Global existence and boundedness for a class of second-order nonlinear differential equations

In this paper we obtain new conditions for the global existence and boundedness of solutions for nonlinear second-order equations of the form ${\left(r\left(t\right){\left|u^{\prime }\right|}^{p?2}{u}^{\prime }\right)}^{\prime }+g(t,u,u^{\prime })u^{\prime }+a\left(t\right)f\left(u\right)=e\left(t\right)\text{,}$ where $p>1$ is a real constant. The results are applicable to well-known Emden–Fowler and Lienard type equations. An illustrative example is also provided.     

Lump solutions to nonlinear partial differential equations via Hirota bilinear forms

Lump solutions are analytical rational function solutions localized in all directions in space. We analyze a class of lump solutions, generated from quadratic functions, to nonlinear partial differential equations. The basis of success is the Hirota bilinear formulation and the primary object is the class of positive multivariate quadratic functions. A complete determination of quadratic functions positive in space and time is given, and positive quadratic functions are characterized as sums of squares of linear functions. Necessary and sufficient conditions for positive quadratic functions to solve Hirota bilinear equations are presented, and such polynomial solutions yield lump solutions to nonlinear partial differential equations under the dependent variable transformations $u=2{(\ln ?f)}_x$ and $u=2{(\ln ?f)}_{xx}$, where x is one spatial variable. Applications are made for a few generalized KP and BKP equations.     

Weighted pseudo-almost periodic solutions of a class of semilinear fractional differential equations

We study the existence and uniqueness of a weighted pseudo-almost periodic (mild) solution to the semilinear fractional equation ${?}_t^{\alpha }u=Au+{?}_t^{\alpha ?1}f(?,u)$, $1<\alpha <2$, where $A$ is a linear operator of sectorial negative type. This article also deals with the existence of these types of solutions to abstract partial evolution equations.     

On a conjecture of the Randić index and the minimum degree of graphs

The Randi? index $R\left(G\right)$ of a graph $G$ is defined by $R\left(G\right)={\sum }_{uv}\frac{1}{\sqrt{d\left(u\right)d\left(v\right)}}$, where $d\left(u\right)$ is the degree of a vertex $u$ and the summation extends over all edges $uv$ of $G$. Delorme et al. (2002)  [6] put forward a conjecture concerning the minimum Randi? index among all$n$-vertex connected graphs with the minimum degree at least $k$. In this work, we show that the conjecture is true given the graph contains $k$ vertices of degree $n?1$. Further, it is true among $k$-trees.     

Exponential independence

For a set $S$ of vertices of a graph $G$, a vertex $u$ in $V\left(G\right)?S$, and a vertex $v$ in $S$, let ${\mathrm{dist}}_{(G,S)}(u,v)$ be the distance of $u$ and $v$ in the graph $G?(S?\left\{v\right\})$. Dankelmann et al. (2009) define $S$ to be an exponential dominating set of $G$ if $w_{(G,S)}\left(u\right)\ge 1$ for every vertex $u$ in $V\left(G\right)?S$, where $w_{(G,S)}\left(u\right)={\sum }_{v\in S}{\left(\frac{1}{2}\right)}^{{\mathrm{dist}}_{(G,S)}(u,v)?1}$. Inspired by this notion, we define $S$ to be an exponential independent set of $G$ if $w_{(G,S?\left\{u\right\})}\left(u\right)<1$ for every vertex $u$ in $S$, and the exponential independence number ${\alpha }_e\left(G\right)$ of $G$ as the maximum order of an exponential independent set of $G$.Similarly as for exponential domination, the non-local nature of exponential independence leads to many interesting effects and challenges. Our results comprise exact values for special graphs as well as tight bounds and the corresponding extremal graphs. Furthermore, we characterize all graphs $G$ for which ${\alpha }_e\left(H\right)$ equals the independence number $\alpha \left(H\right)$ for every induced subgraph $H$ of $G$, and we give an explicit characterization of all trees $T$ with ${\alpha }_e\left(T\right)=\alpha \left(T\right)$.     

Fractional index convolution complementarity problems

Convolution complementarity problems have the form: given a kernel function $k$ and a function $q$, find a function $u$ such that $u\left(t\right)\ge 0$, $(k1u)\left(t\right)+q\left(t\right)\ge 0$ for (almost) all $t$, and where ${\int }_0^{T}u{\left(t\right)}^T[(k1u)\left(t\right)+q\left(t\right)]dt=0$. A fractional index problem of this kind has $k\left(t\right)\sim K_0{t}^{\alpha -1}$ for $t$ small, with $0<\alpha <1$. Such problems are shown to have unique solutions under mild conditions.     

Existence of weak solutions of the g-Kelvin–Voight equation

The 2D $g$-Navier–Stokes equations have the form $\frac{?u}{?t}?\nu \Delta u+u.?u+?p=f\text{in }\Omega$ with the continuity equation $?.\left(gu\right)=0\text{in }\Omega$ in a bounded domain $\Omega ?{\mathbb{R}}^2$ where $g=g\left(x_{1,}{x}_2\right)$ is a smooth real valued function defined on $\Omega$. We use the method described by Roh [J. Roh, $g$-Navier Stokes equations, Ph.D. Thesis, University of Minnesota, 2001] for the derivation of $g$-Kelvin–Voight equations represented by $\frac{?u}{?t}?\nu {\Delta }_{g}u+\frac{\nu }{g}(?g??)u?\alpha {\Delta }_g{u}_t+\frac{\alpha }{g}(?g??)u_t+u??u+?p=f\left(x\right)\text{ in }\Omega$$?.\left(gu\right)=0\text{in }\Omega$ We discuss the existence and uniqueness of weak solutions of $g$-Kelvin–Voight equations by the use of the well known Feado–Galerkin method.     

Existence of positive periodic solutions to nonlinear second order differential equations

In this paper, we discuss the existence of positive periodic solutions to the nonlinear differential equation $u^{″}\left(t\right)+a\left(t\right)u\left(t\right)=f(t,u\left(t\right))\text{,}t\in R\text{,}$ where $a:R\to [0,+\infty )$ is an $\omega$-periodic continuous function with $a\left(t\right)⁄\equiv 0$, $f:R\times [0,+\infty )\to [0,+\infty )$ is continuous and $f(\cdot ,u):R\to [0,+\infty )$ is also an $\omega$-periodic function for each $u\in [0,+\infty )$. Using the fixed point index theory in a cone, we get an essential existence result because of its involving the first positive eigenvalue of the linear equation with regard to the above equation.