Le Thi Ngoc Trang , Nguyen Huynh Duy Khang , Nguyen Thi Truc Linh , Nguyen Thanh Dat , Huynh Dinh Chuong , Hoang Duc Tam
{"title":"基于瑞利-康普顿散射比的宽能量范围内质量衰减系数的确定:曲线拟合和机器学习方法","authors":"Le Thi Ngoc Trang , Nguyen Huynh Duy Khang , Nguyen Thi Truc Linh , Nguyen Thanh Dat , Huynh Dinh Chuong , Hoang Duc Tam","doi":"10.1016/j.nima.2025.170555","DOIUrl":null,"url":null,"abstract":"<div><div>In this study, we present two novel methods for determining the mass attenuation coefficient over a broad energy range based on the Rayleigh and Compton scattering spectra collected by a Si(Li) detector. These methods involve developing either curve-fitting models or artificial neural network models to obtain (i) the relationship between the effective atomic number and the Rayleigh to Compton scattering ratio, and (ii) the dependence of the mass attenuation coefficient on both the effective atomic number and photon energy. Using these models, the mass attenuation coefficient can be calculated from input data consisting of the Rayleigh to Compton scattering ratio and photon energy. Next, we applied the proposed methods to 12 different materials, thereby confirming their accuracy. The results show that both methods offer equivalent accuracy. Specifically, within the energy range of 200 keV to 10 MeV, the mass attenuation coefficients determined by these methods exhibit relative deviations of less than 6 % when compared to XCOM (NIST) values. However, in the low-energy range of 50 keV–200 keV, the relative deviations can be significant for multi-element materials (reaching up to 43 %). Overall, these findings demonstrate the feasibility of our proposed methods as additional solutions for determining the mass attenuation coefficient of materials. Two notable advantages of these methods are that they can derive the mass attenuation coefficient across a broad energy range without requiring any information about the sample composition and that the data set used to fit the calibration curves or train the artificial neural network is generated via Monte Carlo simulations.</div></div>","PeriodicalId":19359,"journal":{"name":"Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment","volume":"1077 ","pages":"Article 170555"},"PeriodicalIF":1.5000,"publicationDate":"2025-04-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Determination of the mass attenuation coefficient over a broad energy range based on the Rayleigh to Compton scattering ratio: Curve-fitting and machine learning methods\",\"authors\":\"Le Thi Ngoc Trang , Nguyen Huynh Duy Khang , Nguyen Thi Truc Linh , Nguyen Thanh Dat , Huynh Dinh Chuong , Hoang Duc Tam\",\"doi\":\"10.1016/j.nima.2025.170555\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>In this study, we present two novel methods for determining the mass attenuation coefficient over a broad energy range based on the Rayleigh and Compton scattering spectra collected by a Si(Li) detector. These methods involve developing either curve-fitting models or artificial neural network models to obtain (i) the relationship between the effective atomic number and the Rayleigh to Compton scattering ratio, and (ii) the dependence of the mass attenuation coefficient on both the effective atomic number and photon energy. Using these models, the mass attenuation coefficient can be calculated from input data consisting of the Rayleigh to Compton scattering ratio and photon energy. Next, we applied the proposed methods to 12 different materials, thereby confirming their accuracy. The results show that both methods offer equivalent accuracy. Specifically, within the energy range of 200 keV to 10 MeV, the mass attenuation coefficients determined by these methods exhibit relative deviations of less than 6 % when compared to XCOM (NIST) values. However, in the low-energy range of 50 keV–200 keV, the relative deviations can be significant for multi-element materials (reaching up to 43 %). Overall, these findings demonstrate the feasibility of our proposed methods as additional solutions for determining the mass attenuation coefficient of materials. Two notable advantages of these methods are that they can derive the mass attenuation coefficient across a broad energy range without requiring any information about the sample composition and that the data set used to fit the calibration curves or train the artificial neural network is generated via Monte Carlo simulations.</div></div>\",\"PeriodicalId\":19359,\"journal\":{\"name\":\"Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment\",\"volume\":\"1077 \",\"pages\":\"Article 170555\"},\"PeriodicalIF\":1.5000,\"publicationDate\":\"2025-04-21\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0168900225003560\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"INSTRUMENTS & INSTRUMENTATION\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0168900225003560","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"INSTRUMENTS & INSTRUMENTATION","Score":null,"Total":0}
Determination of the mass attenuation coefficient over a broad energy range based on the Rayleigh to Compton scattering ratio: Curve-fitting and machine learning methods
In this study, we present two novel methods for determining the mass attenuation coefficient over a broad energy range based on the Rayleigh and Compton scattering spectra collected by a Si(Li) detector. These methods involve developing either curve-fitting models or artificial neural network models to obtain (i) the relationship between the effective atomic number and the Rayleigh to Compton scattering ratio, and (ii) the dependence of the mass attenuation coefficient on both the effective atomic number and photon energy. Using these models, the mass attenuation coefficient can be calculated from input data consisting of the Rayleigh to Compton scattering ratio and photon energy. Next, we applied the proposed methods to 12 different materials, thereby confirming their accuracy. The results show that both methods offer equivalent accuracy. Specifically, within the energy range of 200 keV to 10 MeV, the mass attenuation coefficients determined by these methods exhibit relative deviations of less than 6 % when compared to XCOM (NIST) values. However, in the low-energy range of 50 keV–200 keV, the relative deviations can be significant for multi-element materials (reaching up to 43 %). Overall, these findings demonstrate the feasibility of our proposed methods as additional solutions for determining the mass attenuation coefficient of materials. Two notable advantages of these methods are that they can derive the mass attenuation coefficient across a broad energy range without requiring any information about the sample composition and that the data set used to fit the calibration curves or train the artificial neural network is generated via Monte Carlo simulations.
期刊介绍:
Section A of Nuclear Instruments and Methods in Physics Research publishes papers on design, manufacturing and performance of scientific instruments with an emphasis on large scale facilities. This includes the development of particle accelerators, ion sources, beam transport systems and target arrangements as well as the use of secondary phenomena such as synchrotron radiation and free electron lasers. It also includes all types of instrumentation for the detection and spectrometry of radiations from high energy processes and nuclear decays, as well as instrumentation for experiments at nuclear reactors. Specialized electronics for nuclear and other types of spectrometry as well as computerization of measurements and control systems in this area also find their place in the A section.
Theoretical as well as experimental papers are accepted.