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BY 4.0 license Open Access Published by De Gruyter May 8, 2019

The Concentration Behavior of Ground States for a Class of Kirchhoff-type Problems with Hartree-type Nonlinearity

  • Guangze Gu and Xianhua Tang EMAIL logo

Abstract

In this paper, we consider the Kirchhoff equation with Hartree-type nonlinearity

{ - ( ε 2 a + ε b 3 | u | 2 d x ) Δ u + V ( x ) u = ε μ - 3 ( 3 K ( y ) F ( u ( y ) ) | x - y | μ d y ) K ( x ) f ( u ) , u H 1 ( 3 ) ,

where ε>0 is a small parameter, a,b>0, μ(0,3), V,K are two positive continuous function and F is the primitive function of f which is superlinear but subcritical at infinity in the sense of the Hardy–Littlewood–Sobolev inequality. We show that the equation admits a positive ground state solution for ε>0 sufficiently small. Furthermore, we prove that these ground state solutions concentrate around such points which are both the minima points of the potential V and the maximum points of the potential K as ε0.

1 Introduction and Main Results

In the present paper, we investigate the existence and concentration behavior of solutions for the Kirchhoff equation with Hartree-type nonlinearity

(1.1) { - ( ε 2 a + ε b 3 | u | 2 d x ) Δ u + V ( x ) u = ε μ - 3 ( 3 K ( y ) F ( u ( y ) ) | x - y | μ d y ) K ( x ) f ( u ) , u H 1 ( 3 ) ,

where the potentials V and K satisfy the following conditions:

  1. V , K L ( 3 ) are uniformly continuous and Vmin:=minx3V(x)>0, infK>0;

  2. either Vmin<V<+ and there exists x1𝒱 such that K(x1)K(x) for |x|R with R0 sufficiently large,

  3. or Kmax>KinfK>0 and there exists x2𝒦 such that V(x2)V(x) for |x|R with R0 sufficiently large, where Kmax:=maxx3K(x).

Moreover, we also need to assume that the nonlinearity fC1(,) verifies the following hypotheses:

  1. f ( t ) = o ( t ) as t0 and f(t)=0 for all t0;

  2. there exists c1 and 2<q<6-μ such that |f(t)|c1(1+|t|q-1) for all t>0;

  3. lim t + f ( t ) t = + ;

  4. f ( t ) t is a strictly increasing function for t>0.

We should mention that problem (1.1) is related to the stationary analogue of the Kirchhoff equation

(1.2) { u t t - ( a + b Ω | u | 2 d x ) Δ u = f ( x , u ) in Ω , u = 0 on Ω ,

which was proposed by Kirchhoff [14] as an extension of the well-known D’Alembert wave equation

ρ 2 u t 2 - ( p 0 λ + E 2 L 0 L | u x | 2 d x ) 2 u x 2 = f ( x , u )

for free vibrations of elastic strings. It is worth to notice that nonlocal problems (1.2) also appear in other fields as biological systems, where u describes a process depending on the average of itself (see, e.g., population density). Problem (1.2) began to receive a lot of attention after Lions [17] introduced a functional analysis approach.

In recent years, the Kirchhoff equation

(1.3) { - ( ε 2 a + ε b 3 | u | 2 d x ) Δ u + V ( x ) u = f ( x , u ) , u H 1 ( 3 ) ,

has been widely investigated by many researchers. He and Zou [10] firstly considered the multiplicity and concentration behavior of the positive solutions of (1.3) via using the variational methods; they showed that the number of positive solutions are related to the topology of the set where V attains its minimum and these positive solutions concentrate at a global minimum of V(x) as ε0+. For the critical case f(u)=λg(u)+|u|4u, where the subcritical term g(u)|u|p-2u with 4<p<6, Wang et al. [34] also obtain a similar result. He, Li and Peng [13] constructed a family of positive solutions which concentrates at a local minimum of V as ε0+ for a critical problem f(u)=g(u)+|u|4u with g(u)|u|p-2u (4<p<6). For the more complicated case f(u)=λ|u|p-2u+|u|4u with 2<p4, that is, f(u) does not satisfy the Ambrosetti–Rabinowitz condition (there exists μ>4 such that 0<μ0ug(s)dsg(u)u), we refer to He and Li [12]. Here we also refer to [6, 11, 28, 30, 31, 38] and the references therein for more results.

On the other hand, when b=0, problem (1.1) reduces to the nonlocal Choquard equation

(1.4) - ε 2 Δ u + V ( x ) u = ε μ - 3 ( 3 K ( y ) F ( u ( y ) ) | x - y | μ d y ) K ( x ) f ( u ) ,

which arises, for example, in some physical field such as quantum mechanics, self-gravitating matter, Hartree–Fock theory and one-component plasma; for more details, we refer to [27, 15, 23] and the references therein. There have been some works concerning the existence, multiplicity and concentration behavior of solutions to equation (1.4) via variational methods. For the case N=3, α=2 and F(u)=u2, Cingolani, Secchi and Squassina [7] proved that there exists a family of solutions which concentrates around several minimum points of the electric potential via a global penalization method. Moroz and Van Schaftingen [25] showed that equation (1.4) with F(u)=|u|q, q[2,N+αN-2), admits a family of solutions concentrating at the local minimum of the potential V via a new nonlocal penalization technique. Alves et al. [2] established the existence of ground state solutions for the critical Choquard equation (1.4) with constant coefficients and also established the existence, multiplicity and concentration behavior of semiclassical solutions by variational methods.

Recently, Alves and Yang [4] considered the Choquard equation

(1.5) - ε 2 Δ p u + V ( x ) | u | p - 2 u = ε μ - N ( N K ( y ) F ( u ( y ) ) | x - y | μ d y ) K ( x ) f ( u ) .

Using variational methods and the Ljusternik–Schnirelmann category theory, they proved the existence, multiplicity and concentration of solutions for (1.5) with K=1. They also gave some results about existence and multiplicity and concentration behavior of positive solutions under different assumptions on V and the nonlinearity f in [3, 5]. For more results, we refer the readers to [1, 18, 22, 24, 36] and the references therein.

