S.K. Samanta , Purbali Das , S. Sodaye , R. Acharya
{"title":"Applications of a mono-standard NAA method using upgraded Apsara research reactor for trace element determination in glass matrices","authors":"S.K. Samanta , Purbali Das , S. Sodaye , R. Acharya","doi":"10.1016/j.radphyschem.2025.113295","DOIUrl":"10.1016/j.radphyschem.2025.113295","url":null,"abstract":"<div><div>The <em>k</em><sub><em>0</em></sub>-based Internal Mono-standard Neutron Activation Analysis (IM-NAA) technique was optimized utilizing a core irradiation position at the Apsara-U research reactor of BARC, Mumbai, India. The cadmium ratio method was utilized to evaluate the epi-thermal neutron shape parameter, <em>α</em>, using both dual and multiple monitor methods and the <em>f</em>-value was derived from <sup>197</sup>Au. The IM-NAA and the conventional <em>k</em><sub><em>0</em></sub>-NAA methods were validated by analyzing SMELS-II (synthetic multi-element standards from IRMM), whereas United States Geological Survey Certified Reference Material (USGS CRM), Granite (G-2) and Rhyolite Glass Mountain (RGM-1) were analyzed to evaluate the accuracy of <em>k</em><sub><em>0</em></sub>-NAA and IM-NAA methods utilizing <sup>197</sup>Au and <sup>45</sup>Sc as mono standards. The determined concentrations were found to be in good agreement with certified or recommended values, and this is supported by calculated Z-scores in the range of ±(0.1–1), for many elements in SMELS-II, G-2 & RGM-1 at 95.5 % confidence level. The IMNAA method, utilizing Sc as the mono-standard was utilized to determine mostly trace elemental concentrations in two different soda-lime glass samples. The IMNAA method, utilized for analyzing USGS CRM RGM-1 and one Glass sample was further compared with relative NAA method.</div></div>","PeriodicalId":20861,"journal":{"name":"Radiation Physics and Chemistry","volume":"239 ","pages":"Article 113295"},"PeriodicalIF":2.8,"publicationDate":"2025-09-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145057373","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Jaber H. Alsalah Alyami , M.H. Nassef , Fahad F. Almutairi , Hanadi M. Khalifa
{"title":"Radiation dose assessment on the i-CAT Cone Beam Computed Tomography (CBCT) scanner","authors":"Jaber H. Alsalah Alyami , M.H. Nassef , Fahad F. Almutairi , Hanadi M. Khalifa","doi":"10.1016/j.radphyschem.2025.113291","DOIUrl":"10.1016/j.radphyschem.2025.113291","url":null,"abstract":"<div><h3>Objective</h3><div>The aim of this study was to assess radiation doses to surrounding organs from i-CAT Cone Beam Computed Tomography (CBCT) used in dental imaging and compare protocols with other similar clinical purpose by means of effective dose value. The radiation levels during the examination protocols inside the facility were also determined for protection purposes.</div></div><div><h3>Materials and methods</h3><div>The measured dose-area product (DAP) in mGycm<sup>2</sup> was used to assess the effective dose in microsievert (μSv) and a correction factor. The dose to the organ was measured using a type 100 thermoluminescent dosimeter, specifically LiF (Lithium Fluoride) TLDs Thermo Electron Corporation (TLD-100) and an adult anthropomorphic head and neck RANDO male phantom.</div><div>Measurements of dose area product in every protocol were performed using a dose area product meter coupled to a transmission ionization chamber. The measured DAP in mGycm<sup>2</sup> was used to assess the effective dose in microsievert (μSv) and a correction factor. The radiation doses to surrounding organs from i-CAT CBCT were also determined with TLD-100 inserted in the position of organs/tissues of an adult male anthropomorphic head and neck RANDO male phantom.</div></div><div><h3>Results</h3><div>The estimated value of the DAP ranged from 136.9 to 782.2 mGycm<sup>2</sup> with an average value of 337.8 mGycm<sup>2</sup> and was found to be low compared with the published data in the literature. At different fields of view and voxel sizes, the effective dose ranged between 25.44 and 145.33 μSv. The head and neck's radio-sensitive organs received doses ranging from 0.022 to 1.07 mGy. The radiation level ranged from 0.233 to 1.045 μSv/hr. with an average value of 0.622μSv/hr and was found to be less than the daily limit of 10μSv/hr. All the measured doses were compared with the available data published in the literature.</div></div><div><h3>Conclusions</h3><div>In cone beam CT scanners, the DAP, and the effective dose are simple and faster techniques to measure the patient dose. The voxel size parameters and field of view (FOV) considerably impact effective radiation dose. It is important to optimize the exposure parameters during CBCT scans to reduce the radiation risk to patients.