<?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>Structures, spectral indexes, and optical identifications of radio sources
selected from the B3 catalogue.</title>
	<altname type="ADC">J/AJ/98/419</altname>
		<altname type="CDS">J/AJ/98/419</altname>
		<altname type="brief">Observed quantities from B3 sources</altname>
	<reference>
		<source>
<journal>
	<title>Structures, spectral indexes, and optical identifications of radio sources
selected from the B3 catalogue.</title>
	<author>
			<initial>M</initial>
			<lastName>Vigotti</lastName></author>
	<author>
			<initial>G</initial>
			<lastName>Grueff</lastName></author>
	<author>
			<initial>R</initial>
			<lastName>Perley</lastName></author>
	<author>
			<initial>B</initial>
			<initial>G</initial>
			<lastName>Clark</lastName></author>
	<author>
			<initial>A</initial>
			<initial>H</initial>
			<lastName>Bridle</lastName></author>
	<name>Astron. J.</name>
	<volume>98</volume>
	<pageno>419</pageno>
		<date>
			<year>1989</year></date>
	<bibcode>1989AJ.....98..419V</bibcode></journal></source>
	<related>
			<holding role="similar">VIII/37 : The Third Bologna Survey (B3)<xlink:simple href="VIII/37"/></holding>
			  Kron, 1986, Private communication</related></reference>
	<keywords parentListURL="http://messier.gsfc.nasa.gov/xml/keywordlists/adc_keywords.html">
			<keyword xlink:href="Radio_sources.html">Radio sources</keyword></keywords>
	<descriptions>
				<description>
				<para>
    This  catalog   contains  results  of  a   large  program  of  optical
    identifications  of radio sources from the Third Bologna (B3)  Catalog
    (Ficarra et al.,  1985A&amp;AS...59..255F,  Cat.&lt;VIII/37>).  A homogeneous
    sample of 1103 radio sources,  selected from the B3 catalog at 408 MHz
    and covering a flux density range from 2.0 to 0.1 Jy,  has been mapped
    at 1465  MHz using  the VLA  at 15"  resolution.  Both  positional and
    structural information  have been  derived  and  are  presented  here.
    Optical identifications  have been  attempted for  all of  the sources
    within the  range of right  ascension studied,  using  the Palomar Sky
    Survey prints, resulting in 354 proposed identifications. The RA range
    was restricted to exclude sky areas at low galactic latitude,  because
    obscuration makes  these unsuitable for  optical identifications,  and
    confusion  makes  them unsuitable for  VLA snapshot-mode observations.
    Thus the samples  were selected  only from  the RA  intervals  23h-3h,
    7h-15h.  The number of rows of this  table (1474)  is larger  than the
    number of  sources (1103)  because each  radio component  of  multiple
    sources is listed as a separate line.</para></description>
                        <details/></descriptions>
	<tableHead>
		<tableLinks>
				<tableLink xlink:href="b3id.dat">
	<title>Optical Identifications of B3 Radio Sources
                                 (37{deg}..Dec..47{deg})</title></tableLink></tableLinks>
	<fields>
		<field>
			<name>Name</name>
			<definition>Name of source
	<footnote footnoteId="???"><para>number=1</para>
			<para>The IAU name is given in the name column. This was not given in
          the B3 Catalogue, and was obtained from the B3 position (hours,
          minutes, degrees, and tenths of degrees) adding a letter (a, b,
          etc.) in order of right ascension, in case of ambiguity. Note
          that this designation does not always match the new VLA position,
          although this happens rarely. In the case of physically connected
          multiple sources, a single name is given if they correspond to a
          single source in the B3 Catalogue; however, some sources listed
          separately in B3 happen to be parts of the same source
          (e.g. 0050+401, 0050+403, and 0050+402B) and in this case they
          retain their individual B3 names.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>Oname</name>
			<definition>3C or 4C name of source
	<footnote footnoteId="???"><para>number=2</para>
			<para>The othername column gives the 4C name. If the source is also in
          the 3CR Catalogue, the 3CR name is given instead. 3CR names are
          recognizable by the format (integer number, or at most one
          decimal digit), while 4C names are in the DD.NN format.
          Identification with a 4C source is sometimes ambiguous, as
          discussed in the B3 Catalogue.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>Sample</name>
			<definition>Number of B3 sample which contained source
	<footnote footnoteId="???"><para>number=3</para>
			<para>This column indicates the source parent subsample. This number
          indicates inclusion in the sample as originally selected; for
          example, the physical double 0218+399(A+B) is listed as

