**Open Access Library Journal**

Vol.03 No.06(2016), Article ID:69408,8 pages

10.4236/oalib.1102732

Proofs of the Density Theorem and Fatou’s Radial Limit Theorem Using the Poisson Integral

John Marafino

Department of Mathematics and Statistics, James Madison University, Harrisonburg, VA, USA

Copyright © 2016 by author and OALib.

This work is licensed under the Creative Commons Attribution International License (CC BY).

http://creativecommons.org/licenses/by/4.0/

Received 29 May 2016; accepted 20 June 2016; published 23 June 2016

ABSTRACT

Using only the Poisson integral and elementary convergence theorems, we prove the well-known Density theorem and Fatou’s radial limit theorem.

**Keywords:**

Poisson Integral, Density, Radial Limits, Harmonic Functions

**Subject Areas:** **Function Theory**

1. Introduction

In most texts, [1] (p. 261), [2] (p. 187), [3] (p. 129), to name a few, the Density Theorem is proven using the fact that if f is Lebesgue integrable and if σ = òf, then σ¢ = f a.e. This result in turn is proven using the Vitali Covering Theorem. The same procedure is also used in the proof of Fatou’s radial limit theorem (see [4] , p. 129, and [5] , Vol. II, p. 362-364). We circumvent this reasoning in an attempt to make the Density and Fatou theorems more accessible to the reader. Our major reference will be Royden’s book Real Analysis, and we will restrict ourselves to its first four chapters. These include a general introduction to set theory, the real number system, Lebesgue measurable functions, and the Lebesgue integral. Our major analytical tool will be the Poisson integral and we will use some of its well-known fundamental properties.

We first introduce the background material that will be used in the course of this note. Our setting is the unit disk D and its boundary C. We shall say that a sequence {I_{k}} of arcs in C converges to and write I_{k} ® e^{iθ}, , if for each k and. Let A be any subset of C and let m^{*} and m denote respectively the outer Lebesgue measure and the Lebesgue measure on C. For any measurable set E in C we define. We shall say that the derivative of σ_{A} at e^{iθ} exists if there exists a number such that for any sequence {I_{k}} of arcs converging to e^{iθ},

If, e^{iθ} is called a point of density of A and if, e^{iθ} is called a point of dispersion of A.

The Density Theorem states that if A is any set (measurable or not) in C, then e^{iθ} is a point of density for A for almost all e^{iθ} in A. We shall prove that this result in the case A is measurable.

Let u(z), , be defined by the Poisson integral,

(1)

where is the characteristic function on the measurable set, and

is the Poisson kernel. When A is a finite union of open arcs, then χ_{A} is a bounded piecewise continuous function on C. So, if ξ is a point of continuity of χ_{A}, then a straight-forward examination of the integral in (1) shows that the limit of u(z), as z approaches ξ exists and equals χ_{A}(ξ) (see [6] , Vol. II, p. 156; [7] , p. 206; and [4] , p. 130). The kernel has two nice properties:

i) and

ii) (see [8] , p. 165-167 and [9] , p. 305-307).

It follows that for all. We will use these elementary results in Sections 2 and 3.

2. The Density Theorem

Theorem: Let A be measurable. Then almost every point of A is a point of density of A.

Proof: Let B be those points of A that are not points of density of A; that is,

where I_{δ}, δ > 0, denotes an arc containing e^{iθ} having length δ. For each, let. We will first show that B can be rewritten as

where is an arc centered at e^{iθ} with length 2ξ_{k} such that ξ_{k} → 0 as k → ∞. This reformulation of B is

crucial to our proof. Clearly, any point in this set is in B. Now suppose. Then there exists a positive number ε and a sequence {δ_{n}} such that δ_{n} ® 0 as n ® ¥ and

For each n let s_{n} denote the length of the largest component of and choose k_{n} such that. Then