As far as we know, there are only a few results considering equation (1.1). In a very recent paper [21], Lü considered the Kirchhoff equation with Hartree-type nonlinearity

(1.6) - ( ε 2 a + ε b 3 | u | 2 d x ) Δ u + V ( x ) u = ε μ - 3 ( 3 | u ( y ) | p | x - y | μ d y ) | u ( x ) | p - 2 u ( x ) ,

where μ(0,3), p[2,6-μ) and the potential V(x) satisfies suitable conditions. The existence, concentration behavior and decay estimate of a positive ground state solution was established. Lü [20] also showed that (1.6) with ε=1 and V(x)=1+λg(x) possesses at least one ground state solution when the parameter λ is large enough and obtained the concentration behavior of these ground state solutions as λ+.

To the best of our knowledge, it seems that the concentration behavior of solutions of (1.1) with competing potentials was not considered in the previous articles. It goes without saying that there are some difficulties in our problem. The first one is that there exists competition between the potentials V and K, which leads to difficulties for determining the concentration position of positive ground state solutions. This kind of results can be also found in [35]; see also [8, 9] for a different concentration phenomenon of semiclassical solutions for a Dirac system and a Schrödinger equation with magnetic fields. The second one is that one does not know in general 3|un|2dx3|u|2dx from unu due to the appearance of the nonlocal (3|u|2dx)Δu. So we cannot verify directly that Iε satisfies the (PSc)-condition, not to mention the unboundedness of the domain 3. Moreover, since the Hartree-type nonlinearity (3K(y)F(u(y))|x-y|μdy)K(x)f(u) is also nonlocal, this also makes our problem more complicated than problem (1.3). Thus novel technical estimates need to be established. Motivated by the above works, in this paper, we will give an affirmative answer to the above question.

We introduce the following notations before giving our main result:

𝒱 : = { x 3 : V ( x ) = V min } , V : = lim inf | x | + V ( x ) ,
𝒦 : = { x 3 : K ( x ) = K max } , K : = lim sup | x | + K ( x ) .

If (A1) holds, without loss of generality, we can assume K(x1)=maxx𝒱K(x) and set

1 = { x 𝒱 : K ( x ) = K ( x 1 ) } { x 𝒱 : K ( x ) > K ( x 1 ) } .

If (A2) holds, we may also assume V(x2)=minx𝒦V(x) and set

2 = { x 𝒦 : V ( x ) = V ( x 2 ) } { x 𝒦 : V ( x ) < V ( x 2 ) } .

Obviously, 1 and 2 are both bounded sets. Moreover, 1=2=𝒱𝒦 if 𝒱𝒦.

Our main results are the following.

Theorem 1.1.

Suppose (A0), (A1) and (f1)(f4) hold. Then we have the following statements for sufficiently small ε>0.

  1. Problem ( 1.1 ) admits a positive ground state solution w ε .

  2. w ε has a global maximum point x ε such that, up to a subsequence,

    lim ε 0 x ε = x 0 , lim ε 0 dist ( ε y ε , 1 ) = 0 .

    Moreover, v ε ( x ) : = w ε ( ε x + x ε ) converges in H 1 ( 3 ) to a positive ground state solution of

    { - ( a + b 3 | u | 2 d x ) Δ u + V ( x 0 ) u = K 2 ( x 0 ) ( 3 F ( u ( y ) ) | x - y | μ d y ) f ( u ) , u H 1 ( 3 ) .

    In particular, if 𝒱 𝒦 , then lim ε 0 dist ( x ε , 𝒱 𝒦 ) = 0 , and v ε (up to a subsequence) converges in H 1 ( 3 ) to a positive ground state solution of

    { - ( a + b 3 | u | 2 d x ) Δ u + V min u = K max 2 ( 3 F ( u ( y ) ) | x - y | μ d y ) f ( u ) , u H 1 ( 3 ) .

  3. There exists C > 0 such that

    w ε ( x ) C e - τ ε | x - η ε | .

Theorem 1.2.

The conclusions of Theorem 1.1 remain valid if we replace H1 and (A1) by H2 and (A2), respectively.

This paper is organized as follows. In Section 2, we will give some necessary preliminary lemmas. In Section 3, we study the autonomous problem of (1.1). In Section 4, we prove the existence of a positive ground state solution of problem (1.1). We are devoted to prove our main results in Section 5.

2 Preliminary Results

To prove our theorem, we consider the Sobolev space H1(3) with the standard norm

u H 1 ( 3 ) = ( 3 | u | 2 d x + 3 | u | 2 d x ) 1 / 2 .

If we make the change of variable xεx, then we may rewrite equation (1.1) in the form

(2.1) { - ( a + b 3 | u | 2 d x ) Δ u + V ( ε x ) u = ( K ( y ) F ( u ( y ) ) | x - y | μ ) K ( x ) f ( u ) , u H 1 ( 3 ) .

Thus it is enough to consider problem (2.1). In view of the presence of potential V(x), the subspace

H ε = { u H 1 ( 3 ) : 3 V ( ε x ) u ( x ) 2 d x < + }

is a Hilbert space equipped with the norm

u ε 2 = a 3 | u | 2 d x + 3 V ( ε x ) u 2 ( x ) d x

and the inner product

( u , v ) ε = a 3 u v d x + 3 V ( ε x ) u v d x .

We denote by the H-norm in the sequel for convenience.

To study problem (2.1), we will use the following Hardy–Littlewood–Sobolev inequality [16].

Proposition 2.1.

Let t,r>1 and 0<μ<N with 1t+1r+μN=2, fLt(RN) and hLr(RN). There exists a positive constant C(t,r,N,μ) (independent of f and h) such that

N N f ( x ) h ( y ) | x - y | μ d x d y C ( t , r , N , μ ) f t h r .

In particular, when F(u)=|u|q for some q>0, by Proposition 2.1, 33F(u(x))F(u(y))|x-y|μdxdy is well defined if F(u)Lt(3), where t=66-μ. Therefore, it suffices to require that

6 - μ 3 < q < 6 - μ .

The energy functional associated with (2.1) is

I ε ( u ) = 1 2 u ε 2 + b 4 ( 3 | u | 2 d x ) 2 - 1 2 3 3 K ( y ) F ( u ( y ) ) K ( x ) F ( u ( x ) ) | x - y | μ d x d y .

By Proposition 2.1, Iε is well defined in Hε and IεC1(Hε,).

The following vanishing lemma will be used later (see, e.g., [19, 37], etc.).

Lemma 2.1.

Let {un} be a bounded sequence in H1(R3), and it satisfies

lim n + sup y 3 B R ( y ) | u n ( x ) | 2 d x = 0 ,

where R>0. Then un0 in Lt(R3) for every 2<t<6.

