Aperiodic tiling of compact space by small number of basic tiles

Question

Suppose we have compact space, like sphere or torus in particular dimension $d$. Is it possible to construct aperiodic tiling in such setting? It seems obvious, answer is yes, because we may just divide its surface on finite number of basic shapes ( "curved polygons") but every one of those may be different than another. It is relatively easy I suppose.

Some of curved polygons above may be isomorphic tiles according to Euclidean group, translation and rotation, action in $d+1$ dimensional space, in which case we may say they have the same shape.

What is the smallest number of basic tiles of the same shape for which we may get aperiodic tilling? In particular: is it possible to construct aperiodic Penrose tiling on sphere? Torus? On cylinder?

If answers are known, could you take some references?

Edit: of course you may always use two different, "curved polygons" so probably question need some refactoring. Tiling I am asking should be defined as some kind of limit, where tiles are small in comparison to surface of the compact space of sphere or torus. So to make it nontrivial and mathematically interesting, more details are needed. From the other side, intuitive meaning here's clear. We want to exclude trivial cases of very few, very deformed polygons, and focus rather on very small tiles, building something like mesh rather than just dividing surface in finite number if shapes.

Answer 1

Not sure if this is what you are looking for, but some of the compact spaces you mentioned have a natural group operation. And you can talk abou aperiodic tilings in any LCA group.

For example the unit circle $U(1)\simeq \mathbb R/ \mathbb Z $ is a group. A tiling of this group is simply a partition in arcs.

Some of those partitions are periodic, for example pick the vertices of a regular $n$-gon, but if for example the arcs have pairwise distinct lenghts, the tiling is automatically periodic.

Same way, the torrus is a group, you can think about it as $U(1) \times U(1)$.

Note As you mention, you can also pick a group which acts on your space, and talk about periodicity/aperiodicity with respect to this action. This actually makes a lot of sense, since the set of periods of any tiling in $\mathbb R^d$ is just the stabilizer of the translation action of $\mathbb R^d$ on $\mathbb R^d$.

Thus, an element is periodic if and only if its stabilizer is non-trivial.

The advantage of the group action approach over the compact group is that in this case you can speak about "fully periodic elements".

But you have to also be careful. If your space is for example $U(1)$, the "natural" action to consider is the rotation by elements in $\mathbb R$, but then, since this action is not faithful, every element is automatically periodic. So you need make sure that your action is faithful.