<?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>Deep imaging of the field of the high-redshift radio source 4C 23.56</title>
	<altname type="ADC">J/ApJS/109/367</altname>
		<altname type="CDS">J/ApJS/109/367</altname>
		<altname type="brief">4C 23.56 field deep imaging</altname>
	<reference>
		<source>
<journal>
	<title>Deep imaging of the field of the high-redshift radio source 4C 23.56</title>
	<author>
			<initial>G</initial>
			<initial>P</initial>
			<lastName>Knopp</lastName></author>
	<author>
			<initial>K</initial>
			<initial>C</initial>
			<lastName>Chambers</lastName></author>
	<name>Astrophys. J. Suppl. Ser.</name>
	<volume>109</volume>
	<pageno>367</pageno>
		<date>
			<year>1997</year></date>
	<bibcode>1997ApJS..109..367K</bibcode></journal></source></reference>
	<keywords parentListURL="http://messier.gsfc.nasa.gov/xml/keywordlists/adc_keywords.html">
			<keyword xlink:href="Galaxies_radio.html">Galaxies, radio</keyword>
			<keyword xlink:href="Photometry_infrared.html">Photometry, infrared</keyword></keywords>
	<keywords parentListURL="http://messier.gsfc.nasa.gov/xml/keywordlists/apj_keywords.html">
			<keyword xlink:href="galaxies_individual_(4C_23.56).html">galaxies: individual (4C 23.56)</keyword>
			<keyword xlink:href="galaxies_photometry.html">galaxies: photometry</keyword>
			<keyword xlink:href="galaxies_structure.html">galaxies: structure</keyword>
			<keyword xlink:href="infrared_galaxies.html">infrared: galaxies</keyword>
			<keyword xlink:href="radio_continuum_galaxies.html">radio continuum: galaxies</keyword></keywords>
	<descriptions>
				<abstract>
					<para>
    We present deep infrared and optical imaging of a 1.25arcmin^2^ field
    centered on the giant (~0.5Mpc) high-redshift (z=2.479)
    ultra-steep-spectrum radio source 4C 23.56. The optical/infrared
    continuum morphology of the host galaxy is asymmetric, with strong
    color gradients and an enormous biconical emission-line nebula. The
    morphology of 4C 23.56 is best described by a dusty galaxy illuminated
    by a beam from an active galactic nucleus that is scattered into our
    line of sight. We determine the K' band number counts in the field to
    a limit of K'=22.5mag and find a marginally significant excess of
    objects with K'=19-21mag, compared to other K' band surveys. Spectral
    energy distributions (SEDs) of 117 objects in the field are
    constructed from aperture photometry in five bands (U', NB, V, I, and
    K'). From the SEDS we distinguish three subsets of objects as possible
    candidates for z~2.48 companions: emission-line galaxies, very red
    galaxies, and flat-spectrum star-forming galaxies. The field has nine
    candidate objects with line emission in a narrow band centered on the
    redshifted Ly{alpha} line, compared to an expected number of at most
    three foreground [O II] emitters that could mimic Ly{alpha} alpha
    sources. We find a high density of faint, very red objects with
    I-K'>4mag in the field, including two with I-K'>6mag.</para></abstract>
                        <details/></descriptions>
	<tableHead>
		<tableLinks>
				<tableLink xlink:href="table4">
	<title>Photometry of 4C 23.56 field sources</title></tableLink></tableLinks>
	<fields>
		<field>
			<name>Seq</name>
			<definition>Source sequential number</definition>
			<units>---</units></field>
		<field>
			<name>RAh</name>
			<definition>Right ascension (2000)</definition>
			<units>h</units></field>
		<field>
			<name>RAm</name>
			<definition>Right ascension (2000)</definition>
			<units>min</units></field>
		<field>
			<name>RAs</name>
			<definition>Right ascension (2000)</definition>
			<units>s</units></field>
		<field>
			<name>DEd</name>
			<definition>Declination (2000)</definition>
			<units>deg</units></field>
		<field>
			<name>DEm</name>
			<definition>Declination (2000)</definition>
			<units>arcmin</units></field>
		<field>
			<name>DEs</name>
			<definition>Declination (2000)</definition>
			<units>arcsec</units></field>
		<field>
			<name>l_U'mag</name>
			<definition>Limit flag on U'mag</definition>
			<units>---</units></field>
		<field>
			<name>U'mag</name>
			<definition>U' magnitude (3402{AA})</definition>
			<units>mag</units></field>
		<field>
			<name>e_U'mag</name>
			<definition>rms uncertainty on U'mag</definition>
			<units>mag</units></field>
		<field>
			<name>n_U'mag</name>
			<definition>Note on U'mag
