Absolute continuity vs total singularity - George Washington University

51
Absolute continuity vs total singularity Absolute continuity vs total singularity E. Arthur (Robbie) Robinson The George Washington University February 16, 2012

Transcript of Absolute continuity vs total singularity - George Washington University

Page 1: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Absolute continuity vs totalsingularity

E. Arthur (Robbie) Robinson

The George Washington University

February 16, 2012

Page 2: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Outline

1 Introduction

2 preliminaries

3 The Banach Lemma

4 Villani’s lemma

5 Proof of Kakeya’s lemma

6 Next. . .

Page 3: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Introduction

1 Introduction

2 preliminaries

3 The Banach Lemma

4 Villani’s lemma

5 Proof of Kakeya’s lemma

6 Next. . .

Page 4: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Introduction

Part 1

In the first lecture I want to prove the following theorem (andsome related results).

Lemma (Kakeya’s Lemma)

If f : [0, 1]→ R is continuous, strictly monotone and satisfies|f ′(x)| ≥ a > 0 a.e., then f−1(x) is absolutely continuous, and|(f−1)′(x)| ≤ 1/a a.e..

This was stated without proof by Soichi Kakeya in his 1924 paperon representing real numbers. The necessity of this theorem wasmissed in Fritz Schweiger’s 1995 account of Kakeya’s theorem(which he thus states incorrectly).

I was surprised by how difficult it turned out to be!

We will begin by reviewing some of the relevant background.

Page 5: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Introduction

Part 2

In the second lecture, I will discuss examples of strictly increasingcontinuous functions f : [0, 1]→ [0, 1] with f ′(x) = 0 a.e. I callthese totally singular (TS) functions.

The most famous TS function is Minkowski’s “question mark”function ?(x). The inverse ?−1(x), which is also TS, is known asJohn H. Conway’s “box” function. Both implement a strictlymonotone bijection between the rationals and dyadic rationals in[0, 1].

We will also look at some examples of TS functions due to RaphelSalem, which are related to the Koch snowflake.

This will be in 2 weeks.

Page 6: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Introduction

Math Classes

Some results and definitions quoted in this talk come from specificmath classes. The GW numbering for them is:

M 1231: Calculus I

M 1232: Calculus II

M 4239/40: Undergraduate Analysis I & II

M 6214: Measure theory (Graduate Analysis I)

M 6215: Functional Analysis (Graduate Analysis II)

Page 7: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

preliminaries

1 Introduction

2 preliminaries

3 The Banach Lemma

4 Villani’s lemma

5 Proof of Kakeya’s lemma

6 Next. . .

Page 8: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

preliminaries

Monotonicity

A function f : [0, 1]→ R is increasing if x < y, x, y ∈ [0, 1]implies f(x) ≤ f(y).A function f : [0, 1]→ R is strictly increasing if x < y,x, y ∈ [0, 1] implies f(x) < f(y).

The definitions of decreasing and strictly decreasing areanalogous.

A function is monotonic if it is either increasing or decreasingand strictly monotonic if it is either strictly increasing orstrictly decreasing.

(M 1231)

Page 9: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

preliminaries

properties of monotonic functions

A monotonic function is continuous except, at most, on acountable set. The discontinuities are all jumps. By changingcountably many values, we can assume it is right continuous(M 4839/40 or M 6214).

A monotonic function is differentiable almost everywhere (theset of x so that

f ′(x) = limh→0

f(x+ h)− f(x)h

either does not exist or is ±∞ has measure zero (M 6214)).

Page 10: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

preliminaries

The Riesz representation theorem

Any regular finite Borel measure µ on [0, 1] is defined by a rightcontinuous increasing function g : [0, 1]→ R.

In particular,µ([a, b]) = g−(b)− g(a),

andµ((a, b)) = g(b)− g+(a),

where [a, b] ⊆ [0, 1]. (g+ and g− are right and left limits.)

Conversely, any such g defines a measure µg. (M6215)

Page 11: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

preliminaries

Bounded variation

A function has bounded variation (BV) if

V (f) = supP

n∑k=1

|f(xk)− f(xk−1)| <∞,

where P is a partition of [0, 1] of the form

P : 0 = x0 < x1 < · · · < xn = 1.

Using Riesz representation, µf is a signed measure.

This is an element of the ball B of radius V (f) in the dualC([0, 1])∗ via f 7→

∫fdµg. This ball is weak-* compact

(M 6215).

