In mathematics, and more specifically in the theory of C*-algebras, the noncommutative tori A<sub>ø</sub>, also known as irrational rotation algebras for irrational values of ø, form a family of noncommutative C*-algebras which generalize the algebra of continuous functions on the 2-torus. Many topological and geometric properties of the classical 2-torus have algebraic analogues for the noncommutative tori, and as such they are fundamental examples of a noncommutative space in the sense of Alain Connes.
For any irrational real number ø, the noncommutative torus is the C*-subalgebra of , the algebra of bounded linear operators on square-integrable functions on the unit circle , generated by two unitary operators defined as<blockquote></blockquote>A quick calculation shows that VU = e<sup>âÂÂ2ài ø</sup>UV.
The K-theory of A<sub>ø</sub> is Z<sup>2</sup> in both even dimension and odd dimension, and so does not distinguish the irrational rotation algebras. But as an ordered group, K<sub>0</sub> â Z + øZ. Therefore, two noncommutative tori A<sub>ø</sub> and A<sub>÷</sub> are isomorphic if and only if either ø + ÷ or ø â ÷ is an integer.
Two irrational rotation algebras A<sub>ø</sub> and A<sub>÷</sub> are strongly Morita equivalent if and only if ø and ÷ are in the same orbit of the action of SL(2, Z) on R by fractional linear transformations. In particular, the noncommutative tori with ø rational are Morita equivalent to the classical torus. On the other hand, the noncommutative tori with ø irrational are simple C*-algebras.