<?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>Radio Sources Observed with the Culgoora Circular Array (CCA) at 80 and 160 MHz</title>
	<altname type="ADC">8035</altname>
		<altname type="CDS">VIII/35</altname>
		<altname type="brief">Radio Sources observed with Culgoora Circular Array</altname>
	<reference>
		<source>
<journal>
	<title>Radio Sources Observed with the Culgoora Circular Array (CCA) at 80 and 160 MHz</title>
	<author>
			<initial>O</initial>
			<initial>B</initial>
			<lastName>Slee</lastName></author>
	<name>Australian J. Phys.</name>
	<volume>48</volume>
	<pageno>143-186</pageno>
		<date>
			<year>1995</year></date>
	<bibcode>1995AuJPh..48..143S</bibcode></journal></source></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 is a final, updated and recalibrated list of sources that were
    observed with the Culgoora Circular Array (CCA) in the interval
    1970-1984. The list contains all the sources that were published in
    the Culgoora-1,2,3 Lists plus additional sources resulting from a
    survey of 353 Abell clusters of galaxies.</para><para>    The observations were made at 80 MHz and 160 MHz with HPBW in RA of
    3.70' and 1.85' respectively. The beamwidth in Dec is wider by
    sec(30.3 + Dec). This list brings together all CCA measurements of
    flux density, position, spectral index and angular size, with limiting
    flux densities of 4 Jy at 80 MHz and 2 Jy at 160 MHz. References to
    the original Culgoora publications are given for each source.</para><para>    The sources were selected for CCA observations from the Parkes, 4C and
    Ohio catalogues if an extrapolation of the then existing spectral data
    indicated that the 80 MHz flux density would be > 5 Jy. In addition,
    about 300 additional sources were added from lists of special classes
    of objects such as those discovered at higher frequencies from surveys
    of the galactic plane, lists of pulsars and supernova remnants, from a
    list of nearby bright galaxies and finally from a CCA survey of 353
    Abell clusters of galaxies. An area of 16'x16' was surveyed about the
    centres of 3500 fields, resulting in a total survey area of about 0.1
    sr at 80 MHz.</para><para>    Nomenclature Notes:
    Sources from this catalogue are designated "Cul HHMM+DDd" in the
    literature. Note that the original Cul 1,2,3 lists have only HHMM+DD
    as a name, but the present names should be preferred.</para></description>
                        <details/></descriptions>
	<tableHead>
		<tableLinks>
				<tableLink xlink:href="catalog">
	<title>The CCA survey</title></tableLink></tableLinks>
	<fields>
		<field>
			<name>Cul</name>
			<definition>Source name
	<footnote footnoteId="???"><para>number=1</para>
			<para>the Cul designation contains the B1950 name of the source,
    using IAU recommended standards. The first four characters are the
    hours and minutes of right ascension, and the last four the signed
    declination in tenths of a degree (truncated). The source names in the
    original Culgoora-1,2,3 Lists contained the signed declination in
    degrees (truncated). IAU names given to tenths of declination in
    previous papers (e.g. ref #4 in section 9 below) may differ by one or
    two in the last digit.
    The Cul designation is followed by symbols:
  * An asterisk (*) following the source name denotes that this is
    the centroid of two or more components, which can be located in the
    maps and tables of references 3,4 and 5 below. The components are
    not always parts of the same source.
  # the flag '#' indicates that the Culgoora position was lost, but
    the source can confidently be identified with a source whose
    coordinates are given in the publication listed in the reference
    column.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>n_Cul</name>
			<definition>Note on Source
	<footnote footnoteId="???"><para>number=1</para>
			<para>the Cul designation contains the B1950 name of the source,
    using IAU recommended standards. The first four characters are the
    hours and minutes of right ascension, and the last four the signed
    declination in tenths of a degree (truncated). The source names in the
    original Culgoora-1,2,3 Lists contained the signed declination in
    degrees (truncated). IAU names given to tenths of declination in
    previous papers (e.g. ref #4 in section 9 below) may differ by one or
    two in the last digit.
    The Cul designation is followed by symbols:
  * An asterisk (*) following the source name denotes that this is
    the centroid of two or more components, which can be located in the
    maps and tables of references 3,4 and 5 below. The components are
    not always parts of the same source.