Lemma 2.2.

Assume that (f1)(f4) hold. Then

  1. for each δ > 0 , there is C δ > 0 such that | f ( t ) | δ | t | + C δ | t | q - 1 and | F ( t ) | δ | t | 2 + C δ | t | q for all t ,

  2. F ( t ) > 0 and t f ( t ) > f ( t ) if t > 0 ,

  3. f ( t ) t 2 F ( t ) > 0 for all t > 0 , and f ( t ) t - 2 F ( t ) is increasing for t > 0 ,

  4. F ( t ) t 2 is increasing for t > 0 and lim t + F ( t ) t 2 = + .

Let us define the Nehari manifold associated with Iε by

𝒩 ε : = { u H ε { 0 } : I ε ( u ) , u = 0 } .

Below, we give some properties of the Nehari manifold 𝒩ε.

Lemma 2.3.

The following statements hold for any uHε{0}.

  1. There exists a unique t u > 0 such that t u u 𝒩 ε . Moreover, t u 𝒩 ε if and only if t = t u .

  2. There exist T 1 > T 2 > 0 independent of ε > 0 such that T 2 t ε T 1 .

Proof.

(i) Let uHε{0} be fixed, and, for t>0, by Lemma 2.2, we have

h ( t ) : = I ε ( t u ) = t 2 2 u ε 2 + b 4 t 4 ( 3 | u | 2 d x ) 2 - 1 2 3 3 K ( y ) F ( t u ( y ) ) K ( x ) F ( t u ( x ) ) | x - y | μ d x d y t 2 2 u ε 2 + b 4 t 4 ( 3 | u | 2 d x ) 2 - δ t 4 u ε 4 - C δ t q u ε 2 q ,

which implies h(t)>0 for small t>0. Moreover, by the above equation, we get

h ( t ) = lim t + t 4 { 1 2 t 2 u ε 2 + b 4 ( 3 | u | 2 d x ) 2 - 1 2 3 3 K ( y ) F ( t u ( y ) ) K ( x ) F ( t u ( x ) ) ( u ( x ) u ( y ) ) 2 | x - y | μ ( t u ( y ) ) 2 ( t u ( x ) ) 2 d x d y } - as t .

Hence h has a positive maximum, that is, there exists tu>0 such that h(tu)=0 and tuu𝒩ε. It follows from h(t)=0 that

1 t 2 3 ( a | u | 2 + V ( ε x ) u 2 ) d x + b ( 3 | u | 2 d x ) 2 = 3 3 K ( y ) F ( t u ( y ) ) K ( x ) f ( t u ( x ) ) u ( x ) t 3 | x - y | μ d x d y .

If there exists tu>tu such that tuu, tuu𝒩ε, we have

( 1 t u 2 - 1 t u 2 ) u ε = 3 3 K ( y ) K ( x ) u 2 ( y ) u 2 ( x ) | x - y | μ ( F ( t u u ( y ) ) f ( t u u ( x ) ) ( t u u ( y ) ) 2 ( t u u ( x ) ) - F ( t u u ( y ) ) f ( t u u ( x ) ) ( t u u ( y ) ) 2 ( t u u ( x ) ) ) d x d y ,

which is impossible in view of Lemma 2.2.

(ii) By tεu𝒩ε, we have

1 t ε 2 u ε 2 + C u ε 4 1 t ε 2 u ε 2 + b 4 ( 3 | u | 2 d x ) 2 3 3 K ( y ) K ( x ) u 2 ( y ) u 2 ( x ) F ( t ε u ( y ) ) f ( t ε u ( x ) ) | x - y | μ ( t ε u ( y ) ) 2 ( t ε u ( x ) ) d x d y .

So there exists T1>0 independent of ε such that T1tε.

By tε𝒩ε and Proposition 2.1, we have

t ε 2 u ε 2 t ε 2 u ε 2 + b t ε 4 4 ( 3 | u | 2 d x ) 2 δ t ε 4 u ε 4 + C δ t ε 2 q u ε 2 q ,

which implies that there exists T2>0 independent of ε such that tεT2. ∎

Lemma 2.4.

The functional Iε satisfies the mountain pass geometry.

  1. There exist α , ρ > 0 such that I ε ( u ) α if u ε = ρ .

  2. There exists an e H ε with e ε ρ such that I ε ( e ) < 0 .

Proof.

(i) For any uHε{0}, by Proposition 2.1 and Lemma 2.1, we have

I ε ( u ) = 1 2 u ε 2 + b 4 ( 3 | u | 2 d x ) 2 - 1 2 3 3 K ( y ) F ( u ( y ) ) K ( x ) F ( u ( x ) ) | x - y | μ d x d y 1 2 u ε 2 - C u ε 4 - C u ε 2 q .

Hence there exist α,ρ>0 such that Iε(u)α with uε=ρ.

(ii) Similar to Lemma 2.3, for fixed uHε{0}, we have Iε(tu)- as t+. Thus there exists t*>0 large enough such that Iε(e)<0, where e:=t*u and eερ. ∎

Lemma 2.5.

If {un} is a (PSc) sequence for Iε, then {un} is bounded in Hε.

Proof.

Assume that {un} is a (PSc) sequence for Iε, i.e.,

I ε ( u n ) c and I ε ( u n ) 0 as n + .

By Lemma 2.2, we obtain

c + o n ( 1 ) I ε ( u n ) - 1 4 I ε ( u n ) , u n = 1 4 u n ε + 1 4 3 3 K ( ε y ) F ( u ( y ) ) K ( ε x ) ( f ( u ( x ) ) u ( x ) - 2 F ( u ( x ) ) ) | x - y | μ d x d y 1 4 u n ε .

The conclusion follows. ∎

By a standard argument (see, e.g., [29, 37]), we have the following lemma.

Lemma 2.6.

Assume that (A0), (A1) and (f1)(f4) are satisfied. Then

c ε : = inf γ Γ max t [ 0 , 1 ] I ε ( γ ( t ) ) = inf u 𝒩 ε I ε ( u ) = inf u H ε { 0 } max t 0 I ε ( t u ) ,

where Γ={γ([0,1],Hε):γ(0)=0,Iε(γ(1))<0}.

3 The Autonomous Problem

In this section, we shall study the autonomous problem associated to (2.1), namely,

(3.1) { - ( a + b 3 | u | 2 d x ) Δ u + α 2 u = β 2 ( 3 F ( u ( y ) ) | x - y | μ d y ) f ( u ) , u H 1 ( 3 ) .

