Home Strong Comparison Principle for the Fractional p-Laplacian and Applications to Starshaped Rings
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Strong Comparison Principle for the Fractional p-Laplacian and Applications to Starshaped Rings

  • Sven Jarohs ORCID logo EMAIL logo
Published/Copyright: December 5, 2017

Abstract

In the following, we show the strong comparison principle for the fractional p-Laplacian, i.e. we analyze

{ ( - Δ ) p s v + q ( x ) | v | p - 2 v 0 in  D , ( - Δ ) p s w + q ( x ) | w | p - 2 w 0 in  D , v w in  N ,

where s(0,1), p>1, DN is an open set, and qL(N) is a nonnegative function. Under suitable conditions on s, p and some regularity assumptions on v, w, we show that either vw in N or v>w in D. Moreover, we apply this result to analyze the geometry of nonnegative solutions in starshaped rings and in the half space.

MSC 2010: 35B51; 35B06

1 Introduction

In the following, we investigate an ordered pair of functions v,w:N which are the sub- and supersolution of the equation

(1.1) ( - Δ ) p s u + q ( x ) | u | p - 2 u = g in  D ,

where s(0,1), p>1, qL(D) is a nonnegative function, gLp(D) with p=pp-1 being the conjugate of p, and (-Δ)ps is the s-fractional p-Laplacian (up to a constant). Recall that for suitable (s,p) and some smoothness conditions on u we may write (see [11, Proposition 2.12])

( - Δ ) p s u ( x ) = lim ϵ 0 + N B ϵ ( x ) | u ( x ) - u ( y ) | p - 2 ( u ( x ) - u ( y ) ) | x - y | N + s p 𝑑 y , x N .

In order to derive a strong comparison principle for the fractional p-Laplacian we use a weak setting. We denote by Ws,p(N) as usual the fractional Sobolev space of order (s,p) given by

W s , p ( N ) = { u L p ( N ) : N N | u ( x ) - u ( y ) | p | x - y | N + s p 𝑑 x 𝑑 y < } ,

and for an open set DN we denote

(1.2) 𝒲 0 s , p ( D ) := { u W s , p ( N ) : u 0  on  N D } .

For an introduction into fractional Sobolev spaces, we refer to [6]. Finally, we also use the space

(1.3) W ~ s , p ( D ) := { u L loc p ( N ) : D N | u ( x ) - u ( y ) | p | x - y | N + s p 𝑑 x 𝑑 y < }

to admit functions with a certain growth at infinity. Given an open set DN, qL(D), a function vW~s,p(D) is called a supersolution of (1.1) if for all nonnegative φ𝒲0s,p(D) with compact support in N we have

(1.4) N N | v ( x ) - v ( y ) | p - 2 ( v ( x ) - v ( y ) ) ( φ ( x ) - φ ( y ) ) | x - y | N + s p 𝑑 x 𝑑 y + D q | v | p - 2 v φ 𝑑 x D g φ 𝑑 x .

Similarly, we call v a subsolution of (1.1) if -v is a supersolution of (1.1). If v is a sub- and a supersolution of (1.1) andv𝒲0s,p(D), then we call v a solution of (1.1). We note that indeed the left-hand side in (1.4) is well-defined as is shown in Lemma 2.4 below.

Equations involving the fractional Laplacian, that is, the case of p=2, have been studied extensively in recent years (see, e.g., [1] and the references therein), whilst for its nonlinear counterpart there are still several unanswered questions. Existence of solutions and their regularity has been treated in [5, 15, 10, 11]. In particular, the question of existence of nontrivial solutions to problem (1.1) in the case q=0 with nontrivial outside data has been studied in [5, 15]. Let us also mention [17], where the Rayleigh quotient associated to (-Δ)ps has been studied, and [14], which analyzes the obstacle problem associated with the fractional p-Laplacian. In this work, we prove a strong comparison principle for equations of type (1.1) and apply this to equations in starshaped rings and in the half space.

Theorem 1.1 (Strong Comparison Principle).

Let s(0,1), let p>1, let DRN be an open set, let qL(D), q0, let gLp(D), where p=pp-1, and let v,wW~s,p(D) be such that v is a supersolution and w a subsolution of (1.1) with vw. Assume one of the following conditions holds:

  1. 1 1 - s < p 2 , and v L ( N ) or w L ( N ) .

  2. p 2 and for some α ( 0 , 1 ] with α ( p - 2 ) > s p - 1 we have v C loc α ( D ) L ( N ) or w C loc α ( D ) L ( N ) .

Then either v=w a.e. in RN or

essinf K ( v - w ) > 0 for all  K D .

The weak comparison principle for the fractional p-Laplacian with q=0 goes back to [17] (see also [11, 15]). However, the validity of a strong comparison principle is already a delicate question in the case s=1, i.e. the case of the classical p-Laplacian. We refer here to the works [18, 19]. Note that in the above nonlocal case neither v nor w need to be solutions, and indeed to achieve such a statement we strongly use the nonlocal structure of the fractional p-Laplacian. In the case p=2, of course, the strong comparison principle follows from the strong maximum principle by linearity (see, e.g., [7]). But in general, when p2, the strong maximum principle for the fractional p-Laplacian does not imply the strong comparison principle due to the nonlinear structure of the operator. For the strong maximum principle and a Hopf-type lemma for the fractional p-Laplacian, we refer to the recent work [4].

