Rotationally Broadened Synthetic Spectra forHSTandIUEObservations of Exposed White Dwarfs in Cataclysmic Variables1

In many dwarf novae during quiescence, the underlying white dwarf dominates the flux in the far ultraviolet. By observing these exposed degenerate stars with theHubble Space TelescopeGoddard High Resolution Spectrograph and Faint Object Spectrograph (HSTGHRS and FOS), the white‐dwarf rotation rates...

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Veröffentlicht in:Publications of the Astronomical Society of the Pacific 1998-01, Vol.110 (743), p.39-46
Hauptverfasser: Nguyen, Quyen, Fabian, Dirk, Belle, Kunegunda, Huang, M., Sion, E. M.
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container_end_page 46
container_issue 743
container_start_page 39
container_title Publications of the Astronomical Society of the Pacific
container_volume 110
creator Nguyen, Quyen
Fabian, Dirk
Belle, Kunegunda
Huang, M.
Sion, E. M.
description In many dwarf novae during quiescence, the underlying white dwarf dominates the flux in the far ultraviolet. By observing these exposed degenerate stars with theHubble Space TelescopeGoddard High Resolution Spectrograph and Faint Object Spectrograph (HSTGHRS and FOS), the white‐dwarf rotation rates can be determined or constrained by fitting synthetic spectra broadened by rotation. Using TLUSTY and SYNSPEC, we present a grid of rotationally broadened white‐dwarf synthetic spectra, convolved with the resolution of theHSTGHRS (G140L, G160M), FOS (G130H), andIUElow‐resolution short‐wavelength prime (SWP) spectra, computed for \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 $\mathrm{log}\,g=8$ \end{document} , solar composition, \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 $T_{\mathrm{eff}\,}=1$ \end{document} 5,000, 25,000, and 50,000 K, and rotational velocities of 0–5000 km s−1. We examine the predicted appearance of accreted solar‐composition white‐dwarf atmospheres in the context of determining or constraining the white‐dwarf rotational velocities. We present model grids that demonstrate this capability. We present the first application of these grids to the SWP low‐resolution spectra of the white dwarf in the nova‐like variable TT Ari, exposed during the very low brightness state of that system. We also rule out the possibility that the absence of Lyα absorption in many cataclysmic variables in quiescence (specifically those containing white dwarfs with \documentclass{aastex} \usepackage{amsbsy} \use
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By observing these exposed degenerate stars with theHubble Space TelescopeGoddard High Resolution Spectrograph and Faint Object Spectrograph (HSTGHRS and FOS), the white‐dwarf rotation rates can be determined or constrained by fitting synthetic spectra broadened by rotation. Using TLUSTY and SYNSPEC, we present a grid of rotationally broadened white‐dwarf synthetic spectra, convolved with the resolution of theHSTGHRS (G140L, G160M), FOS (G130H), andIUElow‐resolution short‐wavelength prime (SWP) spectra, computed for \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 $\mathrm{log}\,g=8$ \end{document} , solar composition, \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 $T_{\mathrm{eff}\,}=1$ \end{document} 5,000, 25,000, and 50,000 K, and rotational velocities of 0–5000 km s−1. We examine the predicted appearance of accreted solar‐composition white‐dwarf atmospheres in the context of determining or constraining the white‐dwarf rotational velocities. We present model grids that demonstrate this capability. We present the first application of these grids to the SWP low‐resolution spectra of the white dwarf in the nova‐like variable TT Ari, exposed during the very low brightness state of that system. We also rule out the possibility that the absence of Lyα absorption in many cataclysmic variables in quiescence (specifically those containing white dwarfs with \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 $T_{\mathrm{eff}\,}=1$ \end{document} 5,000–20,000 K) could be due to rotational velocities of the white dwarf near breakup.