In plain words
Round a closed loop a well-behaved function integrates to zero, provided the region inside has no holes. The single exception, round the origin, is where all the content lives.
Statements
- Cauchy–Goursat: f holomorphic on a simply connected for every closed in .
- Integral formula: dz for winding once around .
- Derivatives: f⁽⁾ dz.
Why simple connectedness matters
dz although 1/z is holomorphic on ∖{0} — the domain is not simply connected. This single integral is the seed of all residue theory.
Choosing the tool
| Integrand inside | Method |
|---|---|
| no singularity | Cauchy's theorem: 0 |
| one simple pole | integral formula |
| a pole of order n | derivative formula |
| several poles | residue theorem |
| essential singularity | Laurent coefficient a₋ |
Worked patterns
dz — residues at ±i are 1/(2i) and −1/(2i), which cancel. (Zero without Cauchy's theorem applying!) eᶻ/zᵏ dz ! for k ≥ 1, and 0 for k ≤ 0. dz if n = −1, else 0 — the only integral you really need.
Consequences
- Mean value property: is the average of f over any circle centred at .
- Maximum modulus: a non-constant holomorphic function on a domain has no interior maximum of |f|; on a bounded domain the max of |f| is attained on the boundary.
- Minimum modulus: same for |f| minimum provided f has no zeros.
- Schwarz lemma: f : 𝔻 → 𝔻 holomorphic with f(0) = 0 ⇒ |f(z)| ≤ |z| and |f′(0)| ≤ 1, with equality only for a rotation.
Key takeaways
dz is the whole story; everything else is bookkeeping.
- Vanishing of an integral does not mean the theorem applies — residues can just cancel.
- Maximum modulus pushes extrema to the boundary; that is how "bounded on the boundary" arguments work.