Abstract
The essence of the noncommutative geometry consists in reformulating the geometry in terms of commutative algebras and modules of smooth functions, and then generalizing them to their noncommutative analogs, [1]. Here we shall describe models on a Fuzzy cylinder R S 1={τ on real line interpreted as the time, x ±=ρe ±iϕ identified with the circle S1}, for details see [2], [3].
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References
A. Connes, Geometrie Noncommutative (Inter Editions, Paris 1990).
H. Grosse and P. Prešnajder, Acta Phys. Slovaca 49 (1999) 185.
M. Chaichian, A. Demichev and P. Prešnajder, Quantum field theory on non-commutative space-times and the persistence of ultraviolet divergences, hepth/981280.
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© 2000 Springer-Verlag Berlin Heidelberg
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Pavšič, M., Chaichian, M., Demichev, A., Grosse, H., Prešnajder, P. (2000). Fields on Noncommutative Manifolds. In: Gausterer, H., Pittner, L., Grosse, H. (eds) Geometry and Quantum Physics. Lecture Notes in Physics, vol 543. Springer, Berlin, Heidelberg. https://doi.org/10.1007/3-540-46552-9_21
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DOI: https://doi.org/10.1007/3-540-46552-9_21
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