nLab invariant set

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Limits and colimits

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Monoid theory

Measure and probability theory

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Idea

An invariant set is a subset which is invariant under a given action of a group or a monoid.

Definition

Let XX be a set, let MM be a monoid (or a group), and consider an action of MM on XX. (For each mMm\in M, denote the resulting action on XX again by m:XXm:X\to X.)

A subset SS of XX is called invariant if and only if for each mMm\in M, m 1(S)=Sm^{-1}(S)=S. Equivalently, if for every xXx\in X we have that xSx\in S if and only if m(x)Sm(x)\in S.

Note that the elements (“points”) of an invariant set need not themselves be fixed points: they might move under the action (but they remain in the set SS). For example, for rotations in the plane, any circle centered at the origin is an invariant set, but each point in each nontrivial circle is not a fixed point.

Variations of the definition

Since the original definition was given for the case of group actions, which are invertible, there are a number of variants of the same definition which differ for the case of arbitrary monoids. In particular, sometimes one calls a subset SXS\subseteq X invariant if and only if m 1(S)Sm^{-1}(S)\subseteq S, i.e. if for every xSx\in S, m(x)Sm(x)\in S as well. (Without requiring that if m(x)Sm(x)\in S, then xSx\in S.) In other words, it is a set “which we cannot leave” under the specified action. Sometimes such a set is called an absorbing set instead. (But that term may itself be used for other concepts, to make matters even worse.)

Also, in different categories than Set, similar variations of the notion of invariant set are given:

…and so on.

Examples

Invariant sigma-algebras

Let XX be a measurable set. Let MM be a monoid (or group), and consider an action of MM on XX via measurable functions m:XXm:X\to X.

A measurable subset AXA\subseteq X is called invariant if and only if for every mMm\in M, m 1(A)=Am^{-1}(A)=A.

Invariant sets form naturally a sigma-algebra, often called the invariant sigma-algebra.

The exchangeable sigma-algebra and the tail sigma-algebra? are examples of this. (Sometimes one uses the almost sure versions, see below.)

The invariant sigma-algebra gives a colimit of the action of MM in the category of Markov kernels (MP’23). More precisely, denote by X invX_inv the set XX together with the invariant sigma-algebra, and denote by q:XX invq:X\to X_inv the kernel induced by the set-theoretic identity. Then the (X inv,q)(X_inv,q) forms a universal cocone (i.e. colimit), meaning that for every kernel k:XYk:X\to Y satisfying km=kk\circ m=k, (i.e. right-invariant under the action of mm), there exists a unique kernel u:X invYu:X_inv\to Y making the following diagram commute, where δ m\delta_m is the kernel induced by mm. The kernel uu has the same entries as kk: by invariance, kk is indeed measurable for the sigma-algebra of invariant sets.

Note that X invX_inv is not the colimit simply in the category of measurable functions: the colimit in that case also takes a set-theoretic quotient. It is however a colimit also in the category of zero-one kernel.

In the category of kernels, the set-theoretic quotient and X invX_inv are isomorphic. This can be seen from the fact that Markov kernels are Kleisli morphisms of the Giry monad on Meas, and that left adjoints preserve colimits. The same can be said about zero-one kernels and the sobrification monad.

For stochastic actions

A monoid MM can also act stochastically on XX, via Markov kernels k m:XXk_m:X\to X such that for all xXx\in X and all measurable AXA\subseteq X,

k m(A|x)=1 A(x)={1 xA; 0 xA, k_m(A|x) \;=\; 1_A(x) \;=\; \begin{cases} 1 & x\in A ; \\ 0 & x\notin A , \end{cases}

and

k mn(A|x)= Xk m(A|x)k n(dx|x). k_{m\cdot n}(A|x) \;=\; \int_X k_m(A|x')\,k_n(d x'|x) .

(This is equivalently a functor BMStochB M\to Stoch, see the discussion at invariant measure.)

In this case, an invariant set is a measurable set AA such that for all mMm\in M and xXx\in X,

k(A|x)=1 A(x)={1 xA; 0 xA. k(A|x) \;=\; 1_A(x) \;=\; \begin{cases} 1 & x\in A ; \\ 0 & x\notin A . \end{cases}

These sets form again a sigma-algebra, generalizing the case of actions via functions.

This sigma-algebra is in general not a colimit in a category of kernels (EP’23, Example 3.9). See however the almost sure case below.

Almost surely invariant sets

For stationary actions, i.e. for actions of MM on a probability space (X,p)(X,p) via measure-preserving functions, (or equivalently, for measurable actions equipped with an invariant measure pp, we can define a notion of almost surely invariant set: a measurable subset AXA\subseteq X such that

p(Am 1(A))=p(m 1(A)A)=0. p(A\setminus m^{-1}(A)) \;=\; p(m^{-1}(A)\setminus A) \;=\; 0 .

Equivalently, if for all measurable SXS\subseteq X,

p(Sm 1(A))=p(SA). p(S\cap m^{-1}(A)) \;=\; p(S\cap A) .

More generally, if we have measure-preserving kernels k m:(X,p)(X,p)k_m:(X,p)\to(X,p), we call almost surely invariant a measurable subset AXA\subseteq X such that for all mMm\in M,

k m(A|x)=1 A(x)={1 xA; 0 xA k_m(A|x) \;=\; 1_A(x) \;=\; \begin{cases} 1 & x\in A ; \\ 0 & x\notin A \end{cases}

for pp-almost all xXx\in X. Equivalently, if for all measurable SXS\subseteq X,

Sk m(A|x)p(dx)=p(SA). \int_S k_m(A|x) \,p(d x) \;=\; p(S\cap A) .

These sets form again a sigma-algebra, called the almost surely invariant sigma-algebra (or sometimes, possibly confusingly, again invariant sigma-algebra).

Similarly to the deterministic case, this sigma-algebra is the colimit of the action of MM in the category of couplings (EP’23, Section 3.1).

Further properties

See also

References

category: probability

Last revised on July 13, 2024 at 20:11:49. See the history of this page for a list of all contributions to it.