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Course 5

Cauchy Integral Formula & Derivatives

Master Cauchy's integral formula, learn derivative formulas for analytic functions, understand Morera's theorem, and explore the mean value property.

Intermediate5-6 hours10 Practice Questions
Learning Objectives
Understand and apply Cauchy's integral formula
Derive formulas for derivatives of analytic functions
Master Morera's theorem and its applications
Understand the mean value property
Learn higher derivative formulas
Apply these formulas to evaluate integrals
Understand the relationship between analyticity and integral representation
Work with derivative estimates

Cauchy's Integral Formula

Theorem 5.1: Cauchy's Integral Formula
Let f(z)f(z) be analytic in a domain DD, and let CC be a simple closed curve in DD with interior also in DD. Then for any point z0z_0 inside CC:
f(z0)=12πiCf(z)zz0dzf(z_0) = \frac{1}{2\pi i} \oint_C \frac{f(z)}{z-z_0}dz
Proof of Theorem 5.1:

Consider a small circle Cε:zz0=εC_\varepsilon: |z-z_0| = \varepsilon inside CC. Since f(z)zz0\frac{f(z)}{z-z_0} is analytic in the region between CC and CεC_\varepsilon, by deformation:

Cf(z)zz0dz=Cεf(z)zz0dz\oint_C \frac{f(z)}{z-z_0}dz = \oint_{C_\varepsilon} \frac{f(z)}{z-z_0}dz

Parameterizing CεC_\varepsilon as z=z0+εeiθz = z_0 + \varepsilon e^{i\theta}:

Cεf(z)zz0dz=02πf(z0+εeiθ)εeiθiεeiθdθ=i02πf(z0+εeiθ)dθ\oint_{C_\varepsilon} \frac{f(z)}{z-z_0}dz = \int_0^{2\pi} \frac{f(z_0 + \varepsilon e^{i\theta})}{\varepsilon e^{i\theta}} i\varepsilon e^{i\theta}d\theta = i\int_0^{2\pi} f(z_0 + \varepsilon e^{i\theta})d\theta

As ε0\varepsilon \to 0, by continuity: =2πif(z0)= 2\pi i f(z_0), giving the result.

Corollary 5.1: Mean Value Property
If ff is analytic and C:zz0=RC: |z-z_0| = R is a circle in the domain, then:
f(z0)=12π02πf(z0+Reiθ)dθf(z_0) = \frac{1}{2\pi} \int_0^{2\pi} f(z_0 + Re^{i\theta})d\theta
Example 5.1

Problem: Evaluate z=2ezz1dz\oint_{|z|=2} \frac{e^z}{z-1}dz.

Solution:

Since eze^z is analytic everywhere and z=1z=1 is inside z=2|z|=2, by Cauchy's integral formula:

z=2ezz1dz=2πie1=2πie\oint_{|z|=2} \frac{e^z}{z-1}dz = 2\pi i \cdot e^1 = 2\pi i e

Derivative Formulas

Theorem 5.2: Derivative Formula
Under the same conditions as Theorem 5.1, ff has derivatives of all orders at z0z_0, and:
f(n)(z0)=n!2πiCf(z)(zz0)n+1dzf^{(n)}(z_0) = \frac{n!}{2\pi i} \oint_C \frac{f(z)}{(z-z_0)^{n+1}}dz
for n=1,2,3,n = 1, 2, 3, \ldots.
Proof of Theorem 5.2:

Differentiate Cauchy's integral formula with respect to z0z_0:

f(z0)=ddz0[12πiCf(z)zz0dz]=12πiCf(z)(zz0)2dzf'(z_0) = \frac{d}{dz_0}\left[\frac{1}{2\pi i} \oint_C \frac{f(z)}{z-z_0}dz\right] = \frac{1}{2\pi i} \oint_C \frac{f(z)}{(z-z_0)^2}dz

Continuing this process gives the formula for higher derivatives. The differentiation under the integral sign is justified by uniform convergence.

Example 5.2

Problem: Find f(i)f'(i) if f(z)=12πiz=2ezzz0dzf(z) = \frac{1}{2\pi i} \oint_{|z|=2} \frac{e^z}{z-z_0}dz for z0<2|z_0| < 2.

