A NNALI DELLA
S CUOLA N ORMALE S UPERIORE DI P ISA Classe di Scienze
J AAK P EETRE
Pointwise convergence of singular convolution integrals
Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 3
esérie, tome 20, n
o1 (1966), p. 45-61
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CONVOLUTION INTEGRALS by
JAAK PEETRE0.
Introduction.
This article is in a way of survey character. What we
attempt
to dois to relate known work on
singular
convolutionintegrals
in jR~ associated with the namesCalderon, Zygmund, Michlin, Hormander,
Cotlar and many others.Although
we obtain nostrictly
new results wehope
that this inve-stigation
will have somevalue, since,
up to ourknowledge,
not much hasbeen done
previously
in this sense, at least not inprint.
We shall in the first
place
be concerned withpointwise
convergence(almost everywhere,
a.e.),
one of ourpoints being
thatpointwise
conver-gence can be derived
fairly easily directly
from norm convergence, in facta rather weak form of
it, using only
ratherstraight
forward estimates and the maximal theorem ofHardy-Littlewood,
thusroughly Lebesgtie’s
theoremon differentiation of
integrals.
We believe that this methodmight
be usefulalso in other more
complicated
cases.To fix the ideas let us start with the
simple
case of the Hilbert transform on the real line .R = Ri :There are
basically
two ways ofinterpreting
lim :a)
Norm convergence8-0
(usually
theL, norm), b)
Pointwise convergence a. e. The classical results in this direction are thefollowing:
In casea)
convergence in the.Lp
normholds for every
f
E.Lp provided
1p
oo. Inparticular
.g maps intoLp
Pervenuto alla Redazione il 10 Settembre 1965.
(M. Riesz). For p
=1 this isobviously
not true but thefollowing
weakersubstitute holds :
H maps Lp
into the weak Marcinkievicz spaceLi (Kolmogo-
rov).
In caseb)
convergence a. e holds forevery f E Lp provided
1p C o0 (Plessner
andothers).
Our thesis is thus that the result in caseb)
followfrom the results in case
a) by
theintermediary
of the maximal theorem.This is
particularly simple
if 1p
oo. Then our basic idea is to consider the differenceWe show that this is a convolution with a « nice » function ae, « nice >>
from the
point
of view of the maximaltheorem,
and thus tends to 0 a. e.On the other hand
.gf’ (,x)
tends toHf (x)
a. e.,again by
themaximal theorem. This
simple proof might
also have some didacticvalue. It is also
possible
tomodify
theproof
so as to cover the casep
=1,
but then it is not anylonger
soelementary,
andby
the way very close to known ones ; see, inparticular,
Cotlar[5], chapter
III.The
theory
of the Hilbert transform as outlined above can be extended in several directions. In the firstplace
comes the so-calledCalderon-Zygmund
transform which is convolution with a function a(x)
inRn, homogeneous
ofdegree - n
and withvanishing spherical
meanvalues(see [3], [4], [20]).
It is thestudy
of this case(« homogeneous
case») and,
inparticular,
the case of still moregeneral
functions a(x)
which will be theobject
of this article.The
plan
is thefollowing.
In Section 1 we collect somepreliminaries mainly
concerned with the maximal theorem. In Section 2 we thengive
the
proof
ofpointwise
convergence a. e. in the case of the Hilbert trans-form,
as outlined above. Thisproof
we then(Section 3)
extend to the caseof convolution
by
ageneral
fucntion a(x)
in Rn. We find thatpointwise
convergence a. e. holds if a
(x)
satisfies certainHypothesis 0,
1 and 2 ofwhich
Hypothesis
2 is thedeeper
one. In Section 4 we discuss thisHypothesis
2 and variants ofit, Hypothesis
2’ and 2" - the latter of interest of its on because it isprecisely
the condition for norm convergencegiven by
Hormander[7]
- and relate them inparticular
to other condi-tions
given by
Cotlar[5], [6]
on one hand and Michlin[10],[11],
Hormander[7]
on the other hand.Finally (Section 5)
we show thatHypothesis
2’(stronger
thanHypothesis 2) actually implies
convergence a. e. also when~ =1. As we said above in this case our method is close to that of Cotlar
[5].
We remark that for theunderstanding
of this Section thereading
of Section 4 is not necessary.In conclusion I wish to thank Guido Weiss and Sven
Spanne
forseveral
helpful suggestions
in connection with this work.1.
Some preliminaries.
