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1.
We investigate the low regularity local and global well-posedness of the Cauchy problem for the coupled Klein-Gordon-Schrödinger system with fractional Laplacian in the Schrödinger equation in R1+1. We use Bourgain space method to study this problem and prove that this system is locally well-posed for Schrödinger data in Hs1 and wave data in Hs2 ×Hs2?1 for 3/4?α < s1 ≤ 0 and ?1/2 < s2 < 3/2, where α is the fractional power of Laplacian which satisfies 3/4 < α ≤ 1. Based on this local well-posedness result, we also obtain the global well-posedness of this system for s1 = 0 and ?1/2 < s2 < 1/2 by using the conservation law for the L2 norm of u.  相似文献   

2.
We consider a semigroup of Markovian and symmetric operators to which we associate fractional Sobolev spaces Dαp (0 < α < 1 and 1 < p < ∞) defined as domains of fractional powers (−Ap)α/2, where Ap is the generator of the semigroup in Lp. We show under rather general assumptions that Lipschitz continuous functions operate by composition on Dαp if p ≥ 2. This holds in particular in the case of the Ornstein-Uhlenbeck semigroup on an abstract Wiener space.  相似文献   

3.
In this paper, we derive global sharp heat kernel estimates for symmetric ??-stable processes (or equivalently, for the fractional Laplacian with zero exterior condition) in two classes of unbounded C 1,1 open sets in ${\mathbb R^d}$ : half-space-like open sets and exterior open sets. These open sets can be disconnected. We focus in particular on explicit estimates for p D (t, x, y) for all t?>?0 and ${x, y\,{\in}\,D}$ . Our approach is based on the idea that for x and y in D far from the boundary and t sufficiently large, we can compare p D (t, x, y) to the heat kernel in a well understood open set: either a half-space or ${\mathbb R^d}$ ; while for the general case we can reduce them to the above case by pushing x and y inside away from the boundary. As a consequence, sharp Green functions estimates are obtained for the Dirichlet fractional Laplacian in these two types of open sets. Global sharp heat kernel estimates and Green function estimates are also obtained for censored stable processes (or equivalently, for regional fractional Laplacian) in exterior open sets.  相似文献   

4.
We study functions which are harmonic in the upper half space with respect to (−Δ)α/2, 0<α<2. We prove a Fatou theorem when the boundary function is Lp-Hölder continuous of order β and βp>1. We give examples to show this condition is sharp.  相似文献   

5.
We prove uniqueness of ground state solutions Q = Q(|x|) ≥ 0 of the non-linear equation $$(-\Delta)^s Q+Q-Q^{\alpha+1}= 0 \quad {\rm in} \, \mathbb{R},$$ ( ? Δ ) s Q + Q ? Q α + 1 = 0 i n R , where 0 < s < 1 and 0 < α < 4s/(1?2s) for ${s<\frac{1}{2}}$ s < 1 2 and 0 < α <  for ${s\geq \frac{1}{2}}$ s ≥ 1 2 . Here (?Δ) s denotes the fractional Laplacian in one dimension. In particular, we answer affirmatively an open question recently raised by Kenig–Martel–Robbiano and we generalize (by completely different techniques) the specific uniqueness result obtained by Amick and Toland for ${s=\frac{1}{2}}$ s = 1 2 and α = 1 in [5] for the Benjamin–Ono equation. As a technical key result in this paper, we show that the associated linearized operator L + = (?Δ) s +1?(α+1)Q α is non-degenerate; i.e., its kernel satisfies ker L + = span{Q′}. This result about L + proves a spectral assumption, which plays a central role for the stability of solitary waves and blowup analysis for non-linear dispersive PDEs with fractional Laplacians, such as the generalized Benjamin–Ono (BO) and Benjamin–Bona–Mahony (BBM) water wave equations.  相似文献   

6.
7.
We study the fractional power dissipative equations, whose fundamental semigroup is given by et(−Δ)α with α>0. By using an argument of duality and interpolation, we extend space-time estimates of the fractional power dissipative equations in Lebesgue spaces to the Hardy spaces and the modulation spaces. These results are substantial extensions of some known results. As applications, we study both local and global well-posedness of the Cauchy problem for the nonlinear fractional power dissipative equation ut+(−Δ)αu=|u|mu for initial data in the modulation spaces.  相似文献   

