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1.
When Hardy-Littlewood maximal operator is bounded on Lp(⋅)(Rn) space we prove θ[Lp(⋅)(Rn),BMO(Rn)]=Lq(⋅)(Rn) where q(⋅)=p(⋅)/(1−θ) and θ[Lp(⋅)(Rn),H1(Rn)]=Lq(⋅)(Rn) where 1/q(⋅)=θ+(1−θ)/p(⋅).  相似文献   

2.
In this paper we establish Lp-boundedness (1<p<∞) for a class of singular convolution operators on the Heisenberg group whose kernels satisfy regularity and cancellation conditions adapted to the implicit (n+1)-parameter structure. The polyradial kernels of this type arose in [A.J. Fraser, An (n+1)-fold Marcinkiewicz multiplier theorem on the Heisenberg group, Bull. Austral. Math. Soc. 63 (2001) 35-58; A.J. Fraser, Convolution kernels of (n+1)-fold Marcinkiewicz multipliers on the Heisenberg group, Bull. Austral. Math. Soc. 64 (2001) 353-376] as the convolution kernels of (n+1)-fold Marcinkiewicz-type spectral multipliers m(L1,…,Ln,iT) of the n-partial sub-Laplacians and the central derivative on the Heisenberg group. Thus they are in a natural way analogous to product-type Calderón-Zygmund convolution kernels on Rn. Here, as in [A.J. Fraser, An (n+1)-fold Marcinkiewicz multiplier theorem on the Heisenberg group, Bull. Austral. Math. Soc. 63 (2001) 35-58; A.J. Fraser, Convolution kernels of (n+1)-fold Marcinkiewicz multipliers on the Heisenberg group, Bull. Austral. Math. Soc. 64 (2001) 353-376], we extend to the (n+1)-parameter setting the methods and results of Müller, Ricci, and Stein in [D. Müller, F. Ricci, E.M. Stein, Marcinkiewicz multipliers and two-parameter structures on Heisenberg groups I, Invent. Math. 119 (1995) 199-233] for the two-parameter setting and multipliers m(L,iT) of the sub-Laplacian and the central derivative.  相似文献   

3.
The function spaces Dk(Rn) are introduced and studied. The definition of these spaces is based on a regularity property for the critical Sobolev spaces Ws,p(Rn), where sp=n, obtained by J. Bourgain, H. Brezis, New estimates for the Laplacian, the div-curl, and related Hodge systems, C. R. Math. Acad. Sci. Paris 338 (7) (2004) 539-543 (see also J. Van Schaftingen, Estimates for L1-vector fields, C. R. Math. Acad. Sci. Paris 339 (3) (2004) 181-186). The spaces Dk(Rn) contain all the critical Sobolev spaces. They are embedded in BMO(Rn), but not in VMO(Rn). Moreover, they have some extension and trace properties that BMO(Rn) does not have.  相似文献   

4.
Following our previous paper [LZ] which deals with the groupU(n, n), we study the structure of certain Howe quotients Ω p,q and Ω p,q (1) which are natural Sp(2n,R) modules arising from the Oscillator representation associated with the dual pair (O(p, q), Sp(2n,R)), by embedding them into the degenerate principal series representations of Sp(2n,R) studied in [L2].  相似文献   

5.
In this paper we consider the so-called p-system with linear damping, and we will prove an optimal decay estimates without any smallness conditions on the initial error. More precisely, if we restrict the initial data (V0,U0) in the space H3(R+)∩L1,γ(R+H2(R+)∩L1,γ(R+), then we can derive faster decay estimates than those given in [P. Marcati, M. Mei, B. Rubino, Optimal convergence rates to diffusion waves for solutions of the hyperbolic conservation laws with damping, J. Math. Fluid Mech. 7 (2) (2005) 224-240; H. Zhao, Convergence to strong nonlinear diffusion waves for solutions of p-system with damping, J. Differential Equations 174 (1) (2001) 200-236] and [M. Jian, C. Zhu, Convergence to strong nonlinear diffusion waves for solutions to p-system with damping on quadrant, J. Differential Equations 246 (1) (2009) 50-77].  相似文献   

6.
It is well known that the commutator Tb of the Calderón-Zygmund singular integral operator is bounded on Lp(Rn) for 1 < p < +∞ if and only if b ∈ BMO [1]. On the other hand, the commutator Tb is bounded from H1(Rn) into L1(Rn) only if the function b is a constant [2]. In this article, we will discuss the boundedness of commutator of certain pseudo-differential operators on Hardy spaces H1. Let Tσ be the operators that its symbol is S01,δ with 0 ≤ δ < 1, if b ∈ LMO, then, the commutator [b, Tσ] is bounded from H1(Rn) into L1(Rn) and from L1(Rn) into BMO(Rn); If [b, Tσ] is bounded from H1(Rn) into L1(Rn) or L1(Rn) into BMO(Rn), then, b ∈ LMOloc.  相似文献   