              0218+399A    1
              0218+399B    2

          since the respective B3 flux densities are 0.36 and 0.49 Jy, and
          the components were originally selected as parts of two different
          samples. The VLA map showed them to be part of the same source;
          consequently the total 408 MHz flux density is now listed as 0.85
          Jy (S408 column) and in any subsequent analysis the source will
          be considered part of sample 3, 0.8..S..1.6 Jy.
          Another example is given by the following double source
          0218+402(A+B); only one component (A) was originally included in
          sample 2 (although both components are separately listed in B3)
          since component B did not meet the selection criteria as given in
          the published paper. See the paper for full details.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>RAh</name>
			<definition>Right Ascension (B1950) (hour)
	<footnote footnoteId="???"><para>number=4</para>
			<para>These columns give the B1950 position of the source (or
          component). When no source component was detected with the VLA,
          the f_S1465 column is marked with an '-' and the given position
          is from B3 (Ficarra et al. 1985A&amp;AS...59..255F).</para></footnote></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)
	<footnote footnoteId="???"><para>number=4</para>
			<para>These columns give the B1950 position of the source (or
          component). When no source component was detected with the VLA,
          the f_S1465 column is marked with an '-' and the given position
          is from B3 (Ficarra et al. 1985A&amp;AS...59..255F).</para></footnote></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>f_S1465</name>
			<definition>Flagged if flux is integrated or
                                     upper limit
	<footnote footnoteId="???"><para>number=5</para>
			<para>The f_S1465 column is marked with a "+" if the source
          (component) was resolved, and an integrated flux density is
          given. A '-' in the f_S1465 column indicates that the source
          component was not detected with the VLA and the given flux is an
          upper limit. For these sources, the listed position is from B3.
          The S1465 columns gives the source (or component) flux density at
          1465 MHz in mJy.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>S1465</name>
			<definition>Flux density at 1465 MHz in mJy
	<footnote footnoteId="???"><para>number=5</para>
			<para>The f_S1465 column is marked with a "+" if the source
          (component) was resolved, and an integrated flux density is
          given. A '-' in the f_S1465 column indicates that the source
          component was not detected with the VLA and the given flux is an
          upper limit. For these sources, the listed position is from B3.
          The S1465 columns gives the source (or component) flux density at
          1465 MHz in mJy.</para></footnote></definition>
			<units>mJy</units></field>
		<field>
			<name>MType</name>
			<definition>Morphological classification of source
	<footnote footnoteId="???"><para>number=6</para>
			<para>This column gives a simple morphological classification of the
          radio structure, as follows:

           U   unresolved, the synthesized beam is not appreciably broadened.
           R   resolved, only one emission peak is present, but the source map
                 or 'response' is wider than the antenna beam.
           D   double source, two emission peaks are present and they appear
                 to be physically related.
           T   triple source, three peaks present and possibly related.

          The morphological classification is followed by the source's
          largest angular size (LAS), measured in arcseconds. U implies an
          (average) upper limit of 5 arcsec; R sources were given a size by
          measuring the largest HPBW, and deconvolving it with the antenna
          beam; for D and T sources the separation between the (outermost)
          components is given.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>S408</name>
			<definition>Flux density at 408 MHz in Jy
	<footnote footnoteId="???"><para>number=7</para>
			<para>This column gives the total 408 MHz flux density in Jy; generally
          it is taken from B3, but for extended, strong sources it has been
          remeasured integrating from the B3 map on the structure revealed
          by the VLA data.</para></footnote></definition>
			<units>Jy</units></field>
		<field>
			<name>Sp+Index</name>
			<definition>Spectral index between 1465 and 408 MHz
	<footnote footnoteId="???"><para>number=8</para>
			<para>This column gives the spectral index, computed between 1465 and
          408 MHz. For multiple sources, the 1465 MHz flux densities have
          been added. Alpha is defined in the sense S {prop.to} nu^(alpha)^.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>ID</name>
			<definition>Proposed source identification (type)
	<footnote footnoteId="???"><para>number=9</para>
			<para>This column gives the proposed optical identification, as
          follows:

          G   galaxy
          B   starlike, blue object
          N   starlike object of neutral color

          Note that the optical identification for multiple sources (e.g.
          type D or T) is ONLY given for the FIRST listed component, and
          omitted for all others.

