“…As is known to us, many structures in our real life can be represented by a connected graph whose vertices represent nodes and whose edges represent their links, such as the internet, brain, organizations and so on. In recent years, the investigations of discrete weighted Laplacians and various equations on graphs have attracted attention from many authors (see [1,4,5,9,10,11,12,16,18,20] and references therein). There have been some works on dealing with blow-up phenomenon of the equations on graphs, for example, Xin et al [20] investigated the blow-up properties of the Dirichlet boundary value problem for u t = ∆u + u p (p > 0) on a finite graph.…”
Let G = (V, E) be a locally finite connected weighted graph, ∆ be the usual graph Laplacian. In this paper, we study the blow-up problems for the nonlinear parabolic equationThe blow-up phenomenons of the equation are discussed in terms of two cases: (i) an initial condition is given; (ii) a Dirichlet boundary condition is given. We prove that if f satisfies appropriate conditions, then the solution of the equation blows up in a finite time.
“…As is known to us, many structures in our real life can be represented by a connected graph whose vertices represent nodes and whose edges represent their links, such as the internet, brain, organizations and so on. In recent years, the investigations of discrete weighted Laplacians and various equations on graphs have attracted attention from many authors (see [1,4,5,9,10,11,12,16,18,20] and references therein). There have been some works on dealing with blow-up phenomenon of the equations on graphs, for example, Xin et al [20] investigated the blow-up properties of the Dirichlet boundary value problem for u t = ∆u + u p (p > 0) on a finite graph.…”
Let G = (V, E) be a locally finite connected weighted graph, ∆ be the usual graph Laplacian. In this paper, we study the blow-up problems for the nonlinear parabolic equationThe blow-up phenomenons of the equation are discussed in terms of two cases: (i) an initial condition is given; (ii) a Dirichlet boundary condition is given. We prove that if f satisfies appropriate conditions, then the solution of the equation blows up in a finite time.
“…There are works related to some important geometric inequalities on graphs [3,20]. Many aspects about heat equation such as existence and non-existence of global solutions [7,24,25], uniqueness and blow-up properties [21,30], estimates for heat kernel [20,23,29] have also been considered. For the elliptic case, Grigoryan et al [16][17][18] established existence results on graphs for some nonlinear elliptic equations based on the variational framework and this inspires us to deal with the Schödinger type equations on graphs.…”
We consider the nonlinear Schrödinger equation −∆u + (λa(x) + 1)u = |u| p−1 u on a locally finite graph G = (V, E). We prove via the Nehari method that if a(x) satisfies certain assumptions, for any λ > 1, the equation admits a ground state solution u λ . Moreover, as λ → ∞, the solution u λ converges to a solution of the Dirichlet problem −∆u + u = |u| p−1 u which is defined on the potential well Ω. We also provide a numerical experiment which solves the equation on a finite graph to illustrate our results.
“…To do analysis works, it is necessary to study partial differential equations on graphs and this subject has attracted much attention recently. For example, several fundamental aspects of heat equations on graphs, such as heat kernel [14,29], existence and uniqueness [16,20,22] are investigated by different authors.…”
In this paper, we first prove some propositions of Sobolev spaces defined on a locally finite graph G = (V, E), which are fundamental when dealing with equations on graphs under the variational framework. Then we consider a nonlinear biharmonic equationUnder some suitable assumptions, we prove that for any λ > 1 and p > 2, the equation admits a ground state solution u λ . Moreover, we prove that as λ → +∞, the solutions u λ converge to a solution of the equationwhere Ω = {x ∈ V : a(x) = 0} is the potential well and ∂Ω denotes the the boundary of Ω.
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