8.
In this paper, the two fractional periodic boundary value problems $$_0^C D_{0 + }^\alpha u\left( t \right) - \lambda u\left( t \right) = f\left( {t,u\left( t \right)} \right), u\left( 0 \right) = u\left( 1 \right), 0 < \alpha < 1,$$ and $$_0^C D_{0 + }^\beta u\left( t \right) - \lambda u\left( t \right) = f\left( {t,u\left( t \right)} \right), u\left( 0 \right) = u\left( 1 \right),u'\left( 0 \right) = 0 1 < \beta < 2,$$ will be studied where 0 C D t α is the ordinary Caputo fractional derivative and λ ∈ ? ?{0}. Under some suitable assumptions on the function f, the existence of at least one mild solution will be proved. Under some conditions, the uniqueness of this mild solution will be proved to both problems. Finally, these mild solutions will be strong solutions under certain conditions.  相似文献   

9.
We take up in this paper the existence of positive continuous solutions for some nonlinear boundary value problems with fractional differential equation based on the fractional Laplacian (-D|D)\fraca2{(-\Delta _{|D})^{\frac{\alpha }{2}}} associated to the subordinate killed Brownian motion process ZaD{Z_{\alpha }^{D}} in a bounded C 1,1 domain D. Our arguments are based on potential theory tools on ZaD{Z_{\alpha }^{D}} and properties of an appropriate Kato class of functions K α (D).  相似文献   

10.
In this paper we introduce higher order numerical methods for solving fractional differential equations. We use two approaches to this problem. The first approach is based on a direct discretisation of the fractional differential operator: we obtain a numerical method for solving a linear fractional differential equation with order 0<α<1. The order of convergence of the numerical method is O(h 3?α ). Our second approach is based on discretisation of the integral form of the fractional differential equation and we obtain a fractional Adams-type method for a nonlinear fractional differential equation of any order α>0. The order of convergence of the numerical method is O(h 3) for α≥1 and O(h 1+2α ) for 0<α≤1 for sufficiently smooth solutions. Numerical examples are given to show that the numerical results are consistent with the theoretical results.  相似文献   

11.
This paper concerns with the existence of solutions for the following fractional Kirchhoff problem with critical nonlinearity:
$${\left( {\int {\int {_{{\mathbb{R}^{2N}}}\frac{{{{\left| {u\left( x \right) - u\left( y \right)} \right|}^2}}}{{{{\left| {x - y} \right|}^{N + 2s}}}}dxdy} } } \right)^{\theta - 1}}{\left( { - \Delta } \right)^s}u = \lambda h\left( x \right){u^{p - 1}} + {u^{2_s^* - 1}} in {\mathbb{R}^N},$$
where (?Δ) s is the fractional Laplacian operator with 0 < s < 1, 2 s * = 2N/(N ? 2s), N > 2s, p ∈ (1, 2 s *), θ ∈ [1, 2 s */2), h is a nonnegative function and λ a real positive parameter. Using the Ekeland variational principle and the mountain pass theorem, we obtain the existence and multiplicity of solutions for the above problem for suitable parameter λ > 0. Furthermore, under some appropriate assumptions, our result can be extended to the setting of a class of nonlocal integro-differential equations. The remarkable feature of this paper is the fact that the coefficient of fractional Laplace operator could be zero at zero, which implies that the above Kirchhoff problem is degenerate. Hence our results are new even in the Laplacian case.
  相似文献   

12.
For 0<p,α<∞, let ‖fp,α be the Lp-norm with respect the weighted measure . We define the weighted Bergman space Aαp(D) consisting of holomorphic functions f with ‖fp,α<∞. For any σ>0, let Aσ(D) be the space consisting of holomorphic functions f in D with . If D has C2 boundary, then we have the embedding Aαp(D)⊂A−(n+α)/p(D). We show that the condition of C2-smoothness of the boundary of D is necessary by giving a counter-example of a convex domain with C1,λ-smooth boundary for 0<λ<1 which does not satisfy the embedding.  相似文献   

13.
The paper deals with the solution of some fractional partial differential equations obtained by substituting modified Riemann-Liouville derivatives for the customary derivatives. This derivative is introduced to avoid using the so-called Caputo fractional derivative which, at the extreme, says that, if you want to get the first derivative of a function you must before have at hand its second derivative. Firstly, one gives a brief background on the fractional Taylor series of nondifferentiable functions and its consequence on the derivative chain rule. Then one considers linear fractional partial differential equations with constant coefficients, and one shows how, in some instances, one can obtain their solutions on by-passing the use of Fourier transform and/or Laplace transform. Later one develops a Lagrange method via characteristics for some linear fractional differential equations with nonconstant coefficients, and involving fractional derivatives of only one order. The key is the fractional Taylor series of non differentiable functionf(x + h) =E α (h α D x α )f(x).  相似文献   

