GROUND STATES OF NONLOCAL SCALAR FIELD EQUATIONS WITH TRUDINGER-MOSER CRITICAL NONLINEARITY ˜ MARCOS DO O, ´ OL´IMPIO H. MIYAGAKI, AND MARCO SQUASSINA JOAO Abstract. We investigate the existence of ground state solutions for a class of nonlinear scalar field equations defined on whole real line, involving a fractional Laplacian and nonlinearities with Trudinger-Moser critical growth. We handle the lack of compactness of the associated energy functional due to the unboundedness of the domain and the presence of a limiting case embedding.
1. Introduction and main result The goal of this paper is to investigate the existence of ground state solutions u ∈ H 1/2 (R) for the following class of nonlinear scalar field equations (−∆)1/2 u + u = f (u)
(1.1)
in R,
where f : R → R is a smooth nonlinearity in the critical growth range. Precisely, we focus here on the case when f has the maximal growth which allows to study problem (1.1) variationally in the Sobolev space u ∈ H 1/2 (R), see Section 2. We are motivated by the following Trudinger-Moser type inequality due to Ozawa [28]. Theorem A. There exists 0 < ω ≤ π such that, for all α ∈ (0, ω), there exists Hα > 0 with Z 2 (eαu − 1) dx ≤ Hα kuk2L2 , (1.2) for all u ∈
H 1/2 (R)
with
R 1/4 k(−∆) uk2L2
≤ 1.
From inequality (1.2) we have naturally associated notions of subcriticality and criticality for this class of problems. Precisely, we say that f : R → R has subcritical growth at ±∞ if f (s) lim sup αs2 = 0, for all α > 0, −1 s→±∞ e and has α0 -critical growth at ±∞ if there exists ω ∈ (0, π] and α0 ∈ (0, ω) such that f (s) = 0, for all α > α0 , 2 s→±∞ eαs − 1 f (s) = ±∞, for all α < α0 . lim sup αs2 −1 s→±∞ e For instance let f be given by lim sup
f (s) = s3 eα0 |s|
ν
for all s ∈ R.
2000 Mathematics Subject Classification. 35J60, 35B09, 35B33, 35R11. Key words and phrases. Trudinger-Moser inequality, fractional Laplacian, ground state solutions. ´ was supported by The present research was partially supported by INCTmat/MCT/Brazil. Jo˜ ao Marcos do O CNPq, CAPES/Brazil, Ol´ımpio H. Miyagaki was partially supported by CNPq/Brazil and CAPES/Brazil (Proc 2531/14-3). The paper was completed while the second author was visiting the Dept of Math of Rutgers University, whose hospitality he gratefully acknowledges. 1
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´ O.H. MIYAGAKI, AND M. SQUASSINA J.M. DO O,
If ν < 2, f has subcritical growth, and while if ν = 2 and α0 ∈ (0, ω], f has critical growth. By a ground state solution to problem (1.1) we mean a nontrivial weak solution of (1.1) with the least possible energy. The following assumptions on f will be needed throughout the paper: (f1): f : R → R is C 1 , odd, convex function on R+ , and f (s) = 0. s→0 s (f2): s 7→ s−1 f (s) is an increasing function for s > 0. (f3): there are q > 2 and Cq > 0 with lim
F (s) ≥ Cq |s|q ,
for all s ∈ R.
(AR): there exists ϑ > 2 such that Z ϑF (s) ≤ sf (s),
for all s ∈ R,
s
f (σ)dσ.
F (s) = 0
The main result of the paper is the following Theorem 1.1. Let f (s) and f 0 (s)s have α0 -critical growth and satisfy (f1)-(f3) and (AR). Then problem (1.1) admits a ground state solution u ∈ H 1/2 (R) provided Cq in (f3) is large enough. The nonlinearity 2
f (s) = λs|s|q−2 + |s|q−2 seα0 s , q > 2 and s ∈ R, satisfies all the hypotheses of Theorem 1.1 provided that λ is sufficiently large. More examples of nonlinearities which satisfy the above assumptions can be found in [19]. In R2 one can use radial estimates, then apply, for instance, the Strauss lemma [32] to recover some compactness results. In R analogous compactness results fail, but in [21], the authors used the concentration compactness principle by Lions [34] for problems with polynomial nonlinearities. In this paper, we use the minimization technique over the Nehari manifold in order to get ground state solutions. We adopt some arguments from [4] combined with those used in [10, 23]. 1.0.1. Quick overview of the literature. In Coti Zelati and Rabinowitz [12] investigated (1.3)
− ∆u + V (x)u = f (x, u)
in RN ,
u ∈ H 1 (RN ),
RN
u > 0,
