Experimental Observation of 2– Anion and its para → ortho Conversion in Solid para hydrogen Using High–Resolution ESR Spectroscopy

被引:0
作者
T. Kumada
Y. Aratono
T. Miyazaki
机构
[1] Japan Atomic Energy Research Institute,Advanced Science Research Center
[2] Tokai–mura,Department of Applied Chemistry
[3] Naka–gun,undefined
[4] School of Engineering,undefined
[5] Nagoya University,undefined
[6] Furo-cho,undefined
来源
Journal of Low Temperature Physics | 1998年 / 111卷
关键词
Hydrogen; Spectroscopy; Magnetic Field; Experimental Observation; Magnetic Material;
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摘要
We present experimental observations and study of\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $${\text{H}}_{\text{2}}^ - $$ \end{document}in solid parahydrogen. Since the parahydrogen molecule does not produce local magnetic fields, high–resolution ESR spectra of trapped radicals can be observed in the solid parahydrogen matrices. Using this high–resolution ESR spectroscopy, new quartet ESR signals were observed in γ–rays irradiated solid parahydrogen and assigned as\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $${\text{H}}_{\text{2}}^ - $$ \end{document}In addition, para–\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $${\text{H}}_{\text{2}}^ - $$ \end{document}was observed to convert into ortho–\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $${\text{H}}_{\text{2}}^ - $$ \end{document}on the storage at 4.2 K. On the other hand, ortho–H2molecule converts into para–\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $${\text{H}}_{\text{2}}^ - $$ \end{document}at cryogenic temperatures. The difference in the conversion between the H2molecule and the\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $${\text{H}}_{\text{2}}^ - $$ \end{document}anion is explained by the parity conservation law of wavefunctions on exchanging the protons in homonuclear diatomic molecules such as the\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $${\text{H}}_{\text{2}}^ - $$ \end{document}anion and H2molecule.
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页码:509 / 514
页数:5
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