M. Salagram, K. Madhukar , T.S.N. Murthy , C.S. Sunandana
{"title":"x射线照射的KMgClSO4.3H2O中SO−3和SO−4自由基的ESR表征","authors":"M. Salagram, K. Madhukar , T.S.N. Murthy , C.S. Sunandana","doi":"10.1016/0584-8539(94)80097-9","DOIUrl":null,"url":null,"abstract":"<div><p>The ESR spectra of the kainite (KMgClSO<sub>4</sub>.3H<sub>2</sub>O) crystal revealed an intense isotropic (<em>g</em> = 2.004) peak C attributed to the SO<sup>−</sup><sub>3</sub> radical and two pairs of lines (A<sub>1</sub>, A<sub>2</sub>) and (B<sub>1</sub>, B<sub>2</sub>) bearing intensity ratio 5:3. The intensity and linewidth variation of peak C suggested that the signal contains an unresolved shf structure. The power saturation studies on SO<sup>−</sup><sub>3</sub> indicate that its ESR line is homogeneously broadened and its line shape is Lorentzian. The spin—lattice and spin—spin relaxation times (<em>T</em><sub>1</sub> and <em>T</em><sub>2</sub>) of SO<sup>−</sup><sub>3</sub> have been estimated to be 0.44 s and 656 μs, respectively. The analysis of the anisotropic pairs of lines show that they constitute two sets A and B and are due to two chemically inequivalent SO<sup>−</sup><sub>4</sub> radical species in the lattice. The ESR spectra of the polycrystalline samples recorded at 300 and 77 K confirm the isotropic behaviour of SO<sup>−</sup><sub>3</sub> and chemical inequivalence of two types of SO<sup>−</sup><sub>4</sub> radicals. The principal <em>g</em>-values of the SO<sup>−</sup><sub>4</sub> radical were evaluated to be: <em>g</em><sub>1</sub> = 2.007, <em>g</em><sub>2</sub> = 2.011, <em>g</em><sub>3</sub> = 2.014 for species A and <em>g</em><sub>1</sub> = 2.008, <em>g</em><sub>2</sub> = 2.012, <em>g</em><sub>3</sub> = 2.015 for species B. The low microsymmetry of the SO<sup>2−</sup><sub>4</sub> ion in the lattice seems to promote the radiation damage.</p></div>","PeriodicalId":82782,"journal":{"name":"Spectrochimica acta. Part A: Molecular spectroscopy","volume":"50 7","pages":"Pages 1309-1315"},"PeriodicalIF":0.0000,"publicationDate":"1994-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0584-8539(94)80097-9","citationCount":"7","resultStr":"{\"title\":\"ESR characterisation of SO−3 and SO−4 radicals in X-irradiated kainite (KMgClSO4.3H2O)\",\"authors\":\"M. Salagram, K. Madhukar , T.S.N. Murthy , C.S. Sunandana\",\"doi\":\"10.1016/0584-8539(94)80097-9\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>The ESR spectra of the kainite (KMgClSO<sub>4</sub>.3H<sub>2</sub>O) crystal revealed an intense isotropic (<em>g</em> = 2.004) peak C attributed to the SO<sup>−</sup><sub>3</sub> radical and two pairs of lines (A<sub>1</sub>, A<sub>2</sub>) and (B<sub>1</sub>, B<sub>2</sub>) bearing intensity ratio 5:3. The intensity and linewidth variation of peak C suggested that the signal contains an unresolved shf structure. The power saturation studies on SO<sup>−</sup><sub>3</sub> indicate that its ESR line is homogeneously broadened and its line shape is Lorentzian. The spin—lattice and spin—spin relaxation times (<em>T</em><sub>1</sub> and <em>T</em><sub>2</sub>) of SO<sup>−</sup><sub>3</sub> have been estimated to be 0.44 s and 656 μs, respectively. The analysis of the anisotropic pairs of lines show that they constitute two sets A and B and are due to two chemically inequivalent SO<sup>−</sup><sub>4</sub> radical species in the lattice. The ESR spectra of the polycrystalline samples recorded at 300 and 77 K confirm the isotropic behaviour of SO<sup>−</sup><sub>3</sub> and chemical inequivalence of two types of SO<sup>−</sup><sub>4</sub> radicals. The principal <em>g</em>-values of the SO<sup>−</sup><sub>4</sub> radical were evaluated to be: <em>g</em><sub>1</sub> = 2.007, <em>g</em><sub>2</sub> = 2.011, <em>g</em><sub>3</sub> = 2.014 for species A and <em>g</em><sub>1</sub> = 2.008, <em>g</em><sub>2</sub> = 2.012, <em>g</em><sub>3</sub> = 2.015 for species B. The low microsymmetry of the SO<sup>2−</sup><sub>4</sub> ion in the lattice seems to promote the radiation damage.</p></div>\",\"PeriodicalId\":82782,\"journal\":{\"name\":\"Spectrochimica acta. Part A: Molecular spectroscopy\",\"volume\":\"50 7\",\"pages\":\"Pages 1309-1315\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1994-07-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/0584-8539(94)80097-9\",\"citationCount\":\"7\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Spectrochimica acta. Part A: Molecular spectroscopy\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/0584853994800979\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Spectrochimica acta. Part A: Molecular spectroscopy","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/0584853994800979","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
ESR characterisation of SO−3 and SO−4 radicals in X-irradiated kainite (KMgClSO4.3H2O)
The ESR spectra of the kainite (KMgClSO4.3H2O) crystal revealed an intense isotropic (g = 2.004) peak C attributed to the SO−3 radical and two pairs of lines (A1, A2) and (B1, B2) bearing intensity ratio 5:3. The intensity and linewidth variation of peak C suggested that the signal contains an unresolved shf structure. The power saturation studies on SO−3 indicate that its ESR line is homogeneously broadened and its line shape is Lorentzian. The spin—lattice and spin—spin relaxation times (T1 and T2) of SO−3 have been estimated to be 0.44 s and 656 μs, respectively. The analysis of the anisotropic pairs of lines show that they constitute two sets A and B and are due to two chemically inequivalent SO−4 radical species in the lattice. The ESR spectra of the polycrystalline samples recorded at 300 and 77 K confirm the isotropic behaviour of SO−3 and chemical inequivalence of two types of SO−4 radicals. The principal g-values of the SO−4 radical were evaluated to be: g1 = 2.007, g2 = 2.011, g3 = 2.014 for species A and g1 = 2.008, g2 = 2.012, g3 = 2.015 for species B. The low microsymmetry of the SO2−4 ion in the lattice seems to promote the radiation damage.