이종락 2018-11-15T16:30:07Z 2018-11-15T16:30:07Z 2018 2073-8994 OAK-23598 http://dspace.ewha.ac.kr/handle/2015.oak/246474 We herein discuss the following elliptic equations: M( integral(RN)integral(RN) vertical bar u(x)-u(y)vertical bar(p)/vertical bar x-y vertical bar(N+ps) dx dy)(-Delta)(p)(s)u + V(x)vertical bar u vertical bar(p-2) u = lambda f(x,u) in R-N, where (-Delta)(p)(s) is the fractional p-Laplacian defined by (-Delta)(p)(s) u(x) = 2 lim(epsilon SE arrow 0 )integral(RN\B epsilon(x)) vertical bar u(x)-u(y)vertical bar(p-2)(u(x)-u(y))/vertical bar x-y vertical bar(N+ps) dy, x is an element of R-N. Here, B-epsilon(x): = {y is an element of R-N: vertical bar x-y vertical bar &lt; epsilon}, V : R-N -&gt; (0, infinity) is a continuous function and f : R-N x R -&gt; R is the Caratheodory function. Furthermore, M : R-0(+)-&gt; R+ is a Kirchhoff-type function. This study has two aims. One is to study the existence of infinitely many large energy solutions for the above problem via the variational methods. In addition, a major point is to obtain the multiplicity results of the weak solutions for our problem under various assumptions on the Kirchhoff function M and the nonlinear term f. The other is to prove the existence of small energy solutions for our problem, in that the sequence of solutions converges to 0 in the L-infinity-norm. English MDPI fractional p-Laplacian Kirchhoff-type equations fountain theorem modified functional methods Moser iteration method Multiplicity of Small or Large Energy Solutions for Kirchhoff-Schrodinger-Type Equations Involving the Fractional p-Laplacian in R-N Article 10 10 SCIE SCOPUS SYMMETRY-BASEL 10.3390/sym10100436 WOS:000448561000016 2-s2.0-85055751918 Kim, Jae-Myoung Kim, Yun-Ho Lee, Jongrak 20190701081002