A NNALI DELLA
S CUOLA N ORMALE S UPERIORE DI P ISA Classe di Scienze
B. F ISHEL
An abstract Lebesgue-Nikodym theorem
Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 3
esérie, tome 23, n
o2 (1969), p. 363-372
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AN ABSTRACT LEBESGUE-NIKODYM THEOREM
B. FISIIEL
The
developement
of thetheory
of Radon measures, continuous linear forms on the vector space of continuous real-valued functions withcompact supports
on thelocally compact
spaceT,
endowed with a suitable inductive-limittopology [B3],
leansheavily
on the order structure of9((T).
We have shown elsewhere
[F1,2]
how someaspects
of thetheory
ofintegra-
tion for Radon measures can
equally
bedeveloped by availing
oneself ot’the
algebraic
structure of9((T)
rather than its order structure. Wenote, however,
that such a treatment does notyield
atheory
ofintegration
inthat,
forexample,
theobjects
which therecorrespond
to theintegrable
functions of the more familiar
development
are elements of an abstractcompletion
of9((T),
i.e. are not functions. Ourobject
ininvestigating
the rôle of the
algebraic
structure was toexplore
thepossibility
of itsapplication
to(i)
vector measures and theintegration
of vector - valuedfunctions,
where
rarely
is there an order structure which arises in a natural way from the structure of’ the space which we areconcerned,
and(ii)
thetheory
ofdistributions,
where utilisation of anaturally-occur- ring
orderimposes
excessive restrictions - apositive
distribution is a measure.In
[ F2J
weattempted
to establish aLebesgue-Nikodym
theorem withinour order-free
structure,
but were unable to do so without the aid of asupplementary hypothesis (loc
citProp 2.3)
which is not verified for Radon measures, but which holds in thetheory
of distributionIn the
present
paper we obtain aLebesgue-Nikodym
in a form ap-plicable
to thetheory
ofintegration. §
1.1gives
an account of some ideasfrom the
theory
ofduality
fortopological
vector spaces, inparticular,
ofan extension of Grothendieck’s
completion theorem. §
1.2 introduces the pre-Perveuuto Redazione il 21 Ottobre 1968.
hilbert structure defined
by
apositive
linear form on a normedalgebra.
§
1.3 describes dualities definedby
a linear form on analgebra. § §
1.4-5formulate a
concept
of absolutecontinuity
of one linear form on a normedalgebra
withrespect
to another such form andapply
thecompletion
theo-rem
of §
1.1 to establish an abstractLebesgue Nikodym
theorem.In §
1.6this theorem is
applied
togive
theLebesgue Nikodym
theorem for Radonmeasures on a
compact space. §
2.1 describes an extension of the results of§§
1.1-5 to the inductive limit(as
atopological
vectorspace)
of afamily
of normed
algebras,
andin §
2.2 we obtain theLebesgue-Nikodym
theoremon a
locally compact
space.§
1.1 We make use of the ideas of thetheory
ofduality
fortopologi-
cal vector spaces. We summarize
here, briefly,
the definitions and results which we shall need.Let
Et ,
be a dualsystem (pairing)
of vector spacesE, , E2
overthe
complex
field C.A
family
of subsets of= 1,2)
is said to be saturated withrespect
to
El ~’2 )
if it contains(1)
the subsets of each of itsmembers, (2)
the scalarmultiples
of itsmembers,
(3)
theabsolutely
convex,weakly
closed hulls of finite unions ofits members.
9x
will denote thefamily
obtainedby saturating
thefamily
of finitesubsets of
E;).
A saturated
family 1:’t
ofweakly
bounded subsetsof Et
defines alocally
convex
topology arc! on E2 (the topology
of uniform convergence on the sets of If isseparated
then is Hausdorff(separated)
if71 (The corresponding
statements obtainedby interchanging
thesuffixes 1 and 2 also
apply).
With this notation we writeaY2
for the weaktopology
a(2~ ~
C)C2
denotes thefamily
obtainedby saturating
thefamily
ofabsolutely
convex
weakly compact
sets inE2 . 9g
cC)(2 .