</div><div>The occupational exposure in the supervised area of the CBCT scanner facility did not exceed the annual dose limit of 20mSv/year. The KAU Dental Hospital's radiation protection program was effective because it followed the national guidelines that have been widely accepted.</div></div>","PeriodicalId":20861,"journal":{"name":"Radiation Physics and Chemistry","volume":"239 ","pages":"Article 113291"},"PeriodicalIF":2.8,"publicationDate":"2025-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145019837","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Deep learning optimization of modular neutron beam shutters via Monte Carlo simulations","authors":"Li-Fang Chen","doi":"10.1016/j.radphyschem.2025.113289","DOIUrl":"10.1016/j.radphyschem.2025.113289","url":null,"abstract":"<div><div>This work presents a novel data-driven methodology for optimizing modular neutron beam shutters by integrating Monte Carlo simulations (MCNP) with deep learning techniques. The novelty lies in combining physics-based simulations with machine learning to rapidly screen and identify high-performance shielding designs, reducing both radiation exposure and computational effort. The study targets a compact neutron science platform where a shutter on the thermal neutron line is required to minimize occupational dose during maintenance.</div><div>A dataset of 200 shutter configurations with different material sequences was generated using MCNP and used to train a fully connected neural network for neutron flux prediction. The trained model was then applied to 1,000 additional random designs, allowing rapid performance ranking. The top 20 candidates were re-evaluated by MCNP to verify accuracy.</div><div>Results show that the optimized design attenuates the neutron flux from 5.61 × 10<sup>9</sup> n·cm<sup>-2</sup>·s<sup>-1</sup> at the shutter entrance to 4.96 × 10<sup>5</sup> n·cm<sup>-2</sup>·s<sup>-1</sup> at the exit—achieving a reduction of four orders of magnitude. Compared to the best design among the initial 200 random cases, the machine learning–guided design further improves flux suppression by ∼13 %, while reducing MCNP evaluations by 82 %.</div><div>These findings highlight the application relevance of deep learning–assisted optimization in neutron system design, demonstrating its capability to lower radiation risks and accelerate the development of advanced shielding solutions.</div></div>","PeriodicalId":20861,"journal":{"name":"Radiation Physics and Chemistry","volume":"239 ","pages":"Article 113289"},"PeriodicalIF":2.8,"publicationDate":"2025-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145019835","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Numerical modeling and circuit simulation of alpha particle detection using CdTe-based sensor arrays","authors":"Asgar Hosseinnezhad, Hadi Sabri","doi":"10.1016/j.radphyschem.2025.113292","DOIUrl":"10.1016/j.radphyschem.2025.113292","url":null,"abstract":"<div><div>This paper investigates the design and simulation of cadmium telluride (CdTe)-based semiconductor sensors optimized for alpha particle detection in controlled environments. Leveraging the superior radiation sensitivity and high atomic number of CdTe, a compact detection module is modeled using finite element techniques to estimate charge collection efficiency and transient response characteristics. The electrical output signal generated by alpha interactions is then mapped onto an analog signal processing circuit and simulated using LTspice for performance evaluation. Signal amplification, noise reduction, and time response are quantitatively analyzed and benchmarked against existing detection systems. The results demonstrate that CdTe sensors provide reliable sensitivity and fast detection capability, making them suitable for real-time radiation monitoring applications.</div></div>","PeriodicalId":20861,"journal":{"name":"Radiation Physics and Chemistry","volume":"239 ","pages":"Article 113292"},"PeriodicalIF":2.8,"publicationDate":"2025-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145019836","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
W.N.A.W. Ghazali, N.M. Noor, A.A. Zurihanaz, N.H.A. Rashid, M.S. Khaidzir, N. Shamshurim