For an application of Theorem 1.1, we investigate bounded nonnegative solutions of (1.1) in starshaped rings, i.e. we analyze

(1.5) { ( - Δ ) p s u + q ( x ) | u | p - 2 u = 0 in  D = D 0 D ¯ 1 , u = 0 on  N D 0 , u = 1 on  D 1 ,

where D0,D1N are open sets with 0D1¯D0. For our main statement, we recall that a subset A of N is said starshaped with respect to the pointx¯A if for every xA the segment (1-s)x¯+sx, s[0,1], is contained in A. If x¯=0 (as we can always assume up to a translation), we simply say that A is starshaped, meaning that for every xA we have sxA for s[0,1], or equivalently

A  is starshaped if  s A A  for every  s [ 0 , 1 ] .

The set A is said strictly starshaped if 0 is in the interior of A and any ray starting from 0 intersects the boundary of A in only one point.

By U(), , we denote the superlevel sets of a function u:N:

U ( ) := { u } = { x N : u ( x ) } .

Theorem 1.2.

Let s(0,1), let p>1, and let D=D0D¯1, where D0,D1RN are open bounded sets such that 0D1 and D¯1D0. Let q:D[0,) such that the following conditions hold:

  1. q is a bounded Borel-function.

  2. For all t 1 and x N such that t x D , we have t s p q ( t x ) q ( x ) .

Moreover, let u be a continuous bounded weak solution of (1.5) such that 0u1, and assume D0 and D1 are starshaped. Then the superlevel sets U() of u are starshaped for (0,1).

If in addition D0 and D1 are strictly starshaped sets and

  1. 1 1 - s < p 2 or

  2. p 2 and u C loc α ( D ) for some α ( 0 , 1 ] with α ( p - 2 ) > s p - 1 ,

then the superlevel sets U() of u are strictly starshaped for (0,1).

Remark 1.3.

  1. The starshapedness of superlevel sets is indeed a consequence of the weak comparison principle, hence the assumptions are rather general in this case. To prove the strict starshapedness of superlevel sets, however, we need the strong comparison principle and hence stronger assumptions on u, s, and p in view of Theorem 1.1. We note that in the case q0, existence and local Hölder regularity of solutions of (1.5) has been discussed in [5], so Theorem 1.2 can be applied for p(0,1), s<p-1p, and for any p2, s<1p.

  2. In the case p=2, neither the bounds on s nor the regularity assumption on u are necessary (see [12]).

Let us close this introduction with the following further result in half spaces (see also [8, 3, 2] for similar results).

Theorem 1.4.

Let s(0,1), p>1 and set R+N:={xRN:x1>0}. Moreover, let qL(R+N), q0, and let uW0s,p(R+N)L(R+N) be a nonnegative continuous function which satisfies

( - Δ ) p s u + q ( x ) | u | p - 2 u = 0 in  + N , lim | x | u ( x ) = 0 .

If q is increasing in the direction of x1, i.e. q(x+te1)q(x) for all xΩ, t0, and

  1. 1 1 - s < p 2 or

  2. p 2 and u C loc α ( + N ) for some α ( 0 , 1 ] with α ( p - 2 ) > s p - 1 ,

then u0 on RN.

The article is organized as follows: In Section 2, we give some basic properties on the involved function spaces and useful elementary inequalities. In Section 3, we give the proof of a variant of a weak comparison principle and then prove Theorem 1.1. The proofs of Theorem 1.2 and 1.4 are given in Section 4.

2 Preliminaries and Notation

We will use the following notation: For subsets D,UN, we denote by Dc:=ND the complement of D in N, and we write dist(D,U):=inf{|x-y|:xD,yU}. If D={x} is a singleton, we write dist(x,U) in place of dist({x},U). The notation UD means that U¯ is compact and contained in D. For UN and r>0, we consider Br(U):={xN:dist(x,U)<r}, and we let, as usual Br(x)=Br({x}) be the open ball in N centered at xN with radius r>0. For any subset MN, we denote by 1M:N the characteristic function of M, and by diam(M) the diameter of M. If M is measurable, |M| denotes the Lebesgue measure of M. For the unit ball, we will use in particular ωN:=|B1(0)|. Moreover, if w:M is a function, we let w+=max{w,0} and w-=-min{w,0} denote the positive and negative part of w, respectively.

2.1 Some Elementary Inequalities

We use the notation aq:=|a|q-1a for any a, q>0. Note that for a0 we have aq=aq, and for a<0 we have aq=-|a|q. Moreover, we have the following elementary inequalities of this function.

Lemma 2.1 (see [11, Section 2.2]).

For all b0, q>0,

(2.1) ( a + b ) q max { 1 , 2 q - 1 } ( a q + b q ) if  a 0 .
(2.2) ( a + b ) q - a q 2 1 - q b q if  a , q 1 .

Lemma 2.2.

Let M,q>0. Then there are CM,1,CM,2>0 such that for all a[-M,M], b0,

(2.3) a q - ( a - b ) q C M , 1 max { b , b q } ,
(2.4) ( a + b ) q - a q C M , 2 min { b , b q } .

Proof.

