<?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>X-ray studies of coeval star samples. III. X-ray emission in the Ursa Major
stream.</title>
	<altname type="ADC">J/ApJ/351/492</altname>
		<altname type="CDS">J/ApJ/351/492</altname>
		<altname type="brief">X-ray emission in the Ursa Major stream.</altname>
	<reference>
		<source>
<journal>
	<title>X-ray studies of coeval star samples. III. X-ray emission in the Ursa Major
stream.</title>
	<author>
			<initial>J</initial>
			<initial>H</initial>
			<initial>M</initial>
			<initial>M</initial>
			<lastName>Schmitt</lastName></author>
	<author>
			<initial>G</initial>
			<lastName>Micela</lastName></author>
	<author>
			<initial>S</initial>
			<lastName>Sciortino</lastName></author>
	<author>
			<initial>G</initial>
			<initial>S</initial>
			<lastName>Vaiana</lastName></author>
	<author>
			<initial>F</initial>
			<initial>R</initial>
			<lastName>Harnden</lastName></author>
	<author>
			<initial>R</initial>
			<lastName>Rosner</lastName></author>
	<name>Astrophys. J.</name>
	<volume>351</volume>
	<pageno>492</pageno>
		<date>
			<year>1990</year></date>
	<bibcode>1990ApJ...351..492S</bibcode></journal></source>
	<related>
			<holding role="similar">J/ApJ/315/687  X-Ray emission from solar-type stars :  F and G
   J/ApJ/348/253  Einstein Survey of Late-type Giant and Supergiant Stars
   J/ApJ/325/798  Einstein Survey of Hyades-cluster Region
   J/ApJ/348/557  Einstein Survey of the Pleiades Cluster<xlink:simple href="J/ApJ/315/687  X-Ray emission from solar-type stars"/></holding>
			  Harnden, F.R., Jr., Fabricant, D.G., Harris, D.E., and Schwarz, J.  1984,
     Smithsonian Ap. Obs. Spec. Rept., No. 393.</related></reference>
	<keywords parentListURL="http://messier.gsfc.nasa.gov/xml/keywordlists/adc_keywords.html">
			<keyword xlink:href="Clusters_open.html">Clusters, open</keyword>
			<keyword xlink:href="Stars_emission.html">Stars, emission</keyword>
			<keyword xlink:href="X-ray_sources.html">X-ray sources</keyword></keywords>
	<keywords parentListURL="http://messier.gsfc.nasa.gov/xml/keywordlists/apj_keywords.html">
			<keyword xlink:href="open_clusters_and_associations_general.html">open clusters and associations: general</keyword>
			<keyword xlink:href="stars_rotation.html">stars: rotation</keyword>
			<keyword xlink:href="X-rays_stars.html">X-rays: stars</keyword></keywords>
	<descriptions>
				<abstract>
					<para>
    Results are  reported from  a comprehensive  survey of  X-ray emission
    from  stars known or suspected to be members of the UMa cluster and/or
    stream. Of the 42 UMa member stars surveyed, 18 were detected as X-ray
    sources,  and spectral  analysis  was  performed  for  10  stars  with
    sufficient  X-ray counts.  Consideration is given to relations between
    X-ray luminosity, color,  and kinematics of the sample stars,  and the
    X-ray  spectra of the  UMa stars are  discussed in the  context of the
    general  problem of stellar X-ray temperatures.  Also confirmed is the
    lack of X-ray-emitting  A dwarfs  among UMa  members;  among  stars of
    later spectral type there  is  a  rather  large  dispersion  in  X-ray
    luminosity.   This  dispersion  cannot   readily   be   explained   by
    contamination  with field star interlopers and  appears rather to be a
    property of the UMa X-ray luminosity distribution function.</para></abstract>
                        <details><para><observatory base="space"> Einstein</observatory></para></details></descriptions>
	<tableHead>
		<tableLinks>
				<tableLink xlink:href="st_uma_1.dat">
	<title>X-ray Emssion in the Ursa Major Stream:
                              X-ray Results and Optical Properties</title></tableLink></tableLinks>
	<fields>
		<field>
			<name>HR</name>
			<definition>HR (Bright Star Catalog) number
	<footnote footnoteId="???"><para>number=1</para>
			<para>These columns give the HR (Bright Star Catalog) and HD (Henry
    Draper Catalog) numbers of the sample star.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>HD</name>
