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20 - Nonlocal critical equations with concave-convex nonlinearities

from Part III - Nonlocal critical problems

Published online by Cambridge University Press:  05 March 2016

Giovanni Molica Bisci
Affiliation:
Università di Reggio Calabria, Italy
Vicentiu D. Radulescu
Affiliation:
Institute of Mathematics of the Romanian Academy
Raffaella Servadei
Affiliation:
Università degli Studi di Urbino, Italy
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Summary

In this chapter, we focus our attention on the following critical nonlocal fractional problem:

where s ∈ (0, 1) is fixed, and (− Δ)s is the fractional Laplace operator defined, up to normalization factors, as in (1.20), while Ω ∈ ℝn, n > 2s, is open, bounded and with continuous boundary and λ > 0. The main results of this chapter show the existence and multiplicity of solutions to problem (20.1) for different values of λ. The dependency on this parameter changes according to whether we consider the concave power case (0 < q < 1) or the convex power case (1 < q < 2s*−1). These two cases will be treated separately.

One also can define a fractional power of the Laplacian using spectral decomposition, as discussed in Chapter 5. The same problem is considered here, but this spectral fractional Laplacian was treated in [22]. Some related problems involving this operator have been studied in [42, 51, 73, 214]. As in [22], the purpose of this chapter is to study the existence of weak solutions for (20.1).

Problems similar to (20.1) have been also studied in the local setting with different elliptic operators. As far as we know, the first example in this direction was given in [111] for the p-Laplacian operator, Δp (see Chapter 1). Other results, this time for the Laplacian (or essentially the classical Laplacian) operator, can be found in [2, 8, 22, 39]. More generally, the case of fully nonlinear operators was studied in [66].

It is worth noting here that problem (20.1), with λ = 0, has no solution whenever Ω is a star-shaped domain. This was proved in [103, 185] using a Pohozaev identity for the operator (− Δ)s. This fact motivates the perturbation term λuq, λ > 0. The results of this chapter were obtained in [23].

Main results

We now summarize the main results of this chapter. First, in Section 20.2, we will look at problem (20.1) in the concave case q < 1, and we will prove the following result:

Theorem 20.1Let s ∈ (0, 1), n > 2s, and q ∈ (0, 1).

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Publisher: Cambridge University Press
Print publication year: 2016

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