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Markov uniqueness of degenerate elliptic operators

DEREKW. ROBINSON ANDADAMSIKORA

Abstract. Let!be an open subset ofRdand H! =!d

i,j=1ici jj be a second-order partial differential operator onL2(!)with domainCc(!), where the coefficientsci j W1,(!)are real symmetric andC =(ci j)is a strictly positive-definite matrix over!. In particular,H!is locally strongly elliptic. We analyze the submarkovian extensions ofH!,i.e., the self-adjoint extensions that generate submarkovian semigroups. Our main result states that H!is Markov unique,i.e., it has a unique submarkovian extension, if and only if cap!(∂!)=0 where cap!(∂!)is the capacity of the boundary of!measured with respect to H!. The second main result shows that Markov uniqueness ofH!is equivalent to the semigroup generated by the Friedrichs extension ofH!being conservative.

Mathematics Subject Classification (2010):47B25 (primary); 47D07, 35J70 (secondary).

1. Introduction

The Markov uniqueness problem [9] consists of finding conditions which ensure that a diffusion operator has a unique submarkovian extension, i.e. an extension that generates a submarkovian semigroup. An operator with this property is said to be Markov unique. Our aim is to analyze this problem for the class of second-order, divergence-form, elliptic operators with real Lipschitz continuous coefficients act- ing on an open subset of ! ofRd. Each of these operators has at least one sub- markovian extension, the Friedrichs extension [16]. This extension corresponds to Dirichlet boundary conditions on∂!and alternative boundary conditions can lead to different submarkovian extensions. Our principal results establish that Markov uniqueness is equivalent to the boundary∂!having zero capacity, Theorem 1.2, or to conservation of probability, Theorem 1.3.

DefineH!as the positive symmetric operator onL2(!)with domainD(H!)= Cc(!)and action

H!ϕ=−

"d i,j=1

ici jjϕ=−

"d i,j=1

ci jijϕ

"d i,j=1

(∂ici j)∂jϕ (1.1)

Received February 4, 2010; accepted May 26, 2010.

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where theci j =cjiW1,(!)are real,C =(ci j)is a non-zero, positive-definite matrix over!andi = ∂/∂xi. We assume throughout thatC(x) =(ci j(x)) > 0 for allx!. This ensures thatH!is locally strongly elliptic,i.e.for each compact subset K of ! there is aµK > 0 such that C(x)µKI for allxK. This ellipticity property is fundamental as it ensures that the various possible self-adjoint extensions of H!differ only in their boundary behaviour (see Section 2).

The Markov uniqueness problem has been considered in a variety of contexts (see [9] for background material and an extensive survey). It is related to a number of other uniqueness problems. For example, the operatorH!, which can be viewed as an operator on Lp(!)for each p∈[1,∞], is defined to beLp-unique if it has a unique extension which generates anLp-continuous semigroup. In particularH!

is L2-unique if and only if it is essentially self-adjoint (see [9, Corollary 1.2]).

Then the self-adjoint closure is automatically submarkovian and H! is Markov unique. Moreover, ifH!isL1-unique then it is Markov unique [9, Lemma 1.6]. In Theorem 1.3 we will establish a converse to this statement for the class of operators under consideration. As a byproduct of our analysis of Markov uniqueness we also derive criteria for various other forms of uniqueness.

In the sequel we extensively use the theory of positive closed quadratic forms and positive self-adjoint operators (see [21, Chapter 6]) and the corresponding the- ory of Dirichlet forms and submarkovian operators (see [4, 15, 23]). First we intro- duce the quadratic formh!associated withH!by

h!(ϕ)=

"d i,j=1

#

!

dx ci j(x) (∂iϕ)(x)(∂jϕ)(x) (1.2) with domain D(h!) = D(H!) = Cc(!). The form h! is closable with re- spect to the graph normϕ %→ 'ϕ'D(h!) = (h!(ϕ)+'ϕ'22)1/2and its closureh!

is a Dirichlet form. The positive self-adjoint operator corresponding to h! is the Friedrichs extension H!F of H!. It is automatically submarkovian. Moreover, it is the largest positive self-adjoint extension of H!with respect to the usual ordering of self-adjoint operators. Krein [22] established thatH!also has a smallest positive self-adjoint extension. But the Krein extension is not always submarkovian. For ex- ample, if!is bounded the Krein extension of the Laplacian restricted toCc(!)is not submarkovian (see [15, Theorem 3.3.3]). Our first aim is to establish that H!

also has a smallest submarkovian extension. Then the Markov uniqueness problem is reduced to finding conditions which ensure that this latter extension coincides with the Friedrichs extension (see [9, Chapter 3]).

