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    1/17

    6. Integral of simple functions

    135

    Integral of simple functions

    Let

    {X

    A, L} be a measure space, and let E

    E

    A.

    For a measurable set

    A

    and

    x E JR, define

    if x

    =I= 0

    if x = O.

    Since /L E nA) E

    JR ,

    the first

    of

    these is well defined

    as an

    element of

    JR

    for

    all

    x

    E JR - {O}.

    Let f : E --7 JR be a nonnegative simple function, with canonical representation

    n

    f = 2:. fi XEi

    i=1

    6.1)

    where {E1

    E2,

    ,

    En}

    is a finite collection of mutually disjoint measurable sets

    exhausting E and {f l 12, ... , f;,} is a finite collection of mutually distinct, non

    negative numbers. The Lebesgue integral

    of

    a nonnegative simple function f is

    defined by

    Ie

    f x)d/L

    =

    Ie

    fiXEid/L

    = fi/L E

    i

    ).

    6.2)

    This could be finite or infinite.

    I f

    it is finite, then f is said

    to

    be integrable in E.

    Remark 6.1. I f f : E --7 JR is nonnegative. simple. and integrable. the set

    [ f > 0] has finite measure.

    Now let {E

    1

    E2,

    Em}

    be a finite collection of measurable disjoint sets

    exhausting

    E

    and consider the nonnegative. simple function

    m

    f =

    2:. fj XEj '

    j=1

    6.1 )

    where

    / j

    are nonnegative numbers. This is not, in general, in canonical form. Since

    the sets E are mutually disjoint and exhaust

    E

    this would occur if the numbers

    f j are mutually distinct. We put it into its canonical form by setting

    Ei = U{Ej l f j =

    fil,

    i = 1,2,

    ..

    n,

    6.3)

    and then by writing the representation 6.1) by means of the sets E

    i

    .

    From the definitions 6.2) and 6.3), it follows that

    lef

    d

    /L=tfi 2:..

    /L Ej) =

    t / j /L (E j ) .

    1=1

    { j : j= t l J=1

    Thus the integral of a nonnegative simple function is independent of the represen

    tation of f.

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    136 HI. The Lebesgue Integral

    Let

    f.

    g :

    E -

    lit be nonnegative simple functions. If

    I

    g a.e. in

    E,

    then

    L

    x)df l

    L

    i x)dfl

    6.4)

    If both I and g are nonnegative, simple, and integrable,

    L

    al

    +

    f3g)dfl =

    aL

    df l

    + 3L

    dfl

    6.5)

    for all a, f3 E

    lit.

    7 The Lebesgue integral of nonnegative functions

    Let

    I : E - lIt*

    be measurable and nonnegative, and let Sf denote the collection

    of all nonnegative simple functions : E - lit such that

    : S I

    Since == 0 is

    one such function, the class Sf is nonempty.

    The Lebesgue integral of lover E is defined by

    I

    fd f l = sup r d f l

    E ~ S r J

    7.1 )

    This could be finite or infinite. The elements

    E

    Sf are

    not

    required

    to

    vanish

    outside a set of finite measure. For example, if I is a positive constant on a

    measurable set of infinite measure, its integral is well defined by (7.1) and is

    infinity.

    The key new idea of this notion of integral is that the range of a nonnegative

    function

    I

    is partioned, as opposed to its domain as in the notion

    of

    the Riemann

    integra1.

    6

    If

    I

    :

    E - lIt* is

    measurable and nonpositive, we define

    (7.1)-

    A nonnegative measurable function

    I : E - lIt* is

    said

    to

    be

    integrable if

    the

    number defined by (7.1) is finite. For example, if

    fl is

    the counting measure on N,

    a nonnegative function I : N -

    lit

    is integrable if and only if L I n)

    0, there exists an index

    nO

    x) such that

    fn x) 2: t x) - E for all n 2: n(x).