when V is a strictly positive potential and f : × R → R is a periodic function in x ∈ RN and f has Sobolev subcritical growth, that is, f behaves at infinity like sp with 2 < p < 2∗ − 1, where 2∗ = 2N/(N − 2) is the critical Sobolev exponent, N ≥ 3. This was extended or complemented in several ways, see e.g. [34]. For N = 2 formally 2∗ ; +∞, but H 1 (RN ) 6,→ L∞ (RN ). Instead, the Trudinger-Moser inequality [27, 33] states that H 1 is continuously embedded into an Orlicz 2 space defined by the Young function φ(t) = eαt − 1. In [1, 14, 15, 25], with the help of TrudingerMoser embedding, problems in a bounded domain were investigated, when the nonlinear term 2 f behaves at infinity like eαs for some α > 0. We refer the reader to [13] for a recently survey on this subject. In [11] the Trudinger-Moser inequality was extended to the whole R2 and the authors gave some applications to study equations like (1.3) when the nonlinear term has critical growth of Trudinger-Moser type. For further results and applications, we would like to mention also [2, 3, 17, 29] and references therein. When the potential V is a positive constant and f (x, s) = f (s) for (x, s) ∈ RN × R, that is the autonomous case, the existence of ground states for subcritical nonlinearities was established in [6] for N ≥ 3 and [7] for N = 2 respectively, while in [3] the critical case for N ≥ 3 and N = 2 was treated. For fractional problem of the form (1.4)
(−∆)s u + V (x)u = f (u)
in RN ,
NONLOCAL PROBLEMS WITH TRUDINGER-MOSER NONLINEARITY
3
with N > 2s and s ∈ (0, 1), we refer to [10, 20] where positive ground states were obtained in subcritical situations. For instance, [10] extends the results in [6] to the fractional Laplacian. In [20] is obtained regularity and qualitative properties of the ground state solution, while in [31] a ground state solution is obtained for coercive potential. For fractional problems in bounded domains of RN with N > 2s involving critical nonlinearities we cite [5, 9, 22, 30] and [18] for the whole space with vanishing potentials. In [21] the authors investigated properties of the ground state solutions of (−∆)s u + u = up in R. Recently, in [23], nonlocal problems defined in bounded intervals of the real line involving the square root of the Laplacian and exponential nonlinearities were investigated, using a version of the Trudinger-Moser inequality due to Ozawa [28]. As it was remarked in [23] the nonlinear problem involving exponential growth with fractional diffusion (−∆)s requires s = 1/2 and N = 1. In [19] some nonlocal problems in R with vanishing potential, thus providing compactifying effects, are considered. 2. Preliminary stuff We recall that o (u(x) − u(y))2 dxdy < ∞ , |x − y|2
Z n H 1/2 (R) = u ∈ L2 (R) : R2
endowed with the norm kuk =
kuk2L2
Z + R2
1/2 (u(x) − u(y))2 dxdy . |x − y|2
The square root of the Laplacian, (−∆)1/2 , of a smooth function u : R → R is defined by F((−∆)1/2 u)(ξ) = |ξ|F(u)(ξ), where F denotes the Fourier transform, that is, 1 F(φ)(ξ) = √ 2π
Z
e −iξ·x φ(x) dx,
R
for functions φ in the Schwartz class. Also (−∆)1/2 u can be equivalently represented [16] as Z u(x + y) + u(x − y) − 2u(x) 1 1/2 dy. (−∆) u = − 2π R |y|2 Also, in light of [16, Propostion 3.6], we have Z (u(x) − u(y))2 1 1/4 2 (2.1) k(−∆) ukL2 := dxdy, 2π R2 |x − y|2
for all u ∈ H 1/2 (R),
and, sometimes, we identify these two quantities by omitting the normalization constant 1/2π. From [26, (iii) of Theorem 8.5] we also know that, for any m ≥ 2, there exists Cm > 0 such that (2.2)
for all u ∈ H 1/2 (R).
kukLm ≤ Cm kuk,
Proposition 2.1. The integral Z (2.3) R
is finite for any positive α and u ∈
2
(eαu − 1) dx
H 1/2 (R).
´ O.H. MIYAGAKI, AND M. SQUASSINA J.M. DO O,
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Proof. Let α0 ∈ (0, ω) and consider the convex function defined by 2