Definel!by setting l!(ϕ)=

#

!

dx

"d i,j=1

ci j(x) (∂iϕ)(x)(∂jϕ)(x) (1.3) where the iϕ denote the distributional derivatives and the domain D(l!) of the form is defined to be the space of allϕWloc1,2(!)for which the integral is finite.

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It is clear thatl! is an extension of h! but it is not immediately obvious thatl!

is closed and that the corresponding operator L! is an extension of H!. These properties were established in [15] for operators of the form (1.1) but with smooth coefficients. Our first result is a generalization for operators with Lipschitz coeffi- cients which also incorporates some regularity and domination properties.

Recall that the positive semigroupSt is defined to dominate the positive semi- groupTt ifStϕTtϕfor all positiveϕL2(!)and allt >0. Moreover,D(k!)is defined to be an order ideal of D(l!)if the conditions 0≤ϕψ,ψD(k!)and ϕD(l!)implyϕD(k!). (See [24], Chapter 2, for these and related concepts.) Theorem 1.1. Let!be an open subset ofRd andH! = −!d

i,j=1ici jj be a second-order partial differential operator on L2(!)with domainCc(!), where theci jW1,(!)are real symmetric andC(x)=(ci j(x)) >0for allx!.

Then the following are true.

I. l!is a Dirichlet form andD(l!)C(!)is a core ofl!.

II. The submarkovian operatorL!associated withl!is an extension ofH!. III. IfK!is any submarkovian extension of H!andk!the corresponding Dirich-

let form thenl!k!h!. Therefore0≤ L!K!H!F in the sense of operator order.

IV. IfK!is any self-adjoint extension ofH! thenCc(!)D(K!)D(H!)and ifK!is a submarkovian extension thenCc (!)D(k!)D(h!).

V. If K! is a submarkovian extension of H! then D(h!) is an order ideal of D(k!)andet K! dominateset H!F. Moreover,et L!dominateset K! if and only ifD(k!)is an order ideal ofD(l!).

The first three statements are a generalization of [15, Lemma 3.3.3 and Theo- rem 3.3.1]. They establish that the operator L! is the smallest submarkovian ex- tension of H!, but not necessarily the smallest self-adjoint extension. The fourth statement is an interior regularity property. It establishes, in particular, that every submarkovian extension ofH!is a Silverstein extension in the terminology of [30]

(see [9, Definition 1.4]).

The third statement of the theorem implies that H! is Markov unique if and only ifl! = h!,i.e.if and only if D(l!) = D(h!). It is this criterion that has been used extensively in the analysis of the Markov uniqueness problem (see [2]

[15] and [9, Chapter 3]). But the fourth statement implies that all the Dirichlet form extensions coincide in the interior of !and consequently differ only on the boundary. Our first criterion for Markov uniqueness is in terms of the capacity of the boundary.

The (relative) capacity of a measurable subset A!is defined by cap!(A)=inf$

'ψ'2D(l!) :ψD(l!)and there exists an open set U ⊂Rd such thatUAandψ =1 a. e. onU!

%

. (1.4)

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Thus cap! is directly related to the capacity occurring in the theory of Dirichlet forms [4, 15].

Theorem 1.2. Under the assumptions of Theorem1.1, the following conditions are equivalent:

I. H!is Markov unique, II. cap!(∂!)=0.

It should be emphasized that there is no comparable geometric or potential-theoretic characterization of essential self-adjointness, i.e. L2-uniqueness. Folklore would suggest thatH!isL2-unique if and only if the Riemannian distance to the boundary

∂!, measured with respect to the metricC1, is infinite. But this is not true in dimension one (see Example 6.5).

Our second result on Markov uniqueness is based on a conservation property.

