A NNALES DE L ’I. H. P., SECTION B
T HOMAS G. K URTZ É TIENNE P ARDOUX P HILIP P ROTTER
Stratonovich stochastic differential equations driven by general semimartingales
Annales de l’I. H. P., section B, tome 31, n
o2 (1995), p. 351-377
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Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques
351
Stratonovich stochastic differential
equations driven by general semimartingales
Thomas G. KURTZ
(1)
Departments of Mathematics and Statistics, University of Wisconsin, Madison, Wisconsin 53706, U.S.A.
Étienne
PARDOUXMathematiques, U.R.A. 225, Universite de Provence, 13331 Marseille Cedex 3, France
Philip
PROTTER(2)
Departments of Mathematics and Statistics, Purdue University, West Lafayette, IN 47907-1395, U.S.A.
Vol. 31, n° 2, 1995, p. 377 Probabilités et Statistiques
ABSTRACT. - We
investigate
stochastic differentialequations
drivenby semimartingales
withjumps.
These areinterpreted
as Stratonovichtype
equations,
with the"integrals" being
of the kind introducedby
S.Marcus,
rather than the more well known
type proposed by
P. A.Meyer.
Weestablish existence and
uniqueness
ofsolutions;
we show the flows arediffeomorphisms
when the coefficients are smooth(not
the case forMeyer-Stratonovich differentials);
we establishstrong
Markovproperties;
and we prove a
"Wong-Zakai" type
weak convergence result when theapproximating
differentials are smooth and continuous eventhough
thelimits are discontinuous.
Key words: Stratonovich integrals, stochastic differential equations, reflection, semimar-
tingale.
A.M.S. Classification : 60 H 10, 60 H 20, 60 J 25, 60 J 60.
e)
Supported in part by NSF grant #DMS-8901464.(2 )
Supported in part by NSF grant #DMS-9103454.Annales de l’Institut Henri Poincaré - Probabilités et Statistiques - 0246-0203
Vol. 31/95/02/$ 4.00/@ Gauthier-Villars
352 T. G. KURTZ, E. PARDOUX AND P. PROTTER
RÉSUMÉ. - On considère des
equations stochastiques
differentielles ou le« bruit » est une
semimartingale quelconque (avec
dessauts).
On proposeune
interpretation
desintégrales stochastiques
dutype
« Stratonovich », mais du genre de celles introduites par S.Marcus, plutot
que du genre de celles de P. A.Meyer.
On etablit l’existence et l’unicité des solutions et on démontre que les flots sont desdiffeomorphismes quand
les coefficientssont convenables
(ce qui
n’est pas le cas pour1’ interpretation
deMeyer- Stratonovich).
Deplus
on etablit lespropriétés
de Markovfortes,
et on démontre un genre de convergence faible dutype
«Wong-Zakai » quand
les
approximants
sontréguliers
etcontinus,
meme si les limites ne sontpas continues.
1. INTRODUCTION
We
investigate
here a stochastic differentialequation
of "Stratonovichtype",
where the differentialsemimartingales
Z can havejumps.
We writethe
equation
with thecustomary
"circle" notation to indicate that it is not a standard Itotype semimartingale integral:
The
"integral"
in theequation
is a newtype
of Stratonovich stochasticintegral
withrespect
to asemimartingale
Z withjumps. (Our integral
isdifferent from the one
given by Meyer [16]
or Protter[17].) Unfortunately
we have been able to define our new
integral only
forintegrands
that aresolutions of stochastic
integral equations,
and not forarbitrary integrands.
The
equation ( 1.1 )
above isgiven
thefollowing meaning,
for the caseof scalar processes
X, Z:
.where
p(g, x)
denotes the value at time u = 1 of the solution of thefollowing ordinary
differentialequation:
We also write to denote the solution at time u; thus
(~(~) ==
x~1).
The first term on the
right
side ofequation (1.2)
is the standard Ito-semimartingale
stochasticintegral
withrespect
to thesemimartingale Z;
the second term is a
(semimartingale or) Stieltjes integral
withrespect
to theincreasing
process[Z, Z]~,
where[Z, Z]
denotes thequadratic
variationprocess of Z and
[Z, Z] ~
denotes itspath by path
continuouspart (see
Protter
[17],
p.62).
The third term is a(possibly countable)
sum of termsof order and therefore converges
absolutely (see
Section2).
