Master Cauchy's integral formula, learn derivative formulas for analytic functions, understand Morera's theorem, and explore the mean value property.
Consider a small circle inside . Since is analytic in the region between and , by deformation:
Parameterizing as :
As , by continuity: , giving the result.
Problem: Evaluate .
Solution:
Since is analytic everywhere and is inside , by Cauchy's integral formula:
Differentiate Cauchy's integral formula with respect to :
Continuing this process gives the formula for higher derivatives. The differentiation under the integral sign is justified by uniform convergence.
Problem: Find if for .
Solution:
By Cauchy's formula, for , so .
Alternatively, using the derivative formula: .
Suppose for all . For any , use the derivative formula with a large circle:
Since this holds for arbitrarily large , we have for all , so is constant.
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 , ) is unbounded.
Suppose for all . Then is entire. Since as , we have , so is bounded. By Liouville's theorem, is constant, hence is constant, a contradiction.
Problem: Use Cauchy's integral formula to show that if is analytic in and , then .
Solution:
Using the derivative formula on :
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.
The formula for derivatives shows that analytic functions are infinitely differentiable, a remarkable property not shared by real differentiable functions.
The derivative formulas are essential for proving that analytic functions have power series representations, connecting complex analysis to series theory.
Suppose attains a maximum at an interior point . By the mean value property:
For equality to hold, must be constant on every circle centered at , which implies is constant (by analytic continuation).
Problem: Find the maximum of on the closed disk .
Solution:
Since is entire, by the maximum modulus principle, the maximum occurs on the boundary .
On the boundary, , so
Maximum occurs when (aligned with 1), giving maximum
Problem: Use Cauchy's integral formula to show that if is entire and bounded, then is constant.
Solution:
This is Liouville's theorem. For any , use the derivative formula with a large circle of radius :
Since this holds for arbitrarily large , , so is constant.
Problem: Evaluate .
Solution:
The function has a pole at . Using the derivative formula:
Actually, since , we have , so the residue (coefficient of ) is 0.
Problem: Prove that if is analytic in and , then .
Solution:
Using the derivative formula on a circle of radius :
Taking gives the result.
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.
Use the derivative formula when the integrand has the form where is analytic. The th derivative is given by .
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.
Problem: Use Cauchy's integral formula to evaluate .
Solution:
The function is analytic inside , and we have the form where .
By Cauchy's integral formula:
Problem: Find if .
Solution:
Using the derivative formula:
Here , , and
Problem: Prove that if is analytic and for large , then is a polynomial of degree at most .
Solution:
Using the derivative estimate with and a large circle, we find .
By uniqueness of power series, all coefficients beyond degree are zero, so is a polynomial.
Problem: Show that if is entire and for all , then is constant.
Solution:
Consider . Since , we have .
is entire and bounded, so by Liouville's theorem, is constant.
Therefore is constant.
Problem: Use Cauchy's integral formula to show that if is analytic and for , then .
Solution:
Using the derivative formula on :
Problem: Evaluate .
Solution:
Using the derivative formula with :
where
Since , we have
Therefore:
Problem: Prove that if is entire and for all , and is bounded in the strip , then is constant.
Solution:
By periodicity, is bounded everywhere. By Liouville's theorem, is constant.
Problem: Show that if is analytic in and , then .
Solution:
Using the derivative formula with and a circle of radius :
Taking gives the result.
Problem: Show that if is analytic in and , then for with equality only if is constant.
Solution:
This follows from the maximum modulus principle. If attains its maximum at an interior point, then must be constant.
Problem: Evaluate .
Solution:
Using the derivative formula with :
Problem: Use Cauchy's integral formula to evaluate .
Solution:
The function is entire. By Cauchy's integral formula:
Problem: Show that an entire function with for large is a polynomial of degree at most .
Solution:
Using the derivative estimate on large circles, we find that . Since is entire, its Taylor series is valid everywhere, and all coefficients beyond degree are zero.
Problem: Show that if is analytic and on , and , then for some constant .
Solution:
Consider for . Then on .
By maximum modulus principle, for , and since on the boundary, is constant.
Therefore with .
Problem: Prove that if is entire and , then is constant.
Solution:
Using the derivative estimate with on large circles, we find that .
Since is entire, shifting the argument shows for all , so is constant.
Problem: Evaluate .
Solution:
Using the derivative formula with and :
Problem: Show that if is entire and for all , then is constant.
Solution:
Consider . Then .
Since is entire and bounded, by Liouville's theorem, is constant, so is constant.
Problem: Prove that a non-constant entire function cannot be bounded away from zero. That is, if is entire and for all , then is constant.
Solution:
If for all , then is entire and .
By Liouville's theorem, since is entire and bounded, it must be constant.
Therefore, is constant. This shows that non-constant entire functions must take values arbitrarily close to zero.
Problem: Use the maximum modulus principle to show that if is analytic in a bounded domain and continuous on , then the maximum of occurs on the boundary , unless is constant.
Solution:
Suppose the maximum occurs at an interior point . By the maximum modulus principle, if attains its maximum at an interior point, then must be constant in a neighborhood of .
Since is connected, the identity theorem (which we'll see later) implies that is constant throughout .
Therefore, if is not constant, the maximum must occur on the boundary .
This is a fundamental result in complex analysis with applications to harmonic functions, potential theory, and optimization problems.
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.
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.
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.
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.
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.