If 1
~ ~ ~=
oo andf
is a measurable function in Rn let us setand
we shall write
IlfIIL¡-)
Denoteby -L,
andLp
respec-tively
thecorresponding
spaces.They
are both linear. Moreover it is well- known is a norm and thatLp
iscomplete
in this norm(F.
Riesz-Fischer
theorem).
p
is no norm but
only
aquasi-norni (i.
e. inplace
of theordinary triangle inequality
we have the weakerinequality []
but not for I it is
equivalent
to a norm. In any caseLp
iscomplete.
We note also that
f E Lp
orJ~
if andonly
if orEl respectively.
Let B be a Banach space A
mapping
T of jE7 into A =Zp
orJ~
issaid to be
quasi-linear
iffor some lc and all
f,
g, c, and bounded iffor some C.
Consider a
family
ofquasi-linear mappings T~
i~ > 0,
from .E into A.We define
(maximal function)
LEMMA. 1.
Suppose M
isbounded,
asmapping from
.E intoA,
and11Ef(x)
converges a. e. in some dense subsetof
E. Then converges a. e.in the whole
of
E.Next we recall
LEMMA 2
(Marcinkiewicz interpolation theorem). Suppose
T is a boundedquasi- linear mapping
intoLpo
andfrom Lp,
intoLpl’
1 1p1
IV N
c 00. Then T is also bounded
from Lp
intoLp
orfrom Lp
intoLp for
any pwith 1
We define also
(Hardy.Littlewood
maximalfunction)
(volume
of the unitsphere)
It is
obviously quasi-linear.
LEMMA 3
(Hardy-Littlewood
maximaltheorem). mapping from Lt
into15t and, thus by
Lernma 1from Lp
intoLp
or intoFinally
we defineObviously,
sinceLEMMA 4. The norm
11
all*
isequivalent
to thefollowing
one :We remark that it follows from Lemma 3 and Lemma 4 that Lemma 1 can be
applied
toprovided
For the
proof
of Lemma 1-3 see e. g. Cotlar[5], chapter
III. For the oneof Lemma 4 see e. g. Alexits
[1],
p. 240-246.2. The case
of
the Hilberttransform,
1-P
oo.Consider thus
again
We assume that it is known that lim exists in some sense, say, distribu-
e-O
tion sense, for every
f E Lp
and defines a bounded linearmapping
H fromLp
intoLp (weak
form of M. Riesztheorem). (Here
as in the rest of this and thefollowing
Section we take 1 poo.)
~Te claim that for everyf E Lp
holdswhere
and
Indeed this is
certainly
true whenf
is a « smooth >>function,
say, continu-ously
differentiable and withcompact support,
so thegeneral
case followsby
adensity argument.
We want to evaluate thenorm || a 11*.
First
let x I C E,
Then We may writefor and moreover holds
Hence
by
the mean valuetheorem,
since(p’
is boundedNext
>
8. NowBut
Hence, since 99
isbounded,
From
(1)
and(2)
we conclude thatHence by
Lemma 4where the last bound is
independent
of s. Thus we obtainSince the
mapping
definedby
theright
hand side isquasi-linear
andby
Lem-ma 3 bounded from
Lp
intoZp
it followsby
Lemma 1 that con-verges a. e. to
Hf(x)
for everyfE Lp .
Thus we have proven Plessner’stheorem in this
special
case.REMARK 1.
By Lebesgue’s
theorem on dominated convergence it fol- lows now also that converges in theE,
norm to i. e. thestronger
form of M. Riesz’ theorem.3.
The general
case, 1p
00.We now consider
r
where a (x)
is anarbitrary >> function.
We assume theanalogue
ofM. Riesz’
theorem,
i. e. that lim existsin,
say, distribution sense and defines8-0
a bounded linear
mapping
H fromLp
into.Lp . (We
recall that 1p
ooby assumption.)
Then holdsagain
where now
and
We assume
Hypothesis
Then
by
theargument
if Section 2 weget
If we also assume
Hypothesis
1we thus obtain
By
theargument
of Section 2 we alsoget
or
I
a,if we set
Let us now also assume
n 1 f8
Then it follows from
(3)
and(4)
thatand as in Section 2 we obtain thus the
following
THEOREM 1. Assicme that H is a bounded linear
mapping from Lp
intoLp
1 p oo, and assume alsoffypothesis 0,
1 and 2. Thenfor
every1
p
convergences a. e. toHf (x).