eα0 t − 1 , t ∈ R, Hα0 where Hα0 > 0 is defined as in Theorem A. We introduce the Orlicz norm induced by φ by setting Z n o u φ kukφ := inf γ > 0 : dx ≤ 1 , γ R and the corresponding Orlicz space Lφ∗ (0, 1), see the monograph by Krasnosel’ski˘ı & Ruticki˘ı [24, Chapter II, in particular p.78-81] for properties of this space. We claim that kvkφ ≤ kvk, for all v ∈ H 1/2 (R). Let v ∈ H 1/2 (R) \ {0} and set w = kvk−1 v, so that by formula (2.1) we conclude Z (v(x) − v(y))2 1/2 1 1 1 ≤ (2π)− 2 < 1. dxdy (2.4) k(−∆) 4 wkL2 = 1 2 |x − y| (2π) 2 kvk R2 φ(t) =
Therefore, in light of Theorem A, we have Z α0 w 2 Z e v −1 dx = φ dx ≤ kwk2L2 ≤ 1, kvk Hα0 R R which proves the claim by the very definition of k · kφ . Fix now an arbitrary function u ∈ H 1/2 (R). Hence, there exists a sequence (ψn ) in Cc∞ (R) such that ψn → u in H 1/2 (R), as n → ∞. By the claim this yields kψn −ukφ → 0, as n → ∞. Fix now n = n0 sufficiently large that kψn0 −ukφ < 1/2. Then we have, in light of [24, Theorem 9.15, p.79], that Z φ(2u − 2ψn0 )dx ≤ k2u − 2ψn0 kφ < 1. R
Finally, writing u = 12 (2u − 2ψn0 ) + 12 (2ψn0 ), and since Z Z Z 2 2 1 1 4α0 ψn 0 φ(2ψn0 )dx = (e (e4α0 ψn0 − 1)dx < ∞, − 1)dx = H H α0 R α0 supt(ψn0 ) R R the convexity of φ yields R φ(u)dx < ∞. Hence, the assertion follows by the arbitrariness of u. A different proof can be given writing (in the above notations) Z Z Z 2 2 2 2 (eαu − 1) dx = (eαψn − 1) dx + (eαu − eαψn ) dx, R
R
R
2 2 |eαu −eαψn |
2
2
estimating the right-hand side by ≤ 2α(|ψn −u|+|ψn |)e2α|ψn −u| e2α|ψn | |ψn −u|, using H¨older inequality, the smallness of kψn − uk and Theorem A to conclude, for n large enough. Define the functional J : H 1/2 (R) → R associated with problem (1.1), given by Z Z 1 1/4 2 2 (|(−∆) u| + u ) dx − F (u) dx. J(u) = 2 R R Under our assumptions on f , by Proposition 2.1 we can easily see that J is well defined. Also, it is standard to prove that J is a C 1 functional and Z Z Z 0 1/4 1/4 J (u)v = (−∆) u(−∆) v dx + uv dx − f (u)v dx, ∀u, v ∈ H 1/2 (R). R
R
R
Thus, the critical points of J are precisely the solutions of (1.1), namely u ∈ H 1/2 (R) with Z Z Z 1/4 1/4 (−∆) u(−∆) v dx + uv dx = f (u)v dx, ∀v ∈ H 1/2 (R), R
is a (weak) solution to (1.1).
R
R
NONLOCAL PROBLEMS WITH TRUDINGER-MOSER NONLINEARITY
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Lemma 2.2. Let u ∈ H 1/2 (R) and ρ0 > 0 be such that kuk ≤ ρ0 . Then Z 2 (eαu − 1) dx ≤ Λ(α, ρ0 ), for every 0 < αρ20 < ω; R
Proof. Let 0 < Z
αρ20 2
eαu
R
< ω. Then, by Theorem A, we have Z 2 u kuk2L2 αρ20 kuk e − 1 dx ≤ ≤ Hαρ20 := Λ(α, ρ0 ), − 1 dx ≤ Hαρ20 kuk2 R
since k(−∆)1/4 ukuk−1 k2L2 < 1, see inequality (2.4).
Remark 2.3. From assumptions (f1)-(f2) and (AR) we see that, for all s ∈ R \ {0}, (2.5)
s2 f 0 (s) − sf (s) > 0,
(2.6)
f 0 (s) > 0,
(2.7)
H(s) := sf (s) − 2F (s) > 0,
(2.8)
H is even, and increasing on R+ , H(s) > H(λs),
(2.9)
for all λ ∈ (0, 1).
Suppose that u 6= 0 is a critical point of J, that is, J 0 (u) = 0, then necessarily u belongs to n o N := u ∈ H 1/2 (R) \ {0} : J 0 (u)u = 0 . So N is a natural constraint for the problem of finding nontrivial critical points of J. Lemma 2.4. Under assumptions (f1)-(f3) and (AR), N satisfies the following properties: (a) N is a manifold and N 6= ∅. (b) For u ∈ H 1/2 (R) \ {0} with J 0 (u)u < 0, there is a unique λ(u) ∈ (0, 1) with λu ∈ N . (c) There exists ρ > 0 such that kuk ≥ ρ for any u ∈ N . (d) If u ∈ N is a constrained critical point of J|N , then J 0 (u) = 0 and u solves (1.1). (e) m = inf u∈N J(u) > 0. Proof. Consider the C 1 -functional Φ : H 1/2 (R) \ {0} → R defined by Z 0 2 Φ(u) = J (u)u = kuk − f (u)u dx. R
Note that N =
Φ−1 (0)
and
Φ0 (u)u
< 0, if u ∈ N . Indeed, if u ∈ N , then Z 0 Φ (u)u = f (u)u − f 0 (u)u2 dx < 0, R
where we have used (2.5). Then c = 0 is regular value of Φ and consequently N = Φ−1 (0) is a C 1 -manifold, proving (a). Now we prove N 6= ∅ and that (b) holds. Fix u ∈ H 1/2 (R) \ {0} and consider the function Ψ : R+ → R, Z t2 2 F (tu) dx. Ψ(t) = kuk − 2 R Then Ψ0 (t) = 0 if and only if tu ∈ N , in which case it holds Z f (tu) (2.10) kuk2 = u dx. t R In light of (2.5) the function on the right-hand side of (2.10) is increasing. Whence, it follows that a critical point of Ψ, if it exists, it is unique. Now, there exist δ > 0 and R > 0 such that Ψ(t) > 0
if t ∈ (0, δ)
and
Ψ(t) < 0
if t ∈ (R, ∞).
