{"title":"剂量测定荧光粉 BaSO4-Dy 中电子激发向杂质的能量转移","authors":"T.N. Nurakhmetov, K.B. Zhangylyssov, R.K. Shamiyeva, T.T. Alibay, Zh.M Salikhodzha, B.M. Sadykova, D.A. Tolekov, B.N. Yussupbekova","doi":"10.1016/j.nimb.2024.165459","DOIUrl":null,"url":null,"abstract":"<div><p>The formation of new radiative states from the combination of <span><math><mrow><msup><mrow><mi>D</mi><mi>y</mi></mrow><mrow><mn>2</mn><mo>+</mo></mrow></msup><mo>-</mo><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mo>-</mo></msubsup></mrow></math></span> and <span><math><mrow><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mrow><mn>3</mn><mo>-</mo></mrow></msubsup><mo>-</mo><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mo>-</mo></msubsup></mrow></math></span> electron trapping centers in the range of 2.95–3.1 eV has been investigated using VUV and thermal activation spectroscopy. During the excitation process, there is a charge transfer between the oxygen ion of the sulfate anion and <span><math><msup><mrow><mi>D</mi><mi>y</mi></mrow><mrow><mn>3</mn><mo>+</mo><mspace></mspace></mrow></msup></math></span> leading to the formation of a combined emissive state <span><math><mrow><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mrow><mn>3</mn><mo>-</mo></mrow></msubsup><mo>→</mo><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mo>-</mo></msubsup></mrow></math></span>. These states can be formed from the electron-hole trapping centers of <span><math><mrow><msup><mrow><mi>D</mi><mi>y</mi></mrow><mrow><mn>2</mn><mo>+</mo></mrow></msup><mo>-</mo><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mo>-</mo></msubsup></mrow></math></span> and <span><math><mrow><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mrow><mn>3</mn><mo>-</mo></mrow></msubsup><mo>-</mo><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mo>-</mo></msubsup></mrow></math></span>. The combined radiative state at 2.95–3.1 eV and impurity emission at 2.16 eV and 2.56 eV are excited simultaneously by photons of 3.95 eV and 4.5 eV, respectively. During the thermal or optical excitation process, the <span><math><msup><mrow><mi>D</mi><mi>y</mi></mrow><mrow><mn>2</mn><mo>+</mo></mrow></msup></math></span> and <span><math><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mrow><mn>3</mn><mo>-</mo></mrow></msubsup></math></span> electronic centers are ionized. Electrons recombine with a hole trapped by the ground state of the impurity (<span><math><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mo>-</mo></msubsup></math></span> <span><math><mo>-</mo></math></span> <span><math><msup><mrow><mi>D</mi><mi>y</mi></mrow><mrow><mn>3</mn><mo>+</mo></mrow></msup></math></span>), and the released energy is transferred to the <span><math><msup><mrow><mi>D</mi><mi>y</mi></mrow><mrow><mn>3</mn><mo>+</mo></mrow></msup></math></span> impurities.</p></div>","PeriodicalId":19380,"journal":{"name":"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms","volume":"555 ","pages":"Article 165459"},"PeriodicalIF":1.4000,"publicationDate":"2024-07-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"The energy transfer of electronic excitations to impurities in dosimetric phosphors BaSO4-Dy\",\"authors\":\"T.N. Nurakhmetov, K.B. Zhangylyssov, R.K. Shamiyeva, T.T. Alibay, Zh.M Salikhodzha, B.M. Sadykova, D.A. Tolekov, B.N. Yussupbekova\",\"doi\":\"10.1016/j.nimb.2024.165459\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>The formation of new radiative states from the combination of <span><math><mrow><msup><mrow><mi>D</mi><mi>y</mi></mrow><mrow><mn>2</mn><mo>+</mo></mrow></msup><mo>-</mo><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mo>-</mo></msubsup></mrow></math></span> and <span><math><mrow><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mrow><mn>3</mn><mo>-</mo></mrow></msubsup><mo>-</mo><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mo>-</mo></msubsup></mrow></math></span> electron trapping centers in the range of 2.95–3.1 eV has been investigated using VUV and thermal activation spectroscopy. During the excitation process, there is a charge transfer between the oxygen ion of the sulfate anion and <span><math><msup><mrow><mi>D</mi><mi>y</mi></mrow><mrow><mn>3</mn><mo>+</mo><mspace></mspace></mrow></msup></math></span> leading to the formation of a combined emissive state <span><math><mrow><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mrow><mn>3</mn><mo>-</mo></mrow></msubsup><mo>→</mo><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mo>-</mo></msubsup></mrow></math></span>. These states can be formed from the electron-hole trapping centers