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Probability Measures Defined on Polish Spaces are Tight 📂Probability Theory

Probability Measures Defined on Polish Spaces are Tight

Theorem

Let’s say that a metric space (S,ρ)(S,\rho) is a Polish space. Then, all probability measures defined in SS are tight.

Explanation

A Polish space refers to a separable complete metric space. The reason we discuss the tightness of probability measures is precisely that, under these conditions, most probabilities are tight. This, conversely, implies the need to study probabilities defined in non-Polish spaces.

Proof

Strategy: We need to bring in several theorems from topology to follow the definition of tight probability measures.

Given that the space SS is both a metric space (S,ρ)( S , \rho) and a measurable space (S,B(S))(S,\mathcal{B}(S)) according to the definition of tight probability measures.

Let PP be a probability measure defined in SS. If there exists a compact set for all ε>0\varepsilon > 0 such that P(K)>1εP(K) > 1 - \varepsilon, then PP is considered tight.

Furthermore, when distance ρ\rho is given, an open ball centered at x0x_{0} with radius ε\varepsilon is represented as Bρ(x0;ε)B_{\rho} ( x_{0} ; \varepsilon ), and the closed ball as Bρ[x0;ε]B_{\rho} [ x_{0} ; \varepsilon].


Since SS is a separable space, a dense countable set D:={a1,a2,}D:= \left\{ a_{1}, a_{2}, \cdots \right\} of SS can be chosen. For all δ>0\delta > 0, k=1Bρ(ak;δ)=S\displaystyle \bigcup_{k=1}^{\infty} B_{\rho} \left( a_{k} ; \delta \right) = S holds, and by the continuity of measure, P(S)=limnP(k=1nBρ(ak;δ))\displaystyle P(S) = \lim_{n \to \infty} P \left( \bigcup_{k=1}^{n} B_{\rho} \left( a_{k} ; \delta \right) \right) follows. Now, if we set ε>0\varepsilon>0, for all mNm \in \mathbb{N} there exists nmn_{m} satisfying the following: P(k=1nmBρ(ak;1m))>P(S)2mε P \left( \bigcup_{k=1}^{n_{m}} B_{\rho} \left( a_{k} ; {{ 1 } \over { m }} \right) \right) > P(S) - 2^{-m}\varepsilon Let’s define KSK \subset S as follows: K:=m=1k=1nmBρ[ak;1m] K := \bigcap_{m=1}^{\infty} \bigcup_{k=1}^{n_{m}} B_{\rho} \left[ a_{k} ; {{ 1 } \over { m }} \right] KK is a set obtained by taking an infinite intersection of a finite union of closed balls, thus KK is a closed set in SS, and by selecting mm such that for all δ\delta, m>1/δm > 1 / \delta holds, Kk=1nmBρ[ak;1m]k=1nmBρ(ak;δ) K \subset \bigcup_{k=1}^{n_{m}} B_{\rho} \left[ a_{k} ; {{ 1 } \over { m }} \right] \subset \bigcup_{k=1}^{n_{m}} B_{\rho} \left( a_{k} ; \delta \right) Hence, KK is a totally bounded space.

Properties of Complete Metric Spaces: Since KK is a totally bounded space     \iff XX, the closed set KK is compact

Therefore, the closed set KK is compact, and according to the property of the probability measure PP, P(SK)=P(m=1(Sk=1nmBρ[ak;1m]))=m=1P(Sk=1nmBρ[ak;1m])=m=1[P(S)P(k=1nmBρ[ak;1m])]<m=12mε=ε \begin{align*} P(S \setminus K) =& P \left( \bigcup_{m=1}^{\infty} \left( S \setminus \bigcup_{k=1}^{n_{m}} B_{\rho} \left[ a_{k} ; {{ 1 } \over { m }} \right] \right) \right) \\ =& \sum_{m=1}^{\infty} P \left( S \setminus \bigcup_{k=1}^{n_{m}} B_{\rho} \left[ a_{k} ; {{ 1 } \over { m }} \right] \right) \\ =& \sum_{m=1}^{\infty} \left[ P \left( S \right) - P \left( \bigcup_{k=1}^{n_{m}} B_{\rho} \left[ a_{k} ; {{ 1 } \over { m }} \right] \right) \right] \\ <& \sum_{m=1}^{\infty} 2^{-m} \varepsilon \\ =& \varepsilon \end{align*}