The submarkovian semigroupStF generated by the Friedrichs extensionH!F is de- fined to be conservative onL(!)ifStF11!=11!for allt ≥0.

Theorem 1.3. Adopt the assumptions of Theorem1.1. LetStFdenote the semigroup generated by the Friedrichs extension H!F ofH!.

The following conditions are equivalent:

I. H!is Markov unique, II. StF is conservative, III. H!is L1-unique.

The implications II⇔III⇒I are already known under slightly different hypothe- ses. The equivalence of Conditions II and III was established by Davies [7, Theo- rem 2.2], for a different class of second-order operators with smooth coefficients.

His proof is based on an earlier result of Azencott [3]. The implication III ⇒ I is quite general and is given by [9, Lemma 1.6]. Moreover, the implication I ⇒ II follows from [9, Corollary 3.4], if|!| < ∞. The proof of this implication for general!is considerably more complicated (see Section 5). In the broader setting of second-order operators acting on weighted spaces considered in [9] this impli- cation is not always valid. The weights can introduce singular boundary behaviour (see [9, Remark following Corollary 3.4]).

Combination of the foregoing theorems gives the conclusion that Markov uniqueness, L1-uniqueness and the conservation property are all characterized by the capacity condition cap!(∂!)=0. This is of interest since the latter condition can be estimated in terms of the boundary behaviour of the coefficientsci jand the geometric properties of∂!. In Section 4 we derive estimates in terms of the order of degeneracy of the coefficients and the Minkowski dimension of the boundary (see Proposition 4.2).

The proofs of Theorems 1.1, 1.2 and 1.3 will be given in Sections 3, 4 and 5, respectively. In Section 6 we demonstrate that versions of the capacity estimates also give sufficient conditions forLp-uniqueness for all p∈[1,2]and we establish that the semigroupStF is irreducible if and only if!is connected.

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ACKNOWLEDGEMENTS. Our interest in the characterization of operator extensions by their boundary behaviour originated in a series of interesting discussions with Ricardo Weder and Gian Michele Graf whilst the first author was visiting the Institut f¨ur Theoretische Physik at the Eidgen¨ossische Technische Hochschule, Z¨urich in 2007. The author is indebted to J¨urg Fr¨ohlich and Gian Michele Graf for facilitating this visit and to the ETH for providing financial support. Both authors are grateful to Michael R¨ockner and Masayoshi Takeda for comments on an earlier draft of the paper.

2. Elliptic regularity

In this section we derive some basic regularity properties of the operators H!de- fined by (1.1). Since H! is symmetric its adjoint H! is an extension of its clo- sure H! and the domain D(K!)of each self-adjoint extension K! of H! satis- fies D(H!)D(K!)D(H!). The principal observation is that D(H!)and D(H!)only differ on the boundary∂!. Hence the various possible extensions are distinguished by their boundary behaviour.

The comparison ofD(H!)andD(H!)can be articulated in various ways but it is convenient for the sequel to express it as a multiplier property.

Theorem 2.1. Adopt the assumptions of Theorem 1.1. Then Cc (!)D(H!)D(H!).

Proof. The principal step in the proof consists of establishing that D(H!)Wloc1,2(!). Once this is achieved the rest of the proof is given by the following argument.

Let !0 be a bounded open subset of! which is strictly contained in !, i.e.

!0!. (Strict containment will be denoted by!0 ! !.) IfψD(H!)and D(H!)Wloc1,2(!)thenψW1,2(!0). Setξ = H!ψthenξL2(!0)and

"d i,j=1

(ci jjη,∂iψ)=(η,ξ)

for allηCc(!0),i.e.ψ is a weak solution of the elliptic equationH!0ψ =ξ on

!0. Since H!0 is strongly elliptic on L2(!0)it follows by elliptic regularity (see, for example, [20] Theorem 8.8) thatψW2,2(!00)for all!00 ! !0. ThusψWloc2,2(!0)Wloc2,2(!). Therefore D(H!)Wloc2,2(!). Hence ifηCc(!)then η ψW02,2(!). ButW02,2(!)D(H!), because the coefficients are bounded, and the statement of the theorem is established.

It remains to prove thatD(H!)Wloc1,2(!).