          A question mark indicates an uncertain optical classification, it
          does *not* necessarily indicate an uncertain identification. An
          asterisk preceding the optical classification indicates that the
          identification was accepted even if it does not meet a uniform
          criterion of positional agreement (see the paper for details).
          Note that this column is three characters, with the optical
          identification being the second character. Thus, to search for
          all galaxies, one must search for all sources with a 'G' in this
          column</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>f_z</name>
			<definition>'*' if redshift is from the literature
	<footnote footnoteId="???"><para>number=10</para>
			<para>For galaxies, the redshift is given in the z column. If a
          spectroscopic redshift is available in the literature, the f_z
          column is marked with an asterisk (*). In this case the reference
          given in the ref column is to the redshift measurement. To
          estimate redshifts for those not available in the literature, the
          image size was measured and from it the redshift was inferred,
          following an established procedure for radio galaxies (Sandage
          (1972ApJ...178...25S); Grueff and Vigotti 1979A&amp;AS...35..371G).
          The method has been recalibrated using spectroscopic redshifts
          available for 33 radio galaxies in our sample. Some of these are
          available in the literature, and many were measured by Kron
          (1986) as an optical follow-up of this program.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>z</name>
			<definition>Estimated or measured redshift
	<footnote footnoteId="???"><para>number=10</para>
			<para>For galaxies, the redshift is given in the z column. If a
          spectroscopic redshift is available in the literature, the f_z
          column is marked with an asterisk (*). In this case the reference
          given in the ref column is to the redshift measurement. To
          estimate redshifts for those not available in the literature, the
          image size was measured and from it the redshift was inferred,
          following an established procedure for radio galaxies (Sandage
          (1972ApJ...178...25S); Grueff and Vigotti 1979A&amp;AS...35..371G).
          The method has been recalibrated using spectroscopic redshifts
          available for 33 radio galaxies in our sample. Some of these are
          available in the literature, and many were measured by Kron
          (1986) as an optical follow-up of this program.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>Rmag</name>
			<definition>Red magnitude
	<footnote footnoteId="???"><para>number=11</para>
			<para>For N and B objects, the red magnitude is given, except for some
          B objects, whose spectroscopic redshift from the literature is
          given.</para></footnote></definition>
			<units>mag</units></field>
		<field>
			<name>RAoh</name>
			<definition>Optical position Right Ascension (B1950)(hour)</definition>
			<units>h</units></field>
		<field>
			<name>RAom</name>
			<definition>Optical position Right Ascension (B1950)(min)</definition>
			<units>min</units></field>
		<field>
			<name>RAos</name>
			<definition>Optical position Right Ascension (B1950)(sec)</definition>
			<units>s</units></field>
		<field>
			<name>DEo-</name>
			<definition>Optical position Declination sign (B1950)
	<footnote footnoteId="???"><para>number=12</para>
			<para>Right ascension and declination of the optical object.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>DEod</name>
			<definition>Optical position Declination (B1950) (deg)</definition>
			<units>deg</units></field>
		<field>
			<name>DEom</name>
			<definition>Optical position Declination (B1950) (arcmin)</definition>
			<units>arcmin</units></field>
		<field>
			<name>DEos</name>
			<definition>Optical position Declination (B1950) (arcsec)</definition>
			<units>arcsec</units></field>
		<field>
			<name>oRA</name>
			<definition>Radio-optical RA offset
	<footnote footnoteId="???"><para>number=13</para>
			<para>These columns give the radio-minus-optical coordinates
          differences, in arcsec.</para></footnote></definition>
			<units>arcsec</units></field>
		<field>
			<name>oDE</name>
			<definition>Radio-optical Dec offset
	<footnote footnoteId="???"><para>number=13</para>
			<para>These columns give the radio-minus-optical coordinates
          differences, in arcsec.</para></footnote></definition>
			<units>arcsec</units></field>
		<field>
			<name>pos_flg</name>
			<definition>Flag indicating which radio position
                                         was adopted
	<footnote footnoteId="???"><para>number=14</para>
			<para>This column gives a single digit indicating, for multiple
          sources, the radio position adopted as follows:

          1   first component
          2   second component
          3   third component
          4   unweighted average position (midpoint)
          5   weighted average position (radio centroid)</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>r_ID</name>
			<definition>Reference code
	<footnote footnoteId="???"><para>number=15</para>
			<para>This column gives a reference code number. For sources with a
          measured redshift, only the reference for the redshift is given;
          for 3CR sources, the reader is referred also to Spinrad et al.
          (1985PASP...97..932S).
</para></footnote></definition>
			<units>---</units></field></fields></tableHead>
	<tableHead>
		<tableLinks>
				<tableLink xlink:href="refs.dat">
	<title>References</title></tableLink></tableLinks>
	<fields>
		<field>
			<name>code</name>
			<definition>reference code</definition>
			<units>---</units></field>
		<field>
			<name>reftxt</name>
			<definition>reference text</definition>
			<units>---</units></field></fields></tableHead>
	
	<history>
		<ingest>
	
			<creator>
				<lastName>Patricio Ortiz</lastName>
				<affiliation>CDS</affiliation></creator>
	<date>
		<year>1999</year><month>Mar</month><day>30</day></date></ingest>
		
		<revisions>
	<revision>
		<creator>
			<lastName>UNKNOWN</lastName></creator>
		<date><year>UNKNOWN</year></date>
		<para>    "The catalogue was  originally  archived  as  A016  by  H.   Andernach
    (heinz@astro.ugto.mx)   and  the   ADS   documentation   prepared   in
    collaboration with Carolyn Stern Grant (stern@cfa.harvard.edu)."</para></revision></revisions></history>
	<identifier>J_AJ_98_419.xml</identifier></dataset>
