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Noncommutative torus

In mathematics, and more specifically in the theory of C*-algebras, the noncommutative tori A<sub>θ</sub>, 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.

Definition

For any irrational real number θ, 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>−2π i θ</sup>UV.

Alternative characterizations

  • Universal property: A<sub>θ</sub> can be defined (up to isomorphism) as the universal C*-algebra generated by two unitary elements U and V satisfying the relation VU&nbsp;=&nbsp;e<sup>2π i θ</sup>UV. This definition extends to the case when θ is rational. In particular when θ&nbsp;=&nbsp;0, A<sub>θ</sub> 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 S<sup>1</sup> by the rotation action by angle 2iθ. This induces an action of Z by automorphisms on the algebra of continuous functions C(S<sup>1</sup>). The resulting C*-crossed product C(S<sup>1</sup>) ⋊ Z is isomorphic to A<sub>θ</sub>. The generating unitaries are the generator of the group Z and the identity function on the circle z : S<sup>1</sup> → C.
  • Twisted group algebra: The function σ : Z<sup>2</sup> × Z<sup>2</sup> → C; σ((m,n), (p,q)) = e<sup>2πinpθ</sup> is a group 2-cocycle on Z<sup>2</sup>, and the corresponding twisted group algebra C*(Z<sup>2</sup>;&nbsp;σ) is isomorphic to A<sub>θ</sub>.

Properties

  • Every irrational rotation algebra A<sub>θ</sub> is simple, that is, it does not contain any proper closed two-sided ideals other than and itself.
  • Every irrational rotation algebra has a unique tracial state.
  • The irrational rotation algebras are nuclear.

Classification and K-theory

The K-theory of A<sub>θ</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> ≃ Z + θZ. Therefore, two noncommutative tori A<sub>θ</sub> and A<sub>η</sub> are isomorphic if and only if either θ&nbsp;+&nbsp;η or θ&nbsp;−&nbsp;η is an integer.

Two irrational rotation algebras A<sub>θ</sub> and A<sub>η</sub> are strongly Morita equivalent if and only if θ and η are in the same orbit of the action of SL(2,&nbsp;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.

References