First, fixηCc(!)and setK =suppη. Next let!0 !!be a bounded open subset which contains K. Sinceci jW1,(!)andC(x) > 0 for all x!the restrictionH!0of H!toCc (!0)is strongly elliptic.

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Secondly,ϕD(H!)if and only if there is ana>0 such that

|(ϕ,H!ψ)|≤a'ψ'2

for allψCc(!). In particular ifϕD(H!)then these bounds are valid for all ψCc(!0). Thus the restriction 11!0ϕofϕto!0is inD(H!0)andH!0(11!0ϕ)= 11!0(H!ϕ). Butη ϕ = 11!0(η ϕ)= η(11!0ϕ). In particular ifη(11!0ϕ)D(H!0) thenη ϕD(H!). ThusηD(H!)D(H!)if and only ifηD(H!0)D(H!0) for all possible choices of η and !0. Therefore it suffices to prove D(H!0)Wloc1,2(!0)for the strongly elliptic operator H!0 on L2(!0)for all bounded open subsets!0!!.

Thirdly, we extend H!0to a strongly elliptic operatorLonL2(Rd)with coef- ficientscˆi jW1,(Rd)such thatH!0 = L|Cc(!0). This is achieved in two steps.

Since theci j are continuous on!,C(x)µI for allx!0 andC(x) > 0 for all x!one may choose an!00 such that!0 ! !00 ! ! andC(x)(µ/2)I for all x!00. Then one may choose aχC(Rd) such that 0 ≤ χ ≤ 1, χ(x) = 1 if x!0 and χ(x) = 0 if x is in the complement of!00. Then set

&

C = χC+(1χ) (µ/2)I. It follows thatC& ≥ (µ/2)I. Now let L be the di- vergence form operator on L2(Rd)with the matrix of coefficientsC&=(cˆi j). It is strongly elliptic,cˆi jW1,(Rd)andL|Cc (!0) = H!0by construction. Therefore the proof is completed by the following lemma.

Lemma 2.2. Let H!0 = L|Cc(!0) where L is a strongly elliptic operator, with coefficientscˆi jW1,(Rd), acting onL2(Rd). Then D(H!0)Wloc1,2(!0).

Proof. The proof exploits some basic properties of strongly elliptic operators with Lipschitz continuous coefficients summarized in Proposition A.1 of the appendix.

In particular Lis essentially self-adjoint onCc(Rd)and its self-adjoint closure L has domainD(L)=W2,2(Rd).

Let D(!0) denote Cc (!0) equipped with the Frechet topology and D0(!0) the dual space, i.e. the space of distributions on !0. If ψL2(!0)then ϕCc(!0)%→ (ψ,H!0ϕ)is a continuous linear function overD(!0). Thus for each ψL2(!0)there is a distributionH!0(ψ)D0(!0)such that

(H!0(ψ),ϕ)=(ψ,H!0ϕ)

for allϕCc(!0). Similarly for eachψL2(Rd)there is a distributionL(ψ)W2,2(Rd), the dual ofW2,2(Rd), such that

(L(ψ),ϕ)=(ψ,Lϕ) for allϕCc(Rd). But by assumption

(ψ,H!0ϕ)=(ψ,Lϕ)=(L(ψ),ϕ)

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for allψL2(!0)and allϕCc(!0). Therefore (H!0(ψ),ϕ)=(L(ψ),ϕ)

for allϕCc(!0). In particularψD(H!0)if and only ifL(ψ)L2(!0).

Next fix ψD(H!0). Then L(ψ)L2(!0). Moreover, ifηCc(!0) thenη ψD(H!0)if and only ifL(η ψ)L2(!0). But one has the distributional relation

L(η ψ)=ηL(ψ)+L(η)ψ+(η (2.1) where

(η=−2

"d i,j=1

ˆ

ci j(∂jη) (∂iψ) .

