<?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>2026-05-31T21:03:59Z</responseDate><request verb="GetRecord" identifier="oai:riuma.uma.es:10630/16757" metadataPrefix="marc">https://riuma.uma.es/rest/oai/request</request><GetRecord><record><header><identifier>oai:riuma.uma.es:10630/16757</identifier><datestamp>2026-02-03T12:42:10Z</datestamp><setSpec>com_10630_2254</setSpec><setSpec>col_10630_37957</setSpec></header><metadata><record xmlns="http://www.loc.gov/MARC21/slim" xmlns:dcterms="http://purl.org/dc/terms/" xmlns:doc="http://www.lyncode.com/xoai" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.loc.gov/MARC21/slim http://www.loc.gov/standards/marcxml/schema/MARC21slim.xsd">
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      <subfield code="a">Aké Hau, Luis Alberto</subfield>
      <subfield code="e">author</subfield>
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      <subfield code="c">2018-05</subfield>
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      <subfield code="a">Causality is a specific tool of Lorentzian Geometry, with a clear physical motivation, which has played a&#xd;
central role in proving important theorems about the global structure of spacetimes. Causality&#xd;
conditions are classified in terms of the so called causal ladder,&#xd;
whose steps determine how these conditions are logically related.&#xd;
Each of these levels presents some specific&#xd;
properties, standing out at the top one, which is occupied by the condition of global hyperbolicity.&#xd;
In fact, it is believed that any physical spacetime must be globally hyperbolic&#xd;
(roughly, this is the content of the strong cosmic censorship hypothesis), and then, will admit&#xd;
a global splitting in terms of a Cauchy surface, on which the Einstein equations can be posed as an initial value problem.&#xd;
&#xd;
Causality theory also provides a&#xd;
boundary construction for the very general class of strongly causal spacetimes, namely, the so-called causal boundary or just&#xd;
c-boundary. This boundary is less commonly used in General Relativity than the conformal one, because some classical spacetimes present a simple conformal boundary with quite a few of interesting properties. However, beyond such examples, there is no a general way to ensure that the conformal boundary exists. In contraposition, the c-boundary is not only conformally invariant but also intrinsic and it can be&#xd;
computed systematically; such properties make it more suitable in general situations. This includes the holographic principle, which original started at a restricted situation concerning the conformal boundary of Anti-de Sitter spacetime for the AdS/CFT correspondence. The main purpose of this memory is to improve our knowledge about the c-boundary and the causal ladder of some important classes of spacetimes.</subfield>
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      <subfield code="a">https://hdl.handle.net/10630/16757</subfield>
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      <subfield code="a">Geometría - Tesis doctorales</subfield>
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   <datafield ind2="0" ind1="0" tag="245">
      <subfield code="a">Some global causal properties in certain classes of spacetimes</subfield>
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