´ O.H. MIYAGAKI, AND M. SQUASSINA J.M. DO O,
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In fact, by virtue of (f3), there exist C, C 0 > 0 such that Z t2 2 Ψ(t) = kuk − F (tu) dx ≤ Ct2 − C 0 tq < 0, 2 R provided that t > 0 is chosen large enough. Using (f1) and the fact that f has α0 -Trudinger-Moser critical growth at +∞, for some α ∈ (α0 , ω) and for any ε > 0, there exists Cε > 0 such that 2
F (s) ≤ ε[s2 + s4 (eαs − 1)] + Cε s4 , Then, for any u ∈
H 1/2 (R)
\ {0},
t2 Ψ(t) ≥ kuk2 − εt2 kuk2L2 − Cε t4 kuk4L4 − εt4 2 For 0 < t < τ
0 such that 1/2 Z 2 2 4 α(tu)2 4 e2ατ u − 1 ≤ C. u (e − 1) ≤ kukL8 R
R
Then for some
s ∈ R.
B, B 0
> 0, we have Ψ(t) ≥ Bt2 − B 0 t4 > 0,
for t > 0 small enough.
Thus, we conclude that there exists a unique maximum t0 = t0 (u) > 0 such that t0 u ∈ N , and consequently N is a nonempty set. Given u ∈ H 1/2 (R) \ {0} with J 0 (u)u < 0, we have Z 0 2 Ψ (1) = kuk − f (u)u dx = J 0 (u)u < 0, R
which implies t0 < 1. Let us prove (c). Let α ∈ (α0 , ω) and ρ0 > 0 with αρ20 < ω. By the growth conditions on f , there exists r > 1 so close to 1 that rαρ20 < ω, ` > 2 and C > 0 with 1 2 f (s)s ≤ s2 + C(erαs − 1)1/r |s|` , for all s ∈ R. 4 Let now u ∈ N with kuk ≤ ρ ≤ ρ0 . Then, by Lemma 2.2 and (2.2), we have for u ∈ N Z 1/r ` 1 2 erαu − 1 |u| dx 0 = Φ(u) ≥ kuk2 − kuk2L2 − C 4 R Z Z 1/r 3 0 0 2 rαu2 e − 1 dx (2.11) |u|r ` dx)1/r ≥ kuk − C 4 R R 3 ≥ kuk2 − Ckuk` , 4 which yields 3 1/(`−2) ≤ kuk ≤ ρ, 0 < ρˆ := 4C a contradiction if ρ < min{ˆ ρ, ρ0 }. Then u ∈ N implies kuk ≥ min{ˆ ρ, ρ0 }, proving (c). Concerning 0 0 (d), if u ∈ N is a minimizer, then J (u) = λΦ (u) for some λ ∈ R. Testing with u and recalling the previous conclusions yields λ = 0, hence the assertion. Finally, assertion (e) follows by condition (AR) and (c), since u ∈ N implies J(u) ≥ (1/2 − 1/ϑ)kuk2 ≥ (1/2 − 1/ϑ)ρ2 > 0. Lemma 2.5. Let (un ) ⊂ N be a minimizing sequence for J on N , that is, (2.12)
J 0 (un )un = 0
and
J(un ) → m := inf J(u) u∈N
as n → ∞,
then the following facts hold (a) (un ) is bounded in H 1/2 (R). Thus, up to a subsequence, un * u weakly in H 1/2 (R). (b) lim supn kun k < ρ0 , for some ρ0 > 0 sufficiently small.
NONLOCAL PROBLEMS WITH TRUDINGER-MOSER NONLINEARITY
7
(c) (un ) does not converge strongly to zero in Lσ (R), for some σ > 2. Proof. Let (un ) ⊂ H 1/2 (R) satisfying (2.12). Using (AR) condition, we have for ϑ > 2, Z 1 1 kun k2 1 (2.13) m + o(1) = J(un ) ≥ f (un )un dx = − − kun k2 , 2 ϑ R 2 ϑ which implies (a). To prove (b) we use assumption (f3) and the fact that, by (2.2), (2.14)
Sq :=
inf v∈H 1/2 (R)\{0}
Sq (v) > 0,
Sq (v) =
kvk . kvkLq
Let (un ) ⊂ N and u ∈ N satisfying (2.12). Then inequality (2.13) yields 2ϑ (2.15) lim sup kun k2 ≤ m. ϑ −2 n Notice that, for every v ∈ H 1/2 (R) \ {0}, arguing as for the proof of (b) of Lemma 2.4, one finds t0 > 0 such that t0 v ∈ N . Hence m ≤ J(t0 v) ≤ max J(tv). t≥0
Now, using assumption (f3) and formula (2.14), for every ψ ∈ H 1/2 (R) \ {0}, we can estimate 2 t q 2 q kψk − Cq t kψkLq m ≤ max J(tψ) ≤ max t≥0 t≥0 2 Sq (ψ)2 2 q 2 q ≤ max t kψkLq − Cq t kψkLq t≥0 2 1 1 Sq (ψ)2q/(q−2) = , − 2 q (qCq )2/(q−2) which together with (2.15) implies that 2ϑ lim sup kun k ≤ ϑ−2 n 2
1 1 − 2 q
Sq (ψ)2q/(q−2) . (qCq )2/(q−2)
Taking the infimum over ψ ∈ H 1/2 (R) \ {0}, we get 2q/(q−2)
(2.16)
ϑ q − 2 Sq lim sup kun k ≤ < ρ20 , ϑ − 2 q (qCq )2/(q−2) n 2
provided Cq is large enough, proving (b). Let us prove (c). By Lemma 2.4 (part (c)) we have Z 2 kun k = f (un )un dx ≥ ρ2 > 0. R
In view of assertion (b) the norm kun k is small (precisely, we can assumed that rαkun k2 < rαρ20 < ω for r very close to 1). Arguing as in the proof of (2.11), we can find ε ∈ (0, 1) and C > 0 such that Z Z 1/r 2 kun k2 = f (un )un dx ≤ εkun k2L2 + C erαun − 1 |un |` dx R R Z 1/r 2 ≤ εkun k2 + C erαun − 1 dx kun k`Lr0 ` R 2
≤ εkun k + Ckun k`Lr0 ` , which implies 0 < (1 − ε)ρ2 ≤ (1 − ε)kun k2 ≤ Ckun k`Lr0 ` ,
´ O.H. MIYAGAKI, AND M. SQUASSINA J.M. DO O,
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0
and, consequently, (un ) cannot vanish in Lr ` (R), as n → ∞. This concludes the proof.