Since the last expression approaches 1 − ε/2 as k_{n} ® ¥, it follows that

Using this reformulation of B, the facts that for each k, is a continuous function of θ and consequently measurable, theorem 20 in [10] (p. 56), and that A is a measurable set, it readily follows that B is a measurable set. Hence, it is the union of an F-σ set and a set N of measure zero; that is,

where each F_{n} is a closed subset of B. If we show each F_{n} has measure zero, then the theorem is proved. We pick a F_{n} and denote it by F in order to avoid layered subscript notation. Now, where O_{k} are pairwise

disjoint open arcs. For each, let, χ_{n} be the characteristic function of D_{n}, and set for. Note that for all n, , and. We know from our introductory remarks that except for a finite number of e^{iθ} on C,. Let S_{n} denote this exceptional set. If we set, then for all and for all n,

(2)

Also, for all e^{iθ} Î C,

(3)

We now show that m(F) = 0 using an indirect argument. Before we formally proceed we indicate the direction our proof will take: We define the Poisson integral of the characteristic function on F and using Equations (2) and (3), along with the assumption that F has positive measure, find a subset of F where the radial limit of this function is 1. We then use the reformulation of B to show that this cannot happen.

So, suppose that m(F) > 0. Momentarily fix θ. For each, define. Then r_{k} ® 1 as k ® ¥. Since for each k, is a nonnegative and integrable function of j, we have ( [10] , p. 73) that for each ξ_{k} there exists δ_{k} > 0 such that if E is any set with m(E) < δ_{k}, then

(4)

For each, let. Using Egorov’s Theorem ( [10] , p. 59), we have for each k an open set M_{k} such that

and uniformly on M_{k}. (5)

Note that, and since S is at most countable, has positive measure. Set.

We now claim that if e^{iθ} is in, then. Let ε be an arbitrary positive number and choose K such that for k > K, ξ_{k} < ε/4. Now for k > K,

Since χ_{n} converges uniformly to χ_{F} on M_{k} we choose N = N(ε) such that on M_{k}. Thus,

Using (4) with the fact that one also has

Hence, for all k > K. Because, Equation (2) holds. In addition, we have for all n that χ_{n} = χ_{F} on F. Consequently, for k sufficiently large,

and since ε was arbitrary, our claim is established.

However, using the reformulation of B we know that since and, there exists a positive number η and a subsequence of arcs with the property that

Since, we have

Since the last expression approaches η/2π as or as, we have that the

and this contradicts our previous claim. Thus, the measure of F cannot be positive and so m(F) = 0.

3. Density and the Radial

In this section we establish relationships between the density of A at a point of C and the radial limit of the Poisson integral of the characteristic function on A at this point. The proofs of the first two theorems employ well-known procedures and inequalities. Theorem 3 highlights the last result in the proof of the Density Theorem. We then use these relationships and prove in Corollary 5 Fatou’s radial limit theorem.

Theorem 1. If e^{iθ} is a point of density of A and u(z) represents the Poisson integral of, then the radial limit of u(z) at e^{iθ} is 1.

Proof: Without loss of generality we can assume e^{i}^{q} = e^{i}^{0} = 1 and we express the Poisson integral of χ_{A} over the interval [−π, π] instead of [0, 2π]. We must show that.

Since 1 is a point of density of the measurable set A, it follows that 1 is a point of dispersion of A^{C}, the complement of A with respect to C. Letting, where I_{δ}(1) denotes the arc on C centered at 1with length 2δ, we know that ε(δ) ® 0 as δ ® 0. Let z = r. Then

(6)

There are two possibilities that can happen with the function ε(δ), δ > 0. Either there exists a δ_{0} such that ε(δ_{0}) = 0; or for all δ, ε(δ) ≠ 0.

In the first case it follows that for all. We now rewrite (6) as

In the first integral we know that; and for,. Hence, the integral is zero. For the second integral we have that and so. Now

On [0, π/2] we have that sin(x) ≥ (2/π)x. So if r > 1/2 we get, and hence

The third integral is handled like the second, and so our theorem follows.

