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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Astron. Space Sci.</journal-id>
<journal-title>Frontiers in Astronomy and Space Sciences</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Astron. Space Sci.</abbrev-journal-title>
<issn pub-type="epub">2296-987X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fspas.2017.00058</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Astronomy and Space Sciences</subject>
<subj-group>
<subject>Perspective</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Probing the Gas Fueling and Outflows in Nearby AGN with ALMA</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name><surname>Audibert</surname> <given-names>Anelise</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="author-notes" rid="fn001"><sup>&#x0002A;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/473116/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Combes</surname> <given-names>Fran&#x000E7;oise</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/340256/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Garc&#x000ED;a-Burillo</surname> <given-names>Santiago</given-names></name>
<xref ref-type="aff" rid="aff3"><sup>3</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/483123/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Salom&#x000E9;</surname> <given-names>Philippe</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
</contrib>
</contrib-group>
<aff id="aff1"><sup>1</sup><institution>Observatoire de Paris, LERMA, Centre National de la Recherche Scientifique, PSL University, Sorbonne University, UPMC</institution>, <addr-line>Paris</addr-line>, <country>France</country></aff>
<aff id="aff2"><sup>2</sup><institution>College de France</institution>, <addr-line>Paris</addr-line>, <country>France</country></aff>
<aff id="aff3"><sup>3</sup><institution>Observatorio Astron&#x000F3;mico Nacional, Observatorio de Madrid</institution>, <addr-line>Madrid</addr-line>, <country>Spain</country></aff>
<author-notes>
<fn fn-type="edited-by"><p>Edited by: Mauro D&#x00027;Onofrio, Universit&#x000E0; degli Studi di Padova, Italy</p></fn>
<fn fn-type="edited-by"><p>Reviewed by: Daniela Bettoni, Osservatorio Astronomico di Padova (INAF), Italy; Anna Lia Longinotti, National Institute of Astrophysics, Optics and Electronics, Mexico</p></fn>
<fn fn-type="corresp" id="fn001"><p>&#x0002A;Correspondence: Anelise Audibert <email>anelise.audibert&#x00040;obspm.fr</email></p></fn>
<fn fn-type="other" id="fn002"><p>This article was submitted to Milky Way and Galaxies, a section of the journal Frontiers in Astronomy and Space Sciences</p></fn></author-notes>
<pub-date pub-type="epub">
<day>12</day>
<month>12</month>
<year>2017</year>
</pub-date>
<pub-date pub-type="collection">
<year>2017</year>
</pub-date>
<volume>4</volume>
<elocation-id>58</elocation-id>
<history>
<date date-type="received">
<day>30</day>
<month>09</month>
<year>2017</year>
</date>
<date date-type="accepted">
<day>27</day>
<month>11</month>
<year>2017</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#x000A9; 2017 Audibert, Combes, Garc&#x000ED;a-Burillo and Salom&#x000E9;.</copyright-statement>
<copyright-year>2017</copyright-year>
<copyright-holder>Audibert, Combes, Garc&#x000ED;a-Burillo and Salom&#x000E9;</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/"><p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) or licensor are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p></license>
</permissions>
<abstract><p>Feeding and feedback in AGN play a very important role to gain a proper understanding of galaxy formation and evolution. The interaction between activity mechanisms in the nucleus and its influence in the host galaxy are related to the physical processes involved in feedback and the gas fueling of the black hole. The discovery of many massive molecular outflows in the last few years have been promoting the idea that winds may be major actors in sweeping the gas out of galaxies. Also, the widely observed winds from the central regions of AGN are promising candidates to explain the scaling relations (e.g., the black hole-bulge mass relation, BH accretion rate tracking the star formation history) under the AGN feedback scenario. Out goal is to probe these phenomena through the kinematic and morphology of the gas inside the central kpc in nearby AGN. This has recently been possible due to the unprecedented ALMA spatial resolution and sensitivity. We present results on NGC7213 and NGC1808, the latter is part of a new ALMA follow-up of the NuGa project, a previous high-resolution (0.5&#x02013;1&#x02033;) CO survey of low luminosity AGN performed with the IRAM PdBI.</p></abstract>
