Irrational rotation

In the mathematical theory of dynamical systems, an irrational rotation is a map
where Template:Math is an irrational number. 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
The relationship between the additive and multiplicative notations is the group isomorphism
- .
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 and , then when . It can also be shown that when .
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
- If Template:Math is irrational, then the orbit of any element of Template:Math under the rotation Template:Math is dense in Template:Math. Therefore, irrational rotations are topologically transitive.
- Irrational (and rational) rotations are not topologically mixing.
- Irrational rotations are uniquely ergodic, with the Lebesgue measure serving as the unique invariant probability measure.
- Suppose Template:Math. Since Template:Math is ergodic,
.
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 a lift of Template:Math if where .[1]
- 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[2] 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."[3]
See also
- Bernoulli map
- Modular arithmetic
- Siegel disc
- Toeplitz algebra
- Phase locking (circle map)
- Weyl sequence
References
Further reading
- C. E. Silva, Invitation to ergodic theory, Student Mathematical Library, vol 42, American Mathematical Society, 2008 Template:ISBN