Page 12: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

preliminaries

Properties of bounded variation

Clearly, any monotonic f has V (f) = |f(1)− f(0)| <∞ (i.e.,BV).

If V (f) <∞ (i.e., BV) then there exist increasing g anddecreasing h so that f(x) = g(x) + h(x). Almost unique(M 6214).

BV functions are continuous except on an at most countableset.

BV functions are differentiable almost everywhere.

If f ∈ C1([0, 1]), then f has BV (M 4839/40).

Page 13: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

preliminaries

Continuity

A function f : [0, 1]→ R is continouos (C) if for all ε > 0 andx ∈ [0, 1], there exists δ > 0 so that if |x− y| < δ, y ∈ [0, 1]then |f(x)− f(y)| < ε (M 1231).

A function f : [0, 1]→ R is uniformly continouos (UC) if forall ε > 0, there exists δ > 0 so that if |x− y| < δ, x, y ∈ [0, 1]then |f(x)− f(y)| < ε (M 4239).

Page 14: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

preliminaries

Absolute continuity

Let I = {(xi, yi) : i = 1, . . . , n} denote a finite collection ofdisjoint open intervals in [0, 1].We say f : [0, 1]→ R is absolutely continuous (AC) if for all ε > 0there exists δ > 0 so that for any I with

n∑i=1

(xi − yi) < δ

we haven∑i=1

|f(xi)− f(yi)| < ε.

(M 6214).

Page 15: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

preliminaries

Continuity properties

AC =⇒ UC =⇒ C.

C =⇒ UC (since [0, 1] is compact. M 4239/40)

AC =⇒ BV (M 6214).

Thus AC =⇒ f ′(x) exists a.e.

UC (or C) 6 =⇒ BV (M 6214).

Thus UC 6 =⇒ AC.

Also UC + BV 6 =⇒ AC (we will see this and much more).

Page 16: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

preliminaries

Fundamental theorem of calculus

If f : [0, 1]→ R is increasing then

f(x) ≥ f(0) +∫ x

0f ′(t)dt.

f : [0, 1]→ R is AC if and only if

f(x) = f(0) +

∫ x

0f ′(t)dt.

(both M 6214)

This holds for f ∈ C1 (M 1231) so C1 =⇒ AC.

Page 17: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

preliminaries

Examples & Facts

The Cantor function is an increasing continuous surjectionf : [0, 1]→ [0, 1] so that f ′(x) = 0 a.e. (f ′(x) = 0 on a denseopen set). It is not strictly increasing (not 1:1). (SC=“singularcontinuous”)

(Source: http://mathworld.wolfram.com/CantorFunction.html)

Page 18: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

preliminaries

Examples & Facts

There exist strictly increasing continuous functionsg : [0, 1]→ [0, 1] so that g′(x) = 0 a.e. These correspond tosingular Borel measures that are positive on open sets (!) Theseare the topic of the second lecture. (TS=“totally singular”)

(Source:http://en.wikipedia.org/wiki/Minkowski%27s question mark function)

The Cantor and ? functions both show UC + BV 6 =⇒ AC.

Page 19: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

preliminaries

Examples & Facts

(Lebesgue decomposition theorem) An increasing f can bewritten as a sum of increasing functions

f(x) = fac(x) + fsc(x) + fd(x)

where fac ∈ AC, fsc is continuous with f ′sc(x) = 0 a.e. (SC),and fd is a step function (M 6214).

If f is strictly a increasing bijection, then f is continuous, andf−1 is also strictly increasing, bijective and thus continuous.

If A,B ⊆ [0, 1] are dense open sets, and f : A→ B is astrictly increasing bijection, then f extends to a strictlyincreasing bijection f : [0, 1]→ [0, 1].

Page 20: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

The Banach Lemma

1 Introduction

2 preliminaries

3 The Banach Lemma

4 Villani’s lemma

5 Proof of Kakeya’s lemma

6 Next. . .

Page 21: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

The Banach Lemma

Statement

Let λ denote Lebesgue measure on I = [0, 1]. A functionf : I → R is said to satisfy Lusin’s property-N if λ(f(E)) = 0whenever E ⊆ I has λ(E) = 0 (see Natanson).

Lemma (Banach)

A continuous function f : I → R of bounded variation is absolutelycontinuous if and only if it satisfies Lusin’s property-N.