Next, we formulate a Brezis-Lieb type lemma in our framework. Lemma 2.6. Let (un ) ⊂ H 1/2 (R) be a sequence such that un * u weakly in H 1/2 (R) and kun k < ρ0 with ρ0 > 0 small. Then, as n → ∞, we have Z Z Z f (un )un dx = f (un − u)(un − u) dx + f (u)u dx + o(1), R R R Z Z Z F (un ) dx = F (un − u) dx + F (u) dx + o(1). R
R
R
Proof. We shall apply [8, Lemma 3 and Theorem 2]. Since f is convex on R+ and by the properties collected in Remark 2.3, we have that the functions F (s) and G(s) := f (s)s are convex on R with F (0) = G(0) = 0. We let α ∈ (α0 , ω) and ρ0 ∈ (0, 1/2) with αρ20 < ω. Thus, by Lemma 2.2, we have Z 2 eαun − 1 dx < ∞. (2.17) sup n∈N R 0 Choose k ∈ (1, 1−ρ ρ0 ) and let ε > 0 with ε < 1/k. Then, in light of [8, Lemma 3], the functions
φε (s) := j(ks) − kj(s) ≥ 0
ψε (s) := |j(Cε s)| + |j(−Cε s)|,
s ∈ R,
Cε =
1 , ε(k − 1)
satisfy the inequality (2.18)
|j(a + b) − j(a)| ≤ εφε (a) + ψε (b),
∀a, b ∈ R,
and, if vn := un − u and un satisfying (2.17), we claim that (i) vn → 0 almost everywhere; (ii) j(u) ∈ L1 (R); R (iii) RR φε (vn )dx ≤ C for some constant C independent of n ≥ 1; (iv) R ψε (u)dx < ∞, for all ε > 0 small. Assuming this claim, then, by [8, Theorem 2], it holds Z (2.19) lim |j(un ) − j(vn ) − j(u)|dx = 0, n
R
with j = F and with j = G. Next we are going to prove the claim. Item (i) follows by the week convergence of (un ). To prove (ii) it is enough to use Proposition 2.1 (see the growth conditions below). To check (iii) for j = F and j = G, we find α ∈ (α0 , ω), D > 0 and q > 2 such that 2 (2.20) F (s) ≤ s2 + eαs − 1 + D|s|q , for all s ∈ R, 2 (2.21) G(s) ≤ s2 + eαs − 1 + D|s|q , for all s ∈ R, 2 (2.22) |f (s)| ≤ s + eαs − 1 + D|s|q−1 , for all s ∈ R, 2 (2.23) |f 0 (s)s| ≤ s + eαs − 1 + D|s|q−1 , for all s ∈ R. We claim that φε (vn ) verifies (iii). First let us consider the case j = F , that is, φε (vn ) = F (kvn ) − kF (vn ). In fact, by the Mean Value Theorem, there exists ϑ ∈ (0, 1) with wn = vn (k(1 − ϑ) + ϑ) such that φε (vn ) = F (kvn ) − F (vn ) + F (vn ) − kF (vn ) = f (wn )vn (k − 1) + (1 − k)F (vn ) ≤ f (wn )vn (k − 1),
NONLOCAL PROBLEMS WITH TRUDINGER-MOSER NONLINEARITY
9
since k > 1 and F ≥ 0. Analogously, for j = G, we have φε (vn ) = G(kvn ) − G(vn ) + G(vn ) − kG(vn ) = f 0 (wn )wn vn (k − 1) + f (wn )vn (k − 1) + (1 − k)f (vn )vn ≤ f 0 (wn )wn vn (k − 1) + f (wn )vn (k − 1), since k > 1 and f (s)s ≥ 0 for all s ∈ R. Thus, to prove (iii) for F and G, it is sufficient to see that Z Z (2.24) sup f (wn )vn dx < ∞, sup f 0 (wn )wn vn dx < ∞. n∈N R
n∈N R
We know that kun k2 = kvn k2 + kuk2 + o(1), as n → ∞, so that lim supn kvn k ≤ ρ0 . In turn, by the choice of k, we also have lim sup kwn k = kvn k(k(1 − ϑ) + ϑ) ≤ ρ0 (k(1 − ϑ) + ϑ) ≤ ρ0 (k + 1) < 1. n