    By the version

    of

    Egorov s theorem as stated in Proposition 2.4, having fixed

    IJ > 0, there exists a set Fry C F such that JJ-(F - Fry) ::: IJ and this inequality

    holds uniformly in

    Fry;

    i.e., for every fixed

    E

    >

    0, there exists

    n

    such that

    fn x) 2: t x) - E for all n 2: n and for all x E Fry.

    7P. J l atou, Series trigonometriques et series de Taylor, Acta Math., 30 (1906), 335-400.

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    138 III. The Lebesgue Integral

    From this, for

    n ::::: n

    e

    ,

    r

    dj1.:::::

    r

    j ~ d f l : : : : :

    r

    S- -

    E)df.l.

    J

    hi

    JF'I

    i -dj1. -i-F,; ~ d f l - Ej1.(F)

    ::::: [ S-df.l. - 1] sup S -

    Ef.I.(F).

    Since

    j1.(F)

    is finite, this implies

    liminf

    [j;,dj1.

    :::::

    [S-dj1.

    for all integrable

    S

    E

    Sf

    (8.2)

    If S

    is not integrable, it equals some positive number 8 on a measurable set

    F e

    of

    infinite measure. Having fixed

    E

    (0, 8), set

    Fn

    = {x E ElfJ x) :::::

    8 -

    for all

    j

    n}.

    From the definition

    of

    lower limit Fn C

    Fn+l

    and F e U

    Fn.

    Therefore,8

    From this,

    lim inf r

    n

    dj1.:::::

    lim inf r t;,dj1.::::: 8 - E) lim inf f.I.(Fn).

    J JF

    Thus in either case, (S.2) holds for all ESt

    D

    In the conclusion 8.1)

    of

    Fatou s lemma, equality does not hold in general. For

    example, in

    lR

    with the Lebesgue measure, the sequence

    {

    I

    forxE[n, n+l)J,

    f,, x)

    = .

    o

    otherwIse

    satisfies

    S.l)

    with strict inequality. This raises the issue

    of

    when

    S.I)

    holds with

    equality or, equivalently, when one can pass to the limit under the integral.

    Theorem

    8.2 (monotone convergence). Let {fn} be a monotone increasing se-

    quence

    of

    measurable, nonnegative functions in

    E;

    i.e.,

    O.:s

    fn x).:s fn+l(X) for all

    x E and foralln E N.

    Then

    l m [

    f dj1.

    =

    lim fndf.l..

    H

    Sec (3.3) of Proposition 3.1 of Chapter II.

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    9.

    Basic properties of

    the

    Lebesgue integral 139

    Remark 8 1 The integrals are meant in the sense

    of

    (7.1). In particular, both sides

    could be infinite.

    Proof

    o f Theorem 8.2. The sequence

    Un}

    converges for all x E E to a measurable

    function f E --* JR . Therefore, by Fatou s lemma,

    9 Basic properties o the Lebesgue integral

    Proposition

    9 1

    Let

    f,

    g : E

    --*

    R

    be

    integrable. Then

    for

    all

    a,

    f

    E

    R

    f

    f g a.e. in

    E

    then

    l fdJ-L ~

    19dJ-L.

    l dJ-L1 ::: l l f ldJ-L.

    If E

    is a

    measurable subset of

    E then

    D

    (9.1)

    (9.2)

    (9.3)

    (9.4)

    Proof

    For

    a

    0, denote by

    a s

    the collection

    of

    functions

    of

    the form

    al;,

    where

    l;

    E

    Sf f

    a 0 and f 0, then aSf =

    Sexf

    Therefore,

    { afdJ-L=

    sup (

    rydJ-L=a

    sup

    , l ;dJ-L=a , fdJ-L.

    JE

    I} Saf

    JE

    ~ S f

    E E

    Similarly,

    if a

    0 and f is integrable and

    of

    variable sign, then (9.5) continues to hold in

    view of (7.2) and the decomposition

    A similar argument applies if a < 0, and we conclude that (9.5) holds true for

    every integrable function and every

    a

    E

    lR.