Inequality (2.3) is shown in [11, Section 2.2]. Moreover, if q1, then (2.4) follows from (2.2) and indeed no bound on a is needed. For q(0,1), fix M>0 as stated and let a[-M,M]. Note that the map t(t+a)q-tq satisfies, for t[-1,1],

( t + 1 ) q - t q = q t t + 1 | v | q - 1 d v q max { | t | , | t + 1 | } q - 1 q 2 q - 1

since q<1. Hence for b>max{0,|a|} we have

( a + b ) q - a q b q = ( a b + 1 ) q - ( a b ) q q 2 q - 1 .

And for 0b|a|, using again that q<1, we have

( a + b ) q - a q = q b 0 1 | a + v b | q - 1 𝑑 v q ( | a | + | b | ) q - 1 b q 2 q - 1 M q - 1 b .

Lemma 2.3 (see [16, Lemma 2]).

For all q(0,1], there is C>0 such that

(2.5) | ( a + b ) q - a q | C | b | q for all  a , b .

2.2 Function Spaces and Their Properties

In the following, we let s(0,1), p>1, and DN open. We let 𝒲0s,p(D) and W~s,p(D) as introduced in (1.2) and (1.3), respectively. Moreover, we set formally for functions u,v:N,

u , v s , p := N N ( u ( x ) - u ( y ) ) ( p - 1 ) ( v ( x ) - v ( y ) ) | x - y | N + s p 𝑑 x 𝑑 y .

Recall that 𝒲0s,p(D) is a Banach space with the norm

u W s , p := ( u L p ( D ) p + u , u s , p ) 1 p ,

and that it corresponds to the completion of Cc(D) with respect to this norm (see, e.g., [9]).

Lemma 2.4.

The map ,s,p:W~s,p(D)×W0s,p(D)R is well-defined.

Proof.

We have by Hölder’s inequality with q=pp-1,

| u , v s , p | N N | u ( x ) - u ( y ) | p - 1 | v ( x ) - v ( y ) | | x - y | N + s p 𝑑 x 𝑑 y
= D N | u ( x ) - u ( y ) | p - 1 | v ( x ) - v ( y ) | | x - y | N + s p 𝑑 x 𝑑 y + N D D | u ( x ) - u ( y ) | p - 1 | v ( x ) | | x - y | N + s p 𝑑 x 𝑑 y
( D N | u ( x ) - u ( y ) | p | x - y | [ N q + s ( p - 1 ) ] q 𝑑 x 𝑑 y ) 1 q ( D N | v ( x ) - v ( y ) | p | x - y | [ N p + s ] p 𝑑 x 𝑑 y ) 1 p
+ ( N D D | u ( x ) - u ( y ) | p | x - y | [ N q + s ( p - 1 ) ] q 𝑑 x 𝑑 y ) 1 q ( N D D | v ( x ) | p | x - y | [ N p + s ] p 𝑑 x 𝑑 y ) 1 p
2 ( D N | u ( x ) - u ( y ) | p | x - y | N + s p 𝑑 x 𝑑 y ) 1 q v W s , p ( N ) < .

Lemma 2.5.

We have that W~s,p(D) is a vector space with the following properties:

  1. C c 0 , 1 ( N ) W s , p ( N ) W ~ s , p ( D ) .

  2. If u W ~ s , p ( D ) , then u ± W ~ s , p ( D ) .

Proof.

The fact that W~s,p(D) is a vector space follows from (2.1). Moreover, we have Cc0,1(N)Ws,p(N) (see, e.g., [9]), and uWs,p(N)W~s,p(D) is trivial. For the second statement, note that we have |u|W~s,p(D) since

| u ( x ) - u ( y ) | | | u | ( x ) - | u | ( y ) | for all  x , y N .

Hence 2u±=|u|±uW~s,p(D). ∎

Lemma 2.6.

Let D be bounded and uW~s,p(D) with u=0 on RND. Then uW0s,p(D).

Proof.

Since D is bounded, we have uLp(D). Moreover,

N N | u ( x ) - u ( y ) | p | x - y | N + s p 𝑑 x 𝑑 y = D N | u ( x ) - u ( y ) | p | x - y | N + s p 𝑑 x 𝑑 y + N D D | u ( x ) | p | x - y | N + s p 𝑑 x 𝑑 y
D N | u ( x ) - u ( y ) | p | x - y | N + s p 𝑑 x 𝑑 y + N D | u ( x ) - u ( y ) | p | x - y | N + s p 𝑑 x 𝑑 y
= 2 D N | u ( x ) - u ( y ) | p | x - y | N + s p 𝑑 x 𝑑 y ,

which is bounded by assumption. ∎

An immediate consequence of Lemmas 2.6 and 2.5 is the following corollary.

Corollary 2.7.

Let D be bounded and uW~s,p(D) with u0 on RND. Then u-W0s,p(D).

In the following, we also say that vW~s,p(D) satisfies (in weak sense)

( - Δ ) p s v g in  D

for g[𝒲0s,p(D)], the dual of 𝒲0s,p(D), if for all nonnegative φ𝒲0s,p(D) with compact support in N we have

u , φ s , p Ω g ( x ) φ ( x ) 𝑑 x .

Similarly, we use “” and “=”.

Lemma 2.8 (cf. [11, Lemma 2.9]).

Let t>0 and let uW~s,p(D) satisfy (-Δ)psu=g in D for some g[W0s,p(D)]. Then the function v:RNR, v(x)=u(tx) satisfies vW~s,p(t-1D) and

( - Δ ) p s v = t s p g ( t ) on  t - 1 D .

Proof.

