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  <front>
    <journal-meta>
      <journal-id journal-id-type="publisher-id">ijaa</journal-id>
      <journal-title-group>
        <journal-title>International Journal of Astronomy and Astrophysics</journal-title>
      </journal-title-group>
      <issn pub-type="epub">2161-4725</issn>
      <issn pub-type="ppub">2161-4717</issn>
      <publisher>
        <publisher-name>Scientific Research Publishing</publisher-name>
      </publisher>
    </journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.4236/ijaa.2025.152013</article-id>
      <article-id pub-id-type="publisher-id">ijaa-143774</article-id>
      <article-categories>
        <subj-group>
          <subject>Article</subject>
        </subj-group>
        <subj-group>
          <subject>Physics</subject>
          <subject>Mathematics</subject>
        </subj-group>
      </article-categories>
      <title-group>
        <article-title>A New Open Cluster Census in the Region of Cygnus OB2 with Gaia Data</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <name name-style="western">
            <surname>Paíz</surname>
            <given-names>Leonardo G.</given-names>
          </name>
          <xref ref-type="aff" rid="aff1">1</xref>
          <xref ref-type="aff" rid="aff2">2</xref>
        </contrib>
        <contrib contrib-type="author">
          <name name-style="western">
            <surname>Biasi</surname>
            <given-names>María S. De</given-names>
          </name>
          <xref ref-type="aff" rid="aff1">1</xref>
          <xref ref-type="aff" rid="aff2">2</xref>
        </contrib>
        <contrib contrib-type="author">
          <name name-style="western">
            <surname>Orellana</surname>
            <given-names>Rosa B.</given-names>
          </name>
          <xref ref-type="aff" rid="aff1">1</xref>
          <xref ref-type="aff" rid="aff2">2</xref>
        </contrib>
        <contrib contrib-type="author">
          <name name-style="western">
            <surname>Corti</surname>
            <given-names>Mariela A.</given-names>
          </name>
          <xref ref-type="aff" rid="aff1">1</xref>
          <xref ref-type="aff" rid="aff2">2</xref>
        </contrib>
      </contrib-group>
      <aff id="aff1"><label>1</label> Facultad de Ciencias Astronómicas y Geofísicas, UNLP, La Plata, Argentina </aff>
      <aff id="aff2"><label>2</label> Instituto de Astrofísica de La Plata (Centro Científico Tecnológico La Plata, Consejo Nacional de Investigaciones Científicas y Técnicas, Universidad Nacional de La Plata), La Plata, Argentina </aff>
      <author-notes>
        <fn fn-type="conflict" id="fn-conflict">
          <p>The authors declare no conflicts of interest regarding the publication of this paper.</p>
        </fn>
      </author-notes>
      <pub-date pub-type="epub">
        <day>17</day>
        <month>06</month>
        <year>2025</year>
      </pub-date>
      <pub-date pub-type="collection">
        <month>06</month>
        <year>2025</year>
      </pub-date>
      <volume>15</volume>
      <issue>02</issue>
      <fpage>171</fpage>
      <lpage>196</lpage>
      <history>
        <date date-type="received">
          <day>16</day>
          <month>04</month>
          <year>2025</year>
        </date>
        <date date-type="accepted">
          <day>27</day>
          <month>06</month>
          <year>2025</year>
        </date>
        <date date-type="published">
          <day>30</day>
          <month>06</month>
          <year>2025</year>
        </date>
      </history>
      <permissions>
        <copyright-statement>© 2025 by the authors and Scientific Research Publishing Inc.</copyright-statement>
        <copyright-year>2025</copyright-year>
        <license license-type="open-access">
          <license-p> This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license ( <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link> ). </license-p>
        </license>
      </permissions>
      <self-uri content-type="doi" xlink:href="https://doi.org/10.4236/ijaa.2025.152013">https://doi.org/10.4236/ijaa.2025.152013</self-uri>
      <abstract>
        <p>We revisit the Cygnus OB2 region to perform a detailed open cluster census taking profit from the high accuracy of <italic>Gaia</italic> DR3 astrometric and photometric data. HDBSCAN clustering algorithm is applied to the five astrometric parameters (<inline-formula><mml:math display="inline"></mml:math></inline-formula></p>
        <p>α</p>
        <p>, <inline-formula><mml:math display="inline"></mml:math></inline-formula></p>
        <p>δ</p>
        <p>, <inline-formula><mml:math display="inline"></mml:math></inline-formula></p>
        <p>μ</p>
        <p>α</p>
        <p>cosδ</p>
        <p>, <inline-formula><mml:math display="inline"></mml:math></inline-formula></p>
        <p>μ</p>
        <p>δ</p>
        <p>, <inline-formula><mml:math display="inline"></mml:math></inline-formula></p>
        <p>ϖ</p>
        <p>) in a circular region centred at <inline-formula><mml:math display="inline"></mml:math></inline-formula></p>
        <p>(</p>
        <p>l,b</p>
        <p>)=(</p>
        <p>79.8</p>
        <p>∘</p>
        <p>,+</p>
        <p>0.8</p>
        <p>∘</p>
        <p>)</p>
        <p>of radius 1.5˚ up to <inline-formula><mml:math display="inline"></mml:math></inline-formula></p>
        <p>G=19.5</p>
        <p>mag and leads us to detect four unnoticed open clusters named RSL-03, RSL-04, RSL-05 and RSL-06, as well as 20 known clusters. The mean proper motion of the open clusters is determined and the members are identified. The coordinates of the centre of the clusters and radii are calculated and their distances are estimated. The analysis of the mean proper motion and the distance of Bica 1, Bica 2, FSR 0236, FSR 0238, FSR 0224, HSC 625, OC-123, OC-128, NGC 6910, RSL-04, RSL-05, and RSL-06 suggests that these open clusters would be related to Cyg OB2 association. This is the first time that Bica 1 and Bica 2 have been identified using the <italic>Gaia</italic> DR3 five astrometric parameters. Besides, the open cluster HSC 630 would be related to the Left over-density found by our working group in a previous paper as an association candidate.</p>
      </abstract>
      <kwd-group kwd-group-type="author-generated" xml:lang="en">
        <kwd>Galaxy</kwd>
        <kwd>Open Clusters and Associations</kwd>
        <kwd>Astrometry</kwd>
        <kwd>Early-Type Stars</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec1">
      <title>1. Introduction</title>
      <p>The role that open clusters (OCs) play in studying Galactic formation, structure, dynamics and evolution is well known. Since the number of their members can range from a few hundred to a thousand stars forming loose structures, it may be difficult to distinguish this population from field stars. Precise stellar positions and proper motions are employed in most open cluster identification methods. In the pre Gaia era, the most used catalogs of OCs containing their fundamental parameters and stellar membership are the New Catalogue of Optically Visible Open Clusters and Candidates [<xref ref-type="bibr" rid="B1">1</xref>] and The Milky Way Star clusters [<xref ref-type="bibr" rid="B2">2</xref>]. In the Gaia era, the <italic>Gaia</italic> Second Data Release (DR2) [<xref ref-type="bibr" rid="B3">3</xref>] dramatically transforms OCs studies. The parameters and members of most of the known open clusters reported in pre-Gaia catalogues have been improved [<xref ref-type="bibr" rid="B4">4</xref>]-[<xref ref-type="bibr" rid="B6">6</xref>] and many of them are found to be no real clusters [<xref ref-type="bibr" rid="B4">4</xref>]. Visual inspection of the stellar distributions in the sky and proper motion space [<xref ref-type="bibr" rid="B7">7</xref>]-[<xref ref-type="bibr" rid="B9">9</xref>], as well as blind searches in the Galactic disc using machine-learning methods [<xref ref-type="bibr" rid="B4">4</xref>][<xref ref-type="bibr" rid="B10">10</xref>]-[<xref ref-type="bibr" rid="B13">13</xref>], allow the systematic detection of new OCs and upgrade the census.</p>
      <p>The latest data set of <italic>Gaia</italic>, <italic>Gaia</italic> DR3 catalogue [<xref ref-type="bibr" rid="B14">14</xref>], builds upon the <italic>Gaia</italic> Early Data Release 3 (EDR3) [<xref ref-type="bibr" rid="B15">15</xref>] and improves parallax precisions by 30% and proper motion precisions by a factor of 2 with respect to <italic>Gaia</italic> DR2. It has led to the broadening of the OCs census and make new discoveries, such as the studies of Li <italic>et al.</italic> (2022) [<xref ref-type="bibr" rid="B16">16</xref>], Hao <italic>et al.</italic> (2022) [<xref ref-type="bibr" rid="B17">17</xref>], and Castro-Ginard <italic>et al.</italic> (2022) [<xref ref-type="bibr" rid="B18">18</xref>]; the latter refines the census in almost 50% of the known OCs population. Recently, Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>] created a catalogue of clusters using <italic>Gaia</italic> DR3 data down to magnitude <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> G </mml:mi><mml:mo> ~ </mml:mo><mml:mn> 20 </mml:mn></mml:mrow></mml:math></inline-formula> which contains 4105 highly reliable clusters, 739 of which are new ones.</p>
      <p>The region of Cyg OB2 association, the most massive OB association within 2 kpc distance of the Sun, contains a complex spatial structure along the line of sight with several stellar groupings: Cyg OB2 association, Left and Right over-densities found by Orellana <italic>et al.</italic> (2021) [<xref ref-type="bibr" rid="B9">9</xref>] and many open clusters. These OCs have been investigated by Cantat-Gaudin <italic>et al.</italic> (2020) [<xref ref-type="bibr" rid="B5">5</xref>], Castro-Ginard <italic>et al.</italic> (2020) [<xref ref-type="bibr" rid="B12">12</xref>], Dias <italic>et al.</italic> (2021) [<xref ref-type="bibr" rid="B6">6</xref>], Orellana <italic>et al.</italic> (2021) [<xref ref-type="bibr" rid="B9">9</xref>], Hao <italic>et al.</italic> (2022) [<xref ref-type="bibr" rid="B17">17</xref>] and Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>] (see <bold>Table</bold><bold>1</bold>).</p>
      <p>The aim of this work is to perform an elaborate census of the open clusters situated in the Cygnus OB2 region as well as to detect new ones taking profit of the high accuracy of <italic>Gaia</italic> DR3 data up to magnitude <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> G </mml:mi><mml:mo> = </mml:mo><mml:mn> 19.5 </mml:mn></mml:mrow></mml:math></inline-formula> mag. For each OC, the astrometric parameters are determined and their members are identified. In addition, the physical parameters such as age and reddening value are investigated. </p>
      <p>This paper is organized as follows. Section 2 describes the data used in this work. In Section 3 we describe the procedure employed to detect the OCs located in the Cygnus OB2 region. Results are presented in Section 4. Our conclusions are summarised in Section 5.</p>
    </sec>
    <sec id="sec2">
      <title>2. Data</title>
      <p><italic>Gaia</italic> is the current astrometry mission of the European Space Agency (ESA), continuing the success of the Hipparcos mission. Its third release of data, <italic>Gaia</italic> DR3 includes the astrometric solution for 1468 million sources, with a limiting magnitude of about <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> G </mml:mi><mml:mo> ~ </mml:mo><mml:mn> 21 </mml:mn></mml:mrow></mml:math></inline-formula> and a bright limit of about <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> G </mml:mi><mml:mo> ~ </mml:mo><mml:mn> 3 </mml:mn></mml:mrow></mml:math></inline-formula> .</p>
      <p><bold>T</bold><bold>able 1.</bold>Position, mean proper motion and parallax of the known OCs determined by different authors. </p>
      <table-wrap id="tbl1">
        <label>Table 1</label>
        <table>
          <tbody>
            <tr>
              <td rowspan="2">Open Cluster</td>
              <td>
                <inline-formula>
                  <mml:math display="inline">
                    <mml:mrow>
                      <mml:msub>
                        <mml:mi>α</mml:mi>
                        <mml:mi>c</mml:mi>
                      </mml:msub>
                    </mml:mrow>
                  </mml:math>
                </inline-formula>
              </td>
              <td>
                <inline-formula>
                  <mml:math display="inline">
                    <mml:mrow>
                      <mml:msub>
                        <mml:mi>δ</mml:mi>
                        <mml:mi>c</mml:mi>
                      </mml:msub>
                    </mml:mrow>
                  </mml:math>
                </inline-formula>
              </td>
              <td>
                <inline-formula>
                  <mml:math display="inline">
                    <mml:mrow>
                      <mml:msub>
                        <mml:mi>μ</mml:mi>
                        <mml:mi>α</mml:mi>
                      </mml:msub>
                      <mml:mi>cos</mml:mi>
                      <mml:msub>
                        <mml:mi>δ</mml:mi>
                        <mml:mi>c</mml:mi>
                      </mml:msub>
                    </mml:mrow>
                  </mml:math>
                </inline-formula>
              </td>
              <td>
                <inline-formula>
                  <mml:math display="inline">
                    <mml:mrow>
                      <mml:msub>
                        <mml:mi>μ</mml:mi>
                        <mml:mrow>
                          <mml:msub>
                            <mml:mi>δ</mml:mi>
                            <mml:mi>c</mml:mi>
                          </mml:msub>
                        </mml:mrow>
                      </mml:msub>
                    </mml:mrow>
                  </mml:math>
                </inline-formula>
              </td>
              <td>
                <inline-formula>
                  <mml:math display="inline">
                    <mml:mrow>
                      <mml:msub>
                        <mml:mi>ϖ</mml:mi>
                        <mml:mi>c</mml:mi>
                      </mml:msub>
                    </mml:mrow>
                  </mml:math>
                </inline-formula>
              </td>
              <td rowspan="2">Reference</td>
            </tr>
            <tr>
              <td>[deg]</td>
              <td>[deg]</td>
              <td>[mas/yr]</td>
              <td>[mas/yr]</td>
              <td>[mas]</td>
            </tr>
            <tr>
              <td rowspan="3">Dolidze 8</td>
              <td>306.129</td>
              <td>42.300</td>
              <td>−2.633 ± 0.190</td>
              <td>−5.910 ± 0.195</td>
              <td>0.993 ± 0.063</td>
              <td>
                [
                <xref ref-type="bibr" rid="B5">5</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>306.117</td>
              <td>42.299</td>
              <td>−2.661 ± 0.191</td>
              <td>−6.033 ± 0.253</td>
              <td>0.986 ± 0.059</td>
              <td>
                [
                <xref ref-type="bibr" rid="B6">6</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>306.126</td>
              <td>42.290</td>
              <td>−2.540 ± 0.216</td>
              <td>−6.207 ± 0.232</td>
              <td>1.020 ± 0.057</td>
              <td>
                [
                <xref ref-type="bibr" rid="B19">19</xref>
                ]
              </td>
            </tr>
            <tr>
              <td rowspan="3">Roslund 6</td>
              <td>307.185</td>
              <td>39.798</td>
              <td>5.875 ± 0.340</td>
              <td>2.155 ± 0.274</td>
              <td>2.809 ± 0.076</td>
              <td>
                [
                <xref ref-type="bibr" rid="B5">5</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>307.128</td>