    Therefore, it suffices to prove (9.1) for

    a = f 3 = l .

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    140 III The Lebesgue Integral

    Assume first that both

    f

    and g are nonnegative. There exist monotone increasing

    sequences

    of

    simple functions

    { ~ }

    and

    { ~ }

    converging pointwise in

    E

    to

    f

    and

    g respectively. By the monotone convergence theorem,

    e f

    g dfJ- =

    lim e

    ~ n

    n ) d f J -

    = lim e ~ n d f lim e ~ n d f -

    = e fdfJ- e gdfJ-.

    Next, we assume that

    f

    0 and

    g

    :s

    O.

    First, we observe that f

    g

    is integrable

    since I f gl :s If I

    gl

    From the decomposition

    f g +

    -

    g

    =

    f g)-

    f

    and 9.1) proven for the sum of two nonnegative functions,

    This and the definition 7.2)

    proves 9.1) for f 0 and g

    :s

    O.

    f

    f

    and

    g

    are integrable with no further sign restriction,

    To prove 9.2), observe that from f

    - g

    0 and 9.1),

    Inequality 9.3) follows from 9.2) and

    If :s f

    :s

    I f

    I

    Finally, 9.4) follows from 9.1) upon writing

    f

    = fXE fXE-E

    D

    orollary

    9.2.

    Let f

    : E

    JR

    be integrable and let

    E

    be

    of

    inite measure.

    Then

    fJ- E) inf f (x):s [ fdp,:s

    p,(E)

    sup f(x).

    XEE

    JE

    XEE

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    10

    Convergence theorems 141

    1

    Convergence theorems

    The properties

    of

    the Lebesgue integral permit one to formulate various versions

    of

    Fatou s lemma and

    of

    the monotone convergence theorem.

    For example, the conclusion

    of

    Fatou s lemma continues to hold

    ifthe

    functions

    fn are of variable sign, provided they are uniformly bounded below by some

    integrable function

    g

    Proposition 10.1. Let

    g

    :

    E

    ~

    be integrable

    and

    assume that fn

    :::

    g a.e. in

    E

    for

    all n E

    N

    Then

    liminf

    e

    fnd/-L :::

    lel iminf

    fnd/-L.

    Proof

    Since

    fn - g)

    :::

    0,

    the sequence

    Un - g}

    satisfies the assumptions

    of

    Fatou s lemma. Thus

    liminf

    e

    fnd/-L :::

    e

    gd/-L

    e

    liminf

    fn

    - g)d/-L.

    o

    Proposition 10.2. Let Un} be a sequence of nonnegative, measurable functions

    on E Then

    Proof The sequence {L:7= fi} is a monotone sequence

    of

    nonnegative, measur

    able functions.

    0

    Remark 10.1.

    t s not required that the fn be integrable or that

    L:

    fn be integrable.

    The integral ofmeasurable, nonnegative functions, finite or infinite, is well defined

    by (7.1).

    Theorem 10.3 dominated convergence).

    Let Un} be a dominated

    and

    conver-

    gent sequence

    of

    ntegrable functions in E, i.e.,

    lim fn x)

    = f x)

    for all x E

    E,

    and there exists an integrable function g

    :

    E ~ such that

    Ifni :::: g a.e. in E for all n EN.

    Then the limit function f

    :

    E ~ is integrable and

    lim

    e

    fnd/-L

    =

    e

    lim

    fnd/-L.

    Proof

    The limit function f is measurable, and by Fatou s lemma,

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    142

    III. The Lebesgue Integral

    Thus I is integrable. Next,

    g-./;,)::::O

    and

    f,,+g)::::O

    for all n EN.