The solutions of (3.1) are critical points of the functional

I α β ( u ) = a 2 3 | u | 2 d x + 1 2 3 α u 2 d x + b 4 ( 3 | u | 2 d x ) 2 - β 2 2 3 3 F ( u ( y ) ) F ( u ( x ) ) | x - y | μ d x d y .

The Nehari manifold associated to Iαβ is given by

𝒩 α β : = { u H 1 ( 3 ) { 0 } : I α β ( u ) , u = 0 } ,

and the best energy on 𝒩αβ is defined by γαβ:=infu𝒩αβIαβ(u). The infimum γαβ and the manifold 𝒩αβ have some properties which are similar to those of cε and 𝒩ε stated in Lemmas 2.32.6.

Lemma 3.1.

Let α2α1>0 and β1>β2>0. Then γα1β1γα2β2. Moreover, γα1β1<γα2β2 if one of the inequalities is strict.

Proof.

Let u𝒩α2β2 satisfy γα2β2=Iα2β2(u)=maxt>0Iα2β2(tu). Define

u 0 : = t 1 u with I α 1 β 1 ( u 0 ) = max t > 0 I α 1 β 1 ( t u ) .

Then we have

γ α 2 β 2 = I α 2 β 2 ( u ) I α 2 β 2 ( u 0 ) = I α 1 β 1 ( u 0 ) + 1 2 ( α 2 - α 1 ) 3 | u 0 | 2 d x + β 1 2 - β 2 2 2 3 3 K ( y ) F ( u 0 ( y ) ) K ( x ) F ( u 0 ) | x - y | μ d x d y γ α 1 β 1 .

Thus the lemma is proved. ∎

Without loss of generality, we may assume x1=0𝒱. Thus

V ( 0 ) = V min and κ : = K ( 0 ) K ( 0 ) for all | x | R .

Lemma 3.2.

lim sup ε 0 c ε γ V min κ .

Proof.

Set Vc(x):=max{c,V(x)}, Kd(x):=min{d,K(x)}, Vεc(x):=Vc(εx) and Kεd(x):=Kd(εx), where the constants c,d>0. Define the functional

I ε c d ( u ) = a 2 3 | u | 2 d x + 1 2 3 V ε c ( x ) u 2 d x + b 4 ( 3 | u | 2 d x ) 2 - 1 2 3 3 K ε d ( y ) F ( u ( y ) ) K ε d ( x ) F ( u ) | x - y | μ d x d y ,

which implies Icd(u)Iεcd(u) and γcdcεcd, where the number cεcd is the least energy of Iεcd. It follows from the definition of Vmin and Kmax that VεVmin(x)=V(εx) and KεKmax(x)=K(εx). Therefore, we get

(3.2) I ε V min K max ( u ) = I ε ( u ) ,

V ε V min ( x ) V ( 0 ) = V min and KεKmax(x)K(0)=κ uniformly on bounded sets of x as ε0.

We claim lim supε0cεVminKmaxγVlimκ. Indeed, if w is a critical point of the functional IVlimκ, then there exists tε>0 such that tεw𝒩εVminKmax, where 𝒩εVminKmax is the Nehari manifold of the functional IεVminKmax. Thus we get

c ε V min K max I ε V min K max ( t ε w ) = max t 0 I ε V min K max ( t w )

and

(3.3) I ε V min K max ( t ε w ) = I V min κ ( t ε w ) + 1 2 3 ( V ε V min - V min ) | t ε w | 2 d x + 1 2 3 3 ( κ 2 - K ε K max ( x ) K ε K max ( y ) ) F ( t ε w ( y ) ) F ( t ε w ( x ) ) | x - y | μ d x d y .

By Lemma 2.3, we may assume tεt0 as ε0. For any η>0, there exists an R>0 such that

3 B R ( 0 ) | w | 2 d x < η .

Thus, by the fact that VεVmin(x)Vmin uniformly in xBR(0), we get

(3.4) 3 ( V ε V min ( x ) - V min ) | t ε w | 2 d x = 3 ( V ε V min ( x ) - V min ) | t 0 w | 2 d x + o ( 1 ) = 3 B R ( 0 ) ( V ε V min ( x ) - V min ) | t 0 w | 2 d x + B R ( 0 ) ( V ε V min ( x ) - V min ) | t 0 w | 2 d x + o ( 1 ) C t 0 2 η + o ( 1 ) .

Therefore, we obtain

3 ( V ε V min ( x ) - V min ) | t ε w | 2 d x = o ( 1 ) .

Notice that

| 3 3 ( κ 2 - K ε K max ( x ) K ε K max ( y ) ) F ( t ε w ( y ) ) F ( t ε w ( x ) ) | x - y | μ d x d y | | 3 3 κ ( κ - K ε K max ( x ) ) F ( t ε w ( y ) ) F ( t ε w ( x ) ) | x - y | μ d x d y | + | 3 3 K ε K max ( x ) ( κ - K ε K max ( y ) ) F ( t ε w ( y ) ) F ( t ε w ( x ) ) | x - y | μ d x d y | .

Set

Q ( x ) : = 3 F ( t ε w ( y ) ) | x - y | μ d y .

We claim that there exists C>0 such that

(3.5) | Q ( x ) | < C for all x 3 .

By Lemma 2.2, we have

| Q ( x ) | = | 3 F ( t ε w ( y ) ) | x - y | μ d y | C | x - y | 1 | w ( y ) | 2 + | w ( y ) | q | x - y | μ d y + | x - y | 1 | w ( y ) | 2 + | w ( y ) | q | x - y | μ d y C | x - y | 1 | w ( y ) | 2 + | w ( y ) | q | x - y | μ d y + C .

Now we can choose t(33-μ,3) and r(33-μ,6q). By the Hölder inequality, we conclude that

| x - y | 1 | w ( y ) | 2 | x - y | μ d y ( | x - y | 1 | w ( y ) | 2 t d y ) 1 t ( | x - y | 1 1 | x - y | t μ t - 1 d y ) t - 1 t C ρ 1 ρ 2 - t μ t - 1 d ρ C ,
| x - y | 1 | w ( y ) | q | x - y | μ d y ( | x - y | 1 | w ( y ) | q r d y ) 1 r ( | x - y | 1 1 | x - y | r μ r - 1 d y ) r - 1 r C ρ 1 ρ 2 - r μ r - 1 d ρ C .

