Linear flow on the torus

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In mathematics, especially in the area of mathematical analysis known as dynamical systems theory, a linear flow on the torus is a flow on the n-dimensional torus 𝕋n=S1×S1××S1n which is represented by the following differential equations with respect to the standard angular coordinates (θ1,θ2,,θn): dθ1dt=ω1,dθ2dt=ω2,,dθndt=ωn.

The solution of these equations can explicitly be expressed as Φωt(θ1,θ2,,θn)=(θ1+ω1t,θ2+ω2t,,θn+ωnt)mod2π.

If we represent the torus as 𝕋𝕟=n/n we see that a starting point is moved by the flow in the direction ω=(ω1,ω2,,ωn) at constant speed and when it reaches the border of the unitary n-cube it jumps to the opposite face of the cube.

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Irrational rotation on a 2-torus

For a linear flow on the torus either all orbits are periodic or all orbits are dense on a subset of the n-torus which is a k-torus. When the components of ω are rationally independent all the orbits are dense on the whole space. This can be easily seen in the two dimensional case: if the two components of ω are rationally independent then the Poincaré section of the flow on an edge of the unit square is an irrational rotation on a circle and therefore its orbits are dense on the circle, as a consequence the orbits of the flow must be dense on the torus.

Irrational winding of a torus

In topology, an irrational winding of a torus is a continuous injection of a line into a two-dimensional torus that is used to set up several counterexamples.[1] A related notion is the Kronecker foliation of a torus, a foliation formed by the set of all translates of a given irrational winding.

Definition

One way of constructing a torus is as the quotient space 𝕋𝟚=2/2 of a two-dimensional real vector space by the additive subgroup of integer vectors, with the corresponding projection π:2𝕋𝟚. Each point in the torus has as its preimage one of the translates of the square lattice 2 in 2, and π factors through a map that takes any point in the plane to a point in the unit square [0,1)2 given by the fractional parts of the original point's Cartesian coordinates. Now consider a line in 2 given by the equation y=kx. If the slope k of the line is rational, then it can be represented by a fraction and a corresponding lattice point of 2. It can be shown that then the projection of this line is a simple closed curve on a torus. If, however, k is irrational, then it will not cross any lattice points except 0, which means that its projection on the torus will not be a closed curve, and the restriction of π on this line is injective. Moreover, it can be shown that the image of this restricted projection as a subspace, called the irrational winding of a torus, is dense in the torus.

Applications

Irrational windings of a torus may be used to set up counter-examples related to monomorphisms. An irrational winding is an immersed submanifold but not a regular submanifold of the torus, which shows that the image of a manifold under a continuous injection to another manifold is not necessarily a (regular) submanifold.[2] Irrational windings are also examples of the fact that the topology of the submanifold does not have to coincide with the subspace topology of the submanifold.[2]

Secondly, the torus can be considered as a Lie group U(1)×U(1), and the line can be considered as . Then it is easy to show that the image of the continuous and analytic group homomorphism x(eix,eikx) is not a regular submanifold for irrational k,[2][3] although it is an immersed submanifold, and therefore a Lie subgroup. It may also be used to show that if a subgroup H of the Lie group G is not closed, the quotient G/H does not need to be a manifold[4] and might even fail to be a Hausdorff space.

See also

Notes

^ a: As a topological subspace of the torus, the irrational winding is not a manifold at all, because it is not locally homeomorphic to .

References

  1. D. P. Zhelobenko (January 1973). Compact Lie groups and their representations. ISBN 9780821886649. https://books.google.com/books?id=ILhUYVmvHt0C&pg=PA45. 
  2. 2.0 2.1 2.2 Loring W. Tu (2010). An Introduction to Manifolds. Springer. pp. 168. ISBN 978-1-4419-7399-3. https://archive.org/details/introductiontoma00lwtu_506. 
  3. Čap, Andreas; Slovák, Jan (2009), Parabolic Geometries: Background and general theory, AMS, pp. 24, ISBN 978-0-8218-2681-2, https://books.google.com/books?id=G4Ot397nWsQC 
  4. Sharpe, R.W. (1997), Differential Geometry: Cartan's Generalization of Klein's Erlangen Program, Springer-Verlag, New York, pp. 146, ISBN 0-387-94732-9 

Bibliography

  • Katok, Anatole; Hasselblatt, Boris (1996). Introduction to the modern theory of dynamical systems. Cambridge. ISBN 0-521-57557-5.