Let φ𝒲0s,p(t-1D). Then clearly φ(t)𝒲0s,p(D) and

v , φ s , p = N N ( u ( x ) - u ( y ) ) ( p - 1 ) ( φ ( x t ) - φ ( y t ) ) | x t - y t | N + s p 𝑑 x 𝑑 y
= t - N + s p N N ( u ( x ) - u ( y ) ) ( p - 1 ) ( φ ( x t ) - φ ( y t ) ) | x - y | N + s p t - 2 N 𝑑 x 𝑑 y
= t - N + s p D g ( x ) φ ( x t ) 𝑑 x
= t - 1 D t s p g ( t x ) φ ( x ) 𝑑 x .

3 Comparison Principles

The following is a slight variant of the weak maximum principle presented in [11, Proposition 2.10], [15, Lemma 6], and [17, Lemma 9].

Lemma 3.1.

Let DRN be an open set, let qL(D), q0, and gLp(D), where p=pp-1 . If v,wW~s,p(D) are super- and subsolution, respectively, of (-Δ)psu+q(x)u(p-1)=g such that vw in RND and

lim inf | x | ( v ( x ) - w ( x ) ) 0 ,

then vw a.e. in RN.

Proof.

First assume D is bounded and set u(x)=v(x)-w(x) and

Q ( x , y ) := ( p - 1 ) 0 1 | w ( x ) - w ( y ) + t ( u ( x ) - u ( y ) ) | p - 2 𝑑 t , P ( x ) = ( p - 1 ) 0 1 | w ( x ) + t u ( x ) | p - 2 𝑑 t .

Note that P0 on N, and Q(x,y)=Q(y,x)0 for (x,y)N×N. Moreover, if P(x)=0, then w(x)=0=u(x), and if Q(x,y)=0, then w(x)=w(y) and u(x)=u(y). Note that u0 on ND, and hence u-𝒲0s,p(D) due to Corollary 2.7. Note that for any φ𝒲0s,p(D), φ0, we have

- D q ( x ) P ( x ) u ( x ) φ ( x ) 𝑑 x = - D q ( x ) v ( p - 1 ) ( x ) φ ( x ) + q ( x ) w ( p - 1 ) ( x ) φ ( x ) d x
v , φ s , p - w , φ s , p
= N N [ ( v ( x ) - v ( y ) ) ( p - 1 ) - ( w ( x ) - w ( y ) ) ( p - 1 ) ] ( φ ( x ) - φ ( y ) ) | x - y | N + s p 𝑑 x 𝑑 y
= N N Q ( x , y ) | x - y | N + s p ( u ( x ) - u ( y ) ) ( φ ( x ) - φ ( y ) ) 𝑑 x 𝑑 y .

Since D is bounded, we have u-𝒲0s,p(D). Hence, since

[ u ( x ) - u ( y ) ] [ u - ( x ) - u - ( y ) ] = - 2 u + ( x ) u - ( y ) - ( u - ( x ) - u - ( y ) ) 2 0

for x,yN, we have with φ=u-,

- q - L ( D ) D u - ( x ) 2 P ( x ) 𝑑 x - N N Q ( x , y ) | x - y | N + s p ( u - ( x ) - u - ( y ) ) 2 𝑑 x 𝑑 y
- D u - ( x ) 2 N D 2 Q ( x , y ) | x - y | N + s p 𝑑 y 𝑑 x 0 .

Since q0, this implies

0 = D u - ( x ) 2 N D Q ( x , y ) | x - y | N + s p 𝑑 y 𝑑 x ,

which by an argumentation as in [17, Lemma 9] is only possible if u-=0 a.e. Indeed, we have for a.e. (x,y)D×(ND) either u-(x)=0 or Q(x,y)=0, but in the latter case we have u(x)=u(y) as mentioned above. Since xsuppu- and yND, we have u(x)0u(y), so that u(x)=0=u(y). Hence also in the latter case it follows that u-(x)=0. Hence the claim follows for bounded sets.

If D is unbounded, then since

lim inf | x | ( v ( x ) - w ( x ) ) 0 ,

we find for every ϵ>0 a number R>0 such that vϵw in NDR, where vϵ:=v+ϵ and DR:=BR(0)D. Moreover, for φ𝒲0s,p(D), φ0, with compact support in N, using that q0 and tt(p-1) is increasing, we have

v ϵ , φ s , p + D q ( x ) v ϵ ( p - 1 ) ( x ) φ ( x ) 𝑑 x
N N ( v ( x ) + ϵ - ( v ( y ) + ϵ ) ) ( p - 1 ) ( φ ( x ) - φ ( y ) ) | x - y | N + s p 𝑑 x 𝑑 y + D q ( x ) v ( p - 1 ) ( x ) φ ( x ) 𝑑 x
= v , φ s , p + D q ( x ) v ( p - 1 ) ( x ) φ ( x ) 𝑑 x
D g ( x ) φ ( x ) 𝑑 x ,

hence vϵ is a supersolution of (-Δ)psu+q(x)u(p-1)=g in DR, while w is a subsolution of this equation in DR. The first part gives v+ϵ=vϵw in N, and since ϵ>0 is arbitrary, this finishes the proof. ∎

Remark 3.2.

