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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Astron. Space Sci.</journal-id>
<journal-title>Frontiers in Astronomy and Space Sciences</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Astron. Space Sci.</abbrev-journal-title>
<issn pub-type="epub">2296-987X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fspas.2017.00037</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Astronomy and Space Sciences</subject>
<subj-group>
<subject>Perspective</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Catalog of 3 &#x0003C; z &#x0003C; 5.5 Quasar Candidates Selected among XMM-Newton Sources and Its Spectroscopic Verification</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name><surname>Khorunzhev</surname> <given-names>Georgii</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="author-notes" rid="fn001"><sup>&#x0002A;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/447112/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Sazonov</surname> <given-names>Sergey</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
</contrib>
<contrib contrib-type="author">
<name><surname>Burenin</surname> <given-names>Rodion</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
</contrib>
<contrib contrib-type="author">
<name><surname>Eselevich</surname> <given-names>Maxim</given-names></name>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
</contrib>
</contrib-group>
<aff id="aff1"><sup>1</sup><institution>High Energy Astrophysics, Space Research Institute, Russian Academy of Sciences</institution>, <addr-line>Moscow</addr-line>, <country>Russia</country></aff>
<aff id="aff2"><sup>2</sup><institution>Laboratory of Infrared Methods in Astrophysics, Institute of Solar-Terrestrial Physics, Russian Academy of Sciences</institution>, <addr-line>Irkutsk</addr-line>, <country>Russia</country></aff>
<author-notes>
<fn fn-type="edited-by"><p>Edited by: Mauro D&#x00027;Onofrio, Universit&#x000E0; degli Studi di Padova, Italy</p></fn>
<fn fn-type="edited-by"><p>Reviewed by: Paola Severgnini, Brera Astronomical Observatory, Italy; Fabio La Franca, Universit&#x000E0; degli Studi Roma Tre, Italy</p></fn>
<fn fn-type="corresp" id="fn001"><p>&#x0002A;Correspondence: Georgii Khorunzhev <email>horge&#x00040;iki.rssi.ru</email></p></fn>
<fn fn-type="other" id="fn002"><p>This article was submitted to Milky Way and Galaxies, a section of the journal Frontiers in Astronomy and Space Sciences</p></fn></author-notes>
<pub-date pub-type="epub">
<day>13</day>
<month>11</month>
<year>2017</year>
</pub-date>
<pub-date pub-type="collection">
<year>2017</year>
</pub-date>
<volume>4</volume>
<elocation-id>37</elocation-id>
<history>
<date date-type="received">
<day>31</day>
<month>08</month>
<year>2017</year>
</date>
<date date-type="accepted">
<day>24</day>
<month>10</month>
<year>2017</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#x000A9; 2017 Khorunzhev, Sazonov, Burenin and Eselevich.</copyright-statement>
<copyright-year>2017</copyright-year>
<copyright-holder>Khorunzhev, Sazonov, Burenin and Eselevich</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/"><p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) or licensor are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p></license>
</permissions>
<abstract><p>We have compiled a catalog of 903 quasar candidates (including known quasars) at 3 &#x0003C; <italic>z</italic> &#x0003C; 5.5 selected among X-ray sources from the XMM-Newton serendipitous survey (3XMM-DR4 catalog). We used photometric SDSS, 2MASS, and WISE data to select the objects. The surface number density of objects in our sample exceeds that in the SDSS spectroscopic quasar sample at the same redshifts by a factor of 1.5. We have performed spectroscopic observations of a subsample of new quasar candidates using a new low- and medium-resolution spectrograph at the 1.6-m AZT-33IK telescope (Mondy, Russia) and demonstrated that the purity of these candidates is about 65%. We have discovered one of the most distant (<italic>z</italic> &#x0003D; 5.08) X-ray selected quasars.</p></abstract>
<kwd-group>
<kwd>active galactic nuclei</kwd>