<kwd-group>
<kwd>active galactic nuclei</kwd>
<kwd>extragalactic astronomy</kwd>
<kwd>evolution of galaxies</kwd>
<kwd>galaxies</kwd>
<kwd>spectroscopy</kwd>
</kwd-group>
<counts>
<fig-count count="4"/>
<table-count count="0"/>
<equation-count count="1"/>
<ref-count count="25"/>
<page-count count="5"/>
<word-count count="2957"/>
</counts>
</article-meta>
</front>
<body>
<sec sec-type="intro" id="s1">
<title>1. Introduction</title>
<p>The fueling of SMBH at the center of galaxies and the subsequent feedback from its active nuclei, are among the key processes to understand the concerted growth of galaxies and BH. AGN feedback is invoked to explain the formation of massive galaxies when we compare the luminosity function of galaxies to theoretical simulations based on the cold dark matter models (Silk and Mamon, <xref ref-type="bibr" rid="B21">2012</xref>). Winds and outflows produced by the AGN can eject or heat the gas, terminate the star formation and through the lack of fuel for accretion, quench the black hole activity. Recent discovery of many massive molecular outflows (e.g., Feruglio et al., <xref ref-type="bibr" rid="B9">2010</xref>; Fischer et al., <xref ref-type="bibr" rid="B10">2010</xref>; Alatalo et al., <xref ref-type="bibr" rid="B1">2011</xref>; Sturm et al., <xref ref-type="bibr" rid="B22">2011</xref>; Dasyra and Combes, <xref ref-type="bibr" rid="B6">2012</xref>; Veilleux et al., <xref ref-type="bibr" rid="B23">2013</xref>; Cicone et al., <xref ref-type="bibr" rid="B4">2014</xref>; Dasyra et al., <xref ref-type="bibr" rid="B7">2014</xref>; Garc&#x000ED;a-Burillo et al., <xref ref-type="bibr" rid="B13">2014</xref>) have been promoting the idea that winds may be major actors in sweeping the gas out of galaxies, in agreement with theoretical predictions of AGN driven winds models (Faucher-Gigu&#x000E8;re and Quataert, <xref ref-type="bibr" rid="B8">2012</xref>; Zubovas and King, <xref ref-type="bibr" rid="B24">2012</xref>, <xref ref-type="bibr" rid="B25">2014</xref>). However, it is still difficult to distinguish the origin of the outflows, whether they are AGN-driven or starburst-driven.</p>
<p>On the other hand, AGN are fueled by accretion of material onto the BH and the gas component can form stars on its way to the BH (Garc&#x000ED;a-Burillo and Combes, <xref ref-type="bibr" rid="B12">2012</xref>; Combes et al., <xref ref-type="bibr" rid="B5">2014</xref>). It is important to study the efficiency of angular momentum transport in galaxy disks in order to understand how the star formation and nuclear activity are fueled and what are the timescales involved, since both feeding process rely on a common cold gas supply, but in very different periods of time (&#x0007E;10<sup>5</sup> year for BH growth and &#x0007E;10<sup>7&#x02212;9</sup> year for star formation; Garc&#x000ED;a-Burillo, <xref ref-type="bibr" rid="B11">2016</xref>). In addition to this scenario, one of the outstanding problems is to identify the mechanism that drives gas from the disk toward the nucleus, removing its large angular momentum and forming large non-axisymmetric perturbations, such as bars or spirals.</p>
<p>This work aims to better understand the galaxies chemical and thermal evolution by studying in detail the physical processes acting on the nucleus of a sample of nearby AGN. Probing AGN feeding and feedback phenomena through the kinematic and morphology of the gas inside the central kpc have recently been possible due to the unprecedented Atacama Millimeter/Submillimeter Array (ALMA) spatial resolution (&#x02272;0.5&#x02033;) and sensitivity. Since there are only a few AGN observed with high spatial resolution, we investigate the nuclear molecular emission in a sample of nearby AGN making use of spectroscopic techniques.</p>
</sec>
<sec sec-type="methods" id="s2">
<title>2. Methodology</title>