7.
Let L be the divergence form elliptic operator with complex bounded measurable coefficients, ω the positive concave function on (0,∞) of strictly critical lower type pω∈(0,1] and ρ(t)=t−1/ω−1(t−1) for t∈(0,∞). In this paper, the authors study the Orlicz-Hardy space Hω,L(Rn) and its dual space BMOρ,L*(Rn), where L* denotes the adjoint operator of L in L2(Rn). Several characterizations of Hω,L(Rn), including the molecular characterization, the Lusin-area function characterization and the maximal function characterization, are established. The ρ-Carleson measure characterization and the John-Nirenberg inequality for the space BMOρ,L(Rn) are also given. As applications, the authors show that the Riesz transform ∇L−1/2 and the Littlewood-Paley g-function gL map Hω,L(Rn) continuously into L(ω). The authors further show that the Riesz transform ∇L−1/2 maps Hω,L(Rn) into the classical Orlicz-Hardy space Hω(Rn) for and the corresponding fractional integral Lγ for certain γ>0 maps Hω,L(Rn) continuously into , where is determined by ω and γ, and satisfies the same property as ω. All these results are new even when ω(t)=tp for all t∈(0,∞) and p∈(0,1).  相似文献   

8.
《Quaestiones Mathematicae》2013,36(1-2):237-257
Abstract

N. Dunford and J.T. Schwartz gave a complete characterization of those matrices of (bounded) Fourier multiplier operators acting in L 2(RN) n which are spectral operators, [4; ch. XV]. In the present note this characterization is extended to the setting of LP(G)n , where G is a locally compact abelian group and 1 < p < ∞; see Theorem 2.  相似文献   

9.
In this article, we study a second-order expansion for the effect induced on a large quantum particle which undergoes a single scattering with a low-mass particle via a repulsive point interaction. We give an approximation with third-order error in λ to the map , where GB(L2(Rn)) is a heavy-particle observable, ρB1(Rn) is the density matrix corresponding to the state of the light particle, is the mass ratio of the light particle to the heavy particle, SλB(L2(Rn)⊗L2(Rn)) is the scattering matrix between the two particles due to a repulsive point interaction, and the trace is over the light-particle Hilbert space. The third-order error is bounded in operator norm for dimensions one and three using a weighted operator norm on G.  相似文献   

10.
11.
LetA m ,B m ,m=1, ...,p, be linear operators on ann-dimensional unitary space \(V.L = \sum\limits_{m = 1}^p {A_m \otimes B_m } \) is a linear operator on ?2 V, the tensor product space with the customarily induced inner product. The numerical range ofL is defined as $$W\tfrac{1}{2}(L) = \left\{ {(L)x \otimes y,x \otimes y):x,y o.n.} \right\}$$ where “o.n.” means “orthonormal”. In [1], M.Marcus and B.Y. Wang conjecture: There exists no non-zero operatorL of minimum length less thann for whichW 2 1 (L)=0. In this paper, we prove that this conjecture is true.  相似文献   

12.
We study the operadic and categorical formulations of (conformal) full field algebras. In particular, we show that a grading-restricted R×R-graded full field algebra is equivalent to an algebra over a partial operad constructed from spheres with punctures and local coordinates. This result is generalized to conformal full field algebras over VLVR, where VL and VR are two vertex operator algebras satisfying certain finiteness and reductivity conditions. We also study the geometry interpretation of conformal full field algebras over VLVR equipped with a nondegenerate invariant bilinear form. By assuming slightly stronger conditions on VL and VR, we show that a conformal full field algebra over VLVR equipped with a nondegenerate invariant bilinear form exactly corresponds to a commutative Frobenius algebra with a trivial twist in the category of VLVR-modules. The so-called diagonal constructions [Y.-Z. Huang, L. Kong, Full field algebras, arXiv: math.QA/0511328] of conformal full field algebras are given in tensor-categorical language.  相似文献   

13.
In this paper, the existence of (L2(Rn),L2(Rn))-pullback attractors and (L2(Rn),H1(Rn))-pullback attractors are proved for reaction-diffusion equation in unbounded domains.  相似文献   

