduced when different oxides were added instead of ZnO. For example, Young's modulus decreased for glass samples; their recorded values for Young's modulus are 74.516, 72.569, 60.526, and 59.272 GPa for TBZn, TBZMo, TBZBi, and TBZPb, respectively. On the other hand, adding Bi2O3 and PbO led to enhanced shielding properties. For instance, the linear attenuation coefficient values for TBZn, TBZMo, TBZBi, and TBZPb at 0.015 MeV are 168.739, 115.656, 380.711, and 279.162, respectively. Also, the radiation protection efficiency (RPE) at 5 cm and 600 keV is 83.220 %, 79.299 %, 93.919 %, and 90.222 % for TBZn, TBZMo, TBZBi, and TBZPb, respectively. While adding different oxides decreased stability in the current glasses, it also enhanced their shielding properties, recommending their use in the radiation shielding field.

Investigating radiation shielding parameters for X-ray attenuation at various energies in locally produced ceramic materials used in Saudi Arabia

To assess shielding effectiveness against X-rays, a number of locally collected ceramic samples were obtained from the Kingdom of Saudi Arabia. Based on elemental analysis, all of the ceramic samples have a density in the range of 1.68–1.85 g/cm3, with the highest proportions of O, Si, C, and Al atoms and the lowest amounts of Na, Mg, K, Ca, Ti, and Fe. The 320 kV X-ray source (Gulmay Limited, Byfleet, UK) was used to assess the attenuation properties of the ceramic samples. An Exradin A4 ionization chamber (Standard Imaging, Middleton, USA) connected to a UNIDOS electrometer (PTW, Freiburg, Germany) in the control room was used to detect the attenuation properties. Several X-ray attenuation coefficients are evaluated at different X-ray energies in the range of 40–150 kV in this study. These include the mass attenuation coefficient (MAC), linear attenuation coefficient (LAC), half-value layer (HVL), tenth-value layer (TVL), and mean free path (MFP). The ability of any ceramic sample under investigation to shield radiation at low X-ray energy is indicated by the theoretical and experimental values of LAC. The potential applications of these easily accessible, reasonably priced ceramic materials for radiation protection in X-ray labs and low-energy X-ray shielding in a variety of fields have been shown by this investigation.

Investigation of thermal, acoustic, mechanical, and radiation shielding performance of waste and natural fibers

It is crucial to address two pressing global issues, energy shortage and environmental pollution, when producing building insulation materials. Using waste and natural fiber groups can be part of the solution. The insulation material was produced using pumpkin fiber, chicken fiber, cotton waste, vermiculite, and epoxy as binders. The samples were tested for thermal conductivity coefficient, ultrasonic sound transmission rate, density, water absorption rate, compressive and bending strength, and fire resistance at temperatures of 75, 100, 125, and 150C. The samples produced using natural and waste materials yielded a thermal conductivity value of 0.041 W/mK, an ultrasonic sound transmission speed of 0.25 km/s, a compressive strength value of 1.57 MPa, and bending strength values of 0.91 MPa. It has been clearly demonstrated that, with its low volume loss, it can serve as an alternative to the EPS-XPS types available in the market. Furthermore, the linear attenuation coefficients (LAC) were examined to obtain radiation shielding properties of the samples at 1173 and 133 keV energies using a 60Co gamma source. Also, LAC values determined between 0,1167 ± 0,0452 cm−1-0,2315 ± 0,0065 cm−1 for 1173 keV and 0,1042 ± 0,0488 cm−1 - 0,2141 ± 0,0062 cm−1 for 1333 keV. Accordingly, it has been revealed that waste compositions are effective in protecting against radiation.