Since α0 < α < ω, we can find m > 1 very close to 1 such that mα < ω. Then, by (2.22), we get Z Z Z Z 2 αwn f (wn )vn ≤ |wn ||vn |dx + (e − 1)|vn |dx + D |wn |q−1 |vn |dx R R R R Z 1/m 2 mαwn q kv k + (e − 1)dx kvn kLm0 ≤ kwn kL2 kvn kL2 + Dkwn kq−1 q n L L R Z 1/m 2 ≤ Ckwn kkvn k + Ckwn kq−1 kvn k + C (emαwn − 1)dx kvn k R Z 1/m 2 ≤C +C (emαwn − 1)dx ≤ C. R
The last integral is bounded via Lemma 2.2, since kwn k ≤ 1 and mα < ω. The second term in (2.24) can be treated in a similar fashion, using the growth condition (2.23) in place of (2.22). We claim that ψε verifies (iv) for both F and G. It suffices to prove Z F (Cε u)dx < ∞, for all ε > 0. R
By (2.20) this occurs since by Proposition 2.1, we have Z 2 2 (eαCε u − 1)dx < ∞. R
Analogous proof holds for G via (2.21). We can finally apply [8, Theorem 2] yielding (2.19). Thus Z Z Z j(un )dx = j(vn )dx + j(u)dx + o(1), R
R
R
for j = F and j = G. This concludes the proof. The previous Lemma 2.6 yields the following useful technical results. Lemma 2.7. Let (un ) ⊂ H 1/2 (R) be as in Lemma 2.5 then for vn = un − u we have J 0 (u)u + lim inf J 0 (vn )vn = 0, n
so that either
J 0 (u)u
≤ 0 or
lim inf n J 0 (vn )vn
< 0.
´ O.H. MIYAGAKI, AND M. SQUASSINA J.M. DO O,
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Proof. Recalling that vn = un − u, we get kun k2 = kvn k2 + kuk2 + o(1). Then by Lemma 2.6, Z Z Z f (un )un dx = f (vn )vn dx + f (u)u dx + o(1). R
R
R
Since un ∈ N , by using the above equality, the assertion follows.
Lemma 2.8. Let (un ) ⊂ N be a minimizing sequence for J on N , such that un * u weakly in H 1/2 (R) as n → ∞. If u ∈ N , then J(u) = m. Proof. Let (un ) ⊂ N and u ∈ N as above, thus Z 1 0 1 m + o(1) = J(un ) − J (un )un = H(un ) dx 2 2 R which together with Fatou’s lemma (recall that (2.7) holds) implies Z Z 1 1 1 m = lim inf H(un )dx ≥ lim inf H(u)dx = J(u) − J 0 (u)u = J(u), n 2 n 2 2 R R which yields the conclusion.
3. Proof of Theorem 1.1 concluded Let (un ) ⊂ N be a minimizing sequence for J on N . From Lemma 2.5 (a), (un ) is bounded in H 1/2 (R). Thus, up to a subsequence, we have un * u weakly in H 1/2 (R). Assertion 3.1. There exist a sequence (yn ) ⊂ R and constants γ, R > 0 such that Z yn +R lim inf |un |2 dx ≥ γ > 0 n
yn −R
If not, for any R > 0, Z
y+R
|un |2 dx = 0.
lim inf sup n
y∈R
y−R
Using a standard concentration-compactness principle due to P.L. Lions (it is easy to see that the argument remains valid for the case studied here) we can conclude that un → 0 in Lq (R) for any q > 2, which is a contradiction with Lemma 2.5 (c). Define u ¯n (x) = un (x + yn ). Then J(un ) = J(¯ un ) and without of loss generality we can assume yn = 0 for any n. Notice that (¯ un ) is also a minimizing sequence for J on N , which it is bounded and satisfies Z R lim inf |¯ un |2 dx ≥ γ, for some γ > 0, n
and u ¯n * u ¯ weakly in
H 1/2 (R),
−R
then u ¯ 6= 0 (u 6= 0).
