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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Astron. Space Sci.</journal-id>
<journal-title>Frontiers in Astronomy and Space Sciences</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Astron. Space Sci.</abbrev-journal-title>
<issn pub-type="epub">2296-987X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">897904</article-id>
<article-id pub-id-type="doi">10.3389/fspas.2022.897904</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Astronomy and Space Sciences</subject>
<subj-group>
<subject>Mini Review</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Exploitation of the IPHAS to Investigate Planetary Nebulae</article-title>
<alt-title alt-title-type="left-running-head">Sabin et&#xa0;al.</alt-title>
<alt-title alt-title-type="right-running-head">IPHAS PNe</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Sabin</surname>
<given-names>Laurence</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1552849/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Toal&#xe1;</surname>
<given-names>Jes&#xfa;s A.</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Ramos-Larios</surname>
<given-names>Gerardo</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>&#x2009;Guerrero</surname>
<given-names>Mart&#xed;n A.</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>Instituto de Astronom&#xED;a</institution>, <institution>UNAM</institution>, <addr-line>Ensenada</addr-line>, <country>Mexico</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Instituto de Radioastronom&#xED;a y Astrofis&#xED;ca</institution>, <institution>UNAM Campus Morelia</institution>, <addr-line>Morelia</addr-line>, <country>Mexico</country>
</aff>
<aff id="aff3">
<sup>3</sup>
<institution>Instituto de Astronom&#xED;a y Meteorolog&#xED;a</institution>, <institution>CUCEI</institution>, <institution>Universidad de Guadalajara</institution>, <addr-line>Guadalajara</addr-line>, <country>Mexico</country>
</aff>
<aff id="aff4">
<sup>4</sup>
<institution>Instituto de Astrof&#xED;sica de Andaluc&#xED;a</institution>, <institution>IAA-CSIC</institution>, <addr-line>Granada</addr-line>, <country>Spain</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>
<bold>Edited by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1453244/overview">Marcelo Miguel Miller Bertolami</ext-link>, CONICET Instituto de Astrof&#xed;sica de La Plata (IALP), Argentina</p>
</fn>
<fn fn-type="edited-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/224170/overview">Milan S. Dimitrijevic</ext-link>, Astronomical Observatory, Serbia</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Laurence Sabin, <email>lsabin@astro.unam.mx</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Stellar and Solar Physics, a section of the journal Frontiers in Astronomy and Space Sciences</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>10</day>
<month>05</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="collection">
<year>2022</year>
</pub-date>
<volume>9</volume>
<elocation-id>897904</elocation-id>
<history>
<date date-type="received">
<day>16</day>
<month>03</month>
<year>2022</year>
</date>
<date date-type="accepted">
<day>04</day>
<month>04</month>
<year>2022</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2022 Sabin, Toal&#xe1;, Ramos-Larios and &#x2009;Guerrero.</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Sabin, Toal&#xe1;, Ramos-Larios and &#x2009;Guerrero</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p>
</license>
</permissions>
<abstract>
