Interval exchange transformation

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In mathematics, an interval exchange transformation is a kind of dynamical system that generalises the idea of a circle rotation. The phase space consists of the unit interval, and the transformation acts by cutting the interval into several subintervals, and then permuting these subintervals.

Formal definition

Let   and let   be a permutation on  . Consider a vector

 

of positive real numbers (the widths of the subintervals), satisfying

 

Define a map

 

called the interval exchange transformation associated to the pair   as follows. For

 

let

  and let
 

Then for  , define

 


if   lies in the subinterval  . Thus   acts on each subinterval of the form   by an orientation-preserving isometry, and it rearranges these subintervals so that the subinterval at position   is moved to position  .

Properties

Any interval exchange transformation   is a bijection of   to itself which preserves Lebesgue measure. It is not usually continuous at each point   (but this depends on the permutation  ).

The inverse of the interval exchange transformation   is again an interval exchange transformation. In fact, it is the transformation   where   for all  .

If   and   (in cycle notation), and if we join up the ends of the interval to make a circle, then   is just a circle rotation. The Weyl equidistribution theorem then asserts that if the length   is irrational, then   is uniquely ergodic. Roughly speaking, this means that the orbits of points of   are uniformly evenly distributed. On the other hand, if   is rational then each point of the interval is periodic, and the period is the denominator of   (written in lowest terms).

If  , and provided   satisfies certain non-degeneracy conditions, a deep theorem due independently to W.Veech and to H.Masur asserts that for almost all choices of   in the unit simplex   the interval exchange transformation   is again uniquely ergodic. However, for   there also exist choices of   so that   is ergodic but not uniquely ergodic. Even in these cases, the number of ergodic invariant measures of   is finite, and is at most  .