Then the claim is true.

By (3.4) and the fact that KεKmax(x)K(0)=κ uniformly on bounded sets of x as ε0, we have

3 3 κ ( κ - K ε K max ( x ) ) F ( t ε w ( y ) ) F ( t ε w ( x ) ) | x - y | μ d x d y < C 3 | κ - K ε K max ( x ) | F ( t ε w ( x ) ) d x = o ( 1 ) .

Similarly,

3 3 K ε K max ( x ) ( κ - K ε K max ( y ) ) F ( t ε w ( y ) ) F ( t ε w ( x ) ) | x - y | μ d x d y = o ( 1 ) .

From the above arguments, we get

3 3 ( κ 2 - K ε K max ( x ) K ε K max ( y ) ) F ( t ε w ( y ) ) F ( t ε w ( x ) ) | x - y | μ d x d y = o ( 1 ) .

Thus, by (3.3), we have

I ε V min K max ( t ε w ) = I V min κ ( t ε w ) + o ( 1 ) I V min κ ( t 0 w ) as ε 0 .

Then

c ε V min K max I ε V min K max ( t ε w ) I V min κ ( t 0 w ) max t 0 I V min κ ( t w ) = I V min κ ( w ) = γ V min κ .

By(3.2), we obtain cεVminKmax=cε. This completes the proof. ∎

4 Existence of Ground State Solutions

Theorem 4.1.

The minimax value cε is attained at some positive uεHε for small ε>0.

Proof.

By Lemma 2.4 and the mountain pass theorem without Palais–Smale condition (see, e.g., [37]), there exists a sequence {un}Hε such that

I ε ( u n ) c ε and I ε ( u n ) 0 as n + .

It follows from Lemma 2.5 that {un} is bounded in Hε. Up to a sequence, we may assume unuε in Hε, unuε in Lloct(3) for t[2,6), un(x)uε(x) a.e. in 3.

Next we claim that Iε(uε)=0. In fact, if uε=0, then the claim is completed. If uε0, we may assume

3 | u ε | 2 d x lim n + 3 | u n | 2 d x = A ~ 0 .

For each φHε, the weak convergence of {un} implies

( u n , φ ) ε ( u ε , φ ) ε , 3 V ( ε x ) u n φ d x 3 V ( ε x ) u ε φ and 3 u n φ d x 3 u ε φ d x .

Moreover, we deduce from Lemma 2.2 that

3 3 K ( ε y ) F ( u n ( y ) ) K ( ε x ) f ( u n ( x ) ) φ ( x ) | x - y | μ d x d y 3 3 K ( ε y ) F ( u ε ( y ) ) K ( ε x ) f ( u ε ( x ) ) φ ( x ) | x - y | μ d x d y .

By using the above equations, we obtain

o n ( 1 ) = I ε ( u n ) , φ = ( a + b 3 | u n | 2 d x ) 3 u n φ d x + 3 V ( ε x ) u n φ d x - 3 3 K ( ε y ) F ( u n ( y ) ) K ( ε x ) f ( u n ( x ) ) φ ( x ) | x - y | μ d x d y ( a + b 3 | u ε | 2 d x ) 3 u ε φ d x + 3 V ( ε x ) u ε φ d x - 3 3 K ( ε y ) F ( u ε ( y ) ) K ( ε x ) f ( u ε ( x ) ) φ ( x ) | x - y | μ d x d y .

In the case 3|uε|2dx=A~, then Iε(uε)=0. In another case 3|uε|2dx<A~, we obtain Iε(uε),φ<0. In particular, Iε(uε),uε<0. Set h1(t):=Iε(tuε),tuε for t0. Then h1(1)<0. From Lemma 2.2 and 2<q<6-μ, we have

h 1 ( t ) : = t 2 u ε ε + b t 4 ( 3 | u ε | 2 d x ) 2 - 3 3 K ( ε y ) F ( u ε ( y ) ) K ( ε x ) F ( u ε ( x ) ) φ ( x ) | x - y | μ d x d y t 2 u ε ε 2 - δ t 4 u ε ε 4 - C δ t 2 q u ε ε 2 q > 0

for t>0 small. Thus there exists t0(0,1) such that h1(t0)=Iε(t0uε),t0uε=0, that is, t0uε𝒩ε, and hence Iε(t0uε)=maxt[0,1]Iε(tuε). By Lemma 2.2, we get

c ε I ε ( t 0 u ε ) = I ε ( t 0 u ε ) - 1 4 I ε ( t 0 u ε ) , t 0 u ε = t 0 2 4 u ε ε 2 + 1 4 3 3 K ( ε y ) F ( t 0 u ε ( y ) ) K ( ε x ) ( f ( t 0 u ε ( x ) ) t 0 u ε ( x ) - 2 F ( t 0 u ε ( x ) ) ) | x - y | μ d x d y < 1 4 u ε ε 2 + 1 4 3 3 K ( ε y ) F ( u ε ( y ) ) K ( ε x ) ( f ( u ε ( x ) ) u ε ( x ) - 2 F ( u ε ( x ) ) ) | x - y | μ d x d y lim inf n + { I ε ( u n ) - 1 4 I ε ( u n ) , u n } = c ε .

This contradiction yields that the claim holds true and Iε(uε)=0. On the other hand, by Lemma 2.2 and Fatou’s lemma, we obtain

c ε I ε ( u ε ) = I ε ( u ε ) - 1 4 I ε ( u ε ) , u ε = 1 4 u ε ε 2 + 1 4 3 3 K ( ε y ) F ( u ε ( y ) ) K ( ε x ) ( f ( u ε ( x ) ) u ε ( x ) - 2 F ( u ε ( x ) ) ) | x - y | μ d x d y lim inf n + { 1 4 u n ε 2 + 1 4 3 3 K ( ε y ) F ( u n ( y ) ) K ( ε x ) ( f ( u n ( x ) ) u n ( x ) - 2 F ( u n ( x ) ) ) | x - y | μ d x d y } = lim inf n + { I ε ( u n ) - 1 4 I ε ( u n ) , u n } = c ε ,

which implies Iε(uε)=cε.

