<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE dataset SYSTEM "http://tarantella.gsfc.nasa.gov/xml/dataset_048.dtd">
<dataset subject="astronomy" xmlns:xlink="http://www.w3.org/XML/XLink/0.9">
	<title>Luminous asymptotic giant branch stars in the Large Magellanic Cloud</title>
	<altname type="ADC">J/ApJ/348/98</altname>
		<altname type="CDS">J/ApJ/348/98</altname>
		<altname type="brief">LMC AGB stars IRAS fluxes</altname>
	<reference>
		<source>
<journal>
	<title>Luminous asymptotic giant branch stars in the Large Magellanic Cloud</title>
	<author>
			<initial>N</initial>
			<lastName>Reid</lastName></author>
	<author>
			<initial>C</initial>
			<lastName>Tinney</lastName></author>
	<author>
			<initial>J</initial>
			<lastName>Mould</lastName></author>
	<name>Astrophys. J.</name>
	<volume>348</volume>
	<pageno>98</pageno>
		<date>
			<year>1990</year></date>
	<bibcode>1990ApJ...348...98R</bibcode></journal></source></reference>
	<keywords parentListURL="http://messier.gsfc.nasa.gov/xml/keywordlists/adc_keywords.html">
			<keyword xlink:href="Infrared_sources.html">Infrared sources</keyword>
			<keyword xlink:href="Magellanic_Clouds.html">Magellanic Clouds</keyword>
			<keyword xlink:href="Stars_giant.html">Stars, giant</keyword></keywords>
	<keywords parentListURL="http://messier.gsfc.nasa.gov/xml/keywordlists/apj_keywords.html">
			<keyword xlink:href="galaxies_stellar_content.html">galaxies: stellar content</keyword>
			<keyword xlink:href="infrared_sources.html">infrared: sources</keyword>
			<keyword xlink:href="Magellanic_Clouds.html">Magellanic Clouds</keyword>
			<keyword xlink:href="stars_evolution.html">stars: evolution</keyword>
			<keyword xlink:href="stars_late-type.html">stars: late-type</keyword>
			<keyword xlink:href="stars_variables_other_(long-period_variables).html">stars: variables: other (long-period variables)</keyword></keywords>
	<descriptions>
				<abstract>
					<para>
    We present the results of a search for optically obscured asymptotic
    giant branch (AGB) stars in the Large Magellanic Cloud (LMC),
    combining data obtained using the IRAS satellite with near-infrared
    photographic plate material of a 15deg^2^ region in the northern LMC.
    Of the 156 IRAS sources that are detected either in separate
    cross-scans or in more than one passband, 63 have [12-25] colors
    consistent with their being either stellar photospheres or
    circumstellar dust shells. Seventeen of these we identify with bright
    (I_c_&lt;9) foreground stars in our own Galaxy, while a further 17 are
    associated with red supergiants in the LMC. Of the remaining stars, no
    more than five are likely to be optically visible AGB stars, while the
    rest have no obvious optical counterpart. This immediately rules out
    the presence of sufficient high-luminosity "cocoon" stars to explain
    the observed deficit of several hundred luminous (M_bol_&lt;-6) AGB
    stars between the predictions of standard models of AGB evolution and
    the observed luminosity function. It remains possible that most of
    the unidentified sources are dusty AGB stars, evolving through a
    phase of enhanced mass loss toward becoming planetary nebulae. We
    infer bolometric magnitudes as low as M_bol_~-5 for these sources and
    suggest that this phase can be triggered at low luminosities,
    truncating AGB evolution and leading to the observed scarcity of
    asymptotic giant branch stars with bolometric magnitudes brighter
    than -6.0mag.</para></abstract>
                        <details><para><observatory base="space"> IRAS</observatory></para></details></descriptions>
	<tableHead>
		<tableLinks>
				<tableLink xlink:href="table3">
	<title>TRM selected sources in LMC north</title></tableLink></tableLinks>
	<fields>
		<field>
			<name>TRM</name>
			<definition>TRM designation
	<footnote footnoteId="???"><para>number=1</para>
			<para>TRM (1990ApJ...348...98R) selected sources in the LMC north field.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>RAh</name>
			<definition>Right ascension (1950)</definition>
			<units>h</units></field>
		<field>
			<name>RAm</name>
			<definition>Right ascension (1950)</definition>
			<units>min</units></field>
		<field>
			<name>RAs</name>
			<definition>Right ascension (1950)</definition>
			<units>s</units></field>
		<field>
			<name>DE-</name>
			<definition>Declination sign</definition>
			<units>---</units></field>
		<field>
			<name>DEd</name>
			<definition>Declination (1950)</definition>
			<units>deg</units></field>
		<field>
			<name>DEm</name>
			<definition>Declination (1950)</definition>
			<units>arcmin</units></field>
		<field>
			<name>DEs</name>
			<definition>Declination (1950)</definition>
			<units>arcsec</units></field>
		<field>
			<name>Scan</name>
			<definition>Information on the scan directions
	<footnote footnoteId="???"><para>number=2</para>
			<para>Information on the scan directions in which each source was detected
           unambiguously is given.
            1: detected in EW scan
            2: detected in NS scan