Werewe to have
interpreted ( 1.1 )
as a Stratonovichequation
in the sense ofthe
semimartingale
Stratonovichintegral
as definedby Meyer [16] (see
also Protter
[17]),
theright
side of(1.2)
would have contained the first two termsonly.
The inclusion of the third term on the
right
side of(1.2)
has severalbeneficial consequences. The first
(as
we show in Section6)
is that thesolution to
( 1.1 )
is the weak limit of the solutions toapproximate equations
where the
driving semimartingales
are continuouspiecewise approximations
of the
driving semimartingale
Z(a "Wong-Zakai" type
ofresult).
The secondis that the solution remains on a manifold M whenever it starts there and the coefficients of the
equation
are vector fields over M.(This
isproved
in Section
4.)
The third(see
Section3)
is that the flows of the solution arediffeomorphisms
when the coefficients are smooth. This lastproperty
doesnot hold in
general
forsemimartingale
norStratonovich-semimartingale
stochastic differential
equations,
because(for example)
theinjectivity
fails(see
Protter[17], Chapter V, §10).
We feel that the first consequence mentioned
above,
that of the"Wong-
Zakai"
property,
isimportant
from amodelling viewpoint,
since ajump
inthe differential can be
regarded
as a mathematical idealization for a veryrapid
continuouschange.
The idea to
interpret equation (1.1) by ( 1.2)
is not new. It was introducedby
S. Marcus([13], [14])
in the case where Z hasfinitely
manyjumps
on
compact
time intervals. Thecorresponding "Wong-Zakai"
results wereinvestigated by
Kushner[12]. Recently
Estrade[4]
has studiedequations
similar to
( 1.1 )
and(1.2)
on Lie groups, and Cohen[2]
hasgiven
anintrinsic
language
for stochastic differentialequations
onmanifolds,
whichrelates to section four of this article.
Vol. 31, n° 2-1995.
354 T. G. KURTZ, E. PARDOUX AND P. PROTTER
In this paper we prove existence and
uniqueness
of a solution of(1.2),
we show the associated flow is adiffeomorphism
of(~d
in thevector case, we show the solution is a
strong
Markov process when thedriving semimartingales
Z areLevy
processes, and of course we establish"Wong-Zakai" type approximation
results for weak convergence.One notation caveat: the
ith component
of a vector x will be denotedthe jth
column vector of a matrixf
will be denotedfj,
and hencefj
stands for the(i, j )
term of the matrixf. Finally,
when themeaning
is
clear,
we use the convention ofimplicit summing
over indicesthat
iswe write ai to denote
ai).
2. DISCUSSION OF THE
EQUATION
Let
(SZ, .r ’, .~’t, P)
be aprobability
spaceequipped
with a filtration~.~’t; t > 0~
of sub-a-fields of 0. We assume the filtration satisfies the"usual
hypotheses",
i. e. it isright-continuous,
andFa
contains all P-zeromeasure sets of 0.
A process Z which has
right
continuouspaths
with left limits a.s.(known
as
"càdlàg ",
after the Frenchacronym)
is called asemimartingale
if it hasa
decomposition
Z = M +A,
where M is acàdlàg
localmartingale
andA is an
adapted, càdlàg
process, whosepaths
are a.s. of finite variation oncompacts.
For all details ofsemimartingales
the reader is referred to, forexample,
Protter[17].
A k-dimensionalsemimartingale
Z ={Z~ ~ 0~
isassumed
given
withZo
= 0.~Z, Z~ - (([Z~ Z’~~ ) )
will denote the matrix of covariations and[Z, Z] = [Z, Z]~
+[Z,
denotes itsdecomposition
into continuous and
purely
discontinuousparts. [Z]
will denote the scalarquadratic variation,
thatis, [Z] = [Zj, Zj],
with and thej=i
corresponding
continuous andpurely
discontinuousparts.
Let
f
E Given an00
measurable d-dimensional random vectorXo,
we want tostudy
anequation,
which we writesymbolically
as:and is to be understood as
Let us
explain
themeaning
of the three last terms on theright
of(2.2).
where the sum runs
from j
= 1to j
= k(we
usethroughout
the convention of summation ofrepeated indices),
is the "Itointegral"
of thepredictable process ~ f (Xt_ ) ~
withrespect
to thesemimartingale
Z.is a
Stieltjes integral
withrespect
to the continuous bounded variation processes which are the continuousparts
of thequadratic
covariation process
(cf.
Protter[ 17],
p.58).