Solution:

By Cauchy's formula, f(z0)=ez0f(z_0) = e^{z_0} for z0<2|z_0| < 2, so f(i)=eif'(i) = e^i.

Alternatively, using the derivative formula: f(i)=12πiz=2ez(zi)2dz=eif'(i) = \frac{1}{2\pi i} \oint_{|z|=2} \frac{e^z}{(z-i)^2}dz = e^i.

Theorem 5.3: Morera's Theorem
If ff is continuous in a domain DD and Cf(z)dz=0\oint_C f(z)dz = 0 for every closed curve CC in DD, then ff is analytic in DD.
Remark 5.1
Morera's theorem is the converse of Cauchy's theorem. It provides a useful criterion for proving analyticity when direct verification of the Cauchy-Riemann equations is difficult.

Morera's Theorem (Converse of Cauchy's Theorem)

Theorem 5.4: Morera's Theorem
If ff is continuous in a simply connected domain DD and Cf(z)dz=0\oint_C f(z)dz = 0 for every closed curve CC in DD, then ff is analytic in DD.
Remark 5.1
Morera's theorem provides a necessary and sufficient condition for analyticity in simply connected domains. Together with Cauchy's theorem, it shows that analyticity is equivalent to the vanishing of contour integrals.

Liouville's Theorem and Applications

Theorem 5.5: Liouville's Theorem
If ff is entire (analytic in the entire complex plane) and bounded, then ff is constant.
Proof of Theorem 5.5:

Suppose f(z)M|f(z)| \leq M for all zz. For any z0z_0, use the derivative formula with a large circle:

f(z0)=12πizz0=Rf(z)(zz0)2dz12πMR22πR=MR|f'(z_0)| = \left|\frac{1}{2\pi i} \oint_{|z-z_0|=R} \frac{f(z)}{(z-z_0)^2}dz\right| \leq \frac{1}{2\pi} \cdot \frac{M}{R^2} \cdot 2\pi R = \frac{M}{R}

Since this holds for arbitrarily large RR, we have f(z0)=0f'(z_0) = 0 for all z0z_0, so ff is constant.

Example 5.3

Problem: Show that a non-constant entire function cannot be bounded.

Solution:

This is a direct consequence of Liouville's theorem. If an entire function is bounded, it must be constant. Therefore, any non-constant entire function (like eze^z, sinz\sin z) is unbounded.

Corollary 5.3: Fundamental Theorem of Algebra
Every non-constant polynomial P(z)P(z) has at least one complex root.
Proof of Corollary 5.3:

Suppose P(z)0P(z) \neq 0 for all zz. Then 1/P(z)1/P(z) is entire. Since P(z)|P(z)| \to \infty as z|z| \to \infty, we have 1/P(z)0|1/P(z)| \to 0, so 1/P(z)1/P(z) is bounded. By Liouville's theorem, 1/P(z)1/P(z) is constant, hence P(z)P(z) is constant, a contradiction.

Example 5.4

Problem: Use Cauchy's integral formula to show that if ff is analytic in zR|z| \leq R and f(z)M|f(z)| \leq M, then f(n)(0)n!MRn|f^{(n)}(0)| \leq \frac{n!M}{R^n}.

Solution:

Using the derivative formula on z=R|z| = R:

f(n)(0)=n!2πiz=Rf(z)zn+1dzn!2πMRn+12πR=n!MRn|f^{(n)}(0)| = \left|\frac{n!}{2\pi i} \oint_{|z|=R} \frac{f(z)}{z^{n+1}}dz\right| \leq \frac{n!}{2\pi} \cdot \frac{M}{R^{n+1}} \cdot 2\pi R = \frac{n!M}{R^n}

Significance of Cauchy's Integral Formula

Representation of Analytic Functions

The formula shows that the value of an analytic function at any point is determined by its values on surrounding curves, demonstrating the "rigidity" of analytic functions.

Infinite Differentiability

The formula for derivatives shows that analytic functions are infinitely differentiable, a remarkable property not shared by real differentiable functions.

Connection to Power Series

The derivative formulas are essential for proving that analytic functions have power series representations, connecting complex analysis to series theory.

