Essentially all approaches to Furstenburg's Conjecture and related problems have so far been the same, namely the use of isometric directions for the action, where the action acts as a translation on a certain foliation, and invoking the observation that the only translation-invariant measures are Lebesgue on this foliation. The positive entropy assumption is then used to show that this forces the measure itself to be Lebesgue.
For example, if and
are integers such that
is close to
, then
is
nearly an isometry on the circle, or more accurately on the
-adic solenoid since we must invert one of the two maps. This
solenoid has a copy of the reals wrapping densely through it, and
the conditional measures on nearby pieces of leaves induced by an
invariant measure must have the property that under iterates in
the isometric direction they are nearly translation-invariant.
This is the key idea in Rudolph's proof.
The existence of isometric directions for certain
-actions is a special case of a very general
phenomenon called ``subdynamics'', or the study of such actions
along subgroups of
, or more generally along
subspaces of
, introduced by Boyle and Lind
[
MR 97d:58115]. Every topological
-action on an
infinite compact space has a non-empty set of lower-dimension
subspaces, closed in the Grassmann topology, along which the
action is nonexpansive. Dynamical properties within a connected
component of the complement of this set vary nicely or are
constant, while passing from one component to another typically
results in abrupt changes, roughly analogous to a phase
transition. It is these nonexpansive directions that have been the
key to all attempts so far to prove Furstenburg's Conjecture.
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