We note that almost with the same proof it is possible to show the following: Let DN be an open bounded set, let qL(D), q0, and assume v,wW~s,p(D) satisfy in weak sense

( - Δ ) p s v - ( - Δ ) p s w - q ( x ) ( v - w ) ( p - 1 ) in  D ,
v w in  N D .

Then vw a.e. in N.

Lemma 3.3 (see [11, Lemma 2.8]).

Let DRN be an open bounded set, let KRND, and let hLloc1(RN). Then for any vW~s,p(D) we have in weak sense

( - Δ ) p s ( v + h 1 K ) = ( - Δ ) p s v + H in  D ,

with

H ( x ) = 2 K ( ( v ( x ) - v ( y ) ) - h ( y ) ) ( p - 1 ) - ( v ( x ) - v ( y ) ) ( p - 1 ) | x - y | N + s p 𝑑 y

for a.e. xD.

Lemma 3.4.

Let DRN be an open bounded set and let KRND with |K|>0.

  1. If p 2 , then there is C > 0 such that for any v W ~ s , p ( D ) and any δ ( 0 , 1 ] we have in weak sense

    (3.1) ( - Δ ) p s ( v - δ 1 K ) ( - Δ ) p s v + C δ p - 1 , ( - Δ ) p s ( v + δ 1 K ) ( - Δ ) p s v - C δ p - 1 .

  2. If p ( 1 , 2 ) , then for any M > 0 there is C > 0 such that for any v W ~ s , p ( D ) with v L ( N ) M and any δ ( 0 , 1 ] we have in weak sense

    (3.2) ( - Δ ) p s ( v - δ 1 K ) ( - Δ ) p s v + C δ , ( - Δ ) p s ( v + δ 1 K ) ( - Δ ) p s v - C δ .

Proof.

By Lemma 3.3, we have in weak sense

( - Δ ) p s ( v - δ 1 K ) = ( - Δ ) p s v + 2 K ( v ( x ) - v ( y ) + δ ) ( p - 1 ) - ( v ( x ) - v ( y ) ) ( p - 1 ) | x - y | N + s p 𝑑 y .

We will start by showing the first inequalities in (3.1) and (3.2).

Case 1: p2. Then by inequality (2.2) we have

2 K ( v ( x ) - v ( y ) + δ ) ( p - 1 ) - ( v ( x ) - v ( y ) ) ( p - 1 ) | x - y | N + s p 𝑑 y 2 3 - p δ ( p - 1 ) K 1 | x - y | N + s p 𝑑 y .

Hence the first inequality in (3.1) holds with C1=23-p|K|supxD,yK|x-y|-N-sp.

Case 2: p(1,2). Then with (2.4) we have

2 K ( v ( x ) - v ( y ) + δ ) ( p - 1 ) - ( v ( x ) - v ( y ) ) ( p - 1 ) | x - y | N + s p 𝑑 y C M , 2 δ K 1 | x - y | N + s p 𝑑 y .

Hence the first inequality in (3.2) holds with C2=CM,2|K|supxD,yK|x-y|-N-sp.

For the second inequalities in (3.1) and (3.2), note that

( - Δ ) p s ( v - δ 1 K ) = ( - Δ ) p s v + 2 K ( v ( x ) - v ( y ) - δ ) ( p - 1 ) - ( v ( x ) - v ( y ) ) ( p - 1 ) | x - y | N + s p 𝑑 y
= ( - Δ ) p s v - 2 K ( v ( x ) - v ( y ) - δ + δ ) ( p - 1 ) - ( v ( x ) - v ( y ) - δ ) ( p - 1 ) | x - y | N + s p 𝑑 y .

Hence this part follows similarly. ∎

Lemma 3.5.

Let DRN be an open bounded set and let s(0,1), p>1, and fCc2(D).

  1. If 1 1 - s < p 2 , then for any v W ~ s , p ( D ) there is C > 0 such that for all a [ - 1 , 1 ] in weak sense

    (3.3) | ( - Δ ) p s ( v - a f ) - ( - Δ ) p s v | | a | p - 1 C in  supp f .

  2. If p 2 , then for any v W ~ s , p ( D ) C loc α ( D ) L ( N ) , α(0,1] with α(p-2)>sp-1, there is C>0 such that for all a[-1,1] in weak sense

    (3.4) | ( - Δ ) p s ( v - a f ) - ( - Δ ) p s v | | a | C in  supp f .

Proof.

Let s(0,1) and a[-1,1], fix fCc2(D), R=2diam(D)+1, U:=suppf, and

K := | α | 2 α f L ( N ) .

Moreover, let vW~s,p(D). If p(11-s,2], then we have for any φ𝒲0s,p(U), φ0, and a constant C1>0 given by (2.5),

| N N ( ( v ( x ) - v ( y ) - a ( f ( x ) - f ( y ) ) ) ( p - 1 ) - ( v ( x ) - v ( y ) ) ( p - 1 ) ) ( φ ( x ) - φ ( y ) ) | x - y | N + s p 𝑑 x 𝑑 y |
2 C 1 | a | p - 1 N φ ( x ) N | f ( x ) - f ( x + y ) | p - 1 | y | N + s p 𝑑 x 𝑑 y
2 C 1 | a | p - 1 K p - 1 U φ ( x ) ( B R ( 0 ) | y | - N + ( 1 - s ) p - 1 𝑑 y + N B R ( 0 ) | y | - N - s p 𝑑 y ) 𝑑 x
2 C 1 N ω N | a | p - 1 K p - 1 U φ ( x ) ( 0 R r ( 1 - s ) p - 2 𝑑 r + R r - 1 - s p 𝑑 r ) 𝑑 x
2 | a | p - 1 C 1 K p - 1 N ω N ( 1 ( 1 - s ) p - 1 + 2 s p ) U φ ( x ) 𝑑 x ,

where ωN=|B1(0)|. Hence (3.3) holds with

C = 2 C 1 K p - 1 N ω N ( 1 ( 1 - s ) p - 1 + 2 s p ) .