Maximum Modulus Principle

Theorem 5.6: Maximum Modulus Principle
If ff is analytic and non-constant in a domain DD, then f(z)|f(z)| cannot attain a maximum at any interior point of DD. If DD is bounded and ff is continuous on D\overline{D}, then the maximum occurs on the boundary D\partial D.
Proof of Theorem 5.6:

Suppose f|f| attains a maximum at an interior point z0z_0. By the mean value property:

f(z0)=12π02πf(z0+reiθ)dθ12π02πf(z0+reiθ)dθf(z0)|f(z_0)| = \left|\frac{1}{2\pi} \int_0^{2\pi} f(z_0 + re^{i\theta})d\theta\right| \leq \frac{1}{2\pi} \int_0^{2\pi} |f(z_0 + re^{i\theta})|d\theta \leq |f(z_0)|

For equality to hold, f|f| must be constant on every circle centered at z0z_0, which implies ff is constant (by analytic continuation).

Example 5.5

Problem: Find the maximum of z2+1|z^2 + 1| on the closed disk z2|z| \leq 2.

Solution:

Since z2+1z^2 + 1 is entire, by the maximum modulus principle, the maximum occurs on the boundary z=2|z| = 2.

On the boundary, z=2eiθz = 2e^{i\theta}, so z2+1=4ei2θ+1|z^2 + 1| = |4e^{i2\theta} + 1|

Maximum occurs when 4ei2θ=44e^{i2\theta} = 4 (aligned with 1), giving maximum 4+1=5|4 + 1| = 5

Theorem 5.7: Minimum Modulus Principle
If ff is analytic and non-constant in a domain DD, and f(z)0f(z) \neq 0 for all zDz \in D, then f(z)|f(z)| cannot attain a minimum at any interior point of DD.
Corollary 5.4: Open Mapping Theorem
If ff is analytic and non-constant in a domain DD, then f(D)f(D) is an open set. In other words, analytic functions map open sets to open sets.

Additional Worked Examples

Example 5.6

Problem: Use Cauchy's integral formula to show that if ff is entire and bounded, then ff is constant.

Solution:

This is Liouville's theorem. For any z0z_0, use the derivative formula with a large circle of radius RR:

f(z0)=12πizz0=Rf(z)(zz0)2dz12πMR22πR=MR|f'(z_0)| = \left|\frac{1}{2\pi i} \oint_{|z-z_0|=R} \frac{f(z)}{(z-z_0)^2}dz\right| \leq \frac{1}{2\pi} \cdot \frac{M}{R^2} \cdot 2\pi R = \frac{M}{R}

Since this holds for arbitrarily large RR, f(z0)=0f'(z_0) = 0, so ff is constant.

Example 5.7

Problem: Evaluate z=2sinzz3dz\oint_{|z|=2} \frac{\sin z}{z^3}dz.

Solution:

The function sinzz3\frac{\sin z}{z^3} has a pole at z=0z = 0. Using the derivative formula:

z=2sinzz3dz=2πisin(0)2!=2πisin(0)2=0\oint_{|z|=2} \frac{\sin z}{z^3}dz = 2\pi i \cdot \frac{\sin''(0)}{2!} = 2\pi i \cdot \frac{-\sin(0)}{2} = 0

Actually, since sinz=zz36+\sin z = z - \frac{z^3}{6} + \cdots, we have sinzz3=1z216+\frac{\sin z}{z^3} = \frac{1}{z^2} - \frac{1}{6} + \cdots, so the residue (coefficient of 1/z1/z) is 0.

Example 5.8

Problem: Prove that if ff is analytic in z<R|z| < R and f(z)M|f(z)| \leq M, then f(n)(0)n!MRn|f^{(n)}(0)| \leq \frac{n!M}{R^n}.

Solution:

Using the derivative formula on a circle of radius r<Rr < R:

f(n)(0)=n!2πiz=rf(z)zn+1dzn!2πMrn+12πr=n!Mrn|f^{(n)}(0)| = \left|\frac{n!}{2\pi i} \oint_{|z|=r} \frac{f(z)}{z^{n+1}}dz\right| \leq \frac{n!}{2\pi} \cdot \frac{M}{r^{n+1}} \cdot 2\pi r = \frac{n!M}{r^n}

Taking rRr \to R gives the result.

Study Tips

1. Understanding Cauchy's Formula

The formula expresses the value of an analytic function at a point as an integral over surrounding curves. This is remarkable: the entire function is determined by its boundary values.

