In the book "Index Transforms" by S.B. Yakubovich (World Scientific, 1996), I encountered the notion of a "smooth function of the order two" with compact support on $\mathbb R\_+$, denoted $C^{(2)}(\mathbb R\_+)$, cf. [here](https://books.google.com/books?id=vODsCgAAQBAJ&pg=PA49&lpg=PA49&dq=yakubovich%20smooth%20function%20order%20two&source=bl&ots=_FzcfSznMP&sig=ACfU3U39t7-IFseD6_bmn-do0ITRRaZ_XQ&hl=de&sa=X&ved=2ahUKEwj15LfskaPmAhVC3qQKHbynAsAQ6AEwAHoECAYQAQ#v=onepage&q=yakubovich%20smooth%20function%20order%20two&f=false) (I hope the link works). 


What does that mean? 


At first I thought it refers to the space of functions with continuous first and second derivative, but then it is the term "smooth" which puzzles me in this context. So maybe it means something different. 


Annoyingly, the notation is not explained in the book, and it also is not obvious for me from the context. Yakubovich cites the result that $C^{(2)}(\mathbb R\_+)$ is dense in $L\_{1,2}(\mathbb R\_+):=L^2 (\mathbb R\_+, x\, dx)$ and refers to the book of Titchmarsh, "Introduction to the Theory of Fourier Integrals" (1937), but I could not find the result in there. So maybe someone of you knows more about this. Thank you in advance!



Notion of a "smooth function of the order two" (Yakubovich, "Index Transforms")
The symbols $C^k$, with $k=0,\dots,\infty$ are today universally acknowledged and can be used with no need of other specification; yet sometimes (and more often $20$ years ago) for the sake of clarity, or style, one would still insert them in expressions like *regular/regularity* or *smooth/smoothness of order/class $C^k$* and equivalently *smooth/smoothness*, using *smooth/smoothness* as a generic term. Note that this author has *infinitely smooth* at page $72$. In conclusion, I would bet for $C^2$.


PS: I remember seminars where the lecturer would state hypotheses like "Let $\Omega$ be a bounded open set with smooth boundary...", and as soon as somebody asked "What order of smoothness" the answer was "Smooth enough for the needed Sobolev theorems to hold true", followed by a not convinced, respectful silence of the audience. "OK, let's say infinitely smooth". Maybe this is the origin of the meaning of *smooth* as $C^\infty$?