Sinceψ,L(ψ)L2(!0)andη,L(η)L(!0)it follows that the first two terms on the right of (2.1) are inL2(!0). But there is ana>0 such that

|((η,ϕ)|≤a'ψ'2'ϕ'1,2

for all ϕCc(Rd) where '· '1,2 denotes the W1,2-norm. Therefore (ηW1,2(Rd), the dual of W1,2(Rd). Hence it follows from (2.1) that L(η ψ)W1,2(Rd). But

η ψ =(I +L)1η ψ+L(I+L)1η ψ =(I +L)1η ψ +(I +L)1L(η ψ) andη ψW1,2(Rd)by Proposition A.1.III of the appendix applied to the strongly elliptic operatorL. SinceηCc(!0)it follows thatη ψW01,2(!0).

Finally let K be an arbitrary compact subset of!0. If η1Cc(!0) with η1 = 1 on K it follows thati1ψ)|K = iψ|K. Thus iψL2(K) for all i ∈{1, . . . ,d}. ThereforeψWloc1,2(!).

One can also draw a conclusion about the domain of a general self-adjoint extension ofH!and partially establish Statement IV of Theorem 1.1.

Corollary 2.3. If K! is any self-adjoint extension of H! thenCc(!)D(K!)D(H!).

Proof. SinceD(H!)D(K!)D(H!)one hasCc(!)D(K!)Cc(!)D(H!)D(H!)by Theorem 2.1.

Note that D(H!)D(H!)Wloc2,2(!). ThereforeCc(!)D(K!)D(H!)D(K!)Wloc2,2(!)for each self-adjoint extensionK!.

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3. The minimal Markov extension

In this section we prove Theorem 1.1. The proof of the first parts of the theorem broadly follows the reasoning used in [15] to prove the analogous result, Theo- rem 3.3.1, for operators withC-coefficients. The essential new ingredient is the elliptic regularity properties of Theorem 2.1 and its corollaries.

Proof of Theorem1.1. I. The Markov property of l! follows by the calculations of [15, Example 1.2.1]. Moreover, the form is closed with respect to the graph norm by the arguments in [23, Section II.2.b]. The latter arguments depend crucially on the local strong ellipticity property. Therefore the forml! is a Dirichlet form.

Finally D(l!)C(!)is a core ofl!by the proof of [15, Lemma 3.3.3].

II. The proof thatL!is an extension ofH!is identical to the proof of [15, Lemma 3.3.4] modulo a regularity argument.

LetϕL2(!). Thenψ =(I +L!)1ϕD(L!)D(l!). Moreover,

(ϕ,η)=(ψ,η)+l!(ψ,η)=(ψ,η)+

# "d i,j=1

ci j(∂iψ)(∂jη)

for allηCc (!). Now fix anη1Cc(!)such thatη1 = 1 on the support of η. Thenψ1 = η1ψD(l!)by a straightforward estimate andψ1W01,2(!)by local strong ellipticity. Therefore

(ϕ,η)=1,η)+

# "d i,j=1

ci j(∂iψ1)(∂jη)=1, (I +H!)η)=(ψ, (I +H!)η)

by partial integration. HenceψD(I+H!)and(I+H! =ϕ. ThusD(L!)D(H!)andH!is an extension ofL!. SoD(H!)D(L!)andL!is an extension of H!.

III. This is the lengthiest part of the proof. We divide it into two steps.

Step1. First, we prove that D(k!)D(H!)D(l!)(see proof of [15, Lemma 3.3.5]). Clearly it suffices to prove that

k!(ϕ)

#

!

dx

"d i,j=1

ci j(x) (∂iϕ)(x)(∂jϕ)(x) (3.1)

for allϕD(k!)D(H!).

Set Rλ=(λI +K!)1for allλ>0 and introduce the bounded forms

k(λ)! (ϕ)=λ(ϕ, (IλRλ)ϕ) (3.2)

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for allϕL2(!). Thek!(λ)are Dirichlet forms and k!(ϕ)=sup

λ>0

k!(λ)(ϕ)=lim sup

λ→∞ k!(λ)(ϕ) (3.3)

with D(k!)the subspace ofL2(!)for which the supremum is finite (see, for ex- ample [15, Lemma 1.3.4(ii)]).

