If T is an area preserving homeomorphism of the two dimensional torus, it can be approximated uniformly by permutations of
squares
of size 1/m. The orbit of the map
is a permutation
of the squares. For example, if
then
is a permutation of the n squares which consists of m cycles. Let
be the left lower corner of a square
. Define the matrix valued map
and define
, we can look at the function $f(T,q) =tr(A(x_{\pi(n)}/m+q_n/m) \cdots A(x_{\pi(1)}/m+q_1/m)$. It is a trigonometric polynomial in the n variables
. What we see numerically is that for every permutation
or transformation T respectively, the maximum
is
. This is a bold linear algebra problem, discussed already last week.
I studied related problems for many years. In 1998/1999 I did not take the maximum but took and integrated over
. The maximum has the advantage that we see the estimate to hold for all n and not just for large enough n. We can reformulate the above problem as in the youtube presentation of today. It case
makes small
cases already work so that the uniform conjecture can be formulated. If we just take permutations of
intervals of length
partitioning
the uniform estimate does not hold for smaller n, but the proof suggestion below would get it done for large enough n and still imply the strong consequences we were talking about. To establish it then also for smaller n would require more technical effort (if the proof at all would go through).
One of the consequences of the bold linear algebra problem would be to show that the metric entropy of the standard map is larger or equal than
for any real
(by Pesin). An other consequence would be that every random Jacobi operator
has no absolutely continuous spectrum for almost every initial point
on the torus, if
is an ergodic area preserving homeomorphism (by Kotani). The reason is Lax theorem allowing to approximate an area preserving homeomorphism to be approximated by periodic permutations of cubes (squares) and then upper-semicontinuity of the integrated Lyapunov exponent as a function of
, noting that it is the liminf of continuous functions. I established in 1993 that the Lyapunov exponent is positive on a dense set of cocycles if the map
is aperiodic and fixed and that we in general have discontinuity. There are always cocycles A with positive exponents which can be approximated uniformly by cocycles with zero exponents.
Again, to repeat from last time, the bold linear algebra problem is much stronger than these consequences but making a problem stronger does in general not make it harder. It can make it easier as we can do not have to bother with a particular transformation but establish it for all transformations. Obviously as the function is the same when composing its permutation with a cyclic permutation (by the trace invariance), we only have to establish that if it holds for a permutation, then it holds also for a permutation in which the first two elements are flipped. The reason is that we can use cyclic conjugations to get any adjacent elements flipped and so can bubble sort the permutation. We need less
steps to do that. The flip of the first two elements is a special pancake flip but the entire difficulty is already there. If we flip the first two elements in a product of three matrices, a very large trace can become small. The elementary relation
illustrates this and it also gives immediately an idea how to solve the problem. If we have established the bold result for a specific transformation, we can modify the transformation by a flip of the first two elements if the matrix
which is the product of the last
matrices has the property that the side diagonals have different sign. Call g(T,q) the function which establishes with
that we can flip, we can now just use a gradient flow on the manifold M where
to get to
. This is possible in time which exponentially small in n if we can establish that the gradients of f,g are not parallel and large. The gradient flow is
, where
is the projection onto the tangent space of
in
.
If we are on , then the gradients of f and g involve matrix entries of
and
and so are exponentially large and also should not correlate too much. These are technical conditions to check, but if
has exponentially large length in
, then we need only exponentially small time to reach from a starting point the manifold
where we can safely apply the flip and keep the value
. Once we have flipped, the entire process starts again. We are again on
but the manifold now looks different. But again, we can move on
towards
with an exponentially small change of q. After less than
such steps we have reached any transformation for which we wanted to check the bold result.