In the second case it follows that if δ is sufficiently small, is a continuous increasing function of δ. So there exists a δ_{0} such that the expression is continuous and increasing

on (0, δ_{0}). Consequently, the expression is a continuous increasing function of δ on (0, δ_{0}) with the

property that as δ→0. Using this result we know that as r ® 1, 1 − r ® 0 and so it can be

represented by for some δ_{r}. Furthermore, 1 - r ® 0 iff δ_{r} ® 0. On the interval [−δ_{r}, δ_{r}] we use the inequality to get

We now rewrite (6) as was done in the first case but using δ_{r} instead of δ_{0}. The first integral is handled above. The second integral is handled exactly as before. We get

The third integral is handled like above. Hence, our theorem follows. Using a similar argument we can obtain the second result of this section.

Theorem 2. If e^{iθ} is a point of dispersion of A, then the radial limit of u(z) at e^{iθ} is 0.

Theorem 3. If e^{iθ} is neither a point of density of A nor a point of dispersion of A, then the radial limit, if it exists, cannot be 1 or 0.

Proof: From the hypothesis we know there exists an ε > 0 and two sequences of arcs, where δ_{n} and ρ_{n} denote the length of and respectively, such that for all n, for all n,

for all n,

for all n,

and δ_{n} ® 0 and ρ_{n} ® 0 as n ® ¥. Since the arcs are not centered at e^{iθ} we define ξ_{n} to be the maximum of the lengths of the components of and define to be the arc centered at e^{iθ} with length 2ξ_{n}. Using we define τ_{n} similarly. Let and. Then,

Since the last expression approaches ε/4π as ξ_{n} ® 0 or as r_{n} ® 1, we have that the

(7)

A similar argument using shows that the. It follows that if the radial limit of u(z) at e^{iθ} exists, then it cannot be 1 or 0.

Corollary 1: Let A be any measurable set in C. Let Then for almost every e^{iθ} Î C,.

Proof: Using the Density Theorem on A and Theorem 1, we have for almost every e^{iθ} in A,. Since A^{C} is also measurable we have that almost every point of A^{C} is a point of density of A^{C}. Hence, almost every point of A^{C} is a point of dispersion of A. By Theorem 2 we have that for almost every e^{iθ} in A^{C},.

Corollary 2: Let f be a simple function defined on C. Let Then for almost every e^{iθ} Î C,

Proof: If f is simple, then where the A_{i} are pair-wise disjoint and measurable and the a_{i} are distinct and nonzero. Using Corollary 1, our result follows.

Corollary 3: Let f be a bounded measurable function defined on C. Let Then for almost every e^{iθ} Î C,

Proof: Since f is bounded and measurable, there exists simple functions ψ_{n}, ψ_{n} £ f, such that uniformly on C. By adding and subtracting the appropriate terms and using the triangle inequality one can show that

We analyze each term on the right hand side of this inequality. Since the kernel P(z, j) is non-negative and its definite integral is 2π (see Section 1), and since ψ_{n} converges uniformly to f on C, the first term can be made arbitrarily small when n is sufficiently large. From Corollary 2 we get that the second term can be made arbitrarily small as r approaches 1. The last term approaches 0 for n sufficiently large since ψ_{n} converges uniformly to f on C. Consequently, our result follows.

Corollary 4: Let f be a nonnegative integrable function defined on C. Let Then for almost every,

Proof: Let. Since f is integrable we know that m(S) = 2π. For each, define. Each f_{n} is bounded, nonnegative, and measurable on S. The functions also satisfy the following on S: and Since P(z, j) is non-negative we have that and hence on S. By the Monotone Convergence Theorem ( [10] , p. 72) we know that

Once again, by adding and subtracting the appropriate terms and using the triangle inequality one can show that

From our above remarks, the first term can be made arbitrarily small for n sufficiently large. Using Corollary 3, the second term can be made arbitrarily small as r approaches 1. The last term approaches 0 on S as n gets large. Consequently, our result follows.

Corollary 5: (Fatou) Let f be integrable on C. Let Then for almost every e^{iθ}ÎC,

Proof: We know that where and. Since f is integrable, both and must be integrable. We can now use Corollary 4 on and to get our result.

Cite this paper

John Marafino, (2016) Proofs of the Density Theorem and Fatou’s Radial Limit Theorem Using the Poisson Integral. *Open Access Library Journal*,**03**,1-8. doi: 10.4236/oalib.1102732

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