Lastly, we show that uε0 for small ε>0. Argue by contradiction that there exists a sequence εj0 such that uεj=0. Then un0 in Hε, un0 in Lloct(3) for t[2,6) and un(x)0 a.e. in 3. By (A1), we may choose β(Vmin,V). Let tn>0 satisfy tnun𝒩εjβκ. By Lemma 2.3, we may assume tnt0 as n+. The set Oε:={x3:Vε(x)<β} and O¯ε:={x3:Kε(s)κ} are both bounded by (A1). From the fact that Iεj(tnun)Iεj(un), we have

c ε j β κ I ε j β κ ( t n u n ) = I ε j ( t n u n ) + 1 2 3 ( V ε j β ( x ) - V ( ε j x ) ) | t n u n | 2 d x + 1 2 3 3 ( K ( ε j y ) K ( ε j x ) - K ε j κ ( y ) K ε j κ ( x ) ) F ( t n u n ( y ) ) F ( t n u n ( x ) ) | x - y | μ d x d y .

It is easy to check that

3 ( V ε j β ( x ) - V ( ε j x ) ) | t n u n | 2 d x = O ε j ( β - V ( ε j x ) ) | t n u n | 2 d x = o ( 1 ) .

One the other hand, we have

3 3 ( K ( ε j y ) K ( ε j x ) - K ε j κ ( y ) K ε j κ ( x ) ) F ( t n u n ( y ) ) F ( t n u n ( x ) ) | x - y | μ d x d y = 3 3 K ( ε j y ) F ( t n u n ( y ) ) ( K ( ε j x ) - K ε j κ ( x ) ) F ( t n u n ( x ) ) | x - y | μ d x d y + 3 3 K ε j κ ( y ) F ( t n u n ( y ) ) ( K ( ε j x ) - K ε j κ ( x ) ) F ( t n u n ( x ) ) | x - y | μ d x d y : = Π 1 + Π 2 .

Define

G ¯ n : = 3 K ( ε j y ) F ( t n u n ( y ) ) | x - y | μ d y .

By the boundedness of K, {tn} and {un}, similar to (3.5), there is a constant C>0 such that

| G ¯ n | C .

Therefore,

| Π 1 | C 3 | K ( ε j x ) - K ε j κ ( x ) | F ( t n u n ( x ) ) d x C O ¯ ε | K ( ε j x ) - K ε j κ ( x ) | F ( t n u n ( x ) ) d x = o ( 1 ) .

Similarly, Π2=o(1). From the above equalities, we have cεjβκIεj(tnun)+o(1)Iεj(un)+o(1)cεj. It follows from γβκcεjβκ that γβκcεj. By using Lemma 3.2, we have

γ β κ γ V min κ ,

which is impossible due to γVminκ<γβκ. Therefore, cε is attained at some uε0 for sufficiently small ε>0.

Moreover, by using uε-:=min{uε,0} as a test function in (2.1), we obtain

0 = I ε ( u ) , u ε - = ( a + b 3 | u ε | 2 d x ) 3 u ε u ε - d x + 3 V ( ε x ) u ε u ε - d x a 3 | u ε - | 2 d x + 3 V ( ε x ) | u ε - | 2 d x 0 ,

which yields uε-=0 and uε0. The strong maximum principle and standard arguments (see, e.g., [32, 33]) imply that uε(x) is positive for all x3. Therefore, uε is a positive ground state solution of problem (2.1). ∎

5 Concentration and Convergence of Ground State Solutions

The main objection of this section is to prove the following theorem.

Theorem 5.1.

Assume that uε is a solution of equation (2.1) given by Theorem 4.1. Then uε has a global maximum point yε in R3 such that, up to a subsequence, εyεx0 as ε0, limε0dist(εyε,H1)=0 and vε(x):=uε(x+yε) converges in H1(R3) to a positive ground state solution of

{ - ( a + b 3 | u | 2 d x ) Δ u + V ( x 0 ) u = K 2 ( x 0 ) ( 3 F ( u ( y ) ) | x - y | μ d y ) f ( u ) , u H 1 ( 3 ) .

In particular, if VK, then limε0dist(εyε,VK)=0 and, up to a subsequence, vε converges in H1(R3) to a positive ground state solution of

{ - ( a + b 3 | u | 2 d x ) Δ u + V min u = K max 2 ( 3 F ( u ( y ) ) | x - y | μ d y ) f ( u ) , u H 1 ( 3 ) .

5.1 Concentration Behavior of Ground State Solutions

In this subsection, we give some preliminary lemmas which are useful to prove Theorem 5.1.

Lemma 5.1.

There exist ε*>0, a family {yε}R3 and R~,σ>0 such that

B R ~ ( y ε ) u ε 2 d x σ for all ε ( 0 , ε * ) .

Proof.

Arguing by contradiction, if there exists a sequence εj0 as j+ such that

lim j + sup y 3 B R ( y ) u ε j 2 d x = 0 for all R > 0 .

So, by Lemma 2.1, we have uεj0 in Lt(3) for 2<t<6. By Lemma 2.2, we see that

3 3 K ( ε j y ) F ( u ε j ( y ) ) K ( ε j x ) F ( u ε j ( x ) ) | x - y | μ d x d y 0 as j +

and

0 u ε j ε j 2 + b 4 ( 3 | u ε j | 2 d x ) 2 0 as j + .

Therefore, Iεj(uεj)0 as j+, which contradicts Iεj(uεj)cεj>0. ∎

Let vε(x):=uε(x+yε), Vε(x):=V(ε(x+yε)) and Kε(x):=K(ε(x+yε)). Then vε satisfies

(5.1) - ( ε 2 a + ε b 3 | v ε | 2 d x ) Δ v ε + V ε ( x ) v ε = ( 3 K ε ( y ) F ( v ε ( y ) ) | x - y | μ d y ) K ε ( x ) f ( v ε ) .

The functional associated with problem (5.1) reduces to

J ε ( v ε ) : = a 2 3 | v ε | 2 d x + 1 2 3 V ε ( x ) v ε 2 d x + b 4 ( 3 | v ε | 2 d x ) 2 - 1 2 3 3 K ε ( y ) F ( v ε ( y ) ) K ε ( x ) F ( v ε ( x ) ) | x - y | μ d x d y = a 2 3 | u ε | 2 d x + 1 2 3 V ( ε x ) u ε 2 d x + b 4 ( 3 | u ε | 2 d x ) 2 - 1 2 3 3 K ( ε y ) F ( u ε ( y ) ) K ( ε x ) F ( u ε ( x ) ) | x - y | μ d x d y = I ε ( u ε ) = c ε .

