• Keine Ergebnisse gefunden

Necessity of parameter-ellipticity for multi-order systems of differential equations

N/A
N/A
Protected

Academic year: 2022

Aktie "Necessity of parameter-ellipticity for multi-order systems of differential equations"

Copied!
14
0
0

Wird geladen.... (Jetzt Volltext ansehen)

Volltext

(1)

Universität Konstanz

Necessity of parameter-ellipticity for multi-order systems of differential equations

Robert Denk Melvin Faierman

Konstanzer Schriften in Mathematik Nr. 278, Februar 2011

ISSN 1430-3558

© Fachbereich Mathematik und Statistik Universität Konstanz

Fach D 197, 78457 Konstanz, Germany

Konstanzer Online-Publikations-System (KOPS) URN: http://nbn-resolving.de/urn:nbn:de:bsz:352-opus-130872

URL: http://kops.ub.uni-konstanz.de/volltexte/2011/13087/

(2)
(3)

MULTI-ORDER SYSTEMS OF DIFFERENTIAL EQUATIONS

R. DENK AND M. FAIERMAN

Abstract. In this paper we investigate parameter-ellipticity conditions for multi-order systems of differential equations on a bounded domain. Under suitable assumptions on smoothness and on the order structure of the system, it is shown that parameter-dependent a priori-estimates imply the conditions of parameter-ellipticity, i.e., interior ellipticity, conditions of Shapiro-Lopatinskii type, and conditions of Vishik-Lyusternik type. The mixed-order systems con- sidered here are of general form; in particular, it is not assumed that the diag- onal operators are of the same order. This paper is a continuation of an article by the same authors where the sufficiency was shown, i.e., a priori-estimates for the solutions of parameter-elliptic multi-order systems were established.

1. Introduction and main results

In this paper, we will study multi-order boundary value problems defined over a bounded domain in Rn. Under rather general assumptions on the structure of the system, it was shown in the paper [DF] that parameter-ellipticity implies uniform a priori-estimates for the solutions. Now we will show that the conditions of parameter-ellipticity are also necessary.

Parameter-elliptic boundary value problems and a priori estimates for them were treated, e.g., in [ADF] (scalar problems), [DFM] (systems of homogeneous type), and [F] (multi-order systems). The notion of parameter-ellipticity for general multi- order systems was introduced by Kozhevnikov ([K1], [K2]) and by Denk, Mennicken, and Volevich ([DMV]). The mentioned papers had restrictions on the orders of the operators which excluded, for instance, boundary conditions of Dirichlet type (see [ADN, Section 2], [G, p. 448]). In the paper [DF], these restrictions were removed.

Let us consider in a bounded domain Ω ⊂ Rn, n ≥ 2, with boundary Γ the boundary value problem

A(x, D)u(x)−λu(x) =f(x) in Ω,

B(x, D)u(x) =g(x) on Γ. (1.1)

HereA(x, D) = Ajk(x, D)

j,k=1,...,N is anN×N-matrix of linear differential op- erators,N ∈N,N ≥2,u(x) = (u1(x), . . . , uN(x))T andf(x) = (f1(x), . . . , fN(x))T are defined on Ω (T denoting the transpose), whereasB(x, D) = Bjk(x, D)

j=1,...,Ne k=1,...,N

is anNe ×N-matrix of boundary operators, and g(x) = (g1(x), . . . , g

Ne(x))T is de- fined on Γ.

Date: February 24, 2011.

1991Mathematics Subject Classification. Primary 35J55; Secondary 35S15.

Key words and phrases. Parameter-ellipticity, multi-order systems, a priori estimates.

1

(4)

To describe the order structure of the boundary value problem (A, B), let{sj}Nj=1 and{tj}Nj=1 denote sequences of integers satisfyings1≥ · · · ≥sN,t1≥ · · · ≥tN ≥ 0, and putmj :=sj+tj(j= 1, . . . , N). We assume

m1=· · ·=mk1 > mk1+1=· · ·=mkd−1 > mkd−1+1=· · ·=mkd>0, wherekd=N. We setmej:=mkj (j= 1, . . . , d), and assume that 2Nr:=Pkr

j=1mj

is even for r = 1, . . . , d. We also set k0 := 0 and N0 := 0. Further, let {σj}Nj=1e , Ne :=Nd, be a sequence of integers satisfying maxjσj < sN. It was shown in [DF, Section 2] that we may also assumesj≥0 (j= 1, . . . , N) andσj <0 (j= 1, . . . ,Ne).