  # the flag '#' indicates that the Culgoora position was lost, but
    the source can confidently be identified with a source whose
    coordinates are given in the publication listed in the reference
    column.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>o_S(160)</name>
			<definition>Number of observations at 160 MHz
	<footnote footnoteId="???"><para>number=2</para>
			<para>These columns contain the numbers of independent observations
    at 160 MHz and 80 MHz respectively. Each observation consists of
    averaging 10-20 drift scans with the central 8 or 16 beams (spaced in
    declination) of the CCA.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>o_S(80)</name>
			<definition>Number of observations at 80 MHz
	<footnote footnoteId="???"><para>number=2</para>
			<para>These columns contain the numbers of independent observations
    at 160 MHz and 80 MHz respectively. Each observation consists of
    averaging 10-20 drift scans with the central 8 or 16 beams (spaced in
    declination) of the CCA.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>RAh</name>
			<definition>Right Ascension B1950 (hours)
	<footnote footnoteId="???"><para>number=3</para>
			<para>The 160 MHz position is given if available, otherwise the
    80 MHz position. The positional calibration was obtained by observing
    at 2-hourly intervals strong unresolved sources with accurate
    high-frequency positions. Position errors are tabulated for various
    flux ranges and numbers of observations in the original Culgoora-1,2,3
    Lists. The positions of sources with contour maps at 160 MHz (entries
    in the angular size columns) are the centroids of the brightness
    distributions. Positions of other sources were found by fitting a
    one-dimensional Gaussian to the hour angle drift response and another
    Gaussian across the declination channels.</para></footnote></definition>
			<units>h</units></field>
		<field>
			<name>RAm</name>
			<definition>Right Ascension B1950 (minutes)
	<footnote footnoteId="???"><para>number=3</para>
			<para>The 160 MHz position is given if available, otherwise the
    80 MHz position. The positional calibration was obtained by observing
    at 2-hourly intervals strong unresolved sources with accurate
    high-frequency positions. Position errors are tabulated for various
    flux ranges and numbers of observations in the original Culgoora-1,2,3
    Lists. The positions of sources with contour maps at 160 MHz (entries
    in the angular size columns) are the centroids of the brightness
    distributions. Positions of other sources were found by fitting a
    one-dimensional Gaussian to the hour angle drift response and another
    Gaussian across the declination channels.</para></footnote></definition>
			<units>min</units></field>
		<field>
			<name>RAs</name>
			<definition>Right Ascension B1950 (seconds)
	<footnote footnoteId="???"><para>number=3</para>
			<para>The 160 MHz position is given if available, otherwise the
    80 MHz position. The positional calibration was obtained by observing
    at 2-hourly intervals strong unresolved sources with accurate
    high-frequency positions. Position errors are tabulated for various
    flux ranges and numbers of observations in the original Culgoora-1,2,3
    Lists. The positions of sources with contour maps at 160 MHz (entries
    in the angular size columns) are the centroids of the brightness
    distributions. Positions of other sources were found by fitting a
    one-dimensional Gaussian to the hour angle drift response and another
    Gaussian across the declination channels.</para></footnote></definition>
			<units>s</units></field>
		<field>
			<name>DE-</name>
			<definition>Declination B1950 (sign)
	<footnote footnoteId="???"><para>number=3</para>
			<para>The 160 MHz position is given if available, otherwise the
    80 MHz position. The positional calibration was obtained by observing
    at 2-hourly intervals strong unresolved sources with accurate
    high-frequency positions. Position errors are tabulated for various
    flux ranges and numbers of observations in the original Culgoora-1,2,3
    Lists. The positions of sources with contour maps at 160 MHz (entries
    in the angular size columns) are the centroids of the brightness
    distributions. Positions of other sources were found by fitting a
    one-dimensional Gaussian to the hour angle drift response and another
    Gaussian across the declination channels.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>DEd</name>
			<definition>Declination B1950 (degrees)
	<footnote footnoteId="???"><para>number=3</para>
			<para>The 160 MHz position is given if available, otherwise the
    80 MHz position. The positional calibration was obtained by observing
    at 2-hourly intervals strong unresolved sources with accurate