Next forηCc(!)with 0≤η≤1 define the truncated form k!,η(λ)(ϕ)=k(λ)! (ϕ,ηϕ)−21k!(λ)(η,ϕ2)

for allϕL2(!)L(!). It then follows from the Dirichlet form structure that k!(λ)(ϕ)k!,η(λ) (ϕ) (3.4) for allϕL2(!)L(!)(see [4, Proposition I.4.1.1]). Moreover,

k!,η(λ)(ϕ)=λ(ϕ, (IλRλ)ηϕ)−21λ(ϕ(IλRλ)η,ϕ) (3.5) for all ϕL2(!)L(!) since (IλRλL(!)by the submarkovian property of K!. Then, however, (3.5) extends to all ϕL2(!)by continuity.

Combination of (3.2), (3.3), (3.4) and (3.5) immediately gives

k!(ϕ)λ(ϕ, (IλRλ)ηϕ)−21λ(ϕ(IλRλ)η,ϕ) (3.6) for allϕD(k!). Now we consider the limitλ→ ∞.

IfϕD(H!)thenηϕD(H!)D(K!)by Theorem 2.1. Therefore

λlim→∞λ(ϕ, (IλRλ)ηϕ)=(ϕ,K!ηϕ)=(ϕ,H!ηϕ) .

Now let S denote the submarkovian semigroup generated by K! on L2(!) and S() the corresponding weak semigroup onL(!). Further letK!()denote the generator ofS() andR(λ) =(λI +K!())1the resolvent. ThenηD(H!)L(!)D(K!)L(!)andK!η= H!ηL(!). ThereforeηD(K!()) andK!()η= H!η. Consequently

H!η= K!()η=weaklimλ→∞λ(IλRλ() and one concludes that

λlim→∞λ(ϕ(IλRλ)η,ϕ)= lim

λ→∞λ((IλR(λ))η,ϕ2)=(K!()η,ϕ2)=(ϕH!η,ϕ) . Then it follows from taking the limitλ→ ∞in (3.6) that

k!(ϕ)(ϕ,H!ηϕ)−21(ϕH!η,ϕ)

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for allϕD(k!)D(H!). SinceηCc(!)and D(H!)Wloc2,2(!), by the proof of Theorem 2.1, it follows by direct calculation that

k!(ϕ)

#

!

dx

"d i,j=1

η(x)ci j(x) (∂iϕ)(x)(∂jϕ)(x)

for all ϕD(k!)D(H!)and ηCc(!) with 0 ≤ η ≤ 1. Butk!(ϕ) is independent ofη. Therefore taking the limit over a sequence ofηwhich converges monotonically upward to 11!one deduces that (3.1) is valid by the Lebesgue domi- nated convergence theorem.

Step2.Next we argue that the inclusionD(k!)D(H!)D(l!)established by Step 1 impliesD(k!)D(l!).

By definitionD(h!)is a subspace ofD(k!). But the orthogonal complement of D(h!)with respect to the graph norm'·'D(k!)is D(k!)N where

N = {ϕD(H!):(I +H!=0}

(see [15, Lemma 3.3.2(ii)]). Therefore eachϕD(k!)has a unique decomposition ϕ=ϕ1+ϕ2withϕ1D(h!)andϕ2D(k!)N such that

'ϕ'2D(k!) ='ϕ1'2D(h

!)+'ϕ2'2D(k!) .

But ϕ2D(k!)D(H!). So ϕ2D(l!) andk!2)l!2) by Step 1.

Therefore

'ϕ'2D(k!)≥ 'ϕ1'2D(h!)+'ϕ2'2D(l!) ='ϕ1'2D(l!)+'ϕ2'2D(l!)='ϕ'2D(l!). The last equality follows becausel!12)+12)=0. It follows immediately thatD(k!)D(l!). This completes the proof of Statement III of Theorem 1.1.

IV. The inclusionCc(!)D(K!)D(H!), was established in Corollary 2.3. But ifηCc(!)andϕD(K!)thenηϕD(H!)D(K!)D(k!)D(l!) and

h!(ηϕ)=l!(ηϕ)≤2'η'2l!(ϕ)+2'*(η)''ϕ'22

≤2('*(η)'+'η'2)'ϕ'2D(k!) where*(η)=!d

i,j=1ci j(∂iη) (∂jη),i.e.*is thecarr´e du champas defined in [4], Section I.8. Since D(K!)is a core ofk!with respect to theD(k!)-graph norm it follows thatCc(!)D(k!)D(h!)by continuity.