Let usfinally
define the notationGiven g
EC1(lRd;lRd)
and x E thefollowing equation:
has a
unique
maximal solution{(~(~,~~);0 ~
u~}
andIf ~ 1,
is undefined: the solution of(2.1 ) explodes
at thecorresponding jump
time of Z. We shall bemainly
concerned with thecase where
f
isglobally Lipschitz,
in which caseXs-)
isalways
defined as a d-dimensional
Fs
measurable random vector(given
thatXs-
is
Fs-measurable).
Vol. 31, n° 2-1995.
356 T. G. KURTZ, E. PARDOUX AND P. PROTTER
For
equation (2.2)
to make sense we must show that the sum on theright
side is
absolutely convergent.
This follows fromTaylor’s
theorem: Sinceu - is
C2,
we have:for 0 E
(0, 1)
whichdepends
on(s,
w,x).
Note that the notationused
above is defined in
equation (2.3).
Thuswhich is a.s. finite since
K(w)
oo and the sum of squares of thejumps
of a
semimartingale
isalways
finite a.s.The next observation allows us to use many of the results of the well
developed theory
of stochastic differentialequations,
and it hasgreatly simplified
aprevious
version of this paper. For agiven
vectorof
semimartingales Z,
we definewhere the cv comes from the terms
0394Zs
=0394Zs(w).
We have thefollowing
obvious result:
LEMMA 2.1. - For
f
and welldefined
andLipschitz continuous,
a solution Xof equation (2.1 ), interpreted
as a solutionof
is also a solution
of
and
conversely.
3.
EXISTENCE, UNIQUENESS
AND FLOWS OF THEEQUATION
One can
study equation (2.1 ) directly (as
the authors didduring
theirpreliminary efforts),
but it is much more efficient to consider(2.5).
Wewill call an
operator
F on processes processLipschitz
as defined in Protter([17],
p.195)
if(i)
wheneverXT-
= thenF(X)T-
=for any
stopping
timeT ;
and(it) F ( X ) t - Kt ( X t - Yt ( ,
foran
adapted
process K.LEMMA 3.1. - For
f
andf’ f Lipschitz continuous,
thefunction h(s ,
úJ,x)
is process
Lipschitz. If
Z has boundedjumps,
then h is randomLipschitz
with a bounded
Lipschitz
constant.Proof. -
To show the result weapply Taylor’s
theorem to themapping
to obtain
where the last
inequality
follows from Gronwall’s lemma. Thisimplies
and the result follows.
Vol. 31, n° 2-1995.
358 T. G. KURTZ, E. PARDOUX AND P. PROTTER
Lemma 3.1 allows us to use the
already
welldeveloped theory
ofstochastic differential
equations
as found inChapter
V of Protter[17].
THEOREM 3.2. - Let
f
andf’ f be globally Lipschitz.
Then there exists acàdlàg
solution to(2.1 ),
it isunique,
and it is asemimartingale.
Proof - Rewriting equation (2.1 )
in itsequivalent
form(2.5),
we observethat
(2.5)
is a standard stochastic differentialequation
withsemimartingale
differentials
Z, [Z, Z]C,
and[Z]~,
and processLipschitz
coefficients. There is one technicalproblem:
the coefficienth( s, w, x)
is notpredictable
foreach fixed x, and does not map the collection of
càglàd (left
continuous withright limits), adapted
processes to itself. However the process[Z, Z] ~
is anincreasing,
finite variation process, and since h isoptionally
measurable for each fixed x, this does not pose aproblem.
Thus we needonly
toapply
atrivial extension of
(for example)
Theorem V.7 of Protter([ 17],
p.197)
todeduce the result. D
We can weaken the
globally Lipschitz hypotheses
of Theorem 3.1 tolocally Lipschitz, by
standardtechniques (see
e.g., Métivier[15],
Theorem34.7,
p. 246 or Protter[ 17],
pp.247-249).
We will call a functiong
locally Lipschitz
if for any n there exists a constant cn such that for allx, y E
~d
with n, n,II9(x) - g(~)~~
°COROLLARY 3.3. ,- Let
f
andf’ f
belocally Lipschitz
continuous. Then there exists astopping
timeT,
called theexplosion time,
and acàdlàg, adapted
d-dimensional process~Xt,
0 tT)
that is theunique
solutionof equation (2.1 ).
