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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
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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<∞, wW, where Tg is the integration operator
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3.
We consider the following question: given ASL(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 qL2([0,2π]) to , the lift to the universal cover of SL(2,R) of the fundamental matrix map ,
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4.
Let F(z)=∑n=1a(n)qn denote the unique weight 16 normalized cuspidal eigenform on . In the early 1970s, Serre and Swinnerton-Dyer conjectured that
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5.
In this paper, for the multilinear oscillatory singular integral operators TA defined by
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6.
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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7.
8.
Let Tn(A,B,α) denote the class of functions of the form:
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9.
Let (|q|<1). For kN it is shown that there exist k rational numbers A(k,0),…,A(k,k−1) such that
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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:
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11.
Let A1, A2 be algebras and let M:A1A2, M:A2A1 be maps. An elementary map of A1×A2 is an ordered pair (M,M) such that
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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:
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13.
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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14.
15.
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:
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16.
Let A1,…,An be finite subsets of a field F, and let
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17.
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 ΩR3, 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 uL8(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 u0D(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
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19.
Let q?0, p?0, T?∞, D=(0,a), , Ω=D×(0,T), and Lu=xqutuxx. This article considers the following degenerate semilinear parabolic initial-boundary value problem,
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20.
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