<?xml version="1.0" encoding="UTF-8"?>
<collection>
<dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:invenio="http://invenio-software.org/elements/1.0" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd"><dc:identifier>doi:10.1103/PhysRevD.101.064062</dc:identifier><dc:language>eng</dc:language><dc:creator>Relancio, J.J.</dc:creator><dc:creator>Liberati, S.</dc:creator><dc:title>Phenomenological consequences of a geometry in the cotangent bundle</dc:title><dc:identifier>ART-2020-117883</dc:identifier><dc:description>A deformed relativistic kinematics can be understood within a geometrical framework through a maximally symmetric momentum space. However, when considering this kind of approach, usually one works in a flat spacetime and in a curved momentum space. In this paper, we will discuss a possible generalization to take into account both curvatures and some possible observable effects. We will first explain how to construct a metric in the cotangent bundle in order to have a curved spacetime with a nontrivial geometry in momentum space and the relationship with an action in phase space characterized by a deformed Casimir. Then, we will study within this proposal two different space-time geometries. In the Friedmann-Robertson-Walker universe, we will see the modifications in the geodesics (redshift, luminosity distance, and geodesic expansion) due to a momentum dependence of the metric in the cotangent bundle. Also, we will see that when the spacetime considered is a Schwarzschild black hole, one still has a common horizon for particles with different energies, differently from a Lorentz invariance violation case. However, the surface gravity computed as the peeling off of null geodesics is energy dependent.</dc:description><dc:date>2020</dc:date><dc:source>http://zaguan.unizar.es/record/89774</dc:source><dc:doi>10.1103/PhysRevD.101.064062</dc:doi><dc:identifier>http://zaguan.unizar.es/record/89774</dc:identifier><dc:identifier>oai:zaguan.unizar.es:89774</dc:identifier><dc:relation>info:eu-repo/grantAgreement/EUR/COST-Action/CA18108</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/DGIID-DGA/2015-E24-2</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MINECO-FEDER/PGC2018-095328-B-I00</dc:relation><dc:identifier.citation>Physical Review D 101, 6 (2020), 064062 1-15</dc:identifier.citation><dc:rights>All rights reserved</dc:rights><dc:rights>http://www.europeana.eu/rights/rr-f/</dc:rights><dc:rights>info:eu-repo/semantics/openAccess</dc:rights></dc:dc>

</collection>