There is a huge difference in the qualitative behavior of real and complex differentiable functions.
Real differentiable functions, even smooth (infinitely differentiable) functions, have very little that can be said about their global behavior: for any open $U \subset \mathbb{R}^n$ there is a smooth function $\mathbb{R}^n \to \mathbb{R}^m$ that is zero outside $U$, but nonzero inside. (A very useful tool in analysis, as it lets one construct partitions of unity.)
However, a holomorphic (complex differentiable) function is necessarily analytic, i.e. locally determined by its own Taylor series. This has big implications: it is uniquely determined by its behavior near a single point (assuming the domain is connected). We also get results such as:
- Liouville's theorem states that there are no bounded holomorphic functions $\mathbb{C} \to \mathbb{C}$ except for constant functions.
- The Schwarz lemma says that any holomorphic function $f \colon D \to \overline{D}$ on the unit disc $D = \{ z : |z| < 1 \}$ with $f(0) = 0$ must have $|f'(0)| \le 1$ and $|f(z)| \le |z|$ for all $z$, and if $|f'(0)| = 1$ or $|f(z)| = |z|$ for some $z$ then $f$ is linear.
- The Riemann mapping theorem tells us that for any simply connected domains $U,U' \subset \mathbb{C}$ which are not all of $\mathbb{C}$, there is a biholomorphic map $f \colon U \to U'$ (i.e. a holomorphic bijection whose inverse is holomorphic). Moreover, by the Schwarz lemma it is unique if $f(z_0)$ and $\arg f'(z_0)$ are prescribed for some $z_0 \in U$.
Much of this can be seen as a consequence of the fact that because of the Cauchy-Riemann equations, the real and imaginary parts of a holomorphic function are harmonic (i.e. satisfy Laplace's equation $\nabla^2 u = 0$); harmonic functions similarly enjoy a lot of rigidity results.