A NNALES DE LA FACULTÉ DES SCIENCES DE T OULOUSE
N ICOLAS P RIVAULT
On logarithmic Sobolev inequalities for normal martingales
Annales de la faculté des sciences de Toulouse 6
esérie, tome 9, n
o3 (2000), p. 509-518
<http://www.numdam.org/item?id=AFST_2000_6_9_3_509_0>
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- 509 -
On logarithmic Sobolev inequalities
for normal martingales(*)
NICOLAS
PRIVAULT(1)
E-mail: nprivaul@univ-lr.fr
Annales de la Faculte des Sciences de Toulouse Vol. IX, n° 3, 2000
pp. 509-518
Soit une martingale dans L4 qui satisfait la pro-
priete de representation chaotique, avec d (Zt, Zt ) = dt. On montre que les fonctionnelles positives F de satisfont l’inégalité de Sobolev logarithmique modifiee
ou D est 1’operateur gradient qui abaisse le degre des integrales stochas- tiques multiples par rapport a et C
{0,1}
est unprocessus donne par 1’equation de structure satisfaite par ’
ABSTRACT. - Let be a martingale in L4 having the chaos representation property and angle bracket d (Zt, Zt) = dt. We show that the positive functionals F of satisfy the modified logarithmic
Sobolev inequality
where D is the gradient operator defined by lowering the degree of multiple
stochastic integrals with respect to and C f 0,1~ is a
process given by the structure equation satisfied by .
~ * ~ Reçu le 17 mars 2000, accepte Ie 19 octobre 2000
~ > Departement de Mathematiques, Universite de La Rochelle, Avenue Michel Crepeau, 17042 La Rochelle Cedex 1, France
1. Introduction
The
multiple
stochasticintegrals
with respect tomartingales having
de-terministic
angle
bracket dt(i.e.
normalmartingales)
share the same or-thogonality
and normsproperties.
As a consequence, a number of commonproperties
hold for all suchmartingales,
and inparticular
for Brownian mo-tion,
thecompensated
Poisson process and Azéma’smartingales. Examples
of such
properties
are the coincidence of thedivergence
operator with the stochasticintegral
onadapted
processes(3),
the Clark formula(4),
andvariance and
spectral
gapinequalities (5). Although
the second moments of suchmartingales
are the same,higher
order moments may differ. In fact the structure of eachmartingale implies
aparticular multiplication
formula formultiple
stochasticintegrals,
see§
IV.3 of[10]
and[12],
whichcorresponds
to a
particular probabilistic interpretation
of Fock space. Inpractice,
fewproperties
of chaosexpansions
remain common to all suchmartingales,
forexample
thegradient
operator D definedby lowering
thedegree
of mul-tiple
stochasticintegrals
satisfies the chain rule of derivationonly
in theBrownian case.
The entropy of a random variable F under a
given probability
measure7r, defined as
is
independent
of the dimension of theprobability
space. The variance andentropy
operators share the sameproduct
property, cf.Prop.
2.2 of[8].
Thismakes the entropy a
good
candidate in order to statesinequalities
that areindependent
of theprobabilistic interpretation
chosen for the Fock space.Corollary
5.3 of[8] (see
also[3])
states thatwhere Y is a Poisson distributed random variable on N with mean 8 >
0,
andit is
pointed
out in[8]
that the constant 0 is the bestpossible.
Thisinequality
has been extended in
[1], [2], [13], [14],
to functionals of the Poisson process.Although
theproof
of(1)
relies on theparticularities
of the Poissonlaw,
its extension will appear to be valid not
only
on Poisson space but also fora
large family
of normalmartingales,
and distributions: the law of e.g. the Azemamartingale
is connected to the arcsinelaw,
cf.[6]
and Ch. 15 of[15].
In Sect. 2 we will show that the
proof
of modifiedlogarithmic
Sobolevinequalities
on Poisson space of[1], [2], [3], [4]
extends to thegeneral setting
of normal
martingales,
see Cor. 1. We also consider theextension,
in thecontext of normal
martingales,
of theinequalities given
in[14],
cf.Prop.
1.The case of normal
martingales satisfying
deterministic structureequations
is
given particular
attention in Sect. 3.2. Modified
logarithmic
Sobolevinequality
for normal
martingales
Let be a
martingale
such that(i)
has deterministicangle
bracketd(Zt, Zt)
= dt.We denote
by
the filtrationgenerated by
Themultiple
stochastic
integral In(fn)
is defined aswith
We assume that
(ii) (Zt)tE1R+
has the chaosrepresentation property,
i.e. every F E has a
decomposition
as F =A
martingale satisfying (i)
is called a normalmartingale
in[5].
