DE L ’U NIVERSITÉ DE C LERMONT -F ERRAND 2 Série Mathématiques
E. D ETTWEILER
Infinitely divisible measures on the cone of an ordered locally convex vector spaces
Annales scientifiques de l’Université de Clermont-Ferrand 2, tome 61, série Mathéma- tiques, n
o14 (1976), p. 11-17
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INFINITELY DIVISIBLE MEASURES ON THE CONE OF AN ORDERED LOCALLY CONVEX VECTOR SPACES
E. DETTWEILER
,UNIVERSITE DE TUBINGEN. R.F .A .
iThere are at least two reasons for the
study
ofprobability
measureson the cone of an ordered vector space. First of all there are some
applications
to thetheory
of random measures andespecially
to thetheory
ofpoint
processes : let T be alocally compact
second countable space,#£(Tl
the space of all continuous functions on T withcompact support (with
the usual inductive limittopology), M(T)
the space of allRadon measures on T and
Jt + (T)
the cone of allpositive
Radon measures.If one
provides
with the weaktopology $i(T)),
the Borelfield of
uu(T)
isexactly
the0-algebra usually
considered in thetheory
of random measures
(E3], E4]).
So a random measure on T as a measurable map X from someprobability
space(n. 0l, P)
intoJL + (T)
can be viewedas a
probability
measure of the coneJt + (T)
of£(T).
Moreover one canprove, that a sequence of random measures converges in distribution
(see
for ex.E3])
if andonly
if the associated sequence of measures onconverges
weakly.
The second reason is after myopinion
the con-nection with the structure of ordered
locally
convex spaces,especially
Banach
lattices,
similar to thesituation,
when one studiesprobability
measures on not
necessarily
ordered Banach spaces.In this paper I treat
only one topic
which is of interest in thetheory
ofprobability
measures on vector spaces,namely
thedescription
of the -structure of those
probability
measures on a cone which are in-finitely
divisible.1. Preliminaries
For the moment let E be an
arbitrary
reallocally
convex space with theonly
additionalproperty,
that everycompact
subset of E is contained in acompact
convex circled one(this
is the case forexample
if E iscomplete).
Let
(E), Ji?CE). g>(E)
denote the set of allpositive
Radonmeasures, all
positive
and bounded Radon measures and allprobability
measures
respectively.
denotes the set of allinfinitely
divi-sible
probability
measures.D6finition
(i)
v E~(E)
is called a Poisson measure ;(ii) p
EJ(E)
is called a Gaussianmeasure ;
, v Poisson measure => v = e o
(Dirac
measure)(iii) p
E is called ageneralized
Poisson measure :(a) (e(G.)
* e)
is anuniformly tight
net andi xi
(b)
the net(Gi
isincreasing.
One has : F := sup
G. 1 uniquely describes p
in the sense that if(e[G.)
* e)
isuniformly tight
then every limitpoint
of this net isi
yi
of the form
v =u
*e
for some x e E(see [1J
for this and thefollowing) ,
We therefore use the
notation u = e(F)
and call FLevy measure.
F has the
property : 3
K C E(compact) : F(Kc)
~.We have the
following
result(s. [1],
p.290) :
Every 11
is of theform p =
p *6(F)
with asymmetric
Gaussian measure p.
With the aid of this result one can
compute
the Fourier transformof p :
with a E E,
Q
thepositive quadratic form belonging
to p([1L
p.289) ,
F
Levy
measureof y
withF(K’)
00.2. The
Laplace transform
ofinfinitely
divisible measures on a coneFrom now on we demand that E has the
following
additionalproperties :
(i)
E is an orderedlocally
convex space withpositive
cone C.(ii)
C is a normal cone, i.e. there is agenerating family .9
of semi-norms on E such that
p (x) :5 p(x+y)
for all x, y E C and all(iii) Every
order bounded, directed net in C converges.(See [5]
andE6]).
Remark :
Every
Banach lattice with order continuous norm(E6],
p.92),
forexample
theLP-spaces (1 ~
p fullfills the above conditions.Let denote the set of all
infinitely
divisibleprobability
measures concentrated on C. We have the
following
Theorem
Every p E ’J(C)
has thefollowing Laplace
transformwhere a E C and the
Levy
measure F(also
concentrated onC)
has the pro-perty
that for everyneighborhood
Uthe following
condition holds :Proof :
First of all one can
easily
prove with the aid of the Hahn Banach theorem thatwith
also theLevy
measure Fof u
must be concentratedon C.
