A NDREI K HRENNIKOV S HINICHI Y AMADA A RNOUD VAN R OOIJ
The measure-theoretical approach to p-adic probability theory
Annales mathématiques Blaise Pascal, tome 6, n
o1 (1999), p. 21-32
<http://www.numdam.org/item?id=AMBP_1999__6_1_21_0>
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The measure-theoretical approach to p-adic probability theory
Andrei
Khrennikov,
ShinichiYamada,
Arnoud vanRooij
1 Introduction
The
development
of a non-Archimedean(especially, p-adic)
mathematicalphysics [20]-[22], [1]-[4], {6], [8]-[13]
induced some new mathematical struc- tures over non-Archimedean fields. Inparticular, probability theory
withp-adic
valuedprobabilities
wasdeveloped
in[11], [8], (4~1.
The first
theory
withp-adic probabilities
was thefrequency theory
inwhich
probabilities
were defined as limits of relativefrequencies
vN =r~/N
in the
p-adic topology2.This frequency probability theory
was a natural ex-tension of the
frequency probability theory
of R. von Mises[15], [16].
The next
step
was the creation ofp-adic probability
formalism on thebasis of a
theory
ofp-adic
valuedprobability
measures. It was natural to dothis
by following
the fundamental work of A.N.Kolmogorov [14]
in whichhe had
proposed
the measure-theoretical axiomatics ofprobability theory.
Kolmogorov
usedproperties
of thefrequency probability (non-negativity,
normalization
by
1 andadditivity)
as the basis of his axiomatics. Then he added the technical condition ofu-additivity
forusing Lebesgue’s integra-
tion
theory.
In works[11],[8]
we tried to follow A.N.Kolmogorov. p-adic frequency probability
has also theproperties
ofadditivity.
it is normalizedby
1 and the set ofpossible
values of thisprobability
is the whole field ofp-adic
numbersQp.
Thus it was natural to definep-adic probability
as aQp-valued
measure normalizedby
1. .Ip-adic
probability theory appeared in connection with a model of quantum mechanics with p-adic valued wave functions[12].
The main task of this probability formalism wasto present the probability interpretation for p-adic valued wave functions.
2The following trivial fact is the cornerstone of this theory: the relative frequencies belong to the field of rational numbers Q; we can study their behaviour not only in the real topology on Q, but also in the p-adic topologies on Q.
[18], [19].
Therefore the creators of non-Archimedeanintegration theory (A.
Monna and T.Springer [17])
did nottry
todevelop
abstract measuretheory,
butthey proposed
anintegration
formalism via Bourbaki based onintegrals
of continuous functions. Thisintegration theory
has been used forcreating p-adic probability theory
in the measure-theoretical framework[8].
The main
disadvantage
of thisprobability
model is thestrong
connection with thetopological
structure of asample spaced
An abstract
theory
of non-Archimedean measures has beendeveloped
in[19].
The basic idea of thisapproach
is tostudy
measures defined onrings
which in
principle
cannot be extended to measures ona-rings.
Thisgives
the
possibility
forconstructing
non-discrete valued measures with values in non-Archimedean fields(and,
inparticular,
in fieldsof p-adic numbers).
Onthe other
hand,
the condition ofcontinuity
for measures in[19] implies
the03C3-additivity
in all natural cases.In this paper we
develop
ap-adic probability
formalism based on mea-sure
theory
of(19~ . By probabilistic
reasons we use thespecial
case of thismeasure
theory: (1)
measures are defined onalgebms (such
measures havesome
special properties); (2)
measures take values in fields ofp-adic
num-bers
(here
values ofprobabilities
can beapproximated by
rational relativefrequencies).
However, probabilistic applications
stimulate also thedevelopment
of thegeneral theory
of non-Archimedean measures defined onrings.
We prove the formula of thechange
of variables for these measures and use this formula fordeveloping
the formalism of conditionalexpectations
forp-adic
valuedrandom variables.