<kwd>quasars</kwd>
<kwd>X-ray surveys</kwd>
<kwd>photometric redshifts</kwd>
<kwd>spectroscopy</kwd>
<kwd>XMM-Newton</kwd>
<kwd>SDSS</kwd>
</kwd-group>
<contract-num rid="cn001">14.619.21.0004</contract-num>
<contract-num rid="cn001">NSh-10222.2016.2</contract-num>
<contract-sponsor id="cn001">Ministry of Education and Science of the Russian Federation<named-content content-type="fundref-id">10.13039/501100003443</named-content></contract-sponsor>
<counts>
<fig-count count="2"/>
<table-count count="0"/>
<equation-count count="2"/>
<ref-count count="25"/>
<page-count count="5"/>
<word-count count="3224"/>
</counts>
</article-meta>
</front>
<body>
<sec sec-type="intro" id="s1">
<title>1. Introduction</title>
<p>Searching for quasars at <italic>z</italic> &#x0003E; 3 is one of the key elements of studying the growth history of supermassive black holes and the evolution of massive galaxies in the Universe. For this purpose, multiwavelength observations of a large number of quasars are needed. Particularly valuable are X-ray observations: the intensive X-ray emission is directly connected with powerful processes of accretion onto the black hole. In order to improve our fairly poor knowledge of the evolution of the X-ray luminosity function of quasars at <italic>z</italic> &#x0003E; 3, larger X-ray samples of distant quasars are needed.</p>
<p>We have made an attempt to obtain a large sample of luminous X-ray quasars at <italic>z</italic> &#x0003E; 3 in the fields of the serendipitous XMM-Newton 3XMM-DR4 (Watson et al., <xref ref-type="bibr" rid="B23">2009</xref>) survey at Galactic latitudes |<italic>b</italic>| &#x0003E; 20&#x000B0; using photometric data from SDSS (Eisenstein et al., <xref ref-type="bibr" rid="B7">2011</xref>), 2MASS (Skrutskie et al., <xref ref-type="bibr" rid="B20">2006</xref>) and WISE (Wright et al., <xref ref-type="bibr" rid="B24">2010</xref>). The 3XMM-DR4/SDSS overlapping area is &#x0007E;300 sq. deg, exceeding by several times the areas covered by known samples of distant X-ray quasars such as Champ (Kalfountzou et al., <xref ref-type="bibr" rid="B9">2014</xref>) and XMM-XXL (north) (Menzel et al., <xref ref-type="bibr" rid="B13">2016</xref>). The sample of Kalfountzou et al. (<xref ref-type="bibr" rid="B9">2014</xref>) covers &#x02248;33 sq. deg and includes 87 X-ray selected optically bright (detected by SDSS) quasars. Half of them have photometric redshifts only. The spectroscopic program of (Menzel et al., <xref ref-type="bibr" rid="B13">2016</xref>) has revealed 61 X-ray objects at <italic>z</italic><sub>spec</sub> &#x0003E; 3 in a 18 sq. deg subfield of XMM-XXL (north). Our sample thus provides an opportunity to study a population of rare high-luminosity, distant quasars and complements recent studies of less luminous high-redshift quasars conducted using deep small-area surveys (e.g., Onoue et al., <xref ref-type="bibr" rid="B15">2017</xref>; Ricci et al., <xref ref-type="bibr" rid="B18">2017</xref>; Vito et al., <xref ref-type="bibr" rid="B22">2017</xref>).</p>
<p>It should be noted that SDSS spectroscopic data provide redshift measurements for 33 thousand optically selected quasars at <italic>z</italic><sub>spec</sub> &#x0003E; 3 (Alam et al., <xref ref-type="bibr" rid="B3">2015</xref>) over 11,000 sq. deg in the sky. However, existing wide-area X-ray surveys are too shallow to study these objects. It is only the forthcoming all-sky X-ray survey by eROSITA aboard the Spektrum-Roentgen-Gamma observatory (Pavlinsky et al., <xref ref-type="bibr" rid="B16">2011</xref>; Merloni et al., <xref ref-type="bibr" rid="B14">2012</xref>) that will be capable of finding X-ray counterparts for a substantial fraction of known quasars at <italic>z</italic><sub>spec</sub> &#x0003E; 3.</p>