Let D : :Dom(D)
->L2(0
xlf8+,
xdt)
denote theclosable,
unboundedgradient
operator defined aswith F =
~°° ~ In(fn).
Theadjoint
b of D is definedby
theduality
and it coincides with the stochastic
integral
with respect to forevery
predictable square-integrable
process(u(t) , cf. Prop.
4.4 of~9~ :
The Clark formula is a consequence of the chaos
representation
property forsee e.g.
~9),
and states that any F EDom(D)
c hasa
representation
It admits a
simple proof
via the chaosexpansion
of F:The Clark formula shows the
spectral
gapinequality
The
spectral decomposition
of 6D iscompletely
known in terms of multi-ple
stochasticintegrals
since =nIn(fn),
,f n
E How-ever,
apart
from the Brownian and Poisson cases, suchintegrals
may not beexpressed
aspolynomials,
see[12].
If is inL4
then the chaosrepresentation property implies
that it satisfies the structureequation
where a
predictable square-integrable
process. Let it = andjt
=1 - it
=R+ .
The continuous part of isgiven by dZf
=itdZt
and the eventualjump
of time t ER+
isgiven
as
AZt = ~t
on0~,
t EIIg+,
see~6~,
p. 70.In the
following
two cases, we have the chaoticrepresentation
property for(Zt)tER+ satisfying (6):
a)
deterministic. Then fromProp.
4 of[6],
can berepresented
aswith
(1 -
t ER+,
where is a standard Brownian motion, and a Poisson processindependent
ofwith
in-tensity
vt =fo 03BBsds, t E cf. Prop.
4 of [6].
b)
Azemamartingales where ~t
=[-2,0[,
seeProp.
6 of[6].
We now show that the modified
logarithmic
Sobolevinequality
stated in[1]
for the Poisson process extends to all normalmartingales
inL4
with thechaos
representation
property, that is inparticular
to the Azemamartingale.
We
proceed by
firststating
theanalog
of thelogarithmic
Sobolev of[13], [14].
LetPROPOSITION l. - Let F E
Dom(D)
be bounded andFT-measurable,
with F > r~
for
some ~7 > 0. We haveProof -
We follow[2]
and~14J.
LetMt
= 0 ~ t x T. We have thepredictable representation
with
Ht
=~
, 0 t T . The Ito formula for , seeProp.
2 of[6]
states that forf
EC2(JR),
If
03C6t
= 0 the terms(f(Mt-
+ -f(Mt- ))/03C6t
and( f (Mt-
+ -f (Mt-) -
have to bereplaced by
their limits as03C6t
~0,
that isHtf’(Mt-)
andZHt f"(Mt-) respectively.
Since is uni-formly
bounded from belowby
astrictly positive
constant, we mayapply
this formula to
f (~) _ ~ log ~
to obtain:where we
applied
Jensen’sinequality:
to the convex function ~ as in
[13],
and theCauchy-Schwarz inequality
to
itDtF.
oThe modified
logarithmic
Sobolevinequality
is obtained as aCorollary
of
Prop.
1.COROLLARY 1. - Let F E
Dom(D)
be bounded andFT-measurable,
with F > r~
for
some r~ > 0. We haveProof. -
Weapply Prop.
1 with theinequality
u >0,
u + v >
0,
cf.[2]
and Cor. 2.1 of[14] :
Another
proof
of(9)
consists inusing
the boundb log b -
alog
a -(b -
a)(l
+log a) (b -
a, b > 0directly
as in[2],
Th. 4.1.COROLLARY 2. - Let F E
Dom(D)
be bounded andFT-measurable,
with F > ~7
for
some r~ > 0. We haveProof.
- Weapply Prop.
1 and the bound~Y(u, v)
xv(log( u+v) -log u),
u >
0, u
+ v >0,
as in Cor. 2.2 of[14].
DFor the Azema
martingale
with parameter,~
E[-2, 0[
wehave it
= 0a.e., hence
and from Cor. 2:
3. Deterministic structure
equations
In this
section,
is a deterministicfunction,
i.e.(Zt) tER+
is writ-ten as in
(7).
In this caseit Dt
is still a derivation operator, and we have theproduct
rulecf.
Prop.
1.3 of[11].
In factDt
can be written aswhere
Llt
is the finite difference operator defined on random functionalsby
addition at time t of a
jump
ofheight 03C6t
to If0,
thisimplies
which converges to
eF DtF
as~t
--~ 0. Thefollowing proposition
extends Cor. 2.2of [14]
and Th. 2.1of [13],
which are valid for1, t
ER+.