              <td>39.730</td>
              <td>5.919 ± 0.344</td>
              <td>2.175 ± 0.285</td>
              <td>2.816 ± 0.088</td>
              <td>
                [
                <xref ref-type="bibr" rid="B6">6</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>307.593</td>
              <td>40.356</td>
              <td>5.950 ± 0.275</td>
              <td>2.130 ± 0.231</td>
              <td>2.831 ± 0.062</td>
              <td>
                [
                <xref ref-type="bibr" rid="B19">19</xref>
                ]
              </td>
            </tr>
            <tr>
              <td rowspan="3">Cr421</td>
              <td>305.829</td>
              <td>41.701</td>
              <td>−3.651 ± 0.123</td>
              <td>−8.334 ± 0.113</td>
              <td>0.813 ± 0.048</td>
              <td>
                [
                <xref ref-type="bibr" rid="B5">5</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>305.837</td>
              <td>41.703</td>
              <td>−3.651 ± 0.131</td>
              <td>−8.336 ± 0.128</td>
              <td>0.818 ± 0.062</td>
              <td>
                [
                <xref ref-type="bibr" rid="B6">6</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>305.817</td>
              <td>41.695</td>
              <td>−3.640 ± 0.115</td>
              <td>−8.372 ± 0.138</td>
              <td>0.831 ± 0.054</td>
              <td>
                [
                <xref ref-type="bibr" rid="B19">19</xref>
                ]
              </td>
            </tr>
            <tr>
              <td rowspan="3">NGC 6910</td>
              <td>305.797</td>
              <td>40.771</td>
              <td>−3.415 ± 0.150</td>
              <td>−5.359 ± 0.164</td>
              <td>0.545 ± 0.052</td>
              <td>
                [
                <xref ref-type="bibr" rid="B5">5</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>305.789</td>
              <td>40.767</td>
              <td>−3.431 ± 0.170</td>
              <td>−5.373 ± 0.151</td>
              <td>0.539 ± 0.054</td>
              <td>
                [
                <xref ref-type="bibr" rid="B6">6</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>305.802</td>
              <td>40.774</td>
              <td>−3.296 ± 0.174</td>
              <td>−5.423 ± 0.021</td>
              <td>0.569 ± 0.031</td>
              <td>
                [
                <xref ref-type="bibr" rid="B19">19</xref>
                ]
              </td>
            </tr>
            <tr>
              <td rowspan="4">UBC 585</td>
              <td>306.986</td>
              <td>40.558</td>
              <td>−2.819 ± 0.056</td>
              <td>−5.520 ± 0.063</td>
              <td>0.663 ± 0.017</td>
              <td>
                [
                <xref ref-type="bibr" rid="B12">12</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>307.000</td>
              <td>40.548</td>
              <td>−2.829 ± 0.048</td>
              <td>−5.528 ± 0.053</td>
              <td>0.663 ± 0.015</td>
              <td>
                [
                <xref ref-type="bibr" rid="B5">5</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>306.998</td>
              <td>40.542</td>
              <td>−2.830 ± 0.070</td>
              <td>−5.500 ± 0.070</td>
              <td>0.690 ± 0.025</td>
              <td>
                [
                <xref ref-type="bibr" rid="B9">9</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>306.964</td>
              <td>40.555</td>
              <td>−2.852 ± 0.076</td>
              <td>−5.544 ± 0.123</td>
              <td>0.675 ± 0.027</td>
              <td>
                [
                <xref ref-type="bibr" rid="B19">19</xref>
                ]
              </td>
            </tr>
            <tr>
              <td rowspan="2">FSR 0238</td>
              <td>308.693</td>
              <td>41.417</td>
              <td>−2.902 ± 0.177</td>
              <td>−4.547 ± 0.127</td>
              <td>0.596 ± 0.059</td>
              <td>
                [
                <xref ref-type="bibr" rid="B5">5</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>308.710</td>
              <td>41.476</td>
              <td>0.198 ± 0.288</td>
              <td>−3.206 ± 0.138</td>
              <td>0.736 ± 0.046</td>
              <td>
                [
                <xref ref-type="bibr" rid="B19">19</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>FSR 0236</td>
              <td>308.168</td>
              <td>41.442</td>
              <td>−2.491 ± 0.394</td>
              <td>−4.076 ± 0.243</td>
              <td>0.522 ± 0.163</td>
              <td>
                [
                <xref ref-type="bibr" rid="B6">6</xref>
                ]
              </td>
            </tr>
            <tr>
              <td rowspan="2">OC-124</td>
              <td>306.448</td>
              <td>40.911</td>
              <td>−3.017 ± 0.223</td>
              <td>−4.558 ± 0.440</td>
              <td>0.546 ± 0.026</td>
              <td>
                [
                <xref ref-type="bibr" rid="B17">17</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>306.438</td>
              <td>40.924</td>
              <td>−3.115 ± 0.073</td>
              <td>−4.137 ± 0.064</td>
              <td>0.491 ± 0.028</td>
              <td>
                [
                <xref ref-type="bibr" rid="B19">19</xref>
                ]
              </td>
            </tr>
            <tr>
              <td rowspan="2">OC-123</td>
              <td>306.321</td>
              <td>40.793</td>
              <td>−3.005 ± 0.176</td>
              <td>−4.828 ± 0.319</td>
              <td>0.551 ± 0.026</td>
              <td>
                [
                <xref ref-type="bibr" rid="B17">17</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>306.356</td>
              <td>40.895</td>
              <td>−3.047 ± 0.077</td>
              <td>−4.733 ± 0.136</td>
              <td>0.547 ± 0.025</td>
              <td>
                [
                <xref ref-type="bibr" rid="B19">19</xref>
                ]
              </td>
            </tr>
            <tr>
              <td rowspan="2">OC-128</td>
              <td>308.029</td>
              <td>40.857</td>
              <td>−2.835 ± 0.303</td>
              <td>−4.526 ± 0.372</td>
              <td>0.580 ± 0.032</td>
              <td>
                [
                <xref ref-type="bibr" rid="B17">17</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>307.939</td>
              <td>40.741</td>
              <td>−3.039 ± 0.130</td>
              <td>−4.348 ± 0.138</td>
              <td>0.574 ± 0.029</td>
              <td>
                [
                <xref ref-type="bibr" rid="B19">19</xref>
                ]
              </td>
            </tr>
            <tr>
              <td rowspan="2">FSR 0224</td>
              <td>306.351</td>
              <td>40.224</td>
              <td>−3.242 ± 0.343</td>
              <td>−4.373 ± 0.268</td>
              <td>0.566 ± 0.068</td>
              <td>
                [
                <xref ref-type="bibr" rid="B6">6</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>306.339</td>
              <td>40.220</td>
              <td>−3.162 ± 0.069</td>
              <td>−4.327 ± 0.072</td>
              <td>0.574 ± 0.026</td>
              <td>
                [
                <xref ref-type="bibr" rid="B19">19</xref>
                ]
              </td>
            </tr>
            <tr>
              <td rowspan="2">Dolidze 11</td>
              <td>306.682</td>
              <td>41.372</td>
              <td>−1.255 ± 0.109</td>
              <td>−4.260 ± 0.184</td>
              <td>0.490 ± 0.092</td>
              <td>
                [
                <xref ref-type="bibr" rid="B5">5</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>306.691</td>
              <td>41.376</td>
              <td>−1.214 ± 0.194</td>
              <td>−4.133 ± 0.201</td>
              <td>0.471 ± 0.070</td>
              <td>
                [
                <xref ref-type="bibr" rid="B19">19</xref>
                ]
              </td>
            </tr>
            <tr>
              <td rowspan="2">Bica 2</td>
              <td>308.315</td>
              <td>41.307</td>
              <td>−2.660 ± 0.244</td>
              <td>−4.378 ± 0.230</td>
              <td>0.555 ± 0.102</td>
              <td>
                [
                <xref ref-type="bibr" rid="B6">6</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>308.319</td>
              <td>41.301</td>
              <td>−2.691 ± 0.107</td>
              <td>−4.413 ± 0.108</td>
              <td>0.576 ± 0.024</td>
              <td>
                [
                <xref ref-type="bibr" rid="B19">19</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>HSC 618</td>
              <td>306.745</td>
              <td>40.053</td>
              <td>−1.997 ± 0.166</td>
              <td>−3.963 ± 0.251</td>
              <td>1.015 ± 0.040</td>
              <td>
                [
                <xref ref-type="bibr" rid="B19">19</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>HSC 625</td>
              <td>308.198</td>
              <td>40.838</td>
              <td>−2.601 ± 0.085</td>
              <td>−4.900 ± 0.098</td>
              <td>0.574 ± 0.026</td>
              <td>
                [
                <xref ref-type="bibr" rid="B19">19</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>HSC 626</td>
              <td>306.691</td>
              <td>41.669</td>
              <td>−3.102 ± 0.077</td>
              <td>−4.680 ± 0.101</td>
              <td>0.535 ± 0.035</td>
              <td>
                [
                <xref ref-type="bibr" rid="B19">19</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>HSC 630</td>
              <td>307.710</td>
              <td>41.449</td>
              <td>−2.007 ± 0.058</td>
              <td>−2.918 ± 0.114</td>
              <td>0.751 ± 0.033</td>
              <td>
                [
                <xref ref-type="bibr" rid="B19">19</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>FSR 0227</td>
              <td>307.250</td>
              <td>40.486</td>
              <td>−1.838 ± 0.145</td>
              <td>−4.584 ± 0.106</td>
              <td>0.497 ± 0.037</td>
              <td>
                [
                <xref ref-type="bibr" rid="B19">19</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>HSC 624</td>
              <td>307.284</td>
              <td>41.264</td>
              <td>−2.542 ± 0.122</td>
              <td>−3.459 ± 0.365</td>
              <td>0.598 ± 0.028</td>
              <td>
                [
                <xref ref-type="bibr" rid="B19">19</xref>
                ]
              </td>
            </tr>
            <tr>
              <td>IRAS-20306+4005</td>
              <td>308.059</td>
              <td>40.292</td>
              <td>−1.811 ± 0.259</td>
              <td>−3.997 ± 0.162</td>
              <td>1.009 ± 0.098</td>
              <td>
                [
                <xref ref-type="bibr" rid="B19">19</xref>
                ]
              </td>
            </tr>
          </tbody>
        </table>
      </table-wrap>
      <p>The astrometric parameters used in this work are position, parallax, and proper motion, referred to the ICRS at reference epoch J2016.0 [<xref ref-type="bibr" rid="B14">14</xref>]. The median uncertainty in parallax and position at the reference epoch J2016.0 is about 0.01 - 0.02 mas for <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> G </mml:mi><mml:mo> &lt; </mml:mo><mml:mn> 15 </mml:mn></mml:mrow></mml:math></inline-formula> mag, 0.05 mas for <inline-formula><mml:math display="inline"><mml:mrow><mml:mn> 15 </mml:mn><mml:mo> &lt; </mml:mo><mml:mi> G </mml:mi><mml:mo> &lt; </mml:mo><mml:mn> 17 </mml:mn></mml:mrow></mml:math></inline-formula> mag, 0.4 mas for <inline-formula><mml:math display="inline"><mml:mrow><mml:mn> 17 </mml:mn><mml:mo> &lt; </mml:mo><mml:mi> G </mml:mi><mml:mo> &lt; </mml:mo><mml:mn> 20 </mml:mn></mml:mrow></mml:math></inline-formula> mag and 1.0 mas at <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> G </mml:mi><mml:mo> = </mml:mo><mml:mn> 21 </mml:mn></mml:mrow></mml:math></inline-formula> mag. Referred to the proper motion components, the corresponding uncertainties are 0.02 - 0.03 mas yr<sup>−</sup><sup>1</sup> for <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> G </mml:mi><mml:mo> &lt; </mml:mo><mml:mn> 15 </mml:mn></mml:mrow></mml:math></inline-formula> mag, 0.07 mas yr<sup>−</sup><sup>1</sup> for <inline-formula><mml:math display="inline"><mml:mrow><mml:mn> 15 </mml:mn><mml:mo> &lt; </mml:mo><mml:mi> G </mml:mi><mml:mo> &lt; </mml:mo><mml:mn> 17 </mml:mn></mml:mrow></mml:math></inline-formula> mag, 0.5 mas yr<sup>−</sup><sup>1</sup> for <inline-formula><mml:math display="inline"><mml:mrow><mml:mn> 17 </mml:mn><mml:mo> &lt; </mml:mo><mml:mi> G </mml:mi><mml:mo> &lt; </mml:mo><mml:mn> 20 </mml:mn></mml:mrow></mml:math></inline-formula> mag and 1.4 mas yr<sup>−</sup><sup>1</sup> at <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> G </mml:mi><mml:mo> = </mml:mo><mml:mn> 21 </mml:mn></mml:mrow></mml:math></inline-formula> mag [<xref ref-type="bibr" rid="B20">20</xref>]. The photometric data employed in this research are the <italic>Gaia</italic> DR3 bands (<inline-formula><mml:math display="inline"><mml:mi> G </mml:mi></mml:math></inline-formula> , <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> G </mml:mi><mml:mrow><mml:mi> B </mml:mi><mml:mi> P </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> , and <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> G </mml:mi><mml:mrow><mml:mi> R </mml:mi><mml:mi> P </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> ) and the near-infrared (NIR) bands (<inline-formula><mml:math display="inline"><mml:mrow><mml:mi> J </mml:mi><mml:mi> H </mml:mi><mml:mi> K </mml:mi></mml:mrow></mml:math></inline-formula> ) from the Two Micron All Sky Survey (2MASS) [<xref ref-type="bibr" rid="B21">21</xref>]. The photometric errors are those provided by the respective catalogue being <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> σ </mml:mi><mml:mi> G </mml:mi></mml:msub><mml:mo> ≤ </mml:mo><mml:mn> 0.01 </mml:mn></mml:mrow></mml:math></inline-formula> mag, <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> σ </mml:mi><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> B </mml:mi><mml:mi> P </mml:mi><mml:mo> − </mml:mo><mml:mi> R </mml:mi><mml:mi> P </mml:mi></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo> ≤ </mml:mo><mml:mn> 0.1 </mml:mn></mml:mrow></mml:math></inline-formula> mag and <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> σ </mml:mi><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> J </mml:mi><mml:mi> H </mml:mi><mml:mi> K </mml:mi></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo> ≤ </mml:mo><mml:mn> 0.05 </mml:mn></mml:mrow></mml:math></inline-formula> mag.</p>
      <p>A detailed description about the construction of <italic>Gaia</italic> DR3 catalogue can be found in [<xref ref-type="bibr" rid="B14">14</xref>]. Data extraction has been performed using the VizieR catalogue database of the Strasbourg astronomical Data Center (CDS).</p>
    </sec>
    <sec id="sec3">
      <title>3. Open Cluster Identification, Membership Determination and Physical Parameters Estimation</title>
      <sec id="sec3dot1">
        <title>3.1. The Sample</title>