Let
(7J
be a saturatedfamily
in and letc) 9(2 (c
be a saturated
family
inEz ,
y both familiesbeing
ofweakly
bounded sets.We shall need the
following
form of Grothendieck’sconipletion
theo14em:if
E2 )
isseparated,
G
= f °9L2-continuous
on the sets ofM1} (1)
is the(sepa-
rated) completion (E2 ,
of for thetopology
(1)
F;~
denotes the algebraic dual of Ei.365
This result may be established
by showing
(i) (as
in[K]
p.272)
that Q’ iscomplete,
andseparated
forc
M1
andE1,
isseparated),
and
(ii)
that E is-dense
in G.The
argument establishing
thenecessity
of[S]
Th.6.2,
p. 148 proves(ii)
when weput (E, r)
= since(E, r)’
=(Eu o~ )~ == E 2(where (~ r)~
denotes the
topological
dual of E for thetopology r) by
theMackey-Arens
theorem
([S]
Th.3.2,
p.131),
since92
ccrl2
c~C2 .
(A « proof »
of this theoremgiven
in[F2J
is false. It relies on the falseinequality (3)
of[IK]
p.272).
§
1.2. We shallapply
this theorem to a situation where we take(essen- tially)
forE2 two copies
of a *-normedalgebra
A(i,e.
a normedalgebra
overC on which there is defined an involution. such =
11 $ 11
for allEA, (see [R] p. 180). Elements f
for are said to beself-adjoint.
We consider a linear form p on A
having
theproperties
(this
isequivalent
to : IA is real onself-adjoint
elements ofA,
andimplies
that the
sesqui-linear
formsand
are
bermitian,
it is an easy matter to construct anexample
for whichthey
do notcoincide),
andis
positive,
i. e.
(and
soso that the
sesqui.linear
forms arepositiiTe-definite.
We shall henceforth consider
only
the first of these two forms de- fined and shall write It defines aprehilbert
structure on A1
with
corresponding
semi-norm po(E)
_(p ($$*))2.
If Z =t,:
,u(EE*)
=0)
=~~ :,u (~~) = 0
thepositive
hermitian form anA/Z
associated with ,u( , ), (wlich
we shall denoteby It ( , )
defines aseparated prehilbert
struc-ture. The norm p for this structure is that associated with the semi-norm extends
uniquely
to theseparated completion (which
wewrite of
A/Z
for po , and makes it a Hilbert space. We canequally
construct the
separated completion (or A")
of A for p, andII § 3.7) (A/Z)"
isisomorphic
withA",
to which we may thereforetransport
the extendedform Ï-t ( , ),
and if i is the map ofII § 3.7,
Th.
3, i (A)
is dense in A^(loc. cit. § 3.8).
i is here a linear map, and is in fact the canonical mapA -~ A/Z,
so thati (A)
isisomorphic
withA/Z.
We now
impose
upon a the furtherrequirement
is continuous on A.
(If
A has a unit and iscomplete,
i.e. is a Banach*-algebra,
the conti-nuity
of ,u follows from thehypothesis
that it ispositive ((N],
p.200)).
If
since
ind so
Now i ( V )
is contained in the unit ball of the Hilbert spaceA ^,
and theclosed unit ball is
compact
for the weaktopology a (A A, A A)
definedby
thecanonical
duality ( A ^, A ^ ) of A ^
with itsHilbert-space
dualA",
so thati ( Y)
and thereforei (U)
arerelatively weakly compact
in A". The the weak closure ofi ( U )
in A iscompact
for and is thereforecompact
forthe coarser
topology
a(A", i (A)).
§
1.3. Our form p defines aduality (Do)
on A X A - which it is con-venient to write
A1
xA2 - by
It is clear that this
duality
will not ingeneral
beseparated.
Let
9N
be thefamily
obtainedby saturating
thefamily
inA1
forthe
duality ~Da),
and letck
be the samefamily
considered as afamily
inAz.
367
’1’he sets of
í)Jl and 9Z
areweakly
bounded for since’rhe extension to
.t11 X At
defines aduality (1)}
on XA2.
Let
= i (’)/[).
Since i is continuous for po and p,i (U)
is boundedfor p and so for the weak
topology
a(i (A,), A2),
which is the weaktopology
defined
hy (D).
It follows that the sets of areweakly
bounded for(D).
Since i is
linear,
to prove that is saturated for(I))
it suffices to prove that thei-iinages
ofabsolutely
convexweakly
closed(for (D,))
setsof
9X
areagain weakly
closed. Such a set ~I is closed for po, and since i is the canonical map isclosed,
so thati (M)
is closed for y.Since it is
absolutely
convex andA~ _ (i (~11), p)^,
i(M )
is also a(i(A 1)’ Ag)
-
closed,
i. e. isweakly
closed for(I)).
Finally,
we definesC)t2
to 1~e thesaturate,
forC i {A1), A~ ~
of Itis clear that the sets of are
weakly
bounded for(D).