{"title":"Skin dose assessment using direct and indirect measurement for pregnant patient undergoing abdominal fluoroscopy procedure","authors":"W.N.A.W. Ghazali, N.M. Noor, A.A. Zurihanaz, N.H.A. Rashid, M.S. Khaidzir, N. Shamshurim","doi":"10.1016/j.radphyschem.2025.113294","DOIUrl":"https://doi.org/10.1016/j.radphyschem.2025.113294","url":null,"abstract":"Radiation exposure during complex Interventional Radiology (IR) procedures is often high, particularly in pregnant patients. It is important to monitor the patient's post-procedure condition by determining their Peak Skin Dose (PSD) value. However, direct measurements require a longer time to obtain the value. This study aimed to assess the accuracy of PSD in pregnant patients during abdominal procedures using direct and indirect measurements. PSD measurements were performed using thermoluminescent dosimeters (TLDs), Gafchromic LDV1 Film and Dose Monitoring Software (GE DoseWatch). Direct measurements were conducted using 20 sets of TLDs and a 21 cm × 30 cm LDV1 Film; placed on the patient's skin towards the X-ray tube. The patient underwent an abdominal procedure by using a Philips Allura Xper FD20/15 scanner. Indirect PSD measurements were simulated instantaneously using a GE DoseWatch. PSD distribution of TLDs revealed to be very low which is 290.23 mGy with deviation of 15.11 %, while PSD value for LDV1 Film and GE Dosewatch were 341.88 mGy and 345.44 mGy respectively with ±1.03 % percentage difference. An uncertainty of approximately ±25 % or less can be considered acceptable for PSD measurements in IR. The most accurate method for determining the PSD Value in patients is the Gafchromic LDV1 Film. The values of the radiation dose monitoring systems are comparable to those of the Gafchromic LDV1 Film, with a tolerable deviation. Thus, the dose monitoring system (GE DoseWatch) and the TLDs are reliable for determining the PSD Value for patients in the absence of Gafchromic LDV1 Film. However, the TLDs need to have some modifications to the methodology, and it is necessary to cover the whole beam during irradiation. Even though it is a high-risk procedure involving pregnant patients, PSD value for the patient was almost 0.2Gy, which is 10 % lower than the threshold value for early transient erythema symptoms (2Gy).","PeriodicalId":20861,"journal":{"name":"Radiation Physics and Chemistry","volume":"39 1","pages":""},"PeriodicalIF":2.9,"publicationDate":"2025-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145093878","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Measurement of fission product yields in the spectrum averaged neutron-induced fission of 232Th","authors":"H. Naik , Meghna Karkera , Vibha Vansola , Santhi Sheela Yeraguntla , Mayur Mehta , S.V. Suryanarayana , R. Makwana","doi":"10.1016/j.radphyschem.2025.113287","DOIUrl":"10.1016/j.radphyschem.2025.113287","url":null,"abstract":"<div><div>Cumulative yields of various fission products within the mass range of 77–151 have been measured in the spectrum averaged 4.93 and 8.31 MeV neutron induced fission of <sup>232</sup>Th by using an off-line γ-ray spectrometric technique. The neutron beams were obtained from the <sup>7</sup>Li(p,n) reaction with the proton energies of 7 and 15 MeV. Since the cumulative yield is not for the end mass fission product of an isobaric chain, charge distribution correction was applied to obtain the mass chain yield. From the mass chain yield data, the peak-to-valley (P/V) ratio, the average value of light mass (<A<sub>L</sub>>), heavy mass (<A<sub>H</sub>>) and the average number of neutrons (<ν>) were obtained. The data from the present work and literature in the <sup>232</sup>Th(n, f) reaction at various neutron energies were compared with the similar data in the <sup>232</sup>Th(γ, f) reaction. In both the reactions, it was found that the mass yield distribution are asymmetric with triple humps. The fission product yields for A = 133–134, A = 138–140, and A = 143–144 and their complementary products are higher than the yields of other fission products, which is the role of nuclear structure effect. The yields of symmetric products increase with excitation energy, which causes the decrease of peak-to-valley (P/V) ratio. The <A<sub>L</sub>>, <A<sub>H</sub>> and <<em>ν</em>> values at comparable excitation energy show a similar trend with a <strong>surprising</strong> differences in between the <sup>232</sup>Th(n, f) and <sup>232</sup>Th(γ, f) reactions.</div></div>","PeriodicalId":20861,"journal":{"name":"Radiation Physics and Chemistry","volume":"239 ","pages":"Article 113287"},"PeriodicalIF":2.8,"publicationDate":"2025-09-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145057374","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
E. Suljovrujic , D. Milicevic , S. Galovic , G. Stamboliev , H. Lewandowska , M. Rzepna , J. Sadlo
