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1.
Consider an operator T:C2(R)→C(R) and isotropic maps A1,A2:C1(R)→C(R) such that the functional equation
2.
We completely describe those positive Borel measures μ in the unit disc D such that the Bergman space Ap(w)⊂Lq(μ), 0<p,q<∞, where w belongs to a large class W of rapidly decreasing weights which includes the exponential weights , α>0, and some double exponential type weights.As an application of that result, we characterize the boundedness and the compactness of Tg:Ap(w)→Aq(w), 0<p,q<∞, w∈W, where Tg is the integration operator
3.
We consider the following question: given A∈SL(2,R), which potentials q for the second order Sturm-Liouville problem have A as its Floquet multiplier? More precisely, define the monodromy map μ taking a potential q∈L2([0,2π]) to , the lift to the universal cover of SL(2,R) of the fundamental matrix map ,
4.
Matthew Boylan 《Journal of Number Theory》2003,98(2):377-389
Let F(z)=∑n=1∞a(n)qn denote the unique weight 16 normalized cuspidal eigenform on . In the early 1970s, Serre and Swinnerton-Dyer conjectured that
5.
Huoxiong Wu 《Journal of Mathematical Analysis and Applications》2004,296(2):479-494
In this paper, for the multilinear oscillatory singular integral operators TA defined by
6.
Xiongping Dai 《Journal of Differential Equations》2006,225(2):549-572
In this paper, the author considers, by Liao methods, the stability of Lyapunov exponents of a nonautonomous linear differential equations: with linear small perturbations. It is proved that, if A(t) is a upper-triangular real n by n matrix-valued function on R+, continuous and uniformly bounded, and if there is a relatively dense sequence in R+, say 0=T0<T1<?<Ti<?, such that
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8.
Ding-Gong Yang 《Applied mathematics and computation》2010,215(9):3473-3481
Let Tn(A,B,α) denote the class of functions of the form:
9.
Let (|q|<1). For k∈N it is shown that there exist k rational numbers A(k,0),…,A(k,k−1) such that
10.
For finite subsets A1,…,An of a field, their sumset is given by . In this paper, we study various restricted sumsets of A1,…,An with restrictions of the following forms:
11.
Pengtong Li 《Journal of Mathematical Analysis and Applications》2006,320(1):174-191
Let A1, A2 be algebras and let M:A1→A2, M∗:A2→A1 be maps. An elementary map of A1×A2 is an ordered pair (M,M∗) such that
12.
Let 1 ? p ? ∞, 0 < q ? p, and A = (an,k)n,k?0 ? 0. Denote by Lp,q(A) the supremum of those L satisfying the following inequality:
13.
U.-W. Schmincke 《Journal of Mathematical Analysis and Applications》2003,277(1):51-78
Starting from a selfadjoint Schrödinger operator A=−d2/dx2+q with a gap G in its spectrum F. Gesztesy, B. Simon, G. Teschl [J. Analyse Math. 70 (1996) 267-324] succeed in constructing another Schrödinger operator that is unitarily equivalent (and thus isospectral) to A. As the means they apply come from the Weyl-Titchmarsh theory the connections prove to be intricate, in particular the relation between A and . We show that a central assertion in GST's paper rests substantially on factorizations of the form
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María Burgos Moisés Villegas-Vallecillos 《Journal of Mathematical Analysis and Applications》2009,359(1):1-117
Let T:Lip0(X)→Lip0(Y) be a surjective map between pointed Lipschitz ∗-algebras, where X and Y are compact metric spaces. On the one hand, we prove that if T satisfies the non-symmetric norm ∗-multiplicativity condition:
16.
Hao Pan 《Journal of Combinatorial Theory, Series A》2009,116(8):1374-1381
Let A1,…,An be finite subsets of a field F, and let
17.
Reinhard Farwig Hermann Sohr 《Nonlinear Analysis: Theory, Methods & Applications》2010,73(6):1459-1465
There are only very few results on the existence of unique local in time strong solutions of the Navier-Stokes equations for completely general domains Ω⊆R3, although domains with edges and corners, bounded or unbounded, are very important in applications. The reason is that the Lq-theory for the Stokes operator A is available in general only in the Hilbert space setting, i.e., with q=2. Our main result for a general domain Ω is optimal in a certain sense: Consider an initial value and a zero external force. Then the condition is sufficient and necessary for the existence of a unique local strong solution u∈L8(0,T;L4(Ω)) in some interval [0,T), 0<T≤∞, with u(0)=u0, satisfying Serrin’s condition . Note that Fujita-Kato’s sufficient condition u0∈D(A1/4) is strictly stronger and therefore not optimal. 相似文献
18.
Let A1,…,AN be complex self-adjoint matrices and let ρ be a density matrix. The Robertson uncertainty principle
19.
Nadejda E. Dyakevich 《Journal of Mathematical Analysis and Applications》2008,338(2):892-901
Let q?0, p?0, T?∞, D=(0,a), , Ω=D×(0,T), and Lu=xqut−uxx. This article considers the following degenerate semilinear parabolic initial-boundary value problem,