For sufficiency, note that the rays generate the stipulated sigma-algebra: , and , with integer . The familyis a sigma-algebra because inverse images preserve complements and countable unions. If it contains all upper rays, it contains their generated Borel sigma-algebra. Therefore upper-ray preimages suffice to prove Borel measurability.
Every open interval is Borel, since , omitting empty pieces. Open subsets of the line are countable unions of open intervals and hence Borel. Conversely, each half-open interval is obtained from open sets by sigma-algebra operations, so this is the usual Borel sigma-algebra.
A continuous function has open, and therefore Borel, inverse images of open sets. Since open sets generate the target Borel sigma-algebra, it is a Borel measurable function. A discontinuous example is , whose only level sets are built from the Borel half-lines; it jumps at zero.
For a lower semicontinuous function, each upper-ray inverse image is open, hence Borel, so part (a)(i) applies directly. For an upper semicontinuous , the function is lower semicontinuous becauseis open. Negation is continuous and Borel measurable, so is Borel measurable too. Thus both semicontinuity classes are Borel measurable.
Boundedness of makes finite and nonnegative. Suppose . By its infimum definition, some satisfies . If , thenThe supremum over the smaller interval cannot exceed that over the larger one. HenceThus is open for every , proving is upper semicontinuous. Measurability of the original was never needed: these are purely pointwise oscillation bounds.
If is continuous at , choose a small interval on which . The triangle inequality makes its oscillation less than , so .
Conversely, if , then for every some has . As itself belongs to the interval used in that supremum, for . Thus is continuous at .
The continuity set of a function is thereforeEach set in the intersection is open by part (i), so this is a G-delta set and in particular a Borel set, even if itself is not measurable.
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