text: Noncommutative torus - Wikipedia
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  In mathematics, and more specifically in the theory of C*-algebras, the noncommutative tori Aθ, also known as irrational rotation algebras for irrational values of θ, 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.
  4 Classification and K-theory
  For any real number θ, the noncommutative torus Aθ is the C*-subalgebra of B(L2(S1)), the algebra of bounded linear operators of square-integrable functions on the unit circle S1 of C, generated by the unitary elements U and V, where U(f)(z)=zf(z) and V(f)(z)=f(e−2π iθz). A quick calculation shows that VU = e−2πiθUV.[1]
  Universal property: Aθ can be defined (up to isomorphism) as the universal C*-algebra generated by two unitary elements U and V satisfying the relation VU = e2πiθUV.[1] This definition extends to the case when θ is rational. In particular when θ = 0, Aθ is isomorphic to continuous functions on the 2-torus by the Gelfand transform.
  Irrational rotation algebra: Let the infinite cyclic group Z act on the circle S1 by the rotation action by angle 2πiθ. This induces an action of Z by automorphisms on the algebra of continuous functions C(S1). The resulting C*-crossed product C(S1) ⋊ Z is isomorphic to Aθ. The generating unitaries are the generator of the group Z and the identity function on the circle z : S1 → C.[1]
  Twisted group algebra: The function σ : Z2 × Z2 → C; σ((m,n), (p,q)) = e2πinpθ is a group 2-cocycle on Z2, and the corresponding twisted group algebra C*(Z2; σ) is isomorphic to Aθ.
  Every irrational rotation algebra Aθ is simple, that is, it does not contain any proper closed two-sided ideals other than { 0 } {\displaystyle \{0\}}
  and itself.[1]
  Every irrational rotation algebra has a unique tracial state.[1]
  The irrational rotation algebras are nuclear.
  Classification and K-theoryEdit
  The K-theory of Aθ is Z2 in both even dimension and odd dimension, and so does not distinguish the irrational rotation algebras. But as an ordered group, K0 ≃ Z + θZ. Therefore, two noncommutative tori Aθ and Aη are isomorphic if and only if either θ + η or θ − η is an integer.[1][2]
  Two irrational rotation algebras Aθ and Aη are strongly Morita equivalent if and only if θ and η are in the same orbit of the action of SL(2, Z) on R by fractional linear transformations. In particular, the noncommutative tori with θ rational are Morita equivalent to the classical torus. On the other hand, the noncommutative tori with θ irrational are simple C*-algebras.[2]
  ^ a b c d e f Davidson, Kenneth (1997). C*-Algebras by Example. Fields Institute. pp. 166, 218–219, 234. ISBN 0-8218-0599-1.
  ^ a b Rieffel, Marc A. (1981). "C*-Algebras Associated with Irrational Rotations" (PDF). Pacific Journal of Mathematics. 93 (2): 415–429 [416]. doi:10.2140/pjm.1981.93.415. Retrieved 28 February 2013.