    high-frequency positions. Position errors are tabulated for various
    flux ranges and numbers of observations in the original Culgoora-1,2,3
    Lists. The positions of sources with contour maps at 160 MHz (entries
    in the angular size columns) are the centroids of the brightness
    distributions. Positions of other sources were found by fitting a
    one-dimensional Gaussian to the hour angle drift response and another
    Gaussian across the declination channels.</para></footnote></definition>
			<units>deg</units></field>
		<field>
			<name>DEm</name>
			<definition>Declination B1950 (minutes)
	<footnote footnoteId="???"><para>number=3</para>
			<para>The 160 MHz position is given if available, otherwise the
    80 MHz position. The positional calibration was obtained by observing
    at 2-hourly intervals strong unresolved sources with accurate
    high-frequency positions. Position errors are tabulated for various
    flux ranges and numbers of observations in the original Culgoora-1,2,3
    Lists. The positions of sources with contour maps at 160 MHz (entries
    in the angular size columns) are the centroids of the brightness
    distributions. Positions of other sources were found by fitting a
    one-dimensional Gaussian to the hour angle drift response and another
    Gaussian across the declination channels.</para></footnote></definition>
			<units>arcmin</units></field>
		<field>
			<name>DEs</name>
			<definition>Declination B1950 (seconds)
	<footnote footnoteId="???"><para>number=3</para>
			<para>The 160 MHz position is given if available, otherwise the
    80 MHz position. The positional calibration was obtained by observing
    at 2-hourly intervals strong unresolved sources with accurate
    high-frequency positions. Position errors are tabulated for various
    flux ranges and numbers of observations in the original Culgoora-1,2,3
    Lists. The positions of sources with contour maps at 160 MHz (entries
    in the angular size columns) are the centroids of the brightness
    distributions. Positions of other sources were found by fitting a
    one-dimensional Gaussian to the hour angle drift response and another
    Gaussian across the declination channels.</para></footnote></definition>
			<units>arcsec</units></field>
		<field>
			<name>GLON</name>
			<definition>Galactic longitude</definition>
			<units>deg</units></field>
		<field>
			<name>GLAT</name>
			<definition>Galactic latitude</definition>
			<units>deg</units></field>
		<field>
			<name>l_S(160)</name>
			<definition>Limit flag on S(160).</definition>
			<units>---</units></field>
		<field>
			<name>S(160)</name>
			<definition>Flux density at 160 MHz
	<footnote footnoteId="???"><para>number=4</para>
			<para>a recalibration of the flux scales was carried out by
    Slee &amp; Siegman (1988MNRAS.235.1313S). This resulted in our increasing
    the flux density by an average of 10% at 80 MHz and 12% at 160 MHz.
    The 160 MHz flux densities of sources with contour maps (entries in
    the angular size columns) were obtained by integrating the brightness
    contours.</para></footnote></definition>
			<units>Jy</units></field>
		<field>
			<name>l_S(80)</name>
			<definition>Limit flag on S(80).</definition>
			<units>---</units></field>
		<field>
			<name>S(80)</name>
			<definition>Flux density at 80 MHz
	<footnote footnoteId="???"><para>number=4</para>
			<para>a recalibration of the flux scales was carried out by
    Slee &amp; Siegman (1988MNRAS.235.1313S). This resulted in our increasing
    the flux density by an average of 10% at 80 MHz and 12% at 160 MHz.
    The 160 MHz flux densities of sources with contour maps (entries in
    the angular size columns) were obtained by integrating the brightness
    contours.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>SpIndex</name>
			<definition>Spectral index between 80 and 160 MHz
	<footnote footnoteId="???"><para>number=5</para>
			<para>this column contains the power-law spectral index between
    80 and 160 MHz (S(nu) {prop.to} nu^SpIndex^). A negative spectral
    index implies that flux density is decreasing with frequency.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>l_MajAxis</name>
			<definition>Limit flag on MajAxis</definition>
			<units>---</units></field>
		<field>
			<name>MajAxis</name>
			<definition>Major axis to 0.10 brightness at 160 MHz
	<footnote footnoteId="???"><para>number=6</para>
			<para>These columns contain the major and minor axes of a
    2-dimensional Gaussian ellipse that has been fitted to the 160 MHz
    contour map together with the position angle of the major axis (from
    north through east).The axes are given to the 0.10 brightness points
    (1.82 x half-brightness diameter). Where only the major axis is
    presented as a lower limit of 1.8 arcmin, the limit was derived (at