REMARK 2.
By Lebesgue’s
theorem on dominated convergence it fol- lowsagain
that converges in theL,
norm to4.
Discussion of
theprevious hypotheses.
Hypothesis
0 and 1 arequite
easy toverify
inpraxis.
Therefore Weshall concentrate upon
Hypothesis
2. We shallmainly
work with the fol-lowing (obviously) stronger
one.Hypothesis
2’.11 be,
y(x) 1/* C C
ifI y ~ ~ E .
We shall now show that
Hypothesis
2’ is fulfilled in several morespecial
situations. We shall here use,though
this is of course notessential,
some ideas of the abstract
theory
ofinterpolation
spaces(see
inparti-
cular
[13]
as well as referencesgiven there).
a’. Let us introduce the
(semi-)norms
and
We
get
at onceas well as
where we have made use of
If we set
(see [13])
it follows that
Taking
the sum weget
We have thus proven THEOREM 2’.
If
then
Hypothesis
2’ isfulfilled.
In the
homogeneous
case, where co(x)
is a functiondefined
=1 only,
it is not hard to see that this is the consequence of anordinary
Dini condition for m(x),
i. e.precisely
the case consideredby
Calderon andZygmund [3].
We
interrupt
thepresentation by temporarily considering
thefollowing (obviously)
weaker.REMARK 3. This
Hypothesis
2" has also interest of its ownbecause,
as Hörmander
[7] (see
also Benedek-Calderon-Panzone[2],
J. Schwartz[16]
where the vector valued case is
treated)
hasshown,
itimplies
that g isa bounded linear
mapping
fromL1 into L1
andthus, by
Lemma2,
fromLp
into 1p
oo,provided
this latterproperty
holds for some fixedI say, po = 2. Hormander’s
proof
which is adevelopment
of the onegiven by Calderon-Zygmund [3]
is thehomogeneous
case,depends
in anessential way on a
covering
lemmagiven by
theseauthors,
whichagain
goes back to F. Riesz. For the Hilbert transform there are,
apart
fromseveral
complex
variableproofs, including
theoriginal
one of M.Riesz,
also some rather
elementary
real variable ones(see
Stein-Weiss[17],
Weiss[18],
0’ Neil-Weiss[12],
Loomis[9]).
On the otherhand, according
to anidea of Calderon and
Zygmund [4],
thehomogeneous
case in several varia- bles can be reduced to the one dimensional case, as a matter of fact under the even weakerassumption a (x)
E Llog
L. Such weak conditions are of course excluded from thepresent
discussion.We now
give
the discussion ofHypothesis
2"analogous
to the inter-rupted
one forHypothesis
2’a". Let us introduce the
(semi-)norms
and
(Note
that Then we haveTHEOREM 2".
If (Dini condition)
thenHypothesis
2"v
is
fulfilled.
The
proof
isparallel
to the one of Theorem 2’. Therefore we shall omit it. Notethat,
in thehomogeneous
case, we thus obtain norm convergence under weakerassumptions
than inCalderon-Zygmund [3].
b". In a number of
publications (see [5], [6])
Cotlar has considered the case when a(x)
admitsdecomposition
of thetype (Cotlar decomposition)
where
and
(or, slightly
moregenerally,
with 0 a1,
The
following
result holds true.THEOREM 3".
If
a admits a Cotlardecompositiorc of
the abovetype
thenHypothesis
2" isful, filled.
We
only
consider thestronger
case of(7). Indeed,
in this case, weeasily
convince ourselves that
and
Applying
this to a(x)
= Uj(x)
weget
where has a similar
meaning (with respect
to 1aej(x))
asb,, y (x) (with respect
to ac~x)). Finally
upontaking
the sum weget
where the last bound is
independent
of 8REMARK 4. We note also that under the some
assumptions
one canprove, as was done
by Cotlar,
that g is a boundedmapping
fromL2
intoL2 .
Thusby
Remark 3 g is a boundedmapping
fromLp
into.Lp ,
1p cxJ.
’REMARK 5". We do not know what is the
precise
relation betweenour Dini condition and the Cotlar
decomposition.
However it is easy to show at least that cY, implies
that a(x)
admits a Cotlardecompo- sition, simply by taking
where
(x)
is a suitablepartition
ofunity.
