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1.
Lp (\mathbbRn )L^{p} (\mathbb{R}^{n} ) boundedness is considered for the maximal multilinear singular integral operator which is defined by
$T^{*}_{A} f(x) = {\mathop {\sup }\limits_{ \in > 0} }{\left| {{\int_{|x - y| > \in } {\frac{{\Omega (x - y)}} {{|x - y|^{{n + 1}} }}} }(A(x) - A(y) - \nabla A(y)(x - y))f(y)dy} \right|},$T^{*}_{A} f(x) = {\mathop {\sup }\limits_{ \in > 0} }{\left| {{\int_{|x - y| > \in } {\frac{{\Omega (x - y)}} {{|x - y|^{{n + 1}} }}} }(A(x) - A(y) - \nabla A(y)(x - y))f(y)dy} \right|},  相似文献   

2.
Let A k be an integral operator defined by
$ A_k f\left( x \right) = \frac{1} {{K\left( x \right)}}\int_{\Omega _2 } {k\left( {x,y} \right)f\left( y \right)d\mu _2 \left( y \right),} $ A_k f\left( x \right) = \frac{1} {{K\left( x \right)}}\int_{\Omega _2 } {k\left( {x,y} \right)f\left( y \right)d\mu _2 \left( y \right),}   相似文献   

3.
First of all, by studying the existence and stability of traveling wave fronts of the following nonlinear nonlocal model equation
we derive relation between speed index function and stability index function for each of the waves. This model was derived when studying working memory in synaptically coupled neuronal networks, which incorporates low persistent activity rate θ and high saturating rate Θ. We will investigate dynamics of neuronal waves. For this purpose, we will be concerned with the equation for several different kinds of symmetric and asymmetric kernels and will compare speeds of the waves. Our analysis and results on the speed index functions facilitate our investigation on stability of the waves and the estimates of speeds. Secondly, we are concerned with standing waves of the nonlinear nonhomogeneous system of integral-differential equations
and the scalar equation
Dedicated to Professor Yulin Zhou on the occasion of his eighty-fifth birthday.  相似文献   

4.
Fujita exponents for evolution problems with nonlocal diffusion   总被引:1,自引:0,他引:1  
We prove the existence of a critical exponent of Fujita type for the nonlocal diffusion problem
$\left\{{l@{\quad}l}u_t(x, t) = J*u(x, t)-u(x, t) + u^p(x, t), & \qquad x \in \mathbb{R}^N,\; t > 0,\\ u(x, 0) = u_0(x), & \qquad x \in\mathbb{R}^N,\right.$\left\{\begin{array}{l@{\quad}l}u_t(x, t) = J*u(x, t)-u(x, t) + u^p(x, t), & \qquad x \in \mathbb{R}^N,\; t > 0,\\ u(x, 0) = u_0(x), & \qquad x \in\mathbb{R}^N,\end{array}\right.  相似文献   

5.
We study existence and multiplicity of homoclinic type solutions to the following system of diffusion equations on \mathbbR ×W{\mathbb{R}} \times \Omega :
$ \left\{ {{*{20}c} {\,\,{\partial}_t u - {\Delta}_x u + b(t,x) \cdot {\nabla}_x u + V(x)u = H_v (t,x,u,v),} \\ { - {\partial}_t v - {\Delta}_x v - b(t,x) \cdot {\nabla}_x v + V(x)v = H_u (t,x,u,v),}\\ } \right. $ \left\{ {\begin{array}{*{20}c} {\,\,{\partial}_t u - {\Delta}_x u + b(t,x) \cdot {\nabla}_x u + V(x)u = H_v (t,x,u,v),} \\ { - {\partial}_t v - {\Delta}_x v - b(t,x) \cdot {\nabla}_x v + V(x)v = H_u (t,x,u,v),}\\ \end{array} } \right.   相似文献   

6.
7.
We are interested in parabolic problems with L1 data of the type
with i, j=0, 1, (i, j) (0, 0), 0 = 0 and 1 = 1. Here, is an open bounded subset of with regular boundary and is a Caratheodory function satisfying the classical Leray-Lions conditions and is a monotone graph in with closed domain and such that We study these evolution problems from the point of view of semi-group theory, then we identify the generalized solution of the associated Cauchy problem with the entropy solution of in the usual sense introduced in [5].  相似文献   