2. Computing Derivatives

Use the derivative formula when the integrand has the form f(z)(zz0)n+1\frac{f(z)}{(z-z_0)^{n+1}} where ff is analytic. The nnth derivative is given by n!2πif(z)(zz0)n+1dz\frac{n!}{2\pi i} \oint \frac{f(z)}{(z-z_0)^{n+1}}dz.

3. Liouville's Theorem Applications

If you can show a function is entire and bounded, it must be constant. This is often used to prove identities or show that certain functions don't exist.

Additional Worked Examples

Example 5.9

Problem: Use Cauchy's integral formula to evaluate z=2ezz1dz\oint_{|z|=2} \frac{e^z}{z-1}dz.

Solution:

The function eze^z is analytic inside z=2|z| = 2, and we have the form f(z)z1\frac{f(z)}{z-1} where f(z)=ezf(z) = e^z.

By Cauchy's integral formula: z=2ezz1dz=2πie1=2πie\oint_{|z|=2} \frac{e^z}{z-1}dz = 2\pi i \cdot e^1 = 2\pi i e

Example 5.10

Problem: Find f(0)f''(0) if f(z)=12πiz=1eζζ3dζf(z) = \frac{1}{2\pi i} \oint_{|z|=1} \frac{e^{\zeta}}{\zeta^3}d\zeta.

Solution:

Using the derivative formula: f(n)(z0)=n!2πif(ζ)(ζz0)n+1dζf^{(n)}(z_0) = \frac{n!}{2\pi i} \oint \frac{f(\zeta)}{(\zeta-z_0)^{n+1}}d\zeta

Here n=2n = 2, z0=0z_0 = 0, and f(ζ)=eζf(\zeta) = e^{\zeta}

f(0)=2!2πiz=1eζζ3dζ=22πi2πie02!=1f''(0) = \frac{2!}{2\pi i} \oint_{|z|=1} \frac{e^{\zeta}}{\zeta^3}d\zeta = \frac{2}{2\pi i} \cdot 2\pi i \cdot \frac{e^0}{2!} = 1

Example 5.11

Problem: Prove that if ff is analytic and f(z)zn|f(z)| \leq |z|^n for large z|z|, then ff is a polynomial of degree at most nn.

Solution:

Using the derivative estimate with f(n+1)(0)f^{(n+1)}(0) and a large circle, we find f(n+1)(0)=0|f^{(n+1)}(0)| = 0.

By uniqueness of power series, all coefficients beyond degree nn are zero, so ff is a polynomial.

Example 5.12

Problem: Show that if ff is entire and Re(f(z))0\text{Re}(f(z)) \leq 0 for all zz, then ff is constant.

Solution:

Consider g(z)=ef(z)g(z) = e^{f(z)}. Since Re(f(z))0\text{Re}(f(z)) \leq 0, we have g(z)=eRe(f(z))1|g(z)| = e^{\text{Re}(f(z))} \leq 1.

gg is entire and bounded, so by Liouville's theorem, gg is constant.

Therefore ff is constant.

Example 5.13

Problem: Use Cauchy's integral formula to show that if ff is analytic and f(z)M|f(z)| \leq M for zR|z| \leq R, then f(n)(0)n!MRn|f^{(n)}(0)| \leq \frac{n!M}{R^n}.

Solution:

Using the derivative formula on z=R|z| = R:

f(n)(0)=n!2πiz=Rf(z)zn+1dzn!2πMRn+12πR=n!MRn|f^{(n)}(0)| = \left|\frac{n!}{2\pi i} \oint_{|z|=R} \frac{f(z)}{z^{n+1}}dz\right| \leq \frac{n!}{2\pi} \cdot \frac{M}{R^{n+1}} \cdot 2\pi R = \frac{n!M}{R^n}

Example 5.14

Problem: Evaluate z=2ez(z1)2dz\oint_{|z|=2} \frac{e^z}{(z-1)^2}dz.

Solution:

Using the derivative formula with n=1n = 1:

z=2ez(z1)2dz=2πif(1)\oint_{|z|=2} \frac{e^z}{(z-1)^2}dz = 2\pi i \cdot f'(1) where f(z)=ezf(z) = e^z

Since f(z)=ezf'(z) = e^z, we have f(1)=ef'(1) = e

Therefore: z=2ez(z1)2dz=2πie\oint_{|z|=2} \frac{e^z}{(z-1)^2}dz = 2\pi i e

Example 5.15

Problem: Prove that if ff is entire and f(z+1)=f(z)f(z+1) = f(z) for all zz, and f(z)|f(z)| is bounded in the strip 0Re z10 \leq \text{Re } z \leq 1, then ff is constant.