V. First let D(k!)c denote the subspace of functions with compact support in D(k!). IfϕD(k!)c then by regularization one can construct a sequenceϕnCc(!)such that'ϕnϕ'D(k!) → 0 asn → ∞. Sincek! is an extension of

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h! it follows that ϕD(h!). Therefore D(k!)cD(h!). Now the first part of Statement V follows from [10, Proposition 2.1]. But then D(h!) is an ideal (see [24, Definition 2.19]) of D(k!)by [24, Corollary 2.22]. In particular it is an order ideal.

For the proof of the second part of Statement V we again appeal to [24, Corol- lary 2.22]. First ifet L! dominateset K! then it follows from this corollary that D(k!)is an ideal of D(l!). Secondly, for the converse statement, it suffices to prove that D(k!)is an ideal ofD(l!). Then the domination property follows from another application of [24, Corollary 2.22]. Thus ifψD(k!), ϕD(l!)and

|ϕ|≤|ψ|then one must deduce thatϕsgnψD(k!). Butϕ,ψD(l!). There- fore ϕsgnψD(l!)by [24, Proposition 2.20]. (See the remark following this proposition.) Moreover,|ψ|∈ D(k!)andsgnψ)+D(l!)becausek!andl!

are Dirichlet forms. Since

0≤sgnψ)+ ≤|ϕ|≤|ψ|

and sinceD(k!)is an order ideal ofD(l!)it follows thatsgnψ)+D(k!). Ap- plying the same argument to−ϕone deduces thatsgnψ)D(k!). Therefore ϕsgnψD(k!)andD(k!)is an ideal ofD(l!).

We note in passing that the existence of l! gives a criterion for uniqueness of the submarkovian extension ofH! similar to the standard criterion for essential self-adjointness.

Proposition 3.1. The following conditions are equivalent:

I. H!has a unique submarkovian extension.

II. ker(I +H!)D(l!)= {0}.

Proof. Condition I is equivalent tol! = h! by Theorem 1.1, i.e. equivalent to D(l!)= D(h!). ButD(l!) = D(h!)H!withH! = ker(I + H!)D(l!) by Lemma 3.3.2(ii) in [15]. Therefore the equivalence of the conditions of the proposition is immediate.

Statement III of Theorem 1.1 establishes thatH!is Markov unique if and only ifl! =h!or, equivalently,D(l!)= D(h!). This is the criterion used extensively in the analysis of Markov uniqueness (see [9], Chapter 3). It will also be used to prove Theorem 1.2.

Statement IV of the theorem establishes that each submarkovian extension of H! is a Silverstein extension (see [30] or [9, Definition 1.4]). Therefore Markov uniqueness ofH!and Silverstein uniqueness are equivalent.

Statement V gives an alternative approach to establishing Markov uniqueness ofH!if the submarkovian semigroup generated by the Friedrichs extension is con- servative. This will be discussed in Section 5.

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4. Markov Uniqueness

In this section we prove Theorem 1.2. Throughout the section we assume that the coefficientsci j are real, symmetric, Lipschitz continuous andC(x)=(ci j(x)) >0 for allx!.

Proof of Theorem1.2. It follows from Theorem 1.1 that H! has a unique sub- markovian extension if and only ifl! = h!, i.e.if and only if Cc (!) is a core of l!. Therefore Theorem 1.2 is a direct corollary of the following proposition which is a variation of [26, Proposition 3.2].

Proposition 4.1. Under the assumptions of Theorem1.2, the following conditions are equivalent:

I. cap!(∂!)=0.

II. Cc(!)is a core ofl!.

Proof. I⇒II First, sincel! is a Dirichlet form D(l!)L(!)is a core ofl!. Therefore it suffices that each ϕD(l!)L(!) can be approximated by a sequenceϕnCc(!) with respect to the graph norm'·'D(l!). Now fix ϕ

D(l!)L(!).

Secondly, let ρnCc(Rd)be a sequence of functions with 0 ≤ ρn ≤ 1, '∇ρn'n1 and such thatρn → 11 pointwise asn → ∞. Then 11−ρnW1,(Rd). But W1,(Rd)D(l!)D(l!). Therefore (11ρnD(l!)L(!). It then follows from Leibniz’ rule and the Cauchy–Schwarz inequality that

'ϕρnϕ'2D(l!) ≤2

#

!

