The aim of this answer is to make the question self-contained, and propose a generalization of
the answer by Sangchul Lee.
The basic formula to be employed is (anticipating with $y$ instead of $x$ and $g$ instead of $f$):
$$
e^{\lambda\frac{d}{dy}}\,g(y) = g(y+\lambda)
$$
Which is easily proved with Taylor series expansions for differential operators and functions:
$$
e^{\lambda\frac{d}{dy}}\,g(y) = \sum_{k=0}^\infty \frac{1}{k!}\left(\lambda\,\frac{d}{dy}\right)^k g(y) =
\sum_{k=0}^\infty \frac{g^{(k)}(y)}{k!}\lambda^k = g(y+\lambda)
$$
Generalization. Substitute $y = \phi(x)$ , then:
$$
\frac{d}{dy} = \frac{d}{d\phi(x)} = \frac{dx}{d\phi(x)}\frac{d}{dx} =
\frac{1}{\phi'(x)}\frac{d}{dx}
$$
Also notice that $g(y) = g(\phi(x)) = f(x) = f(\phi^{-1}(y))$. Thus:
$$
e^{\lambda\frac{d}{dy}}\,g(y) = e^{\frac{\lambda}{\phi'(x)}\frac{d}{dx}} f(x) =
g(y+\lambda) = f(\phi^{-1}(\phi(x)+\lambda))
$$
Third formula in the question as a specialization of the above generalization:
$$
1/\phi'(x) = x^3 \quad \Longrightarrow \quad \phi(x) = \int \frac{dx}{x^3} = \frac{-1}{2x^2} = y
\quad \Longrightarrow \quad x = \sqrt{\frac{-1}{2y}} \quad \Longrightarrow \\ \phi^{-1}(x) = \sqrt{\frac{-1}{2x}}
\quad \Longrightarrow \quad \phi^{-1}(\phi(x)+\lambda) = \sqrt{\frac{-1}{2(-1/(2x^2)+\lambda)}} =
\frac{x}{\sqrt{1-2\lambda x^2}}
$$
Hence it follows that:
$$
e^{\lambda\,x^3\,\frac{d}{dx}}\,f(x) = f\left(\frac{x}{\sqrt{1-2\lambda\,x^2}}\right)
$$
But, with the general formula, another old puzzle is now solved completely !
Let $g$ be an arbitrary (real-valued, neat) function. Consider a Lie series as in
Exponential of a function times derivative :
$$
e^{g(x)\partial}f(x) \qquad \mbox{with} \quad \partial = \frac{d}{dx}
$$
First solve the differential equation:
$$
g(x) = \frac{1}{\phi'(x)} \quad \Longrightarrow \quad \phi(x) = \int \frac{dx}{g(x)}
$$
Then we have:
$$
\boxed{ e^{g(x)\partial} f(x) = f(\phi^{-1}(\phi(x)+1)) }
$$