Itcan also be viewed as a tensorisation of
logarithmic
Sobolevinequalities
forindependent
Brownian and Poisson processes.COROLLARY 3. - Let F E
Dom(D)
be bounded andFT-measurable,
with F > ~
for
some ~7 > 0. We haveProof.
Weapply
Cor. 2 and the relation03C6tDteF
= -1 )
which shows that for
positive F,
The
following corollary
is theanalog
of thesharp inequality
Cor. 5.8 of(8).
For~t
=1,
t ElI8+,
it coincides with Th. 3.4 of~13~
and Cor. 2.3 of~14~.
COROLLARY 4. - Let F E
Dom(D)
be bounded andFT-measurable,
with F > r~
for
some ~7 > 0. We haveProof.
- We use the relations F +03C6tDtF
=log( eF
+ and-
eF
:and
apply Prop.
1. DIn Cor. 4
(as
in Cor.2),
the limit of the term in~t~
as
03C6t
tends to zero is 2 times the term init : it 1 F |DtF|2dt.
If03C6t
=0,
i.e. it = 1, t E then is a Brownian motion and from Cor. 1
we obtain the classical modified Sobolev
inequality
If
~
=1~
~R+ then it
=0,~
~R+,
a standardcompensated
Poisson process and from Cor. 1 we obtain the modified Sobolev
inequality
of
[I], [2]=
Remark. -
a)
It is known thatDt
is a derivationonly
in the Brownian case, cf.[9], [12],
henceonly
in this case can the modified Sobolevinequal- ity (14)
be transformed into the standard Sobolevinequality
2E03C0[~DF~2L2([0,T])]
ofb)
It follows fromProp.
6 of[12]
that for the Azemamartingale, 03C6tDt
is not a finite difference operator, hence
(12)
and(13)
do not hold in thiscase.
Bibliography
[1] ANÉ (C.). 2014 Grandes déviations et inégalités fonctionnelles pour des processus de Markov à temps continu sur un graphe. Thèse, Université Paul Sabatier - Toulouse III, 2000.
[2] ANÉ (C.) and LEDOUX (M.). 2014 On logarithmic Sobolev inequalities for continuous time random walks on graphs. Probab. Theory Related Fields, 116(4):573-602, 2000.
[3]
BOBKOV (S. G.) and LEDOUX (M.). 2014 On modified logarithmic Sobolev inequalitiesfor Bernoulli and Poisson measures. J. Funct. Anal., 156(2):347-365, 1998.
[4]
CAPITAINE (M.), Hsu (E.P.) and LEDOUX (M.). 2014 Martingale representation and a simple proof of logarithmic Sobolev inequalities on path spaces. Electron. Comm.Probab., 2:71-81 (electronic), 1997.
[5]
DELLACHERIE (C.), MAISONNEUVE (B.) and MEYER (P.A.). - Probabilités et Poten- tiel, volume 5. Hermann, 1992.[6]
ÉMERY (M.). 2014 On the Azéma martingales. In Séminaire de Probabilités XXIII,volume 1372 of Lecture Notes in Mathematics, pages 66-87. Springer Verlag, 1990.
[7] GROSS (L.). 2014 Logarithmic Sobolev inequalities. Amer. J. Math., 97(4):1061-1083,
1975.
[8]
LEDOUX (M.). 2014 Concentration of measure and logarithmic Sobolev inequalities. InSéminaire de Probabilités XXXIII, volume 1709 of Lecture Notes in Math., pages 120-216. Springer, 1999.
[9] MA (J.), PROTTER (Ph.) and SAN MARTIN (J.). 2014 Anticipating integrals for a class
of martingales. Bernoulli, 4:81-114, 1998.
[10] MEYER (P.A.). 2014 Quantum Probability for Probabilists, volume 1538 of Lecture Notes in Mathematics. Springer-Verlag, 1993.
[11] PRIVAULT (N.). 2014 Independence of a class of multiple stochastic integrals. In Seminar
on Stochastic Analysis, Random Fields and Applications (Ascona, 1996), pages 249-
259. Birkhäuser, Basel, 1999.
[12] PRIVAULT (N.), SOLÉ (J.L.) and VIVES (J.). 2014 Chaotic Kabanov formula for the Azéma martingales. Bernoulli, 6(4):633-651, 2000.
- 518 -
[13]
WU (L.). 2014 L1 and modified logarithmic Sobolev inequalities and deviation inequal-ities for Poisson point processes. Preprint, 1998.
[14] Wu (L.). 2014 A new modified logarithmic Sobolev inequality for Poisson point pro-
cesses and several applications. Probab. Theory Relat. Fields, to appear, 2000.