For a sample space Ω, let A be a set of subsets of Ω. Suppose we want to generate a σ-field using A. Note that there may be many different σ-fields F such that A⊆F. Hence, to make this generation unique, we will focus on the smallest such F.
Denoted by B, the Borel σ-field is defined on the sample space Ω=(0,1]. It is the σ-field generated by B0={finite unions of disjoint subintervals of Ω} (recall that we saw this set earlier as a counterexample for σ-fields). Note that one can define the Borel σ-field on R in the same way as we did for Ω.
It is well known that B can also be generated by open, closed, and half-open sets. Formally, let
Q={(a,b]⊆Ω}
R={(a,b)⊆Ω}
S={[a,b]⊆Ω}
T={[a,b)⊆Ω}
The notation above may feel a little weird, but essentially it says that Q is the set of all intervals of Ω that are open on the left and closed on the right (similarly for the other three sets).