Furthermore y
cannot have any non trivial Gaussian factor p. For suppose p = p * o withp / Eo
andsymmetric.
Because ofthere is a bEE with
p(C-b) =
1.Symmetry implies p(-C+b) =
1. there-fore
p([-b,bl) =
1.But
now : 3
x’ E C’(dual Cone) : r (p) =
e0
(where r
x’ ,
denotes the canonical
projection :
TIx ~(x) - x,x’> ~
x e E). Therefore,which is
impossible.
Now we
have u = e(F)
with 00 for somecompact,
convex circled set K c E. Let i be aneighborhood
base, and setG. 1
i :=RestKnUc n i
F.Then we have for all
I y = X. * e (Rest Kc
F).Intoducing centering
i i K °
elements a. E C, defined
by
a.,x’> =dG,(x),
weget
i i 1
One can prove
(see Ell,
p.294),
that the net(vi)
converges to apoints
i measure
e z
with z E C and the net(6 -ai
*e(Gi))
isuniformly tight
andconverges to a certain
probability
measure X. Now it is easy to show z 2t a. for alli,
i.e.(a.)
is an order bounded net, which convergesby
i i
assumption
about Eagainst
a certain element b of C. Therefore in thecase of an
infinitely
divisible measure on Ccentering
is not necessary, and with a = z-b onecomputes
theLaplace
transform as asserted. The condition about F follows noweasily
from thenormality
of C :Hence
i J J
Because of then
)
onegets
the final assertion.Remarks :
1. It is not
clear,
wether or not the above formula for theLaplace
transform of aninfinitely
divisible measure on C is stiil valid in spaces, in which not every order bounded directed net in C converges.For
example
inC[0,11
itmight happen
that thecentering
elementsonly
converge in the bidual of
CEO,11.
2. If E is a Hilbert space
(not necessarily
ordered) one knowsthat a measure F is a
Levy
measure if andonly
if F fullfills the con-dition
f
~. Forprobability
measures on R one has thestronger property j
00. If E is anCAL)-space,
one can also
prove J inf (1E’ llxll )dF(x)
00 for everyLevy
measure onthe
positive
cone of E whereas this result is not correctfor £2.
Thequestion
is now : if onehas f inf(1E’ll)dF(x)
00 for some measureF on C, is then F a
Levy
measure ? Moreover : for which spaces is this valid ?3.
The Laplace
transf orm of stable measures on a coneIf E is an
arbitrary locally
convex space, aprobability
measurep is called stable,
if p
satisfies theproperty
where for every s >
0,
H : E + E denotes themapping
definedby
s
H
(x) =
s x for all x E E.s
Let p
be a stable measure withLevy
measure F. Let K be acompact
convex, circled subset of E with
F(Kc)
00. and letE K
denote the Banach space with unit ball K andsphere S K := IX E E K
:lixll I
=1}.
Considerthe
following diagramm:
where i denotes the inclusion map
and Y
is definedby 1-t’(a,x) =
ax forall a >
0,
x ESK.
One can show(see [2L
p. 156 for the idea of theproof),
that there exist a measure H EXb (SK)
K and a measureV E with
density
t~ 1for some a cJO. 2C)
withrespect
t1+a
to
Lebesgue
measure, such that F =(i
oH).
Let now E be an ordered
locally
convex space with the three pro-perties
of the last section. Then onegets
theLaplace transform
(for
all x’ EC’).
Furthermore one has for all x’ C’Since the function t +
t a
isintegrable
over[0. 1J only
for a E10, 1[
we have the
following
Theorem
For every stable measure p dn the
positive
cone C of E, there existan a E
10,lE,
an a E C and a measure H E such that theLaplace
transform
of y
is of the formwhere the constant A > 0
only depends
on a.References
[1]
Dettweiler, E. : Grenzwertsätze für Wahrscheinlichkeitsmasze auf Badrikianschen Räumen. Z. Wahrscheinlichkeitstheorie verw. Gebiete 34, 285-311(1976)
[2] Dettweiler,
E. : Stabile Masze auf Badrikianschen Räumen. Math. Z.146, 149-166
(1976)
[3] Kallenberg,
0 : Lectures on random measures.University
of NorthCarolina at
Chapel Hill,
Institute of Statistics Mineo Seriesn°
963