<p>By applying the velocity channel maps on the dense molecular gas tracers, e.g., HCN, HCO<sup>&#x0002B;</sup>, CS, and mid transition of CO, we can access the gas kinematics. To detect possible inflows or outflows, we can compare the CO rotation curve with a rotational velocity model based on the H&#x003B1; kinematics and then subtract the model to analyse the velocity residuals in order to search for blue and redshifted patterns. Another possibility is to explore the current models for the rotation curve, when previous H&#x003B1; or H <sc>i</sc> are not available in the literature. One of this model is described by Bertola et al. (<xref ref-type="bibr" rid="B2">1991</xref>), assuming the gas is on circular orbits in a plane, <inline-formula><mml:math id="M1"><mml:msub><mml:mrow><mml:mi>&#x003C5;</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mi>A</mml:mi><mml:mi>r</mml:mi><mml:mo>/</mml:mo><mml:msup><mml:mrow><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:msup><mml:mrow><mml:mi>r</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mo>&#x0002B;</mml:mo><mml:msup><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mo>/</mml:mo><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, where for <italic>p</italic> &#x0003D; 1 the velocity curve is asymptotically flat and <italic>p</italic> &#x0003D; 3/2 the system has a finite total mass, therefore we expect 1 &#x02264; <italic>p</italic> &#x02264; 3/2. The observed radial velocity at a position (<italic>R</italic>, &#x003A8;) on the plane of the sky can be described as:</p>
<disp-formula id="E1"><label>(1)</label><mml:math id="M2"><mml:mtable class="eqnarray" columnalign="right center left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>&#x003C5;</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>o</mml:mi><mml:mi>d</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>R</mml:mi><mml:mo>,</mml:mo><mml:mtext>&#x003A8;</mml:mtext></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>&#x003C5;</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>y</mml:mi><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:mfrac><mml:mrow><mml:mi>A</mml:mi><mml:mi>R</mml:mi><mml:mi>c</mml:mi><mml:mi>o</mml:mi><mml:mi>s</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mtext>&#x003A8;</mml:mtext><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mtext>&#x003A8;</mml:mtext></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mi>s</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003B8;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mi>c</mml:mi><mml:mi>o</mml:mi><mml:msup><mml:mrow><mml:mi>s</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi></mml:mrow></mml:msup><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003B8;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:msup><mml:mrow><mml:mrow><mml:mo>{</mml:mo><mml:mrow><mml:msup><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mi>s</mml:mi><mml:mi>i</mml:mi><mml:msup><mml:mrow><mml:mi>n</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mtext>&#x003A8;</mml:mtext><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mtext>&#x003A8;</mml:mtext></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>&#x0002B;</mml:mo><mml:mi>c</mml:mi><mml:mi>o</mml:mi><mml:msup><mml:mrow><mml:mi>s</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003B8;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mi>c</mml:mi><mml:mi>o</mml:mi><mml:msup><mml:mrow><mml:mi>s</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mtext>&#x003A8;</mml:mtext><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mtext>&#x003A8;</mml:mtext></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>&#x0002B;</mml:mo><mml:msup><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mi>c</mml:mi><mml:mi>o</mml:mi><mml:msup><mml:mrow><mml:mi>s</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003B8;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mo>}</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mo>/</mml:mo><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:mfrac></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>where &#x003B8; is the inclination of the disk (with &#x003B8; &#x0003D; 0 for a face-on disk), &#x003A8;<sub>0</sub> is the position angle of the line of nodes, <italic>v</italic><sub><italic>sys</italic></sub> is the systemic velocity and <italic>R</italic> is the radius and <italic>A</italic>, <italic>c</italic>, and <italic>p</italic> are parameters of the model. In the cases of NGC 7213 and NGC 1808, we have used the Bertola et al. (<xref ref-type="bibr" rid="B2">1991</xref>) model to search for non-circular motions in their observed velocity field.</p>
</sec>
<sec sec-type="results" id="s3">
<title>3. Results</title>
<sec>