Moreover limsup ~Xt~
= 00 a. s. on the event{T ~}.
t-T
Remark. - A more
general equation
than(2.2)
is thefollowing
where J is a
càdlàg, adapted
process such that[J, Z]~
exists(in
the sensedefined in Protter
[17],
p.215),
and moreoverL |0394Js|2
oo,Os::;t,
each t >
0.Also,
ERdx(k+d)
is defined asThis
equation
can beshown, by
aslight
extension of Theorem6.5,
to bethe natural limit of
approximating equations
of the formExistence and
uniqueness
of solutions forequation (3.3)
follows as inTheorem 3.2. Note that if J is a
semimartingale,
thenequation (3.3)
can beput
into the form ofequation (2.2).
We shall restrict ourselves to the casewhere J is a
semimartingale
in this paper.Letting
the initial condition be x EIRd,
we can writeXt (x, w)
for thesolution
The
flow
of the stochastic differentialequation (3.4)
is the functionx -
Xt(x, w),
which can be considered as amapping
fromR~
for(t, w) fixed,
or as amapping
fromDd,
whereDd
denotes the space ofcàdlàg
functions fromR+
toequipped
with thetopology
of uniformconvergence on
compacts,
for w fixed.THEOREM 3.4. - Let
f
andf’ f be globally Lipschitz.
Then theflow
~ 2014~
X (z, w) from IRd to Dd is
continuous in thetopology of uniform
convergence on
compacts.
Proof. -
We can expressequation (3.4)
in theequivalent
form(2.5).
Sincef
andf’ f
areglobally Lipschitz
and h is processLipschitz,
Theorem 3.4is a
special
case of Theorem V.37 in Protter([ 17],
p.246).
DWe henceforth consider the flow of
equation (3.4)
as a function fromRd
to
IRd,
for each fixed(t, w).
Let 03A8 denote the flow: thatis,
W :Rd
isgiven by
=Xt(x, w)
for fixed(t, w),
where X is the solution ofequation (3.4).
For a
semimartingale
Z withZo
=0,
let Z = N + A be adecomposition
into a local
martingale
N and anadapted, càdlàg
process A withpaths
offinite variation on
compacts,
andNo
=Ao
= 0. For 1p
oo defineVol. 31, n° 2-1995.
360 T. G. KURTZ, E. PARDOUX AND P. PROTTER
where H ~Lp
denotes the Lp norm withrespect
to theunderlying probability
..oo
measure
.P, and ~0 |dAs denotes
the total variation of thepaths
ofA,
wby
~. Next definewhere the infimum is taken over all
decompositions
Z = N + A. We willbe
especially
interested in the 1-{oo norm. Note that if then thejumps
of eachcomponent
of Z are boundedby
~.For a
given c
>0,
and Z =( 21, ... ,
we can findstopping
times0=ToTi?2"’ tending
a.s. to 0o such thathas an norm less
than 1 ~ a
m.(See
TheoremV.5,
p. 192 of Protter[17].)
The above observation allows us to first considersemimartingale
differentials with small norm.Let
Xl (x) satisfy
where
Za e
= Outside of the interval thesolution is:
Define the
linkage operators Hj by H~ (~ j
=x j .
The next lemma is classical:
LEMMA 3.5. - Let
f
be Coo with all derivatives bounded. ThenH~
is a.s.a Coo
diffeomorphism of Rd.
Next we have the obvious result:
THEOREM 3.6. - The solution
of (3.4)
isgiven by
where ~ -
THEOREM 3.7. - Let
f
be C°° with all derivatives bounded. Theflow
W : x -
Xt(x, cv) of
the solution Xof (3.4)
is adiffeomorphism if, for
eachj,
is a
diffeomorphism.
Proof. - By
Theorem3.6,
the solution X of(3.4)
can be constructedby composition
of the functionsXj
and thelinkage operators Hj .
But thelinkage operators
arediffeomorphisms by
Lemma3.5,
and since thecomposition
ofdiffeomorphisms
is adiffeomorphism,
the theoremis
proved.
DTo show the functions x - are
diffeomorphisms
we are ableto use the results of Section 10 of
Chapter
V of Protter[17].
THEOREM 3.8. - Let
f, f’ f in (3.4)
be C°° with all derivatives bounded.> 0
suficiently small,
then thecorresponding flow W
is a
diffeomorphism of
IR.Proof. -
We rewrite theequation (3.4)
in the form(2.5). Equation (2.5)
isin the classical form with process
Lipschitz,
smooth coefficients. We then invoke Hadamard’s theorem(Theorem 59,
p.275), along
with Theorem 62(p. 279)
and Theorem 64(p. 281)
of Protter[17]
to deduce the result. DCombining
Theorems 3.7 and3.8,
we have:THEOREM 3.9. - Let
f in (3.4)
be C°° with all derivativesof f
andf’ f
bounded. Then theflow ~ :
z -Xt(x, cv) of
the solution X is adiffeomorphism of ~d.