			<definition>HD (Henry Draper Catalog) number
	<footnote footnoteId="???"><para>number=1</para>
			<para>These columns give the HR (Bright Star Catalog) and HD (Henry
    Draper Catalog) numbers of the sample star.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>inst</name>
			<definition>Instrument
	<footnote footnoteId="???"><para>number=2</para>
			<para>These columns give the instrument used and the sequence number of
    the observation. Listed in the instrument column will be an "I" if the
    Imaging Proportional Counter  (IPC)  was  used,  an  "H"  if  the High
    Resolution  Imager (HRI)  was used,  or an  "EXO"  if the data is from
    EXOSAT.  The Einstein  sequence number is  a two to  five digit number
    which  uniquely identifies the observation.  The numbers were assigned
    sequentially at the time of proposal submission. In most cases we used
    IPC data, for a few stars the HRI was used, and in one case the EXOSAT
    Low Energy experiment was used.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>Seqno</name>
			<definition>Sequence Number
	<footnote footnoteId="???"><para>number=2</para>
			<para>These columns give the instrument used and the sequence number of
    the observation. Listed in the instrument column will be an "I" if the
    Imaging Proportional Counter  (IPC)  was  used,  an  "H"  if  the High
    Resolution  Imager (HRI)  was used,  or an  "EXO"  if the data is from
    EXOSAT.  The Einstein  sequence number is  a two to  five digit number
    which  uniquely identifies the observation.  The numbers were assigned
    sequentially at the time of proposal submission. In most cases we used
    IPC data, for a few stars the HRI was used, and in one case the EXOSAT
    Low Energy experiment was used.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>f_CCR</name>
			<definition>Flagged "1" if count rate is an upper limit
	<footnote footnoteId="???"><para>number=3</para>
			<para>The "f_CCR" column is marked with a "1" if the corrected count
    rate is  an upper limit.  The "CCR"   column gives the corrected count
    rate (per 1000 seconds). For detections, the "f_CCR"  column is marked
    with a "0", and the 1 sigma error is given in the "e_CCR" column.  For
    upper limits, the value given is a 3 sigma upper limit,  and the error
    is given as zero. Count rate is corrected for scattering,  vignetting,
    and detector dead time.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>CCR</name>
			<definition>Corrected Count Rate
	<footnote footnoteId="???"><para>number=3</para>
			<para>The "f_CCR" column is marked with a "1" if the corrected count
    rate is  an upper limit.  The "CCR"   column gives the corrected count
    rate (per 1000 seconds). For detections, the "f_CCR"  column is marked
    with a "0", and the 1 sigma error is given in the "e_CCR" column.  For
    upper limits, the value given is a 3 sigma upper limit,  and the error
    is given as zero. Count rate is corrected for scattering,  vignetting,
    and detector dead time.</para></footnote></definition>
			<units>ct/ks</units></field>
		<field>
			<name>e_CCR</name>
			<definition>Error on count rate
	<footnote footnoteId="???"><para>number=3</para>
			<para>The "f_CCR" column is marked with a "1" if the corrected count
    rate is  an upper limit.  The "CCR"   column gives the corrected count
    rate (per 1000 seconds). For detections, the "f_CCR"  column is marked
    with a "0", and the 1 sigma error is given in the "e_CCR" column.  For
    upper limits, the value given is a 3 sigma upper limit,  and the error
    is given as zero. Count rate is corrected for scattering,  vignetting,
    and detector dead time.</para></footnote></definition>
			<units>ct/ks</units></field>
		<field>
			<name>method</name>
			<definition>Detect method
	<footnote footnoteId="???"><para>number=4</para>
			<para>This column marks what kind of detect algorithm was used to
    locate the source; an "M" indicates MDETECT, an "L"  indicates LDETECT
    (see Harnden,  et al.   1984).  This  pertains only  to the  IPC data.