~ 1.4. is another linear form on A we now define : A
absolutely
continuous vithrespect to a
to mean :
A is o
-continuous
on the sets of(where
a~~~
is definedby
theduality (1)0))’
It tolloBvs 0 :
Since E
E for some ilf E0rl (F
c9/C)y
theo.continuity
of y on M showsthat 1
(~)
= 0.~, is thus well-defined on
A/Z.
We shall denoteby I
the functional sodefined,
and shall prove that it is(i, .2-continuous
z on the sets of Forthis it suffices to establish
continuity
for the coarsertopology °, (N).
10 dnaali della Scuola Norm. Sup.. Pisa.
Since A
= Ä
o i and i is the canonical map of M ontoM/Z,
it suffices([B1J §. 3.4)
to prove that is thequotient by
Z of This is imme- diate from consideration of theneighbourhoods
for the twotopologies
sincea
D,y;-neighbourhood
~jsup:
is saturated for theequivalence
relation defined
by 1 II § 3.4).
§
1.5 We nowapply
Grothendieck’scompletion
theorem to establish aLebesgue-Nikodym
theorem.o
is coarser than thepo-topology,
i
is coarser then the
p-topology.
PROOF.
Since p
ispositive
Therefore
so that
neighbonrhood
definedby
M = U contains a poneighbourhood,
i. e.
o
cp-topolog.y.
The second assertion is now immediate.’’ °
defines a linear form A which is
absolutely
continuous withrespect
to p.PROOF.
p (¿.)
iso’Tl¡
-continuous onA2
forall ~ E A1,
IE
0Jlt),
and so extends(uniquely)
toThis extension
defines u (EE).
~y : ~
-+1* (~~)
isclearly
linear on A. To prove that it is absolute con-tinnous with
respect
to ~~, let M Er ) 0. (a o
minimal369
Cauchy
filter onA2 (( B1] II § 3.7)),
there exists P such thatChoose 03C0 E P.
(a)
EN
andso III (8n) ) e/2 implies
thati.e., Cp
is°Cf-continuous
on u.THEOREM 2. If A is
absolutely
continuous withrespect
there existsC
E(A, °C)/l) "
such~,u.
PROOF. A is
N-continuous
on the sets ofby definition,
thereforey
.
is
0. (0- -continuous
t) on the setso2-continuous
N2on the sets of
0Jlt
since0. (:")’"
co 1. by
Grothendieck’s. () "Ilt theorem.
Nov
o
epo-topology
and so, if denotes the adherence of 0 inby [F,l Prop.
2.3. It follows thatSince
4
is
clearly
the associatedseparated topology
on( A2 , " ,
we haveFinally,
y since,denoting by Zo
the adherence of 0 in(A2 ,
it is easyto
verify
thatZo
= we havethere
follows,
from(1)
and(2),
This shows
that I,
as a linear form anA2",
isrepresented
via theduality (1))
Thuswhere $ = I
is aCauchy
filter onA2 .
since
u(E)
isoC1-continuous A2 , ({E)
E and so§
1.6. Weapply
our abstractLebesgue-Nikodym
theorem to Radonmeasures on a
compact
space.Let T be a
compact
Hausdorff’ space. We take A to beCK (T),
the al-gebra
of continuous real-valued functions withcompact supports, (which
here coincides with
C(T)-continuous functions).
Our involution is the iden-tity
map, and the norm on A is the uniform =(t) I. (A
tET
has a unit and is
complete
for thisnorm).
We take ,u to be apositive
Radon measure, and so ,u is continuous for the norm of A.
If A is a Radon measure on T which is
absolutely
continuous withrespect
to ,u in the sense of[B.] V §
5.5 we have shownProp.
3.1that it is
gcN-continuous
on g(in
thepresent
context =cSp 9l
=cS2
andCK cS
=cS,
in the notation of[F2]).
In order toapply
our abstractLebesgue-
Nikodym
theorem we must show that y is°c52-continuous
on9N,
thefamily
obtained
by saturating { U).
Itclearly
suffices to establisha62-continuity
onthe weak closure of U for the
duality (Do). However,
U isalready weakly
closed
(in 9Ci),
for if this were not so there wouldexist j
E9Q n
U~]
1 forsome to
ET)
which isweakly
adherent toU,
i.e.given e >
0and T there would exist ja E U such
that (Cf - h) g)
e, which isclearly
false.Finally,
we observe that the space(A,
of Theorems 1 and 2 is hereby Prop. 3.4,
since forcompact
T(/l)
= L(p)
andfll c3
=cS.
