Get AI summaries of any video or article — Sign up free
Complex Analysis 27 | Cauchy's Integral Formula [dark version] thumbnail

Complex Analysis 27 | Cauchy's Integral Formula [dark version]

5 min read

Based on The Bright Side of Mathematics's video on YouTube. If you like this content, support the original creators by watching, liking and subscribing to their content.

TL;DR

Cauchy’s integral formula reconstructs f(z) for any interior point z from the contour integral of f over the surrounding circle.

Briefing

Cauchy’s integral formula turns the “zero around closed curves” message of Cauchy’s theorem into a precise reconstruction rule: for a holomorphic function on a domain containing a disk, the value at any interior point is determined entirely by the function’s values on the surrounding circle. That matters because it sharply limits how much freedom holomorphic functions can have—knowing them on the boundary essentially pins them down everywhere inside.

The setup starts with a holomorphic function f on an open domain D. Choose a disk centered at 0 with radius r such that the closed disk lies inside D (so the circle never hits the boundary of the domain). Let γ be the positively oriented circle (the boundary of that disk). For any point z inside the disk, Cauchy’s integral formula gives an explicit expression for f(z) as a contour integral over γ:

f(z) = (1/(2πi)) ∮_γ f(ζ)/(ζ − z) dζ.

Equivalently, many texts write the same circle integral using ∂B_r instead of γ, and the formula relies on the fact that the winding number of γ around z is 1 (the contour goes once around the point).

The proof uses a standard trick: build an auxiliary function G that is holomorphic everywhere except at one chosen point. Here, the point of exception is not fixed at the disk’s center; it is the interior point z where the value f(z) is sought. The construction is:

G(ζ) = f(ζ)/(ζ − z).

Because f is holomorphic and the only singularity comes from the denominator, G is holomorphic on the punctured disk (holomorphic with one exception at ζ = z). The argument then compares integrals over two contours: a large circle around the origin and a smaller “keyhole” circle around the singularity at ζ = z. Since Cauchy’s theorem applies to holomorphic functions away from the exception, the contour integral can be reduced to the contribution coming from the small circle around ζ = z.

To compute that contribution, the proof splits the integrand by adding and subtracting f(z) in the numerator:

f(ζ)/(ζ − z) = (f(ζ) − f(z))/(ζ − z) + f(z)/(ζ − z).

The second term is straightforward: its integral equals 2πi times the constant f(z). The first term involves a difference quotient. As the small radius ε of the inner circle shrinks to 0, the difference quotient approaches f′(z), and the contour length shrinks proportionally to ε, forcing the integral of that first part to vanish in the limit. What remains is exactly the 2πi f(z) term, yielding the formula.

In short, the formula is strong not because it’s complicated, but because it’s rigid: holomorphic functions are fully controlled by their boundary values on circles contained in the domain. The next logical step—hinted at for later—is what this rigidity implies for analyticity and further properties of holomorphic functions.

Cornell Notes

Cauchy’s integral formula states that if f is holomorphic on a domain D containing a closed disk of radius r, then every interior value f(z) is determined by an integral of f over the boundary circle. For z inside the disk and γ the positively oriented circle |ζ| = r, the formula is f(z) = (1/(2πi)) ∮_γ f(ζ)/(ζ − z) dζ. The proof constructs an auxiliary function G(ζ) = f(ζ)/(ζ − z), which is holomorphic except at ζ = z. By comparing integrals over a large circle and a small circle around the singularity, and then splitting (f(ζ) − f(z))/(ζ − z) + f(z)/(ζ − z), the shrinking-circle estimate forces the difference-quotient part to vanish, leaving the constant term 2πi f(z).

Why does Cauchy’s integral formula require the closed disk to lie inside the domain D?

The contour γ is the boundary of the disk (a circle). For the integral to make sense and for Cauchy’s theorem to apply, the entire contour must stay inside the region where f is holomorphic. Requiring the closure of the disk to lie in D ensures the circle γ—and also the smaller circles used in the proof—never touch the boundary of D.

What is the role of the auxiliary function G(ζ) = f(ζ)/(ζ − z)?

G is engineered to have exactly one singularity: at ζ = z. Everywhere else on the chosen punctured disk, G is holomorphic because f is holomorphic and the only problematic factor is the denominator ζ − z. This “one exception point” structure lets Cauchy’s theorem reduce contour integrals to the contribution near the singularity.

How does the proof use two contours (a large circle and a small circle around z)?

The integral over the large circle can be related to integrals over smaller circles by applying Cauchy’s theorem to holomorphic regions. The key idea is that away from ζ = z, the integrand is holomorphic, so contributions cancel when deforming contours. The only surviving effect comes from the small circle around the exception point ζ = z.

Why does splitting f(ζ)/(ζ − z) into (f(ζ) − f(z))/(ζ − z) + f(z)/(ζ − z) help?

The term f(z)/(ζ − z) has a constant numerator, making its contour integral directly computable as 2πi times f(z). The remaining term (f(ζ) − f(z))/(ζ − z) is a difference quotient that approaches f′(z) as the small radius ε shrinks, but the contour length also shrinks like 2π ε, forcing that part’s integral to go to 0 in the limit.

Where does the factor 2πi come from?

It comes from the standard contour integral around a simple pole: ∮ dζ/(ζ − z) over a positively oriented circle that winds once around z equals 2πi. In the proof, the constant term f(z) multiplies this integral, producing 2πi f(z), which then becomes f(z) after dividing by 2πi.

Review Questions

  1. State Cauchy’s integral formula precisely, including the contour and the factor in front.
  2. In the proof, what happens to the integral of (f(ζ) − f(z))/(ζ − z) as the inner radius ε → 0, and why?
  3. Why is the winding number of the contour around z equal to 1 in this setup, and how does that affect the result?

Key Points

  1. 1

    Cauchy’s integral formula reconstructs f(z) for any interior point z from the contour integral of f over the surrounding circle.

  2. 2

    The formula requires f to be holomorphic on a domain containing the entire closed disk so the contour stays inside D.

  3. 3

    For a positively oriented circle γ around z with winding number 1, f(z) = (1/(2πi)) ∮_γ f(ζ)/(ζ − z) dζ.

  4. 4

    The proof introduces G(ζ) = f(ζ)/(ζ − z), which is holomorphic everywhere except at ζ = z.

  5. 5

    Contour comparison reduces the problem to the contribution from a small circle around the singularity at ζ = z.

  6. 6

    Splitting the integrand into a difference-quotient part and a constant-pole part makes one term vanish as the inner radius shrinks.

  7. 7

    The remaining term yields the universal 2πi factor tied to integrating 1/(ζ − z) around a simple pole.

Highlights

Cauchy’s integral formula turns Cauchy’s theorem’s “integral is zero” idea into an explicit value-recovery rule for holomorphic functions.
Defining G(ζ) = f(ζ)/(ζ − z) isolates the singularity at ζ = z, letting contour deformation work cleanly.
The difference-quotient term disappears in the ε → 0 limit because the contour length shrinks while the quotient stays bounded.
The entire result hinges on the classic pole integral ∮ dζ/(ζ − z) = 2πi for a contour winding once around z.

Topics