Solution:

By periodicity, ff is bounded everywhere. By Liouville's theorem, ff is constant.

Example 5.16

Problem: Show that if ff is analytic in z<R|z| < R and f(z)M|f(z)| \leq M, then f(0)M/R|f'(0)| \leq M/R.

Solution:

Using the derivative formula with n=1n = 1 and a circle of radius r<Rr < R:

f(0)=12πiz=rf(z)z2dz12πMr22πr=Mr|f'(0)| = \left|\frac{1}{2\pi i} \oint_{|z|=r} \frac{f(z)}{z^2}dz\right| \leq \frac{1}{2\pi} \cdot \frac{M}{r^2} \cdot 2\pi r = \frac{M}{r}

Taking rRr \to R gives the result.

Example 5.17

Problem: Show that if ff is analytic in zR|z| \leq R and f(z)M|f(z)| \leq M, then f(z)M|f(z)| \leq M for z<R|z| < R with equality only if ff is constant.

Solution:

This follows from the maximum modulus principle. If f|f| attains its maximum at an interior point, then ff must be constant.

Example 5.18

Problem: Evaluate z=1coszz2dz\oint_{|z|=1} \frac{\cos z}{z^2}dz.

Solution:

Using the derivative formula with n=1n = 1:

z=1coszz2dz=2πicos(0)=2πi(sin(0))=0\oint_{|z|=1} \frac{\cos z}{z^2}dz = 2\pi i \cdot \cos'(0) = 2\pi i \cdot (-\sin(0)) = 0

Example 5.19

Problem: Use Cauchy's integral formula to evaluate z=1e2zzdz\oint_{|z|=1} \frac{e^{2z}}{z}dz.

Solution:

The function e2ze^{2z} is entire. By Cauchy's integral formula:

z=1e2zzdz=2πie20=2πi\oint_{|z|=1} \frac{e^{2z}}{z}dz = 2\pi i \cdot e^{2 \cdot 0} = 2\pi i

Example 5.20

Problem: Show that an entire function ff with f(z)zn|f(z)| \leq |z|^n for large z|z| is a polynomial of degree at most nn.

Solution:

Using the derivative estimate on large circles, we find that f(n+1)(0)=0f^{(n+1)}(0) = 0. Since ff is entire, its Taylor series is valid everywhere, and all coefficients beyond degree nn are zero.

Example 5.21

Problem: Show that if ff is analytic and f(z)=1|f(z)| = 1 on z=1|z| = 1, and f(0)=0f(0) = 0, then f(z)=czf(z) = cz for some constant c=1|c| = 1.

Solution:

Consider g(z)=f(z)/zg(z) = f(z)/z for z0z \neq 0. Then g(z)=1|g(z)| = 1 on z=1|z| = 1.

By maximum modulus principle, g(z)1|g(z)| \leq 1 for z1|z| \leq 1, and since g=1|g| = 1 on the boundary, gg is constant.

Therefore f(z)=czf(z) = cz with c=1|c| = 1.

Example 5.22

Problem: Prove that if ff is entire and f(z)1+z1/2|f(z)| \leq 1 + |z|^{1/2}, then ff is constant.

Solution:

Using the derivative estimate with n=1n = 1 on large circles, we find that f(0)=0f'(0) = 0.

Since ff is entire, shifting the argument shows f(z)=0f'(z) = 0 for all zz, so ff is constant.

Example 5.23

Problem: Evaluate z=1ez2z3dz\oint_{|z|=1} \frac{e^{z^2}}{z^3}dz.

Solution:

Using the derivative formula with n=2n = 2 and f(z)=ez2f(z) = e^{z^2}:

z=1ez2z3dz=2πif(0)2!=πi2e0=2πi\oint_{|z|=1} \frac{e^{z^2}}{z^3}dz = 2\pi i \cdot \frac{f''(0)}{2!} = \pi i \cdot 2e^0 = 2\pi i

Example 5.24

Problem: Show that if ff is entire and Re(f(z))0\text{Re}(f(z)) \geq 0 for all zz, then ff is constant.