<p>Based on broadband photometry, we obtained photometric redshift estimates (<italic>z</italic><sub>phot</sub>) and compiled a catalog of 903 candidates for distant quasars with <italic>z</italic><sub>phot</sub> &#x0003E; 2.75 (Khorunzhev et al., <xref ref-type="bibr" rid="B11">2016</xref>). The catalog includes 515 known quasars (with spectroscopic redshifts, of which 266 are at <italic>z</italic><sub>spec</sub> &#x0003E; 3) and 388 new quasar candidates. Most (80%) of the spectroscopic redshifts have been obtained by SDSS (Alam et al., <xref ref-type="bibr" rid="B3">2015</xref>). The remaining <italic>z</italic><sub>spec</sub> have been gathered from various sources (Flesch, <xref ref-type="bibr" rid="B8">2015</xref>). The new quasar candidates selected by <italic>z</italic><sub>phot</sub> constitute a substantial addition to the spectroscopic sample. Thus, if most of these candidates prove to be quasars at <italic>z</italic> &#x0003E; 3, the existing 3XMM-DR4/SDSS sample of distant quasars will be enhanced by a factor of &#x0007E;1.5.</p>
<p>Spectroscopic verification is necessary to determine the accuracy of our <italic>z</italic><sub>phot</sub> estimates and assess the purity of our selection of quasar candidates. We have thus started a spectroscopy identification program for the new quasar candidates (Khorunzhev et al., <xref ref-type="bibr" rid="B12">2017</xref>). Some initial results of this program are reported below.</p>
</sec>
<sec id="s2">
<title>2. Sample selection</title>
<p><italic>K16</italic> considered point SDSS sources at Galactic latitudes |<italic>b</italic>| &#x0003E; 20&#x000B0; that have an X-ray counterpart in 3XMM-DR4<xref ref-type="fn" rid="fn0001"><sup>1</sup></xref>. In addition, we used near- (2MASS) and medium-infrared (WISE) photometry if available. To keep sources with reliable photometry and to get rid of M-dwarfs, we applied the following condition:
<disp-formula id="E1"><label>(1)</label><mml:math id="M4"><mml:mrow><mml:mi>&#x003B4;</mml:mi><mml:msub><mml:mi>m</mml:mi><mml:mrow><mml:mi>z</mml:mi><mml:mo>&#x02032;</mml:mo></mml:mrow></mml:msub><mml:mo>&#x0003C;</mml:mo><mml:mn>0.2</mml:mn><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x00026;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:mi>i</mml:mi><mml:mo>&#x02032;</mml:mo><mml:mo>&#x02212;</mml:mo><mml:mi>z</mml:mi><mml:mo>&#x02032;</mml:mo><mml:mo>&#x0003C;</mml:mo><mml:mn>0.6</mml:mn><mml:mtext>&#x000A0;</mml:mtext><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
where <italic>i</italic>&#x02032; and <italic>z</italic>&#x02032; are the PSF magnitudes in the appropriate SDSS bands and <inline-formula><mml:math id="M2"><mml:mi>&#x003B4;</mml:mi><mml:msub><mml:mrow><mml:mi>m</mml:mi></mml:mrow><mml:mrow><mml:msup><mml:mrow><mml:mi>z</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x02032;</mml:mi></mml:mrow></mml:msup></mml:mrow></mml:msub><mml:mo>&#x0003C;</mml:mo><mml:mn>0</mml:mn><mml:mo>.</mml:mo><mml:mn>2</mml:mn></mml:math></inline-formula> is the corresponding error. This is a well-known technique (e.g., Richards et al., <xref ref-type="bibr" rid="B19">2002</xref>; Wu et al., <xref ref-type="bibr" rid="B25">2012</xref>; Skrzypek et al., <xref ref-type="bibr" rid="B21">2015</xref>) for separating M-dwarfs from distant quasars. Stars have <italic>i</italic>&#x02032; &#x02212; <italic>z</italic>&#x02032; &#x0003E; 0.8, while quasars have <italic>i</italic>&#x02032; &#x02212; <italic>z</italic>&#x02032; &#x0003C; 0.4. This color remains approximately constant up to a redshift of &#x02248;5.5, until the Ly&#x003B1; line passes from <italic>i</italic>&#x02032; to <italic>z</italic>&#x02032;. The color of quasars then becomes <italic>i</italic>&#x02032; &#x02212; <italic>z</italic>&#x02032; &#x02248; 2.</p>
<p>We then performed a broadband energy distribution fitting using the EAZY software (Brammer et al., <xref ref-type="bibr" rid="B4">2008</xref>) to obtain photometric redshift estimates. We made two fitting iterations for each object using libraries of quasar (by various authors) and star (Pickles, <xref ref-type="bibr" rid="B17">1998</xref>) templates. Those objects with
<disp-formula id="E2"><label>(2)</label><mml:math id="M50"><mml:mrow><mml:msubsup><mml:mi>&#x003C7;</mml:mi><mml:mrow><mml:mi>s</mml:mi><mml:mi>t</mml:mi><mml:mi>a</mml:mi><mml:mi>r</mml:mi></mml:mrow><mml:mn>2</mml:mn></mml:msubsup><mml:mo>/</mml:mo><mml:msubsup><mml:mi>&#x003C7;</mml:mi><mml:mrow><mml:mi>q</mml:mi><mml:mi>s</mml:mi><mml:mi>o</mml:mi></mml:mrow><mml:mn>2</mml:mn></mml:msubsup><mml:mo>&#x0003E;</mml:mo><mml:mn>1</mml:mn><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x00026;</mml:mo><mml:msub><mml:mi>z</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0003E;</mml:mo><mml:mn>2.75</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