    Sources detected with other detectors contain a "." in this column.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>logLx</name>
			<definition>Log of X-ray luminosity from 0.16-4.0 keV
	<footnote footnoteId="???"><para>number=5</para>
			<para>This column gives the log of the X-ray luminosity (in erg/s) in
    the 0.16-4.0  keV passband,  computed  with the distance  given in the
    table st_uma_2.dat  .  When  the count  rate is  an upper  limit,  the
    luminosity is also an upper limit.  For the conversion from count rate
    to  fluxes,   we   used  the   "standard"   conversion   of  2x10^-11^
    erg/cm^2^/count.</para></footnote></definition>
			<units>[10-7W]</units></field>
		<field>
			<name>note</name>
			<definition>Notes on the source
	<footnote footnoteId="???"><para>number=6</para>
			<para>This column contains notes on individual sources. The following
    notes are used:

      a:  HR 1971: observed with Ribs and Edges COde (RECO; see text) 1008
      b:  HR 5328/29: not separated by IPC; observed with RECO  200
      c:  HR 5727/28: not separated by IPC
      d:  HR 8207: observed with RECO 1006
      e:  HR 8410: observed with RECO 400</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>RAh</name>
			<definition>Right Ascension (B1950) (hour)</definition>
			<units>h</units></field>
		<field>
			<name>RAm</name>
			<definition>Right Ascension (B1950) (min)</definition>
			<units>min</units></field>
		<field>
			<name>RAs</name>
			<definition>Right Ascension (B1950) (sec)</definition>
			<units>s</units></field>
		<field>
			<name>DE-</name>
			<definition>Declination sign (B1950)</definition>
			<units>---</units></field>
		<field>
			<name>DEd</name>
			<definition>Declination (B1950) (deg)</definition>
			<units>deg</units></field>
		<field>
			<name>DEm</name>
			<definition>Declination (B1950) (arcmin)</definition>
			<units>arcmin</units></field>
		<field>
			<name>DEs</name>
			<definition>Declination (B1950) (arcsec)</definition>
			<units>arcsec</units></field>
		<field>
			<name>Dist</name>
			<definition>Distance to star
	<footnote footnoteId="???"><para>number=7</para>
			<para>In these columns, we give the adopted distance, the B-V color
    index, and the spectral type.</para></footnote></definition>
			<units>pc</units></field>
		<field>
			<name>B-V</name>
			<definition>B-V color index
	<footnote footnoteId="???"><para>number=7</para>
			<para>In these columns, we give the adopted distance, the B-V color
    index, and the spectral type.</para></footnote></definition>
			<units>mag</units></field>
		<field>
			<name>Sp</name>
			<definition>Spectral type
	<footnote footnoteId="???"><para>number=7</para>
			<para>In these columns, we give the adopted distance, the B-V color
    index, and the spectral type.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>U</name>
			<definition>U velocity
	<footnote footnoteId="???"><para>number=8</para>
			<para>The space velocities, U, V, and W are given (in km/s) in the
    first  three columns listed here.  Note that we are using a coordinate
    system with  the positive U-axis pointing  toward the Galactic center.
    In  the "Rho"  column,  we give the modulus of the velocity difference
    between  the   star  and  the  cluster   nucleus  adopted  from  Eggen
    (1983AJ.....88..642E) to be U(nuc)= 13.9 km/s, V(nuc)=  1.5 km/s,  and
    W(nuc)= -9.4 km/s.