        <p>We select the stars in a circular region with centre at <inline-formula><mml:math display="inline"><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> l </mml:mi><mml:mn> , </mml:mn><mml:mi> b </mml:mi></mml:mrow><mml:mo> ) </mml:mo></mml:mrow><mml:mo> = </mml:mo><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:msup><mml:mrow><mml:mn> 79.8 </mml:mn></mml:mrow><mml:mo> ∘ </mml:mo></mml:msup><mml:mn> , </mml:mn><mml:mo> + </mml:mo><mml:msup><mml:mrow><mml:mn> 0.8 </mml:mn></mml:mrow><mml:mo> ∘ </mml:mo></mml:msup></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> of radius 1.5˚ taking into account the following criteria: 1) The values of the proper motions components are <inline-formula><mml:math display="inline"><mml:mrow><mml:mo> − </mml:mo><mml:mn> 5 </mml:mn><mml:mo> &lt; </mml:mo><mml:msub><mml:mi> μ </mml:mi><mml:mi> α </mml:mi></mml:msub><mml:mi> cos </mml:mi><mml:mi> δ </mml:mi><mml:mo> &lt; </mml:mo><mml:mn> 5 </mml:mn></mml:mrow></mml:math></inline-formula> mas yr<sup>−</sup><sup>1</sup>, <inline-formula><mml:math display="inline"><mml:mrow><mml:mo> − </mml:mo><mml:mn> 10 </mml:mn><mml:mo> &lt; </mml:mo><mml:msub><mml:mi> μ </mml:mi><mml:mi> δ </mml:mi></mml:msub><mml:mo> &lt; </mml:mo><mml:mn> 0 </mml:mn></mml:mrow></mml:math></inline-formula> mas yr<sup>−</sup><sup>1</sup> (except the case of Roslund 6 whose proper motion values are <inline-formula><mml:math display="inline"><mml:mrow><mml:mo> − </mml:mo><mml:mn> 1 </mml:mn><mml:mo> &lt; </mml:mo><mml:msub><mml:mi> μ </mml:mi><mml:mi> α </mml:mi></mml:msub><mml:mi> cos </mml:mi><mml:mi> δ </mml:mi><mml:mo> &lt; </mml:mo><mml:mn> 10 </mml:mn></mml:mrow></mml:math></inline-formula> mas yr<sup>−</sup><sup>1</sup> , <inline-formula><mml:math display="inline"><mml:mrow><mml:mo> − </mml:mo><mml:mn> 1 </mml:mn><mml:mo> &lt; </mml:mo><mml:msub><mml:mi> μ </mml:mi><mml:mi> δ </mml:mi></mml:msub><mml:mo> &lt; </mml:mo><mml:mn> 10 </mml:mn></mml:mrow></mml:math></inline-formula> mas yr<sup>−</sup><sup>1</sup> ) because a visual inspection of the Vector Point Diagram (VPD) of the region showed low proper motions for the possible OCs candidates. 2) The stars having the Dup value in the catalogue equal to 1 are not selected because they have multiple source identifiers. 3) The parallax values adopted are <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> ϖ </mml:mi><mml:mn><mml:mo> &gt; </mml:mo>0.4 </mml:mn></mml:mrow></mml:math></inline-formula> mas. This is based on the range of observed parallaxes in region by Orellana <italic>et al.</italic> (2021) [<xref ref-type="bibr" rid="B9">9</xref>]. 4) Stellar parallaxes having fractional error <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> f </mml:mi><mml:mo> = </mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mi> σ </mml:mi><mml:mi> ϖ </mml:mi></mml:msub></mml:mrow><mml:mi> ϖ </mml:mi></mml:mfrac><mml:mo> &gt; </mml:mo><mml:mn> 0.20 </mml:mn></mml:mrow></mml:math></inline-formula> are excluded. This restriction reduces the problems in the transformation of parallax to distance. 5) The stars with RUWE parameter ≤ 1.4 [<xref ref-type="bibr" rid="B22">22</xref>] are selected because this value is a quality indicator of the astrometric solution. The final sample consists of 23,106 stars with <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> G </mml:mi><mml:mo> ≤ </mml:mo><mml:mn> 19.5 </mml:mn></mml:mrow></mml:math></inline-formula> mag, this cutoff in the magnitude is due to the adopted value of the fractional error.</p>
      </sec>
      <sec id="sec3dot2">
        <title>3.2. Astrometric Analysis</title>
        <p>3.2.1. HDBSCAN Algorithm</p>
        <p>We apply the HDBSCAN (Hierarchical Density Based Spatial Clustering of Applications with Noise) clustering algorithm [<xref ref-type="bibr" rid="B23">23</xref>] to the <italic>Gaia</italic> DR3 astrometric parameters (<inline-formula><mml:math display="inline"><mml:mi> α </mml:mi></mml:math></inline-formula> , <inline-formula><mml:math display="inline"><mml:mi> δ </mml:mi></mml:math></inline-formula> , <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> μ </mml:mi><mml:mi> α </mml:mi></mml:msub><mml:mi> cos </mml:mi><mml:mi> δ </mml:mi></mml:mrow></mml:math></inline-formula> , <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> μ </mml:mi><mml:mi> δ </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> , <inline-formula><mml:math display="inline"><mml:mi> ϖ </mml:mi></mml:math></inline-formula> ) to detect the clusters and their members in the Cygnus OB2 region. HDBSCAN is an unsupervised learning tool that allows us to identify stellar groups with different density and shape. This algorithm can work with multidimensional data, which must be previously normalized. Normalization allows us to compare different astrometric parameters and make inferences about their distribution. When the entire set of parameters is on the same scale, it is possible to identify and visualize the relationships between them and make meaningful comparisons. In this work, we use Min-Max scaling which transforms the values of each set of parameters between 0 and 1 by</p>
        <disp-formula id="FD1">
          <label>(1)</label>
          <mml:math display="inline">
            <mml:mrow>
              <mml:msub>
                <mml:mi>x</mml:mi>
                <mml:mrow>
                  <mml:mi>s</mml:mi>
                  <mml:mi>c</mml:mi>
                  <mml:mi>a</mml:mi>
                  <mml:mi>l</mml:mi>
                  <mml:mi>e</mml:mi>
                  <mml:mi>d</mml:mi>
                </mml:mrow>
              </mml:msub>
              <mml:mo>=</mml:mo>
              <mml:mfrac>
                <mml:mrow>
                  <mml:mi>x</mml:mi>
                  <mml:mo>−</mml:mo>
                  <mml:mi>min</mml:mi>
                  <mml:mrow>
                    <mml:mo>(</mml:mo>
                    <mml:mi>x</mml:mi>
                    <mml:mo>)</mml:mo>
                  </mml:mrow>
                </mml:mrow>
                <mml:mrow>
                  <mml:mi>max</mml:mi>
                  <mml:mrow>
                    <mml:mo>(</mml:mo>
                    <mml:mi>x</mml:mi>
                    <mml:mo>)</mml:mo>
                  </mml:mrow>
                  <mml:mo>−</mml:mo>
                  <mml:mi>min</mml:mi>
                  <mml:mrow>
                    <mml:mo>(</mml:mo>
                    <mml:mi>x</mml:mi>
                    <mml:mo>)</mml:mo>
                  </mml:mrow>
                </mml:mrow>
              </mml:mfrac>
              <mml:mo>,</mml:mo>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>where <inline-formula><mml:math display="inline"><mml:mi> x </mml:mi></mml:math></inline-formula> is the original value of the astrometric parameter; <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> min </mml:mi><mml:mrow><mml:mo> ( </mml:mo><mml:mi> x </mml:mi><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> max </mml:mi><mml:mrow><mml:mo> ( </mml:mo><mml:mi> x </mml:mi><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> are the minimum and maximum values of the parameter in its dataset, respectively and <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> x </mml:mi><mml:mrow><mml:mi> s </mml:mi><mml:mi> c </mml:mi><mml:mi> a </mml:mi><mml:mi> l </mml:mi><mml:mi> e </mml:mi><mml:mi> d </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> is the normalized value of the parameter.</p>
        <p>The algorithm requires a metric that calculates the distance between points in the normalized dataset to identify the different densities. The Euclidean metric is the most commonly used [<xref ref-type="bibr" rid="B24">24</xref>].</p>
        <p>HDBSCAN needs two hyperparameters previously defined to be executed [<xref ref-type="bibr" rid="B23">23</xref>]: <italic>minimum number of samples</italic> (mPts) and <italic>minimum cluster size</italic> (mcSize). One of them, mPts, defines the minimum number of neighbouring stars that any star must have to be considered in a grouping. The other hyperparameter, mcSize, is the minimum number of stars required to define a cluster. Different combinations of these hyperparameters give different sizes of clusters. Thus: 1) small <italic>minimum number of samples</italic> and <italic>minimum cluster size</italic> results in many small clusters; 2) small <italic>minimun number of samples</italic> and large <italic>minimun cluster size</italic> results in larger clusters and 3) a large <italic>minimun number of samples</italic> and large <italic>minimun cluster size</italic> results in very large clusters.</p>
        <p>Besides, the HDBSCAN algorithm has the disadvantage of identifying false clusters. The identification of real clusters is carried out by adopting the following empirical criteria proposed by Hunt &amp; Reffert (2021) [<xref ref-type="bibr" rid="B25">25</xref>]:</p>
        <p>a) the dispersion of the total proper motion of their members must satisfy</p>
        <disp-formula id="FD2">
          <label>(2)</label>
          <mml:math display="inline">
            <mml:mrow>
              <mml:msqrt>
                <mml:mrow>
                  <mml:msubsup>
                    <mml:mi>σ</mml:mi>
                    <mml:mrow>
                      <mml:msub>
                        <mml:mi>μ</mml:mi>
                        <mml:mi>α</mml:mi>
                      </mml:msub>
                      <mml:mi>cos</mml:mi>
                      <mml:mi>δ</mml:mi>
                    </mml:mrow>
                    <mml:mn>2</mml:mn>
                  </mml:msubsup>
                  <mml:mo>+</mml:mo>
                  <mml:msubsup>
                    <mml:mi>σ</mml:mi>
                    <mml:mrow>
                      <mml:msub>
                        <mml:mi>μ</mml:mi>
                        <mml:mi>δ</mml:mi>
                      </mml:msub>
                    </mml:mrow>
                    <mml:mn>2</mml:mn>
                  </mml:msubsup>
                </mml:mrow>
              </mml:msqrt>
              <mml:mo>≤</mml:mo>
              <mml:mrow>
                <mml:mo>{</mml:mo>
                <mml:mrow>
                  <mml:mtable columnalign="left">
                    <mml:mtr columnalign="left">
                      <mml:mtd columnalign="left">
                        <mml:mrow>
                          <mml:mn>1</mml:mn>
                          <mml:mtext>
                             
                          </mml:mtext>
                          <mml:mtext>mas</mml:mtext>
                          <mml:mo>⋅</mml:mo>
                          <mml:msup>
                            <mml:mrow>
                              <mml:mtext>yr</mml:mtext>
                            </mml:mrow>
                            <mml:mrow>
                              <mml:mo>−</mml:mo>
                              <mml:mn>1</mml:mn>
                            </mml:mrow>
                          </mml:msup>
                        </mml:mrow>
                      </mml:mtd>
                      <mml:mtd columnalign="left">
                        <mml:mrow>
                          <mml:mtext>if</mml:mtext>
                          <mml:mtext>
                             
                          </mml:mtext>
                          <mml:mi>ϖ</mml:mi>
                          <mml:mo>≤</mml:mo>
                          <mml:mn>0.67</mml:mn>
                          <mml:mtext>
                             
                          </mml:mtext>
                          <mml:mtext>mas</mml:mtext>
                        </mml:mrow>
                      </mml:mtd>
                    </mml:mtr>
                    <mml:mtr columnalign="left">
                      <mml:mtd columnalign="left">
                        <mml:mrow>
                          <mml:mn>1.49</mml:mn>
                          <mml:mo>⋅</mml:mo>
                          <mml:mi>ϖ</mml:mi>
                          <mml:mtext>
                             
                          </mml:mtext>
                          <mml:mtext>mas</mml:mtext>
                          <mml:mo>⋅</mml:mo>
                          <mml:msup>
                            <mml:mrow>
                              <mml:mtext>yr</mml:mtext>
                            </mml:mrow>
                            <mml:mrow>
                              <mml:mo>−</mml:mo>
                              <mml:mn>1</mml:mn>
                            </mml:mrow>
                          </mml:msup>
                        </mml:mrow>
                      </mml:mtd>
                      <mml:mtd columnalign="left">
                        <mml:mrow>
                          <mml:mtext>if</mml:mtext>
                          <mml:mtext>
                             
                          </mml:mtext>
                          <mml:mi>ϖ</mml:mi>
                          <mml:mo>&gt;</mml:mo>
                          <mml:mn>0.67</mml:mn>
                          <mml:mtext>
                             
                          </mml:mtext>
                          <mml:mtext>mas</mml:mtext>
                          <mml:mn>
                            <mml:mo>;</mml:mo>
                          </mml:mn>
                        </mml:mrow>
                      </mml:mtd>
                    </mml:mtr>
                  </mml:mtable>
                </mml:mrow>
              </mml:mrow>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>b) the radius of the open cluster containing half of its members (<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> r </mml:mi><mml:mrow><mml:mn> 50 </mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> ) must be less than 20 pc;</p>
        <p>c) those candidates that have a density compatible with the field stars are discarded. This is implemented by calculating the distance from each star to its ninth nearest neighbour.</p>
        <p>In order to determine the optimal values of mPts and mcSize to detect the OCs, and setting mPts and mcSize to the same value as recommended by Campello <italic>et al.</italic> (2013) [<xref ref-type="bibr" rid="B23">23</xref>], several runs of HDBSCAN are performed using different combinations of these hyperparameters, both values are in the 5 - 80 range.</p>
        <p>Then, for each pair mPts-mcSize we evaluate if the different clusters fulfil a), b) and c) criteria in order to obtain well-characterized OCs.</p>
        <p>3.2.2. Stellar Membership Determination and Cluster Parameters </p>
        <p>A probable cluster member is found when its HDBSCAN membership probability is <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> P </mml:mi><mml:mo> ≥ </mml:mo><mml:mn> 0.5 </mml:mn></mml:mrow></mml:math></inline-formula> , following the Bayes minimum error rate decision rule [<xref ref-type="bibr" rid="B26">26</xref>]. The number of stars that fulfil this condition is the number of members <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> , and their coordinates guide to compute the cluster radius <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> r </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> .</p>
        <p>Among the <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> members, we define as the highly probable members <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> those with <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> P </mml:mi><mml:mo> ≥ </mml:mo><mml:mn> 0.80 </mml:mn></mml:mrow></mml:math></inline-formula> . These <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> lead to calculate the coordinates of the cluster centre (<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> α </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> , <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> δ </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> ), the components of the mean proper motion (<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> μ </mml:mi><mml:mi> α </mml:mi></mml:msub><mml:mi> cos </mml:mi><mml:msub><mml:mi> δ </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> , <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> μ </mml:mi><mml:mrow><mml:msub><mml:mi> δ </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> ), and calculate the mean value of the parallaxes of the members weighed for their squared uncertainty <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> ϖ </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> . An estimation of the distance <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> d </mml:mi><mml:mrow><mml:msub><mml:mi> ϖ </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> is calculated by the inverse of <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> ϖ </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> , taking into account the general offset of −0.017 mas [<xref ref-type="bibr" rid="B20">20</xref>].</p>