<p>Similar to other classes of astronomical objects, there is a large discrepancy between the total count of theoretically predicted planetary nebulae (PNe) and the number of those actually observed. This discrepancy introduces bias in our attempt to globally understand and characterize the PNe population. Major efforts have been made to find the <italic>missing PNe</italic>. In particular, the INT Photometric H<italic>&#x3b1;</italic> Survey (IPHAS) has, since its debut, provided a whelm of new (candidate) PNe, some of which have been studied in depth using various methodologies such as deep imaging and low- and high-resolution spectroscopy. Here, we present the outcome of the analysis of a first group of these well-investigated <italic>IPHAS PNe</italic> with a focus on the extended ones. We show that, in general, the missing objects that were expected to be unveiled by the survey (low density, evolved, and distant) are indeed discovered, but the survey also allows the retrieval of &#x201c;simply&#x201d; overlooked PNe.</p>
</abstract>
<kwd-group>
<kwd>survey</kwd>
<kwd>optical</kwd>
<kwd>planetary nebulae</kwd>
<kwd>IPHAS</kwd>
<kwd>census</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="s1">
<title>1 Introduction</title>
<p>Planetary nebulae (PNe) are ionized shells of gas and dust that represent the late stage of the evolution of low- and intermediate-mass stars (&#x223c;1&#x2013;8&#xa0;M&#x2299;). Their importance in terms of chemical enrichment of the Galaxy, distance estimators, and plasma laboratories is well known, and a full review can be found in <xref ref-type="bibr" rid="B17">Kwitter and Henry&#xa0;(2022)</xref>.</p>
<p>In order to improve our knowledge of PNe, a good census of this population is needed, if not crucial. Actually, the &#x223c;3,500 currently known Galactic PNe<xref ref-type="fn" rid="fn1">
<sup>1</sup>
</xref>
<fn id="fn1">
<label>1</label>
<p>They are compiled in the Hong Kong/AAO/Strasbourg H<italic>&#x3b1;</italic> planetary nebula database (HASH) (<xref ref-type="bibr" rid="B19">Parker&#xa0;et&#xa0;al.,&#xa0;2016)</xref>.</p>
</fn> only represent a fraction of the total estimated number of &#x223c;25,000 objects (<xref ref-type="bibr" rid="B16">Jacoby&#xa0;et&#xa0;al.,&#xa0;2010</xref>; <xref ref-type="bibr" rid="B9">Frew,&#xa0;2017</xref>). Several surveys, particularly with narrowband H<italic>&#x3b1;</italic> filters, have been conducted to unveil the missing PNe, that is, those with low surface brightness, compact, and located in crowded areas, obscured by dust, for example (<xref ref-type="bibr" rid="B27">Sabin,&#xa0;2008</xref>; <xref ref-type="bibr" rid="B10">Frew&#xa0;et&#xa0;al.,&#xa0;2016</xref>).</p>
<p>We focus on the outcome of the INT Photometric H<italic>&#x3b1;</italic> Survey (IPHAS) by <xref ref-type="bibr" rid="B7">Drew&#xa0;et&#xa0;al.&#xa0;(2005)</xref>, which scanned the northern Galactic plane over 1800 deg<sup>2</sup> and allowed the discovery of various new PNe. The subsequent deep analysis of these objects will be the center of our discussion, so we can see the characteristics of PNe unveiled by this survey.</p>
<p>This article is organized as follows. In <xref ref-type="sec" rid="s2">Section&#xa0;2</xref>, we present the IPHAS. In <xref ref-type="sec" rid="s3">Section&#xa0;3</xref>, we present the different works conducted on specific PNe and a comparative analysis based on various parameters. Our discussion and conclusions are presented in <xref ref-type="sec" rid="s4">Section&#xa0;4</xref>.</p>
</sec>
<sec id="s2">
<title>2 INT Photometric H<italic>&#x3b1;</italic> Survey</title>