    Therefore, by Fatou s lemma,

    L

    df l

    :::

    lim inf

    L/;,

    lim sup

    L

    dfl :::

    Ldfl

    D

    Absolute continuity o the integral

    Theorem 11 1 (Vitali

    9

    ). Let E be measurable, and let

    I :

    E

    -- ]]{

    be integrable.

    For every

    E

    > O.

    there exists

    8

    >

    0

    such that

    lor

    eve }' measurable subset [;

    c

    E

    olmeasure less than

    8.

    Proof We may assume that I O For = 1. 2 consider the functions

    1

    -

    {/ X)

    1

    n

    Since {f,,} is increasing,

    if I x) < n.

    if

    I (x) :::: n.

    Having fixed E > 0, there exists some index n

    E

    such that

    { In[dfl > { fdf l ~ E

    J J 2

    Choose 8

    =

    - 2 .

    Then for every measurable set [; C

    E

    of

    measure less than

    8,

    1[

    2 Product o measures

    D

    Let {X.

    A.

    fl}

    and

    {Yo

    B.

    v}

    be two measure spaces. Any pair

    of

    sets A C X and

    eY

    generates a subset A x B of the Cartesian product X x Y called a

    generalized rectangle.

    YG.

    Vitali. SuI Ie funzioni integrali. Alii Rend. Accad. Sci. Torino.

    40

    (1905). 1021-1034.

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    12 Product of measures 143

    There are subsets o

    X

    x Y) that are not rectangles. The intersection o any two

    rectangles is a rectangle by the formula

    The mutual complement o any two rectangles, while not a rectangle, can be written

    as the disjoint union o two rectangles by the decomposition

    A2

    x

    B2)

    AI

    x BI) =

    { A2

    AI) x

    B2}

    U

    AIn 2)

    x

    B2

    BI)}

    .

    Thus the collection

    R

    o

    all rectangles

    is

    a semialgebra.

    O

    f A E

    A

    and B E B the rectangle A x B is called a measurable rectangle. The

    collection o all measurable rectangles

    is

    denoted by Ro. By the previous remarks,

    Ro

    is a semialgebra.

    Since X

    x

    Y E

    Ro

    such a collection forms a sequential covering o X

    x

    Y).11

    The semialgebra Ro can be endowed with a nonnegative set function by setting

    A A x

    B)

    =

    fL A)v B)

    12.1 )

    for all measurable rectangles A x B.

    Proposition 12 1

    Let

    { n

    X

    Bn}

    be a countable collection

    of

    disjoint measurable

    rectangles whose union is a measurable rectangle A x B. Then

    Proof

    For each

    x

    E

    A

    B

    =

    U{B j l x ,

    Y

    E A j

    x

    Bi;

    Y

    E B}.

    Since, for each

    x

    E A fixed, this is a disjoint union,

    Integrating in dfL over A and using Proposition 10.2 now gives

    o

    Thus A is unambiguously defined since the measure o a measurable rectangle

    does not depend on its partitions into countably many pairwise-disjoint measurable

    rectangles.

    Proposition 12 1 also implies that A is a measure on the semia1gebra

    Ro.

    There

    fore, Acan be extended to a complete measure fL x v) on X x y), which coincides

    with A on

    Ro.12

    IOSec

    Section 9 o Chapter 11

    II See Section 4 o Chapter II.

    12See Theorem 1

    J . J o

    Chapter II.

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    44

    Ill. The Lebesgue Integral

    Theorem 12 2 Every pair {X, A, Id and {f, E, v} ofmeasure spaces generates

    a complete product measure space

    { X

    x

    Y),

    A x

    3 ,

    IL x

    v)},

    where (A x 3 is a

    5

    -algebra containing Ro and

    IL

    x v is a measure on (A x 3

    that coincides with 12.1) on measurable rectangles.

    3 On the structure

    o

    A x B)

    Denote by A x

    3)0

    the smallest 5-algebra generated by the collection of all

    measurable rectangles. Also set

    Ra =

    {countable unions of elements of

    R

    o

    },

    RaJ

    = {countable intersections of elements of Ra

    }.

