$\dfrac{d}{dx}$ is what analysts would call an operator, meaning that you give it an element of a certain vector space and it gives you another element in that vector space. So then what is a vector space? Well a vector space is any collection of objects that satisfy certain axioms (like you can add two of of these objects together to get another object in the collection, you can multiply an object with a number to get another object in the collection, every object has a negative, etc). Vector spaces are in some way a generalization of the real numbers.
With that out of the way, how does this relate to $\dfrac{d}{dx}$? Well, you can look at $\dfrac{d}{dx}f$ for some function $f$. This is nothing more than the derivative of $f$. Particularly, there is a very nice vector space of functions called the "smooth" functions. These functions are infinitely differentiable and every derivative is continuous (though this is a bit redundant to say). Examples of such functions are polynomials (but these are not all of the smooth functions). Another would be $\arctan(x)$. If you differentiate a smooth function, you get another smooth function! So then if we denote the smooth functions by the symbol $C^{\infty}(\mathbb{R})$, we have that $\dfrac{d}{dx}:C^{\infty}(\mathbb{R})\rightarrow C^{\infty}(\mathbb{R})$.