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A totally non-atomic set-valued measureAbstract. A necessary and sufficient condition for a vector-valued measure with values in

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ANNALES SOCIETATIS MATHEMAT1CAE POLONAE Series I: COMMENTATIONES MATHEMATICAE XX!V (1984) ROCZNIK1 POLSK1EGO TOWARZYSTWA MATEMATYCZNEGO

Séria I: PRACE MATEMATYCZNE XXIV (1984)

H. H u d z i k , J. M u s ie l a k and R. U r b a n s k i (Poznan)

A totally non-atomic set-valued measure

Abstract. A necessary and sufficient condition for a vector-valued measure with values in a locally convex topological vector space given by I. Tweddle [3] is generalized to the case of multimeasures.

Let £ be a Hausdorff locally convex topological vector space over the reals, with topology

t

, and let E' be the strong dual of E. For any sequence of sets E„ с E, £ En will mean the set of all x e E of the form x = ]T x„

n ÿ 1 1

with x e E„ for every n, the series being convergent in the sense of the topology

t

. The series £ E„ will be called (

t

)-convergent, if for any sequence

n ^ 1

(yn)® with y„eEn for every n the series y„ is convergent in the topology

t

;

n Z 1

then we shall write (

t

) £ En.

n ÿ 1

Let S be a non-void set and let I be a cr-algebra of subsets of S. In this paper there will be considered a set-valued measure M: I -* E assigning to every element A in I a non-empty subsets M(A) of E in such a way that M(A) = ( t ) ]T M(A„), whenever A is the disjoint union of the sets A„ in I .

n > 1

We denote by <5*(-| A) the support function of a subset E i of E : ô*(x'\ E J — sup {<x, x'>: x e £ j} , x'eE '.

It is easy to prove that for every x 'e E ' the mapping A M(A)) is a measure with values in ] — oo, oo].

Let us denote M v (A) — (J (A/(S): l a S c d } . A set A e E is called an atom of M, if M V( T ) # { 0} and for every В c A either M(B) = {0} or M v (A \B) = {0}. M is said to be non-atomic if it has no atoms. M is called totally non-atomic, if for each x 'e E ' the set-valued measure x'oM (A )

= x'[Af(A)] is non-atomic.

T h e o r e m . Let /jU be a base of absolutely convex neighbourhoods of the orgin in E. A set-valued measure M : I E is totally non-atomic, if and only If, for each U e there exists a non-negative, non-atomic, finite measure ji: I R+ with respect to which each function S* (xj M ( • )) with x 'e V 0 (U° being the polar of U) is absolutely continuous.

~ Prace Matematyczne 24.1

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6 6 H. H u d z i k , J. M u s i e l a k , R. U r b a n s k i

P ro o f. The sufficiency follows from the fact that if a scalar-valued measure is absolutely continuous with respect to p, then the total variation of this scalar-valued measure is also absolutely continuous with respect to p and, moreover, it is non-atomic. Hence the total variation (5*(x'| M ()) is non-atomic for arbitrary x'eE ', but this implies M to be totally non-atomic.

In order to prove the necessity, let us first remark that (5*(xj M ( ) ) is a measure on 1. We shall prove that the family {<5*(x'| M(-)): x 'e U 0}, where Ue%, is a family of uniformly countably additive measures. It is sufficient to prove that this family is uniformly exhausting. Let us suppose the converse. Then there exist a sequence (T„)f of pairwise disjoint sets in 1, an e > 0 and a sequence of functionals x'n e U° such that

|<5*(xJJ M(A„j)\ ^ e, i.e. there exist x ne M (A n) for every n such that l(x„, x'„)j ^ e for n = 1, 2, ... Thus > 1, where x'„ e U°. But this

implies - x n$U for n — 1, 2, . . . Consequently, writing Ut = eU, we have E

х„фи1 for all n. However, x„eM (A n) and so £ x„ is convergent, which П& 1

gives a contradiction.

Hence, by Theorem 10.7 of [1], there exists a non-negative, finite measure p such that <5*(x'| M(*)) with x'eU ° is absolutely continuous with respect to I .

Now, let us suppose that A e l is an atom of p and let x'eU °, B cz A, B e l . Then ц(В) = 0 implies |<5*(x'| M(B))\ = 0 and ц{А \В ) = 0 implies |<5*(x'| M (T \B ))|= 0 . Hence, if M is totally non-atomic, then

|<5*(x'| M(A))\ = 0 , since otherwise A would be an atom of |<>*(x'| M(-))|.

Let us suppose that (see [2]) has a countable set {A „ e l : n e l\} of pairwise disjoint atoms. We define a finite measure /q in the following manner :

ц 1(А) = ц (А \ (J An) for A e l . neN

Then is a non-negative, non-atomic measure on I and for every

<5*(x'| M (-)) with respect to ii1. We have for /q(T) = 0:

S*(x'\ M(A)) = S * (x 'I M (E \ (J A.))+ I S*(x'\ M (AnA„)) = 0,

n e N n e N

because otherwise we should have ц ( А п А п) = 0 or E n A n would be an atom of ix.

C o r o l l a r y . Let E be metrizable. M is totally non-atomic, if and only if, there exists a non-negative, non-atomic, finite measure on 1 such that

<5*(x'| M( •)) is absolutely continuous with respect to this measure for arbitrary x’eE'.

The proof is analogous to that in [3].

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Totally non-atomic set-valued measure 67

References

£1] L. D r e w n o w s k i, Topological rings o f sets, continuous set functions, integration III, Bull.

Acad. Polon. Sci. Ser. Sci. Math. Astr. 20 N o 6 (1972), 439-445.

[2] R. S ik o rsk i, Funckje rzeczywiste, t. I, Warszawa 1958.

[3] I. T w e d d le , The range of a vector-valued measure, Glasgow Math. J. 13 (1972), 64-68.

INSTITUTE OF MATHEMATICS, A. MICKIEWICZ UNIVERSITY, POZNAN

INSTITUTE OF MATHEMATICS, POLISH ACADEMY O F SCIENCES, POZNAN

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