      </sec>
      <sec id="sec3dot3">
        <title>3.3. Photometric Analysis</title>
        <p>With the goal to know some physical parameters of the clusters found from the proper motion and parallax analysis, we add the study of colour-magnitude diagram (CMD) with <italic>Gaia</italic> photometric data.</p>
        <p>Since Cygnus OB2 is one of the major stellar formation region, it is important to distinguish whether the red colour of each star is due to dust present in the line of sight or it is inherent to the star itself. To achieve this, we cross-match the optical <italic>Gaia</italic> data of the stars identified as cluster members with the near-infrared (NIR) photometric data from the 2MASS catalogue (<italic>JHK</italic> bands). For this, we take a maximum angular distance of 1''. Then, using the NIR photometric data, we calculate the reddening-free photometric parameter <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> Q </mml:mi><mml:mrow><mml:mi> N </mml:mi><mml:mi> I </mml:mi><mml:mi> R </mml:mi></mml:mrow></mml:msub><mml:mo> = </mml:mo><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> J </mml:mi><mml:mo> − </mml:mo><mml:mi> H </mml:mi></mml:mrow><mml:mo> ) </mml:mo></mml:mrow><mml:mo> − </mml:mo><mml:mn> 1.7 </mml:mn><mml:mo> × </mml:mo><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> H </mml:mi><mml:mo> − </mml:mo><mml:mi> K </mml:mi></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> [<xref ref-type="bibr" rid="B27">27</xref>] to avoid any confusion arising from the intrinsic degeneracy between reddening and spectral type. We substantiate our star classification by analysing the <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> Q </mml:mi><mml:mrow><mml:mi> N </mml:mi><mml:mi> I </mml:mi><mml:mi> R </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> value on the guidelines provided by Borissova <italic>et al.</italic> (2012) [<xref ref-type="bibr" rid="B28">28</xref>] and Messineo <italic>et al.</italic> (2012) [<xref ref-type="bibr" rid="B29">29</xref>]. Then, <inline-formula><mml:math display="inline"><mml:mrow><mml:mo> − </mml:mo><mml:mn> 0.3 </mml:mn><mml:mo> &lt; </mml:mo><mml:msub><mml:mi> Q </mml:mi><mml:mrow><mml:mi> N </mml:mi><mml:mi> I </mml:mi><mml:mi> R </mml:mi></mml:mrow></mml:msub><mml:mo> &lt; </mml:mo><mml:mn> 0.5 </mml:mn></mml:mrow></mml:math></inline-formula> indicates early main sequence stars, <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> Q </mml:mi><mml:mrow><mml:mi> N </mml:mi><mml:mi> I </mml:mi><mml:mi> R </mml:mi></mml:mrow></mml:msub><mml:mo> &lt; </mml:mo><mml:mo> − </mml:mo><mml:mn> 0.3 </mml:mn></mml:mrow></mml:math></inline-formula> Pre-Main Sequence Stars (PMS) or Young Stellar Objects (YSO) and <inline-formula><mml:math display="inline"><mml:mrow><mml:mn> 0.5 </mml:mn><mml:mo> &lt; </mml:mo><mml:msub><mml:mi> Q </mml:mi><mml:mrow><mml:mi> N </mml:mi><mml:mi> I </mml:mi><mml:mi> R </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> late reddening stars.</p>
        <p>The extinction value (<inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi></mml:mrow></mml:math></inline-formula> ) for clusters is estimated using the new three-dimensional (3D) map of dust reddening, which integrates <italic>Gaia</italic> DR2 parallaxes, stellar photometry data from Pan-STARRS1 and 2MASS, and a hierarchical Bayesian model of dust distribution [<xref ref-type="bibr" rid="B30">30</xref>]. The <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi></mml:mrow></mml:math></inline-formula> value derived from this approach is applied in conjunction with the reddening law: <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> A </mml:mi><mml:mi> G </mml:mi></mml:msub><mml:mo> = </mml:mo><mml:mn> 0.83627 </mml:mn><mml:mi> A </mml:mi><mml:mi> v </mml:mi></mml:mrow></mml:math></inline-formula> , <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> A </mml:mi><mml:mrow><mml:mi> B </mml:mi><mml:mi> P </mml:mi></mml:mrow></mml:msub><mml:mo> = </mml:mo><mml:mn> 1.08337 </mml:mn><mml:mi> A </mml:mi><mml:mi> v </mml:mi></mml:mrow></mml:math></inline-formula> , and <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> A </mml:mi><mml:mrow><mml:mi> R </mml:mi><mml:mi> P </mml:mi></mml:mrow></mml:msub><mml:mo> = </mml:mo><mml:mn> 0.63439 </mml:mn><mml:mi> A </mml:mi><mml:mi> v </mml:mi></mml:mrow></mml:math></inline-formula> , to fit the appropriate isochrone. When the <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi></mml:mrow></mml:math></inline-formula> value appears to be inaccurate, we adopt an initial assumption of an <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi></mml:mrow></mml:math></inline-formula> that closely aligns with the values provided by Wright <italic>et al.</italic> (2015) [<xref ref-type="bibr" rid="B31">31</xref>]. Additionally, we consult the APASS<sup>1</sup> catalogue to obtain the <italic>V</italic> and <italic>B</italic> photometric data for each star, which are combined with JHK 2MASS bands to estimate the visual extinction for each cluster.</p>
        <p>The PARSEC v1.2S isochrones [<xref ref-type="bibr" rid="B32">32</xref>] are adjusted to the observed data in the photometric diagram <inline-formula><mml:math display="inline"><mml:mi> G </mml:mi></mml:math></inline-formula> vs (<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> G </mml:mi><mml:mrow><mml:mi> B </mml:mi><mml:mi> P </mml:mi></mml:mrow></mml:msub><mml:mo> − </mml:mo><mml:msub><mml:mi> G </mml:mi><mml:mrow><mml:mi> R </mml:mi><mml:mi> P </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> ). To achieve this, we consider the cluster’s distance derived from its parallax determination and adopt an initial value of visual absorption as explained previously, which sometimes requires refinement through successive isochrone adjustments. Estimating the age of the open cluster using broadband photometric data and a limited number of stellar members leads to less reliable results. For this reason, we fit multiple isochrones and in all of them we use solar metallicity as a fixed parameter. The true metallicity value of a cluster is determined through the spectral analysis of its individual members. For this reason, we consulted the spectroscopic catalogue by Fu <italic>et al.</italic> (2022) [<xref ref-type="bibr" rid="B33">33</xref>], in which the open cluster Collinder 421 is reported to have a metallicity index of [Fe/H] = −0.02 ± 0.04 dex, and the Qin <italic>et al.</italic> (2023) paper [<xref ref-type="bibr" rid="B34">34</xref>], where Roslund 6 is given a metallicity index of [Fe/H] = −0.01 ± 0.10 dex. Therefore, as a first approximation, solar-metallicity isochrones could be adopted for all the open clusters studied in the region. In the figures presenting the CMDs for each open cluster, we show the minimum and maximum values of the selected age range with solar metallicity isochrones.</p>
      </sec>
    </sec>
    <sec id="sec4">
      <title>4. Results</title>
      <sec id="sec4dot1">
        <title>4.1. Astrometric Results</title>
        <p>The astrometric analysis of the Cyg OB2 region is done following the procedure given in subsections 3.2.1 and 3.2.2. For different values of the hyperparameters (mPts-mcSize), the HDBSCAN algorithm is applied to the sample and several groupings are found. We evaluate if these groupings fulfill the empirical criteria a), b) and c) in order to detect OCs. Therefore, the values of the pair (mPts-mcSize) that well characterize the detected 24 OCs for each final run are given in <bold>Table</bold><bold>2</bold>.</p>
        <p><bold>Table</bold><bold>2.</bold> The pair (mPts-mcSize) that well characterize the detected 24 OCs.</p>
        <table-wrap id="tbl2">
          <label>Table 2</label>
          <table>
            <tbody>
              <tr>
                <td>OC</td>
                <td>mPts</td>
                <td>mcSize</td>
                <td>OC</td>
                <td>mPts</td>
                <td>mcSize</td>
              </tr>
              <tr>
                <td>Dolidze 8</td>
                <td>15</td>
                <td>15</td>
                <td>Dolidze 11</td>
                <td>15</td>
                <td>15</td>
              </tr>
              <tr>
                <td>IRAS-20306 + 4005</td>
                <td>15</td>
                <td>15</td>
                <td>NGC 6910</td>
                <td>15</td>
                <td>15</td>
              </tr>
              <tr>
                <td>Cr421</td>
                <td>15</td>
                <td>15</td>
                <td>UBC 585</td>
                <td>15</td>
                <td>15</td>
              </tr>
              <tr>
                <td>HSC 630</td>
                <td>15</td>
                <td>15</td>
                <td>HSC 618</td>
                <td>15</td>
                <td>15</td>
              </tr>
              <tr>
                <td>RSL-03</td>
                <td>5</td>
                <td>5</td>
                <td>HSC 625</td>
                <td>20</td>
                <td>20</td>
              </tr>
              <tr>
                <td>RSL-04</td>
                <td>10</td>
                <td>10</td>
                <td>HSC 626</td>
                <td>10</td>
                <td>10</td>
              </tr>
              <tr>
                <td>RSL-05</td>
                <td>5</td>
                <td>5</td>
                <td>FSR 0227</td>
                <td>15</td>
                <td>15</td>
              </tr>
              <tr>
                <td>RSL-06</td>
                <td>5</td>
                <td>5</td>
                <td>OC-123</td>
                <td>15</td>
                <td>15</td>
              </tr>
              <tr>
                <td>FSR 0238</td>
                <td>15</td>
                <td>15</td>
                <td>OC-128</td>
                <td>15</td>
                <td>15</td>
              </tr>
              <tr>
                <td>FSR 0236</td>
                <td>15</td>
                <td>15</td>
                <td>Bica 1</td>
                <td>15</td>
                <td>15</td>
              </tr>
              <tr>
                <td>OC-124</td>
                <td>15</td>
                <td>15</td>
                <td>Bica 2</td>
                <td>5</td>
                <td>5</td>
              </tr>
              <tr>
                <td>FSR 0224</td>
                <td>15</td>
                <td>15</td>
                <td>Roslund 6</td>
                <td>30</td>
                <td>30</td>
              </tr>
            </tbody>
          </table>
        </table-wrap>
        <p><xref ref-type="fig" rid="fig1">Figure 1</xref> shows the spatial distribution of all clusters identified in the line of sight of Cygnus OB2. <bold>Table</bold><bold>3</bold> shows the values of the cluster parameters found and defined in Subsection 3.2.2. A catalogue containing the position <inline-formula><mml:math display="inline"><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> α </mml:mi><mml:mn> , </mml:mn><mml:mi> δ </mml:mi></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> , the Gaia DR3 identifier, the parallax <inline-formula><mml:math display="inline"><mml:mi> ϖ </mml:mi></mml:math></inline-formula> and its error <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> σ </mml:mi><mml:mi> ϖ </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> , the proper motion components <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> μ </mml:mi><mml:mi> α </mml:mi></mml:msub><mml:mi> cos </mml:mi><mml:mi> δ </mml:mi></mml:mrow></mml:math></inline-formula> , <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> μ </mml:mi><mml:mi> δ </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and the <inline-formula><mml:math display="inline"><mml:mi> G </mml:mi></mml:math></inline-formula> magnitude of the members of each cluster will be available online. </p>
        <fig id="fig1">
          <label>Figure 1</label>
          <graphic xlink:href="https://html.scirp.org/file/4501403-rId187.jpeg?20251223111458" />
        </fig>
        <p><bold>F</bold><bold>igure 1.</bold>Spatial distribution of the 24 OCs found in the region. Dolidze 8 is drawn in blue circles, Cr421 in black dots, OC-124 in black circles, NGC6910 in green dots, OC-123 in pink circles, FSR 0224 in brown circles, HSC 618 in green circles, UBC 585 in yellow dots, FSR 0227 in turquoise triangles, Roslund 6 in blue triangles, IRAS-20306+4005 in red dots, OC-128 in red circles, HSC 625 in yellow circles, Bica 1 in brown dots, Bica 2 in blue dots, FSR 0238 in pink dots, FSR 0236 in turquoise dots, HSC 630 in green triangles, RSL-03 in turquoise circles, Dolidze 11 in red triangles, RSL-04 in black triangle, RSL-05 in yellow triangle, RSL-06 in pink triangle and HSC 626 in brown triangles. </p>
        <p>At the beginning of our investigation, a cross-match of the 24 open clusters detected with those known in the region (see <bold>Table</bold><bold>1</bold>) indicated that we had found 18 known clusters and six new ones identified as RSL-01, RSL-02, RSL-03, RSL-04, RSL-05 and RSL-06. We detected that the clusters Bica 1, Bica 2, FSR 0238 and FSR 0236, among the known clusters, are located in the core of the Cyg OB2 association.</p>
        <p>During the process of this work, a new OC census is published by Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>] using <italic>Gaia</italic> DR3. In their publication, RSL-01 is identified as IRAS-20306+4005 and RSL-02 as HSC 630 (see <bold>Table</bold><bold>1</bold> and <bold>Table</bold><bold>2</bold>). <xref ref-type="fig" rid="fig2">Figure 2</xref> shows the stellar positions, VPD, and parallax histogram for the four new OC members found, IRAS-20306+4005 and HSC 630, while <xref ref-type="fig" rid="fig3">Figure 3</xref> displays the same for Bica 1, Bica 2, FSR 0236 and FSR 0238.</p>
        <p>We want to remark that: a) the parallax histogram of IRAS-20306+4005 shows a large range of values. This is because most of the members of this cluster have magnitudes <inline-formula><mml:math display="inline"><mml:mrow><mml:mn> 17 </mml:mn><mml:mo> &lt; </mml:mo><mml:mi> G </mml:mi><mml:mo> &lt; </mml:mo><mml:mn> 19 </mml:mn></mml:mrow></mml:math></inline-formula> mag with parallax uncertainties of 0.4 mas; b) an inspection of the RSL-06 VPD shows a considerable dispersion of its members that has not been possible to justify. However, the stellar position, the parallax histogram and the <italic>Gaia</italic> photometric diagram show it as a cluster. To make a final decision, we will wait for a new series of data from the Gaia mission and we consider RSL-06 as a tentative cluster.</p>
        <p><bold>Table</bold><bold>3.</bold> Centre coordinates (<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> α </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> , <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> δ </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> ) , mean proper motion (<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> μ </mml:mi><mml:mi> α </mml:mi></mml:msub><mml:mi> cos </mml:mi><mml:msub><mml:mi> δ </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> , <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> μ </mml:mi><mml:mrow><mml:msub><mml:mi> δ </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> ), number of members <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> , number of highly probable members <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> between parentheses, radius <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> r </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> , mean parallax <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> ϖ </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and estimated distance <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> d </mml:mi><mml:mrow><mml:msub><mml:mi> ϖ </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> of the detected OCs in the region.</p>