<p>As aforementioned, IPHAS scanned the northern part of the Galactic plane in the restricted galactic latitude range &#xb1;5&#xb0;. The survey was conducted in the H<italic>&#x3b1;</italic>, using r&#x2019; and i&#x2019; filters with a wide-field camera mounted on the 2.5-m Isaac Newton Telescope (La Palma, Spain). One of the advantages of this CCD survey compared to previous ones is the depth reached. Indeed, IPHAS can target compact sources down to &#x223c;21 mag in r&#x2019; and &#x223c;20 mag in H<italic>&#x3b1;</italic> and extended sources down to 2.5 &#xd7; 10<sup>&#x2013;16</sup>&#xa0;erg&#xa0;cm<sup>&#x2212;2</sup> s<sup>&#x2212;1</sup> arcsec<sup>&#x2212;2</sup>&#xa0;at binning 1 (0.33 arcsec/pixel) and <inline-formula id="inf1">
<mml:math id="m1">
<mml:mo>&#x223c;</mml:mo>
<mml:mn>1</mml:mn>
<mml:msup>
<mml:mrow>
<mml:mn>0</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>17</mml:mn>
</mml:mrow>
</mml:msup>
</mml:math>
</inline-formula> erg&#xa0;cm<sup>&#x2212;2</sup> s<sup>&#x2212;1</sup> arcsec<sup>&#x2212;2</sup>&#xa0;at binning 15 (5 arcsec/pixel).</p>
<p>The survey produced various general photometric and imaging catalogs (<xref ref-type="bibr" rid="B12">Gonz&#xe1;lez-Solares&#xa0;et&#xa0;al.,&#xa0;2008</xref>; <xref ref-type="bibr" rid="B2">Barentsen&#xa0;et&#xa0;al.,&#xa0;2014</xref>; <xref ref-type="bibr" rid="B29">Sale&#xa0;et&#xa0;al.,&#xa0;2014</xref>; <xref ref-type="bibr" rid="B30">Scaringi&#xa0;et&#xa0;al.,&#xa0;2018</xref>; <xref ref-type="bibr" rid="B18">Mongui&#xf3;&#xa0;et&#xa0;al.,&#xa0;2020</xref>; <xref ref-type="bibr" rid="B8">Fratta&#xa0;et&#xa0;al.,&#xa0;2021</xref>; <xref ref-type="bibr" rid="B13">Greimel&#xa0;et&#xa0;al.,&#xa0;2021</xref>), but it also focused on dedicated astronomical objects such as PNe for instance.</p>
<p>Hence, within the IPHAS consortium, several articles and catalogs reporting the detection of new PN candidates have been presented by <xref ref-type="bibr" rid="B3">Corradi&#xa0;et&#xa0;al.&#xa0;(2005)</xref>, <xref ref-type="bibr" rid="B31">Viironen&#xa0;et&#xa0;al.&#xa0;(2009a)</xref>, <xref ref-type="bibr" rid="B28">Sabin&#xa0;et&#xa0;al.&#xa0;(2010)</xref>, and <xref ref-type="bibr" rid="B26">Sabin&#xa0;et&#xa0;al.&#xa0;(2014)</xref>, and some still have to be introduced (see Ritters et&#xa0;al. submitted).</p>
<p>The first results of these searches indicated 781 compact PNe candidates and 157 true, likely, and possibly extended PNe. In addition to the detection reports, studies directed toward distance determination using the extinction method (<xref ref-type="bibr" rid="B11">Giammanco&#xa0;et&#xa0;al.,&#xa0;2011</xref>; <xref ref-type="bibr" rid="B6">Dharmawardena&#xa0;et&#xa0;al.,&#xa0;2021</xref>), the H<sub>2</sub> molecular content (<xref ref-type="bibr" rid="B22">Ramos-Larios&#xa0;et&#xa0;al.,&#xa0;2017</xref>), a classification system (<xref ref-type="bibr" rid="B1">Akras&#xa0;et&#xa0;al.,&#xa0;2019</xref>), and deep imaging of a sample of PNe (<xref ref-type="bibr" rid="B24">Sabin&#xa0;et&#xa0;al.,&#xa0;2021a</xref>) were conducted.</p>
<p>Detailed characteristics of the <italic>IPHAS PNe</italic> need to be studied in order to better understand the type of objects that would preferentially be detected using the survey and to identify how it is contributing to the increase of our knowledge of these evolved stars.</p>
</sec>
<sec id="s3">
<title>3 Comparative Study of Investigated INT Photometric H<italic>&#x3b1;</italic> Survey Planetary Nebulae</title>