14.
Existence of positive solutions for the nonlinear fractional differential equation Dsu(x)=f(x,u(x)), 0<s<1, has been studied (S. Zhang, J. Math. Anal. Appl. 252 (2000) 804-812), where Ds denotes Riemann-Liouville fractional derivative. In the present work we study existence of positive solutions in case of the nonlinear fractional differential equation:
L(D)u=f(x,u),u(0)=0,0<x<1,  相似文献   

15.
We consider the random variable Zn,α=Y1+2αY2+?+nαYn, with αR and Y1,Y2,… independent and exponentially distributed random variables with mean one. The distribution function of Zn,α is in terms of a series with alternating signs, causing great numerical difficulties. Using an extended version of the saddle point method, we derive a uniform asymptotic expansion for P(Zn,α<x) that remains valid inside (α≥−1/2) and outside (α<−1/2) the domain of attraction of the central limit theorem. We discuss several special cases, including α=1, for which we sharpen some of the results in Kingman and Volkov (2003).  相似文献   

16.
We study fractional integrals on spaces of homogeneous type defined byI α f(x)=∫Xf(y)|B(x,d(x,y))|ga?1dμ(y), 0<α<1. If \(1< p\frac{1}{\alpha },\frac{1}{q} = \frac{1}{p} - \alpha \) , we show that Iαf is of strong type (p,q) and is of weak type ( \(\left( {1,\frac{1}{{1 - \alpha }}} \right)\) ). We also consider the necessary and sufficient conditions on two weights for which Iαf is of weak type (p,q) with respect to (w,v).  相似文献   

17.
It is shown that the second term in the asymptotic expansion as t→0 of the trace of the semigroup of symmetric stable processes (fractional powers of the Laplacian) of order α, for any 0<α<2, in Lipschitz domains is given by the surface area of the boundary of the domain. This brings the asymptotics for the trace of stable processes in domains of Euclidean space on par with those of Brownian motion (the Laplacian), as far as boundary smoothness is concerned.  相似文献   

18.
In this paper we consider the following m-point fractional boundary value problem with p-Laplacian operator on infinite interval where 0<????1, 2<????3, $D_{0+}^{\alpha}$ is the standard Riemann-Liouville fractional derivative, ?? p (s)=|s| p?2 s,p>1, (?? p )?1=?? q , $\frac{1}{p}+\frac{1}{q}=1$ . 0<?? 1<?? 2<?<?? m?2<+??, ?? i ??0, i=1,2,??,m?2 satisfies $0 <\sum_{i=1}^{m-2}\beta_{i}\xi_{i}^{\alpha-1} < \Gamma(\alpha)$ . We establish solvability of the above fractional boundary value problems by means of the properties of the Green function and some fixed-point theorems.  相似文献   

19.
We are concerned with the existence of least energy solutions of nonlinear Schrödinger equations involving the fractional Laplacian
$$\begin{array}{*{20}c} {( - \Delta )^s u(x) + \lambda V(x)u(x) = u(x)^{p - 1} ,} & {u(x) \geqslant 0,} & {x \in \mathbb{R}^N ,} \\ \end{array} $$
for sufficiently large λ, 2 < p < \(\frac{{2N}}{{N - 2s}}\) for N ≥ 2. V (x) is a real continuous function on RN. Using variational methods we prove the existence of least energy solution u λ(x) which localizes near the potential well int V ?1(0) for λ large. Moreover, if the zero sets int V ?1(0) of V (x) include more than one isolated component, then u λ(x) will be trapped around all the isolated components. However, in Laplacian case s = 1, when the parameter λ is large, the corresponding least energy solution will be trapped around only one isolated component and become arbitrarily small in other components of int V ?1(0). This is the essential difference with the Laplacian problems since the operator (?Δ)s is nonlocal.
  相似文献   

20.
In this paper, a meshless collocation method is considered to solve the multi-term time fractional diffusion-wave equation in two dimensions. The moving least squares reproducing kernel particle approximation is employed to construct the shape functions for spatial approximation. Also, the Caputo’s time fractional derivatives are approximated by a scheme of order O(τ 3?α ), 1< α < 2. Stability and convergence of the proposed scheme are discussed. Some numerical examples are given to confirm the efficiency and reliability of the proposed method.  相似文献   

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