4. A CHANGE OF VARIABLE FORMULA AND MANIFOLD-VALUED SOLUTIONS
One could argue that even the Stratonovich
integral
for Brownian motion should not be called an"integral",
since it does notsatisfy
aminimally acceptable
"dominated convergencetheorem",
as does - forexample -
thesemimartingale "Ito-type" integral.
However our"integral"
is even less ofan
integral
than theMeyer-Stratonovich integral,
since it isonly
defined forintegrands
which are solutions of stochastic differentialequations.
Vol. 31, n° 2-1995.
362 T. G. KURTZ, E. PARDOUX AND P. PROTTER
Nevertheless there are circumstances under which we can establish a
change
of variables formula. Let X denote a solution of(2.1).
We willestablish
for g
E that we can define anintegral
for t >
0,
which we call the Stratonovichintegral
ofg(X)
withrespect
to Z.(Note
that this definition is not consistent with that ofMeyer [16]
and Protter[17],
when Z hasjumps; however,
it agrees with theintegral originally proposed by
Stratonovich for Brownian motion. Also allgeneralizations
of the Stratonovichintegral
agree when Z iscontinuous.)
For d E N and
f
E we shall say that the d-dimensional process Xbelongs
to if there exists a d-dimensionalF0-
measurable random vector
Xo
such that:DEFINITION 4.1. - Let d E
N,
X E~‘~(Z, f )
and g E Wedefine the Stratonovich
integral
of the row vectorg(X)
withrespect
to Z as follows:The first two terms on the
right
side of the above formula should be clear from the usual definition of Stratonovichintegrals. However,
the lastterm merits some comment.
First,
note that each term in the sum is of the orderof
so that the sum converges. Furthermore thatexpression
tells us that:
This formula can be
interpreted
as follows. At eachjump
time ofZ,
weopen a unit
length
interval of "fictitioustime",
over which theintegrand
varies
continuously
fromg(Xt_ )
tog(Xt),
and thejump
of theintegral equals
thejump
of thedriving semimartingale multiplied by
the mean ofalong
the curvejoining Xt-
toXt.
We can now state and prove the associated
change
of variable formula:PROPOSITION 4.2. - Let d E
N, f
E Xe ~(~/).
and~ E We then have:
Proof. -
We know that X is asemimartingale
and that:We
plug
theseexpressions
into the Ito formula:It is then easy to check that this
expression
coincides withwith the
help
of Definition4.1.
B DNow let M be a
C2
manifold withoutboundary
embedded inRd,
andassume that
E are vector fields over M. It is then
intuitively
clear
that, starting
onM,
the solution X shouldstay
on M.Indeed,
betweenjumps,
itobeys
a continuous Stratonovich differentialequation,
andVol. 31, n° 2-1995.
364 T. G. KURTZ, E. PARDOUX AND P. PROTTER
maps M onto M.
However,
since there can beinfinitely
manyjumps
ina
compact
timeinterval,
the aboveargument
does notimmediately imply
that X
stays
on M.Suppose
that the dimension of M is. f d.Locally,
one canfind a
C2
chart p s.t. ..., are coordinates onM,
and... = = 0 if and
only
if x E M. The desired result then follows fromProposition 4.2, by using
the sameargument
as for ODE’s(see,
forexample,
Hirsch[7],
pp.149-152).
"
PROPOSITION 4.3. - Let M be a
C2 manifold
withoutboundary
embeddedin
IRd,
and suppose x E are vectorfields
over M.Then
P(Xo
EM)
= 1implies
thatP(Xt E M, t > 0)
= 1. D5. STRONG MARKOV PROPERTY
In the usual
theory
of stochastic differentialequations,
if Z is aLevy
process
(i.e.,
a process withstationary
andindependent increments),
and iff :
isLipschitz,
then the solution ofis
strong
Markov(see
Protter[ 17],
p.238). Recently
the converse hasbeen shown:
Suppose f
never vanishes and let X~ denote the solution with initial conditionXo
= x. If the processes X~ are timehomogeneous
Markov with the same transition
semigroup
for all x, then Z is aLevy
process
(see
Jacod-Protter[6]).