Defineκ0:= max{t1,−σ1, . . . ,−σ

Ne}. Concerning (A, B), we will assume that ordAjk≤sj+tk (j, k= 1, . . . , N),

ordBjk≤σj+tk (j= 1, . . . ,N , ke = 1, . . . , N).

Using the standard multi-index notationDα=D1α1· · ·Dαnn,Dj =−i∂x

j, we write Ajk(x, D) =P

|α|≤sj+tkajkα(x)Dα forx∈Ω andj, k = 1, . . . , N and Bjk(x, D) = P

|α|≤σj+tkbjkα(x)Dα for x∈ Γ, j = 1, . . . ,Ne, and k= 1, . . . , N. With respect to the smoothness, we will suppose

(S) (1) Γ is of classCκ0−1,1∩Cs1,

(2)ajkα ∈Csj(Ω) (|α| ≤sj+tk) ifsj>0 and

ajkα ∈C0(Ω) (|α|=sj+tk), ajkα ∈L(Ω) (|α|< sj+tk) ifsj= 0, (3)bjkα ∈C−σj−1,1(Γ) (|α| ≤σj+tk).

Let ˚Ajk(x, ξ) consist of all terms in Ajk(x, ξ) which are exactly of order sj+tk, and set

A(x, ξ) := ˚˚ Ajk(x, ξ)

j,k=1,...,N (x∈Ω, ξ∈Rn).

Analogously, define ˚B(x, ξ) = ˚Bjk(x, ξ)

j=1,...,Ne k=1,...,N

forx∈Γ, ξ∈Rn. The operator B(x, D) is said to be essentially upper triangular if ˚Bjk(x, D) = 0 for j =N`−1+ 1, . . . , N`, k= 1, . . . , k`−1,`= 2, . . . , d.

To formulate the ellipticity conditions, let A(r)11(x, ξ) := ˚Ajk(x, ξ)

j,k=1,...,kr (r= 1, . . . , d).

LetI` denote the `×` unit matrix,Ie` :=Ik`−k`−1, andIe`,0 := diag 0·Ie1, . . . ,0· Ie`−1,Ie`

. In the following, let L ⊂Cbe a closed sector in the complex plane with vertex at the origin. The following condition is taken from [DF, Section 2] (cf. also [DMV, Section 3]).

(E) For eachx∈Ω,ξ∈Rn\ {0},λ∈ L, andr= 1, . . . , dwe have det A(r)11(x, ξ)−λeIr,0

6= 0.

If condition (E) holds, the operatorA(x, D)−λIN is said to be parameter-elliptic in L. In order to formulate conditions of Shapiro-Lopatinskii type, for x0 ∈Γ we rewrite the boundary value problem (1.1) in terms of local coordinates associated to x0. In these coordinates x0 = 0, and the positive xn-axis coincides with the direction of the inner normal to Γ. We will keep the notation for Aand B in the

(5)

new coordinates. In local coordinates associated tox0∈Γ, let B(r,r)r,1 (0, ξ0, Dn) := ˚Bjk(0, ξ0, Dn)

j=1,...,Nr

k=1,...,kr

(r= 1, . . . , d), Br,1(1,r)(0, ξ0, Dn) := ˚Bjk(0, ξ0, Dn)

j=Nr−1+1,...,Nr k=1,...,kr

(r= 2, . . . , d),

The following conditions (see [DF, Section 2]) are of Shapiro-Lopatinskii type and of Vishik-Lyusternik type, respectively (cf. also [DV, Section 2.3]).

(SL) For each x0 ∈Γ rewrite (1.1) in local coordinates associated to x0. Then forr= 1, . . . , d, the boundary value problem on the half-line,

A(r)11(0, ξ0, Dn)v(xn)−λeIr,0v(xn) = 0 (xn>0), Br,1(r,r)(0, ξ0, Dn)v(xn) = 0 (xn= 0),

|v(xn)| →0 (xn→ ∞)

(1.2)

has only the trivial solution forξ0 ∈Rn−1\ {0}, λ∈ L.

(VL) For each x0 ∈Γ rewrite (1.1) in local coordinates associated to x0. Then forr= 2, . . . , d, the boundary value problem on the half-line,

A(r)11(0,0, Dn)v(xn)−λeIr,0v(xn) = 0 (xn>0), B(1,r)r,1 (0,0, Dn)v(xn) = 0 (xn= 0),

|v(xn)| →0 (xn→ ∞)

(1.3)

has only the trivial solution forλ∈ L \ {0}.

We will show that (E), (SL), and (VL) are necessary for a priori estimates to hold. In order to formulate these estimates, we will introduce parameter-dependent norms.

