<?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>2026-06-10T15:44:05Z</responseDate><request verb="GetRecord" identifier="oai:riubu.ubu.es:10259/10323" metadataPrefix="oai_dc">https://riubu.ubu.es/oai/request</request><GetRecord><record><header><identifier>oai:riubu.ubu.es:10259/10323</identifier><datestamp>2025-03-14T01:05:36Z</datestamp><setSpec>com_10259.4_2557</setSpec><setSpec>com_10259_5086</setSpec><setSpec>com_10259_2604</setSpec><setSpec>col_10259.4_2558</setSpec></header><metadata><oai_dc:dc xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:doc="http://www.lyncode.com/xoai" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:dc="http://purl.org/dc/elements/1.1/" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:title>Vacuum Energy for Generalized Dirac Combs at T = 0</dc:title>
<dc:creator>Bordag, Michael</dc:creator>
<dc:creator>Muñoz Castañeda, José María</dc:creator>
<dc:creator>Santamaría Sanz, Lucía</dc:creator>
<dc:subject>Quantum vacuum</dc:subject>
<dc:subject>Casimir effect (theory)</dc:subject>
<dc:subject>Condensed matter</dc:subject>
<dc:subject>Quantum field theories (QFT)</dc:subject>
<dc:subject>Selfadjoint extensions</dc:subject>
<dc:subject>Física</dc:subject>
<dc:subject>Matemáticas</dc:subject>
<dc:subject>Physics</dc:subject>
<dc:subject>Mathematics</dc:subject>
<dc:description>The quantum vacuum energy for a hybrid comb of Dirac δ-δ′ potentials is computed by using the energy of the single δ-δ′ potential over the real line that makes up the comb. The zeta function of a comb periodic potential is the continuous sum of zeta functions over the dual primitive cell of Bloch quasi-momenta. The result obtained for the quantum vacuum energy is non-perturbative in the sense that the energy function is not analytical for small couplings.</dc:description>
<dc:description>The authors acknowledge support from the German Research Foundation (DFG) and Universität Leipzig within the program of Open Access Publishing. JMM-C and LS-S are grateful to the Spanish Government-MINECO (MTM2014-57129-C2-1-P) and the Junta de Castilla y León (BU229P18, VA137G18 and VA057U16) for the financial support.</dc:description>
<dc:date>2025-03-13T10:27:50Z</dc:date>
<dc:date>2025-03-13T10:27:50Z</dc:date>
<dc:date>2019-04</dc:date>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:identifier>http://hdl.handle.net/10259/10323</dc:identifier>
<dc:identifier>10.3389/fphy.2019.00038</dc:identifier>
<dc:identifier>2296-424X</dc:identifier>
<dc:language>eng</dc:language>
<dc:relation>Frontiers in Physics. 2019, V. 7, n. 38</dc:relation>
<dc:relation>https://doi.org/10.3389/fphy.2019.00038</dc:relation>
<dc:rights>Atribución 4.0 Internacional</dc:rights>
<dc:rights>http://creativecommons.org/licenses/by/4.0/</dc:rights>
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:format>application/pdf</dc:format>
<dc:publisher>Frontiers</dc:publisher>
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