By Lemma 5.1, we may assume vεu0 in Hε with u0, vεu in Lloct(3) for t[2,6), vε(x)u(x) a.e. in 3. By V,KL(3), without loss of generality, we can assume V(εyε)V0 and K(εyε)K0 as ε0.

Lemma 5.2.

u is a positive ground state solution of the problem

(5.2) - ( a + b 3 | u | 2 d x ) Δ u + V 0 u = K 0 2 ( 3 F ( u ( y ) ) | x - y | μ d y ) f ( u ) .

Proof.

Since V,K are uniformly continuous, we know that

| V ( ε ( x + y ε ) ) - V ( ε y ε ) | 0 and | K ( ε ( x + y ε ) ) - K ( ε y ε ) | 0

as ε0 uniformly on bounded sets of x3. Then we have

| V ( ε ( x + y ε ) ) - V 0 | | V ( ε ( x + y ε ) ) - V ( ε y ε ) | + | V ( ε y ε ) - V 0 | 0 ,
| K ( ε ( x + y ε ) ) - K 0 | | K ( ε ( x + y ε ) ) - K ( ε y ε ) | + | K ( ε y ε ) - K 0 | 0

as ε0 uniformly on bounded sets of x3. Furthermore, V(ε(x+yε))V0 and K(ε(x+yε))K0 as ε0 uniformly on bounded sets of x3. Therefore, by (5.1), for any φC0(3),

0 = lim ε 0 3 ( - ( a + b 3 | v ε | 2 d x ) v ε + V ( ε ( x + y ε ) ) v ε - ( 3 K ( ε ( y + y ε ) ) F ( v ε ( y ) ) | x - y | μ d y ) K ( ε ( x + y ε ) ) f ( v ε ( x ) ) ) φ d x = lim ε 0 3 ( - ( a + b 3 | u | 2 d x ) Δ u + V 0 u - K 0 2 ( 3 F ( u ( y ) ) | x - y | μ d y ) f ( u ( x ) ) ) φ d x ,

which yields that u is a solution of (5.2). Then the energy functional associated with (5.2) is

I V 0 K 0 ( u ) : = a 2 3 | u | 2 d x + V 0 2 3 u 2 d x + b 4 ( 3 | u | 2 d x ) 2 - K 0 2 2 3 3 F ( u ( y ) ) F ( u ( x ) ) | x - y | μ d x d y = I V 0 K 0 ( u ) - 1 4 I V 0 K 0 ( u ) , u = a 4 3 | u | 2 d x + V 0 4 3 u 2 d x + K 0 2 4 3 3 F ( u ( y ) ) ( f ( u ( x ) ) u ( x ) - 2 F ( u ( x ) ) ) | x - y | μ d x d y γ V 0 K 0 .

Similar to Lemma 3.2, we obtain

γ V 0 K 0 a 4 3 | u | 2 d x + V 0 4 3 u 2 d x + K 0 2 4 3 3 F ( u ( y ) ) ( f ( u ( x ) ) u ( x ) - 2 F ( u ( x ) ) ) | x - y | μ d x d y lim inf ε 0 ( a 4 3 | v ε | 2 d x + 1 4 3 V ε ( x ) v ε 2 d x + 1 4 3 3 K ε ( y ) F ( v ε ( y ) ) K ε ( x ) ( f ( v ε ( x ) ) v ε ( x ) - 2 F ( v ε ( x ) ) ) | x - y | μ d x d y ) = lim inf ε 0 J ε ( v ε ) lim inf ε 0 I ε ( u ε ) γ V 0 K 0 .

So

(5.3) lim ε 0 = J ε ( v ε ) = lim ε 0 c ε = I V 0 K 0 ( u ) = γ V 0 K 0 .

Therefore, u is a ground state solution of problem (5.2). By using the same arguments as in Theorem 4.1, u is positive. ∎

Lemma 5.3.

The sequence {εyε} is bounded.

Proof.

In fact, suppose by contradiction that there exists a subsequence still denoted by {εyε} such that |εyε|. Since V,KL(3), we may assume V(εyε)V0 and K(εyε)K0 as ε0. Recalling that V(0)=Vmin and κ=K(0)K(x) for all |x|R, we get V0>Vmin and K0κ. Thus γV0K0>γVminK0. However, by (5.3) and Lemma 3.2, cεγV0K0γVminK0, which is absurd, and the conclusion follows. ∎

Up to a subsequence, we may assume εyεx0 as ε0, so V0=V(x0) and K0=K(x0).

Lemma 5.4.

lim ε 0 dist ( ε y ε , 1 ) = 0 .

Proof.

It is enough to prove that x01. Arguing by contradiction, suppose that x01. Then, by (A1) and Lemma 3.1, it is easy to see that γV(x0)K(x0)>γVminK0. Thus, by Lemma 3.2, we get

lim ε 0 c ε = γ V ( x 0 ) K ( x 0 ) > γ V min κ = lim ε 0 c ε ,

which yields a contradiction. ∎

Lemma 5.5.

v ε u in H1(R3).

Proof.

Since u solves equation (5.2), we get

1 4 3 | u | 2 d x lim inf ε 0 1 4 3 | v ε | 2 d x lim sup ε 0 1 4 3 | v ε | 2 d x + lim inf ε 0 1 4 3 V ε ( x ) v ε 2 d x - V 0 4 3 u 2 d x + lim inf ε 0 1 4 3 3 K ε ( y ) F ( v ε ( y ) ) K ε ( x ) ( f ( v ε ( x ) ) v ε ( x ) - 2 F ( v ε ( x ) ) ) | x - y | μ d x d y - K 0 2 4 3 3 F ( u ( y ) ) ( f ( u ( x ) ) u ( x ) - 2 F ( u ( x ) ) ) | x - y | μ d x d y lim sup ε 0 1 4 [ 3 | v ε | 2 d x + 3 V ε ( x ) v ε 2 d x + 3 3 K ε ( y ) F ( v ε ( y ) ) K ε ( x ) ( f ( v ε ( x ) ) v ε ( x ) - 2 F ( v ε ( x ) ) ) | x - y | μ d x d y ] - V 0 4 3 u 2 d x - K 0 2 4 3 3 F ( u ( y ) ) ( f ( u ( x ) ) u ( x ) - 2 F ( u ( x ) ) ) | x - y | μ d x d y = 1 4 3 | u | 2 d x .

Thus

lim ε 0 3 | v ε | 2 d x = 3 | u | 2 d x and lim ε 0 3 V ε ( x ) v ε 2 d x = V 0 3 u 2 d x .