The impact of CuO in modifying the radiation shielding performance of PbO–BaO–CaO–B2O3–CuO: An experimental approach

The current work aims to develop a new lead calcium barium borate glasses doped with CuO (10PbO–20BaO–10CaO-(60-x)B2O3-xCuO, (x = 0, 5, 10, and 15 mol%)) and to experimentally report the radiation shielding properties of the developed glasses. The linear attenuation coefficient (LAC) was determined in two methods and we compared the results of both methods to check the accuracy in the experimental method. The effect of CuO on the LAC was examined and the results showed a positive relation between the amount of CuO and the LAC values and this is clearly seen at low energy range. The half and tenth thickness layers (HTL and TTL) were determined and the results showed that the HTL values equal to 0.051, 0.049, 0.047 and 0.045 cm at 60 keV, while they were 0.170, 0.163, 0.156 and 0.149 cm for TTL for the glasses with 0, 5, 10 and 15 mol% CuO respectively. The transmission efficiency (TF) results demonstrated that the addition of CuO to the glasses causes a reduction in the number of photons that can penetrate the glasses. The shielding efficiency parameter also confirms that the addition of CuO causes an enhancement in the radiation shielding properties for the prepared glasses.

Indirect effect of elevated pressure via the modulations of crystals intrinsic parameters on radiation shielding efficacy: A comparative study between two α-quartz homeotypes SiO2and GeO2

This study investigates the indirect effects of elevated pressure on the radiation shielding competence of two α-quartz homeotypes, SiO2 and GeO2, by examining the modulations of their crystal intrinsic tetrahedral parameters. The study focuses on structural modifications and their correlations with radiation attenuation properties. The results show that both homeotypes exhibit energy-dependent mass attenuation coefficients (MAC) and linear attenuation coefficients (LAC). SiO2 demonstrates higher transparency to incident radiation compared to GeO2, with a relative difference in MAC values of 91% at 0.015 MeV, decreasing to 28% at 15 MeV. However, within the energy range of 0.4 < E < 4 MeV, SiO2 exhibits higher MAC values than GeO2, with the MAC of SiO2 surpassing GeO2 by 17% at 0.4 MeV. The pressure dependence of LAC values indicates that both SiO2 and GeO2 become more effective in attenuating radiation under higher pressure conditions. For instance, at 0.015 MeV, the LAC of GeO2 increased from 274.826 cm−1 at 0.001 GPa to 308.073 cm−1 at 5.57 GPa. GeO2 generally exhibits higher LAC values than SiO2 across the energy and pressure ranges studied. It can be concluded that the structural modifications induced by elevated pressure significantly enhance the radiation shielding capabilities of α-quartz homeotypes, particularly GeO2, making them promising candidates for advanced shielding materials in various high-radiation environments.

Investigation of the gamma ray shielding properties of Epoxy based on Bi2O3/GO nanocomposite

Abstract One of the important carbon materials, graphene oxide (GO), has several oxygen-containing functional groups. Due to its unique structure, it has attracted increasing interest in multidisciplinary studies of physical and chemical attributes. In this work, Bismuth Oxide nanoparticles (Bi2O3) is prepared and functionalized with graphene oxide nanosheets (Bi2O3-GO). The Bi2O3 and Bi2O3-GO nanocomposite were mixed with epoxy by changing the percentages to 1%, 2.5%, 5%, and 10%. The study used a hyper-pure germanium detector to investigate the attenuation characteristics of the prepared samples. Ba133, Cs137, and Co60 point sources were used at photon energies of 81, 276, 302, 356, and 383 keV for Ba133, 661 keV for Cs137, and 1173 and 1332 keV for Co60. The linear attenuation coefficient, mass attenuation coefficient, half-value layer, and tenth-value layer were estimated to investigate the radiation shielding characteristics of the prepared samples. The linear attenuation coefficient (μ) values varied from 0.45 to 0.88, 0.23 to 0.89, and 0.31 to 0.77 for Ba133, Cs137, and Co60, respectively. The mass attenuation coefficient (μm) values varied from 0.18 to 0.50, 0.19 to 0.50, and 0.15 to 0.50 for Ba133, Cs137, and Co60, respectively. Half-value layer (HVL) values varied from 0.79 to 1.55, 0.78 to 3.07, and 0.9 to 2.26 for Ba133, Cs137, and Co60, respectively. Tenth-value layer (TVL) values varied from 2.61 to 5.16, 2.58 to 10.19, and 2.98 to 7.51 for Ba133, Cs137, and Co60, respectively.