2 Measures
Everywhere
below K denotes acomplete
non-Archimedeanfield,
R denotesthe field of real numbers. The valuations on these fields are denoted
by
thesame
symbol)-).
We setUR(a)
={2?
E A’:R},
a 6K,
jRR, R
> 0.By
definition these are balls in K.Let X be an
arbitrary
set and let ?t be aring
of subsets of X. Thepair (X, ~Z)
is called a measurable space. Thering
?Z is said to besepamting
if for every two distinctelements, r
and y, of X there exists an A E R such 3This is quite similar to the old probability formalisms of Frechet[6]
and Cramer[5]
in which the topological structure of the sample space played the important role.
that x e
A,
y~
A. We shall consider measurable spacesonly
overseparating rings
which cover the set X.’
Every ring
R can be used as a base for the zero-dimensionaltopology
which we shall call the
R-topology.
Thistopology
is Hausdorff iff R isseparating.
Throughout
thissection,
R, is aseparating ring
of a set X.A subcollection S of R is said to be
shrinking
if the intersection of any two elements of S contains an element of S. If S isshrinking,
and iff
is amap 7~ 2014~ K or 7~ 2014~
R,
we say thatlimAEs I{A)
= 0 if for every e >0,
there exists an
Ao
E S such that e for all A ES, A
cAo.
A measure on R is a map J.L : R --i K with the
properties: (i)
isadditive; (ii)
for all AE R, IIAII
= B 67~,
B c~4}
oo;(iii)
if S C R is
shrinking
and hasempty intersection,
thenlimAEs
= 0.We call these conditions
respectively additivity, boundedness, continuity.
The latter condition is
equivalent
to thefollowing: limAEs
= 0 for ev-ery
shrinking
collection S withempty
intersection.Further,
we shallbriefly
discuss the main
properties
of measures, see[19]
for the details.For any set
D,
we denote its characteristic function(the indicator) by
thesymbol iD.
Forf
: X ~ K and03C6
: X -[0,~), put
= supx~X |f(x)|03C6(x). We setNu(x)
=infU~R,x~U ~U~
for x E X. Then~A~
=~iA~N
forany A
E R. We set~f~
=~f~N
.A
step function (or R-step function)
is a functionf
: X --~ K of theform
f(x)
=~Nk=1 ckiAk(x)
where ck E K andAk
ER, Ak
flAl
=0,
d.We set for such a function
fx
=ck (Ak).
Denote the space of allstep
functionsby
thesymbol S(X).
Theintegral f
~Ix f(x) (dx)
isthe linear functional on
S(X)
which satisfies theinequality
I x ~f~ . (1)
A function
f
: X --~ K is calledp-integrable
if there exists a sequence ofstep
functions such thatlimn~~ ~f
-fn~
= 0. The-integrable
functions form a vector space
Li(X, ~n) (and S(X)
CLi(X, ~c)).
Theintegral
is extended from
S(X)
onLl (X, by continuity.
Theinequality (1)
holdsfor
f
ELet =
{~4 :
: A cX, iA
EL1(X, u)}.
This is aring.
Elements of thisring
are calledp,-measurable
sets.By setting (A)
=fX iA(x) (dx)
themeasure is extended to a measure on
R .
This is the maximal extension of ~c,i.e.,
if werepeat
theprevious procedure starting
with thering R~,,
wewill obtain this
ring again.
Set
XE
={~
E X ={~c
E X : =0}, X+ _
X
B Xo. Every
A CXo belongs
to We call such sets-negligible.
Now we construct
product
measures. Let=1, 2,
..., n, be measures on(separating) rings Rj
of subsets of setsXj.
The finite unions of the sets ERj,
form a(separating) ring Rl
x ~ ..x R",
ofXl
x ~ ~ ~x Xn.