        <table-wrap id="tbl3">
          <label>Table 3</label>
          <table>
            <tbody>
              <tr>
                <td>
                </td>
                <td rowspan="2">Open Cluster</td>
                <td>
                  <inline-formula>
                    <mml:math display="inline">
                      <mml:mrow>
                        <mml:msub>
                          <mml:mi>α</mml:mi>
                          <mml:mi>c</mml:mi>
                        </mml:msub>
                      </mml:mrow>
                    </mml:math>
                  </inline-formula>
                </td>
                <td>
                  <inline-formula>
                    <mml:math display="inline">
                      <mml:mrow>
                        <mml:msub>
                          <mml:mi>δ</mml:mi>
                          <mml:mi>c</mml:mi>
                        </mml:msub>
                      </mml:mrow>
                    </mml:math>
                  </inline-formula>
                </td>
                <td>
                  <inline-formula>
                    <mml:math display="inline">
                      <mml:mrow>
                        <mml:msub>
                          <mml:mi>μ</mml:mi>
                          <mml:mi>α</mml:mi>
                        </mml:msub>
                        <mml:mi>cos</mml:mi>
                        <mml:msub>
                          <mml:mi>δ</mml:mi>
                          <mml:mi>c</mml:mi>
                        </mml:msub>
                      </mml:mrow>
                    </mml:math>
                  </inline-formula>
                </td>
                <td>
                  <inline-formula>
                    <mml:math display="inline">
                      <mml:mrow>
                        <mml:msub>
                          <mml:mi>μ</mml:mi>
                          <mml:mrow>
                            <mml:msub>
                              <mml:mi>δ</mml:mi>
                              <mml:mi>c</mml:mi>
                            </mml:msub>
                          </mml:mrow>
                        </mml:msub>
                      </mml:mrow>
                    </mml:math>
                  </inline-formula>
                </td>
                <td>
                  <inline-formula>
                    <mml:math display="inline">
                      <mml:mrow>
                        <mml:msub>
                          <mml:mi>N</mml:mi>
                          <mml:mi>c</mml:mi>
                        </mml:msub>
                      </mml:mrow>
                    </mml:math>
                  </inline-formula>
                  (
                  <inline-formula>
                    <mml:math display="inline">
                      <mml:mrow>
                        <mml:msub>
                          <mml:mi>N</mml:mi>
                          <mml:mrow>
                            <mml:mi>h</mml:mi>
                            <mml:mi>p</mml:mi>
                          </mml:mrow>
                        </mml:msub>
                      </mml:mrow>
                    </mml:math>
                  </inline-formula>
                  )
                </td>
                <td>
                  <inline-formula>
                    <mml:math display="inline">
                      <mml:mrow>
                        <mml:msub>
                          <mml:mi>r</mml:mi>
                          <mml:mi>c</mml:mi>
                        </mml:msub>
                      </mml:mrow>
                    </mml:math>
                  </inline-formula>
                </td>
                <td>
                  <inline-formula>
                    <mml:math display="inline">
                      <mml:mrow>
                        <mml:msub>
                          <mml:mi>ϖ</mml:mi>
                          <mml:mi>c</mml:mi>
                        </mml:msub>
                      </mml:mrow>
                    </mml:math>
                  </inline-formula>
                </td>
                <td>
                  <inline-formula>
                    <mml:math display="inline">
                      <mml:mrow>
                        <mml:msub>
                          <mml:mi>d</mml:mi>
                          <mml:mrow>
                            <mml:msub>
                              <mml:mi>ϖ</mml:mi>
                              <mml:mi>c</mml:mi>
                            </mml:msub>
                          </mml:mrow>
                        </mml:msub>
                      </mml:mrow>
                    </mml:math>
                  </inline-formula>
                </td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>[˚]</td>
                <td>[˚]</td>
                <td>[mas/yr]</td>
                <td>[mas/yr]</td>
                <td>
                </td>
                <td>[arcmin]</td>
                <td>[mas]</td>
                <td>[pc]</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>Dolidze 8</td>
                <td>306.101</td>
                <td>42.252</td>
                <td>−2.521 ± 0.207</td>
                <td>−6.135 ± 0.210</td>
                <td>75 (51)</td>
                <td>48.4</td>
                <td>1.018 ± 0.039</td>
                <td>966 ± 4</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>IRAS-20306+4005</td>
                <td>308.104</td>
                <td>40.289</td>
                <td>−1.768 ± 0.263</td>
                <td>−4.096 ± 0.164</td>
                <td>32 (22)</td>
                <td>16.8</td>
                <td>1.034 ± 0.032</td>
                <td>951 ± 6</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>Cr421</td>
                <td>305.821</td>
                <td>41.704</td>
                <td>−3.641 ± 0.106</td>
                <td>−8.359 ± 0.21</td>
                <td>175 (119)</td>
                <td>25.0</td>
                <td>0.822 ± 0.100</td>
                <td>1192 ± 2</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>HSC 630</td>
                <td>307.689</td>
                <td>41.466</td>
                <td>−1.989 ± 0.048</td>
                <td>−2.901 ± 0.129</td>
                <td>16 (11)</td>
                <td>8.1</td>
                <td>0.726 ± 0.054</td>
                <td>1346 ± 10</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>RSL-03</td>
                <td>307.221</td>
                <td>41.436</td>
                <td>−2.426 ± 0.103</td>
                <td>−3.015 ± 0.035</td>
                <td>13 (9)</td>
                <td>9.4</td>
                <td>0.618 ± 0.012</td>
                <td>1575 ± 13</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>RSL-04</td>
                <td>306.780</td>
                <td>40.517</td>
                <td>−3.126 ± 0.176</td>
                <td>−5.179 ± 0.183</td>
                <td>15 (10)</td>
                <td>7.8</td>
                <td>0.558 ± 0.011</td>
                <td>1742 ± 24</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>RSL-05</td>
                <td>307.305</td>
                <td>41.245</td>
                <td>−2.606 ± 0.086</td>
                <td>−3.735 ± 0.082</td>
                <td>23 (16)</td>
                <td>7.9</td>
                <td>0.597 ± 0.011</td>
                <td>1629 ± 15</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>RSL-06</td>
                <td>307.434</td>
                <td>41.323</td>
                <td>−3.115 ± 0.190</td>
                <td>−4.264 ± 0.159</td>
                <td>17 (12)</td>
                <td>6.4</td>
                <td>0.578 ± 0.016</td>
                <td>1682 ± 17</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>FSR 0238</td>
                <td>308.704</td>
                <td>41.412</td>
                <td>−2.825 ± 0.119</td>
                <td>−4.604 ± 0.096</td>
                <td>21 (14)</td>
                <td>5.0</td>
                <td>0.576 ± 0.018</td>
                <td>1686 ± 20</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>FSR 0236</td>
                <td>308.133</td>
                <td>41.419</td>
                <td>−2.334 ± 0.092</td>
                <td>−4.161 ± 0.110</td>
                <td>26 (17)</td>
                <td>4.1</td>
                <td>0.585 ± 0.013</td>
                <td>1661 ± 12</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>OC-124</td>
                <td>306.437</td>
                <td>40.929</td>
                <td>−3.117 ± 0.063</td>
                <td>−4.124 ± 0.044</td>
                <td>22 (15)</td>
                <td>6.1</td>
                <td>0.500 ± 0.013</td>
                <td>1936 ± 21</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>FSR 0224</td>
                <td>306.371</td>
                <td>40.198</td>
                <td>−3.109 ± 0.097</td>
                <td>−4.337 ± 0.087</td>
                <td>20 (13)</td>
                <td>9.9</td>
                <td>0.575 ± 0.017</td>
                <td>1688 ± 14</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>Dolidze 11</td>
                <td>306.699</td>
                <td>41.381</td>
                <td>−1.203 ± 0.120</td>
                <td>−4.164 ± 0.109</td>
                <td>21 (14)</td>
                <td>9.6</td>
                <td>0.518 ± 0.033</td>
                <td>1868 ± 36</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>NGC 6910</td>
                <td>305.807</td>
                <td>40.775</td>
                <td>−3.411 ± 0.115</td>
                <td>−5.416 ± 0.124</td>
                <td>153 (104)</td>
                <td>19.1</td>
                <td>0.575 ± 0.022</td>
                <td>1690 ± 17</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>UBC585</td>
                <td>307.000</td>
                <td>40.549</td>
                <td>−2.858 ± 0.129</td>
                <td>−5.546 ± 0.110</td>
                <td>41 (28)</td>
                <td>10.9</td>
                <td>0.675 ± 0.017</td>
                <td>1444 ± 7</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>HSC 618</td>
                <td>306.880</td>
                <td>40.025</td>
                <td>−2.001 ± 0.178</td>
                <td>−4.044 ± 0.180</td>
                <td>28 (19)</td>
                <td>20.6</td>
                <td>1.018 ± 0.024</td>
                <td>966 ± 7</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>HSC 625</td>
                <td>308.258</td>
                <td>40.792</td>
                <td>−2.595 ± 0.077</td>
                <td>−4.924 ± 0.089</td>
                <td>22 (16)</td>
                <td>16.0</td>
                <td>0.576 ± 0.022</td>
                <td>1686 ± 21</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>HSC 626</td>
                <td>306.661</td>
                <td>41.658</td>
                <td>−3.096 ± 0.128</td>
                <td>−4.678 ± 0.182</td>
                <td>23 (16)</td>
                <td>16.0</td>
                <td>0.530 ± 0.020</td>
                <td>1826 ± 18</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>FSR 0227</td>
                <td>307.218</td>
                <td>40.488</td>
                <td>−1.823 ± 0.157</td>
                <td>−4.546 ± 0.137</td>
                <td>35 (24)</td>
                <td>18.6</td>
                <td>0.504 ± 0.017</td>
                <td>1919 ± 17</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>OC-123</td>
                <td>306.345</td>
                <td>40.840</td>
                <td>−3.049 ± 0.058</td>
                <td>−4.757 ± 0.112</td>
                <td>17 (12)</td>
                <td>7.2</td>
                <td>0.558 ± 0.011</td>
                <td>1740 ± 16</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>OC-128</td>
                <td>307.938</td>
                <td>40.798</td>
                <td>−3.010 ± 0.127</td>
                <td>−4.337 ± 0.107</td>
                <td>85 (55)</td>
                <td>22.1</td>
                <td>0.583 ± 0.014</td>
                <td>1682 ± 14</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>Bica 1</td>
                <td>308.296</td>
                <td>41.217</td>
                <td>−2.775 ± 0.129</td>
                <td>−4.507 ± 0.116</td>
                <td>22 (15)</td>
                <td>1.4</td>
                <td>0.578 ± 0.022</td>
                <td>1688 ± 13</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>Bica 2</td>
                <td>308.320</td>
                <td>41.316</td>
                <td>−2.673 ± 0.084</td>
                <td>−4.443 ± 0.109</td>
                <td>41 (28)</td>
                <td>5.4</td>
                <td>0.587 ± 0.018</td>
                <td>1656 ± 10</td>
                <td>
                </td>
              </tr>
              <tr>
                <td>
                </td>
                <td>Roslund 6*</td>
                <td>307.353</td>
                <td>40.448</td>
                <td>5.999 ± 0.423</td>
                <td>2.150 ± 0.374</td>
                <td>182</td>
                <td>66.7</td>
                <td>2.839 ± 0.098</td>
                <td>350 ± 1</td>
                <td>
                </td>
              </tr>
            </tbody>
          </table>
        </table-wrap>
        <p>[*] We compute the mean parameters from all the members found in the region of this study, where the north part of the cluster is occupied. </p>
        <p>In the case of Roslund 6, we compute the mean parameters from the <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> members found in the region of this study, where the north part of the cluster is occupied.</p>
        <fig id="fig2">
          <label>Figure 2</label>
          <graphic xlink:href="https://html.scirp.org/file/4501403-rId228.jpeg?20251223111458" />
        </fig>
        <p><bold>F</bold><bold>igure 2.</bold> Stellar positions (left column) and VPD (middle column) for the <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> members of the new four OCs detected, IRAS-20306+4005 and HSC 630 (grey circles represent field stars). The <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> members are plotted with red filled circles and the rest of the members with yellow filled circles. The OCs parallax histograms (right column) are shown for the <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> members (red) and for the <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> members (filled with pattern).</p>
        <fig id="fig3">
          <label>Figure 3</label>
          <graphic xlink:href="https://html.scirp.org/file/4501403-rId237.jpeg?20251223111458" />
        </fig>
        <p><bold>F</bold><bold>igure 3.</bold> Stellar positions (left column) and VPD (middle column) for the <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> members of Bica 1, Bica 2, FSR 0236 and FSR 0238 located at the core of Cyg OB2 (grey circles represent field stars). The <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> members are plotted with red filled circles and the rest of the members with yellow filled circles. The OCs parallax histograms (right column) are shown for the <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mi> c </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> members (red) and for the <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> members (filled with pattern).</p>
