A Simple Model for N2Line Oscillator Strengths of the \documentclass{aastex} \usepackage{amsbsy} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{bm} \usepackage{mathrsfs} \usepackage{pifont} \usepackage{stmaryrd} \usepackage{textcomp} \usepackage{portland,xspace} \usepackage{amsmath,amsxtra} \usepackage[OT2,OT1]{fontenc} \newcommand\cyr{ \renewcommand\rmdefault{wncyr} \renewcommand\sfdefault{wncyss} \renewcommand\encodingdefault{OT2} \normalfont \selectfont} \DeclareTextFontCommand{\textcyr}{\cyr} \pagestyle{empty} \DeclareMathSizes{10}{9}{7}{6} \begin{document} \landscape $b^{\prime }\, {}^{1}\Sigma ^{+}_{u}( 1) $ \end{document} , \documentclass{aastex} \usepackage{amsbsy} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{bm} \usepackage{mathrsfs} \usepackage{pifont} \usepackage{stmaryrd} \usepackage{textcomp} \usepackage{portland,xspace} \usepackage{amsmath,amsxtra} \usepackage[OT2,OT1]{fontenc} \newcommand\cyr{ \renewcommand\rmdefault{wncyr} \renewcommand\sfdefault{wncyss} \renewcommand\encodingdefault{OT2} \normalfont \selectfont} \DeclareTextFontCommand{\textcyr}{\cyr} \pagestyle{empty} \DeclareMathSizes{10}{9}{7}{6} \begin{document} \landscape $c^{\prime }_{4}\, {}^{1}\Sigma ^{+}_{u}( 0) $ \end{document} , \documentclass{aastex} \usepackage{amsbsy} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{bm} \usepackage{mathrsfs} \usepackage{pifont} \usepackage{stmaryrd} \usepackage{textcomp} \usepackage{portland,xspace} \usepackage{amsmath,amsxtra} \usepackage[OT2,OT1]{fontenc} \newcommand\cyr{ \renewcommand\rmdefault{wncyr} \renewcommand\sfdefault{wncyss} \renewcommand\encodingdefault{OT2} \normalfont \selectfont} \DeclareTextFontCommand{\textcyr}{\cyr} \pagestyle{empty} \DeclareMathSizes{10}{9}{7}{6} \begin{document} \landscape $b\, {}^{1}\Pi ^{+}_{u}( 4) $ \end{document} , \documentclass{aastex} \usepackage{amsbsy} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{bm} \usepackage{mathrsfs} \usepackage{pifont} \usepackage{stmaryrd} \usepackage{textcomp} \usepackage{portland,xspace} \usepackage{amsmath,amsxtra} \usepackage[OT2,OT1]{fontenc} \newcommand\cyr{ \renewcommand\rmdefault{wncyr} \renewcommand\sfdefault{wncyss} \renewcommand\encodingdefault{OT2} \normalfont \selectfont} \DeclareTextFontCommand{\textcyr}{\cyr} \pagestyle{empty} \DeclareMathSizes{10}{9}{7}{6} \begin{document} \landscape $b\, {}^{1}\Pi ^{+}_{u}( 5) $ \end{document} , and \documentclass{aastex} \usepackage{amsbsy} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{bm} \usepackage{mathrsfs} \usepackage{pifont} \usepackage{stmaryrd} \usepackage{textcomp} \usepackage{portland,xspace} \usepackage{amsmath,amsxtra} \usepackage[OT2,OT1]{fontenc} \newcommand\cyr{ \renewcommand\rmdefault{wncyr} \renewcommand\sfdefault{wncyss} \renewcommand\encodingdefault{OT2} \normalfont \selectfont} \DeclareTextFontCommand{\textcyr}{\cyr} \pagestyle{empty} \DeclareMathSizes{10}{9}{7}{6} \begin{document} \landscape $c_{3}\, {}^{1}\Pi ^{+}_{u}( 0) - X\, {}^{1}\Sigma ^{+}_{g}( 0) $ \end{document} Bands
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Published:2006-07-10
Issue:2
Volume:645
Page:1560-1567
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ISSN:0004-637X
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Container-title:The Astrophysical Journal
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language:en
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Short-container-title:ApJ
Author:
Liu Xianming,Shemansky Donald E.
Publisher
American Astronomical Society
Subject
Space and Planetary Science,Astronomy and Astrophysics
Cited by
12 articles.
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1. Opacities of <inline-formula><tex-math id="Z-20220715033133-1">\begin{document}${ X}^1\Sigma^+_{\rm g}, a'{}^1\Sigma^-_{\rm u}, a{}^1\Pi_{\rm g} \text{ and } { b}^1\Pi_{\rm u}$\end{document}</tex-math><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="14-20220043_Z-20220715033133-1.jpg"/><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="14-20220043_Z-20220715033133-1.png"/></alternatives></inline-formula> electronic states for nitrogen molecule;Acta Physica Sinica;2022
2. SPECTRA, EMISSION YIELDS, CROSS SECTIONS, AND KINETIC ENERGY DISTRIBUTIONS OF HYDROGEN ATOMS FROM H2${X}^{1}{{\rm{\Sigma }}}_{g}^{+}$–${d}^{3}{{\rm{\Pi }}}_{u}$ EXCITATION BY ELECTRON IMPACT;The Astrophysical Journal;2016-02-12
3. ABSORPTION OSCILLATOR STRENGTHS FOR THE c(4)(' 1)Sigma(+)(u)(3,4,6)-X-1 Sigma(+)(g)(nu ''), b(' 1)Sigma(+)(u)(10,13,20)-X-1 Sigma(+)(g)(nu ''), AND c(5)(' 1)Sigma(+)(u)(1)-X-1 Sigma(+)(g)(nu '') PROGRESSIONS IN N-2;ASTROPHYS J;2016
4. ABSORPTION OSCILLATOR STRENGTHS FOR THE ${{c}_{4}^{\prime }}^{1}{{\rm{\Sigma }}}_{{\rm{u}}}^{+}$(3, 4, 6)–${X}^{1}{{\rm{\Sigma }}}_{{\rm{g}}}^{+}(v^{\prime\prime} ),\;$ $b{^{\prime} }^{1}{{\rm{\Sigma }}}_{{\rm{u}}}^{+}$(10, 13, 20)–${X}^{1}{{\rm{\Sigma }}}_{{\rm{g}}}^{+}(v^{\prime\prime} ),$ AND ${{c}_{5}^{\prime }}^{1}{{\rm{\Sigma }}}_{{\rm{u}}}^{+}$(1)–${X}^{1}{{\rm{\Sigma }}}_{{\rm{g}}}^{+}(v^{\prime\prime} )$ PROGRESSIONS IN N2;The Astrophysical Journal;2016-01-05
5. THE HIGH-RESOLUTION EXTREME-ULTRAVIOLET SPECTRUM OF N
2
BY ELECTRON IMPACT;The Astrophysical Journal Supplement Series;2014-04-02