We have the same Markovproperty
for solutions with ourStratonovich-type
differentials.THEOREM 5.1. - Let
f
andf’ f be globally Lipschitz,
let Z be aLevy
process, and let
Xo
beindependent of
Z. Then the solution Xof
is
strong
Markov.Proof. -
We rewriteequation (5.2)
as in(2.5)
as:Note that
[Z, Z]~
= at for some constant a because Z is aLevy
process(see,
e.g., Theorem V.33 of Protter[17],
p.239);
thus[Z, Z]"
istrivially
alsoa
Levy
process. Oneeasily
verifies that[Z]d
is also aLevy
process. Thusequation (5.3)
falls within the "classical"province,
where theequation
isdriven
by Levy semimartingales.
The coefficientsf
andf’ f
areLipschitz,
and h is process
Lipschitz.
There is one technicalpoint:
for fixed x,is not
predictable;
it isoptional.
Moreover for fixed x it does not mapcàglàd (left
continuous withright limits)
processes intocàglàd
processes;
however,
the differential forh, c![~]~,
is anincreasing,
finitevariation process, and thus the established
theory trivially
extends to thiscase.
Adopting
the framework of(~inlar-Jacod-Protter-Sharpe [ 1 ],
we note thatthe coefficients
f , f’ f ,
and h arehomogeneous
in the sense of[ 1 ];
seepage 214.
(The
coefficientsf
andf’ f , being deterministic,
are of coursetrivially homogeneous.)
The result now follows
by
astraightforward
combination of thetechnique
used to prove Theorem V.32 of Protter
([17],
p.288) (where
thecoefficients are
non-random),
and thetechnique
used to prove Theorem 8.11 of(~inlar-Jacod-Protter-Sharpe ([1],
p.215),
where the coefficients arehomogeneous.
D6. "WONG-ZAKAI" TYPE APPROXIMATIONS BY CONTINUOUS DIFFERENTIALS
Wong
and Zakai[ 18]
consider differentiableapproximations
of Brownian motion and show that the solutions ofordinary
differentialequations
drivenby
these smoothapproximants
converge to the solution of ananalogous Stratonovich-type
stochastic differentialequation
drivenby
the Brownianmotion,
and not to the solution of thecorresponding Ito-type equation.
Theirresult has
undergone
manygeneralizations, culminating
in Kurtz-Protter[9],
Vol. 31, n° 2-1995.
366 T. G. KURTZ, E. PARDOUX AND P. PROTTER
where the Brownian differentials are
replaced by general semimartingales.
In Kurtz-Protter
[9], however,
and in all other treatmentsinvolving semimartingales
withjumps,
theapproximating
differentials must also havejumps,
since convergence is in the Skorohodtopology;
and the limit of continuousapproximants
in either the uniform or Skorohodtopologies
mustbe continuous. Here we
approximate
thegeneral semimartingale
differentials with continuousapproximants,
eventhough
theoriginal semimartingale
differentials may have
jumps.
Thelimiting equation
is then of thetype
introduced above. This resultgives
ajustification
for the use of ourintegral
when one ismodelling
verysudden, sharp changes
in anessentially
continuous
system.
For
simplicity
we consider the case where Z is a one-dimensionalsemimartingale.
Ageneralization
tosystems
ofequations
drivenby
vector-valued
semimartingales
ispossible
withappropriate assumptions.
We define the
approximating semimartingales by
for h > 0. Then
Zh
isadapted, continuous,
and of finite variation oncompacts.
Moreover limZt
=Zt-
a.s., each t > 0.Let
f :
R - R andf’
be bounded andLipschitz continuous,
and letX h
denote the
unique
solution of:We want to show that
X h
converges, in anappropriate
sense, to the solution X of theequation
introduced above. Note that
X h
is continuous while X may havediscontinuities,
so convergence in the Skorohodtopology
will not, ingeneral,
hold. Thetype
of convergence we will establish is that studied in Kurtz[8].
Inparticular,
we will show the existence of a sequence of time transformations Th for whichYh (t)
=X:h (t)
satisfies(Yh, Th )
-(Y, T)
inthe
compact
uniformtopology
andX (t)
=The new time scale we introduce includes the "fictitious time"
during
which the solution follows the vector field
f
to form thejump.
DefineThen lh
isstrictly increasing (since [Z]d
isincreasing), continuous,
andadapted.