        <p>4.1.1. Comparison with Other Works</p>
        <p>First, we compare our results given in <bold>Table</bold><bold>3</bold> with the ones given in the literature (see <bold>Table</bold><bold>1</bold>). It can be seen that our values of the centre coordinates, the mean proper motion components and the mean parallax are in good agreement with the literature. The exceptions are the Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>] parameters for FSR 0238 which do not match ours and those obtained by other sources.</p>
        <p>Then, as Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>] identify the OCs in the region that have been previously studied using <italic>Gaia</italic> DR2 data, we compare our lists of members with theirs. This comparison distinguishes between common members—stars identified in both datasets—and non-common members, which are exclusive to either our study or theirs. (see <xref ref-type="fig" rid="fig4">Figure 4</xref>). We find differences in the number of members, although the catalogue used (<italic>Gaia</italic> DR3) and the method (HDBSCAN algorithm) are the same. <bold>Table</bold><bold>4</bold> shows the low percentage of members in common.</p>
        <p>We notice that their results contain very faint members, for which parallax uncertainty may distort the spatial distributions in transforming parallax to distance [<xref ref-type="bibr" rid="B35">35</xref>][<xref ref-type="bibr" rid="B36">36</xref>]. To check if this happens, for each OC we examine the histogram of the geometric distance (<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> r </mml:mi><mml:mrow><mml:mi> g </mml:mi><mml:mi> e </mml:mi><mml:mi> o </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> ) of both lists of members using the data from Bailer-Jones <italic>et al.</italic> (2021) [<xref ref-type="bibr" rid="B37">37</xref>].</p>
        <p><bold>Table</bold><bold>4.</bold> Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>] members in common with ours.</p>
        <table-wrap id="tbl4">
          <label>Table 4</label>
          <table>
            <tbody>
              <tr>
                <td>Open Cluster</td>
                <td>In Common</td>
                <td>Open Cluster</td>
                <td>In Common</td>
              </tr>
              <tr>
                <td>Dolidze 8</td>
                <td>59%</td>
                <td>Cr421</td>
                <td>46%</td>
              </tr>
              <tr>
                <td>NGC 6910</td>
                <td>53%</td>
                <td>UBC 585</td>
                <td>67%</td>
              </tr>
              <tr>
                <td>OC-124</td>
                <td>45%</td>
                <td>OC-123</td>
                <td>38%</td>
              </tr>
              <tr>
                <td>OC-128</td>
                <td>51%</td>
                <td>FSR 0224</td>
                <td>64%</td>
              </tr>
              <tr>
                <td>Dolidze 11</td>
                <td>19%</td>
                <td>Bica 2</td>
                <td>33%</td>
              </tr>
              <tr>
                <td>HSC 618</td>
                <td>61%</td>
                <td>HSC 625</td>
                <td>53%</td>
              </tr>
              <tr>
                <td>HSC 626</td>
                <td>61%</td>
                <td>HSC 630</td>
                <td>68%</td>
              </tr>
              <tr>
                <td>FSR 0227</td>
                <td>55%</td>
                <td>IRAS-20306+4005</td>
                <td>43%</td>
              </tr>
            </tbody>
          </table>
        </table-wrap>
        <fig id="fig4">
          <label>Figure 4</label>
          <graphic xlink:href="https://html.scirp.org/file/4501403-rId248.jpeg?20251223111458" />
        </fig>
        <p><bold>Figure</bold><bold>4.</bold> Bar diagram comparing the number of members for each open cluster between our work and that of Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>]. The names of the clusters are displayed along the X-axis, while the Y-axis represents the total number of members. The bars are grouped to distinguish between members identified exclusively in our study (yellow), members identified exclusively in Hunt &amp; Reffert’s catalogue (blue), and common members found in both lists of members (green).</p>
        <p>As an example, <xref ref-type="fig" rid="fig5">Figure 5</xref> shows the comparison of results from this study and those from [<xref ref-type="bibr" rid="B19">19</xref>] for Dolidze 8. <xref ref-type="fig" rid="fig5">Figure 5b</xref> plots the results for Dolidze 8 where the histogram of our members shows a Gaussian distribution and the one of Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>] members is skewed to the right, indicating false positives and a distance range between 800 and 3300 pc.</p>
        <p>To explain the presence of these false positives, the uncertainties in the parallaxes of the members are plotted against <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> r </mml:mi><mml:mrow><mml:mi> g </mml:mi><mml:mi> e </mml:mi><mml:mi> o </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> in <xref ref-type="fig" rid="fig5">Figure 5c</xref>. It can be seen that the Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>] members with greater parallax uncertainty produce the skewness that distorts their spatial distribution in <xref ref-type="fig" rid="fig5">Figure 5b</xref>.</p>
        <p>On the contrary, <xref ref-type="fig" rid="fig5">Figure 5b</xref> and <xref ref-type="fig" rid="fig5">Figure 5c</xref> do not show this distortion for our members. This is due to the adoption of stellar parallaxes with fractional error <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> f </mml:mi><mml:mo> = </mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mi> σ </mml:mi><mml:mi> ϖ </mml:mi></mml:msub></mml:mrow><mml:mi> ϖ </mml:mi></mml:mfrac><mml:mo> ≤ </mml:mo><mml:mn> 0.20 </mml:mn></mml:mrow></mml:math></inline-formula> (criterion iv) in our sample. For this reason our members have smaller parallax uncertainties, as seen in <xref ref-type="fig" rid="fig5">Figure 5c</xref>.</p>
        <fig id="fig5">
          <label>Figure 5</label>
          <graphic xlink:href="https://html.scirp.org/file/4501403-rId253.jpeg?20251223111459" />
        </fig>
        <p><bold>Figure</bold><bold>5.</bold>Results for the open cluster Dolidze 8. a) parallax histograms for [<xref ref-type="bibr" rid="B19">19</xref>] (green) and this work (filled with pattern). b) geometric distance histograms <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> r </mml:mi><mml:mrow><mml:mi> g </mml:mi><mml:mi> e </mml:mi><mml:mi> o </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> obtained from [<xref ref-type="bibr" rid="B37">37</xref>], for [<xref ref-type="bibr" rid="B19">19</xref>] (green) and this work (filled with pattern). c) uncertainty in parallax <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> σ </mml:mi><mml:mi> ϖ </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> against <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> r </mml:mi><mml:mrow><mml:mi> g </mml:mi><mml:mi> e </mml:mi><mml:mi> o </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> for members from [<xref ref-type="bibr" rid="B19">19</xref>] (green filled circles) and this work (open black circles).</p>
        <p><bold>Table</bold><bold>5.</bold> Mean proper motion and parallax of the stellar over-densities determined by Orellana <italic>et al.</italic> (2021) [<xref ref-type="bibr" rid="B9">9</xref>].</p>
        <table-wrap id="tbl5">
          <label>Table 5</label>
          <table>
            <tbody>
              <tr>
                <td rowspan="2">Association</td>
                <td>
                  <inline-formula>
                    <mml:math display="inline">
                      <mml:mrow>
                        <mml:msub>
                          <mml:mi>μ</mml:mi>
                          <mml:mi>α</mml:mi>
                        </mml:msub>
                        <mml:mi>cos</mml:mi>
                        <mml:msub>
                          <mml:mi>δ</mml:mi>
                          <mml:mi>c</mml:mi>
                        </mml:msub>
                      </mml:mrow>
                    </mml:math>
                  </inline-formula>
                </td>
                <td>
                  <inline-formula>
                    <mml:math display="inline">
                      <mml:mrow>
                        <mml:msub>
                          <mml:mi>μ</mml:mi>
                          <mml:mrow>
                            <mml:msub>
                              <mml:mi>δ</mml:mi>
                              <mml:mi>c</mml:mi>
                            </mml:msub>
                          </mml:mrow>
                        </mml:msub>
                      </mml:mrow>
                    </mml:math>
                  </inline-formula>
                </td>
                <td>
                  <inline-formula>
                    <mml:math display="inline">
                      <mml:mrow>
                        <mml:msub>
                          <mml:mi>d</mml:mi>
                          <mml:mi>c</mml:mi>
                        </mml:msub>
                      </mml:mrow>
                    </mml:math>
                  </inline-formula>
                </td>
              </tr>
              <tr>
                <td>[mas/yr]</td>
                <td>[mas/yr]</td>
                <td>[pc]</td>
              </tr>
              <tr>
                <td>Cyg OB2</td>
                <td>−2.71 ± 0.02</td>
                <td>−4.24 ± 0.02</td>
                <td>1669 ± 6</td>
              </tr>
              <tr>
                <td>Right</td>
                <td>0.04 ± 0.02</td>
                <td>−3.33 ± 0.02</td>
                <td>1281 ± 5</td>
              </tr>
              <tr>
                <td>Left</td>
                <td>−2.09 ± 0.02</td>
                <td>−3.02 ± 0.02</td>
                <td>1284 ± 5</td>
              </tr>
            </tbody>
          </table>
        </table-wrap>
        <p>We also notice that the members of Bica 2 identified by Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>] are located in the place where OC census carried out prior to Gaia era identifies Bica 1 and Bica 2 separately [<xref ref-type="bibr" rid="B38">38</xref>]. Our analysis finds both clusters. Besides, it is not possible to detect HSC 624 in our work, even several runs of HDBSCAN have been done using different values of mPts and mcSize; instead we detect two new OCs named RSL-03 and RSL-05. The former corresponds to the northeast part of HSC 624, and the latter to the southwest part of it.</p>
        <p>4.1.2. Spatial Structure along the Line of Sight of the 24 Open Clusters</p>
        <p>We analyse the spatial structure along the line of sight of the selected circular area. In <xref ref-type="fig" rid="fig6">Figure 6</xref>, we plot the mean proper motion components of the open clusters detected in this study with dots (except Roslund 6, Cr 421 and Dolidze 8 whose values are out of the range of the axes of the figure). The different colours represent the scale of the estimated distances.</p>
        <fig id="fig6">
          <label>Figure 6</label>
          <graphic xlink:href="https://html.scirp.org/file/4501403-rId266.jpeg?20251223111459" />
        </fig>
        <p><bold>Figure</bold><bold>6.</bold> Vector point diagram (VPD) of the region except Dolidze 8, Cr421 and Roslund 6. OCs mean proper motion are plotted with filled circles, and the members of Cyg OB2 association, Left and Right stellar groups are plotted with dots. </p>
        <p>Also, we plot the members of the Cyg OB2 association, Left and Right over-densities found by Orellana <italic>et al.</italic> (2021) [<xref ref-type="bibr" rid="B9">9</xref>] with the colour according to their distance. The red circle contains the proper motion values of the members of Cyg OB2, and the green ones contain the proper motion values of the members of the Left and Right over-densities. The mean proper motion of Cyg OB2 association, Left and Right over-densities are plotted with crosses (see <bold>Table</bold><bold>5</bold>).</p>
        <p>It can be seen that the estimated distance of several clusters is between 1600 and 1800pc, similar to the distance of Cyg OB2 and their mean proper motions lie inside the red circle. These clusters and their numbers in <xref ref-type="fig" rid="fig6">Figure 6</xref> are FSR 0224 (no. 12), FSR 0236 (no. 10), FSR 0238 (no. 9), RSL-04 (no. 6), RSL-05 (no. 7), RSL-06 (no. 8), HSC 625 (no. 17), OC-123 (no. 20), OC-128 (no. 21), NGC 6910 (no. 14), Bica 1 (no. 22) and Bica 2 (no. 23). This suggests that these OCs would be connected to Cyg OB2 association.</p>
        <p>We also notice that the estimated distance of HSC 630 (no. 4) is similar to the distance of the Left over-density, and that the mean proper motion of the OC lies inside the green circle. Then, HSC 630 would be connected to the Left over-density.</p>
        <p>In the case of the Right over-density, there is no OC in the region having similar mean proper motion and estimated distance.</p>
      </sec>
      <sec id="sec4dot2">
        <title>4.2. Photometric Results</title>
        <p>An important result of the photometric analysis is the age of an OC. Its determination is a serious problem related to the contamination by field stars, unresolved binarity of the cluster stars and variable interstellar reddening.</p>
        <p>In order to reduce the first and second effects on the astrometric membership determination, we impose restrictions on the sample (Subsection 3.1) that allow the photometric analysis to be more reliable.</p>
        <p>The Gaia DR3 catalogue allows us to reach fainter magnitudes which provide many more cluster members. However, we must be careful with the contamination by field stars that can be produced by the astrometric parameter uncertainties. The effect of parallax uncertainty has been reduced by considering <inline-formula><mml:math display="inline"><mml:mrow><mml:mfrac><mml:mrow><mml:msub><mml:mi> σ </mml:mi><mml:mi> ϖ </mml:mi></mml:msub></mml:mrow><mml:mi> ϖ </mml:mi></mml:mfrac><mml:mo> ≤ </mml:mo><mml:mn> 0.20 </mml:mn></mml:mrow></mml:math></inline-formula> in our sample (criterion iv) and demonstrated in 0.0.3. The rest of the possible field stars are eliminated by defining the highly probable members <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> as those with <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> P </mml:mi><mml:mo> ≥ </mml:mo><mml:mn> 0.80 </mml:mn></mml:mrow></mml:math></inline-formula> (section 3.2.2).</p>
        <p>Regarding stellar binarity, Belokurov <italic>et al.</italic> (2020) [<xref ref-type="bibr" rid="B39">39</xref>] demonstrate that a high RUWE value is an effective indicator of it, as well as Lindegren (2022) [<xref ref-type="bibr" rid="B40">40</xref>] remarks that RUWE is its main indicator. Following Castro-Ginard <italic>et al.</italic> (2024) [<xref ref-type="bibr" rid="B41">41</xref>], we can say that our sample is free of its contamination by considering a RUWE ≤ 1.4, which is the criterion v) adopted in Subsection 3.1. Therefore, the astrometric members obtained in 1 are ready for a reliable photometric analysis.</p>
        <p>Interstellar reddening is another important factor to address when determining the age of open clusters. In a region with variable interstellar reddening, to know the extinction value becomes a challenging task. The correct fit of the isochrone to the observations is directly dependent on the value of <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi></mml:mrow></mml:math></inline-formula> . In this work, this value is estimated using the new three-dimensional (3D) dust reddening map and is then applied in conjunction with the <italic>Gaia</italic> photometric reddening law, as explained in Subsection 3.3.</p>