<p>Among all PNe identified with IPHAS, few have been thoroughly investigated, that is, in terms of morphological structure, physical parameters, abundances, and kinematics (<xref ref-type="fig" rid="F1">Figure&#xa0;1</xref>). We cite a group of ten extended PNe (with the nomenclature <italic>IPHASX J</italic>) that have been studied by the following teams:<list list-type="bullet">
<list-item>
<p>&#x2022; IPHASX J191104.8&#x2b;060845 (<xref ref-type="bibr" rid="B23">Rodr&#xed;guez-Gonz&#xe1;lez&#xa0;et&#xa0;al.,&#xa0;2021</xref>)</p>
</list-item>
<list-item>
<p>&#x2022; IPHASX J055242.8&#x2b;262116 (<xref ref-type="bibr" rid="B14">Guerrero&#xa0;et&#xa0;al.,&#xa0;2021</xref>)</p>
</list-item>
<list-item>
<p>&#x2022; IPHASX J193718.6&#x2b;202102 (<xref ref-type="bibr" rid="B25">Sabin&#xa0;et&#xa0;al.,&#xa0;2021b</xref>)</p>
</list-item>
<list-item>
<p>&#x2022; IPHASX J211420.0&#x2b;434136 <xref ref-type="bibr" rid="B4">Corradi&#xa0;et&#xa0;al.&#xa0;(2014)</xref>
</p>
</list-item>
<list-item>
<p>&#x2022; IPHASX J194226.1&#x2b;214522, IPHASX J195248.8&#x2b;255359, and IPHASX J232713.1&#x2b;650923 (<xref ref-type="bibr" rid="B15">Hsia and Zhang,&#xa0;2014</xref>)</p>
</list-item>
<list-item>
<p>&#x2022; IPHASX J194359.5&#x2b;170901 (<xref ref-type="bibr" rid="B5">Corradi&#xa0;et&#xa0;al.,&#xa0;2011</xref>)</p>
</list-item>
<list-item>
<p>&#x2022; IPHASX J052531.2&#x2b;281945.1 <xref ref-type="bibr" rid="B32">Viironen&#xa0;et&#xa0;al.&#xa0;(2011)</xref>
</p>
</list-item>
<list-item>
<p>&#x2022; IPHASX J221118.0&#x2b;552841.0 (<xref ref-type="bibr" rid="B33">Viironen&#xa0;et&#xa0;al.,&#xa0;2009b</xref>)</p>
</list-item>
</list>
</p>
<p>All the investigations were not conducted under the same circumstances. For instance, they did not use the same facilities/instruments, and therefore, while some spectroscopic analyses were realized with 2-m class telescopes (e.g., INT), others were conducted with the 10-m class GranTeCan (La Palma). Although this would affect the precision and accuracy of the emission line detection and measurement, it will still be possible to compare some basic characteristics, as shown in <xref ref-type="table" rid="T1">Table&#xa0;1</xref>.</p>
<p>Hence, most of the PNe analyzed were either bipolar or round, which should be regarded as a selection bias rather than a trend. Indeed, the first objects to be investigated were the &#x201c;brightest&#x201d; (particularly for the spectroscopic analysis) and the most interesting and intriguing ones from a morphological point of view. The objects are small-to-medium sized with a maximum extent of 1 arcmin. The distances were measured either with a statistical method (e.g., H<italic>&#x3b1;</italic> surface brightness method; <xref ref-type="bibr" rid="B10">Frew&#xa0;et&#xa0;al.,&#xa0;2016</xref>) or <italic>via</italic> the extinction method (<xref ref-type="bibr" rid="B11">Giammanco&#xa0;et&#xa0;al.,&#xa0;2011</xref>). The results indicate distances greater than 2&#xa0;kpc in general and up to &#x223c;13&#xa0;kpc with an average of &#x223c;6&#xa0;kpc. The spectroscopic analysis points toward a large range of logarithmic extinction values c (H<italic>&#x3b2;</italic>), from 0.55 to 3.36, indicating a wide variety of nebular environments. While electronic temperatures (T<sub>
<italic>e</italic>
</sub>) can be described as low to typical for PNe (with values between &#x223c;8000&#xa0;K and &#x223c;13000&#xa0;K), the electronic densities (n<sub>
<italic>e</italic>