8.
Let Q 2 = [0, 1]2 be the unit square in two-dimensional Euclidean space ℝ2. We study the L p boundedness of the oscillatory integral operator T α,β defined on the set ℒ(ℝ2+n ) of Schwartz test functions by
$ T_{\alpha ,\beta } f(u,v,x) = \int_{Q^2 } {\frac{{f(u - t,v - s,x - \gamma (t,s))}} {{t^{1 + \alpha _1 } s^{1 + \alpha _2 } }}} e^{it - \beta _{1_s } - \beta _2 } dtds, $ T_{\alpha ,\beta } f(u,v,x) = \int_{Q^2 } {\frac{{f(u - t,v - s,x - \gamma (t,s))}} {{t^{1 + \alpha _1 } s^{1 + \alpha _2 } }}} e^{it - \beta _{1_s } - \beta _2 } dtds,   相似文献   

9.
Let C( \mathbbRm ) C\left( {{\mathbb{R}^m}} \right) be the space of bounded and continuous functions x:\mathbbRm ? \mathbbR x:{\mathbb{R}^m} \to \mathbb{R} equipped with the norm
|| x ||C = || x ||C( \mathbbRm ): = sup{ | x(t) |:t ? \mathbbRm } \left\| x \right\|C = {\left\| x \right\|_{C\left( {{\mathbb{R}^m}} \right)}}: = \sup \left\{ {\left| {x(t)} \right|:t \in {\mathbb{R}^m}} \right\}  相似文献   

10.
We discuss the asymptotic behaviour of the Schrödinger equation ¶¶$ iu_{t} + u_{xx} +i\alpha u -k\sigma(|u|^{2})u\, = f, \;\; x \in \mathbb{R}, \;\; t \geq 0,\;\;\;\alpha,\;k>0 $ iu_{t} + u_{xx} +i\alpha u -k\sigma(|u|^{2})u\, = f, \;\; x \in \mathbb{R}, \;\; t \geq 0,\;\;\;\alpha,\;k>0 ¶¶ with the initial condition u(x,0) = u0 (x) u(x,0) = u_0 (x) . We prove existence of a global attractor in\ H2 (\mathbbR) H^2 (\mathbb{R}) , by using a decomposition of the semigroup in weighted Sobolev spaces to overcome the noncompactness of the classical Sobolev embeddings.  相似文献   

11.
We consider the Cauchy problem for the nonlinear Schrödinger equations $ \begin{array}{l} iu_t + \triangle u \pm |u|^{p-1}u =0, \qquad x \in \mathbb{R}^d, \quad t \in \mathbb{R} \\ u(x,0)= u_0(x), \qquad x \in \mathbb{R}^d \end{array} $ for 1 < p < 1 + 4/d and prove that there is a ${\rho (p ,d) \in (1,2)}We consider the Cauchy problem for the nonlinear Schr?dinger equations
l iut + \triangle u ±|u|p-1u = 0,        x ? \mathbbRd,     t ? \mathbbR u(x,0) = u0(x),        x ? \mathbbRd \begin{array}{l} iu_t + \triangle u \pm |u|^{p-1}u =0, \qquad x \in \mathbb{R}^d, \quad t \in \mathbb{R} \\ u(x,0)= u_0(x), \qquad x \in \mathbb{R}^d \end{array}  相似文献   

12.
It is proved that every two Σ-presentations of an ordered field \mathbbR \mathbb{R} of reals over \mathbbH\mathbbF ( \mathbbR ) \mathbb{H}\mathbb{F}\,\left( \mathbb{R} \right) , whose universes are subsets of \mathbbR \mathbb{R} , are mutually Σ-isomorphic. As a consequence, for a series of functions f:\mathbbR ? \mathbbR f:\mathbb{R} \to \mathbb{R} (e.g., exp, sin, cos, ln), it is stated that the structure \mathbbR \mathbb{R} = 〈R, +, ×, <, 0, 1, f〉 lacks such Σ-presentations over \mathbbH\mathbbF ( \mathbbR ) \mathbb{H}\mathbb{F}\,\left( \mathbb{R} \right) .  相似文献   