Next let p2, assume additionally that vL(N)Clocα(D) for some α(0,1) with α(p-2)>sp-1, and set for x,yN,

Q ( x , y ) := ( p - 1 ) 0 1 | v ( x ) - v ( y ) - a t ( f ( x ) - f ( y ) ) | p - 2 𝑑 t .

Note that Q(x,y)=Q(y,x)0 for any x,yN. Moreover, there is

C 2 = C 2 ( p , v L ( N ) , f ) and C 3 = C 3 ( p , v C s + ϵ ( D ) , f )

such that

(3.5) Q ( x , y ) C 2 for  x , y N ,
(3.6) Q ( x , y ) C 3 | x - y | α ( p - 2 ) for  x , y U ,

where we used that U¯D. Moreover, we have dist(suppf,Dc)=δ>0. Fix φ𝒲0s,p(U), φ0. Then, since

( v ( x ) - v ( y ) - a ( f ( x ) - f ( y ) ) ) ( p - 1 ) - ( v ( x ) - v ( y ) ) ( p - 1 ) = - a Q ( x , y ) ( f ( x ) - f ( y ) ) ,

we have

| N N ( ( v ( x ) - v ( y ) - a ( f ( x ) - f ( y ) ) ) ( p - 1 ) - ( v ( x ) - v ( y ) ) ( p - 1 ) ) ( φ ( x ) - φ ( y ) ) | x - y | N + s p 𝑑 x 𝑑 y |
= | a | | N N ( f ( x ) - f ( y ) ) ( φ ( x ) - φ ( y ) ) | x - y | N + s p Q ( x , y ) 𝑑 x 𝑑 y |
2 | a | U φ ( x ) | lim ϵ 0 B ϵ c ( x ) ( f ( x ) - f ( y ) ) Q ( x , y ) | x - y | N + s p 𝑑 y | 𝑑 x .

We now follow closely the lines of the proof of [13, Lemma 3.8] to show that

(3.7) sup x D | lim ϵ 0 B ϵ c ( x ) ( f ( x ) - f ( y ) ) Q ( x , y ) | x - y | N + s p 𝑑 y | C 4

for a constant C4=C4(D,N,p,f,vCα(D),vL(N))>0. Clearly, once (3.7) is shown, this finishes the proof of (3.4). To see (3.7), fix xU and note that Bδ(x)D. Let ϵ(0,δ). Moreover, since fCc2(D), we have

| 2 f ( x ) - f ( x - y ) - f ( x + y ) | K | y | 2 for all  x , y N ,

and from (3.6) and (2.1) there is K2>0 such that

| Q ( x , x - y ) - Q ( x , x + y ) | K 2 | y | α ( p - 2 ) for all  x supp f , y B δ ( 0 ) .

Hence with (3.5) and (3.6), we have

| B ϵ c ( x ) ( f ( x ) - f ( y ) ) Q ( x , y ) | x - y | N + s p 𝑑 y | = | B ϵ c ( 0 ) ( f ( x ) - f ( x ± y ) ) Q ( x , x ± y ) | y | N + s p 𝑑 y |
= | 1 2 B ϵ c ( 0 ) ( 2 f ( x ) - f ( x + y ) - f ( x - y ) ) Q ( x , x + y ) | y | N + s p d y
+ 1 2 B ϵ c ( 0 ) ( f ( x ) - f ( x - y ) ) ( Q ( x , x + y ) - Q ( x , x - y ) ) | y | - N - s p d y |
C 3 K 2 B δ ( 0 ) B ϵ ( 0 ) | y | 2 - N - s p + α ( p - 2 ) 𝑑 y + C 2 4 K B δ c ( 0 ) | y | - N - s p 𝑑 y
+ K 2 K 2 B δ ( 0 ) B ϵ ( 0 ) | y | 1 + α ( p - 2 ) - N - s p 𝑑 y
C 3 2 N K 1 ω N 0 δ ρ 1 - s p + α ( p - 2 ) 𝑑 ρ + C 2 K 4 N ω N δ ρ - 1 - s p 𝑑 ρ
+ K 2 K 2 N ω N 0 δ ρ α ( p - 2 ) - s p 𝑑 ρ
= C 3 K N ω N δ 2 - s p + α ( p - 2 ) 2 ( 2 - s p + α ( p - 2 ) ) + C 2 K 4 s p N ω N δ - s p + K 2 K N ω N δ 1 - 2 s + α ( p - 2 ) 2 ( 1 - s p + α ( p - 2 ) )
= : C 4 < ,

where we have used α(p-2)>sp-1. ∎

Lemma 3.6.

Let DRN be an open bounded set, let KRND with |K|>0, δ(0,1], s(0,1), and p>1. Moreover, fix fCc2(D) with 0f1.