    By construction,

    For each

    E c X

    x y , the two sets

    E,

    =

    {vl x,y)

    E

    E)

    fora

    fixed

    x

    EX

    X

    E, =

    xl x,y) E

    E) forafixedy

    E

    Y

    are, respectively, the X -section and the Y -section of

    E.

    Proposition 13 1

    Let E

    E (A x 3)0

    Then

    for

    every y

    E

    Y, the Y -section E

    y

    is

    in A, and for every x

    E

    X, the X -section E, is in E.

    Proof The collection F of all sets E E

    (A

    x E such that Ex E E for all x E X

    is a 5-algebra. Since F contains all the measurable rectangles, it must contain the

    smallest 5-algebra generated by the measurable rectangles. D

    Remark 13 1 The converse is false as there exist nonmeasurable sets E

    c

    X x

    Y) such that all the

    x

    and v sections are measurable. An example is in Section 13.5

    of the Problems and Complements.

    Remark 13 2

    There exist

    IL

    x v)-measurable rectangles

    A

    x

    B

    that are not

    measurable rectangles. To construct an example, let Ao

    C

    X not be IL-measurable

    but be included into a measurable set of finite IL-measure. Also let Bo

    E

    E be of

    zero v-measure. The rectangle Ao x

    Bo

    is IL x v)-measurable and has measure

    zero.

    For

    each c

    >

    0, there exists a measurable rectangle

    Rc

    containing Ao x

    Bo

    and

    of

    measure less than c. Therefore, Ao x

    Bn

    is

    IL

    x v)-measurable by the

    criterion of measurability of Proposition 10.2 of Chapter II.

    Remark 13 3

    This example implies that Proposition 13.1 does not hold

    if A

    x

    3)0 is replaced by

    A x

    3 . In particular, the inclusion

    A x

    3 0

    c

    A

    x

    3

    is strict.

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    13. On the structure of A x B 145

    Proposition 13 2

    Let E E

    Ra/i

    be

    of

    finite measure. Then the function x ---?

    v

    Ex)

    is J-t-measurable

    and

    the function

    y

    ---?

    J-t(E

    y) is v-measurable. Moreover,

    ]

    XEd(J-t

    x v)

    = [

    v Ex)dJ-t

    = [

    J-t Ey)dv.

    Xxy )

    }x

    }y

    Proof

    The statement

    is

    obvious

    if

    E is a measurable rectangle.

    I f

    E

    E R

    a

    , it

    can

    be decomposed into the countable union

    of

    disjoint measurable rectangles En. The

    functions

    and

    are measurable, and by monotone convergence,

    ]

    XEd(J-t x

    v)

    ] XE d(J-t x

    v)

    Xxy )

    Xxy)

    L x v En,x)dJ-t

    =

    L i -t En,y)dv

    x

    Lv E n,x)dJ-t

    =

    i

    LJ-t En,y)dv

    x v E

    x

    )dJ-t

    i

    -t Ey)dv.

    I f E E

    Ra/i,

    there exists a countable collection {En} of elements

    of Ra

    such that

    En+l

    C

    En and

    E = n

    En. The functions

    x

    ---?

    v Ex)

    lim

    v En,x)

    and

    Y

    ---?

    J-t(E),)

    =

    limJ-t En.y),

    are measurable. Since

    J-t x v) E) lE be measurable and nonnegative. Then the measurability

    statements

    in 14.1)

    and the double-integral formula

    14.2)

    hold. The integrals

    in 14.2)

    could be either finite or infinite.