</description><identifier>ISSN: 0004-6280</identifier><identifier>EISSN: 1538-3873</identifier><identifier>DOI: 10.1086/316108</identifier><language>eng</language><publisher>The University of Chicago Press</publisher><subject>Absorption spectra ; Boundary layers ; Hemic system ; Rotational spectra ; Solar composition ; Solar rotation ; Solar spectra ; Spectral resolution ; Velocity ; White dwarfs</subject><ispartof>Publications of the Astronomical Society of the Pacific, 1998-01, Vol.110 (743), p.39-46</ispartof><rights>1998. Astronomical Society of the Pacific. All rights reserved. Printed in U.S.A.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,777,781,800,27905,27906</link.rule.ids></links><search><creatorcontrib>Nguyen, Quyen</creatorcontrib><creatorcontrib>Fabian, Dirk</creatorcontrib><creatorcontrib>Belle, Kunegunda</creatorcontrib><creatorcontrib>Huang, M.</creatorcontrib><creatorcontrib>Sion, E. M.</creatorcontrib><title>Rotationally Broadened Synthetic Spectra forHSTandIUEObservations of Exposed White Dwarfs in Cataclysmic Variables1</title><title>Publications of the Astronomical Society of the Pacific</title><description>In many dwarf novae during quiescence, the underlying white dwarf dominates the flux in the far ultraviolet. By observing these exposed degenerate stars with theHubble Space TelescopeGoddard High Resolution Spectrograph and Faint Object Spectrograph (HSTGHRS and FOS), the white‐dwarf rotation rates can be determined or constrained by fitting synthetic spectra broadened by rotation. Using TLUSTY and SYNSPEC, we present a grid of rotationally broadened white‐dwarf synthetic spectra, convolved with the resolution of theHSTGHRS (G140L, G160M), FOS (G130H), andIUElow‐resolution short‐wavelength prime (SWP) spectra, computed for \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 $\mathrm{log}\,g=8$ \end{document} , solar composition, \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 $T_{\mathrm{eff}\,}=1$ \end{document} 5,000, 25,000, and 50,000 K, and rotational velocities of 0–5000 km s−1. We examine the predicted appearance of accreted solar‐composition white‐dwarf atmospheres in the context of determining or constraining the white‐dwarf rotational velocities. We present model grids that demonstrate this capability. We present the first application of these grids to the SWP low‐resolution spectra of the white dwarf in the nova‐like variable TT Ari, exposed during the very low brightness state of that system. We also rule out the possibility that the absence of Lyα absorption in many cataclysmic variables in quiescence (specifically those containing white dwarfs with \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 $T_{\mathrm{eff}\,}=1$ \end{document} 5,000–20,000 K) could be due to rotational velocities of the white dwarf near breakup.</description><subject>Absorption spectra</subject><subject>Boundary layers</subject><subject>Hemic system</subject><subject>Rotational spectra</subject><subject>Solar composition</subject><subject>Solar rotation</subject><subject>Solar spectra</subject><subject>Spectral resolution</subject><subject>Velocity</subject><subject>White dwarfs</subject><issn>0004-6280</issn><issn>1538-3873</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1998</creationdate><recordtype>article</recordtype><sourceid/><recordid>eNqNj8tOwzAQRS0EEuH1DZZYB2YwBK8pQWWFRAoso2niqK5cO5qxgPw94fEBrM7mnisdpc4QLhBsdWmwmrmnCrwxtjT21uyrAgCuy-rKwqE6EtkCIFqEQslzypR9ihTCpO84Ue-i63Uzxbxx2Xe6GV2XmfSQeNmsKPaPL_XTWhy__3ii06DrzzHJbL1tfHb6_oN4EO2jXlCmLkyym39eiT2tgxM8UQcDBXGnfzxW5w_1arEst5ITtyP7HfHUIrTfPe1vj_nf6gvUkk7o</recordid><startdate>199801</startdate><enddate>199801</enddate><creator>Nguyen, Quyen</creator><creator>Fabian, Dirk</creator><creator>Belle, Kunegunda</creator><creator>Huang, M.</creator><creator>Sion, E. M.