</para></footnote></definition>
			<units>km/s</units></field>
		<field>
			<name>V</name>
			<definition>V velocity
	<footnote footnoteId="???"><para>number=8</para>
			<para>The space velocities, U, V, and W are given (in km/s) in the
    first  three columns listed here.  Note that we are using a coordinate
    system with  the positive U-axis pointing  toward the Galactic center.
    In  the "Rho"  column,  we give the modulus of the velocity difference
    between  the   star  and  the  cluster   nucleus  adopted  from  Eggen
    (1983AJ.....88..642E) to be U(nuc)= 13.9 km/s, V(nuc)=  1.5 km/s,  and
    W(nuc)= -9.4 km/s.
</para></footnote></definition>
			<units>km/s</units></field>
		<field>
			<name>W</name>
			<definition>W velocity
	<footnote footnoteId="???"><para>number=8</para>
			<para>The space velocities, U, V, and W are given (in km/s) in the
    first  three columns listed here.  Note that we are using a coordinate
    system with  the positive U-axis pointing  toward the Galactic center.
    In  the "Rho"  column,  we give the modulus of the velocity difference
    between  the   star  and  the  cluster   nucleus  adopted  from  Eggen
    (1983AJ.....88..642E) to be U(nuc)= 13.9 km/s, V(nuc)=  1.5 km/s,  and
    W(nuc)= -9.4 km/s.
</para></footnote></definition>
			<units>km/s</units></field>
		<field>
			<name>Rho</name>
			<definition>Velocity
	<footnote footnoteId="???"><para>number=8</para>
			<para>The space velocities, U, V, and W are given (in km/s) in the
    first  three columns listed here.  Note that we are using a coordinate
    system with  the positive U-axis pointing  toward the Galactic center.
    In  the "Rho"  column,  we give the modulus of the velocity difference
    between  the   star  and  the  cluster   nucleus  adopted  from  Eggen
    (1983AJ.....88..642E) to be U(nuc)= 13.9 km/s, V(nuc)=  1.5 km/s,  and
    W(nuc)= -9.4 km/s.
</para></footnote></definition>
			<units>km/s</units></field></fields></tableHead>
	<tableHead>
		<tableLinks>
				<tableLink xlink:href="st_uma_3.dat">
	<title>X-ray Emission in the Ursa Major Stream:
                              Temperature Fits</title></tableLink></tableLinks>
	<fields>
		<field>
			<name>HD</name>
			<definition>HD (Henry Draper Catalog) number
	<footnote footnoteId="???"><para>number=1</para>
			<para>The HD (Henry Draper Catalog) number of the sample star is given
    in this column.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>Seqno</name>
			<definition>Sequence number
	<footnote footnoteId="???"><para>number=2</para>
			<para>This column gives the Einstein sequence number, a two to five
    digit number which  uniquely  identifies  the  observation.   Sequence
    numbers were assigned sequentially at the time of proposal submission.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>ntemps</name>
			<definition>Number of temperature components in fit
	<footnote footnoteId="???"><para>number=3</para>
			<para>This column gives the number of temperature components which were
    used in the spectral analysis.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>logT1</name>
			<definition>log T for low-temperature component
	<footnote footnoteId="???"><para>number=4</para>
			<para>These columns give the best-fit single temperature for each
    component (logT1 and logT2), along with the one sigma (68% confidence)
    errors.   For fits which had only one component,  the second component
    entries will be zero.</para></footnote></definition>
			<units>[K]</units></field>
		<field>
			<name>e_logT1</name>
			<definition>Downward 68% confidence error
	<footnote footnoteId="???"><para>number=4</para>
			<para>These columns give the best-fit single temperature for each
    component (logT1 and logT2), along with the one sigma (68% confidence)
    errors.   For fits which had only one component,  the second component
    entries will be zero.</para></footnote></definition>
			<units>[K]</units></field>
		<field>
			<name>E_logT1</name>
			<definition>Upward 68% confidence error
	<footnote footnoteId="???"><para>number=4</para>