ForG⊂R`open,`∈N,s∈Nand 1< p <∞, letkuks,p,G denote the norm in the standard Sobolev spaceWps(G). For λ∈C\ {0} andj= 1, . . . , dset

|||u|||(j)s,p,G:=kuks,p,G+|λ|s/mejkuk0,p,G (u∈Wps(G)).

For s < 0, s ∈ Z, and j = 1, . . . , d, let Hps(Rn) be the Bessel-potential space equipped with the parameter-dependent norm |||u|||(j)s,p,

Rn := kF−1hξ, λisjF uk0,p,Rn

whereF denotes the Fourier transform inRn (x→ξ) and wherehξ, λisj:= |ξ|2+

|λ|2/mej1/2

. ForG⊂Rn open, set |||u|||(j)s,p,G := inf{|||v|||ss,p,Rn :v ∈Hps(Rn), v|G = u}. Finally, for s∈N we define the parameter-dependent norm on the boundary by

|||v|||(j)s−1/p,p,∂G:=kvks−1/p,p,∂G+|λ|(s−1/p)/mejkvk0,p,∂G (v∈Wps−1/p(∂G)).

For j = 1, . . . , N, let π1(j) := r if kr−1 < j ≤ kr. Similarly, for j = 1, . . . , Nd let π2(j) := r if Nr−1 < j ≤ Nr. Note that, by definition, meπ1(j) = mj for j= 1, . . . , N.

The aim of the paper is to show the following result.

Theorem 1.1. Let (S)hold, let 1< p <∞, and assume that there exist constants C0, C1>0 such that for allλ∈ L,|λ| ≥C0 and all u∈QN

j=1Wptj(Ω) the a priori

(6)

estimate

N

X

j=1

|||uj|||t 1(j))

j,p,Ω ≤C1

XN

j=1

|||fj|||−s1(j))

j,p,Ω+

Ne

X

j=1

|||gj|||−σ2(j))

j−1/p,p,Γ

(1.4) holds for f :=A(x, D)u−λu andg :=B(x, D)u. Assume further that B(x, D)is essentially upper triangular. Then the parameter-ellipticity conditions (E), (SL), and (VL)are satisfied.

Remark 1.2. In [DF], the following result was shown, where we refer to [DF] for the definitions of properly parameter-elliptic and compatible: Let (S), (E), (SL), and (VL) hold. Assume further that (A, B) is properly parameter-elliptic, thatB(x, D) is essentially upper triangular, and thatA(x0, D) andB(x0, D) are compatible at every x0 ∈Γ. Then there existC0, C1 >0 such that for allλ∈ L, |λ| ≥C0, the boundary value problem (1.1) has a unique solution u ∈ QN

j=1Wptj(Ω) for every f ∈ QN

j=1Hp−sj(Ω) and every g ∈ QNe

j=1Wp−σj−1/p(Γ), and the a priori estimate (1.4) holds.

In this sense, the sufficiency of parameter-ellipticity for the validity of the a priori estimate was shown in [DF] while Theorem 1.1 states the necessity of the conditions (E), (SL), and (VL).

2. Proof of the necessity

Throughout this section, we assume condition (S) to hold, and fix a closed sector L ⊂ C. In the following, C stands for a generic constant which may vary from inequality to inequality but which is independent of the functions appearing in the inequality and independent of λ. LetBδ(x0) :={x∈ Rn :|x−x0|< δ}, and let Rn+ := {x∈ Rn : xn >0}, R+ := (0,∞). We start with some useful remarks on negative-order Sobolev spaces whereC0(Rn+) stands for the set of all restrictions of functions inC0(Rn) toRn+.

Lemma 2.1. Lets∈N,1< p <∞,j∈ {1, . . . , N}. Then for allv∈Lp(Rn)and allλ∈C,|λ| ≥1, we have:

a)|||v|||(j)−s,p,

Rn≤Ckvk−s,p,Rn,

b)|||Dαv|||(j)−s,p,Rn≤ |λ|(|α|−s)/mejkvk0,p,Rn for all |α| ≤s,

c) for each φ∈C0(Rn) there exists a constant Cφ >0 independent of v such that kvφk−s,p,Rn≤Cφkvk−s,p,Rn and|||vφ|||(j)−s,p,Rn≤Cφ|||v|||(j)−s,p,Rn.

The same assertions hold if we replaceRnbyRn+andC0(Rn)in c) byC0(Rn+).