of <span><math><mrow><msup><mrow><mi>D</mi><mi>y</mi></mrow><mrow><mn>2</mn><mo>+</mo></mrow></msup><mo>-</mo><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mo>-</mo></msubsup></mrow></math></span> and <span><math><mrow><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mrow><mn>3</mn><mo>-</mo></mrow></msubsup><mo>-</mo><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mo>-</mo></msubsup></mrow></math></span>. The combined radiative state at 2.95–3.1 eV and impurity emission at 2.16 eV and 2.56 eV are excited simultaneously by photons of 3.95 eV and 4.5 eV, respectively. During the thermal or optical excitation process, the <span><math><msup><mrow><mi>D</mi><mi>y</mi></mrow><mrow><mn>2</mn><mo>+</mo></mrow></msup></math></span> and <span><math><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mrow><mn>3</mn><mo>-</mo></mrow></msubsup></math></span> electronic centers are ionized. Electrons recombine with a hole trapped by the ground state of the impurity (<span><math><msubsup><mrow><mi>S</mi><mi>O</mi></mrow><mrow><mn>4</mn></mrow><mo>-</mo></msubsup></math></span> <span><math><mo>-</mo></math></span> <span><math><msup><mrow><mi>D</mi><mi>y</mi></mrow><mrow><mn>3</mn><mo>+</mo></mrow></msup></math></span>), and the released energy is transferred to the <span><math><msup><mrow><mi>D</mi><mi>y</mi></mrow><mrow><mn>3</mn><mo>+</mo></mrow></msup></math></span> impurities.</p></div>\",\"PeriodicalId\":19380,\"journal\":{\"name\":\"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms\",\"volume\":\"555 \",\"pages\":\"Article 165459\"},\"PeriodicalIF\":1.4000,\"publicationDate\":\"2024-07-14\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0168583X24002295\",\"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 B-beam Interactions With Materials and Atoms","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0168583X24002295","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}
引用次数: 0
摘要
我们利用紫外和热激活光谱法研究了在 2.95-3.1 eV 范围内 Dy2+-SO4- 和 SO43--SO4- 电子俘获中心组合形成的新辐射态。在激发过程中,硫酸根阴离子的氧离子与 Dy3+ 之间发生了电荷转移,从而形成了 SO43-→SO4- 组合发射态。这些状态可由 Dy2+-SO4- 和 SO43--SO4- 的电子-空穴捕获中心形成。3.95 eV 和 4.5 eV 的光子分别同时激发了 2.95-3.1 eV 的组合辐射态和 2.16 eV 和 2.56 eV 的杂质发射态。在热激发或光激发过程中,Dy2+ 和 SO43- 电子中心发生电离。电子与杂质(SO4- - Dy3+)基态捕获的空穴重新结合,释放的能量转移到 Dy3+ 杂质上。
The energy transfer of electronic excitations to impurities in dosimetric phosphors BaSO4-Dy
The formation of new radiative states from the combination of and electron trapping centers in the range of 2.95–3.1 eV has been investigated using VUV and thermal activation spectroscopy. During the excitation process, there is a charge transfer between the oxygen ion of the sulfate anion and leading to the formation of a combined emissive state . These states can be formed from the electron-hole trapping centers of and . The combined radiative state at 2.95–3.1 eV and impurity emission at 2.16 eV and 2.56 eV are excited simultaneously by photons of 3.95 eV and 4.5 eV, respectively. During the thermal or optical excitation process, the and electronic centers are ionized. Electrons recombine with a hole trapped by the ground state of the impurity ( ), and the released energy is transferred to the impurities.
期刊介绍:
Section B of Nuclear Instruments and Methods in Physics Research covers all aspects of the interaction of energetic beams with atoms, molecules and aggregate forms of matter. This includes ion beam analysis and ion beam modification of materials as well as basic data of importance for these studies. Topics of general interest include: atomic collisions in solids, particle channelling, all aspects of collision cascades, the modification of materials by energetic beams, ion implantation, irradiation - induced changes in materials, the physics and chemistry of beam interactions and the analysis of materials by all forms of energetic radiation. Modification by ion, laser and electron beams for the study of electronic materials, metals, ceramics, insulators, polymers and other important and new materials systems are included. Related studies, such as the application of ion beam analysis to biological, archaeological and geological samples as well as applications to solve problems in planetary science are also welcome. Energetic beams of interest include atomic and molecular ions, neutrons, positrons and muons, plasmas directed at surfaces, electron and photon beams, including laser treated surfaces and studies of solids by photon radiation from rotating anodes, synchrotrons, etc. In addition, the interaction between various forms of radiation and radiation-induced deposition processes are relevant.