finally constituted our catalog of 903 candidates for distant quasars selected by photometric redshift. At the same time, our procedure missed 63 known quasars at <italic>z</italic><sub>spec</sub> &#x0003E; 3 (see Figure <xref ref-type="fig" rid="F1">1</xref>). Note that we lowered the threshold of selection from <italic>z</italic><sub>phot</sub> &#x0003D; 3.0 to 2.75 to achieve reasonable selection completeness at <italic>z</italic> &#x0007E; 3.</p>
<fig id="F1" position="float">
<label>Figure 1</label>
<caption><p>Scatter plot of <italic>z</italic><sub>spec</sub> relative to <italic>z</italic><sub>phot</sub> for point objects (having an error <inline-formula><mml:math id="M5"><mml:mi>&#x003B4;</mml:mi><mml:msubsup><mml:mrow><mml:mi>z</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>s</mml:mi><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x02032;</mml:mi></mml:mrow></mml:msubsup><mml:mo>&#x0003C;</mml:mo><mml:mn>0</mml:mn><mml:mo>.</mml:mo><mml:mn>2</mml:mn></mml:math></inline-formula> and spectroscopic SDSS redshift <italic>z</italic><sub>spec</sub> &#x0003C; 5.5). Light gray dots denote all SDSS sources. Black symbols are <italic>K16</italic> objects with known redshift at the time of catalog compilation. Red symbols are objects whose spectra were obtained afterwards at AZT-33IK. The dash&#x02013;dotted lines limit the area of <italic>z</italic><sub>phot</sub> catastrophic outliers. The vertical dotted line at <italic>z</italic><sub>phot</sub> &#x0003D; 2.75 denotes the <italic>K16</italic> low <italic>z</italic><sub>phot</sub> boundary of selection. The horizontal dotted line (<italic>z</italic><sub>spec</sub> &#x0003D; 3.0) denotes our target <italic>z</italic><sub>spec</sub> boundary for distant quasars.</p></caption>
<graphic xlink:href="fspas-04-00037-g0001.tif"/>
</fig>
<p>The completeness of our catalog in the investigated fields relative to existing spectroscopic catalogs of quasars (SDSS DR12 Alam et al. <xref ref-type="bibr" rid="B3">2015</xref> and <italic>The Half Million Quasars</italic> Flesch <xref ref-type="bibr" rid="B8">2015</xref>) with <italic>z</italic><sub>spec</sub> &#x0003E; 3 is about 80%. The normalized median absolute deviation of photometric redshift estimates for the spectroscopically confirmed quasars (&#x00394;<italic>z</italic> &#x0003D; |<italic>z</italic><sub>spec</sub> &#x02212; <italic>z</italic><sub>phot</sub>|) is &#x003C3;<sub>&#x00394;<italic>z</italic>/(1&#x0002B;<sub><italic>z</italic></sub><sub>spec</sub>)</sub> &#x0003D; 0.07, while the catastrophic outlier fraction is &#x003B7; &#x0003D; 9% (when &#x00394;<italic>z</italic>/(1&#x0002B;<italic>z</italic><sub>spec</sub>) &#x0003E; 0.2).</p>
</sec>
<sec id="s3">
<title>3. Spectroscopic verification</title>
<p>We have performed a quasi-random spectroscopic survey of quasar candidates from the <italic>K16</italic> catalog at the 1.6-m AZT-33IK telescope (Kamus et al., <xref ref-type="bibr" rid="B10">2002</xref>; Denisenko et al., <xref ref-type="bibr" rid="B6">2009</xref>) equipped with the low- and medium-resolution ADAM spectrograph (Afanasiev et al., <xref ref-type="bibr" rid="B1">2016</xref>; Burenin et al., <xref ref-type="bibr" rid="B5">2016</xref>). A number of additional observations were conducted with the SCORPIO I (Afanasiev and Moiseev, <xref ref-type="bibr" rid="B2">2005</xref>) spectrograph at the 6-m BTA telescope.</p>
<sec>
<title>3.1. Observations at the AZT-33IK telescope</title>
<p>The AZT-33IK telescope is located at the Sayan Solar Observatory of the Institute of Solar-Terrestrial Physics, the Siberian branch of the Russian Academy of Sciences, and has a primary mirror diameter of 1.6 m. The low- and medium-resolution ADAM spectrograph was produced at the Special Astrophysical Observatory of the Russian Academy of Sciences and was installed on AZT-33IK in 2015. The quantum efficiency of the entire system (telescope mirror, spectrograph, grating and CCD array) reaches 50% (Burenin et al., <xref ref-type="bibr" rid="B5">2016</xref>). The ADAM spectrograph allows the spectra of objects with an apparent magnitude R &#x0007E; 19.5 to be taken with an exposure time of half an hour. If necessary and under good weather conditions, a magnitude I &#x0007E; 21 can be reached with an exposure time of two hours.</p>