  1. If 1 1 - s < p 2 , then for any v W ~ s , p ( D ) L ( N ) there is a 0 , b > 0 such that in weak sense for all a ( 0 , a 0 ] ,

    (3.8)

    ( - Δ ) p s ( v - a f - δ 1 K ) ( - Δ ) p s v + b in  supp f ,
    ( - Δ ) p s v - b ( - Δ ) p s ( v + a f + δ 1 K ) in  supp f .

  2. If p 2 , then for any v W ~ s , p ( D ) C α ( D ) L ( N ) , α(0,1] with α(p-2)>sp-1, there is a0,b>0 such that (3.8) holds in weak sense for all a(0,a0].

Proof.

Fix v, s, p as stated. By Lemma 3.4, we have in all cases

( - Δ ) p s ( v - a f - δ 1 K ) ( - Δ ) p s ( v - a f ) + C min { δ , δ p - 1 }

for some C>0. Moreover, by Lemma 3.5 we have for some C~>0 in weak sense

( - Δ ) p s ( v - a f ) ( - Δ ) p s v - max { a , a p - 1 } C ~ , a ( 0 , 1 ] .

Hence we may fix a0=a0(δ)(0,1] such that b=-max{a0,a0p-1}C~+Cmin{δ,δp-1}>0. This shows the first inequality in (3.8). The second inequality in (3.8) follows similarly. ∎

Proof of Theorem 1.1.

We start with the case vL(N). Assume there is MN with 0<|M|<|D| and δ:=essinfM(v-w)>0. Without loss of generality, we may assume δ1. Fix KDM and let fCc2(DM) be given with f1 in K and 0f1. Let a0,b>0 be given by Lemma 3.6 and fix a(0,a0]. Furthermore, let ua:=v-af-δ1M and note that uW~s,p(suppf). Then, assuming for (ii) in addition vClocα(D) for α(0,1] as stated, we have in weak sense in suppf by Lemma 3.6,

( - Δ ) p s u a ( - Δ ) p s v + b
- q ( x ) v ( p - 1 ) + b
- q ( x ) u a ( p - 1 ) + b + q ( x ) ( ( v - a f ) ( p - 1 ) - v ( p - 1 ) )
- q ( x ) u a ( p - 1 ) + b - q L ( D ) ( v ( p - 1 ) - ( v - a ) ( p - 1 ) ) .

By (2.5) if p2, or by (2.3) with M=vL(N), there is C>0 depending only on p, and if p>2 on M, such that

( v ( p - 1 ) - ( v - a ) ( p - 1 ) ) C max { a , a p - 1 } .

It follows that

b - q L ( D ) ( v ( p - 1 ) - ( v - a ) ( p - 1 ) ) b - q L ( D ) C max { a , a p - 1 } .

Hence we may choose a1(0,a0] such that b-qL(D)Cmax{a1,a1p-1}>0. Then ua1 satisfies

( - Δ ) p s u a 1 + q ( x ) u a 1 ( p - 1 ) g in  supp f ,

and ua1w in Nsuppf. Lemma 3.1 implies ua1w a.e. in suppf, and hence vw+a1f in suppf. In particular,

v w + a 1 in  K .

Since K and f were chosen arbitrarily, this shows

essinf K ( v - w ) > 0 for all  K D M .

Since 0<|M|<|D|, we may fix M~DM with δ~:=essinfM~(v-w)>0. By repeating the above argument now with DM~ in place of DM, this shows the claim for case (i) and for case (ii) with vClocα(D)L(N).

If wClocα(D)L(N), we note that Lemma 3.6 implies also the existence of a0,b>0 such that

( - Δ ) p s ( w + a f + δ 1 K ) ( - Δ ) p s w - b

for all a(0,a0]. Proceeding as in the first case, we find vw+af in suppf, and since f was chosen arbitrarily, this finishes the proof similarly to the first case. ∎

Remark 3.7.

We note that, as for the weak maximum principle, it is also with almost the same proof possible to show the following: Let DN be an open set, let qL(D), q0, s(0,1), p>1, and assume that v,wW~s,p(D) satisfy in weak sense

( - Δ ) p s v - ( - Δ ) p s w - q ( x ) ( v - w ) ( p - 1 ) in  D ,
v w in  N .

If one of the two conditions

  1. 1 1 - s < p 2 and vL(N) or wL(N), or

  2. p 2 and for some α(0,1] with α(p-2)>sp-1 we have vClocα(D)L(N) or wClocs(D)L(N),

holds, then either vw a.e. in N or essinfK(v-w)>0 for all KD.

Corollary 3.8 (Strong Maximum Principle).

Let DRN be an open set and let f:D×R[0,) be such that f(x,0)=0 for all xD and

K f ( x , v ( x ) ) φ ( x ) 𝑑 x < for all  K D and  v , φ L p ( K ) , v , φ 0 .

Moreover, let vW~s,p(D) be a nonnegative function satisfying in weak sense

( - Δ ) p s v f ( x , v ) in  D .

If p>11-s, then either v0 in RN or essinfKv>0 for all KΩ.

Proof.

Since 0Ws,p(N)Cc0,1(N) satisfies (-Δ)ps0=0f(x,v)(-Δ)psv, an application of Theorem 1.1 proves the claim. ∎

4 Starshaped Superlevel Sets

As in [12], we use the following observation.

Lemma 4.1 (see [12, Lemma 3.1]).