</sub>) are particularly low, with a mean of &#x223c;290&#xa0;cm<sup>&#x2212;3</sup> if we remove the only high-density PN IPHASX J194226.1&#x2b;214522. Finally, in various cases, it was possible to derive the (kinematic) ages of the nebulae and all indicated values &#x2265;10,000&#xa0;years, that is, evolved PNe. Joint analysis of the elemental abundances (helium, oxygen, and nitrogen in particular) and velocities of the PNe revealed a wide range of Peimbert&#x2019;s types (<xref ref-type="bibr" rid="B20">Peimbert,&#xa0;1978</xref>; <xref ref-type="bibr" rid="B21">Peimbert and Serrano,&#xa0;1980</xref>), therefore implying a range of masses for the progenitors. In the small sample of investigated IPHAS PN, we found Type I (J191104.8 and maybe J194359.5), Type II (J193718.6 and J052531.2), and Type III (J055242.8) objects. When a larger number of IPHAS PNe will have their elemental abundances determined and investigated, it will be possible to have a better global understanding of the chemistry of these objects.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Nordic Optical Telescope RGB-composite pictures of the IPHAS sources IPHASX J193718.6&#x2b;202102 <bold>(A)</bold> and IPHASX J221118.0&#x2b;552841 <bold>(B)</bold>, respectively, where the color red was assigned to the [N II] <italic>&#x3bb;</italic>
<sub>
<italic>c</italic>
</sub> &#x3d; 6,583&#xa0;&#xc5;,&#x2009;green for the H<italic>&#x3b1;&#xa0;&#x3bb;</italic>
<sub>
<italic>c</italic>
</sub> &#x3d; 6,563&#xa0;&#xc5;,&#x2009;and blue for the [O III] <italic>&#x3bb;</italic>
<sub>
<italic>c</italic>
</sub> &#x3d; 5,007&#xa0;&#xc5; filters. Faint bipolar lobes are barely visible in IPHASX J221118.0&#x2b;552841&#xa0;at the north and south of the main nebula, while IPHASX J193718.6&#x2b;202102 was extensively studied by <xref ref-type="bibr" rid="B25">Sabin&#xa0;et&#xa0;al.&#xa0;(2021b)</xref>, reporting chemical abundances typical of Type II PNe.</p>
</caption>
<graphic xlink:href="fspas-09-897904-g001.tif"/>
</fig>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Optical physical parameters reported for the group of 10 IPHAS PNe.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">PN IPHASX</th>
<th align="center">Main Morph.</th>
<th align="center">Size (&#x201d;)</th>
<th align="center">Distance (kpc)</th>
<th align="center">c (H<italic>&#x3b2;</italic>)</th>
<th align="center">T<sub>
<italic>e</italic>
</sub> (K)</th>
<th align="center">n<sub>
<italic>e</italic>
</sub> (cm<sup>&#x2212;3</sup>)</th>
<th align="center">Age (yrs)</th>
<th align="center">Ref</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">J191104.8</td>
<td align="center">B</td>
<td align="center">30</td>
<td align="center">
<inline-formula id="inf2">
<mml:math id="m2">
<mml:mo>&#x3c;</mml:mo>
<mml:mn>4.9</mml:mn>
<mml:mo>&#xb1;</mml:mo>
<mml:mn>0.6</mml:mn>
<mml:mo>&#x3e;</mml:mo>
</mml:math>
</inline-formula>
</td>
<td align="center">3.36 &#xb1; 0.16</td>
<td align="center">8,000 &#xb1; 1800</td>
<td align="center">260 &#xb1; 20</td>
<td align="center">11,000 &#xb1; 1,500</td>
<td align="center">a</td>
</tr>
<tr>
<td align="left">J055242.8</td>
<td align="center">R</td>
<td align="center">16.4</td>
<td align="center">
<inline-formula id="inf3">
<mml:math id="m3">
<mml:mn>2</mml:mn>
<mml:mo>.</mml:mo>
<mml:msubsup>
<mml:mrow>
<mml:mn>6</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>0.7</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2b;</mml:mo>
<mml:mn>1.3</mml:mn>
</mml:mrow>
</mml:msubsup>
</mml:math>
</inline-formula>
</td>
<td align="center">
<inline-formula id="inf4">
<mml:math id="m4">
<mml:mo>&#x3c;</mml:mo>
<mml:mn>1.84</mml:mn>
<mml:mo>&#xb1;</mml:mo>
<mml:mn>0.07</mml:mn>
<mml:mo>&#x3e;</mml:mo>
</mml:math>
</inline-formula>
</td>
<td align="center">&#x2020;</td>
<td align="center">&#x2020;</td>
<td align="center">
<inline-formula id="inf5">
<mml:math id="m5">
<mml:mn>1040</mml:mn>