NowProp.
2.7 andProp.
3.4 ensure that’p
as here definedfor ~
E L(,u)
is none other than theproduct $p
ofintegration theory.
OurLebesgue-Nikodym
theorem now asserts that A isabsolutely
continuouswith
respect
to p if andonly Clt.
371
§
2.1 We now consider an extension of Theorema 1 and 2 which will enable ns to establish theLebesgue-Nikodym
theorem for Radon measureson a
locally-compact
space. The extension has very little in the wa.y of novel features now that the more restricted Theorems I and 2 have beenestablisheil,
but in the interests of ease ofpresentation
it seemed worth- while to establish thesimpler
results first.We consider A winch is the inductive Hrnit, as a
topolo- gical,
vector space([B2J II 3 Ll),
01’ a directedfamily (Aj)J,
of’ normed* sub-algebras A;
withnorms I lij.
Let It be a linear form ou .11having
theproperties of §
1.2. Asin § 1.2 /t
defines aprehilbert
structure on.4,
with and associated norm p, and A" with normp is a Ililbert space. If’ and
since
if ~ E A~ (where
a is the norm ot’ the restriction of It to~1,,),
we haveIt follows that
if,
asbefore,
i is the canonical map of A into the separa~ted
completion A",
then theweak
closures in A" of the sets arecompact
for0 (A A,
i(,1 )).
We
define,
iis aduality (1)0) on At
xAz
and now take ascg~
the saturate fOI’
(J)o) of Th),~
considered as afamily
of subsets ofAi, Cfl
wi ll be the same
family
considered as afamily
of subsets ofA2 .
andrn.2,
1 tamilies irl andrespectively,
are defined as before. We de-fine
continuity
of another linear form y withrespect
to p as in§ 17
and TIh’orems ! I and 2 can then be established in this newcontext,
the
only change
on theargument
that is needed is an obvious modification of theproof
of the lemmapreceeding
Theorem 1.§
2.2 Inapplying
the theorems to Radon measures on alocally compact
space T we take the
A~
to be the *normedalgebras
where arethe
compact
sets Radon measure It on 7’ has theproperties
If A is
absolutely
continuous withrespect to u (in
the sense of[BaJ V § 5.5)
we have seen
([F 21 Prop. 3.1)
that it isOCK2 62-Continuous
on the sets ofcSl,
in the notation of’[F 211
so that to show that A isabsolutely
conti-nnous with
respect
to p in thepresent
sense it suffices to observei)
thateach
Uj
is contained in a set ofI A-1 cS1
of the formfso
wheref’E ’-K
has thevalue 1 on
Kj
and1},
andii)
that’K2 cS2 9’l
sinceeach
gs
is contained in a setgc So ,
where c is aconstant,
andfor some constant d and
support (g)c K; .
Finally,
ininterpreting
the conclusions of our abstractLebesgue-Niko- dym
theorem in thepresent
context we note that =i) above,
shows that and
ii)
shows that oem. Thus isisomorphic,
as atopological
vector space, withLlo, (p).
REFERENCES
[B1]
N. BOURBAKI, Topologie Générale, Chapters I and II, 3rd Edition, Hermann Paris 1961.[B2]
N. ROURBAKI, Espaces Vectoriels Topologiques, Chapters I and II, 2nd Edition, Her-mann, Paris 1966.
[B3]
N. BOURBAKI, Intégration, Chapters I-IV 2nd Edition Hermann, Paris 1965 Chapter V, Hermann, Paris 1956.[F1]
B. FISHEL, A structure related to the theory of integration, Proc. L.M.S. (3) 14 (1964)415-30.
[F2]
B. FISHICL, A structure related to the theory of integration II, Proc. L.M.S. (3) 16 (1966)403-414.
[F3]
B. FISHEL, Division of distributions and the Lebesgue-Nikodym theorem, Math. Annalen 173 (1967) 281-286.[K]
G. KÖTHE, Topologisohe lineare Räume, Springer, Berlin 1960.[N] M. A. NEUMARK, Normierte Algebren, Dentscher Verlag der Wissenschaften, Berlin 1965.
[R]
C. E. RICKART, General theory of Banach algebras, Van Nostrand, Princeton 1960.[S]
H. H. SCHAEFER, Topological Vector Spaces, Macmillan, New York 1966.Istituto Matematico « Leoinida Via Derno,, Pi8a.
We8tfield College, (University of London), Hampstead, N. I~’. 3,