Let u:RNR such that M=maxRNu=u(0). Then the superlevel sets U(), R, of u are all (strictly) starshaped if and only if u(tx)u(x) (u(tx)<u(x)) for every xRN and every t>1.

Theorem 4.2.

Let D=D0D¯1 with D0,D1RN open bounded sets such that 0D1 and D¯1D0. Moreover, let b0,b1L(RN)W~s,p(RN) such that b00 on D0 and b11 on D1, let qL(D) be a nonnegative function, and let gLp(D) with p=pp-1 such that both functions satisfy (A2), i.e. the following condition holds:

  1. For all t 1 and x N such that t x D 0 D ¯ 1 , we have t s p q ( t x ) q ( x ) and t s p g ( t x ) g ( x ) .

Let uW~s,p(RN) be a continuous solution of

{ ( - Δ ) p s u + q ( x ) | u | p - 2 u = - g in  D , u = b 0 on  D 0 c , u = b 1 on  D 1 ,

such that 0u1 in D. If b0|D0c and b1|D1 have starshaped superlevel sets, then the following holds:

  1. If D 0 and D 1 are starshaped sets, then the superlevel sets U ( ) of u are starshaped for ( 0 , 1 ) .

  2. If D 0 and D 1 are strictly starshaped sets, 0 < u < 1 in D and

    1. 1 1 - s < p 2 or

    2. p 2 and u C loc α ( D ) for some α ( 0 , 1 ] with α ( p - 2 ) > s p - 1 ,

    then the superlevel sets U ( ) of u are strictly starshaped for ( 0 , 1 ) .

Proof.

We proceed as in the proof of [12, Theorem 1.8]. Let D0, D1, b0, b1, and u be given as for (i). Note that by assumption it follows that uL(N). Denote for any t>1 and any function v:N,

v t ( x ) = v ( t x ) x N .

Thanks to Lemma 4.1, the starshapedness of the level sets of u is equivalent to

u u t in  N  for  t > 1 .

Observe that since the superlevel sets of b0 and b1 are starshaped and 0u1 in D, we have uut in ND0 and in t-1D¯1, and

u ( x ) u t ( x ) for  x D 0 ( t - 1 D 0 )  and  x D ¯ 1 ( t - 1 D ¯ 1 ) .

Put Dt=(t-1D0)D¯1. It remains to investigate ut in Dt. Note that since D0 is bounded, Dt is empty for t large enough. By Lemma 2.8, we get (in weak sense)

( - Δ ) p s u t = t s p [ ( - Δ ) p s u ] t = - t s p q ( t x ) u t ( p - 1 ) - t s p g ( t x ) - q ( x ) u t ( p - 1 ) + g ( x ) in  D t ,

where we used that ut0 in N. Hence Lemma 3.1 implies uut in N. This proves (i).

If in addition u, D0, and D1 satisfy the assumptions of (ii), then observe that with the same argument as above Theorem 1.1 yields either utu in N or u>ut in Dt. Since uut in N is not possible for t>1 due to the strict inequality 0<u<1 in D, we must have u>ut in Dt for all t>1. This proves (ii). ∎

Proof of Theorem 1.2.

If D0 and D1 are starshaped, then the result follows immediately from Theorem 4.2 (i). Hence let D0 and D1 be strictly starshaped. Since the functions v1 satisfies (-Δ)psv+q(x)|v|p-2v=q(x)0 in D and vu, vu in Dc, Theorem 1.1 implies u<1 in D. In a similar way, the function w0 satisfies (-Δ)psw+q(x)|w|p-2w=0 in D and uw, uw in Dc, Theorem 1.1 implies u>0 in D. Hence the claim follows from Theorem 4.2 (ii) with b00 and b11. ∎

Proof of Theorem 1.4.

Let q, u be as stated and assume u0 on N. Then by the strong comparison principle we must have u>0 on +N since 0 is solution of (-Δ)psu+q(x)u(p-1)=0 and u0. For t0, denote ut(x):=u(x+te1) for xN and Ht:={x+N:x1>t}. Then we have in weak sense for all t0,

( - Δ ) p s u + q ( x ) u ( p - 1 ) ( - Δ ) p s u t ( x ) + q ( x ) u t ( p - 1 ) on  H t

by the assumptions on q. Hence for all t0, since lim|x|(u(x)-ut(x))=0, Lemma 3.1 implies utu on Ωt. We state the following claim:

(4.1) for all  t > 0 ,  we have  u t < u  on  H t .

Fix t>0 and assume by contradiction that utu on N. But then u0 on {xN:0<x1<t}, which is a contradiction to the fact that u>0 on +N. Hence utu on N, and Theorem 1.1 implies (4.1) since t>0 is arbitrary.

Note that (4.1) implies that u is strictly decreasing in x1, but since u0, u=0 on (+N)c and u is continuous, this is a contradiction, and hence we must have u0 on N as claimed. ∎


Communicated by Patrizia Pucci


Acknowledgements

The author thanks Tadeusz Kulczycki, Paolo Salani, and Giampiero Palatucci for careful reading and discussions. Moreover, he thanks Tobias Weth for raising the question on the strong comparison principle.

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Received: 2017-06-09
Revised: 2017-08-21
Accepted: 2017-11-08
Published Online: 2017-12-05
Published in Print: 2018-11-01

© 2018 Walter de Gruyter GmbH, Berlin/Boston

This work is licensed under the Creative Commons Attribution 4.0 International License.

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