There is no infinite-dimensional Lebesgue measure

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In mathematics, it is a theorem that there is no analogue of Lebesgue measure on an infinite-dimensional space. This fact forces mathematicians studying measure theory on infinite dimensional spaces to use other kinds of measures: often, the abstract Wiener space construction is used.

[edit] Motivation

It can be shown that Lebesgue measure λn on Euclidean space Rn is locally finite, strictly positive and translation-invariant. Explicitly:

  • every point x in Rn has an open neighbourhood Nx with finite measure λn(Nx) < +∞;
  • every non-empty open subset U of Rn has positive measure λn(U) > 0;
  • if A is any Lebesgue measurable subset of Rn, Th : RnRn, Th(x) = x + h, denotes the translation map, and (Th)(λn) denotes the push forward, then (Th)(λn)(A) = λn(A).

Geometrically speaking, these three properties make Lebesgue measure very nice to work with. When we consider an infinite dimensional space such as an Lp space or the space of continuous paths in Euclidean space, it would be nice to have a similarly nice measure to work with. Unfortunately, this is not possible.

[edit] Statement of the theorem

Suppose that H is a Hilbert space with dim(H) = +∞. Then the only locally finite and translation-invariant measure on H is the trivial measure μ, with μ(A) = 0 for every measurable set A.

(Many authors assume that H is separable. This assumption simplifies the proof considerably, since it provides a countable basis for H. However, the result holds even without the separability assumption.)

[edit] Proof of the theorem

Let H be an infinite-dimensional separable Hilbert space and suppose μ is a translation-invariant, locally finite measure on H with μ(H) > 0 (so μ is not the trivial measure). For any point x in H and any real r > 0, the notation B(x,r) denotes the open ball around x of radius r.

The first step is to show that for every positive r and every x in H, μ(B(x,r)) > 0. Suppose not, and fix x and r with μ(B(x,r)) = 0. Then, because μ is translation-invariant, μ(B(y,r)) = 0 for every point y in H. Now

H = \bigcup_{y \in H} B(y,r),

and so, because H is separable, there is a sequence (yi)iN of points of H such that

H = \bigcup_{i \in \mathbb{N}} B(y_i,r).

Thus,

\mu (H) \leq \sum_{i \in \mathbb{N}} \mu(B(y_i,r)) = 0,

contradicting the assumption that μ(H) > 0. This proves the first step.

Since μ is locally finite, there is an open set U of finite measure. Since μ is assumed to be translation-invariant, we may assume that U contains the 0 element of H. Thus, there is some positive real number r0 such that μ(B(0,r0)) is finite. Thus, in light of the first step, for any positive r < r0 and any point x in H, 0 < μ(B(x,r)) < +∞.

Let (ei)iN be a countable, orthonormal basis for H. Then, by the triangle inequality, for each ei,

B \left(\frac{r_0}{2} e_i, \frac{r_0}{4} \right) \subseteq B(\mathbf{0}, r_0).

Now, Pythagoras' theorem holds in any Hilbert space, and thus

d \left(\frac{r_0}{2} e_i ,\frac{r_0}{2} e_j \right) = \frac{r_0\sqrt{2}}{2}

for all distinct i and j. Because

\frac{r_0\sqrt{2}}{2} > 2 \frac{r_0}{4},

the balls B(r0ei/2, r0/4) and B(r0ej/2, r0/4) must be disjoint for all distinct i and j. Thus

\mu (B(\mathbf{0}, r_0)) \geq \sum_{i \in \mathbb{N}} \mu \left( B \left( \frac{r_0}{2}e_i, \frac{r_0}{4} \right) \right).

Because μ(B(r0ei/2, r0/4)) has the same nonzero value independent of i, the right-hand side of this inequality is +∞, and so μ(B(0, r0)) is infinite, contradicting the choice of r0.