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1.
Consider an evolution family U=(U(t,s))t?s?0 on a half-line R+ and a semi-linear integral equation . We prove the existence of stable manifolds of solutions to this equation in the case that (U(t,s))t?s?0 has an exponential dichotomy and the nonlinear forcing term f(t,x) satisfies the non-uniform Lipschitz conditions: ‖f(t,x1)−f(t,x2)‖?φ(t)‖x1x2‖ for φ being a real and positive function which belongs to admissible function spaces which contain wide classes of function spaces like function spaces of Lp type, the Lorentz spaces Lp,q and many other function spaces occurring in interpolation theory.  相似文献   

2.
Positive periodic solutions of functional differential equations   总被引:1,自引:0,他引:1  
We consider the existence, multiplicity and nonexistence of positive ω-periodic solutions for the periodic equation x′(t)=a(t)g(x)x(t)−λb(t)f(x(tτ(t))), where are ω-periodic, , , f,gC([0,∞),[0,∞)), and f(u)>0 for u>0, g(x) is bounded, τ(t) is a continuous ω-periodic function. Define , , i0=number of zeros in the set and i=number of infinities in the set . We show that the equation has i0 or i positive ω-periodic solution(s) for sufficiently large or small λ>0, respectively.  相似文献   

3.
Let u(t,x) be the solution of the heat equation (∂tx)u(t,x)=0 on subject to u(0,x)=f(x) on Rn. The main goal of this paper is to characterize such a nonnegative measure μ on that f(x)?u(t2,x) induces a bounded embedding from the Sobolev space , p∈[1,n) into the Lebesgue space , q∈(0,∞).  相似文献   

4.
Let 1=d1(n)<d2(n)<?<dτ(n)=n be the sequence of all positive divisors of the integer n in increasing order. We say that the divisors of n are t-dense iff max1?i<τ(n)di+1(n)/di(n)?t. Let D(x,t) be the number of positive integers not exceeding x whose divisors are t-dense. We show that for x?3, and , we have , where , and d(w) is a continuous function which satisfies d(w)?1/w for w?1. We also consider other counting functions closely related to D(x,t).  相似文献   

5.
Consider an evolution family U=(U(t,s))t?s?0 on a half-line R+ and a semi-linear integral equation . We prove the existence of invariant manifolds of this equation. These manifolds are constituted by trajectories of the solutions belonging to admissible function spaces which contain wide classes of function spaces like function spaces of Lp type, the Lorentz spaces Lp,q and many other function spaces occurring in interpolation theory. The existence of such manifolds is obtained in the case that (U(t,s))t?s?0 has an exponential dichotomy and the nonlinear forcing term f(t,x) satisfies the non-uniform Lipschitz conditions: ‖f(t,x1)−f(t,x2)‖?φ(t)‖x1x2‖ for φ being a real and positive function which belongs to certain classes of admissible function spaces.  相似文献   

6.
Let 1=d1(n)<d2(n)<?<dτ(n)=n be the sequence of all positive divisors of the integer n in increasing order. We say that the divisors of n are y-dense iff max1?i<τ(n)di+1(n)/di(n)?y. Let D(x,y,z) be the number of positive integers not exceeding x whose divisors are y-dense and whose prime divisors are bigger than z, and let , and . We show that is equivalent, in a large region, to a function d(u,v) which satisfies a difference-differential equation. Using that equation we find that d(u,v)?(1−u/v)/(u+1) for v?3+ε. Finally, we show that d(u,v)=eγd(u)+O(1/v), where γ is Euler's constant and d(u)∼x−1D(x,y,1), for fixed u. This leads to a new estimate for d(u).  相似文献   

7.
The classical criterion of asymptotic stability of the zero solution of equations x=f(t,x) is that there exists a function V(t,x), a(‖x‖)?V(t,x)?b(‖x‖) for some a,bK, such that for some cK. In this paper we prove that if f(t,x) is bounded, is uniformly continuous and bounded, then the condition that can be weakened and replaced by and contains no complete trajectory of , t∈[−T,T], where , uniformly for (t,x)∈[−T,TBH.  相似文献   

8.
9.
10.
In this paper we study Cauchy problem of generalized double dispersion equations uttuxxuxxtt+uxxxx=f(u)xx, where f(u)=p|u|, p>1 or u2k, . By introducing a family of potential wells we not only get a threshold result of global existence and nonexistence of solutions, but also obtain the invariance of some sets and vacuum isolating of solutions. In addition, the global existence and finite time blow up of solutions for problem with critical initial conditions E(0)=d, I(u0)?0 or I(u0)<0 are proved.  相似文献   

