2005
DOI: 10.1016/j.physletb.2005.07.011
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A dynamical 2-dimensional fuzzy space

Abstract: The noncommutative extension of a dynamical 2-dimensional space-time is given and some of its properties discussed. Wick rotation to euclidean signature yields a surface which has as commutative limit the doughnut but in a singular limit in which the radius of the hole tends to zero.

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Cited by 11 publications
(15 citation statements)
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“…The essential ingredients in the definition of the map are the Leibniz rules and the assumption (2.1) on the structure of the differential calculus. Although there have been found [16,17,4,6] numerous particular examples, there is not yet a systematic discussion of either the range or kernel of the map. We have here to a certain extent alleviated this, but only in the context of perturbation theory around a vacuum and even then, only in the case of a high-frequency wave.…”
Section: Recapitulationmentioning
confidence: 99%
“…The essential ingredients in the definition of the map are the Leibniz rules and the assumption (2.1) on the structure of the differential calculus. Although there have been found [16,17,4,6] numerous particular examples, there is not yet a systematic discussion of either the range or kernel of the map. We have here to a certain extent alleviated this, but only in the context of perturbation theory around a vacuum and even then, only in the case of a high-frequency wave.…”
Section: Recapitulationmentioning
confidence: 99%
“…We have here an indication of the importance of the calculi in the description of the geometries: the differential calculus usually introduced on a space described by the Heisenberg algebra is flat, while here the subspace (r, τ ) has a constant negative curvature, [12]. One can find even an example of an algebra over which there are two different calculi with geometries having as the commutative limit two different topologies.…”
Section: A Representationmentioning
confidence: 99%
“…So if we focus on point one, that is ∆q 1 → ǫ > 0 then the second point becomes fuzzier as time passes, that is ∆q 2 → ∞ . We can say that the background space is a dynamical two -dimensional fuzzy space (21). We will transform the problem of the non commuting two dimensional space, to a problem of two coupled harmonic oscillators in a more familiar two dimensional quantum mechanical space.…”
Section: The Two Dimensional Phase Spacementioning
confidence: 99%