<mml:msubsup>
<mml:mrow>
<mml:mn>0</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>3000</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2b;</mml:mo>
<mml:mn>5000</mml:mn>
</mml:mrow>
</mml:msubsup>
</mml:math>
</inline-formula>
</td>
<td align="center">b</td>
</tr>
<tr>
<td align="left">J193718.6</td>
<td align="center">B</td>
<td align="center">60</td>
<td align="center">
<inline-formula id="inf6">
<mml:math id="m6">
<mml:mn>7</mml:mn>
<mml:mo>.</mml:mo>
<mml:msubsup>
<mml:mrow>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>0.3</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2b;</mml:mo>
<mml:mn>0.8</mml:mn>
</mml:mrow>
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</inline-formula>
</td>
<td align="center">
<inline-formula id="inf7">
<mml:math id="m7">
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<mml:mo>&#x3e;</mml:mo>
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<td align="center">
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<td align="center">
<inline-formula id="inf9">
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<mml:mo>&#x3c;</mml:mo>
<mml:mn>380</mml:mn>
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<td align="center">26,000</td>
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<tr>
<td align="left">J211420.0</td>
<td align="center">B</td>
<td align="center">60</td>
<td align="center">&#x2264;5.0 &#xb1; 1.0</td>
<td align="center">0.95 &#xb1; 0.25</td>
<td align="center">13,050 &#xb1; 850</td>
<td align="center">125 &#xb1; 40</td>
<td align="center">&#x2014;</td>
<td align="center">d</td>
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<tr>
<td align="left">J194226.1</td>
<td align="center">B</td>
<td align="center">23</td>
<td align="center">4.76 &#xb1; 2.38</td>
<td align="center">&#x2a;</td>
<td align="center">&#x2a;</td>
<td align="center">
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<mml:mo>&#x2212;</mml:mo>
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<mml:mo>&#x2b;</mml:mo>
<mml:mn>4100</mml:mn>
</mml:mrow>
</mml:msubsup>
</mml:math>
</inline-formula>
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<td align="center">9,900 &#xb1; 4,950</td>
<td align="center">e</td>
</tr>
<tr>
<td align="left">J195248.8</td>
<td align="center">B</td>
<td align="center">26</td>
<td align="center">5.56 &#xb1; 2.78</td>
<td align="center">&#x2a;</td>
<td align="center">&#x2a;</td>
<td align="center">
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<mml:mo>&#x2212;</mml:mo>
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<mml:mn>430</mml:mn>
</mml:mrow>
</mml:msubsup>
</mml:math>
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<td align="center">10,400 &#xb1; 5,300</td>
<td align="center">e</td>
</tr>
<tr>
<td align="left">J232713.1</td>
<td align="center">R</td>
<td align="center">18</td>
<td align="center">&#x2013;</td>
<td align="center">1.63 &#xb1; 1.01</td>
<td align="center">&#x2a;</td>
<td align="center">
<inline-formula id="inf12">
<mml:math id="m12">
<mml:mn>30</mml:mn>
<mml:msubsup>
<mml:mrow>
<mml:mn>0</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>180</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2b;</mml:mo>
<mml:mn>150</mml:mn>
</mml:mrow>
</mml:msubsup>
</mml:math>
</inline-formula>
</td>
<td align="center">&#x2014;</td>
<td align="center">e</td>
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<tr>
<td align="left">J194359.5</td>
<td align="center">B</td>
<td align="center">21</td>
<td align="center">4.6 &#xb1; 1.1</td>
<td align="center">0.55 &#xb1; 0.06</td>
<td align="center">