Then there exists a
unique
measure 1 x ... x n onR1
x ... xRn
suchthat 1 x ... x
n(A1
x ... xAn)
=1(A1)
x ... x We have..., ~~)
= x ... x(2)
Let X be a zero-dimensional
topological space4.
We denote thering
of
clopen (i.e.,
at the same time open andclosed)
subsets of Xby
thesymbol B(X) (in fact,
this is analgebra).
We denote the space of continuous bounded functionsf
: J~ 2014~ ~by
thesymbol Cb(X).
We use the norm~f~~
=sUPzeX on
this space.First we remark that if X is compact and R =
B(X )
then the condition(iii)
in the definition of a measure is redundant. If X is notcompact
then there exist bounded additive set functions which are not continuous.Let X be zero-dimensional
N-compact topological space,i.e.,
there ex-ists a set S such that X is
homeomorphic
to a closed subset ofNS.
We remark that everyproduct
ofN-compact
spaces isN-compact;
every closedsubspace
of anN-compact
space isN-compact.
Then every bounded 03C3-additive
function : B(X)
~ K is a measure. On the otherhand,
if Xis a zero-dimensional space such that every bounded u-additive function
B(X ) --~ K is a
measure, then X isN-compact.
In the
theory
ofintegration
a crucial role isplayed by
theR -topology,
i.e.,
the(zero-dimensional) topology
that has as a base. Of course,R - topology
isstronger
thatR-topology. Every -negligible
set isR -clopen.
The
following
two theorems[19]
will beimportant
for our considerations.Theorem 2.1.
(i) If
is a measure onR,
thenN
isR-upper
semi-continuous, (hence, R -upper semicontinuous)
andfor
every A ER
andE > 0 the set
Ae
= A nXe
isR -compact.
(ii) Conversely,
let : R - K be additive. Assume that there exists anR-upper
semicontinuos03C6
: X -;[0,~)
such that| ~
supx~A03C6(x),
A ER,
and{~
E A :~(a:)
>E}
isR-compact (A
ER,
E >0).
Then is ameasure and
N~ ~.
Theorem 2.2. Let ~ : R --~ K be a measure. A
function f
: X - K is-integrable iff
it has thefollowing
twoproperties : (1) f
isR -continuous;
4We consider only Hausdorff spaces.
(2) for
every E >0,
the settx : :
>~}
isR -compact.
We shall also use the
following
fact.Theorem 2.3. Let
f
EL1(X, )
and let= 0
for
every A E R.(3)
Then supp
f
CXo.
Proof. Let us assume that
f
satisfies(3)
and there exists xo EX+
(hence N (x0)
= a >0)
such that|f(x0)| =
c > 0. Let be a sequenceof
~step
functions whichapproximates f.
For every E > 0 there existNE
such that - aE for all k >
N~.
Inparticular,
thisimplies
that|fk(x0)|
>_ G ‘ ~, k >N~.
Then we have0394B,k
=| ~B fk(x) (dx)| = | ~B fk(x) (dx)
-~B f(x) (dx)|
03B1~, B ~ R.Let
fk(x)
=03A3 ckjiBkj (x),
ekj EK, Bkj
ERa Bkj
nBki
=Ø,
z~ j,
j
and let xo E
Bkjo.
If B cBkjo,
B E?Z,
then03B1~. On the other
hand,
as~Bkj0~
>_ a, then for everyb >
0,
there exists B CBkjo,
B ER,
such that >(a
-b).
Thus weobtain for this B:
0394B,k
>-(a
-6) (c
-E). By choosing
E >0,
b >0.
such that(a - b)(c - e)
> 03B1~, we arrive to a contradiction.Let
(Xj, Rj), j =1, 2,
be two measurable spaces. A functionf X2
such thatf -1 (R2)
cRl
is said to be measurable((R1, R2)-measurable).