14.
For D, a bounded Lipschitz domain in Rn, n ? 2, the classical layer potentials for Laplace's equation are shown to be invertible operators on L2(?D) and various subspaces of L2(?D). For 1 < p ? 2 and data in Lp(?D) with first derivatives in Lp(?D) it is shown that there exists a unique harmonic function, u, that solves the Dirichlet problem for the given data and such that the nontangential maximal function of ▽u is in Lp(?D). When n = 2 the question of the invertibility of the layer potentials on every Lp(?D), 1 < p < ∞, is answered.  相似文献   

15.
A remarkable and much cited result of Bram [J. Bram, Subnormal operators, Duke Math. J. 22 (1955) 75-94] shows that a star-cyclic bounded normal operator in a separable Hilbert space has a cyclic vector. If, in addition, the operator is multiplication by the variable in a space L2(m) (not only unitarily equivalent to it), then it has a cyclic vector in L(m). We extend Bram's result to the case of a general unbounded normal operator, implying by this that the (classical) multiplicity and the multicyclicity of the operator (cf. [N.K. Nikolski, Operators, Functions and Systems: An Easy Reading, vol. 2, Math. Surveys Monogr., vol. 93, Amer. Math. Soc., Providence, 2002]) coincide. It follows that if m is a sigma-finite Borel measure on C (possibly with noncompact support), then there is a nonnegative finite Borel measure τ equivalent to m and such that L2(C,τ) is the norm-closure of the polynomials in z.  相似文献   

16.
By using the Symmetric Mountain Pass Theorem, we establish some existence criteria to guarantee the second-order self-adjoint discrete Hamiltonian system Δ[p(nu(n−1)]−L(n)u(n)+∇W(n,u(n))=0 has infinitely many homoclinic orbits, where nZ, uRN, p,L:ZRN×N and W:Z×RNR are no periodic in n. Our conditions on the potential W(n,x) are rather relaxed.  相似文献   

17.
Ehle [3] has pointed out that then-stage implicit Runge-Kutta (IRK) methods due to Butcher [1] areA-stable in the definition of Dahlquist [2] because they effect the operationR(Ah) whereR(μ) is the diagonal Padé approximation toe µ. The purpose of this note is to point out that ifR(μ)=P(μ)/Q(μ) is a rational polynomial whosen poles are distinct and nonzero, and if degreeP(μ)≦degreeQ(μ)=n, then ann-stage IRK method applied toy=A y can be used for the operation $$y^{n + 1} = R(Ah)y^n $$ This will no longer be of order 2n, nor necessarily the same order as the approximation ofR(Ah) toe Ah. However, if any particularly useful integration formsR can be found, they can be performed by the IRK method.  相似文献   

18.
Akira Saito 《Discrete Mathematics》2009,309(16):5000-1723
We consider 2-factors with a bounded number of components in the n-times iterated line graph Ln(G). We first give a characterization of graph G such that Ln(G) has a 2-factor containing at most k components, based on the existence of a certain type of subgraph in G. This generalizes the main result of [L. Xiong, Z. Liu, Hamiltonian iterated line graphs, Discrete Math. 256 (2002) 407-422]. We use this result to show that the minimum number of components of 2-factors in the iterated line graphs Ln(G) is stable under the closure operation on a claw-free graph G. This extends results in [Z. Ryjá?ek, On a closure concept in claw-free graphs, J. Combin. Theory Ser. B 70 (1997) 217-224; Z. Ryjá?ek, A. Saito, R.H. Schelp, Closure, 2-factors and cycle coverings in claw-free graphs, J. Graph Theory 32 (1999) 109-117; L. Xiong, Z. Ryjá?ek, H.J. Broersma, On stability of the hamiltonian index under contractions and closures, J. Graph Theory 49 (2005) 104-115].  相似文献   

19.
20.
We consider positive functionsh=h(x) defined forxR+0. Conditions for the existence of a power seriesN(x)=∑ cnxn,cn0, with the propertyd1h(x)/N(x)d2, x0,for some constantsd1d2R+, are investigated in [J. Clunie and T. Kövari,Canad. J. Math.20(1968), 7–20; P. Erd s and T. Kövari,Acta Math. Acad. Sci. Hung.7(1956), 305–316; U. Schmid,Complex Variables18(1992), 187–192; U. Schmid, J.Approx. Theory83(1995), 342–346]. In this paper, methods are discussed which allow for a given functionhthe construction of the coefficientscn,n 0, for the above defined power seriesNand to find suitable constantsd1andd2. We also study the power seriesH(x)=∑ xn/un, where we setun=sup{xn/h(x), x0}, forn 0, and the relation betweenhandHconcerning the above stated inequalities.  相似文献   

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