nLab noncommutative torus (changes)

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Contents

Idea

A quotient of the torus, taken in the sense of noncommutative geometry.

Definition

As a Lie groupoid

The noncommutative torus with parameter θ∈U(1)\theta \in \mathrm{U}(1) away from roots of unity is the groupoid quotient of the circle group U(1)\mathrm{U}(1) by the action of the discrete group Z\mathbf{Z} of integers, where the element 1∈Z1 \in \mathbf{Z} acts by multiplication by θ\theta.

Here we can take θ=exp(2πiℏ)\theta = \exp(2\pi i \hbar), for ℏ\hbar an irrational number (which, if we think of the non-commutative algebra here as arising from quantization, may be thought of as Planck's constant).

The following Lie groupoid is Morita equivalent to the above Lie groupoid:

take the groupoid quotient of U(1) 2\mathrm{U}(1)^2 (i.e., a torus) by the action of the Lie group R\mathbf{R} of real numbers such that

a⋅(u,v)=(uexp(2πia),vexp(2πiaℏ)) a \cdot (u,v) \;=\; \big( u \exp(2\pi i a), v \exp(2\pi i a \hbar) \big)

As an algebra

Taking the groupoid algebra of the Lie groupoid constructed above, we obtain a noncommutative space in the sense of Connes noncommutative geometry.

For instance, in the realm of C*-algebras we get the C*-algebra generated by two unitary operators UU and VV subject to the relation

UV=θVU.U V=\theta V U.

Classification

The following classification is due to Rieffel 81.

If θ\theta is a root of unity, then the resulting Lie groupoid is Morita equivalent to the smooth manifold U(1)\mathrm{U}(1), i.e., the circle.

Otherwise, the noncommutative torus with parameter θ\theta is not Morita equivalent to the circle (or any smooth manifold). Furthermore, two noncommutative tori with paremeters θ 1\theta_1 and θ 2\theta_2 are Morita equivalent if and only if θ 1\theta_1 and θ 2\theta_2 are in the same orbit with respect to the action of GL(2,Z)\mathrm{GL}(2,\mathbf{Z}) on U(1)\mathrm{U}(1) defined as follows:

[a b c d]⋅exp(2πiα)≔exp(2πiaα+bcα+d). \left[ \array{ a & b \\ c & d } \right] \cdot \exp(2\pi i \alpha) \;\coloneqq\; \exp \left( 2\pi i \frac {a\alpha + b} {c\alpha + d} \right) \,.

References

Original articles:

  • Marc A. Rieffel , LC *C^\ast-algebras associated with irrational rotations , Pacific Journal of Mathematics 93:2 (1981), 415–429 (pdf93 , 2 (1981) 415–429 [[pdf](https://msp.org/pjm/1981/93-2/pjm-v93-n2-p12-s.pdf),doi:10.2140/pjm.1981.93.415, euclid:pjm/1102736269 ) ]

  • Marc A. Rieffel , :Albert SchwarzNon-Commutative Tori – A Case Study on Non-Commutative Differentiable Manifolds , in Morita Geometric equivalence and Topological Invariants of multidimensional Elliptic noncommutative Operators tori , Int. Contemporary J. Mathematics Math. 10 (1999) 289-299 (arXiv:math/9803057105 ) , AMS (1990) 191-211 [[doi:10.1090/conm/105](https://doi.org/10.1090/conm/105),pdf]

  • Marc Rieffel, Albert Schwarz: Morita equivalence of multidimensional noncommutative tori, Int. J. Math. 10 (1999) 289-299 [[arXiv:math/9803057](https://arxiv.org/abs/math/9803057)]

  • George A. Elliott and Hanfeng Li, Morita equivalence of smooth noncommutative tori, Acta Math. Volume 199, Number 1 (2007), 1-27 (euclid:acta/1485891908)

Review:

Non-commutative tori understood as strict deformation quantizations:

  • Marc A. Rieffel, Deformation quantization of Heisenberg manifolds, Communications in Mathematical Physics 122 (1989) 531–562 [[doi:10.1007/BF01256492](https://doi.org/10.1007/BF01256492)]

Last revised on January 1, 2025 at 18:42:09. See the history of this page for a list of all contributions to it.