        <p>We present the evaluation of the <italic>Gaia</italic> DR3 photometric diagram of the four RSL new open clusters identified, IRAS-20306+4005 and HSC 630 plotted in <xref ref-type="fig" rid="fig7">Figure 7</xref>, and those in the core of Cyg OB2 association, plotted in <xref ref-type="fig" rid="fig8">Figure 8</xref>. Red filled circles correspond to the <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> members, and the yellow circles indicate the rest of the members. The isochrone is fitted based on the red filled circles. In all the CMD figures, the isochrone presented in black corresponds to the most probable age estimated for each OC, while the isochrones in yellow and green, as observed, also appear to fit the stellar member observations. Then, an estimation of the error in the age is the difference between the ages of yellow and black isochrones and between the ages of green and black ones. The isochrones in light blue and blue represent the age range investigated.</p>
        <fig id="fig7">
          <label>Figure 7</label>
          <graphic xlink:href="https://html.scirp.org/file/4501403-rId277.jpeg?20251223111500" />
        </fig>
        <p><bold>Figure</bold><bold>7.</bold><italic>Gaia</italic> photometric diagram for the probable members of the four RSL new open clusters, IRAS-20306+4005 and HSC 630. Light gray dots correspond to the field population. Red filled circles are the <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> members of each cluster obtained in this paper while the yellow ones are the rest of the members. Open blue circles are the members found by Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>]. Magenta triangle in the IRAS-20306+4005 CMD represents the star with IR excess identified as BY DRA Variable by Chen <italic>et al.</italic> (2020) [<xref ref-type="bibr" rid="B43">43</xref>]. The black isochrone corresponds to the most probable age estimated for each OC. The magenta isochrone represents the evolutionary model of stars reported by Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>].</p>
        <p>In these figures, Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>] members are plotted with open blue circles. They are not considered to fit ours isochrones because they may be contaminated by false positives, as shown in Subsection 4.1.1. The magenta curve is the isochrone achieved with the photometric parameters proposed for each open cluster by Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>].</p>
        <fig id="fig8">
          <label>Figure 8</label>
          <graphic xlink:href="https://html.scirp.org/file/4501403-rId280.jpeg?20251223111500" />
        </fig>
        <p><bold>F</bold><bold>igure 8.</bold> Gaia photometric diagram for the probable members of the four known open clusters in the core of CygOB2. Symbols as in <xref ref-type="fig" rid="fig4">Figure 4</xref>. Cyan and green triangles represent stars with IR excess identified as YSO by Kuhn <italic>et al.</italic> (2021) [<xref ref-type="bibr" rid="B44">44</xref>] and X-ray source as [<xref ref-type="bibr" rid="B45">45</xref>], respectively. Black triangle is the emission-line star identified as Schulte 64 by Bhattacharyya <italic>et al.</italic> (2021) [<xref ref-type="bibr" rid="B46">46</xref>]. The black isochrone corresponds to the most probable age estimated for each OC. The magenta isochrone represents the evolutionary model of stars reported by Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>].</p>
        <p>4.2.1. New OCs</p>
        <p>• RSL-01 ≡ IRAS-20306+4005 </p>
        <p>This cluster, located at less than 1 kpc in the southern edge of the study region, in the line of sight of the Cygnus-X DR 15 Region [<xref ref-type="bibr" rid="B42">42</xref>], is plotted in <xref ref-type="fig" rid="fig1">Figure 1</xref> with red dots. The isochrone for the <italic>Gaia</italic> DR3 catalogue data of the 22 <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> members (upper left in <xref ref-type="fig" rid="fig7">Figure 7</xref>), is fitted using a visual absorption value of, <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi><mml:mo> = </mml:mo><mml:msubsup><mml:mrow><mml:mn> 1.3 </mml:mn></mml:mrow><mml:mrow><mml:mo> − </mml:mo><mml:mn> 0.03 </mml:mn></mml:mrow><mml:mrow><mml:mo> + </mml:mo><mml:mn> 0.02 </mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> mag, as determined for this Galactic region in the 3D map. The uncertainties in the <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi></mml:mrow></mml:math></inline-formula> value correspond to those provided by the map. To estimate the age of this cluster, we fit isochrones within an age range of 2 to 15 Myr, ultimately determining an age of 8 ± 1 Myr. Most of the 32 possible members are likely to be late spectral types, with only a few exhibiting early spectral types (B and A).</p>
        <p>One of its members, the <italic>Gaia</italic> DR3 2064713443456205696 star, <inline-formula><mml:math display="inline"><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> α </mml:mi><mml:mn> , </mml:mn><mml:mi> δ </mml:mi></mml:mrow><mml:mo> ) </mml:mo></mml:mrow><mml:mo> = </mml:mo><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mn> 308.0477 </mml:mn><mml:mo> , </mml:mo><mml:mn> 40.3021 </mml:mn></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> has a reddening-free photometric parameter <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> Q </mml:mi><mml:mrow><mml:mi> N </mml:mi><mml:mi> I </mml:mi><mml:mi> R </mml:mi></mml:mrow></mml:msub><mml:mo> = </mml:mo><mml:mo> − </mml:mo><mml:mn> 1.17 </mml:mn><mml:mo> ± </mml:mo><mml:mn> 0.13 </mml:mn></mml:mrow></mml:math></inline-formula> , and according to what we stated in Section 3.3, this <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> Q </mml:mi><mml:mrow><mml:mi> N </mml:mi><mml:mi> I </mml:mi><mml:mi> R </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> value would indicate that this could be a PMS or an YSO star. Additional information available regarding this star indicated in <xref ref-type="fig" rid="fig7">Figure 7</xref> with a magenta triangle is that Chen <italic>et al.</italic> (2020) [<xref ref-type="bibr" rid="B43">43</xref>] classify it as a probable BY Draconis Variable star and they are of K-M type, similar to the spectral type that we can estimate with our best-fitting isochrone. Besides, we notice that all members of Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>] that are below the isochrone determined by us have large uncertainties in the parallax. Their distance histogram shows that 6 of them may be false positives, according to the analysis performed in 4.1.1. The magenta isochrone represents the evolutionary model of stars formed 4.8 Myr ago with solar metallicity, located at a distance of 936 pc and subject to a visual extinction of 3.7 mag, as determined from the 50th percentile results published by Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>].</p>
        <p>• RSL-02 ≡ HSC 630 </p>
        <p>HSC 630 is an OC located near the center of the examined region, at an estimated distance of 1346 pc from the Sun, plotted with green triangles in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The best-fitting isochrone for its 11 <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> members is obtained with the visual absorption value, <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi><mml:mo> = </mml:mo><mml:msubsup><mml:mrow><mml:mn> 2.1 </mml:mn></mml:mrow><mml:mrow><mml:mo> − </mml:mo><mml:mn> 0.05 </mml:mn></mml:mrow><mml:mrow><mml:mo> + </mml:mo><mml:mn> 0.08 </mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> mag, derived from the 3D map. By studying this region employing images from the Digital Sky Server (DSS), it is evident that the initial dust has already been swept away, which would be consistent with a visual absorption value of only two magnitudes. The age of this OC is investigated within the range of 4 to 22 Myr, and the most probable formation age is 12 ± 1 Myr. The <italic>Gaia</italic> DR3 2068009749251662336 star with <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> G </mml:mi><mml:mo> = </mml:mo><mml:mn> 12.38 </mml:mn></mml:mrow></mml:math></inline-formula> mag and <inline-formula><mml:math display="inline"><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:msub><mml:mi> G </mml:mi><mml:mrow><mml:mi> B </mml:mi><mml:mi> P </mml:mi></mml:mrow></mml:msub><mml:mo> − </mml:mo><mml:msub><mml:mi> G </mml:mi><mml:mrow><mml:mi> R </mml:mi><mml:mi> P </mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo> ) </mml:mo></mml:mrow><mml:mo> = </mml:mo><mml:mn> 0.74 </mml:mn></mml:mrow></mml:math></inline-formula> mag would be the earliest, probably a late B spectral type star whose age corresponds very well with the cluster age. The rest of the members are likely of spectral types A, F, and G. The magenta isochrone represents the 50th percentile results by Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>] with <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi><mml:mo> = </mml:mo><mml:mn> 1.9 </mml:mn></mml:mrow></mml:math></inline-formula> mag, an age of 6 Myr and a distance of 1294 pc.</p>
        <p>• RSL-03 </p>
        <p>This cluster, located near the centre of the study region, at an estimated distance of 1575 pc from the Sun, is plotted in <xref ref-type="fig" rid="fig1">Figure 1</xref> with turquoise circles. From the 9 <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> members of RSL- 03, the best-fitting isochrone for the <italic>Gaia</italic> DR3 catalogue is obtained with a visual absorption of <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi><mml:mo> = </mml:mo><mml:msubsup><mml:mrow><mml:mn> 5.2 </mml:mn></mml:mrow><mml:mrow><mml:mo> − </mml:mo><mml:mn> 0.14 </mml:mn></mml:mrow><mml:mrow><mml:mo> + </mml:mo><mml:mn> 0.04 </mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> mag, found with these errors in the 3D map. The age of this OC is investigated within the range of 4 to 22 Myr, with an estimated formation age of 14 ± 1 Myr. The spectral type of these stars would be between B and F0. Although the open cluster HSC 624 determined by Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>] has not been detected (see subsection 4.1), for comparison, we have included their isochrone in <xref ref-type="fig" rid="fig7">Figure 7</xref> because its northeast part coincides with our RSL-03. The physical parameters of HSC 624 determined by Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>] at the 50th percentile for the members of this cluster are similar to ours, with a distance of 1.6 kpc, an age of 15 Myr, and <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi><mml:mo> = </mml:mo><mml:mn> 5.1 </mml:mn></mml:mrow></mml:math></inline-formula> mag.</p>
        <p>• RSL-04 </p>
        <p>This cluster is located in the southern right edge of the study region, at an estimated distance of 1742 pc from the Sun, and is plotted in <xref ref-type="fig" rid="fig1">Figure 1</xref> with a black triangle. The best-fitting isochrone for the 10 <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> members is obtained with a visual extinction of <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi><mml:mo> = </mml:mo><mml:msubsup><mml:mrow><mml:mn> 2.5 </mml:mn></mml:mrow><mml:mrow><mml:mo> − </mml:mo><mml:mn> 0.03 </mml:mn></mml:mrow><mml:mrow><mml:mo> + </mml:mo><mml:mn> 0.05 </mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> mag, as reported for this Galactic region in the 3D map. The age of the cluster is investigated within the range of 16 to 40 Myr, resulting in 26 ± 2 Myr with A-type and late spectral-type stars. Based on this age, the cluster is among the older open clusters in the Cyg OB2 region.</p>
        <p>• RSL-05 </p>
        <p>RSL-05 is an OC located near the centre of the examined region, at an estimated distance of 1629 pc from the Sun, plotted with yellow triangles in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The 16 <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> members of RSL-05 are used to obtain the best-fitting isochrone which suggests a visual absorption of <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi><mml:mo> = </mml:mo><mml:mn> 3.8 </mml:mn></mml:mrow></mml:math></inline-formula> mag and an age of 18 ± 2 Myr. Based on this result, this open cluster would be another member of the older groups of open clusters in the Cyg OB2 region. Some stars are likely to belong to spectral types F and G, while the majority are earlier-type stars, specifically B and A. For this open cluster, the visual extinction value obtained in the Galactic region using the 3D map is <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi><mml:mo> = </mml:mo><mml:msubsup><mml:mrow><mml:mn> 4.6 </mml:mn></mml:mrow><mml:mrow><mml:mo> − </mml:mo><mml:mn> 0.13 </mml:mn></mml:mrow><mml:mrow><mml:mo> + </mml:mo><mml:mn> 0.08 </mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> mag, so it differs by approximately 1 magnitude from our result. This discrepancy is likely due to the high concentration of interstellar material in the region, along with the fact that the 3D map was generated using data from the <italic>Gaia</italic> DR2 catalogue, which has an inherent 30% uncertainty in parallax measurements compared to the <italic>Gaia</italic> DR3 catalogue. It is evident that the [<xref ref-type="bibr" rid="B19">19</xref>] isochrone shown in magenta color exhibits different visual extinction and age, with <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi><mml:mo> = </mml:mo><mml:mn> 5.1 </mml:mn></mml:mrow></mml:math></inline-formula> mag and age of 15 Myr. This open cluster should be reanalyzed using the data provided by the upcoming <italic>Gaia</italic> DR4 catalogue, which is expected to yield more precise and, therefore, more reliable results. Although HSC 624 has not been detected, in <xref ref-type="fig" rid="fig4">Figure 4</xref> we include its [<xref ref-type="bibr" rid="B19">19</xref>] isochrone as in the study of RSL-03 because its southwest part coincides with our RSL-05.</p>
        <p>• RSL-06 </p>
        <p>The OC RSL-06 is located near the center of the study region, at an estimated distance of 1682 pc from the Sun, plotted with pink triangles in <xref ref-type="fig" rid="fig1">Figure 1</xref>. RSL 06 contains 12 <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> members and the best-fitting isochrone for these stars is obtained with a visual absorption of <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi><mml:mo> = </mml:mo><mml:msubsup><mml:mrow><mml:mn> 5.4 </mml:mn></mml:mrow><mml:mrow><mml:mo> − </mml:mo><mml:mn> 0.01 </mml:mn></mml:mrow><mml:mrow><mml:mo> + </mml:mo><mml:mn> 0.10 </mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> mag, found with these errors in the 3D map. The age is investigated within the range of 4 to 30 Myr, with an estimated formation age of 14 ± 1 Myr. These stars would be from B to A9 spectral type. It is important to note that one of the results obtained from the analysis of these six open clusters is that RSL- 03, RSL- 05, and RSL- 06 are located very close to each other, as shown in Figure 0.0.2. They are the clusters for which the highest values of <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi></mml:mrow></mml:math></inline-formula> are estimated, ranging between 3.8 and 5.4 magnitudes.</p>
        <p>4.2.2. Core of Cyg OB2</p>
        <p>• Bica 1 and Bica 2 </p>
