I've attached extracts from two different books. The first two pages are from "Complex Variables and the Laplace Transform for Engineers", by Wilbur R. LePage (I highly recommend this book BTW). And, the third page is from "Calculus of Variations", by Robert Weinstock. I have other books that conform to this definition also, but this is the definition I've always seen and used.
To me the term "continuous" automatically includes our normal well behaved functions, but also includes functions with kinks (first derivative has jump discontinuities). However, it does not include jump discontinuities. This is the reason for the term "Piecewise Continuous". It allows a class of functions that are continuous in a finite number of regions, with jumps at the boundaries. This becomes important for evaluating Laplace transforms of many discontinuous function we deal with in EE and physics.
In the absence of a direct quote from PGs book, I would recommend using this usual definition because, to the best of my knowledge, it is the definition used by mathematicians generally.