			<para>These columns give the best-fit single temperature for each
    component (logT1 and logT2), along with the one sigma (68% confidence)
    errors.   For fits which had only one component,  the second component
    entries will be zero.</para></footnote></definition>
			<units>[K]</units></field>
		<field>
			<name>logT2</name>
			<definition>log T for high-temperature component
	<footnote footnoteId="???"><para>number=4</para>
			<para>These columns give the best-fit single temperature for each
    component (logT1 and logT2), along with the one sigma (68% confidence)
    errors.   For fits which had only one component,  the second component
    entries will be zero.</para></footnote></definition>
			<units>[K]</units></field>
		<field>
			<name>e_logT2</name>
			<definition>Downward 68% confidence error
	<footnote footnoteId="???"><para>number=4</para>
			<para>These columns give the best-fit single temperature for each
    component (logT1 and logT2), along with the one sigma (68% confidence)
    errors.   For fits which had only one component,  the second component
    entries will be zero.</para></footnote></definition>
			<units>[K]</units></field>
		<field>
			<name>E_logT2</name>
			<definition>Upward 68% confidence error
	<footnote footnoteId="???"><para>number=4</para>
			<para>These columns give the best-fit single temperature for each
    component (logT1 and logT2), along with the one sigma (68% confidence)
    errors.   For fits which had only one component,  the second component
    entries will be zero.</para></footnote></definition>
			<units>[K]</units></field>
		<field>
			<name>chi2</name>
			<definition>Reduced chi-square
	<footnote footnoteId="???"><para>number=5</para>
			<para>This column gives the reduced chi-squared of the temperature fit.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>em1d2</name>
			<definition>Emission measure
	<footnote footnoteId="???"><para>number=6</para>
			<para>These columns give the derived emission measure (in units of
    10^49^  cm^-3^  pc^-2^)  of the best-fit spectrum.  For fits which had
    only one component, the entry for the second component will be zero.</para></footnote></definition>
			<units>10+49/cm3/pc2</units></field>
		<field>
			<name>em2d2</name>
			<definition>Emission measure
	<footnote footnoteId="???"><para>number=6</para>
			<para>These columns give the derived emission measure (in units of
    10^49^  cm^-3^  pc^-2^)  of the best-fit spectrum.  For fits which had
    only one component, the entry for the second component will be zero.</para></footnote></definition>
			<units>10+49/cm3/pc2</units></field>
		<field>
			<name>logLx1</name>
			<definition>log X-ray luminosity from 0.16-4.0 keV
	<footnote footnoteId="???"><para>number=7</para>
			<para>These columns give the log of the inferred X-ray luminosity (with
    the  distance as given in st_uma_1.dat)  in ergs/s in the 0.16-4.0 keV
    passband.  For  fits which had only one  component,  the entry for the
    second component will be zero
</para></footnote></definition>
			<units>[10-7W]</units></field>
		<field>
			<name>logLx2</name>
			<definition>log X-ray luminosity from 0.16-4.0 keV
	<footnote footnoteId="???"><para>number=7</para>
			<para>These columns give the log of the inferred X-ray luminosity (with
    the  distance as given in st_uma_1.dat)  in ergs/s in the 0.16-4.0 keV
    passband.  For  fits which had only one  component,  the entry for the
    second component will be zero
</para></footnote></definition>
			<units>[10-7W]</units></field></fields></tableHead>
	
	<history>
		<ingest>
	
			<creator>
				<lastName>Patricio Ortiz</lastName>
				<affiliation>CDS</affiliation></creator>
	<date>
		<year>1999</year><month>Apr</month><day>07</day></date></ingest>
		
		<revisions>
	<revision>
		<creator>
			<lastName>UNKNOWN</lastName></creator>
		<date><year>UNKNOWN</year></date>
		<para>    Prepared from the tables available at the "ADS Catalogue Service"
    (CfA, Harvard-Smithsonian Center for Astrophysics, Cambrigde MA)</para></revision></revisions></history>
	<identifier>J_ApJ_351_492.xml</identifier></dataset>