13.
In this paper, we investigate the positive solutions to the following integral system with a polyharmonic extension operator on R~+_n:{u(x)=c_n,a∫_?R_+~n(x_n~(1-a_v)(y)/|x-y|~(n-a))dy,x∈R_+~n,v(y)=c_n,a∫_R_+~n(x_n~(1-a_uθ)(x)/|x-y|~(n-a))dx,y∈ ?R_+~n,where n 2, 2-n a 1, κ, θ 0. This integral system arises from the Euler-Lagrange equation corresponding to an integral inequality on the upper half space established by Chen(2014). The explicit formulations of positive solutions are obtained by the method of moving spheres for the critical case κ =n-2+a/n-a,θ =n+2-a/ n-2+a. Moreover,we also give the nonexistence of positive solutions in the subcritical case for the above system.  相似文献   

14.
We study nonnegative solutions of the initial value problem for a weakly coupled system
  相似文献   

15.
The backward heat equation is a typical ill-posed problem. In this paper, we shall apply a dual least squares method connecting Shannon wavelet to the following equation ut (x, y, t) = u xx (x, y, t) + uyy (x, y, t), x ∈ R, y ∈ R, 0 ≤ t 1, u(x, y, 1) = (x, y), x ∈ R, y ∈ R. Motivated by Regińska's work, we shall give two nonlinear approximate methods to regularize the approximate solutions for high-dimensional backward heat equation, and prove that our methods are convergent.  相似文献   

16.
In this paper we consider the following elliptic system in \mathbbR3{\mathbb{R}^3}
$\qquad\left\{{ll}-\Delta u+u+\lambda K(x)\phi u=a(x)|u|^{p-1}u \quad &x \in {\mathbb{R}}^{3}\\ -\Delta \phi=K(x)u^{2} \quad &x \in {\mathbb{R}}^{3}\right.$\qquad\left\{\begin{array}{ll}-\Delta u+u+\lambda K(x)\phi u=a(x)|u|^{p-1}u \quad &x \in {\mathbb{R}}^{3}\\ -\Delta \phi=K(x)u^{2} \quad &x \in {\mathbb{R}}^{3}\end{array}\right.  相似文献   

17.
It is proved that if a function from Lp, p > 1, satisfies the condition $$\frac{1}{{t \cdot \tau }}\int_0^t {\int_0^\tau {\left| {f(x + u,y + v) - f(x,y)} \right|} dudv = O\left( {\left[ {1n\frac{1}{{(t^2 + \tau ^2 )}}} \right]^{ - 2} } \right),}$$ then the double Fourier series of function f, under summation over a rectangle, converges almost everywhere.  相似文献   

18.
This article is a continuation of [J. Math. Sci., 99, No.5, 1541–1547 (2000)] devoted to the validity of the Lax formula (cited in the article of Crandall, Ishii, and Lions [Bull. AMS, 27, No.1, 1–67 (2000)])
for a solution to the Hamilton–Jacobi nonlinear partial differential equation
where the Cauchy data are now a function semicontinuous from below, is the usual norm in , , and is a positive evolution parameter. We proved that the Lax formula solves the Cauchy problem (2) at all points , fixed save for an exceptional set of points R of the F type, having zero Lebesgue measure. In addition, we formulate a similar Lax-type formula without proof for a solution to a new nonlinear equation of the Hamilton–Jacobi-type:
where is a diagonal positive-definite matrix, mentioned in Part I and having interesting applications in modern mathematical physics.  相似文献   

19.
In this article, we study the implication of the primitivity of a matrix near-ring ${\mathbb{M}_n(R) (n >1 )}${\mathbb{M}_n(R) (n >1 )} and that of the underlying base near-ring R. We show that when R is a zero-symmetric near-ring with identity and \mathbbMn(R){\mathbb{M}_n(R)} has the descending chain condition on \mathbbMn(R){\mathbb{M}_n(R)}-subgroups, then the 0-primitivity of \mathbbMn(R){\mathbb{M}_n(R)} implies the 0-primitivity of R. It is not known if this is true when the descending chain condition on \mathbbMn(R){\mathbb{M}_n(R)} is removed. On the other hand, an example is given to show that this is not true in the case of generalized matrix near-rings.  相似文献   

20.
A differential calculus for random fields is developed and combined with the S-transform to obtain an explicit strong solution of the Cauchy problem
Here L is a linear second order elliptic operator, hi and c are real functions, and , where W t is a Brownian motion. An application of the solution to nonlinear filtering and mathematical finance is also considered.  相似文献   

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