Proof. a) We have

|||v|||(j)−s,p,Rn=kF−1hξ, λi−sj F vk0,p,Rn=

F−1 hξis

hξ, λisjhξi−sF v 0,p,

Rn

. Now the assertion follows immediately from the Mikhlin-Lizorkin multiplier theo- rem.

b) Similarly,

|λ|(s−|α|)/mej|||Dαv|||(j)−s,p,

Rn =kF−1m(ξ, λ)F vk0,p,Rn

withm(ξ, λ) :=|λ|(s−|α|)/mejξαhξ, λi−sj . Noting thatmis infinitely smooth inξand quasi-homogeneous in (ξ, λ) of degree 0 in the sense that m(ρξ, ρmejλ) = m(ξ, λ)

(7)

for ρ >0, we see that we may apply the Mikhlin-Lizorkin theorem to obtain the statement in b).

c) We make use of the dual pairing ofHp−s(Rn) andWqs(Rn), 1p+1q = 1, and get kvφk−s,p,Rn= sup

ζ

|hvφ, ζi|= sup

ζ

Z

v(x)φ(x)ζ(x)dx = sup

ζ

|hv, φζi|, where the supremum is taken over allζ∈C0(Rn) withkζks,q,Rn≤1. Now we make use ofkφζks,q,Rn ≤Cφkζks,q,Rn withCφ :=Cs,qsup{|Dαφ(x)|: |α| ≤s, x∈ Rn} where Cs,q is a constant depending on s and q only. We obtain supζ|hv, φζi| ≤ Cφsupζ|hv, ζi|=Cφkvk−s,p,Rn.

For the parameter-dependent norms|||·|||(j)−s,p,Rnwe again consider the dual pairing betweenHp−s(Rn) andWqs(Rn), but now with respect to the parameter-dependent norm||| · |||(j)s,q,RnonWqs(Rn). Then the result follows in exactly the same way, noting that

|||φζ|||(j)s,q,Rn =kφζks,q,Rn+|λ|s/mejkφζk0,p,Rn ≤Cφ

kζks,q,Rn+|λ|s/mejkζk0,p,Rn

. Finally, in the case of Rn+ instead of Rn the assertions of the lemma follow easily from the results inRn and the fact that there exists an extension operator E:u 7→ Eu which is continuous as an operator from Hpr(Rn+) to Hpr(Rn) for all

|r| ≤s(see [T, p. 218]).

The following lemma will allow us to consider the model problem inRn for the proof of the necessity.

Lemma 2.2. Assume that there exist constants C0, C1 >0 such that for all u∈ QN

j=1Wptj(Rn) and all λ ∈ L, |λ| ≥ C0, the a priori estimate (1.4) holds. Let x0∈Ω. Then there exist anx1∈Ω, a δ >0 with Bδ(x1)⊂Ω, and a eλ >0 such that for all λ∈ L with |λ| ≥eλ and allu∈QN

j=1Wptj(Rn) with suppu⊂Bδ(x1), we have

N

X

j=1

|||u|||t 1(j))

j,p,Rn≤C

N

X

j=1

|||fj0|||−s1(j))

j,p,Rn, (2.1)

where we have setf0:= ( ˚A(x0, D)−λ)u.

Proof. In [DF, Prop. 4.1] it was shown that for any ε > 0 there exist a δ0 > 0 and a λ0 > 0 such that for λ ∈ L, |λ| ≤ λ0, and all u ∈ QN

j=1Wptj(Rn) with suppu⊂Bδ(x0)∩Ω we have

N

X

j=1

|||fj−fj0|||−s1(j))

j,p,Ω≤ε

N

X

j=1

kujktj,p,Ω

wheref := (A(x, D)−λ)u. Letεbe sufficiently small. Ifx0∈Ω we choosex1:=x0 and δ := 12min{δ0,dist(x0,Γ)}. If x0 ∈ Γ we choose x1 ∈Bδ(x0)∩Ω andδ > 0 sufficiently small such that Bδ(x1)⊂Bδ(x0)∩Ω. In both cases, the statement of the lemma follows easily by arguments similar to those used in the proof of [AV,

Lemma 4.2].

(8)

Proposition 2.3. Under the assumptions of Lemma 2.2, condition (E)is satisfied, i.e., forr= 1, . . . , d,x0∈Ω,ξ0∈Rn\ {0}, andλ0∈ L we have

det A(r)11(x0, ξ0)−λ0Ier,0

6= 0.

Proof. Assume that (E) does not hold. Then there exist r ∈ {1, . . . , d}, x0 ∈ Ω, ξ0∈Rn\{0},λ0∈ L, and a vectorh∈Ckr\{0}such that (A(r)11(x0, ξ0)−λ0Ier,0)h= 0.

