Let $\mu$ be a non-atomic probability measure defined on $\mathbb R$. Let $I$ simply be an interval of length $\beta$, i.e., $ I = [i \beta,(i+1)\beta]$ for some $i \in \mathbb{Z}$, and $B$ any Borel set. I have the following fact given to me, which I was not able to refute yet and might well be correct:
$\mu(I \cap B) \rightarrow \mu(I) \dfrac{\mathrm{Len}(I \cap B)}{\mathrm{Len}(I)}$ as $\beta\downarrow 0$.
Here $\mathrm{Len}$ denotes the 1-D volume or the exterior measure.
This is a bit hard to imagine. The intuition (which may fail most of the times at measure theory) says that this is roughly dividing the probability assigned to interval $I$ by its length so that we have a 'unit/uniform' measure now. Then we assign this unit measure to the length of $I \cap B$ simply by multiplication. How can we prove this result, if this is true? If not, what are the minimum number of assumptions we need such that this is true?
I interpret your question as follows.
This claim is definitely false. One can take $\mu = \sum_{k=1}^\infty 2^{-k}\text{Unif}([2^{-2^k-1},2^{-2^k}])$, where $\text{Unif}(I)$ denotes the uniform probability measure over $I$, and $B = \cup_{k=1}^\infty [2^{-2^k-2},2^{-2^k}]$.