</creator><general>The University of Chicago Press</general><scope/></search><sort><creationdate>199801</creationdate><title>Rotationally Broadened Synthetic Spectra forHSTandIUEObservations of Exposed White Dwarfs in Cataclysmic Variables1</title><author>Nguyen, Quyen ; Fabian, Dirk ; Belle, Kunegunda ; Huang, M. ; Sion, E. M.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-jstor_primary_10_1086_3161083</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1998</creationdate><topic>Absorption spectra</topic><topic>Boundary layers</topic><topic>Hemic system</topic><topic>Rotational spectra</topic><topic>Solar composition</topic><topic>Solar rotation</topic><topic>Solar spectra</topic><topic>Spectral resolution</topic><topic>Velocity</topic><topic>White dwarfs</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Nguyen, Quyen</creatorcontrib><creatorcontrib>Fabian, Dirk</creatorcontrib><creatorcontrib>Belle, Kunegunda</creatorcontrib><creatorcontrib>Huang, M.</creatorcontrib><creatorcontrib>Sion, E. M.</creatorcontrib><jtitle>Publications of the Astronomical Society of the Pacific</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Nguyen, Quyen</au><au>Fabian, Dirk</au><au>Belle, Kunegunda</au><au>Huang, M.</au><au>Sion, E. M.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Rotationally Broadened Synthetic Spectra forHSTandIUEObservations of Exposed White Dwarfs in Cataclysmic Variables1</atitle><jtitle>Publications of the Astronomical Society of the Pacific</jtitle><date>1998-01</date><risdate>1998</risdate><volume>110</volume><issue>743</issue><spage>39</spage><epage>46</epage><pages>39-46</pages><issn>0004-6280</issn><eissn>1538-3873</eissn><abstract>In many dwarf novae during quiescence, the underlying white dwarf dominates the flux in the far ultraviolet. By observing these exposed degenerate stars with theHubble Space TelescopeGoddard High Resolution Spectrograph and Faint Object Spectrograph (HSTGHRS and FOS), the white‐dwarf rotation rates can be determined or constrained by fitting synthetic spectra broadened by rotation. Using TLUSTY and SYNSPEC, we present a grid of rotationally broadened white‐dwarf synthetic spectra, convolved with the resolution of theHSTGHRS (G140L, G160M), FOS (G130H), andIUElow‐resolution short‐wavelength prime (SWP) spectra, computed for \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 $\mathrm{log}\,g=8$ \end{document} , solar composition, \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 $T_{\mathrm{eff}\,}=1$ \end{document} 5,000, 25,000, and 50,000 K, and rotational velocities of 0–5000 km s−1. We examine the predicted appearance of accreted solar‐composition white‐dwarf atmospheres in the context of determining or constraining the white‐dwarf rotational velocities. We present model grids that demonstrate this capability. We present the first application of these grids to the SWP low‐resolution spectra of the white dwarf in the nova‐like variable TT Ari, exposed during the very low brightness state of that system. We also rule out the possibility that the absence of Lyα absorption in many cataclysmic variables in quiescence (specifically those containing white dwarfs with \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 $T_{\mathrm{eff}\,}=1$ \end{document} 5,000–20,000 K) could be due to rotational velocities of the white dwarf near breakup.</abstract><pub>The University of Chicago Press</pub><doi>10.1086/316108</doi></addata></record>
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source IOP Publishing Journals; Elektronische Zeitschriftenbibliothek - Frei zugängliche E-Journals; Jstor Complete Legacy; Institute of Physics (IOP) Journals - HEAL-Link; Alma/SFX Local Collection
subjects Absorption spectra
Boundary layers
Hemic system
Rotational spectra
Solar composition
Solar rotation
Solar spectra
Spectral resolution
Velocity
White dwarfs
title Rotationally Broadened Synthetic Spectra forHSTandIUEObservations of Exposed White Dwarfs in Cataclysmic Variables1
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