Let us first consider the case λ0 = 0. We choose x1 ∈ Ω, δ > 0 and eλ > 0 according to Lemma 2.1. Letφ∈C0(Bδ(x1)) withφ6≡0, and forρ >1 set

uj(x) :=

(φ(x)eiρξ0·xρ−tjhj, j= 1, . . . , kr, 0, j=kr+ 1, . . . , N,

where ·denotes the inner product in Rn. We are now going to use (2.1) to arrive at a contradiction. Indeed, we easily see that forj= 1, . . . , kr,

kujktj,p,Rn≥ |hj| |ξ`0|tjkφk0,p,Rn−Cρ−1 whereξ0` 6= 0. We further chooseµwith

mer+1< µ <mer if r < d and med/2< µ <med if r=d, (2.2) and chooseλ∈ L with|λ|=ρµ. Then it is clear that

|λ|tj/mejkujk0,p,Rn−tj(1−µ/mej)|hj| kφk0,p,Rn. Thus we have shown that

N

X

j=1

|||uj|||t 1(j))

j,p,Rn≥ 1 2

Xkr

j=1

|hj| |ξ`0|tj

kφk0,p,Rn (2.3) for sufficiently largeρ.

Turning next to the right-hand side of (2.1), letj∈ {1, . . . , N}. Then

|||fj0|||−s1(j))

j,p,Rn =

kr

X

k=1

jk(x0, D)uk−δjkλuk

1(j))

−sj,p,Rn

kr

X

k=1

X

|α|=sj+tk

ajkα(x0)X

β

α β

ρ−tkhkDβ(eiρξ0·x)Dα−βφ

1(j))

−sj,p,Rn

+

kr

X

k=1

δjkρ−rk|hk| |||eiρξ0·xφ|||−s1(j))

j,p,Rn=:I1+I2, where δjk denotes the Kronecker delta and where P

β = P

β<α if j ≤ kr and P

β=P

β≤α ifr < dandj > kr. (Here we used the fact thatA(r)11(x0, ξ0)h= 0.) It is clear thatI2 →0 asρ→ ∞. Hence fixing our attention next uponI1, we see thatI1≤Pkr

k=1

P

|α|=sj+tk

P

βI1,kα,β with I1,kα,β:=

α β

ajkα(x0−tkDβ(eiρξ0·x)Dα−βφ

1(j))

−sj,p,Rn

.

To establishI1,kα,β →0 (ρ→ ∞) and, in consequence, a contradiction, it remains to show that for all appearing indices we have

ρ−tk|||Dβ(eiρξ0·x)Dα−βφ|||−s1(j))

j,p,Rn→0 (ρ→ ∞).

(9)

Letj∈ {1, . . . , kr},|α|=sj+tk, andβ < α. If|β| ≤tk, we apply Lemma 2.1 b) to obtain

ρ−tk|||Dβ(eiρξ0·x)Dα−βφ|||−s1(j))

j,p,Rn≤Cρ−tk−sjµ/mjkDβ(eiρξ0·x)Dα−βφk0,p,Rn

≤Cρ−tk+|β|−sjµ/mj|(ξ0)β| kDα−βφk0,p,Rn→0 (ρ→ ∞).

Note here thatsj= 0 implies|β|< tk.

If|β| ≥tk, we write β=β12 with|β1|=tk, |β2|< sj and fixψ∈C0(Rn) withψ= 1 on suppφ. Then, using Lemma 2.1 b) and c),

ρ−tk|||Dβ(eiρξ0·x)Dα−βφ|||−s1(j))

j,p,Rn−tk|||Dβ(eiρξ0·xψ)Dα−βφ|||−s1(j))

j,p,Rn

≤Cρ−tk|||Dβ2(Dβ1eiρξ0·xψ)|||−s1(j))

j,p,Rn

≤Cρ−tk−(sj−|β2|)µ/mjkDβ1eiρξ0·xψk0,p,Rn

≤Cρ−(sj−|β2|)µ/mj kψk0,p,Rn+Cρ−1

→0 (ρ→ ∞).

Now letj∈ {kr+ 1, . . . , N}. Again by Lemma 2.1 b), we have for|α|=sj+tk and|β| ≤ |α|

ρ−tk|||Dβ(eiρξ0·x)Dα−βφ|||−s1(j))

j,p,Rn≤Cρ−sjµ/mj+sjkDα−βφk0,p,Rn →0 (ρ→ ∞) asµ/mj>1.

Finally, the caseλ06= 0 can be dealt with by arguing in a manner similar to that

above, except now we takeλ=λ0ρmer.