            3: detected in both EW and NS scans</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>S12</name>
			<definition>Flux density at 12 {mu}m
	<footnote footnoteId="???"><para>number=3</para>
			<para>Fluxes listed in this table assume a flux distribution which varies
           as {nu}-1 (see Sec. IV).
          Blank entries in the S12, S25, S60, or S100 columns imply either that
           no flux was detected at that wavelength, or that the region was so
           confused that the source extraction algorithm was unable to extract
           any flux, or that the flux density measurement is not reliable.</para></footnote></definition>
			<units>Jy</units></field>
		<field>
			<name>S25</name>
			<definition>Flux density at 25 {mu}m
	<footnote footnoteId="???"><para>number=3</para>
			<para>Fluxes listed in this table assume a flux distribution which varies
           as {nu}-1 (see Sec. IV).
          Blank entries in the S12, S25, S60, or S100 columns imply either that
           no flux was detected at that wavelength, or that the region was so
           confused that the source extraction algorithm was unable to extract
           any flux, or that the flux density measurement is not reliable.</para></footnote></definition>
			<units>Jy</units></field>
		<field>
			<name>S60</name>
			<definition>Flux density at 60 {mu}m
	<footnote footnoteId="???"><para>number=3</para>
			<para>Fluxes listed in this table assume a flux distribution which varies
           as {nu}-1 (see Sec. IV).
          Blank entries in the S12, S25, S60, or S100 columns imply either that
           no flux was detected at that wavelength, or that the region was so
           confused that the source extraction algorithm was unable to extract
           any flux, or that the flux density measurement is not reliable.</para></footnote></definition>
			<units>Jy</units></field>
		<field>
			<name>S100</name>
			<definition>Flux density at 100 {mu}m
	<footnote footnoteId="???"><para>number=3</para>
			<para>Fluxes listed in this table assume a flux distribution which varies
           as {nu}-1 (see Sec. IV).
          Blank entries in the S12, S25, S60, or S100 columns imply either that
           no flux was detected at that wavelength, or that the region was so
           confused that the source extraction algorithm was unable to extract
           any flux, or that the flux density measurement is not reliable.</para></footnote></definition>
			<units>Jy</units></field>
		<field>
			<name>PSC</name>
			<definition>See note
	<footnote footnoteId="???"><para>number=4</para>
			<para>Sources marked with a "*" have been associated positionally with an
           object in the IRAS PSC</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>Rej</name>
			<definition>Rejection (Y: yes, N: no)</definition>
			<units>---</units></field>
		<field>
			<name>Com</name>
			<definition>Comments on rejection
	<footnote footnoteId="???"><para>number=6</para>
			<para>S100: Source was rejected because it had S100>S60>2S25.
          S60 Source was rejected because it had S60>2S25.
          S25>> S12 Source was rejected because it had S25>4S12.
          GC, C, NSO: Source was rejected because it coincided with a globular
            cluster, open cluster, or clearly nonstellar object on the V or I
            band Schmidt plates.
          PN: Source was rejected because it coincided with a planetary nebula
               (Sanduleak refs).
          H{alpha}: Source coincided with a knot of Half in the LMC
                     emission-line survey of Davies et al. (1976MmRAS..81...89D)
          (c), (u): Source extraction algorithm was unable to produce a
            meaningful flux estimate at that wavelength, due to either
            (c) source confusion or (u) unselected source; however, it is clear
            from the IRAS maps that there is sufficient 60 {mu}m or 100 {mu}m
            flux present to reject the source.
          1: TRM 147 showed some weak evidence fro 60 {mu}m flux which was not
              selected by IPAC source extractor. Since this source had a
              PSC 60 {mu}m flux greater than its 25 {mu}m flux, it was therefore
              rejected.
          The flux conditions were held to be stronger reasons for source
            rejection, so although a number of sources listed as being rejected
            on this basis were also coincident positionally with globular
            clusters, galaxies, etc., only the flux conditions has been listed
            here.
</para></footnote></definition>
			<units>---</units></field></fields></tableHead>
	
	<history>
		<ingest>
	
			<creator>
				<lastName>Patricia Bauer</lastName>
				<affiliation>CDS</affiliation></creator>
	<date>
		<year>1996</year><month>Sep</month><day>30</day></date></ingest>
		
		<revisions>
	<revision>
		<creator>
			<lastName>UNKNOWN</lastName></creator>
		<date><year>UNKNOWN</year></date>
		<para> Prepared via OCR at CDS.</para></revision></revisions></history>
	<identifier>J_ApJ_348_98.xml</identifier></dataset>