    Proof

    The integrability requirement in the Fubini theorem was used

    to

    insure the

    existence

    of

    a sequence

    U; }

    of

    integrable functions each vanishing outside a set

    of

    finite measure and converging to f. The positivity

    of f

    and the a-finiteness in

    the Tonelli theorem provide similar information. 0

    If

    f

    is integrable in ~ x v . then Fubini s theorem holds and equality occurs

    in 14.2). f

    f

    is not integrable, then the left-hand side of

    04.2)

    is infinite. Tonelli s

    theorem asserts that in such a case, the right-hand side also is well defined and is

    infinity, provided x \I) is

    a

    -finite.

    In particular. Tonelli s theorem could be used to establish whether a nonnegative.

    measurable function

    f :

    (X x

    Y)

    c>

    JR

    is integrable through the equality

    of

    the

    two right-hand sides of

    4.2).

    The requirement that x \I) be a-finite cannot be removed. as shown by the

    example in 14.5 of the Problems and Complements.

    5 Some applications o the Fubini Tonelli

    theorem

    15.1 Integrals in

    terms

    of distribution functions. Let

    f

    : E

    c>

    JR be mea

    surable and nonnegative. The distribution function of f relative to E is defined

    as

    Jl{+ 0) t ----+ ~ [ f > tl .

    15.1)

    This is a nonincreasing function of

    t

    and if f is finite a.e. in E, then

    lim

    ~ [ f > t]

    =

    0

    unless

    ~ [ f > t] 00.

    1- 00

    15.2)

    f

    f

    is integrable, such a limit can be given a quantitative

    fom1.

    Indeed,

    15.3)

    15L. Tonelli. Sull integrazione per parti, Atti Accad. No;. Lincei (5). 18-2 1909).246-253.

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    15.

    Some applications of the Fubini-Tonelli theorem 149

    Proposition 15 1 Let

    {X, A, I.t} be a-finite and let f : E

    -- jR*

    be measurable

    and nonnegative. Also let v be a a-finite measure on

    jR+

    such that v [O, t)) =

    v [O,

    tl). Then

    l

    v [O,

    f])dJJ- =

    fooo

    JJ- Lf

    >

    t])dv.

    15.4)

    In

    particular, ifv [O,

    t]) =

    t

    P

    for some p

    > 0,

    then

    l5.4)p

    where

    dt

    is the Lebesgue measure on jR+.

    Proof

    The function

    f

    : E -- jR*, when regarded as a function from E x jR+ into

    jR* , is measurable in the product measure JJ- xv). Likewise, the function g t) =

    t

    from

    jR+

    into jR*, when regarded as a function from

    E

    x

    jR

    into jR*, is measurable

    in the product measure JJ- x v). Therefore, the difference

    f

    t is measurable in

    the product measure JJ- x v). This implies that the set

    Lf - t

    > 0] =

    Lf

    >

    t]

    is measurable in the product measure JJ- x v). Therefore, by the Tonelli theorem,

    foOO

    JJ Cff

    > tl)dv =

    lC O

    l

    X[f>tjdJJ-) dv

    =

    l

    foOO Xlf>t]dV)

    dJJ

    =

    l

    fofdV) dJJ

    =

    l

    v [O,

    f])dJJ-.

    o

    Both sides of 15.4) could be infinity and the formula could be used to verify

    whether v [O, f]) is t-t-integrable over

    E.

    In the next two applications in Sections 15.2 and 15.3, the measure space

    {X A,

    JJ-}

    is jRN with the Lebesgue measure.

    15 2 Convolution integrals A measurable function

    f

    from

    jRN

    into jR*, when

    regarded as a function defined on

    jR2N,

    is measurable. Indeed, for every c

    E R

    the set

    Lf

    > c]

    X

    jRN is a measurable rectangle in the product space. This implies

    that the function

    jR2N

    :3

    x,

    y)

    ----+ f x -

    y)

    is

    also measurable with respect to the product measure. Indeed, the set

    { x, y)

    E jR2N

    x y)

    > c)

    coincides with the measurable rectangle

    Lf

    > c]

    X

    jRN in the rotated coordinates

    =

    x -

    y.