<title>3.1. NGC 7213</title>
<p>We report ALMA Cycle 1 observations of CO(2-1) at 229.2 GHz of NGC 7213, an early-type SA(s)a galaxy harboring a Seyfert 1/LINER. Previous neutral and ionized gas observations suggest the presence of a warped gaseous disk that could be the result of a merger. It presents a giant H&#x003B1; filament and two H<sc>i</sc> tidal tails, confirming to be a highly disturbed interaction system (Hameed et al., <xref ref-type="bibr" rid="B14">2001</xref>). Stellar kinematics is dominated by non-circular motions, along two spiral arms (Schnorr-M&#x000FC;ller et al., <xref ref-type="bibr" rid="B20">2014</xref>). In the central &#x0007E;3 kpc, the CO map reveals a a widely distributed multiple-arm spiral structure, tracing the dusty spiral arms, as can be seen in the HST image (Figure <xref ref-type="fig" rid="F1">1</xref>). There is an offset peak located at 200 pc north from the center, meaning that the peak of the CO emission is not concentrated in the very center.</p>
<fig id="F1" position="float">
<label>Figure 1</label>
<caption><p>In the left and middle panels we show an unsharp-masked F606W HST image and the original image with CO(2-1) contours overlaid, respectively. Right: CO(2-1) intensity map of NGC 7213 clipped at &#x0003E;5&#x003C3;. The green circle represents a 30&#x02033; diameter.</p></caption>
<graphic xlink:href="fspas-04-00058-g0001.tif"/>
</fig>
<p>In general, the velocity field in the left panel of Figure <xref ref-type="fig" rid="F2">2</xref> is well-described by rotation, presenting some slightly perturbations along the minor axis (at 10&#x02033;) probably due to streaming motions from the spiral arms. By applying the Bertola et al. (<xref ref-type="bibr" rid="B2">1991</xref>) model to generate a 2-D velocity model that minimizes the residuals, we find that the position angle is &#x02212;18&#x000B0; and the systemic velocity should be corrected in 30 km/s. The residuals do not indicate hints of a significant blue and/or red-shifted components and this result indicates that probably there is no molecular outflow in NGC 7213.</p>
<fig id="F2" position="float">
<label>Figure 2</label>
<caption><p>Left: Velocity map of NGC 7213 clipped at &#x0003E;5&#x003C3;. In the middle panel the best fit model using the Bertola et al. (<xref ref-type="bibr" rid="B2">1991</xref>) function and the residuals, after subtracting the model from the data, are shown on the right.</p></caption>
<graphic xlink:href="fspas-04-00058-g0002.tif"/>
</fig>
</sec>
<sec>
<title>3.2. NGC 1808</title>
<p>The &#x0201C;hot spot&#x0201D; galaxy NGC 1808 is remarkable for its very dusty appearance and especially for its well-known system of dark radial filaments. NGC 1808 is a Starburst/Seyfert 2 galaxy located at 9.1 Mpc and it is classified as a SAB(s)a. Accordingly to Reif et al. (<xref ref-type="bibr" rid="B18">1982</xref>), it has an inclination of 57&#x000B0;. Atomic gas traced with H <sc>i</sc> is concentrated in the galactic bar, disk, and a warped outer ring, indicating a tidal interaction in the past with the neighbor galaxy NGC 1792 (Koribalski et al., <xref ref-type="bibr" rid="B16">1996</xref>). It presents prominent polar dust lanes and gas outflow emerging from the nucleus, as revealed in optical studies that indicate an outflow of dust and neutral and ionized gas (as seen in H&#x003B1;, [N <sc>ii</sc>], Na <sc>i</sc> D, and H <sc>i</sc> by Koribalski et al., <xref ref-type="bibr" rid="B15">1993</xref>; Phillips, <xref ref-type="bibr" rid="B17">1993</xref>). In particular, Na <sc>i</sc> D is seen blueshifted in absorption and redshifted in emission and <italic>B</italic>-<italic>R</italic> images show that the dust plumes associated with the outflow reach &#x0007E;3 kpc above the plane. Near-infrared integral-field spectroscopy with SINFONI by Busch et al. (<xref ref-type="bibr" rid="B3">2017</xref>) showed a large gas reservoir and a disturbed gas velocity field that shows signs of inflowing streaming motion in the central &#x0007E;100 pc.</p>
<p>We report ALMA Cycle 3 observations of CO(3-2), CS(7-6), HCN(4-3), and HCO<sup>&#x0002B;</sup>(4-3) in band 7 with a resolution of 0.27&#x02033;. Figure <xref ref-type="fig" rid="F3">3</xref> shows that the CO emission follows the star-forming central 500 pc ring and the very center has a spiral trailing structure, that is also observed in CS, HCN, and HCO<sup>&#x0002B;</sup>.</p>
<fig id="F3" position="float">
<label>Figure 3</label>