Note also that the Cotlardecomposition
is somewhat related tointerpolation. Namely (5), (7)
expressprecisely
that a E(L1, I x I
’ while as(5)~ (8)
say that2
Here we use the notation of
[13],
denotes.~~
withrespect
to theweight
function w(x).
c". Michlin
[10], [11]
hasgiven
conditions on the Fourier transform a(5)
of a
(x).
Hisresult,
which goes back to a similar result in theperiodic
case due to
Marcinkiewicz,
was latersimplified
and somewhat extendedby
Hormander
[7].
Toput
this in ourpresent
framework we establishTHEOREM 4".
Suppose
thatfor
some 2 Then a(x)
admits a Collardecomposition.
(One
can also consider the case of fractionalN,
see[8], [14]).
Let usassume
slightly
more :2~ ~> 2013 ’)- 1’
Then we canactually
work with the2
stronger
form(7). (The general
case can be treated in a similar wayusing (8)
inplace
of(7).)
We define(x) by
where yj (~)
is apartition
ofunity
such thatIt is clear that
(5)
holdsand,
if wechoose yj (~) depending on 1$1 I only
also
(6). By
a(special
caseof)
well known theorem of S. Bernstein(see Zygmund [19],
vol1,
p.240-241,
for the one-dimensionalperiodic
case, see also[14]
for thegeneral case)
we haveTaking
account of theassumptions
on a(~)
and the aboveproperties
of1Jlj
(~)
also(7)
follows when(9)
isapplied
to a = xuj and a =uj respectively.
After this detour on the
Hypothesis
2" it is now easy tocomplete
the
interrupted
discussion ofHypothesis
2’.b’. We consider
again functions a(x) admitting
adecomposition
oftype (Cotlar decomposition)
where as
previously
but now
(or, slightly
moregenerally,
with 0 a1,
We have
THEOREM
(3’). If a
admits a Cotlardecomposition of
the abovetype
thenHypothesis
2’ isfulfilled.
The reader should have no difficulties in
supplying
the details of theproof
which isquite
similar to the one of Theorem 3".REMARK 5’. Remark
analogous
to Remark 5".c’. We can also
give
theanalogue
of Theorem 4".THEOREM 4’.
Suppose
thatfor
someinteger
N > n. Then a(x)
admits a Cotlardecomposition.
Again
we leave theproof
of the reader. Weonly
note that instead of(9)
we have to useREMARK 6. We conclude
by
the observation that theapparent
relationbetween
theprimed
and dubbleprimed
cases can be made still morepertinent
by working
with a wholefamily
of normsinstead
of just
the twonorms 11 a 11* and 11 a 11 ( corresponding
to the extremal cases q === 1 and q = oorespectively.
REMARK 7, One of the
points
of this Section was to relate the work of Cotlar[5], [6]
to the work of Hormander[7].
Our results may indicate that the « Cotlardecomposition >> might
be of littlepratical
value. This may be true in thisspecial
but there arecertainly
other cases where the « Cotlardecomposition
is most useful: In the firstplace
comes Cotlar’s own exten-sion of the
Calderon-Zygmund theory
so as to includeergodic theory (see [6]).
Otherapplications,
in a differentdirection,
of the « Cotlardecompo-
sition >> are made in
[15].
5.
The general case,
p === 1.We show now how to extend the method of Section 2 and 3 to the extremal case p =1. In a less
explicite
from this isalready
contained in Cotlar[5] (see,
inparticular,
Theorem10,
p.152)
who however works out the detailsessentially
in the case of the Hilbert transformonly.
THEOREM 5. Assume that H is a bounded linear
mapping from Li
into.L1
and assume alsoHypothesis
2’.for
everyfE Hsf(x)
convergesa. e. to
Hf (x).
Indeed from
Hypothesis
2’ weget by
the definition thator
where (lB, is the characteristic function of the set
If we set
we have thus for all x
for
some e >
0(depending
onx).
In view of Lemma 1 the theorem followsnow from the
following
LEMMA 5
(see
Cotlar[~~~
Theorem10,
p.152).
LetM, Ti, T2 , T3
b~mappings
such thatIf T1, T2, ~r3
are boundedfrom L, ’i1
then so is M.For
completeness
webriefly
indicate theproof.
It is easy to reduce the lemma to the case whenonly
one ofT1,
IT2 , T3
is different from0,
i. e. we may
distinguish
three cases :Then it follows that
1
But
T2 f E L1 implies
Thereforeby
Lemma 1Hence
( whichimplies
Case 3° is similar to case 2° and we therefore omit details.
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