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    ISO

    III.

    The Lebesgue Integral

    Given any two nonnegative measurable functions f, g :

    m;,N

    --+ m;, , their

    con-

    volution

    is defined

    as

    x

    - f g) x)

    = f .

    g y) f x

    -

    y)dy.

    llR

    15.5)

    Since

    f

    and

    g

    are both nonnegative, the right-hand side, finite or infinite, is well

    defined for all x E

    m;

    N .

    Proposition 15 2 Let f and g

    be nonnegative

    and integrable in m;,N. Then

    f

    g) x) isfinitefora.e.

    x

    E m;,N,

    thefunction

    f g

    is integrable in

    m;,N

    and

    f

    f

    g)dx

    ::s

    f

    f

    dX

    )

    f

    gdX) .

    lR I

    llR.v

    IIA

    v

    15.6)

    Proof The function

    (x.

    Y --+ K(y) f (x - y) is nonnegative and measurable with

    respect to the product measure. Therefore, by the Tonelli theorem,

    j

    f,. g :v)f x

    -

    y)dxdy

    =

    f .

    f , g y) f x -

    Y)dX) dy

    llR-\

    llR 1;R\

    = lv f

    dX

    ) lv gdX) . 0

    The convolution of any two integrable functions

    f

    and g is defined as in 15.5).

    Since

    Ig y)f x -

    y)1

    ::s

    Ig y)ll f x

    -

    y l.

    the convolution f g) is well defined as an integrable function over

    m;,2N.

    15 3 The Marcinkiewicz integral

    Let E be a nonvoid set in

    m;

    N and let 0

    (x)

    denote the distance from x to E; i.e ..

    OE X)

    = inf Ix

    -

    zl.

    ~

    By definition, 0E

    (x)

    =

    or all x E E.

    Lemma 15 3

    Let

    E be a nonemp v

    set

    in m;,N. Then

    the distance

    function x

    --+

    o x) is

    Lipschitz continuous

    with

    Lipschitz

    constant 1.

    P r o ~ f Fix x and

    y in m;,N

    and assume that

    (5 E

    x) ::::

    (5E

    v). From the definition

    of

    o (Y), having fixed E

    >

    0, there exists z E E such that

    Then estimate

    OEC.V) :::: Iy - z l - E.

    o :s

    0E X)

    - OEc V) ::s inf Ix - zl -

    Iy

    - z l

    +

    E

    ~

    ::s Ix

    - z l - Iy - z l

    + E ::s Ix

    - ) 1

    + E.

    The conclusion follows since E

    >

    0 is arbitrary.

    15.7)

    o

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    16. Signed measures and the Hahn decomposition 151

    Let

    E

    be a bounded, closed set in ][tN. Fix a positive number A and a cube Q

    containing

    E.

    The Marcinkiewicz integral relative to

    E

    and A is the function

    1

    8A

    v)

    ][tN

    3 X ME.A X)

    =

    E .

    NH dy.

    Q x

    - yl

    15.8)

    The right-hand side is well defined as the integral

    of

    a measurable, nonnegative

    function.

    Proposition 15 4 Marcinkiewicz

    I6

    ). The Marcinkiewicz integral ME.A X) isfi-

    nitefora.e.

    x E

    E

    Moreover, thefunction x

    -+

    ME.A X) is integrable

    in E

    and

    where

    WN

    is the measure

    of

    the unit sphere

    in ][tN.

    Proof Since 8E Y) = 0 for all y E E, by the Tonelli theorem,

    1

    E.A X)dx

    =

    1 8 ~ ( Y ) 1 dx N+A) dy

    E Q E x

    - yl

    1

    A

    1 dx

    )

    DE Y) N dv.

    Q E t. x - yl

    A

    .

    For each fixed y E Q - E) and x E E, since E is closed, we estimate

    Therefore, for each fixed

    y

    E Q - E ,

    1

    dx