Pressure measurement and detection of small H<sub>2</sub>O amounts in high‐pressure H<sub>2</sub>O–CO<sub>2</sub> fluid up to 141 MPa using Fermi diad splits and bandwidths of CO<sub>2</sub>
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- Yuuki Hagiwara
- Graduate School of Science Hokkaido University Sapporo Japan
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- Junji Torimoto
- Ore Genesis Research Unit, Project Team for Development of New‐Generation Research Protocol for Submarine Resources JAMSTEC Yokosuka‐shi Japan
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- Junji Yamamoto
- The Hokkaido University Museum Sapporo Japan
書誌事項
- 公開日
- 2020-03-09
- 資源種別
- journal article
- 権利情報
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- http://onlinelibrary.wiley.com/termsAndConditions#vor
- DOI
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- 10.1002/jrs.5865
- 公開者
- Wiley
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説明
<jats:title>Abstract</jats:title><jats:p>Dependence of residual pressures of fluid inclusions on their size and host mineral species provides valuable information related to the depth provenance and <jats:italic>P</jats:italic>–<jats:italic>T</jats:italic>–<jats:italic>t</jats:italic> path of the rocks. Although Raman‐based barometry is an effective method for ascertaining the internal pressure of H<jats:sub>2</jats:sub>O–CO<jats:sub>2</jats:sub> fluid inclusions, few studies have elucidated Raman spectral features of CO<jats:sub>2</jats:sub> in a system of high‐pressure H<jats:sub>2</jats:sub>O–CO<jats:sub>2</jats:sub>. New experiments using a high‐pressure optical cell in this binary system with compositions of 100, 75 ± 2, and 60 ± 2 mol% CO<jats:sub>2</jats:sub> were conducted for this study to verify the availability of Raman CO<jats:sub>2</jats:sub> barometers for use in assessing the temperature and pressure conditions of approximately 22°C and 17.3–141.4 MPa. Our results demonstrate that the existence of H<jats:sub>2</jats:sub>O does not affect the relation between Fermi diad splits (Δ, cm<jats:sup>−1</jats:sup>) and total pressure of pure CO<jats:sub>2</jats:sub>. These results suggest that the Δ–total pressure relation obtained from pure CO<jats:sub>2</jats:sub> is also applicable to H<jats:sub>2</jats:sub>O–CO<jats:sub>2</jats:sub> systems, even at high pressure. However, unlike Δ, because the peak positions of the Fermi diad in the system of H<jats:sub>2</jats:sub>O–CO<jats:sub>2</jats:sub> shift to a higher wavenumber than those of pure CO<jats:sub>2</jats:sub> at given pressure higher than 30 MPa, the peak positions are not very suitable for the pressure scale in an H<jats:sub>2</jats:sub>O–CO<jats:sub>2</jats:sub> system. Additionally, we confirmed the availability of bandwidths of CO<jats:sub>2</jats:sub> as an indicator of compositions that can identify the presence of very small amounts of H<jats:sub>2</jats:sub>O (at least 0.3 mol% H<jats:sub>2</jats:sub>O), even at room temperature.</jats:p>
収録刊行物
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- Journal of Raman Spectroscopy
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Journal of Raman Spectroscopy 51 (6), 1003-1018, 2020-03-09
Wiley
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詳細情報 詳細情報について
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- CRID
- 1361412889656232576
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- DOI
- 10.1002/jrs.5865
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- ISSN
- 10974555
- 03770486
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- Web Site
- https://api.wiley.com/onlinelibrary/tdm/v1/articles/10.1002%2Fjrs.5865
- https://onlinelibrary.wiley.com/doi/pdf/10.1002/jrs.5865
- https://onlinelibrary.wiley.com/doi/full-xml/10.1002/jrs.5865
- https://onlinelibrary.wiley.com/doi/am-pdf/10.1002%2Fjrs.5865
- https://analyticalsciencejournals.onlinelibrary.wiley.com/doi/pdf/10.1002/jrs.5865
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- 資料種別
- journal article
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- データソース種別
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