Page 22: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

The Banach Lemma

Proof of Banach’s lemma

First we prove property-N implies absolute continuity.

For simplicity, we assume f is strictly increasing.

The case of strictly decreasing is the same.

The case of bounded variation is true but harder and we skip ithere.

Page 23: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

The Banach Lemma

Proof of Banach’s lemma. . .

Let I denote a finite set of disjoint open intervals in Ii ⊆ I.Let |I| = ∪Ii∈IIi.

Let J = f(I) = {f(Ii)} be the collection of their images.

Recall that ϕ is absolutely continuous if for all ε > 0 there existsδ > 0 so that λ(|I|) < δ implies λ(|f(I)|) < ε (here we use that fis monotone).

Suppose f satisfies property-N but is not absolutely continuous.

Page 24: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

The Banach Lemma

Proof of Banach’s lemma. . .

Let I denote a finite set of disjoint open intervals in Ii ⊆ I.Let |I| = ∪Ii∈IIi.

Let J = f(I) = {f(Ii)} be the collection of their images.

Recall that ϕ is absolutely continuous if for all ε > 0 there existsδ > 0 so that λ(|I|) < δ implies λ(|f(I)|) < ε (here we use that fis monotone).

Suppose f satisfies property-N but is not absolutely continuous.

Page 25: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

The Banach Lemma

Proof of Banach’s lemma. . .

Since f is not absolutely continuous, there exists ε0 > 0 and

I1, I2, I3, . . .

withλ(|In|) ≥ ε0 (1)

for all n = 1, 2, 3, . . . , and

∞∑n=1

λ(|f(In)|) <∞. (2)

Page 26: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

The Banach Lemma

Proof of Banach’s lemma. . .

Let Nn(y) = χ|f(In)|(y) (the characteristic function of |f(In)|).

Then by (1) ∫ϕ(I)

Nn(y) ≥ ε0 > 0 (3)

for all n.

Page 27: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

The Banach Lemma

Proof of Banach’s lemma. . .

LetB = lim sup |In|.

By (2), the Borel-Cantelli lemma (see two slides ahead) impliesλ(B) = 0.

LetA = lim sup |f(In)|.

Note that A = f(B).

Then λ(A) = 0 since f satisfies property-N.

Page 28: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

The Banach Lemma

Proof of Banach’s lemma. . .

Now, y ∈ A iff Nn(y) 6= 0 infinitely often.

It follows that limn→∞Nn(y) = 0 for y ∈ f(I)\A (that is, a.e. y).

By the Dominated Convergence Theorem (M 6214)

limn→∞

∫f(I)

Nn(y)dy = 0,

contradicting (3).

Page 29: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

The Banach Lemma

Aside: The Borel-Cantelli Lemma

Let In be a sequence of measurable sets in [0, 1]. Recall that

J := lim supn→∞

In =

∞⋂n=1

∞⋃k=n

In.

Then x ∈ J if and only if x ∈ In for infinitely many n.

The sets In are independent if

λ(⋂k=1

Ink) =

∏k=1

λ(Ink),

for any n1 < n2 < · · · < n` where ` <∞.

Page 30: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

The Banach Lemma

Aside: The Borel-Cantelli Lemma

Lemma (Borel-Cantelli)

Let In ⊆ [0, 1] be a sequence of measurable sets, and let λ beLebesgue measure (λ[0, 1] = 1).

If∑∞

n=1 λ(In) <∞ then λ(lim supn→∞ In) = 0.∑∞n=1 λ(In) =∞ and the sets In are independent then

λ(lim supn→∞ In) = 1.

We used only the first part (sometimes called the “easy half”).The proof can be an exercise in (M 6214). The second part (calledthe “hard half”) is considered to be part of probability theory.

Page 31: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

The Banach Lemma

Proof of Banach’s lemma: Converse. . .

Suppose f : [0, 1]→ R is absolutely continuous and increasing (theproof works for BV, but is harder).

Let E ⊆ [0, 1] with λ(E) = 0.

Let ε > 0 be given, and choose δ > 0 for f ∈ AC.

Choose a (possibly infinite) set I of disjoint open intervalsIi ⊆ [0, 1] with

E ⊆ |I|,

andλ(|I|) < δ.

(possible since λ(E) = 0).