To prove the necessity of (SL) and (VL), we transform the problem to the half- space. For this let x0 ∈ Γ and assume that (A, B) is given in local coordinates associated tox0. Let{U,Φ} be a chart on Γ such thatx0= 0∈U, Φ(0) = 0, and Φ is a diffeomorphism of classCκ0−1,1∩Cs1mappingUonto an open set inRnwith Φ(U∩Ω)⊂Rn+, Φ(U ∩Γ)⊂Rn−1. We denote the push-forward of the operators A(x, D) andB(x, D) byA(y, D) ande Be(y, D), respectively, wherey= Φ(x).

Replacing Φ(x) by DΦ(0)−1Φ(x), it is easily seen that we may assume the Jacobian DΦ(0) to be equal to In. Then we have ˚

Aejk(0, ξ) = ˚Ajk(0, ξ) and

˚

Bejk(0, ξ) = ˚Bjk(0, ξ). In particular, (SL) and (VL) are satisfied for (A,e B) at 0e if only if this holds for (A, B) atx0= 0 (see also [DHP, p. 205]).

Lemma 2.4. Under the assumptions of Lemma 2.2, letx0∈Γand assume(A, B) to be written in coordinates associated tox0. Then there exist aδ >0and aeλ >0 such that for all u∈QN

j=1Wptj(Rn+)with suppu⊂Bδ(0)∩Rn+ and all λ∈ Lwith

|λ| ≥eλ, we have

N

X

j=1

|||uj|||t 1(j))

j,p,Rn+ ≤CXN

j=1

|||fj0|||−s1(j))

j,p,Rn++

Ne

X

j=1

|||g0j|||−σ2(j))

j−1/p,p,Rn−1

, (2.4)

wheref0:= ( ˚A(0, D)−λ)u,g0:= ˚B(0, D)u.

Proof. Let Φ be as above, and let A(y, D) ande B(y, D) be the push-forward ofe A(x, D) andB(x, D), respectively. Then

Φ

(ajkα(x)−ajkα(0))Dαuk

= (eajkα(y)−eajkα(0))Dyαuek+ X

|β|<|α|

eajkα,β(y)Dβyuek.

(10)

It was shown in the proof of [DF, Prop. 4.1], that for eachε >0 there exist aδ0>0 and aλ0>0 such that for allu∈QN

j=1Wptj(Ω) with suppu⊂Bδ0(0)∩Ω and all λ∈ L,|λ| ≥λ0, we have

|||Φ

(ajkα(x)−ajkα(0))Dαuk

|||−s1(j))

j,p,Rn+ ≤εkeukktk,p,Rn+

for|α|=sj+tk, and

|||Φ

ajkα(x)Dαuk

|||−s1(j))

j,p,Rn+ ≤εkeukktk,p,Rn+

for|α|< sj+tk. From this we easily obtain that for allε >0 there existδ0, λ0>0 such that for allu∈QN

j=1Wptj(Ω) with suppu⊂Bδ0(0),

N

X

j=1

|||fej|||−sj,p,Rn

+≤C

N

X

j=1

|||ffj0|||−sj,p,Rn

+

N

X

j=1

kujktj,p,Rn

+

where we have setf := (A(x, D)−λ)u,fe:= Φf,ff0:= Φf0.

To estimateg0, we first remark that we may assumebjkα to be defined on Ω with bjkα ∈ C−σj−1,1(Ω). We define the function h on Ω by hj := PNe

j=1bjkα(x)Dαuk, h0j :=PNe

j=1bjkα(0)Dαuk and seteh:= Φh,hf0:= Φh0. In the same way as above, we obtain

Ne

X

j=1

|||egj|||−σ2(j))

j−1/p,p,Rn−1

Ne

X

j=1

|||ehj|||−σ2(j))

j−1/p,p,Rn−1

≤C

Ne

X

j=1

|||fh0j|||−σ2(j))

j−1/p,p,Rn−1

N

X

j=1

kuke tj,p,Rn+.

Finally, it was shown in [DF, p. 362-363] that there exist constantsc1, c2>0 such that for allu∈QN

j=1Wptj(Ω) with suppu⊂Bδ(x0),B(x0)⊂U, we have c1|||uj|||t 1(j))

j,p,Ω ≤ |||euj|||t 1(j))

j,p,Rn+ ≤c2|||uj|||t 1(j))

j,p,Ω , c1|||fj|||−s1(j))

j,p,Ω≤ |||fej|||−s1(j))

j,p,Rn+ ≤c2|||fj|||−s1(j))

j,p,Ω, c1|||gj|||−σ1(j))

j−1/p,p,Γ≤ |||egj|||−σ1(j))

j−1/p,p,Rn−1≤c2|||gj|||−σ1(j))

j−1/p,p,Γ.

