<?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>2026-04-22T20:18:21Z</responseDate><request verb="GetRecord" identifier="oai:riubu.ubu.es:10259/7222" metadataPrefix="marc">https://riubu.ubu.es/oai/request</request><GetRecord><record><header><identifier>oai:riubu.ubu.es:10259/7222</identifier><datestamp>2023-03-24T13:07:23Z</datestamp><setSpec>com_10259.4_2557</setSpec><setSpec>com_10259_5086</setSpec><setSpec>com_10259_2604</setSpec><setSpec>col_10259_7221</setSpec></header><metadata><record xmlns="http://www.loc.gov/MARC21/slim" xmlns:doc="http://www.lyncode.com/xoai" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:dcterms="http://purl.org/dc/terms/" xsi:schemaLocation="http://www.loc.gov/MARC21/slim http://www.loc.gov/standards/marcxml/schema/MARC21slim.xsd">
<leader>00925njm 22002777a 4500</leader>
<datafield tag="042" ind1=" " ind2=" ">
<subfield code="a">dc</subfield>
</datafield>
<datafield tag="720" ind1=" " ind2=" ">
<subfield code="a">Gubitosi, Giulia</subfield>
<subfield code="e">author</subfield>
</datafield>
<datafield tag="720" ind1=" " ind2=" ">
<subfield code="a">Ballesteros Castañeda, Ángel</subfield>
<subfield code="e">author</subfield>
</datafield>
<datafield tag="720" ind1=" " ind2=" ">
<subfield code="a">Herranz Zorrilla, Francisco José</subfield>
<subfield code="e">author</subfield>
</datafield>
<datafield tag="260" ind1=" " ind2=" ">
<subfield code="c">2020-08</subfield>
</datafield>
<datafield tag="520" ind1=" " ind2=" ">
<subfield code="a">Given a group of kinematical symmetry generators, one can construct a compatible noncommutative spacetime and deformed phase space by means of projective geometry. This was the main&#xd;
idea behind the very first model of noncommutative spacetime, proposed by H.S. Snyder in 1947.&#xd;
In this framework, spacetime coordinates are the translation generators over a manifold that is&#xd;
symmetric under the required generators, while momenta are projective coordinates on such a&#xd;
manifold. In these proceedings we review the construction of Euclidean and Lorentzian noncommutative Snyder spaces and investigate the freedom left by this construction in the choice of the&#xd;
physical momenta, because of different available choices of projective coordinates. In particular,&#xd;
we derive a quasi-canonical structure for both the Euclidean and Lorentzian Snyder noncommutative models such that their phase space algebra is diagonal although no longer quadratic.</subfield>
</datafield>
<datafield tag="024" ind2=" " ind1="8">
<subfield code="a">1824-8039</subfield>
</datafield>
<datafield tag="024" ind2=" " ind1="8">
<subfield code="a">http://hdl.handle.net/10259/7222</subfield>
</datafield>
<datafield tag="024" ind2=" " ind1="8">
<subfield code="a">10.22323/1.376.0190</subfield>
</datafield>
<datafield tag="245" ind1="0" ind2="0">
<subfield code="a">Generalized noncommutative Snyder spaces and projective geometry</subfield>
</datafield>
</record></metadata></record></GetRecord></OAI-PMH>