We shall use the
following simple
fact.Lemma 2.1. Let
(Xj,Rj),j
=1, 2,
be measurable spaces and letf
:X i
--~X2
be measurable.If
S isshrinking
inR2
thenf ~~ (S)
isshrinking
in
R1. If S
hasempty intersection,
thenf -1(S)
has alsoempty
intersection.Lemma 2.2. Let
(Xj,
=1, 2,
be measurable spaces and let ~ :X1
~X2
be a measurablefunction. Then, for
every measure :R1
-K,
.the
function
~ :R2
~ Kdefined by
theequality ~(A)
= isa measure on
R2 and, for
everyR2-continuous function,
h: X 2
~ K thefollowing inequality
holds:.
~h~ ~
~~h
°~~ . (4)
Proof. We have for every A E
R2,
~A~ ~
= B E CA} ~ ~~-1(A)~
~.(5)
Thus ~
is bounded. We now prove that is continuous onR2.
Let S beshrinking
inR2
which has theempty
intersection.By
Lemma 2.1~‘ 1 (S)
is
shrinking
inRi
which has also theempty
intersection.By (5)
we obtainthat
limAes
= 0.We prove
inequality (4).
Let h :X2 -~ K
beR2-continucus.
We wish toprove that
(b)
_~h
°~~
for all b EX2.
So we choose b EX2
with0. Then the set
Cb
={y
EX2
_ isR2-open.
Hencethere is a B E
R2
with b E B CCb.
Thensup sup
I(h
° ~)(x)|Nu(x)~h
°~~ .
x~~-1(B) x~~-1(B)
Theorem 2.4.
(Change
ofvariables)
Let =1, 2,
be mea-surable spaces and let y : :
X2
be a measurablefunction,
and letp, : :
Ri
~ K be a measure.If f
:X2
~ K is anR2-continuous func-
tion such that the
function f
o ~belongs
toL1 (X1, ),
thenf
ELl (X2, ~)
and
~X1f(~(x)) (dx) = ~X2f(y) ~(dy). (6)
Proof. It suffices to prove that for every E > 0 there exists a
R2-step function g
such thatp f -
f and ~ f.By (4)
the firstfollows from the second. So we fix f > 0.
By
Theorem 2.2 the setA =
~x
EXl : : I(f °
>E~
is
Ri-compact
and therefore contained in an element ofR1.
ButN
isbounded on every element of
R1,
soNu
is bounded on A. We choose 6 > 0so that
e for all x E A.
As A is compact,
f (r~(A))
is also compact. We can coverf (~(A)) by disjoint
closed balls of radius 6 : C where ao is chosen to be 0 in order to obtain:
It
for t E =o,1,
..., N.(7)
For each n,
Cn
={C
ER2
C C is a collection of open setscovering
thecompact
set~(A)
~f-1(U03B4(03B1n)). Thus,
for each n there is aCn
ECn
such that~(A)
tl CCn.
We now haveCo,
...,Cty
ER2, (8)
Cn C f 1 (Ua(an)), n = o,1, ..., N, (9)
~(A)
CCo
u ... uCN. (10)
Put
g(x)
= Then g isa R2-step
function. We wish to showthat,
for all a EX,
LB(a)
=i(f
°~)(a) - (9
°~)(a)1N’~(a) _
~.Thus, take a EX:
(1)
If a EA,
then there is aunique
n with~(a)
ECn.
Then =|(f o 7?)(0) - 03B1n|N (a)
e.(2)
Ifa g A,
but ECn
for some n, thenby (7)
we obtain that=
I(.f °’~)(a) - i(f
°n)(a)!~~(a)
E.(3)
If a¢ C0~...~CN,
then = o. Thuse
(as a ~ A).
Open problem.
To -find a condition for functionsf
which is weaker thancontinuity,
butimplies
the formula of thechange
of variables.Further we shall obtain some
properties
of measures which arespecific
for measures defined on
algebras5.