(2.5)

Therefore, from the a priori-estimate (1.4) we obtain that for eachε >0 there exist δ,eλ >0 such that for u∈QN

j=1Wptj(Ω) with suppu⊂Bδ(0) andλ∈ L, |λ| ≥eλ, we have

N

X

j=1

|||euj|||t 1(j))

j,p,Rn+ ≤C

N

X

j=1

|||uj|||t 1(j))

j,p,Ω ≤CXN

j=1

|||fj|||−s1(j))

j,p,Ω+

Ne

X

j=1

|||gj|||−σ2(j))

j−1/p,p,Γ

≤CXN

j=1

|||fej|||−s1(j))

j,p,Rn++

Ne

X

j=1

|||gej|||−σ2(j))

j−1/p,p,Rn−1

N

X

j=1

kuejkt 1(j))

j,p,Rn+.

Takingεsmall enough andλlarge enough and noting (2.5) and˚

A(0, D) = ˚e A(0, D) and ˚

B(0, D) = ˚e B(0, D), we obtain the assertion of the Lemma.

(11)

Proposition 2.5. Assume that there exist constants C0, C1 > 0 such that for all u∈QN

j=1Wptj(Rn)and all λ∈ L, |λ| ≥C0, the a priori estimate (1.4) holds.

Further, letx0∈Γ, and assume thatB(x0, D)is essentially upper triangular. Then condition (SL) holds atx0.

Proof. Let (A, B) be written in coordinates associated tox0 and assume that (SL) does not hold. Then there exist r ∈ {1, . . . , d}, λ0 ∈ L, ξ00 = (ξ01, . . . , ξ0n−1) ∈ Rn−1\ {0}, and v 6≡ 0 satisfying (1.2). By Proposition 2.3, we know that the polynomial det(A(r)11(0, ξ00, τ)−λ0Ier,0) as a function ofτhas no real roots. Therefore, v=v(xn) is infinitely smooth and decays exponentially forxn → ∞, in particular, v∈Lp(R+).

Again, let us first consider the caseλ0= 0. We chooseφ0∈C0(Rn−1) such that φ06≡0 and suppφ0⊂Bδ(0) withδfrom Lemma 2.4,ψ∈C0([0, δ)) with 0≤ψ≤1 andψ(xn) = 1 for 0≤xn ≤δ/2, and λ∈ Lwith |λ|=ρµ whereµ satisfies (2.2).

Forx∈Rn+, we set w(x) :=e00·x0v(xn),φ(x) :=φ0(x0)ψ(xn), and uj(x) :=

−tj+1/pwj(ρx)φ(x), j= 1, . . . , kr,

0, j=kr+ 1, . . . , N. (2.6)

We will show that (2.4) leads to a contradiction for largeρ. For this we first remark that forj= 1, . . . , kr

ρkvj(ρxn)ψ(xn)kp0,p,R

+ =ρ Z

0

|vj(ρxn)ψ(xn)|pdxn

= Z

0

|vj(yn)ψ(yn/ρ)|pdyn% kvjkp0,p,

R+ (ρ→ ∞).

Therefore, forρ≥ρ00being sufficiently large, we have 1

−1/pkvjk0,p,R+≤ kvj(ρxn)ψ(xn)k0,p,R+≤ρ−1/pkvjk0,p,R+. In the same way, we see that for anyζ∈C0(Rn+) andα∈Nn0 we have

kDαwj(ρx)ζ(x)k0,p,Rn+ ≤Cζρ|α|−1/pkvjk|α|,p,R+ with a constantCζ depending onζbut not onv orρ.

Turning now to the left-hand side of (2.4), the above considerations show that forρsufficiently large,

|||uj|||t 1(j))

j,p,Rn+≥ kujktj,p,Rn+ ≥1

2|ξ`0|tj0k0,p,Rn−1kvjk0,p,R+. (2.7) On the right-hand side of (2.4), the terms|||fj0|||−s1(j))

j,p,Rn+ can be estimated in the same way as in the proof of Proposition 2.3. Indeed, we have

fj0(x) =

kr

X

k=1

X

|α|=sj+tk

X

β

ajkα(0) α

β

ρ−tk+1/p(Dβw)(ρx)(Dα−βφ)(x) +δjkλuk

where P

β =P

β<α ifj ≤kr and P

β =P

β≤α ifj > kr. Here we used the fact A(0, D)w(x) =˚ e00·x0A(0, ξ˚ 00, Dn)v(xn) = 0. From this we obtain in the same way as in the proof of Proposition 2.3