Solution:

Consider g(z)=ef(z)g(z) = e^{-f(z)}. Then g(z)=eRe(f(z))1|g(z)| = e^{-\text{Re}(f(z))} \leq 1.

Since gg is entire and bounded, by Liouville's theorem, gg is constant, so ff is constant.

Example 5.25

Problem: Prove that a non-constant entire function cannot be bounded away from zero. That is, if ff is entire and f(z)ε>0|f(z)| \geq \varepsilon > 0 for all zz, then ff is constant.

Solution:

If f(z)ε>0|f(z)| \geq \varepsilon > 0 for all zz, then 1/f(z)1/f(z) is entire and 1/f(z)1/ε|1/f(z)| \leq 1/\varepsilon.

By Liouville's theorem, since 1/f1/f is entire and bounded, it must be constant.

Therefore, ff is constant. This shows that non-constant entire functions must take values arbitrarily close to zero.

Example 5.26

Problem: Use the maximum modulus principle to show that if ff is analytic in a bounded domain DD and continuous on D\overline{D}, then the maximum of f(z)|f(z)| occurs on the boundary D\partial D, unless ff is constant.

Solution:

Suppose the maximum occurs at an interior point z0Dz_0 \in D. By the maximum modulus principle, if f|f| attains its maximum at an interior point, then ff must be constant in a neighborhood of z0z_0.

Since DD is connected, the identity theorem (which we'll see later) implies that ff is constant throughout DD.

Therefore, if ff is not constant, the maximum must occur on the boundary D\partial D.

This is a fundamental result in complex analysis with applications to harmonic functions, potential theory, and optimization problems.

Practice Problems

Cauchy Integral Formula & Derivatives Practice
10
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1
Cauchy's integral formula states that if f(z)f(z) is analytic inside and on a simple closed curve CC, then for z0z_0 inside CC:
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2
Using Cauchy's integral formula, z=2ezz1dz\oint_{|z|=2} \frac{e^z}{z-1}dz equals:
Medium
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3
The nn-th derivative formula for analytic functions is:
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4
Morera's theorem states that if Cf(z)dz=0\oint_C f(z)dz = 0 for every closed curve CC in a domain DD, then:
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5
The mean value property states that for an analytic function ff and circle C:zz0=RC: |z-z_0| = R:
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6
Using the derivative formula, z=1coszz3dz\oint_{|z|=1} \frac{\cos z}{z^3}dz equals:
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7
An important consequence of Cauchy's integral formula is that:
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8
If ff is analytic and f(z)M|f(z)| \leq M on zz0=R|z-z_0| = R, then f(n)(z0)|f^{(n)}(z_0)| \leq:
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9
The formula f(z0)=12π02πf(z0+Reiθ)dθf(z_0) = \frac{1}{2\pi} \int_0^{2\pi} f(z_0 + Re^{i\theta})d\theta is called the:
Medium
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10
To evaluate z=2z2z1dz\oint_{|z|=2} \frac{z^2}{z-1}dz using Cauchy's formula, we get:
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Frequently Asked Questions

Why is Cauchy's integral formula so powerful?

It allows us to compute values of analytic functions and their derivatives at interior points using only information on the boundary. This is remarkable because in general, boundary values don't determine interior values, but for analytic functions they do.

How do I use Cauchy's integral formula to evaluate integrals?

If you have an integral of the form $\oint \frac{f(z)}{z-z_0}dz$ where $f$ is analytic, then the integral equals $2\pi i f(z_0)$ if $z_0$ is inside the curve, and $0$ if it's outside.

Why do analytic functions have derivatives of all orders?

This follows from the derivative formulas. Since we can repeatedly differentiate under the integral sign in Cauchy's formula, all derivatives exist. This is much stronger than real differentiability, where a function can be differentiable but not twice differentiable.

What is Liouville's theorem and why is it important?

Liouville's theorem states that every bounded entire function is constant. This is a powerful result with many applications: it proves the Fundamental Theorem of Algebra, shows that non-constant entire functions are unbounded, and is used to prove many other theorems in complex analysis.

What does the mean value property tell us?

It shows that analytic functions behave like harmonic functions: the value at a point equals the average of values on any circle centered at that point. This leads to important properties like the maximum modulus principle.