No, that's not correct! The \delta distribution (not function!) is defined by how it is acting on a function in the sense of a linear functional, written as a formal integral,
\int_{\mathbb{R}} \mathrm{d} x \delta(x) f(x)=f(0),
where f is a function of an appropriate space of functions (e.g., the Schwartz space of quickly vanishing functions or the space of functions with compact support, etc.).
You can prove properties of the distribution by formally handling this kind of integral as if the \delta distribution were a usual function. E.g., you have
\int_{\mathbb{R}} \mathrm{d} x \delta(x-y) f(x) = \int_{\mathbb{R}} \mathrm{d} x' \delta(x') f(x'+y)=f(0+y)=f(y).
Now you can evaluate yourself, what \delta(x+y) must be and also prove the (correct) statement \delta(-x)=\delta(x).