        <p>Bica <italic>et al.</italic> (2003) [<xref ref-type="bibr" rid="B47">47</xref>] detected Bica 1 and Bica 2 by visual inspection while examining the structure of the association Cyg OB2 with DSS images, both objects are located within the core radius of the association and seem to form a physical pair in the association core. Maíz Apellániz <italic>et al.</italic> (2020) [<xref ref-type="bibr" rid="B48">48</xref>] noticed that they are hard to distinguish in proper motion even if they are seen as density concentrations in the plane of the sky. The proper motions in the right ascension of two clusters are very similar while those in declination differ very little. </p>
        <p>This work identifies Bica 1 and Bica 2 using the HDBSCAN algorithm, which detects these two objects separately. They are then confirmed as clusters by fulfilling the three criteria outlined in 3.2.1. Proper motion and parallax values suggest that Cygnus OB2 association and each of these clusters are co-moving (see <xref ref-type="fig" rid="fig6">Figure 6</xref>). The distance measured for both clusters by Maíz Apellániz <italic>et al.</italic> (2020) [<xref ref-type="bibr" rid="B48">48</xref>] is ~1.7 kpc, in accordance to our results in <bold>Table</bold><bold>3</bold>. Bica 1 has 15 <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> members. The lack of evolved stars makes it impossible to determine the position of the turn-off point, thus complicating the selection of the correct isochrone. The best-fitting isochrone is found by studying an age range of 2 to 10 Myr. The 4 ± 1 Myr isochrone, with a visual extinction of <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi><mml:mo> = </mml:mo><mml:msubsup><mml:mrow><mml:mn> 6.3 </mml:mn></mml:mrow><mml:mrow><mml:mo> − </mml:mo><mml:mn> 0.07 </mml:mn></mml:mrow><mml:mrow><mml:mo> + </mml:mo><mml:mn> 0.07 </mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> magnitudes, provides the best fit. It is a very young cluster of stellar members with early spectral types. The <italic>Gaia</italic> DR3 2067782111687592704 star located at <inline-formula><mml:math display="inline"><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> α </mml:mi><mml:mn> , </mml:mn><mml:mi> δ </mml:mi></mml:mrow><mml:mo> ) </mml:mo></mml:mrow><mml:mo> = </mml:mo><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:msup><mml:mrow><mml:mn> 308.2830 </mml:mn></mml:mrow><mml:mo> ∘ </mml:mo></mml:msup><mml:mo> , </mml:mo><mml:msup><mml:mrow><mml:mn> 41.2241 </mml:mn></mml:mrow><mml:mo> ∘ </mml:mo></mml:msup></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> with <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> Q </mml:mi><mml:mrow><mml:mi> N </mml:mi><mml:mi> I </mml:mi><mml:mi> R </mml:mi></mml:mrow></mml:msub><mml:mo> = </mml:mo><mml:mo> − </mml:mo><mml:mn> 0.52 </mml:mn><mml:mo> ± </mml:mo><mml:mn> 0.08 </mml:mn></mml:mrow></mml:math></inline-formula> , indicated with cyan triangle symbol on <xref ref-type="fig" rid="fig8">Figure 8</xref>, represents the YSO by Kuhn <italic>et al.</italic> (2021) [<xref ref-type="bibr" rid="B44">44</xref>]. Bica 2 is older than Bica 1 but contains a greater number of probable stellar members with 28 <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> members. It also lacks evolved stars, and the best isochrone fit is found by studying an age range of 2 to 15 Myr with visual absorption, <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi><mml:mo> = </mml:mo><mml:msubsup><mml:mn> 5 </mml:mn><mml:mrow><mml:mo> − </mml:mo><mml:mn> 0.06 </mml:mn></mml:mrow><mml:mrow><mml:mo> + </mml:mo><mml:mn> 0.06 </mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> mag. The estimated formation age for Bica 2 is 6 ± 1 Myr. All these stars have early spectral types. The <italic>Gaia</italic> DR3 2067783559095152768 star located at <inline-formula><mml:math display="inline"><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> α </mml:mi><mml:mn> , </mml:mn><mml:mi> δ </mml:mi></mml:mrow><mml:mo> ) </mml:mo></mml:mrow><mml:mo> = </mml:mo><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:msup><mml:mrow><mml:mn> 308.3271 </mml:mn></mml:mrow><mml:mo> ∘ </mml:mo></mml:msup><mml:mo> , </mml:mo><mml:msup><mml:mrow><mml:mn> 41.2597 </mml:mn></mml:mrow><mml:mo> ∘ </mml:mo></mml:msup></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> and with <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> Q </mml:mi><mml:mrow><mml:mi> N </mml:mi><mml:mi> I </mml:mi><mml:mi> R </mml:mi></mml:mrow></mml:msub><mml:mo> = </mml:mo><mml:mo> − </mml:mo><mml:mn> 0.18 </mml:mn><mml:mo> ± </mml:mo><mml:mn> 0.071 </mml:mn></mml:mrow></mml:math></inline-formula> , is a Be star identified as Schulte 64 with Spectral type B1 V [<xref ref-type="bibr" rid="B46">46</xref>]. This star is indicated by a black triangle symbol in <xref ref-type="fig" rid="fig8">Figure 8</xref>. The visual extinction values for Bica 1 and Bica 2, along with their associated errors, are the values assigned to this Galactic region in the 3D map. The magenta isochrone represents the evolutionary model of stars reported by Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>] for Bica 1 and Bica 2, as the authors consider the members of both clusters to be part of a single open cluster. This isochrone corresponds to a stellar cluster located at a distance of 1.6 kpc, formed 3.5 Myr ago, with a visual extinction of 5.6 mag. The age difference shows that both clusters formed at different times.</p>
        <p>• FSR 0238 </p>
        <p>The OC FSR 0238 is located east of the centre of the studied region, at an estimated distance of 1686 pc from the Sun, and is plotted with pink dots in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The best-fitting isochrone for these stars suggests a probable visual absorption of <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi><mml:mo> = </mml:mo><mml:mn> 5.2 </mml:mn></mml:mrow></mml:math></inline-formula> mag, which differs by one magnitude from the value obtained for the Galactic region using the 3D map (<inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi><mml:mo> = </mml:mo><mml:msubsup><mml:mrow><mml:mn> 6.2 </mml:mn></mml:mrow><mml:mrow><mml:mo> − </mml:mo><mml:mn> 0.02 </mml:mn></mml:mrow><mml:mrow><mml:mo> + </mml:mo><mml:mn> 0.06 </mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> mag). This discrepancy warrants further investigation with the upcoming <italic>Gaia</italic> DR4. The age is studied in the range of 2 to 24 Myr, and according to our best-fitting isochrone for the 14 <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> members, the age of this open cluster would be 12 ± 2 Myr. This result aligns well with the possible age of the earliest star, <italic>Gaia</italic> DR3 2067870386152902656, with a spectral type of B V. Although we do not know the exact spectral type of the other members, we can reasonably conclude that they are likely B and A type stars.</p>
        <p>• FSR 0236 </p>
        <p>It is an open cluster close to the core of the Cyg OB2 association at a distance of 1661 pc to the Sun, and is plotted with turquoise dots in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The best-fitting isochrone for the 17 <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> N </mml:mi><mml:mrow><mml:mi> h </mml:mi><mml:mi> p </mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> members suggests that the visual absorption, <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi><mml:mo> = </mml:mo><mml:msubsup><mml:mrow><mml:mn> 5.0 </mml:mn></mml:mrow><mml:mrow><mml:mo> − </mml:mo><mml:mn> 0.04 </mml:mn></mml:mrow><mml:mrow><mml:mo> + </mml:mo><mml:mn> 0.08 </mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> mag, with the associated errors from the 3D map, represents the interstellar reddening in the region. This <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> A </mml:mi><mml:mi> v </mml:mi></mml:mrow></mml:math></inline-formula> value is similar to those obtained for Bica 2, and FSR 0238 clusters, which are located in the same region of the Galaxy. The age is study in the range of 2 to 15 Myr and according to our best-fitting isochrone, the age of this open cluster would be 8 ± 1 Myr. The <italic>Gaia</italic> DR3 2067834514587217536 star located at <inline-formula><mml:math display="inline"><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> α </mml:mi><mml:mn> , </mml:mn><mml:mi> δ </mml:mi></mml:mrow><mml:mo> ) </mml:mo></mml:mrow><mml:mo> = </mml:mo><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:msup><mml:mrow><mml:mn> 308.1170 </mml:mn></mml:mrow><mml:mo> ∘ </mml:mo></mml:msup><mml:mo> , </mml:mo><mml:msup><mml:mrow><mml:mn> 41.3803 </mml:mn></mml:mrow><mml:mo> ∘ </mml:mo></mml:msup></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> and with <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> Q </mml:mi><mml:mrow><mml:mi> N </mml:mi><mml:mi> I </mml:mi><mml:mi> R </mml:mi></mml:mrow></mml:msub><mml:mo> = </mml:mo><mml:mo> − </mml:mo><mml:mn> 3.05 </mml:mn><mml:mo> ± </mml:mo><mml:mn> 0.2 </mml:mn></mml:mrow></mml:math></inline-formula> , is represented by a green triangle symbol in <xref ref-type="fig" rid="fig8">Figure 8</xref>. This star is one of those investigated by Rauw (2011) [<xref ref-type="bibr" rid="B45">45</xref>] during the multi-epoch XMM-Newton campaign on the core of the massive Cyg OB2 association, where it is categorized as an X-ray fainter OB star, but not analyzed in detail, with a possible spectral type of O7 V. Our analysis using the PARSEC isochrone suggests that it is likely a late B spectral type and the rest of the members are also likely to be of spectral type B.</p>
      </sec>
    </sec>
    <sec id="sec5">
      <title>5. Conclusions</title>
      <p>The latest version of <italic>Gaia</italic> catalogue, <italic>Gaia</italic> DR3, which has considerably improved proper motions and stellar parallaxes with respect to <italic>Gaia</italic> DR2, allows us to have a better understanding of the objects lying in the direction of the Cyg OB2 association. This region is complex due to the fact that the spatial structure along the line of sight shows several stellar groupings such as the Cyg OB2 association, the Left and Right over-densities found by Orellana <italic>et al.</italic> (2021) [<xref ref-type="bibr" rid="B9">9</xref>] and open clusters.</p>
      <p>Using the five astrometric parameters of the catalogue <italic>Gaia</italic> DR3 (<inline-formula><mml:math display="inline"><mml:mi> α </mml:mi></mml:math></inline-formula> , <inline-formula><mml:math display="inline"><mml:mi> δ </mml:mi></mml:math></inline-formula> , <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> μ </mml:mi><mml:mi> α </mml:mi></mml:msub><mml:mi> cos </mml:mi><mml:mi> δ </mml:mi></mml:mrow></mml:math></inline-formula> , <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> μ </mml:mi><mml:mi> δ </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> , <inline-formula><mml:math display="inline"><mml:mi> ϖ </mml:mi></mml:math></inline-formula> ), the HDBSCAN clustering algorithm allows us to detect 20 known OCs (IRAS-20306+4005, Dolidze 8, Roslund 6, Cr421, NGC 6910, UBC 585, FSR 0238, OC-124, OC-123, OC-128, FSR 0224, Dolidze 11, Bica 1, Bica 2, HSC 618, HSC 625, HSC 626, HSC 630, FSR 0236 and FSR 0227) and four unnoticed ones named as RSL-03, RSL-04, RSL-05 and RSL-06 in a circular region centred at <inline-formula><mml:math display="inline"><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> l </mml:mi><mml:mn> , </mml:mn><mml:mi> b </mml:mi></mml:mrow><mml:mo> ) </mml:mo></mml:mrow><mml:mo> = </mml:mo><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:msup><mml:mrow><mml:mn> 79.8 </mml:mn></mml:mrow><mml:mo> ∘ </mml:mo></mml:msup><mml:mn> , </mml:mn><mml:mo> + </mml:mo><mml:msup><mml:mrow><mml:mn> 0.8 </mml:mn></mml:mrow><mml:mo> ∘ </mml:mo></mml:msup></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> of radius 1.5˚ up to <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> G </mml:mi><mml:mo> = </mml:mo><mml:mn> 19.5 </mml:mn></mml:mrow></mml:math></inline-formula> mag. For all these clusters, we calculate the coordinates of the cluster centre, the mean proper motion, and the mean parallax and estimate the distance. Our values are consistent with those reported in the literature. This is the first time that Bica 1 and Bica 2 have been identified using the Gaia DR3 five astrometric parameters, and their parameters have improved with high precision. In addition, the members of FSR 0236 and FSR 0238 are identified with <italic>Gaia</italic> DR3 data for the first time and the parameters of the clusters are determined. The analysis of the mean proper motion and distance for FSR 0224, FSR 0236, FSR 0238, NGC 6910, RSL-04, RSL-05, RSL-06, HSC 625, OC-123, OC-128, Bica 1 and Bica 2 suggests that these OCs would be related to the Cyg OB2 association. RSL-02 ≡ HSC 630, located at 1346 pc, has similar values of mean proper motion and distance to those of the Left over-density named by Orellana <italic>et al.</italic> (2021) [<xref ref-type="bibr" rid="B9">9</xref>], suggesting that both objects would be related.</p>
      <p>We also identified the members for each of the clusters found in the region. When comparing our results with those present in the literature, we find significant differences especially with those reported by Hunt &amp; Reffert (2023) [<xref ref-type="bibr" rid="B19">19</xref>]. Our analysis demonstrates that these differences are due to the presence of false positives in their results which arise from neglecting the uncertainties in parallaxes. For this reason, we adopt parallaxes with a fractional error <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> f </mml:mi><mml:mo> = </mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mi> σ </mml:mi><mml:mi> ϖ </mml:mi></mml:msub></mml:mrow><mml:mi> ϖ </mml:mi></mml:mfrac><mml:mo> ≤ </mml:mo><mml:mn> 0.20 </mml:mn></mml:mrow></mml:math></inline-formula> in order to eliminate spurious data and ensure the reliability of our results (criterion v). The low percentage of common members, as shown in <xref ref-type="fig" rid="fig4">Figure 4</xref> and <bold>Table</bold><bold>4</bold>, reflects the influence of the selection criteria adopted. Having more accurate membership lists enables a better characterization of clusters. </p>
      <p>Through the analysis of <italic>Gaia</italic> and NIR 2MASS photometric data, using PARSEC isochrone models, we study the physical parameters of the four new open clusters detected, IRAS-20306+4005, HSC 630, and four OCs within the Cyg OB2 core. The age range for these clusters would be between 4 and 26 Myr, and the visual absorption ranges from 1.3 to 6.3 mag.</p>
    </sec>
    <sec id="sec6">
      <title>Acknowledgements</title>
      <p>We thank E. Giorgi and R. Vallverdú for many useful comments which improved this paper. This work has made use of data from the European Space Agency (ESA) mission <italic>Gaia</italic> (<ext-link ext-link-type="uri" xlink:href="https://www.cosmos.esa.int/gaia">https://www.cosmos.esa.int/gaia</ext-link>), processed by the <italic>Gaia</italic> Data Processing and Analysis Consortium (DPAC, <ext-link ext-link-type="uri" xlink:href="https://www.cosmos.esa.int/web/gaia/dpac/consortium">https://www.cosmos.esa.int/web/gaia/dpac/consortium</ext-link>). Funding for the DPAC has been provided by national institutions, in particular the institutions participating in the <italic>Gaia</italic> Multilateral Agreement.</p>
      <p>This research has made use of “Aladin sky atlas” developed at CDS, Strasbourg Observatory, France [<xref ref-type="bibr" rid="B49">49</xref>].</p>
      <p>This research has made use of the APASS database, located at the AAVSO web site. Funding for APASS has been provided by the Robert Martin Ayers Sciences Fund.</p>
      <p>This work was supported by Consejo Nacional de Investigaciones Científicas y Técnicas (CONICET), Argentina, under grants PIP 0507 and by Universidad Nacional de La Plata (UNLP), Argentina, under grants no. 11/G172 and PPID/ G005. </p>
    </sec>
    <sec id="sec7">
      <title>NOTES</title>
      <p><sup>1</sup><ext-link ext-link-type="uri" xlink:href="http://www.aavso.org/apass">http://www.aavso.org/apass</ext-link>.</p>
    </sec>
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