We also definewhich is also
strictly increasing
andadapted, although
not continuous.Note that
For each
h,
the desired timechange
isgiven by
the continuous inverseThen for
all h 2: 0, 7/~(~)
is astopping
time for each t andyyz 1
iscontinuous. For h >
0,
isstrictly increasing and, hence,
is the inverse of Note that eachdiscontinuity AZ(t)
of Zcorresponds
to an intervalof
length
on which is constant. Note also that03B3-10 o 03B30(t)
= t, and ~yo o
-yo 1 (t) > t
forall t 2:
0.The
time-changed driving
processis continuous and has
paths
of finite variation oncompacts,
sinceZh
does.The
time-changed
solution ’is then the
unique
solution ofWe next establish several
preliminary
results.LEMMA 6.1. - For each h > 0 and t >
0,
h andhence, limh~0 03B3-1h(t)
=uniformly
in t.Proof. -
The lemma follows from the observation that+
h).
DVol. 31, n° 2-1995.
368 T. G. KURTZ, E. PARDOUX AND P. PROTTER
To
identify
the limit of the processesVh
defineand
Note that = unless Z has a
discontinuity
at03B3-10 (t)
and that03B3-10
is constant on(t), ~2(t)].
V is thesemimartingale
Ztime-changed according
toexcept
when Zjumps.
At thejump-times
ofZ,
weadd
"imaginary"
time intervals(t),
’r/2(t)~
oflength During
theseintervals V is defined
by
linearinterpolation
over thediscontinuity
of Z.Note that if
]
oo a.s., for each t >0,
then it is clear that V can beinterpreted
as asemimartingale. However,
since it ispossible
tohave
L I
= oo a.s.,every t
>0,
these linearinterpolations
can0st
have infinite
length
even oncompact
timeintervals,
and V need not be asemimartingale.
In all cases,however,
V is a continuous processadapted
to the filtration
LEMMA 6.2. - lim
Vh
=V, uniformly
on bounded intervals.h>0
Proof -
We need to show that 0and th
2014~imply Yth 2014~.
IfZ is continuous at
~yo 1 (t),
thatis,
if(t)
=r~2 (t),
the limit will holdby
Lemma 6.1. Assume that Z has a
discontinuity
at orequivalently,
that
’r/1(t) # ri2 (t). By (6.1), along
asubsequence satisfying
= In
particular, V h o~,_ 1 t ~
andr~l (t). Along
asubsequence satisfying ~o _1 (t),
=
Z ~ro -1 (t)
Notealso,
that +h)
-r~2 (t) .
Observe that
and
It follows that
uniformly
in usatisfying yh 1 (u) 1’ol(t) + h
which is thederivative
of Vt
in(r~l (t), r~2(t)~. Consequently, along
anysubsequence satisfying ’Yo 1 (t) ’Yh 1 (th)
C’Yo 1 (t)
+tz, 01’01 ~t) ~
~~t - W ~t~~
and hence
Before
continuing
we need to introduce aconcept
from Kurtz-Protter[10].
DEFINITION. - For each n let Zn be a
semimartingale
withrespect
toa filtration
{~?},
and suppose that Z" converges in distribution in the Skorohodtopology
to a process Z. Then the sequence(zn, (0? ) )
is saidto be
good
if Z is asemimartingale
and for anyHn, càdlàg
andadapted
to
(0§°),
such that(Hn, Zn)
converges in distribution to(H, Z)
in theSkorohod
topology,
converges in distribution in the Skorohodtopology
Anecessary to
and sufficient condition for aconvergent
sequence ofsemimartingales
Z" to begood
was obtained in Kurtz-Protter[9,10].
Let(1 - ~/r)+,
and defineJs: (0)
-(0) by
Let
Then has
jumps
boundedby
8. LetVol. 31, n° 2-1995.
370 T. G. KURTZ, E. PARDOUX AND P. PROTTER
be any
decomposition
of into a localmartingale Mn,6
and anadapted, càdlàg,
finite variation process The condition for"goodness"
of thesequence {Zn}
is that for each n, there exist suchdecompositions satisfying (*)
For each a >0,
there existstopping
timesTflfi
such thatand
Note that if Zn = Z for each n, then the sequence is
good. Furthermore,
since t for all tand h,
the~.~’~,- ~ ~t~ ~ ) , h
>0}
is
good.
weregood,
then we couldapply
Theorem 5.4 of Kurtz and Protter[9]
to conclude that the solution of(6.5)
converges.Unfortunately,
not
only
is not ingeneral
agood
sequence, the limit V is not ingeneral
asemimartingale.