ϕ2*(ρn)+2

#

!

(11ρn)2*(ϕ)+'(11ρn'22

≤2n2'C' 'ϕ'22+

#

!

(11ρn)2(2*(ϕ)+ϕ2)

where'C'is the supremum over the matrix norms'C(x)'. Clearly the first term on the right hand side tends to zero asn → ∞. Moreover, 0 ≤ (11ρn)2 ≤ 1, (11ρn)2 → 0 pointwise asn → ∞and 2*(ϕ)+ϕ2L1(!). Therefore the second term on the right hand side also tends to zero asn → ∞by the Lebesgue dominated convergence theorem. Thusϕis approximated by the sequenceρnϕin the graph norm.

Thirdly, since cap!(∂!)=0 one may chooseχnD(l!)L(!)and open subsetsUn∂!such that 0≤ χn ≤ 1,l!n)+'χn'22n1andχn = 1 on Un!. Now setϕn =(1χnnϕ. Then

'ϕϕn'2D(l!) ≤2'ϕρnϕ'2D(l!)+2'χnρnϕ'2D(l!)

and the first term on the right hand side converges to zero asn→ ∞by the previous discussion. Moreover,

'χnρnϕ'2D(l!) =l!nρnϕ)+'χnρnϕ'22 (4.1)

(13)

and the second term on the right tends to zero because'χnρnϕ'2 ≤ 'χn'2'ϕ'. But the first term can be estimated by

l!nρnϕ) ≤ 2

#

!

ρn2ϕ2*(χn)+2

#

!

χn2*(ρnϕ)

≤ 2

#

!

ϕ2*(χn)+4

#

!

χn2ϕ2*(ρn)+4

#

!

χn2ρn2*(ϕ)

≤ 2'ϕ'2l!n)+4'C' '∇ρn'2'ϕ'22+4

#

!

χn2*(ϕ) . Sincel!n)→ 0 and'∇ρn' → 0 asn → ∞the first two terms on the right hand side tend to zero. But ifAm= {x!:*(ϕ) >m}one has the equicontinuity

estimate #

!

χn2*(ϕ)m'χn'22+

#

Am

*(ϕ)

because 0≤χn ≤1. Since'χn'2→ 0 and*(ϕ)L1(!)the integral also tends to zero asn→ ∞. Thus both terms on the right hand side of (4.1) tend to zero as n → ∞and one now concludes thatϕis approximated by the sequenceϕn in the graph norm.

Finally suppϕnis contained in the set!n=((suppρn)!)(!\(Un!)).

Hence!nis a bounded subset which is strictly contained in!,i.e.!n !!. Then since C(x) > 0 for all x! one has an estimate l!n)µn'∇ϕn'22 with µn > 0. Therefore ϕnW01,2(!n) and it follows that it can be approximated in the W1,2(!n)-norm by a sequence of Cc-functions. Then because l!(ψ) ≤ 'C' '∇ψ'22for allψD(l!)it follows thatϕn, and henceϕ, can be approximated by a sequence ofCc-functions in the graph norm'·'D(l!).

II ⇒ I LetψD(l!)C(!)withψ = 1 onU!where U is an open subset containing∂!. One may assume 0ψ ≤1. Then by Condition II there is a sequenceψnCc(!)such that'ψnψ'D(l!) →0. In particularψW1,2(!).

Sinceψn has compact support in!it also follows that there is an open subsetUn containing∂!such thatψn =0 onUn!. Thereforeψψn=1 on(UUn)! and one must have cap!(∂!)=0.

The condition cap!(∂!)=0 is of interest as a criterion for Markov uniqueness since the capacity can be estimated by elementary means. The estimates depend on two gross features, the order of degeneracy of the coefficients at the boundary and the dimension of the boundary. There are various ways of assigning a dimension to a measurable subset A(see, for example [14, Chapters 2 and 3]). In the next proposition we characterize the dimension in terms of the volume growth of the δ-neighbourhoods

Bδ= {x ∈Rd : inf

yB|xy|} of the bounded measurable subsetsBofA.

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