Twisted Covariance vs Weyl Quantisation

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dc.contributor.areaMathematicsen_US
dc.contributor.authorPiacitelli, Gherardoen_US
dc.contributor.departmentMathematical Physicsen_US
dc.date.accessioned2009-01-22T12:32:39Zen_US
dc.date.accessioned2011-09-07T20:21:21Z
dc.date.available2009-01-22T12:32:39Zen_US
dc.date.available2011-09-07T20:21:21Z
dc.date.issued2009-01-22T12:32:39Zen_US
dc.description.abstractIn this letter we wish to clarify in which sense the tensor nature of the commutation relations [x^mu,x^nu]=i theta ^{mu nu} underlying Minkowski spacetime quantisation cannot be suppressed even in the twisted approach to Lorentz covariance. We then address the vexata quaestio "why theta"?en_US
dc.format.extent135129 bytesen_US
dc.format.mimetypeapplication/pdfen_US
dc.identifier.urihttps://openscience.sissa.it/handle/1963/3451en_US
dc.language.isoen_USen_US
dc.relation.ispartofseriesSISSA;13/2009/FMen_US
dc.relation.ispartofseriesarXiv.org;0901.3109v1en_US
dc.titleTwisted Covariance vs Weyl Quantisationen_US
dc.typePreprinten_US
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