To address thisproblem,
we first defineand rewrite
(6.5)
asNote that
by
Lemma 6.2 and the fact that7~M
converges tofrom
above,
we haveIn
addition,
the convergence ofUh
to U is in the Skorohodtopology.
Following
thegeneral approach
toWong-Zakai-type
theorems taken inKurtz and Protter
[9],
weintegrate
the last termby parts
to obtainSince
yh
is continuous and of finite variation andf
isC1,
= 0.Consequently,
With the last term in
(6.12)
inmind,
we prove thefollowing
lemma.t
LEMMA 6.3. - The sequence
of semimartingales At
=~
isgood,
andwhere the convergence is in
probability
in the Skorohodtopology.
Proof. - At
can be writtenand
substituting u = -yh 1 (s),
we have[using (6.8)]
It is easy to see that if a sequence of
semimartingales
definedon the same space and
converging
inprobability (not just
indistribution)
is
good
for oneprobability
measureP,
then it is alsogood
for any otherprobability Q equivalent
toP,
because ifQ
P,
then convergence inP-probability implies
convergence inQ-probability.
Thus without loss ofgenerality, by changing
to anequivalent probability
measure if necessary(see
Dellacherie andMeyer [3],
p.251),
we can assume that Z is in7~;
thatis,
Z has a canonicaldecomposition
Z = M +A,
whereE [M, M]t + t0|dAs|}
2
oo, for any finite time t.
Vol. 31, n° 2-1995.
372 T. G. KURTZ, E. PARDOUX AND P. PROTTER
To
verify goodness
of the sequence in(6.13),
we estimate the total variation.giving
a bound on theexpected
total variation that isindependent
of h. Weconclude that
(*)
issatisfied,
and hence we havegoodness.
To
identify
the limit of we useintegration by parts
to obtainBy
the definition ofUh
and Lemma6.2,
theright
side converges toSince U vanishes off of the intervals on which
1’01
is constant, the lastterm in
(6.14) vanishes, completing
theproof
of the lemma. DFinally,
we need to show that the first term on theright
of(6.12)
isrelatively compact.
LEMMA 6.4. - The
relatively compact
in the senseof
convergence in distribution in the Skorohodtopology.
Proof. -
To show relativecompactness,
it is sufficient to show that everysubsequence
has a furthersubsequence
that converges. Let be the times at which Z has ajump.
The boundedness off
andf’,
the"goodness"
of~Z~,h ~ ~
and~Ah~,
and the fact that~~
converges, ensure thatsup Yht
isstochastically
bounded. For any sequence{hn}, hn
-70,
tT
there will be a further
subsequence along
which(~(r~~~(T~’ ...)
converges in distribution Denote the limit
by (Yl , Y2, ... ) .
For~ ~ ~
+h )
and
It follows that
00
where p is defined in Section 2. Let
rh = U [’)’h( Ti), 1’h( Ti
+h)).
Then~==1
for each T >
0,
lim supI Uth
= 0.Noting
that =tE[0,T]-rh
and
(T~
+h)
- 1’0(r2 ~
= 1}2( ’)’0 (~’z ~ ) ~
it follows thatalong
thesubsequence, R,
where(6.15) R(t) = Ibo(Ti-);-YO(Ti)) (t)f
cpf b..ZTi> Yi, Ut
completing
theproof
of the lemma. DWe can now
apply
Theorem 5.4 of Kurtz and Protter[9]
to conclude that isrelatively compact
in the sense of convergence in distribution in the Skorohodtopology
and that any limitpoint
mustsatisfy
where
R(t, Y)
isgiven by (6.15)
andA°
is defined in Lemma 6.3.Vol. 31, n° 2-1995.
374 T. G. KURTZ, E. PARDOUX AND P. PROTTER
Substituting
forA°
in(6.16)
andwriting [Z] =
+[Z] c,
we obtainRecall that
Ut
= 0 unless# 1]2 ( t)
and that ifqi (t) # 1/2 ( t ),
Note
that -2(U2 - [Z]d)
isabsolutely
continuous andnondecreasing,
andits derivative is
With Ti as in
(6.15 ) and Yi
= we have for t EObserve that the solution of
(6.19)
on the interval[~o(~~)?7o(~))
is
unique given Y ,
anddifferentiating,
it is easy to check thatYt
=B J 0394Z03C4i, }i,
|0394Z03C4i|2
/. It follows that