{"title":"方解石、白云石、红锰矿和菱铁矿中δ 13C和δ 18O的激光提取分析","authors":"M.D. Powell, T.K. Kyser","doi":"10.1016/0168-9622(91)90040-4","DOIUrl":null,"url":null,"abstract":"<div><p>δ <sup>13</sup>C- and δ <sup>18</sup>O-values of calcite, dolomite, rhodochrosite and siderite have been determined in situ using a laser extraction system, in which a focused Nd: YAG laser beam excites a sample surface producing a high-energy plasma cloud which forms CO and CO<sub>2</sub>. Laser ionization of calcite, dolomite, rhodochrosite and siderite produces different yields of CO<sub>2</sub> and CO and different CO<sub>2</sub>/CO ratios for each mineral. Isotopic analyses of combined CO and CO<sub>2</sub> are reproducible to ± 1–2‰ for δ <sup>18</sup>O and ± 2–3‰ for δ <sup>13</sup>C and are distinctly different from the isotopic compositions determined using standard acid dissolution techniques. CO<sub>2</sub> produced from laser ionization is consistently enriched in <sup>13</sup>C and <sup>18</sup>O compared to CO. A two-stage model is proposed to explain variations observed in the experimental results. In the first stage, the energy is absorbed by the mineral but the quantity and isotopic composition of gases depends on the chemical composition of the sample, especially the quantity of transition metals which have electronic transitions commensurate with the wavelength of the Nd: YAG. In the second stage, the relative isotopic compositions of CO and CO<sub>2</sub> are affected by reactions in the cooling plasma. This model should be applicable to all laser ionization systems.</p></div>","PeriodicalId":100231,"journal":{"name":"Chemical Geology: Isotope Geoscience section","volume":"94 1","pages":"Pages 55-66"},"PeriodicalIF":0.0000,"publicationDate":"1991-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0168-9622(91)90040-4","citationCount":"0","resultStr":"{\"title\":\"Analysis of δ 13C and δ 18O in calcite, dolomite, rhodochrosite and siderite using a laser extraction system\",\"authors\":\"M.D. Powell, T.K. Kyser\",\"doi\":\"10.1016/0168-9622(91)90040-4\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>δ <sup>13</sup>C- and δ <sup>18</sup>O-values of calcite, dolomite, rhodochrosite and siderite have been determined in situ using a laser extraction system, in which a focused Nd: YAG laser beam excites a sample surface producing a high-energy plasma cloud which forms CO and CO<sub>2</sub>. Laser ionization of calcite, dolomite, rhodochrosite and siderite produces different yields of CO<sub>2</sub> and CO and different CO<sub>2</sub>/CO ratios for each mineral. Isotopic analyses of combined CO and CO<sub>2</sub> are reproducible to ± 1–2‰ for δ <sup>18</sup>O and ± 2–3‰ for δ <sup>13</sup>C and are distinctly different from the isotopic compositions determined using standard acid dissolution techniques. CO<sub>2</sub> produced from laser ionization is consistently enriched in <sup>13</sup>C and <sup>18</sup>O compared to CO. A two-stage model is proposed to explain variations observed in the experimental results. In the first stage, the energy is absorbed by the mineral but the quantity and isotopic composition of gases depends on the chemical composition of the sample, especially the quantity of transition metals which have electronic transitions commensurate with the wavelength of the Nd: YAG. In the second stage, the relative isotopic compositions of CO and CO<sub>2</sub> are affected by reactions in the cooling plasma. This model should be applicable to all laser ionization systems.</p></div>\",\"PeriodicalId\":100231,\"journal\":{\"name\":\"Chemical Geology: Isotope Geoscience section\",\"volume\":\"94 1\",\"pages\":\"Pages 55-66\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1991-11-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/0168-9622(91)90040-4\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Chemical Geology: Isotope Geoscience section\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/0168962291900404\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Chemical Geology: Isotope Geoscience section","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/0168962291900404","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Analysis of δ 13C and δ 18O in calcite, dolomite, rhodochrosite and siderite using a laser extraction system
δ 13C- and δ 18O-values of calcite, dolomite, rhodochrosite and siderite have been determined in situ using a laser extraction system, in which a focused Nd: YAG laser beam excites a sample surface producing a high-energy plasma cloud which forms CO and CO2. Laser ionization of calcite, dolomite, rhodochrosite and siderite produces different yields of CO2 and CO and different CO2/CO ratios for each mineral. Isotopic analyses of combined CO and CO2 are reproducible to ± 1–2‰ for δ 18O and ± 2–3‰ for δ 13C and are distinctly different from the isotopic compositions determined using standard acid dissolution techniques. CO2 produced from laser ionization is consistently enriched in 13C and 18O compared to CO. A two-stage model is proposed to explain variations observed in the experimental results. In the first stage, the energy is absorbed by the mineral but the quantity and isotopic composition of gases depends on the chemical composition of the sample, especially the quantity of transition metals which have electronic transitions commensurate with the wavelength of the Nd: YAG. In the second stage, the relative isotopic compositions of CO and CO2 are affected by reactions in the cooling plasma. This model should be applicable to all laser ionization systems.