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2015
DOI: 10.1016/j.jmaa.2014.07.031
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Multiple positive solutions for Kirchhoff type of problems with singularity and critical exponents

Abstract: In this paper, we study multiplicity of positive solutions for a class of Kirchhoff type of equations with the nonlinearity containing both singularity and critical exponents. We obtain two positive solutions via the variational and perturbation methods.

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Cited by 108 publications
(59 citation statements)
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References 21 publications
(22 reference statements)
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“…This equation extends the classical D'Alembert wave equation for free vibrations of elastic strings, which takes into account the changes in length of the string produced by transverse vibrations; while purely longitudinal motions of a viscoelastic bar of uniform cross section and its generalizations can be found in [2][3][4][5][6][7][8]. A distinguishing feature of equation ( the equation is no longer a pointwise identity.…”
Section: Introduction and Main Resultsmentioning
confidence: 82%
“…This equation extends the classical D'Alembert wave equation for free vibrations of elastic strings, which takes into account the changes in length of the string produced by transverse vibrations; while purely longitudinal motions of a viscoelastic bar of uniform cross section and its generalizations can be found in [2][3][4][5][6][7][8]. A distinguishing feature of equation ( the equation is no longer a pointwise identity.…”
Section: Introduction and Main Resultsmentioning
confidence: 82%
“…on a smooth bounded domain Ω ⊂ R 3 and f : Ω×R → R a continuous function, has been extensively studied (see [1,3,10,11,[15][16][17]19,18,20,23,24,30]). Particularly, in [24] Sun and Tang have considered the following problem…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…In particular, when λ = 1, p = 5, problem (1.4) has at least two solutions for μ > 0 small enough, such as [2,6,12,25,[27][28][29]. However, the singular Kirchhoff type problems have few been considered, except for [15] and [17]. Liu and Sun in [17] have investigated problem (1.2) with f (x, u) = g(x)u −γ + λh(x) u p |x| s , and g, h ∈ C(Ω), 0 ≤ s < 1, 3 < p < 5 − 2s.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
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“…We will remove the singularity by the perturbation method. Our idea comes from [24,27]. The energy functional corresponding to (1.1) is defined by…”
Section: Introductionmentioning
confidence: 99%