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<mml:math id="m13">
<mml:mn>1100</mml:mn>
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<mml:mrow>
<mml:mn>0</mml:mn>
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<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>2000</mml:mn>
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<mml:mrow>
<mml:mo>&#x2b;</mml:mo>
<mml:mn>2000</mml:mn>
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</inline-formula>
</td>
<td align="center">
<inline-formula id="inf14">
<mml:math id="m14">
<mml:mn>36</mml:mn>
<mml:msubsup>
<mml:mrow>
<mml:mn>0</mml:mn>
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<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
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<mml:mo>&#x2b;</mml:mo>
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<td align="center">13,000 (&#x2021;)</td>
<td align="center">f</td>
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<td align="left">J052531.2</td>
<td align="center">R</td>
<td align="center">10</td>
<td align="center">12.8 &#xb1; 3.7</td>
<td align="center">0.8 &#xb1; 0.1</td>
<td align="center">
<inline-formula id="inf15">
<mml:math id="m15">
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<td align="center">190 &#xb1; 120</td>
<td align="center">17,800</td>
<td align="center">g</td>
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<tr>
<td align="left">J221118.0</td>
<td align="center">B</td>
<td align="center">79</td>
<td align="center">6.1 &#xb1; 1.1</td>
<td align="center">1.19 &#xb1;&#xa0;0.15</td>
<td align="center">&#x2014;</td>
<td align="center">&#x2014;</td>
<td align="center">&#x2014;</td>
<td align="center">h</td>
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</table>
<table-wrap-foot>
<fn>
<p>
<italic>a</italic>-<xref ref-type="bibr" rid="B23">Rodr&#xed;guez-Gonz&#xe1;lez&#xa0;et&#xa0;al.&#xa0;(2021)</xref>; <italic>b</italic>-<xref ref-type="bibr" rid="B14">Guerrero&#xa0;et&#xa0;al.&#xa0;(2021)</xref>: (&#x2020;)T<sub>
<italic>e</italic>
</sub> &#x3d; 11200K from CSPN, n<sub>
<italic>e</italic>
</sub> &#x3d; 4,000&#xa0;cm<sup>&#x2212;3</sup> from radio data; <italic>c</italic>-<xref ref-type="bibr" rid="B25">Sabin&#xa0;et&#xa0;al.&#xa0;(2021b)</xref>; <italic>d</italic>-<xref ref-type="bibr" rid="B4">Corradi&#xa0;et&#xa0;al.&#xa0;(2014)</xref>; <italic>e</italic>-<xref ref-type="bibr" rid="B15">Hsia and Zhang&#xa0;(2014)</xref>: (&#x2a;)No H<italic>&#x3b2;</italic> detected, Te &#x3d; 10,000&#xa0;K; <italic>f</italic>-<xref ref-type="bibr" rid="B5">Corradi&#xa0;et&#xa0;al.&#xa0;(2011)</xref>:&#x2021; for the polar caps, 5,000&#xa0;years for the inner ring; <italic>g</italic>-<xref ref-type="bibr" rid="B32">Viironen&#xa0;et&#xa0;al.&#xa0;(2011)</xref>; and <italic>h</italic>-<xref ref-type="bibr" rid="B33">Viironen&#xa0;et&#xa0;al.&#xa0;(2009b)</xref>.</p>
</fn>
</table-wrap-foot>
</table-wrap>
</sec>
<sec id="s4">
<title>4 Discussion and Conclusion</title>
<p>We can infer from <xref ref-type="table" rid="T1">Table&#xa0;1</xref> and the main points described earlier that IPHAS is indeed more prone to detect (very) evolved and low surface brightness objects (some have no detectable H<italic>&#x3b2;</italic> or the emission lines needed for electron temperature and density calculations). This ultimate stage of the nebular evolution is moreover underlined by the very low nebular densities that characterize the objects that were studied.</p>