Assertion 3.2. J 0 (u)u = 0. If Assertion 3.2 holds, then combining (d) of Lemma 2.4 and Lemma 2.8 we have the result. We shall now prove Assertion 3.2. Suppose by contradiction that J 0 (u)u 6= 0. • If J 0 (u)u < 0, by Lemma 2.4 (b), there exists 0 < λ < 1 such that λu ∈ N . Thus Z 2 (3.1) λkuk = f (λu)u dx. R
Using (2.7) in combination with Fatou’s Lemma, we obtain Z Z Z 1 1 1 1 m = lim inf H(un ) dx ≥ H(u) dx > H(λu) dx = J(λu) − J 0 (λu)λu = J(λu), n 2 R 2 R 2 R 2
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which implies that J(λu) < m and, hence, a contradiction. Here we have used (2.9). • If J 0 (u)u > 0, by Lemma 2.7, we get lim inf n J 0 (vn )vn < 0. Taking a subsequence, we have J 0 (vn )vn < 0, for n large. By Lemma 2.4 (b), there exists λn ∈ (0, 1) such that λn vn ∈ N . Assertion 3.3. lim supn λn < 1. If lim supn λn = 1, up to a sub-sequence, we can assume that λn → 1, then J 0 (vn )vn = J 0 (λn vn )λn vn + o(1). This follows provided that Z
Z
f (λn vn )λn vn dx + o(1).
f (vn )vn dx =
(3.2)
R
R
In fact, notice that if ηn := vn + τ vn (λn − 1) for some τ ∈ (0, 1), it follows f (vn )vn − f (λn vn )λn vn = f 0 (ηn )ηn + f (ηn ) vn (1 − λn ). Since kηn k = kvn + τ vn (λn − 1)k ≤ λn kvn k ≤ ρ0 , it follows by arguing as for the justification of formula (2.24), that Z sup |f 0 (ηn )ηn + f (ηn )||vn |dx < ∞, n∈N R
so that (3.2) follows, since λn → 1. Since λn vn ∈ N we have J 0 (λn vn )λn vn = 0 which implies that J 0 (vn )vn = o(1), which is a contradiction with limn J 0 (vn )vn < 0. Thus, up to subsequence, we may assume that λn → λ0 ∈ (0, 1). Arguing as before, from (2.9) we infer Z Z 1 1 m + o(1) = H(un ) dx ≥ H(λn un ) dx, 2 R 2 R since H(un ) ≥ H(λn un ). By means of Lemma 2.6 applied to wn = λn un (whose norm is small, being smaller than the norm of un ) and w = λ0 u we have in turn Z Z Z H(λn un ) dx = H(λn un − λ0 u) dx + H(λ0 u) dx + o(1). R
R
R
Furthermore, we have Z
Z H(λn un − λ0 u) dx =
(3.3) R
H(λn vn ) dx + o(1). R
In fact, notice that λn un − λ0 u = λn vn + γn u, where γn := λn − λ0 → 0 as n → ∞. We have H(λn un − λ0 u) − H(λn vn ) = H0 (ˆ ηn )uγn ,
ηˆn := τ uγn + λn vn
for τ ∈ (0, 1) and kˆ ηn k = kτ uγn + λn vn k ≤ γn kuk + λn kvn k ≤ ρ0 for n large. Then, arguing as for the justification of (2.24), we get Z Z 0 sup |H (ˆ ηn )||u|dx ≤ sup |f 0 (ˆ ηn )ˆ ηn + f (ˆ ηn )||vn |dx < ∞, n∈N R
n∈N R
which yields (3.3) since γn → 0 as n → ∞. Therefore, we obtain Z Z 1 1 H(λn vn ) dx + H(λ0 u) dx m + o(1) ≥ 2 R 2 R Z Z 1 0 1 1 = J(λn vn ) − J (λn vn )λvn + H(λ0 u) dx = J(λn vn ) + H(λ0 u) dx. 2 2 R 2 R R Since u 6= 0, we have R H(λ0 u) dx > 0. Then J(λn vn ) < m for large n, a contradiction.
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References [1] Adimurthi, S.L. Yadava, Multiplicity results for semilinear elliptic equations in a bounded domain of R2 involving critical exponent, Ann. Sc. Norm. Super. Pisa Cl. Sci. (1990), 481–504. 2 ´ O. Miyagaki, On nonlinear perturbations of a periodic elliptic problem in R2 involving [2] C. Alves, J. M. do O, critical growth, Nonlinear Anal. 56 (2004), 781–791. 2 [3] C. Alves, M. Souto, M. Montenegro, Existence of a ground state solution for a nonlinear scalar field equation with critical growth, Calc. Var. Partial Differential Equations 43 (2012), 537–554. 2 [4] A. Ambrosetti, Z.-Q. Wang, Positive solutions to a class of quasilinear elliptic equations on R, Discrete Contin. Dyn. Syst. 9 (2003), 55–68. 2 [5] B. Barrios, E. Colorado, A. de Pablo, U. S´ anchez, On some critical problems for the fractional Laplacian operator, J. Differential Equations 252 (2012), 613–6162. 3 [6] H. Berestycki, P.-L. Lions, Nonlinear scalar field equations, I-existence of a ground state. Arch. Rat. Mech. Anal. 82 (1983), 313–346. 2, 3 [7] H. Berestycki, T. Gallouet, O. Kavian, Equations de Champs scalaires euclidiens non lineaires dans le plan, C. R. Acad. Sci. Paris Ser. I Math. 297 (1984), 307–310. 2 [8] H. Brezis, E. Lieb, A relation between pointwise convergence of functions and convergence of functionals, Proc. Amer. Math. Soc. 88 (1983), 486–490. 8, 9 [9] X. Cabr´e, J. G. Tan, Positive solutions of nonlinear problems involving the square root of the Laplacian, Adv. Math. 224 (2010), 2052–2093. 