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Irrational rotation

From Wikipedia, the free encyclopedia
(Redirected fromIrrational angle)
Rotation of a circle by an angle of π times an irrational number
Sturmian sequence generated by irrational rotation with theta=0.2882748715208621 and x=0.078943143

In the mathematical theory ofdynamical systems, anirrational rotation is amap

Tθ:[0,1][0,1],Tθ(x)x+θmod1,{\displaystyle T_{\theta }:[0,1]\rightarrow [0,1],\quad T_{\theta }(x)\triangleq x+\theta \mod 1,}

whereθ is anirrational number. Under the identification of acircle withR/Z, or with the interval[0, 1] with the boundary points glued together, this map becomes arotation of acircle by a proportionθ of a full revolution (i.e., an angle of2πθ radians). Sinceθ is irrational, the rotation has infiniteorder in thecircle group and the mapTθ has noperiodic orbits.

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

Tθ:S1S1,Tθ(x)=xe2πiθ{\displaystyle T_{\theta }:S^{1}\to S^{1},\quad \quad \quad T_{\theta }(x)=xe^{2\pi i\theta }}

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

φ:([0,1],+)(S1,)φ(x)=xe2πiθ{\displaystyle \varphi :([0,1],+)\to (S^{1},\cdot )\quad \varphi (x)=xe^{2\pi i\theta }}.

It can be shown thatφ is anisometry.

There is a strong distinction in circle rotations that depends on whetherθ is rational or irrational. Rational rotations are less interesting examples of dynamical systems because ifθ=ab{\displaystyle \theta ={\frac {a}{b}}} andgcd(a,b)=1{\displaystyle \gcd(a,b)=1}, thenTθb(x)=x{\displaystyle T_{\theta }^{b}(x)=x} whenx[0,1]{\displaystyle x\in [0,1]}. It can also be shown thatTθi(x)x{\displaystyle T_{\theta }^{i}(x)\neq x} when1i<b{\displaystyle 1\leq i<b}.

Significance

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Irrational rotations form a fundamental example in the theory ofdynamical systems. According to theDenjoy theorem, every orientation-preservingC2-diffeomorphism of the circle with an irrationalrotation numberθ istopologically conjugate toTθ. An irrational rotation is ameasure-preservingergodic transformation, but it is notmixing. ThePoincaré map for the dynamical system associated with theKronecker foliation on atorus with angleθ> is the irrational rotation byθ.C*-algebras associated with irrational rotations, known asirrational rotation algebras, have been extensively studied.

Properties

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Generalizations

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Applications

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  • Skew Products over Rotations of the Circle: In 1969[2]William A. Veech constructed examples ofminimal and not uniquely ergodic dynamical systems as follows: "Take two copies of the unit circle and mark off segmentJ of length2πα in the counterclockwise direction on each one with endpoint at 0. Now takeθ irrational and consider the following dynamical system. Start with a pointp, say in the first circle. Rotate counterclockwise by2πθ until the first time the orbit lands inJ; then switch to the corresponding point in the second circle, rotate by2πθ until the first time the point lands inJ; switch back to the first circle and so forth. Veech showed that ifθ is irrational, then there exists irrationalα for which this system is minimal and theLebesgue measure is not uniquely ergodic."[3]

See also

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References

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  1. ^Fisher, Todd (2007)."Circle Homomorphisms"(PDF).
  2. ^Veech, William (August 1968)."A Kronecker-Weyl Theorem Modulo 2".Proceedings of the National Academy of Sciences.60 (4):1163–1164.Bibcode:1968PNAS...60.1163V.doi:10.1073/pnas.60.4.1163.PMC 224897.PMID 16591677.
  3. ^Masur, Howard;Tabachnikov, Serge (2002). "Rational Billiards and Flat Structures". In Hasselblatt, B.; Katok, A. (eds.).Handbook of Dynamical Systems(PDF). Vol. IA. Elsevier.

Further reading

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