Page 32: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

The Banach Lemma

Proof of Banach’s lemma: Converse. . .

Let |I| = ∪Ii∈IIi (an open set).

Let J = f(I) = {f(Ii)} be the collection of their images. This isalso a collection of intervals (here we use that f is strictlymonotone).

For any finite I ′ ⊆ I we have that J ′ = f(J ) satisfies λ(|J ′|) < ε(because f ∈ AC).

Thus λ(|J |) ≤ ε, so λ(|J |) = 0 since ε > 0 was arbitrary.

But f(E) ⊆ |J | = f(|I|), so λ(E) = 0. It follows that f satisfisproperty-N.

Page 33: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Villani’s lemma

1 Introduction

2 preliminaries

3 The Banach Lemma

4 Villani’s lemma

5 Proof of Kakeya’s lemma

6 Next. . .

Page 34: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Villani’s lemma

Villani’s lemma

Lemma (Villani)

Let ϕ : [a, b]→ R be continuous, strictly monotone. Then ϕ−1(x)is absolutely continuous if and only if |ϕ′(x)| > 0 a.e..

This lemma appears in a paper by Villani (1984) who says he“believes it is known” but cannot find it in the literature.

We often use this in the case where ϕ({a, b}) = {0, 1} so thatf(x) = ϕ−1(x) satisfies f : [0, 1]→ R is continuous andmonotone. The lemma shows f ∈ AC.

Page 35: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Villani’s lemma

An application

Let f : [0, 1]→ [0, 1] be a piecewise continuous, piecewisemonotone interval map (regarded as a dynamical system).

0.0 0.2 0.4 0.6 0.8 1.00.0

0.2

0.4

0.6

0.8

1.0

Figure: The Renyi-Bolyai map: T (x) = x2 + 2x mod 1.

Page 36: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Villani’s lemma

An application. . .

The map f is called non-singular if λ(f−1(E)) = 0 for any E withλ(E) = 0.

We see that f is nonsingular iff |f ′(x)| > 0 a.e. True forRenyi-Bolyai.

Let ρ(x) ≥ 0,∫ 10 ρ(x)dx = 1, and let µρ(E) =

∫E ρ(x)dx

(µρ = ρλ). We call ρ an invariant density if

µρ(f−1(E)) = µρ(E).

Clearly non-singularity is necessary for the existence of an invariantdensity ρ.

Page 37: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Villani’s lemma

Proof of Villani’s lemma

Let

[c, d] = ϕ([a, b]),

λ=Lebeague measure on [a, b], and

λ′=Lebeague measure on [c, d].

By the Lebesgue decomposition (M 6214) we have

λ′ ◦ ϕ = µ+ σ where µ ⊥ σ.

Here µ << λ is the absolutely continuous part.

Page 38: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Villani’s lemma

Proof of Villani’s lemma

Now we use the following fact (see e.g. Rudin).

|ϕ′(x)| = dµ

dλ(x),

that relates the ordinary derivative ϕ′ to the Radon-Nikodymderivative dµ

dλ (M 6214). Thus

λ′ ◦ ϕ = |ϕ′(x)|λ+ σ where λ ⊥ σ.

Page 39: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Villani’s lemma

Proof of Villani’s lemma

By the Banach lemma, it suffices to show ϕ−1 has property-N(i.e., λ ◦ ϕ−1 << λ).

We show λ(A) > 0 implies λ′(ϕ(A)) > 0.

But

(λ′ ◦ ϕ)(A) =∫A|ϕ′(x)| dλ(x) + σ(A) > 0,

since |ϕ′(x)| > 0 a.e.

We skip the converse since we don’t use it.

Page 40: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Proof of Kakeya’s lemma

1 Introduction

2 preliminaries

3 The Banach Lemma

4 Villani’s lemma

5 Proof of Kakeya’s lemma

6 Next. . .

Page 41: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Proof of Kakeya’s lemma

Kakeya’s Lemma

Lemma (Kakeya)

Let ϕ : [a, b]→ R be continuous, strictly monotone and satisfying|ϕ′(x)| > a > 0 a.e., then |ϕ−1(y)| < 1/a a.e..

Proof:For a continuous monotonic function ϕ, the inverse functiontheorem

(ϕ−1)′(ϕ(x)) =1

ϕ′(x),

holds whenever ϕ′(x) exists and is nonzero (see Wade(M 4239/40)).