Scaling up features of photocatalytic degradation and radiation shielding of multicomponent Cr–Co–Zn nanoferrites

Optical, photocatalytic activity, and radiation shielding studies were conducted on CrxCo0.8Zn0.2Fe2-xO4 (0.0 ≤ x ≤ 0.1, Δx = 0.02) nanoferrites for water treatment and radiation shielding applications. The optical absorption analysis revealed that the optical band gap energy values range from 1.864 to 1.803 eV as assessed through Tauc plots. Further analysis of photocatalytic degradation showed that the Cr0.06Co0.8Zn0.2Fe1.94O4 sample exhibited superior methylene blue (MB) dye removal compared to other samples, with an efficiency of 96.74% in 60 min. Additionally, the present nanoferrites exhibited excellent stability in photocatalytic degradation over multiple cycles. The study also investigated the linear attenuation coefficient (LAC) of the current ferrite nanoparticles, demonstrating increased LAC values with higher Cr content, while the half value layer (HVL) diminished with further Cr concentration. The HVL values indicated the potential efficacy of our nanoferrites as radiation shields when compared to standard radiation shielding materials. Overall, this research suggests a new direction for optimizing spinel nanomaterials for applications in water treatment and radiation shielding.

Radiation shielding potential of cellulose acetate-CdO-ZnO polymer composites in comparison with concrete and gypsum

Radiation shielding using polymer composites is becoming more attractive because of their ease of production, lightness, ruggedness and availability. In this work, linear attenuation coefficient (LAC) and tenth value layer (TVL) of Cellulose Acetate - CdO - ZnO Polymer Composites of different concentrations of CdO and ZnO denoted as PB1, PB2 and PB3 were investigated against concrete and gypsum. Cellulose Acetate-CdO-ZnO Polymer Composites were prepared using the open mold cast technique and have been investigated for x-rays shielding ability. Cellulose acetate is a biodegradable good matrix, while CdO and ZnO are good fillers for absorbing x-rays in the diagnostic energy range. Scanning Electron Microscopy (SEM) technique was used to observe the uniform dispersal of fillers within the matrix. X-rays attenuation coefficients were calculated by XCOM computer code for all the samples using the average energies commonly used in diagnostic radiology practice - 20 keV, 30 keV, 40 keV and 60 keV. The SEM confirmed the dispersal of the fillers (CdO and ZnO) within the matrix. The result of this investigation showed that all the polymer composites (PB1, PB2 and PB3) have higher LACs and lower TVLs over gypsum and concrete at 20 keV, 30 keV, 40 keV and 60 keV. Tenth Value Layers (TVLs) of all the polymer composites is less than 1 cm at 20 keV, 30 keV and 40 keV.

Effect of gold nanoparticle dispersion on the structural, optical and radiation shielding parameters of sodium borate glass

Borate-derived radiation shielding glasses have been thoroughly explored, yet the effects of gold nanoparticle (GNP) dispersion on sodium borate glasses remain unstudied. This study investigates the impact of GNP dispersion and varying GNP concentrations on the radiation shielding properties and other parameters of sodium borate glass. All the glasses were prepared using the melt-quench technique with a composition of 30Na2O-70B2O3, containing 0, 2 × 10−10, and 2 × 10−9 mol% of nanoparticles. The x-ray diffractogram (XRD) confirmed the amorphous nature of the prepared glass samples, while Fourier Transform Infrared Spectroscopy (FTIR) confirmed structural modifications, indicated by the formation of non-bridging oxygens due to the incorporation of GNPs. High-resolution transmission electron microscopy (HR-TEM) confirmed the presence of GNPs with an average size of 1.317 nm, and Field Emission Scanning Electron Microscopy (FESEM) revealed further coagulation of GNPs into tiny grains to alleviate surface stresses. Density measurements showed a clear decrease from 2.3051 to 2.1363 g cm−3 with the incorporation of gold nanoparticles. Additionally, a localized surface plasmon resonance peak centered at 612 nm was observed in the UV–Vis spectrogram of the glass with the highest GNP concentration. Radiation shielding parameters, including the mass attenuation coefficient (MAC), linear attenuation coefficient (LAC), half-value layer (HVL), tenth-value layer (TVL), mean free path (MFP), and effective atomic number (Zeff), were analyzed using Phy-X/PSD software. The LAC value initially decreases from 76.073 to 70.502 cm−1 with the incorporation of GNPs but increases to 75.878 cm−1 with a higher GNP concentration. This glass system exhibited superior radiation shielding parameters compared to various reported glass systems, indicating its potential for shielding applications.