Throughout
this paper, A is aseparating algebra
of a set X. First weremark that if we start with a measure defined on the
algebra
A then thesystem A
of-integrable
sets isagain
analgebra.
Proposition
2.1.Let p
: A --~ K be a measure. Thenfor
each E >0,
the set
Xe
isA,-compact.
This fact is a consequence of Theorem 2.1.
Proposition
2.2.Let :
,A -> K be a measure. T’hen thealgebra B(X) of A -clopen
sets coincides with thealgebra A .
Proof. We use Theorem 2.2 and the
previous proposition.
Let B EB(X). Then iB
isA -continuous
and{x : |iB(x)|N(x)
>~}
= B nXE.
AsB is closed and
Xf
iscompact,
B nXe
iscompact.
Thus~ A .
As a consequence of
Proposition 2.2,
we obtain that C~,) (for
the space X endowed withA -topology)
and thefollowing inequality
holds:
I ~f~~~X~ , f
E(11)
Let X be zero dimensional
topological
space. A measure ~ defined onthe
algebra B(X)
of theclopen
sets is called atight
measure. Thusby
An algebra of X is a ring of subsets of X containing X.
Proposition
2.2 every measure ~ : : ,A --~ K is extended to atight
measure onthe space X endowed with the
A -topology.
Proposition
2.3. Let : A - K be a measure and letf
EL1(X, ).
Then
f
is(A , B(K))-measurable.
Proof.
By
Theorem 2.2f
isA -continuous.
Thusf-1(B(K))
cB (X ) .
But
by Proposition
2.2 we have thatA
=B{X ).
3 p-adic probability space
Let :
A -3Qp
be a measure defined on aseparating algebra
A of subsetsof the set H which satisfies the normalization condition = 1. We set
.F ==
A
and denote the extensionof p,
on :Fby
thesymbol
P. Atriple (Q, .~, P)
is said to be ap-adic probability
space(S2
is asample
space, ,~ isan
algebra
ofevents,
P is aprobability).
As in
general
measuretheory
we setQa
=(w o:}~o:
>0, 03A9+
=~03B1>003A903B1, no = 03A9 B 03A9+. Everywhere below,
if aproperty E
is validon the subset
S~+
we say that 2 is valid a.e.(mod P).
Everywhere
below(G, r)
denotes a measurable space over thealgebra
r.
Functions ~ :
S~ -; G which are(.~, Immeasurable
are said to be randomvariables.
Everywhere
below Y is a zero dimensionaltopological
space.We
considerY as the measurable space over the
algebra B(Y). Every
random variable~ :
S~ --~ Y is continuous in the,~ topology.
Inparticular, Qp-valued
randomvariables are
(F, B(Qp))-measurable
functions.If £
EP),
we intro-duce an
expectation
of this random variableby setting Eg
=~03A9 03BE(03C9)P(d03C9).
We note that every bounded random
variable ~ : S~ --~ Qp belongs
toLet ~ :
n ~ G be a random variable. The measureP~
is said to be adistribution of the random variable.
By
Theorem 2.4 we have thatEf(~) = ~Qp f(y)P~(dy) (12)
for every r-continuous function
f
G -Qp
such thatf P).
Inparticular,
we have thefollowing
result.Proposition
3.1. Let ~ : H ~ Y be a random variable and letf
ECb(Y).
Then theformula (12)
holds.We shall also use the
following
technical result.Proposition
3.2.Let ~ : 03A9
~ Y be a random variable and let(
EL1(03A9,P),
and letf
ECb(Y)
. Then =03B6(03C9)f(~(03C9)) belongs Ll(ft,P)
and
E03BE
= ~Qp Yxf(y)Pz(dxdy), z(03C9)
=(03B6(03C9),~(03C9)).
Proof. We have
only
to showthat 03BE
E This fact is a conse-quence of Theorem 2.2.