Therefore,

lim ε 0 ( 3 | v ε | 2 d x + 3 V ε ( x ) v ε 2 d x ) = 3 | u | 2 d x + V 0 3 u 2 d x .

Combining with vεu in H1(3), vεu in (3)1, and the conclusion follows. ∎

5.2 Concentration Behavior of Positive Ground State Solutions

The following uniform L-estimate plays a crucial role in the study of behavior of the maximum points of the solutions (see, e.g., [26, 10]).

Lemma 5.6.

Let vεn be a solution of

(5.4) { - ( a + b 3 | v ε n | 2 d x ) Δ v ε n + V n ( x ) v ε n = ( 3 K n ( y ) F ( v ε n ( y ) ) | x - y | μ d y ) K n ( x ) f ( v ε n ) , u H 1 ( 3 ) ,

where Vn(x):=V(εnx+εnyεn), Kn(x):=K(εnx+εnyεn), yεn is given in Lemma 5.1. Then vεnL(R3), and there exists C>0 such that

v ε n L ( 3 ) C for all n .

Furthermore, lim|x|+vεn(x)=0 uniformly in nN.

For simplicity, we denote vεn and yεn by vn and yn, respectively.

Proof of Theorem 5.1.

First we claim that there exists δ>0 such that vnL(3)δ for all n.

In fact, suppose to the contrary that vnL(3)0. Choosing ε=Vmin2, it follows from (f1) and (f4) that there exists n0 such that, for nn0,

a 3 | v n | 2 d x + 3 V n ( x ) v n 2 d x 3 3 K n ( y ) F ( v n ( y ) ) | x - y | μ K n ( x ) f ( v n ( x ) ) v n ( x ) d x d y C 3 f ( v n ( x ) ) v n ( x ) d x C 3 f ( v n ) v n v n 2 d x C 3 f ( v n L ( 3 ) ) v n L ( 3 ) v n 2 d x < V min 2 3 v n 2 d x ,

which implies vn=0 for nn0. This is impossible since vnu in H1(3) and u0. Then the claim is true.

Using the arguments of [34], there is σ(0,1) such that uCloc1,σ(3). By Lemma 5.6 and the claim above, un possesses a global maximum point pnBR(0) for some R>0. So the global maximum point of uεn is given by zn=pn+yn. Set ψn(x):=uεn(x+pn+yn), where uεn(x)=vn(x+yn). We deduce from the fact that {pn}BR0(0) is bounded that {εn(pn+yn)} is bounded and εn(pn+yn)x01. By the boundedness of {uεn}, {ψn} is bounded in H1(3). Up to a subsequence, we may assume ψnψ in H1(3) and ψnψ in Llocq(3) for all q[1,6). By Lemma 5.1, we obtain

B R ~ + R 0 ( 0 ) ψ n 2 ( x ) d x { | x + P n | < R ~ } ψ n 2 ( x ) d x = B R ~ ( y n ) u ε n 2 ( x ) d x σ ,

which implies ψ0. Similar to the discussion above, we obtain that ψ solves equation (5.2) with ψnψ in H1(3). Thus ψn has the same properties as vn, and we may assume that yn is a global maximum point of uεn. Therefore, Lemmas 5.15.5 yield that Theorem 5.1 holds. ∎

5.3 Decay Estimates of Positive Ground State Solutions

Lemma 5.7.

There exist constants C,τ>0 such that vnCe-τ|x| for all xR3.

Proof.

Since vn solves (5.4) and vn(x)0 as |x| uniformly in n, there exists M>0 such that vnV0M uniformly in n. Therefore, for some large R1>0, for x3BR1(0), we get

(5.5) - Δ v n + V 0 2 ( a + 2 b M ) v n = ( I α F ( v n ) ) f ( v n ) - V n ( x ) v n a + b 3 | v n | 2 d x + V 0 2 ( a + 2 b M ) v n ( I α F ( v n ) ) f ( v n ) - V n ( x ) v n + V 0 2 v n a + b 3 | v n | 2 d x C f ( v n ) - V 0 2 v n a + b 3 | v n | 2 d x C ( δ v n + C δ v n q - 1 ) - V 0 2 v n a + b 3 | v n | 2 d x C ( δ + C δ v n q - 2 ) - V 0 2 a + b 3 | v n | 2 d x v n 0 .

For some C>0, fix (x)=Ce-τ|x|, where τ2V02(a+2M), and let vnCe-τ|x| for |x|=R1. Then we get

(5.6) Δ τ 2 < V 0 2 ( a + 2 b M ) .

Let v~n(x)=(x)-vn(x). By (5.5) and (5.6), we obtain

{ Δ v ~ n ( x ) + V 0 2 ( a + 2 b M ) v ~ n ( x ) > 0 for | x | R 1 , v ~ n 0 for | x | = R 1 , lim | x | + v ~ n = 0 .

The maximum principle implies v~n(x)0 for all |x|R1, and we conclude that vnCe-τ|x| for all |x|R1. Therefore, the proof is completed. ∎

Proof of Theorem 1.1.

Now setting wn(x):=un(xεn), we can easily see that wn(x) is a positive ground state solution of (1.1) and xεn:=εnyn is a maximum point of wn. Moreover, we have

w n ( x ) = u n ( x ε n ) = v n ( x ε n - y n ) C e - τ | x ε n - y n | .

Therefore, the proof of Theorem 1.1 is completed. ∎


Communicated by Paul H. Rabinowitz


Award Identifier / Grant number: 201806370022

Award Identifier / Grant number: CX2018B052

Award Identifier / Grant number: 11571370

Funding statement: This work was supported by China Scholarship Council (201806370022), Hunan Provincial Innovation Foundation for Postgraduate (CX2018B052) and National Natural Science Foundation of China (11571370).

Acknowledgements

The authors would like to thank the anonymous referee for his or her careful readings of the paper and many helpful comments. The research was done when G. Gu visited Department of Mathematics, University of Texas at San Antonio under the support of China Scholarship Council, and the first author thanks professor Changfeng Gui for his invitation and Department of Mathematics, University of Texas at San Antonio for their support and kind hospitality.

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Received: 2019-03-10
Revised: 2019-04-02
Accepted: 2019-04-04
Published Online: 2019-05-08
Published in Print: 2019-11-01

© 2019 Walter de Gruyter GmbH, Berlin/Boston

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

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