11.
12.
We study the differentiability of very weak solutions vL1(Ω) of 0(v,L?φ)=0(f,φ) for all vanishing at the boundary whenever f is in L1(Ω,δ), with δ=dist(x,∂Ω), and L* is a linear second order elliptic operator with variable coefficients. We show that our results are optimal. We use symmetrization techniques to derive the regularity in Lorentz spaces or to consider the radial solution associated to the increasing radial rearrangement function of f.  相似文献   

13.
In this paper, a higher order p-Laplacian neutral functional differential equation with a deviating argument:
[φp([x(t)−c(t)x(tσ)](n))](m)+f(x(t))x(t)+g(t,x(tτ(t)))=e(t)  相似文献   

14.
Let be a contractive gauge function in the sense that φ is continuous, φ(s)<s for s>0, and if f:M→M satisfies d(f(x),f(y))?φ(d(x,y)) for all x,y in a complete metric space (M,d), then f always has a unique fixed point. It is proved that if T:M→M satisfies
  相似文献   

15.
We consider, for p∈(1,2) and q>1, self-similar singular solutions of the equation vt=div(|∇v|p−2v)−vq in Rn×(0,∞); here by self-similar we mean that v takes the form v(x,t)=tαw(|x|tαβ) for α=1/(q−1) and β=(q+1−p)/p, whereas singular means that v is non-negative, non-trivial, and for all x≠0. That is, we consider the ODE problem
(0.1)  相似文献   

16.
We shall be concerned with the existence of heteroclinic orbits for the second order Hamiltonian system , where qRn and VC1(R×Rn,R), V?0. We will assume that V and a certain subset MRn satisfy the following conditions. M is a set of isolated points and #M?2. For every sufficiently small ε>0 there exists δ>0 such that for all (t,z)∈R×Rn, if d(z,M)?ε then −V(t,z)?δ. The integrals , zM, are equi-bounded and −V(t,z)→∞, as |t|→∞, uniformly on compact subsets of Rn?M. Our result states that each point in M is joined to another point in M by a solution of our system.  相似文献   

17.
We show that for every Lipschitz function f defined on a separable Riemannian manifold M (possibly of infinite dimension), for every continuous , and for every positive number r>0, there exists a C smooth Lipschitz function such that |f(p)−g(p)|?ε(p) for every pM and Lip(g)?Lip(f)+r. Consequently, every separable Riemannian manifold is uniformly bumpable. We also present some applications of this result, such as a general version for separable Riemannian manifolds of Deville-Godefroy-Zizler's smooth variational principle.  相似文献   

18.
19.
Let B be the unit ball of with respect to an arbitrary norm. We study certain properties of Loewner chains and their transition mappings on the unit ball B. We show that any Loewner chain f(z,t) and the transition mapping v(z,s,t) associated to f(z,t) satisfy locally Lipschitz conditions in t locally uniformly with respect to zB. Moreover, we prove that a mapping fH(B) has parametric representation if and only if there exists a Loewner chain f(z,t) such that the family {etf(z,t)}t?0 is a normal family on B and f(z)=f(z,0) for zB. Also we show that univalent solutions f(z,t) of the generalized Loewner differential equation in higher dimensions are unique when {etf(z,t)}t?0 is a normal family on B. Finally we show that the set S0(B) of mappings which have parametric representation on B is compact.  相似文献   

20.
Let A be a selfadjoint linear operator in a Hilbert space H. The DSM (dynamical systems method) for solving equation Av=f consists of solving the Cauchy problem , u(0)=u0, where Φ is a suitable operator, and proving that (i) ∃u(t)∀t>0, (ii) ∃u(∞), and (iii) A(u(∞))=f. It is proved that if equation Av=f is solvable and u solves the problem , u(0)=u0, where a>0 is a parameter and u0 is arbitrary, then lima→0limt→∞u(t,a)=y, where y is the unique minimal-norm solution of the equation Av=f. Stable solution of the equation Av=f is constructed when the data are noisy, i.e., fδ is given in place of f, ‖fδf‖?δ. The case when a=a(t)>0, , a(t)↘0 as t→∞ is considered. It is proved that in this case limt→∞u(t)=y and if fδ is given in place of f, then limt→∞u(tδ)=y, where tδ is properly chosen.  相似文献   

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