{"title":"Influence of different irradiation modalities on post-irradiation behavior and properties of highly-crystalline PP and its implications for radiation sterilization of medical devices","authors":"E. Suljovrujic , D. Milicevic , S. Galovic , G. Stamboliev , H. Lewandowska , M. Rzepna , J. Sadlo","doi":"10.1016/j.radphyschem.2025.113288","DOIUrl":"10.1016/j.radphyschem.2025.113288","url":null,"abstract":"<div><div>Concerns regarding the dangers of EtO to health, security, and environmental risks are driving single-use (SU) medical device manufacturers more and more toward radiation technologies. Sterilization can be successfully applied for most biomaterials and disposable medical devices using any of the three ionizing radiation modalities (gamma, X-ray, and e-beam (EB)). However, it is well known that ionizing radiation can significantly alter their structure and properties. Undesired structural changes and property deterioration can occur long after irradiation, i.e., during storage and implementation. Semicrystalline thermoplastic polymers such as isotactic polypropylene (iPP) are particularly sensitive to these effects due to the structural peculiarities and presence of long-lived free radicals in the crystalline core.</div><div>The evolution of long-lived free radicals in the highly crystalline PP structure and their impact on changes in thermal properties, crystallinity, and microstructure after irradiation, i.e., during storage, was investigated. Two different PP homopolymers with a high degree of isotacticity were prepared by slow cooling after compression molding to obtain structures with the highest possible crystallinity. Subsequently, the samples were irradiated by electron beam and gamma radiation, focusing on the maximum sterilization dose of 50 kGy. The presence and evolution of free radicals were followed using electron spin resonance (ESR) spectroscopy for up to 6 months. Additional characterization was conducted by optical microscopy (OM), scanning electron microscopy (SEM), wide angle X-ray diffraction (WAXD), and differential scanning calorimetry (DSC).</div></div>","PeriodicalId":20861,"journal":{"name":"Radiation Physics and Chemistry","volume":"239 ","pages":"Article 113288"},"PeriodicalIF":2.8,"publicationDate":"2025-09-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144996312","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Fabrication and characterization of TiO2 reinforced polydimethylsiloxane nanocomposite for simulation based gamma radiation shielding","authors":"Summan Urooge , Kashif Shahzad , Srosh Fazil , Khuram Liaqat , Ahsan Irshad , Fakhar Alam , Afrasiab Khan , Rehan Hassan , Mehboob Alam","doi":"10.1016/j.radphyschem.2025.113270","DOIUrl":"10.1016/j.radphyschem.2025.113270","url":null,"abstract":"<div><div>Gamma radiation shielding is essential to protect human health and equipment in medical, nuclear, and industrial environments, but conventional materials such as lead and concrete are heavy, rigid, and environmentally hazardous, motivating the development of lightweight, flexible, and effective alternatives like TiO<sub>2</sub>/PDMS nanocomposites. This study investigates the gamma radiation shielding performance of PDMS nanocomposites reinforced with TiO<sub>2</sub> nanoparticles at 0, 3, 4, and 5 wt%. Nanocomposites were synthesized via hydrothermal method. The uniform dispersion and interaction of TiO<sub>2</sub> within the PDMS matrix were confirmed using X-ray diffraction (XRD), Fourier transform infrared spectroscopy (FTIR), and scanning electron microscopy (SEM). Shielding performance was evaluated experimentally using <sup>133</sup>Ba, <sup>137</sup>Cs, and <sup>60</sup>Co sources. The parameters including linear attenuation coefficient (LAC), mass attenuation coefficient (MAC), half value layer (HVL), tenth value layer (TVL), and mean free path (MFP) were quantified. Among all formulations, the 5 wt% TiO<sub>2</sub> composite exhibited the highest shielding efficiency, achieving a LAC of 0.13518 cm<sup>−1</sup>, MAC of 0.11965 cm<sup>2</sup>/g at 356 keV and a HVL reduction from 6.54 cm in pure PDMS to 5.13 cm representing an improvement of 22 %. At 662 keV, the HVL decreased from 8.27 cm (pure PDMS) to 6.75 cm. The 5 wt% composite also showed the lowest TVL (18.88 cm at 356 keV) and shortest MFP (7.40 cm at 356 keV) across all energies tested. Simulation results closely matched experimental data, confirming that the high Z TiO<sub>2</sub> filler enhanced photon attenuation through photoelectric and Compton scattering mechanisms. These findings establish the 5 wt% TiO<sub>2</sub> PDMS nanocomposite as the optimal formulation, offering effective gamma shielding with mechanical flexibility, low density, and non toxicity suitable for medical, nuclear, and aerospace protective applications.