    the 95% confidence level) from one-dimensional Gaussian fits to the
    drift profiles in RA and Dec.</para></footnote></definition>
			<units>arcmin</units></field>
		<field>
			<name>l_MinAxis</name>
			<definition>Limit flag on MinAxis</definition>
			<units>---</units></field>
		<field>
			<name>MinAxis</name>
			<definition>Minor axis to 0.10 brightness at 160 MHz
	<footnote footnoteId="???"><para>number=6</para>
			<para>These columns contain the major and minor axes of a
    2-dimensional Gaussian ellipse that has been fitted to the 160 MHz
    contour map together with the position angle of the major axis (from
    north through east).The axes are given to the 0.10 brightness points
    (1.82 x half-brightness diameter). Where only the major axis is
    presented as a lower limit of 1.8 arcmin, the limit was derived (at
    the 95% confidence level) from one-dimensional Gaussian fits to the
    drift profiles in RA and Dec.</para></footnote></definition>
			<units>arcmin</units></field>
		<field>
			<name>PA</name>
			<definition>Position angle of major axis
                                    (east from north)
	<footnote footnoteId="???"><para>number=6</para>
			<para>These columns contain the major and minor axes of a
    2-dimensional Gaussian ellipse that has been fitted to the 160 MHz
    contour map together with the position angle of the major axis (from
    north through east).The axes are given to the 0.10 brightness points
    (1.82 x half-brightness diameter). Where only the major axis is
    presented as a lower limit of 1.8 arcmin, the limit was derived (at
    the 95% confidence level) from one-dimensional Gaussian fits to the
    drift profiles in RA and Dec.</para></footnote></definition>
			<units>deg</units></field>
		<field>
			<name>Refs</name>
			<definition>References
	<footnote footnoteId="???"><para>number=7</para>
			<para>References are
     1 =1973AuJPS..27....1S Slee &amp; Higgins 1973       (Culgoora-1 List)
     2 =1975AuJPS..36....1S Slee &amp; Higgins 1975       (Culgoora-2 List)
     3 =1977AuJPS..43....1S Slee 1977                 (Culgoora-3 List)
     4 =1983PASAu...5..114S Slee &amp; Siegman, Proc. ASA (Cluster Survey)
     5 =1982PASAu...4..278S Slee, Siegman, &amp; Mulhal   (Culgoora-3 Analysis)
     6 =1979PASAu...3..332S Slee &amp; Quinn, Proc. ASA   (Cluster Survey)
     7 =1972ApL....12...75S Slee, Astrophys. Lett. (Bright Galaxies at 80 MHz)
     8 =1972AuJPh..25..429D Dulk &amp; Slee, Austral.     (Supernova Remnants)
     9 =1975PASAu...2....1S Slee &amp; Sheridan, Proc.ASA (Cen-A &amp; Pictor-A)
    10 =1974Natur.248...33D Dulk &amp; Slee               (Sgr-A at 160 MHz)
    11 =1991ApJS...75....1B Becker, White &amp; Edwards (0736+016,2330+091,2349+135)
    12 =1992ApJS...80..501O Owen, White &amp; Burns       (1005+007)
    13 =1980BAAS...19.1048D Douglas (Texas Survey)
  Additional data in these papers include 80 MHz positions, optical
  identifications and beam broadening from the one-dimensional Gaussian
  fitting. The Culgoora-1,2,3 papers also contain tables listing the
  expected errors in flux density and position. References 3 and 4
  contain the 160 MHz contour maps for many sources. Reference numbers
  11,12,13 do not refer to Culgoora publications, but refer to papers
  containing sources that can be confidently identified with five
  sources, whose Culgoora positions have been lost.
</para></footnote></definition>
			<units>---</units></field></fields></tableHead>
	
	<history>
		<ingest>
	
			<creator>
				<lastName>Heinz J. Andernach</lastName>
				<affiliation>ESA-IUE</affiliation></creator>
	<date>
		<year>1996</year><month>Feb</month><day>19</day></date><acknowledgement>Author's address:
    O.B Slee,
        Australia Telescope National Facility,
        CSIRO, Sydney
       &lt;bslee@atnf.csiro.au></acknowledgement></ingest>
		
		<revisions>
	<revision>
		<creator>
			<lastName>UNKNOWN</lastName></creator>
		<date><year>UNKNOWN</year></date>
		<para>    The basic table was formed by electronically scanning the Culgoora-3
    list. Each line was later checked by visual comparison with the
    unscanned list and scanning errors were corrected manually. Additional
    sources were added manually from other references in &lt;cul_ref>.
    Angular size information was extracted from references 4 and 5 and
    added manually to the final table. Positions of five sources for which
    Culgoora positions had been lost were identified with the help of the
    EINLINE service (telnet to einline.harvard.edu, login as 'einline'
    with no password) and H. Andernach (file r132.new).

    Note that the electronic version differs from the one published in
    AuJPh.48.143 in that it includes several dozen more upper limits at
    160 MHz, taken from the listed references.</para></revision></revisions></history>
	<identifier>VIII_35.xml</identifier></dataset>