Microstructure, thermal and radiation shielding properties of aluminium‐silicon‐boron alloy prepared by mechanical alloying

AbstractThis study focused on developing microstructural, thermal, and radiation shielding changes in Al50Si25B25 powders using mechanical alloying techniques. Based on the x‐ray powder diffraction data, the crystallite size and microstrain of the 100‐hours milled powder were calculated as 0.25 nm and 50.33 %, respectively. The solubility of silicon in the α‐aluminium matrix increased with longer mechanical alloying duration. Transmission electron microscope analyses further showed that the alloy particulates had an average size of 3 μm and an average grain size of 0.226 nm. The radiation shielding properties of the Al50Si25B25 powders indicated that the Linear Attenuation Coefficient value increased from 0.0554±0.1689 cm−1 to 1.0632±0.2425 cm−1 with an increase in the thickness of the Al50Si25B25 alloy. This work successfully demonstrated the potential of mechanical alloying techniques to enhance the microstructural and thermal properties of Al50Si25B25 powders. It highlighted their effectiveness in providing radiation shielding capabilities when varying the thickness of the alloy.

Evaluation of Some Heavyweight Minerals as Sustainable Neutron and Gamma-Ray Attenuating Materials: Comprehensive Theoretical and Simulation Investigations

AbstractThis study comprehensively evaluates the radiation attenuation efficiencies of hematite and barite, commonly used materials in radiation shielding, using theoretical and simulation investigations. The MCNP-5 code was used to obtain the linear attenuation coefficient (LAC) within the energy range of 0.015–15 MeV, with validation by the XCOM program. Based on these LAC values, various gamma-ray shielding parameters were determined: mass attenuation coefficient, half-value layer, radiation protection capacity, mean free path, transmission factor, and equivalent thickness to lead (ETPb). Additionally, effective atomic number (Zeff) and electron density (Neff) were calculated, including both single-energy and energy-dependent forms for photon absorption and interaction. Furthermore, MCNP-5 simulations and NGCal program calculations were used to assess thermal neutron attenuation, while the NXcom program determined fast neutron behavior. This analysis revealed superior γ-ray shielding for barite compared to hematite. Similarly, the NXcom program indicated better fast neutron shielding for barite. However, interestingly, simulations validated a 210% higher effectiveness in thermal neutron attenuation for hematite. Finally, comparing the studied materials with other shielding materials demonstrated promising potential as environmentally friendly alternatives for effective shielding against various radiation types.

Improved mechanical, magnetic and radiation shielding performance of rubbery polymer magnetic nanocomposites through incorporation of Fe3O4 nanoparticles

The current research investigates the impact of magnetite (Fe3O4) nanoparticles (3–12 wt%) on the properties of rubbery polymer nanocomposites fabricated via melt blending method. The tensile and impact properties were improved at an optimal 6 wt% Fe3O4, revealing a good interfacial interaction. Fe3O4 enhanced the thermal stability, as evidenced by the increased integral procedure decomposition temperature up to 26 %. Fe3O4 increased residual and saturated magnetization the most at 6 wt% loading. The gamma-ray shielding properties were explored with energy ranging from 0.2835 to 2.506 MeV, and effectively at low energies. Increased Fe3O4 content correlated positively with linear attenuation coefficient (LAC), enhancing radiation shielding but reducing neutron shielding. At 0.2835 MeV, the LAC values increased up to 0.12431 cm−1 for 12 wt% Fe3O4, while the fast neutron removal cross-section values decreased from 0.10427 cm−1 to 0.08548 cm−1. These findings highlight the multifunctional potential of Fe3O4-incorporated nanocomposites in radiation shielding applications.

