Irrational rotation

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Template:Short description

Sturmian sequence generated by irrational rotation with theta=0.2882748715208621 and x=0.078943143

An irrational rotation in the mathematical theory of dynamical systems, is defined as a map f, as follows:

Let x∈[0,1) be arbitrary, and let θ be any irrational number. For i∈ Template:Math define[1] fθi:[0,1)→[0,1) by

fθi(x)=x+i⋅θ (mod 1)

Under the identification of a circle with Template:Math, or with the interval Template:Math with the boundary points glued together, this map becomes a rotation of a circle by a proportion Template:Math of a full revolution (i.e., an angle of Template:Math radians). Since Template:Math is irrational, the rotation has infinite order in the circle group, and the map Template:Math has no periodic orbits.

Alternatively, we can use multiplicative notation for an irrational rotation by introducing the map

fθ:S1→S1,fθ(x)=xe2πiθ

The relationship between the additive and multiplicative notations is the group isomorphism

φ:([0,1),+)→(S1,⋅)φ(x)=xe2πiθ.

It can be shown that Template:Math is an isometry.

There is a strong distinction in circle rotations that depends on whether Template:Math is rational or irrational. Rational rotations are less interesting examples of dynamical systems because if θ=ab and gcd⁡(a,b)=1, then fθb(x)=x when x∈[0,1). It can also be shown that fθi(x)≠x when 1≤i<b.

Significance

Irrational rotations form a fundamental example in the theory of dynamical systems. According to the Denjoy theorem, every orientation-preserving Template:Math-diffeomorphism of the circle with an irrational rotation number Template:Math is topologically conjugate to Template:Math. An irrational rotation is a measure-preserving ergodic transformation, but it is not mixing. The Poincaré map for the dynamical system associated with the Kronecker foliation on a torus with angle Template:Math is the irrational rotation by Template:Math. C*-algebras associated with irrational rotations, known as irrational rotation algebras, have been extensively studied.

Properties

Generalizations

  • Circle rotations are examples of group translations.
  • For a general orientation preserving homomorphism Template:Math of Template:Math to itself we call a homeomorphism F:ℝ→ℝ a lift of Template:Math if π∘F=f∘π where π(t)=tmod1.[2]
  • The circle rotation can be thought of as a subdivision of a circle into two parts, which are then exchanged with each other. A subdivision into more than two parts, which are then permuted with one-another, is called an interval exchange transformation.
  • Rigid rotations of compact groups effectively behave like circle rotations; the invariant measure is the Haar measure.

Applications

  • Skew Products over Rotations of the Circle: In 1969[3] William A. Veech constructed examples of minimal and not uniquely ergodic dynamical systems as follows: "Take two copies of the unit circle and mark off segment Template:Math of length Template:Math in the counterclockwise direction on each one with endpoint at 0. Now take Template:Math irrational and consider the following dynamical system. Start with a point Template:Math, say in the first circle. Rotate counterclockwise by Template:Math until the first time the orbit lands in Template:Math; then switch to the corresponding point in the second circle, rotate by Template:Math until the first time the point lands in Template:Math; switch back to the first circle and so forth. Veech showed that if Template:Math is irrational, then there exists irrational Template:Math for which this system is minimal and the Lebesgue measure is not uniquely ergodic."[4]

See also

References

Further reading