The random
variables ~,
r~ : S~ -+ G are calledindependent
ifP(~
6B)
=P(~
6JB)
for allA, B
F.(13) Proposition
3.3.Let 03BE,
~ H ~ Y beindependent
mndom variablesand
f unctions f , g
ECb (Y)
. Then we have:=
(14)
Proof. If
f
and g arelocally
constant functions then(14)
is a conse-quence of
(13). Arbitrary
functionsf,g
EC6(Y)
can beapproximated by locally
constant functions(with
the convergence ofcorresponding integrals) by using
thetechnique developed
in theproof
of Theorem 24.Remark 3.1. In
fact,
the formula(14)
is valid for the continuousf , g
such that the random variables
f (~’),
andf (~’)g(r~) belong
toL1 (S~, P).
.Proposition
3.4.Let 03BE and ~
beindependent
random variables. Then the random vector z =(03BE, ~)
has theprobability
distributionPx
=P~
xP03BE.
This fact is a direct consequence of
(13).
Let 03BE and ~
berespectively Qp
and G valued random variables and03BE
E A conditionalexpectation E|03BE|~
=yj
is defined as a functionm E such that
~{03C9~03A9:~(03C9)~B} 03BE(03C9)P(d03C9)
= Bm(y)P~(dy) for every B E r.Proposition
3.5. The conditionalexpectation if
itexists,
isdefined uniquely
a. e. modP,~.
Proof. We assume that there exist two conditional
expectations
mj E andm1(x0) # m2(x0)
at somepoint
x0 andNP~(x0)
> 0. Set=
~r~,2(x).
We have :f8
= 0 for every B E r. Toobtain the
contradiction,
it is sufficient to use Theorem 2.3.As there is no
analogue
of theRadon-Nikodym
theorem in the non-Archimedean case
[17j, [18], [19],
it mayhappens
that a conditional expec- tation does not exist.Everywhere
below we assume thatm(y)
= =y]
is well defined and moreover, that it
belongs
to the classCb(Y) .
Proposition
3.6.Let 03BE :
03A9 ~Qp,
~ H ~ Y be randomvariables,
and~’
E . Theequality
= =
~(~)1 (15)
holds
for
everyfunction f
ECb(Y).
Proof.
By Proposition
3.2 we obtain =where
z(w)
=(~(w), ~(w}).
Set for A EB(Y)
,03BB(A) =
QpY xiA(y)Pz(drdy).
As =
~-1(A)03BE(03C9)P(d03C9)
=Jy
is atight
measure on Y.Then
Qp Y
x
f (y)Pz(dxdy)
=~Y
f (y)03BB(dy)
=~Yf (y)m(y)P~(dy)
=Ef (~)m(~).
The authors
plan
toapply
the measure-theoretical frameworkdeveloped
in this paper for
studying
of the limitstheorems
random walks forp-adic probabilities (compare
with the paper[3]
in thatp-adic
random walk wasstudied on the basis of conventional
probability theory).
One of the authors
(A. Khr.)
would like to thank S. Albeverio for nu- merous discussions on foundations ofprobability theory.
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1.
Albeverio, S., Khrennikov,
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5515-5527(1996).
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Albeverio, S., Khrennikov,
A. Yu. -p-adic
Hilbert space representa- tion ofquantum systems
with an infinite number ofdegrees
of freedom. Int.J. of Modern
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1665-1673(1996).
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Albeverio, S., Karwowski, W.,
A random walk onp-adics -
the gener- ator and itsspectrum.
Stochastic ProcessAppl., 53, 1 - 22 (1994).
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Albeverio, S., Cianci, R.,
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and foundations ofquantum
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for thepublication
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Cramer,
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Prince-ton
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Department of Mathematics,
Statistics andComputer Sciences, University of Växjö, 35195, Växjö,
Sweden.Department of Information Sciences,
ScienceUniversity of Tokyo,
Noda
City,
Chiba~?’8, Japan.
Department of Mathematics, University of Nijmegen,
6525 ED