<?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>2026-04-14T03:35:20Z</responseDate><request verb="GetRecord" identifier="oai:www.recercat.cat:2445/12336" metadataPrefix="oai_dc">https://recercat.cat/oai/request</request><GetRecord><record><header><identifier>oai:recercat.cat:2445/12336</identifier><datestamp>2025-12-04T20:46:28Z</datestamp><setSpec>com_2072_1057</setSpec><setSpec>col_2072_478822</setSpec><setSpec>col_2072_478917</setSpec></header><metadata><oai_dc:dc xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
   <dc:title>Bubble fluctuations in Omega less than 1 inflation</dc:title>
   <dc:creator>Garriga Torres, Jaume</dc:creator>
   <dc:subject>Teoria de camps (Física)</dc:subject>
   <dc:subject>Ones gravitacionals</dc:subject>
   <dc:subject>Field theory (Physics)</dc:subject>
   <dc:subject>Gravitational waves</dc:subject>
   <dc:description>In the context of the open inflationary universe, we calculate the amplitude of quantum fluctuations which deform the bubble shape. These give rise to scalar field fluctuations in the open Friedmann-Robertson-Walker universe which is contained inside the bubble. One can transform to a new gauge in which matter looks perfectly smooth, and then the perturbations behave as tensor modes (gravitational waves of very long wave-length). For &#xd;
(&#xd;
1&#xd;
−&#xd;
Ω&#xd;
)&#xd;
≪&#xd;
1&#xd;
, where &#xd;
Ω&#xd;
 is the density parameter, the microwave temperature anisotropies produced by these modes are of order &#xd;
δ&#xd;
T&#xd;
T&#xd;
∼&#xd;
H&#xd;
(&#xd;
R&#xd;
0&#xd;
μ&#xd;
l&#xd;
)&#xd;
−&#xd;
1&#xd;
2&#xd;
(&#xd;
1&#xd;
−&#xd;
Ω&#xd;
)&#xd;
l&#xd;
2&#xd;
. Here, &#xd;
H&#xd;
 is the expansion rate during inflation, &#xd;
R&#xd;
0&#xd;
is the intrinsic radius of the bubble at the time of nucleation, &#xd;
μ&#xd;
 is the bubble wall tension, and &#xd;
l&#xd;
 labels the different multipoles (&#xd;
l&#xd;
>&#xd;
1&#xd;
). The gravitational back reaction of the bubble has been ignored. In this approximation, &#xd;
G&#xd;
μ&#xd;
R&#xd;
0&#xd;
≪&#xd;
1&#xd;
, and the new effect can be much larger than the one due to ordinary gravitational waves generated during inflation (unless, of course, &#xd;
Ω&#xd;
 gets too close to 1, in which case the new effect disappears).</dc:description>
   <dc:date>2010-05-06T08:53:49Z</dc:date>
   <dc:date>2010-05-06T08:53:49Z</dc:date>
   <dc:date>1996</dc:date>
   <dc:type>info:eu-repo/semantics/article</dc:type>
   <dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
   <dc:identifier>0556-2821</dc:identifier>
   <dc:identifier>https://hdl.handle.net/2445/12336</dc:identifier>
   <dc:identifier>507982</dc:identifier>
   <dc:language>eng</dc:language>
   <dc:relation>Reproducció digital del document publicat en format paper, proporcionada per PROLA i http://dx.doi.org/10.1103/PhysRevD.54.4764</dc:relation>
   <dc:relation>Physical Review D, 1996, vol. 54, núm. 8, p. 4764-4769</dc:relation>
   <dc:relation>http://dx.doi.org/10.1103/PhysRevD.54.4764</dc:relation>
   <dc:rights>(c) The American Physical Society, 1996</dc:rights>
   <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
   <dc:format>6 p.</dc:format>
   <dc:format>application/pdf</dc:format>
   <dc:publisher>The American Physical Society</dc:publisher>
   <dc:source>Articles publicats en revistes (Física de la Matèria Condensada)</dc:source>
</oai_dc:dc></metadata></record></GetRecord></OAI-PMH>