<p>By now, we have obtained the spectroscopic redshifts for 48 quasar candidates, i.e more than 10% of such objects in the <italic>K16</italic> catalog. Approximately 60% of the observed objects proved to be quasars at <italic>z</italic><sub>spec</sub> &#x02273; 2.5, of which 16 have <italic>z</italic><sub>spec</sub> &#x0003E; 3. We found 4 new spectroscopically confirmed quasars at <italic>z</italic><sub>spec</sub> &#x0003E; 4, of which one, <italic>3XMM J125329.4</italic>&#x0002B;<italic>305539</italic> is at <italic>z</italic><sub>spec</sub> &#x0003D; 5.08.</p>
</sec>
<sec>
<title>3.2. Discovery of a quasar at <italic>z</italic> &#x0003D; 5.08</title>
<p><italic>3XMM J125329.4</italic>&#x0002B;<italic>305539</italic> was first reported (Khorunzhev et al., <xref ref-type="bibr" rid="B11">2016</xref>) as a probable quasar at <italic>z</italic><sub>phot</sub> &#x0003D; 4.64 in the <italic>K16</italic> catalog, and there was no information about this source in other photometric catalogs of quasar candidates<xref ref-type="fn" rid="fn0002"><sup>2</sup></xref>. Its SDSS apparent magnitude is <italic>i</italic>&#x02032; &#x02243;21.0. Its 0.5&#x02013;2 keV flux is 1.5 &#x000D7; 10<sup>&#x02212;15</sup> erg/s/cm<sup>2</sup> and the corresponding X-ray luminosity is 4 &#x000D7; 10<sup>44</sup> erg/s (without <italic>k</italic>-correction).</p>
<p>Apart from this source, there are only 3 optically bright (i.e., with reliable SDSS photometry) X-ray quasars at <italic>z</italic><sub>spec</sub> &#x0003E; 5.0, which are not XMM-Newton observational targets, in the <italic>3XMM-DR4</italic> catalog. Thus, <italic>3XMM J125329.4</italic>&#x0002B;<italic>305539</italic> is one of the brightest and most distant X-ray quasars at <italic>z</italic><sub>spec</sub> &#x0003E; 5.0 suitable for constructing the X-ray luminosity function at such redshifts.</p>
</sec>
<sec>
<title>3.3. Purity and selection completeness</title>
<p>We can estimate the purity of the <italic>K16</italic> catalog using the obtained quasi-random spectroscopic sample. Consider the following photometric redshift intervals: 2.75 &#x02264; <italic>z</italic><sub>phot</sub> &#x0003C; 4, 4 &#x02264; <italic>z</italic><sub>phot</sub> &#x0003C; 5 and 5 &#x02264; <italic>z</italic><sub>phot</sub> &#x0003C; 5.5. By purity we mean the ratio of the number of true quasars (|<italic>z</italic><sub>phot</sub> &#x02212; <italic>z</italic><sub>spec</sub>|/(1 &#x0002B; <italic>z</italic><sub>spec</sub>) &#x0003C; 0.2) to that of all objects with available spectra. Here, the value 0.2 reflects the scatter (3 standard deviations) of <italic>z</italic><sub>phot</sub> relative to <italic>z</italic><sub>spec</sub> for all of the known and spectroscopically confirmed quasars in the <italic>K16</italic> catalog. The purity of the spectroscopic sample calculated in this way is shown in Figure <xref ref-type="fig" rid="F2">2</xref> (circles).</p>
<fig id="F2" position="float">
<label>Figure 2</label>
<caption><p>Circles with Poissonian errorbars indicate the purity of the quasar candidates whose spectra have been taken at AZT-33IK or BTA. The arrows indicate the estimated lower limit for the purity of the <italic>K16</italic> catalog relative to the objects with known (from literature or SDSS) spectroscopic redshifts.</p></caption>
<graphic xlink:href="fspas-04-00037-g0002.tif"/>
</fig>
<p>For comparison, the arrows in Figure <xref ref-type="fig" rid="F2">2</xref> indicate the lower limit on the purity of the <italic>K16</italic> catalog estimated at the time of its compilation (before our AZT-33IK observations). This limit was deduced as the ratio of the number of true quasars with known spectroscopic redshifts and |<italic>z</italic><sub>phot</sub> &#x02212; <italic>z</italic><sub>spec</sub>|/(1 &#x0002B; <italic>z</italic><sub>spec</sub>) &#x0003C; 0.2 to the total number of objects in the catalog. Recall that the new candidates without spectroscopic redshifts accounted for about 40% of the <italic>K16</italic> catalog.</p>