N

X

j=1

|||fj0|||−s1(j))

j,p,Rn+→0 (ρ→ ∞). (2.8)

(12)

To estimateg0j, we first remark that B˚jk(0, ρξ00, Dn)vk(ρxn)ψ(xn)

x

n=0σj+tkjk(0, ξ00, Dn)vk(xn) x

n=0

by homogeneity and as ψ(xn) = 1 near xn = 0. Therefore, for j = 1, . . . , Nr we have

gj=

kr

X

k=1

ρ−tk+1/pjk(0, D)wk(ρx)φ(x) x

n=0

=

kr

X

k=1

X

|α|=σj+tk

X

β<α

bjkα(0) α

β

ρ−tk+1/pDβwk(ρx)Dα−βφ(x) x

n=0

due toPkr

k=1jk(0, ξ00, Dn)vk(xn)|xn=0 = 0. For j= 1, . . . , Nr,|α|=σj+tk, and β < αwe can estimate

ρ−tk+1/p

Dβw(ρx)Dα−βφ(x) x

n=0

−σ

j−1/p,p,Rn−1

≤ρ−tk+1/p

Dβw(ρx)Dα−βφ(x)

−σj,p,Rn+

≤Cρ−tk+1/p X

|γ|≤−σj

Dγ

Dβw(ρx)Dα−βφ(x) 0,p,

Rn+

≤Cφρ−tk−σj+|β|kvk0,p,R+ →0 (ρ→ ∞). (2.9) Further, for|λ|=ρµ we obtain

|λ|(−σj−1/p)/meπ2 (j)kgjk0,p,Rn−1

=|λ|(−σj−1/p)/meπ2 (j)

kr

X

k=1

X

|α|=σj+tk

bjkα(0)Dαuk(x) x

n=0

0,p,

Rn−1

≤Cρj+1/p)(1−µ/meπ2 (j))→0 (ρ→ ∞)

asµ/meπ2(j)<1 andσj ≤ −1. From this and (2.9) we see that forj= 1, . . . , Nr

|||g0j|||−σ2(j))

j−1/p,p,Rn−1 →0 (ρ→ ∞). (2.10) Finally, for j > Nr we havegj0 = 0 asB(0, D) is assumed to be essentially upper triangular. From (2.7), (2.8), and (2.10) we obtain a contradiction to the a priori- estimate (2.4).

In the caseλ06= 0, the result follows from similar considerations where we now

setλ=λ0ρmer again.

Proposition 2.6. Under the assumptions of Proposition 2.5, condition(VL)holds atx0.

Proof. The proof is similar to the proof of Proposition 2.5, and we only indicate some changes and additional remarks. Assuming v to be a nontrivial solution of (1.3), defineλ:=ρmerλ0anduas in (2.6), but now settingξ00= 0, i.e., we set

u(x) :=

−tj+1/pφ(x)vj(ρxn), j = 1, . . . , kr, 0, j =kr+ 1, . . . , N.

Now the left-hand side of (2.4) can be estimated from below by

|||uj|||t 2(j))

j,p,Rn+ ≥ kujktj,p,Rn

+ ≥ kDntjujk0,p,Rn

+≥1

2kvjk0,p,R+0k0,p,Rn−1

Referenzen

ÄHNLICHE DOKUMENTE

Manifolds of bounded geometry with noncompact boundary, Dirac operator, boundary value problems, Spin c structures, coercivity at infinity.. The work was initiated during the

In this manuscript, the existence, uniqueness, and stability of solutions to the multiterm boundary value problem of Caputo fractional differential equations of variable order

This analog in some sense was suggested by the deep connection of mixed order problems with large parameter to the Luysternik–Vishik theory of boundary layers, developed for

Метод сплайн-коллокации для решения двумерного интегрального уравнения с логарифмическим ядром.В настоящем сборике, 18-23.. Численные методы

Using this error indicator an adaptive reduced order model strategy is proposed to solve the optimization problem in an efficient way.. This is achieved by combining the finite

This paper is concerned with a boundary value problem defined over a bounded region of Euclidean space, and in particular it is devoted to the establishment of a priori estimates

The viscous model in the higher-dimensional case for the first time was studied by the authors in [12, 13], and results on the time evolution with Cauchy data or insulating

In this paper we prove parameter-dependent a priori estimates for mixed-order boundary value problems of rather general structure.. In partic- ular, the diagonal operators are