Cr-substituted Mn–Zn ferrite nanoparticles: A study of optical, photocatalytic degradation, and radiation shielding evolution

In this work, we investigate the impact of chromium (Cr) additives on the optical, photocatalytic degradation and the radiation attenuation features of chromium-manganese (Mn)-zinc (Zn)-based spinel nanoferrite (named MZCF-nanoferrites. The Kubelka-Munk approach of reflectance results and Tauc's plots were exploited to verify the energy gap (Eg) of the MZCFx ferrite nanoparticles. The nanoferrites MZCF0, MZCF1, MZCF2, MZCF3, MZCF4, and MZCF5 have Eg values 1.826, 1.811, 1.797, 1.784, 1.772, and 1.769 eV, respectively. The comparative study of the photocatalytic degradation for the optimal (Mn0.8Zn0.2Cr0.1Fe1.9O4) nanoferrite sample and many reported photocatalytic materials evidenced that the MZCF5 nanoferrite has methylene blue dye removal ability higher than those materials (96.38 %, in 60 min). Moreover, this comparative study showed the improved photocatalytic degradation stability performance of the present nanoferrites (just 1.65 % efficiency was decreased after five cycles). The present study proposes a novel approach toward spinel nanoferrites, focusing on the optical and photocatalytic characteristics of the MZCFx-nanoferrites that can be applicable in water treatment fields. Examining linear attenuation coefficient (LAC) of MZCFx-nanoferrite at 0.662 MeV, we observe increased LAC values 0.286 cm−1 to 0.344 cm−1 with increasing Cr additions. Conversely, the half value layer (HVL) values at 0.662 MeV decreased 2.421 cm–2.017 cm with increasing Cr additions. By comparing the HVL values of the MZCFx-nanoferrites at 0.662 MeV to some selected radiation shielding materials, the HVL of the MZCFx-nanoferrites showed smaller values. These findings offer promising perspectives for optimization of spinel nano materials for use in radiation shielding applications.

Low-dose energy-resolved X-ray computed tomography using a filter-changing two-dimensional transXend detector

ABSTRACT A novel detector system ‘transXend’ detector, which measured X-rays as electric current and output the energy distribution of X-rays after analysis, has been developed by the authors. With computed tomography (CT) by using the transXend detector, CT image was given in the absolute value of linear attenuation coefficient as a function of X-ray energy and the effective atomic number distribution in a subject was obtained. For the X-ray CT of a large object such as a human body, the development of a two-dimensional transXend detector is necessary and the authors proposed a filter-changing transXend detector previously. The exposure dose to the subject, however, increased due to the multiple inspections with various X-ray spectra tailored by each filter. To reduce the exposure dose, a method is proposed to synchronize filter changes with changes of the inspection angle of the subject. With this method, the exposure dose can be reduced nearly 50% compared to a conventional electric current measurement CT.

Exploration of optical, mechanical and radiation shielding properties in B2O3-BaO-Na2O-ZnO-CaO glasses: A compositional study

We investigated the optical, mechanical, and radiation shielding features of a novel B2O3-BaO-Na2O-ZnO-CaO glasses prepared using the melt-quench method. Using UV–Vis spectroscopy, the optical features were characterized. The results indicate that upon reducing the B2O3 content, the band gap decreases from 3.722 eV to 3.069 eV, and refractive indices increase from 2.225 to 2.378. On the other hand, mechanical properties were studied based on the Makishima–Mackenzie model. Young's modulus, for instance, decreased from 93.314 GPa (G1) to 78.896 GPa (G4). Radiation shielding properties were studied using the Phy-X software, and the results showed significant variations, with the linear attenuation coefficient (LAC) values at 0.015 MeV being 48.378 cm−1 for G1, cm−1 for G2, 75.282 cm−1 for G3, and 89.360 cm−1 for G4. The half-value layer (HVL) at 0.015 MeV ranged from 0.014 cm (G1) to 0.008 cm (G4). The results indicate that increasing BaO-Na2O-ZnO-CaO content improves the glass's radiation shielding ability but decreases its mechanical strength.