<p>Based on these preliminary results, we can expect &#x0007E;250 quasars at <italic>z</italic> &#x02273; 3 to be firmly identified upon completion of the spectroscopy of all new quasar candidates from the <italic>K16</italic> catalog. This would significantly increase the sample of known distant X-ray quasars.</p>
</sec>
</sec>
<sec sec-type="conclusions" id="s4">
<title>4. Conclusion</title>
<p>The obtained spectra of dosens of quasars at <italic>z</italic> &#x0007E; 3 and especially the discovery of one of the most distant X-ray selected quasars (<italic>3XMM J125329.4</italic>&#x0002B;<italic>305539</italic>) at <italic>z</italic><sub>spec</sub> &#x0003D; 5.08 demonstrate that the AZT-33IK telescope of the Sayan Solar Observatory equipped with the new ADAM spectrograph is well suited for identification of distant quasars. This telescope is planned to be one of the instruments employed for optical support of the upcoming all-sky X-ray survey by the Spektrum-Roentgen-Gamma observatory (with its eROSITA and ART-XC telescopes, Pavlinsky et al., <xref ref-type="bibr" rid="B16">2011</xref>; Merloni et al., <xref ref-type="bibr" rid="B14">2012</xref>).</p>
<p>We have demonstrated that the existing sample of distant X-ray quasars can be substationally increased using publicly available X-ray (XMM-Newton) and optical photometry (SDSS) data, complemented by a relatively low-cost spectroscopic identification program.</p>
<p>We are continuing our spectroscopic verification program for <italic>K16</italic> candidates using the AZT-33IK and BTA telescopes and intend to obtain a complete spectroscopic sample at least for brighter X-ray sources from the <italic>K16</italic> catalog.</p>
</sec>
<sec id="s5">
<title>Author contributions</title>
<p>GK provided key contributions to the compilation of the catalog, spectroscopic observations, data analysis and writing of this paper. SS supervised the research at all stages. RB contributed to the aquisition and processing of spectroscopic data. ME organized spectroscopic observations at AZT-33IK.</p>
<sec>
<title>Conflict of interest statement</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
</sec>
</body>
<back>
<ack>
<p>This research was partially supported by the Program of the President of the Russian Federation for support of leading scientific schools (grant NSh-10222.2016.2).</p>
<p>This research is based on observations obtained with XMM-Newton, an ESA science mission with instruments and contributions directly funded by ESA Member States and NASA. Also, we used SDSS-III, 2MASS, WISE data. Funding for SDSS-III has been provided by the Alfred P. Sloan Foundation, the Participating Institutions, the National Science Foundation, and the U.S. Department of Energy Office of Science. The Two Micron All Sky Survey is a joint project of the University of Massachusetts and the Infrared Processing and Analysis Center/California Institute of Technology, funded by the National Aeronautics and Space Administration and the National Science Foundation. The Wide-field Infrared Survey Explorer is a joint project of the University of California, Los Angeles, and the Jet Propulsion Laboratory/California Institute of Technology, funded by the National Aeronautics and Space Administration.</p>
</ack>
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<fn id="fn0001"><p><sup>1</sup><ext-link ext-link-type="uri" xlink:href="http://heasarc.gsfc.nasa.gov/W3Browse/xmm-newton/xmmssc.html">http://heasarc.gsfc.nasa.gov/W3Browse/xmm-newton/xmmssc.html</ext-link></p></fn>
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<fn fn-type="financial-disclosure"><p><bold>Funding.</bold> The observations at the 6-m BTA telescope were financially supported by the Ministry of Education and Science of the Russian Federation (contract no. 14.619.21.0004, project identifier RFMEFI61914X0004).</p>
</fn>
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