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Let $G$ be the cumulative distribution function of the arbitrary Borel probability measure $\mu$. It may have atoms or flat intervals. Use its quantile functionThe limits of $G$ at the two infinities make $Q(u)$ finite. Its monotonicity and right continuity imply the exact equivalence $Q(u)\le x⟺u\le G(x)$. For the nontrivial direction, if $Q(u)\le x$, points with $G\ge u$ lie arbitrarily close above $Q(u)$; if the infimum itself is $x$, right continuity gives $G(x)\ge u$. The other direction follows directly from the defining infimum.

Take independent uniform variables $U_k$ and set $Y_k^{\prime }=Q(U_k)$. Thenso $(Y_k^{\prime })$ has the same entire sequence law as the original iid sample $(Y_k)$. On this construction, the empirical distribution function satisfiesThus part (ii) givesThe supremum is measurable: since both distribution functions are right-continuous, it equals the supremum over rational $x$. The convergence event consequently depends measurably on the coordinate sequence, and equality of the sequence laws transfers its probability one to $(Y_k)$. HenceThis is the Quantile proof of the Glivenko-Cantelli theorem, including arbitrary distributions with atoms. The original PDF supplies the full definition and absolute-value signs in this part, which the TeX conversion incompletely records.