	<footnote footnoteId="???"><para>number=1</para>
			<para>We abbreviate the notes to waveband measurements as
           s = saturated
           o = obscured in the wings of a bright source and thus not identified
           f = failed to meet selection criteria</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>l_NB</name>
			<definition>Limit flag on NB</definition>
			<units>---</units></field>
		<field>
			<name>NB</name>
			<definition>Narrow band magnitude (4229{AA}) in
                                   AB magnitude
	<footnote footnoteId="???"><para>number=2</para>
			<para>In the AB-magnitude system, any object with a flat spectrum
            (F_{nu} prop. to {nu}^0^) has the same magnitude,
            independent of passband: m_AB_=-2.5log(f_{nu}_) - 48.59</para></footnote></definition>
			<units>mag</units></field>
		<field>
			<name>e_NB</name>
			<definition>rms uncertainty on NB in AB magnitude
	<footnote footnoteId="???"><para>number=2</para>
			<para>In the AB-magnitude system, any object with a flat spectrum
            (F_{nu} prop. to {nu}^0^) has the same magnitude,
            independent of passband: m_AB_=-2.5log(f_{nu}_) - 48.59</para></footnote></definition>
			<units>mag</units></field>
		<field>
			<name>n_NB</name>
			<definition>Note on NB
	<footnote footnoteId="???"><para>number=1</para>
			<para>We abbreviate the notes to waveband measurements as
           s = saturated
           o = obscured in the wings of a bright source and thus not identified
           f = failed to meet selection criteria</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>l_Vmag</name>
			<definition>Limit flag on Vmag</definition>
			<units>---</units></field>
		<field>
			<name>Vmag</name>
			<definition>V magnitude (5457{AA})</definition>
			<units>mag</units></field>
		<field>
			<name>e_Vmag</name>
			<definition>rms uncertainty on Vmag</definition>
			<units>mag</units></field>
		<field>
			<name>n_Vmag</name>
			<definition>Note on Vmag
	<footnote footnoteId="???"><para>number=1</para>
			<para>We abbreviate the notes to waveband measurements as
           s = saturated
           o = obscured in the wings of a bright source and thus not identified
           f = failed to meet selection criteria</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>l_Imag</name>
			<definition>Limit flag on Imag</definition>
			<units>---</units></field>
		<field>
			<name>Imag</name>
			<definition>I magnitude (8300{AA})</definition>
			<units>mag</units></field>
		<field>
			<name>e_Imag</name>
			<definition>rms uncertainty on Imag</definition>
			<units>mag</units></field>
		<field>
			<name>n_Imag</name>
			<definition>Note on Imag
	<footnote footnoteId="???"><para>number=1</para>
			<para>We abbreviate the notes to waveband measurements as
           s = saturated
           o = obscured in the wings of a bright source and thus not identified
           f = failed to meet selection criteria</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>l_K'mag</name>
			<definition>Limit flag on K'mag</definition>
			<units>---</units></field>
		<field>
			<name>K'mag</name>
			<definition>K' magnitude (21100{AA})</definition>
			<units>mag</units></field>
		<field>
			<name>e_K'mag</name>
			<definition>rms uncertainty on K'mag</definition>
			<units>mag</units></field>
		<field>
			<name>n_K'mag</name>
			<definition>Note on K'mag
	<footnote footnoteId="???"><para>number=1</para>
			<para>We abbreviate the notes to waveband measurements as
           s = saturated
           o = obscured in the wings of a bright source and thus not identified
           f = failed to meet selection criteria</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>Class</name>
			<definition>Classification
	<footnote footnoteId="???"><para>number=3</para>
			<para>Our tentative object classifications are abbreviated as follows:
           FS = field star
           UG = unidentified galaxy
           E  = elliptical
           S  = spiral
           Im = irregular
           RG = 4C 23.56
</para></footnote></definition>
			<units>---</units></field></fields></tableHead>
	
	<history>
		<ingest>
	
			<creator>
				<lastName>James Marcout, Patricia Bauer</lastName>
				<affiliation>CDS</affiliation></creator>
	<date>
		<year>1997</year><month>Oct</month><day>07</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_ApJS_109_367.xml</identifier></dataset>