<p>It is also worth noticing first that the PNe detected with IPHAS are not necessarily very extinguished, as new PNe with low-to-moderately high c (H<italic>&#x3b2;</italic>) are found. There is no doubt, however, that the survey can allow us to unveil very extinguished objects, as shown with IPHASX J191104.8&#x2b;060845 (<xref ref-type="bibr" rid="B23">Rodr&#xed;guez-Gonz&#xe1;lez&#xa0;et&#xa0;al.,&#xa0;2021</xref>) and its c (H<italic>&#x3b2;</italic>) value of 3.36 &#xb1; 0.16. In this regard, IPHAS is relatively complete in terms of the distance that can be reached through the interstellar medium. Then, we note that several objects show the presence of the HeII <italic>&#x3bb;</italic>4686&#xa0;&#xc5;&#x2009; emission line, which indicates an excitation degree (or class) from moderate (e.g., IPHASX J193718.6&#x2b;202102; <xref ref-type="bibr" rid="B25">Sabin&#xa0;et&#xa0;al.,&#xa0;2021b</xref>) to high (e.g., IPHASX J194359.5&#x2b;170901; <xref ref-type="bibr" rid="B5">Corradi&#xa0;et&#xa0;al.,&#xa0;2011</xref>).</p>
<p>The extended PNe detected and studied with IPHAS are mostly located at large distances, that is, from &#x223c;5&#xa0;kpc to 12.8&#xa0;kpc. We are likely to trace objects at larger galactocentric distances which can therefore be used to trace the chemical distribution. Indeed, this would have some impact on the determination of the Galactic abundance gradient.</p>
<p>Finally, it does not seem that IPHAS is targeting a particular (Peimbert&#x2019;s) type of PNe in terms of chemical abundances, and we would therefore have a spread in terms of progenitor&#x2019;s masses and characteristics. But a caveat is, as stated before, the general faintness of the PNe which makes difficult not only the estimation of the abundances but also the accuracy of the measurements.</p>
<p>In conclusion, based on the data collected for this first reduced sample of IPHAS extended PNe, we can therefore infer that IPHAS is fulfilling its objective as a discovery tool for the missing PNe. Indeed, it is targeting mostly evolved PNe (in terms of kinematic age), distant with low electronic density. In addition, while it can detect highly extinguished objects, IPHAS is also uncovering overlooked more &#x201c;extinction-free&#x201d; PNe. There is no doubt that the survey will strongly contribute to the understanding of the PNe population as a whole, but more complete analyses of IPHAS PNe, which implies observing and pushing the limits of the instrumentation, are needed for a stronger statistical view.</p>
</sec>
</body>
<back>
<sec id="s5">
<title>Author Contributions</title>
<p>LS, JT, and MG contributed to the conception of the study. LS wrote the first draft of the manuscript. GR-L prepared the figure. All authors contributed to manuscript revision, read, and approved the submitted version.</p>
</sec>
<sec id="s6">
<title>Funding</title>
<p>The funding source is UNAM PAPIIT project IN110122.</p>
</sec>
<sec sec-type="COI-statement" id="s7">
<title>Conflict of Interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec sec-type="disclaimer" id="s8">
<title>Publisher&#x2019;s Note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors, and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
<ack>
<p>LS acknowledges support from UNAM PAPIIT project IN110122 (Mexico). JT acknowledges support from the Fundaci&#xf3;n Marcos Moshinsky (Mexico) and UNAM PAPIIT project IA101622 (Mexico). GR-L acknowledges support from Consejo Nacional de Ciencia y Tecnolog&#xed;a (CONACYT) Grant 263373. MG acknowledges the support of Grant PGC 2018-102184-B-I00 of the Ministerio de Educaci&#xf3;n, Innovaci&#xf3;n y Universidades cofunded with FEDER funds.</p>
</ack>
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