<?xml version="1.0" encoding="UTF-8"?><?xml-stylesheet type="text/xsl" href="static/style.xsl"?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-10-02T10:17:07Z</responseDate><request verb="GetRecord" identifier="oai:docta.ucm.es:20.500.14352/7970" metadataPrefix="marc">https://docta.ucm.es/rest/oai/request</request><GetRecord><record><header><identifier>oai:docta.ucm.es:20.500.14352/7970</identifier><datestamp>2024-09-10T17:54:08Z</datestamp><setSpec>com_20.500.14352_14</setSpec><setSpec>col_20.500.14352_15</setSpec></header><metadata><record xmlns="http://www.loc.gov/MARC21/slim" xmlns:dcterms="http://purl.org/dc/terms/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://www.loc.gov/MARC21/slim http://www.loc.gov/standards/marcxml/schema/MARC21slim.xsd">
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      <subfield code="a">Dullo, Bililign</subfield>
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      <subfield code="a">Gil De Paz, Armando</subfield>
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      <subfield code="a">Knapen, Johan H.</subfield>
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      <subfield code="c">2021-02</subfield>
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      <subfield code="a">We investigate the nature of the relations between black hole (BH) mass (M_(BH)) and the central velocity dispersion (σ) and, for core-S´ersic galaxies, the size of the depleted core (R_(b)). Our sample of 144 galaxies with dynamically determined M_(BH) encompasses 24 core-Sérsic galaxies, thought to be products of gas-poor mergers, and reliably identified based on high-resolution HST imaging. For core-S´ersic galaxies—i.e., combining normal-core (R_(b) &lt; 0.5 kpc) and large-core galaxies (R_(b) ˃̰ 0.5 kpc), we find that M_(BH) correlates remarkably well with R_(b) such that M_(BH) ∝ R^(1.20±0.14)_(b) (rms scatter in log M_(BH) of ∆_(rms) ∼ 0.29 dex), confirming previous works on the same galaxies except three new ones. Separating the sample into S´ersic, normal-core and large-core galaxies, we find that S´ersic and normal-core galaxies jointly define a single log-linear M_(BH) − σ relation M_(BH) ∝ σ^(4.88±0.29) with ∆_(rms) ∼ 0.47 dex, however, at the high-mass end large-core galaxies (four with measured M_(BH)) are offset upward from this relation by (2.5 − 4) × σ_(s), explaining the previously reported steepening of the M_(BH) − σ relation for massive galaxies. Large-core spheroids have magnitudes M_(V) ˂̰ −23.50 mag, half-light radii R_(e) ˃̰ 10 kpc and are extremely massive M * ˃̰ 10^(12)Mꙩ. Furthermore, these spheroids tend to host ultramassive BHs (M_(BH) ˃̰ 10^(10)Mꙩ) tightly connected with their R_(b) rather than σ. The less popular M_(BH) – R_(b) relation exhibits ∼ 62% less scatter in log M_(BH) than the M_(BH – σ) relations. Our findings suggest that large-core spheroids form via multiple major ‘dry’ merger events involving super/ultramassive BHs, consistent with the flattening of the σ – L_(V) relation observed at M_(V) ˂̰ −23.5 mag.</subfield>
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      <subfield code="a">0004-637X</subfield>
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      <subfield code="a">10.3847/1538-4357/abceae</subfield>
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      <subfield code="a">https://hdl.handle.net/20.500.14352/7970</subfield>
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      <subfield code="a">http://dx.doi.org/10.3847/1538-4357/abceae</subfield>
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      <subfield code="a">https://iopscience.iop.org/</subfield>
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   <datafield ind1="8" ind2=" " tag="024">
      <subfield code="a">https://arxiv.org/abs/2012.04471v1</subfield>
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   <datafield ind2="0" ind1="0" tag="245">
      <subfield code="a">Ultramassive black holes in the most massive galaxies: M_(BH – σ) versus M_(BH) – R_(B)</subfield>
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