Note that ϕ′(x) exists λ a.e.. Let E = {x : ϕ′(x) ≤ a}

By assumption, λ(E) = 0.

Page 42: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Proof of Kakeya’s lemma

Proof. . .

Now ϕ(E) = {y : ϕ′(ϕ−1(y)) ≤ a}

Let F be the set of y so that (ϕ−1)′(y) does not exist.

Since ϕ−1 is monotone, λ(F ) = 0.

It suffices to show λ(ϕ(E) ∪ F ) = λ(ϕ(E)) = 0, because thenλ((ϕ(E) ∪ F )c) = 1, and the inverse function theorem implies

(ϕ−1)′(y) =1

ϕ′(ϕ−1(y))< 1/a for λ a.e. y.

This follows from the next lemma.

Page 43: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Proof of Kakeya’s lemma

Natanson’s lemma

Lemma (Natanson)

Let ϕ : [0, 1]→ R and let 0 ≤ ϕ′(x) ≤ a for x ∈ E. Then

λ∗(ϕ(E)) ≤ aλ∗(E),

where λ∗ denotes Lebesgue outer measure.

Comment: If λ∗(E) = 0 then E is measurable, and this impliesλ(E) = 0. This is what happens in our case.

Page 44: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Proof of Kakeya’s lemma

Proof of Natanson’s Lemma

Fix ε > 0. Choose G open with E ⊆ G and

λ(G) < λ∗(E) + ε.

Also fix a0 > a.

For each x ∈ E there is a sequence hn > 0, hn → 0 so that

limn→∞

ϕ(x+ hn)− ϕ(x)hn

= ϕ′(x) ≤ a.

Page 45: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Proof of Kakeya’s lemma

Proof of Natanson’s Lemma

By choosing n large enough we can assume:

ϕ(x+ hn)− ϕ(x)hn

< a0,

andIn(x) := [x, x+ hn] ⊆ G.

Assume this WOLOG for all n.

Let Jn(x) = ϕ(In(x)) = [ϕ(x), ϕ(x+ hn)].

Page 46: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Proof of Kakeya’s lemma

Proof of Natanson’s Lemma

Now {In(x) : x ∈ E} is a Vitali cover of E (this means theintervals that cover each point x ∈ E are arbitrarily small).

The Vitali Covering Lemma (see Natanson or Rudin, M 6214) saysthere is a sequence of disjoint intervals:

En1(x1), En2(x2), En3(x3), . . .

such that

λ∗

(E\

∞⋃k=0

Ink(xk)

)= 0.

Page 47: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Proof of Kakeya’s lemma

Proof of Natanson’s Lemma

Thus

λ∗(ϕ(E)) ≤∞∑k=0

λ(Jnk(xk)) < a0

∞∑k=0

λ(Ink(xk)).

Since Ink(xk) are pairwise disjoint, we have

∞∑k=0

λ(Ink(xk)) = λ

( ∞⋃k=0

Ink(xk)

),

and⋃∞k=0 Ink

(xk) ⊆ G.

Page 48: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Proof of Kakeya’s lemma

Proof of Natanson’s Lemma

Finally,λ ∗ (ϕ(E)) < a0λ(G) < a0(λ

∗(E) + ε).

The proof is finished by letting a0 → a and ε→ 0.

λ∗(ϕ(E)) ≤ aλ∗(E).

Page 49: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Next. . .

1 Introduction

2 preliminaries

3 The Banach Lemma

4 Villani’s lemma

5 Proof of Kakeya’s lemma

6 Next. . .

Page 50: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Next. . .

Page 51: Absolute continuity vs total singularity - George Washington University

Absolute continuity vs total singularity

Next. . .

References

Kakeya, S., On the generalized scale of notation, Japan J.Math, 1, (1926), 95-108.

Natanson, I. P., Theory of Functions of a Real Variable,Frederick Unger, New York, (1955).

Rudin, W., Real and Complex Analysis, McGraw-HillScience/Engineering/Math, 3rd ed, (1986)

Schweiger, F., Ergodic Theory of Fibred Systems and MetricNumber Theory, Oxford University Press, (1995)

Villani, A. On Lusin’s condition for the inverse function,Rendiconti del Circolo Matematico di Palermo, Serie II, 33,331-335, (1984).

Wade, W. R., Introduction to Analysis, 4th ed, Pearson,(2010)