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
نویسندگان
چکیده
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ژورنال
عنوان ژورنال: The Astrophysical Journal
سال: 2016
ISSN: 1538-4357
DOI: 10.3847/0004-637x/816/2/58