<caption><p>From the left to the right panels: a WFC/F658N HST image followed by the 26&#x02033; diameter imaged area of CO(3-2) observations with ALMA. The next panels shows a zoom of the spiral trailing structure observed, and the subsequent plots show the same detection as seen in CS(7-6), HCO<sup>&#x0002B;</sup>(4-3), and HCN(4-3). All the intensity maps were clipped at &#x0003E;5&#x003C3;.</p></caption>
<graphic xlink:href="fspas-04-00058-g0003.tif"/>
</fig>
<p>From the velocity map in Figure <xref ref-type="fig" rid="F4">4</xref>, the dominant velocity feature appears to be due to circular rotation in the disk. After subtracting a model for the velocity field by Bertola et al. (<xref ref-type="bibr" rid="B2">1991</xref>), we do not find significant patterns in the residuals and if there is a presence of an molecular outflow in the galaxy, it will be difficult to disentangle from the dominant circular motion in the 1st moment distribution. We need to explore in details the position-velocity diagrams along the dust lanes observed in the HST images. Additionally, Salak et al. (<xref ref-type="bibr" rid="B19">2016</xref>) presented evidence of a molecular gas outflow seen in CO(1-0) from the nuclear starburst region (<italic>r</italic> &#x02272; 250 pc) that could be only detected in the position-velocity diagram. The outflow has a maximum velocity of &#x003C5;<sub><italic>out</italic></sub> &#x0007E;180 km/s and mass outflow rate between 1 and 10 M<sub>&#x02299;</sub>/year, comparable to the total star formation rate in the starburst 500 pc region, that corresponds to SFR &#x0007E; 5M<sub>&#x02299;</sub>/year in the &#x0201C;hot spots.&#x0201D; The kinematics of our CO(3-2) observations do not show strong outflows at this scale. Certainly, the outflow is more significant at larger scales. A further analysis of the molecular gas and the outflow in NGC 1808 will be present in a forthcoming paper (Audibert et al., in preparation).</p>
<fig id="F4" position="float">
<label>Figure 4</label>
<caption><p>Left: Velocity map of NGC 1808 clipped at &#x0003E;5&#x003C3;. In the middle panel the best fit model using the Bertola et al. (<xref ref-type="bibr" rid="B2">1991</xref>) function and the residuals, after subtracting the model from the data, are shown on the right.</p></caption>
<graphic xlink:href="fspas-04-00058-g0004.tif"/>
</fig>
</sec>
</sec>
<sec id="s4">
<title>4. Perspectives</title>
<p>We are going to apply the same methodology to search for outflows and inflows in a modest sample of nearby Seyfert/LINERs galaxies that are part of a new ALMA follow-up of the&#x02014;NUclei of GAlaxies (NuGa) project, a previous CO survey of low luminosity AGN performed with the IRAM PdBI. The new ALMA observations have the remarkable spatial resolution of &#x0007E;0.06&#x02013;0.09&#x02033;.</p>
</sec>
<sec id="s5">
<title>Author contributions</title>
<p>AA has written the article; AA and FC have contributed to reduce the data; FC and SG-B have written the proposal; and all four authors have contributed to interpret the data and comment the paper.</p>
<sec>
<title>Conflict of interest statement</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
</sec>
</body>
<back>
<ack>
<p>AA thanks the organizers of the &#x0201C;Quasars at All Cosmic Epochs&#x0201D; conference for support and the referees for useful comments. AA would like to acknowledge the financial support from the Brazilian scholarship program Science Without Borders&#x02014;CNPq (scholarship reference 234043/2014-8). This paper makes use of the following ALMA data: ADS/JAO.ALMA&#x00023; 2012.1.00474.S (PI: N. Nagar) and ADS/JAO.ALMA&#x00023; 2015.1.00404.S (PI: FC). ALMA is a partnership of ESO (representing its member states), NSF (USA), and NINS (Japan), together with NRC (Canada), NSC and ASIAA (Taiwan), and KASI (Republic of Korea), in cooperation with the Republic of Chile. The Joint ALMA Observatory is operated by ESO, AUI/NRAO, and NAOJ. We used observations made with the NASA/ESA Hubble Space Telescope, and obtained from the Hubble Legacy Archive, which is a collaboration between the Space Telescope Science Institute (STScI/NASA), the Space Telescope European Coordinating Facility (ST-ECF/ESA), and the Canadian Astronomy Data Center (CADC/NRC/CSA). This research has made use of the NASA/IPAC Extragalactic Database (NED) and of the HyperLeda database.</p>
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