3 [10] X. Chang, Z-Q. Wang, Ground state of scalar field equations involving a fractional laplacian with general nonlinearity, Nonlinearity 26 (2013), 479-494. 2, 3 [11] D. Cao, Nontrivial solution of semilinear elliptic equation with critical exponent in R2 , Comm. Partial Differential Equations 17(1992), 407–435. 2 [12] V. Coti Zelati, P. Rabinowitz, Homoclinic type solutions for a semilinear elliptic PDE on RN . Comm. Pure Appl. Math. 45 (1992), 1217–1269. 2 ´ B. Ruf, Elliptic Equations and Systems with critical Trudinger-Moser [13] D. G. de Figueiredo, J. M. do O, nonlinearities, Discrete Contin. Dyn. Syst. 30 (2011), 455–476. 2 [14] D. G. de Figueiredo, O. H. Miyagaki, B. Ruf, Elliptic equations in R2 with nonlinearities in the critical growth range, Calc. Var. Partial Differential Equations 3 (1995), 139–153. 2 ´ B. Ruf, On an inequality by N. Trudinger and J. Moser and related elliptic [15] D. G. De Figueiredo, J. M. do O, equations, Comm. Pure Appl. Math. 55 (2002), 135–152. 2 [16] E. Di Nezza, G. Palatucci, E. Valdinoci, Hitchhiker’s guide to the fractional Sobolev spaces, Bull. Sci. Math. 136 (2012), 521–573. 3 ´ E. Medeiros, U. Severo, A nonhomogeneous elliptic problem involving critical growth in dimension [17] J. M. do O, two, J. Math. Anal. Appl. 345 (2008), 286–304. 2 ´ O. H. Miyagaki, M. Squassina, Critical and subcritical fractional problems with vanishing potentials, [18] J. M. do O, preprint 3 ´ O. H. Miyagaki, M. Squassina, Nonautonomous fractional problems with exponential growth, NoDEA [19] J. M. do O, Nonlinear Differential Equations Applications, to appear. 2, 3 [20] P. Felmer, A. Quaas, J. Tan Positive solutions of nonlinear Schr¨ odinger equation with the fractional Laplacian, Proc. Roy. Soc. Edinburgh A 142 (2012), 1237-1262. 3 [21] R. Frank, E. Lenzmann, Uniqueness of non-linear ground states for fractional laplacians in R, Acta Math. 210 (2013), 261–318. 2, 3 [22] T. Jin, Y. Li, J. Xiong, On a fractional Nirenberg problem, part I: blow up analysis and compactness of solutions, J. Eur. Math. Soc. 16 (2014), 1111–1171. 3 [23] A. Iannizzotto, M. Squassina, 1/2-laplacian problems with exponential nonlinearity, J. Math. Anal. Appl. 414 (2014), 372–385. 2, 3 [24] M.A. Krasnosel’ski˘ı, J.B. Ruticki˘ı, Convex functions and Orlicz spaces, Noordhoff, Groningen, Holland, 1961. 4 [25] N. Lam, G. Lu, Elliptic equations and systems with subcritical and critical exponential growth without the Ambrosetti-Rabinowitz condition, J. Geom. Anal. 24 (2014), 118–143. 2 [26] E. H. Lieb, M. Loss, Analysis, AMS, 2001. 3 [27] J. Moser, A sharp form of an inequality by N. Trudinger, Indiana Univ. Math. J. 20 (1970), 1077–1092. 2 [28] T. Ozawa, On critical cases of Sobolev’s inequalities, J. Funct. Anal. 127 (1995), 259–269. 1, 3 [29] B. Ruf, F. Sani, Ground states for elliptic equations in R2 with exponential critical growth. Geometric properties for parabolic and elliptic PDE’s, 251–267, Springer INdAM 2, Springer, Milan, 2013. 2
NONLOCAL PROBLEMS WITH TRUDINGER-MOSER NONLINEARITY
13
[30] X. Shang, J. Zhang, Y. Yang, On fractional Sch¨ odinger equation in RN with critical growth, J. Math. Phys. 54 (2013), 121502-19 pages. 3 [31] S. Secchi, Ground state solutions for nonlinear fractional Schr¨ odinger equations in RN , J. Math. Phys. 54 (2013), 031501-17 pages. 3 [32] W. Strauss, Existence of solitary waves in higher dimensions,. Comm. Math. Phys. 55 (2) (1977), 149–162. 2 [33] N. Trudinger, On imbeddings into Orlicz spaces and some applications, J. Math. Mech. 17 (1967), 473–483. 2 [34] M. Willem,Minimax Theorems, Progress in Nonlinear Differential Equations and their Applications, 24, Birkh¨ auser 1996. 2
´ Department of Mathematics, Federal University of Para´ıba (J.M. do O) ˜ o Pessoa-PB, Brazil 58051-900, Joa E-mail address:
[email protected] (O. Miyagaki) Department of Mathematics, Federal University of Juiz de Fora 36036-330 Juiz de Fora, Minas Gerais, Brazil E-mail address:
[email protected] ` degli Studi di Verona, (M. Squassina) Dipartimento di Informatica Universita ´ Vignal 2, Strada Le Grazie 15, I-37134 Verona, Italy Ca E-mail address:
[email protected]