</div></div>","PeriodicalId":20861,"journal":{"name":"Radiation Physics and Chemistry","volume":"239 ","pages":"Article 113270"},"PeriodicalIF":2.8,"publicationDate":"2025-09-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145004654","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Multifunctional characterization of biocompatible P2O5-based glasses: Radiation shielding, electrical conductivity, and dielectric relaxation","authors":"Abdulaziz A. Alshihri , Yousef Alshumrani , Wael Alshehri , Merfat Algethami , F.M. Aldosari , A.A. Bendary , Sayed A. Makhlouf , Atef Ismail","doi":"10.1016/j.radphyschem.2025.113265","DOIUrl":"10.1016/j.radphyschem.2025.113265","url":null,"abstract":"<div><div>This study investigates the structural, dielectric, and electrical properties of phosphate-based glasses modified by replacing P<sub>2</sub>O<sub>5</sub> with Fe<sub>2</sub>O<sub>3</sub>. Using Fourier transform infrared (FTIR) spectroscopy and conductivity measurements, the findings confirm the amorphous nature of the glasses prepared via the fast-quench method. The substitution of Fe<sub>2</sub>O<sub>3</sub> impacts the phosphate glass lattice by reducing oxygen content, modifying vibration modes, and increasing glass humidity, which enhances the dielectric constant and radiation shielding efficiency. Temperature-dependent conductivity measurements reveal distinct thermally activated behavior, correlated barrier hopping (CBH) at temperature range (300–500 K). The conductivity changes are attributed to Fe<sub>2</sub>O<sub>3</sub>'s multivalent semiconductor role, which modifies the glass network and facilitates charge carrier mobility. Furthermore, the study highlights the dielectric modulus as a more reliable indicator of relaxation behavior compared to the dielectric constant, as it minimizes distortion from electrode polarization. The substitution of Fe<sub>2</sub>O<sub>3</sub> caused both the activation energy ΔE<sub>d</sub> and the characteristic relaxation time τ<sub>o</sub> to change from 0.723 eV to 0.81 eV and from 53 s to 3.53 s, respectively. This gradual increase in dielectric activation energy (ΔE<sub>d</sub>) due to increased structural rigidity and reduced free space in the glass matrix with higher Fe<sub>2</sub>O<sub>3</sub> content. These findings underscore the potential of Fe<sub>2</sub>O<sub>3</sub>-modified phosphate glasses for applications in electronics, optoelectronics, and energy storage devices.</div></div>","PeriodicalId":20861,"journal":{"name":"Radiation Physics and Chemistry","volume":"239 ","pages":"Article 113265"},"PeriodicalIF":2.8,"publicationDate":"2025-09-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145004651","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Investigation of physicochemical, mechanical, and radiation shielding properties of BaO–ZnO–B2O3–Bi2O3 glasses","authors":"M.I. Sayyed , Nidal Dwaikat , Abdelkrim Mekki , Awatif Alshamari , M Kh Hamad , M.H.A. Mhareb","doi":"10.1016/j.radphyschem.2025.113286","DOIUrl":"10.1016/j.radphyschem.2025.113286","url":null,"abstract":"<div><div>A comprehensive study was conducted on a series of glass samples, consisting of four samples with a composition of BaO–ZnO–B<sub>2</sub>O<sub>3</sub>–Bi<sub>2</sub>O<sub>3</sub>. The glasses were prepared using the melt-quench method, and several physicochemical instruments were employed to characterize the samples, including X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS), and Fourier Transform Infrared Spectroscopy (FTIR). The radiation shielding properties were studied experimentally at 0.184, 0.280, 0.662, 0.710, and 0.810 MeV. The mechanical and structural features were examined theoretically and linked with XPS results. The XRD results exhibited the amorphous nature of all glasses. Meanwhile, the FTIR spectrum revealed the functional groups of B<sub>2</sub>O<sub>3</sub>, with slight variations in their positions. The XPS results showed a reduction in the bridging oxygen bond (BO) with decreasing B<sub>2</sub>O<sub>3</sub>, confirming the decrease in glass stability. A reduction in mechanical and structural properties is observed, confirming a decrease in glass stability. The band gap also showed a reduction with the reduced amount of B<sub>2</sub>O<sub>3</sub>. The mass attenuation coefficient (MAC) for the glasses was experimentally determined, and the measured MAC was compared with that obtained from XCOM software to validate the accuracy of the experimental data. The relative difference (RD) between the two methods varied between a minimum of 1.2 % and a maximum of 9.7 %. The half-value layer results showed that a sample of the prepared glasses with a thickness of approximately 0.5 cm is sufficient to shield 50 % of the photons with an energy of 0.184 MeV. The results also demonstrated that increasing the BaO, ZnO, and Bi<sub>2</sub>O<sub>3</sub> leads to a decrease in the HVL.</div></div>","PeriodicalId":20861,"journal":{"name":"Radiation Physics and Chemistry","volume":"239 ","pages":"Article 113286"},"PeriodicalIF":2.8,"publicationDate":"2025-09-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145004655","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}