{"title":"辐照方解石和文石中亚硫酸盐自由基的电子自旋共振","authors":"Ayako Kai, Toshikatsu Miki","doi":"10.1016/1359-0197(92)90211-W","DOIUrl":null,"url":null,"abstract":"<div><p>Radiation-induced radicals in sulfite-doped calcite and aragonite were characterized by ESR. Among the many ESR signals produced, only four signals are dependent on the SO<sup>2-</sup><sub>3</sub> concentration; an axial signal (<em>g</em><sub>⊥</sub>=2.0038 and <em>g</em>|=2.0024) in calcite, and an orthorhombic signal (<em>g</em><sub>1</sub>=2.0042, <em>g</em><sub>2=2.0038</sub> and <em>g</em><sub>3</sub>=2.0025), an isotropic signal (<em>g</em>=2.0034) and an isotropic signal (<em>g</em>=2.0060) in aragonite. The former two signals exhibit hyperfine structures arising from <sup>33<em>S</em></sup><span><math><mtext>(I=</mtext><mtext>3</mtext><mtext>2</mtext><mtext>, 0.75%</mtext></math></span> natural abundance), and are attributed to SO<sup>-</sup><sub>3</sub> radicals. The isotropic signal at <em>g</em>=2.0034 in aragonite is considered to be due to rotating SO<sup>-</sup><sub>3</sub> radicals. Rotating or tumbling molecules (probably SO<sup>-</sup><sub>2</sub>) produced by thermal decomposition of SO<sup>2-</sup><sub>3</sub> seem to be responsible for the isotropic signal at <em>f=2.0060</em>.</p></div>","PeriodicalId":14262,"journal":{"name":"International Journal of Radiation Applications and Instrumentation. Part C. Radiation Physics and Chemistry","volume":"40 6","pages":"Pages 469-476"},"PeriodicalIF":0.0000,"publicationDate":"1992-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/1359-0197(92)90211-W","citationCount":"32","resultStr":"{\"title\":\"Electron spin resonance of sulfite radicals in irradiated calcite and aragonite\",\"authors\":\"Ayako Kai, Toshikatsu Miki\",\"doi\":\"10.1016/1359-0197(92)90211-W\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>Radiation-induced radicals in sulfite-doped calcite and aragonite were characterized by ESR. Among the many ESR signals produced, only four signals are dependent on the SO<sup>2-</sup><sub>3</sub> concentration; an axial signal (<em>g</em><sub>⊥</sub>=2.0038 and <em>g</em>|=2.0024) in calcite, and an orthorhombic signal (<em>g</em><sub>1</sub>=2.0042, <em>g</em><sub>2=2.0038</sub> and <em>g</em><sub>3</sub>=2.0025), an isotropic signal (<em>g</em>=2.0034) and an isotropic signal (<em>g</em>=2.0060) in aragonite. The former two signals exhibit hyperfine structures arising from <sup>33<em>S</em></sup><span><math><mtext>(I=</mtext><mtext>3</mtext><mtext>2</mtext><mtext>, 0.75%</mtext></math></span> natural abundance), and are attributed to SO<sup>-</sup><sub>3</sub> radicals. The isotropic signal at <em>g</em>=2.0034 in aragonite is considered to be due to rotating SO<sup>-</sup><sub>3</sub> radicals. Rotating or tumbling molecules (probably SO<sup>-</sup><sub>2</sub>) produced by thermal decomposition of SO<sup>2-</sup><sub>3</sub> seem to be responsible for the isotropic signal at <em>f=2.0060</em>.</p></div>\",\"PeriodicalId\":14262,\"journal\":{\"name\":\"International Journal of Radiation Applications and Instrumentation. Part C. Radiation Physics and Chemistry\",\"volume\":\"40 6\",\"pages\":\"Pages 469-476\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1992-12-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/1359-0197(92)90211-W\",\"citationCount\":\"32\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"International Journal of Radiation Applications and Instrumentation. Part C. Radiation Physics and Chemistry\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/135901979290211W\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Journal of Radiation Applications and Instrumentation. Part C. Radiation Physics and Chemistry","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/135901979290211W","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Electron spin resonance of sulfite radicals in irradiated calcite and aragonite
Radiation-induced radicals in sulfite-doped calcite and aragonite were characterized by ESR. Among the many ESR signals produced, only four signals are dependent on the SO2-3 concentration; an axial signal (g⊥=2.0038 and g|=2.0024) in calcite, and an orthorhombic signal (g1=2.0042, g2=2.0038 and g3=2.0025), an isotropic signal (g=2.0034) and an isotropic signal (g=2.0060) in aragonite. The former two signals exhibit hyperfine structures arising from 33S natural abundance), and are attributed to SO-3 radicals. The isotropic signal at g=2.0034 in aragonite is considered to be due to rotating SO-3 radicals. Rotating or tumbling molecules (probably SO-2) produced by thermal decomposition of SO2-3 seem to be responsible for the isotropic signal at f=2.0060.