7,182 research outputs found

    Molecular Characterizations and Dualities of Variable Exponent Hardy Spaces Associated with Operators

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    Let LL be a linear operator on L2(Rn)L^2(\mathbb R^n) generating an analytic semigroup {eβˆ’tL}tβ‰₯0\{e^{-tL}\}_{t\ge0} with kernels having pointwise upper bounds and p(β‹…):Β Rnβ†’(0,1]p(\cdot):\ \mathbb R^n\to(0,1] be a variable exponent function satisfying the globally log-H\"older continuous condition. In this article, the authors introduce the variable exponent Hardy space associated with the operator LL, denoted by HLp(β‹…)(Rn)H_L^{p(\cdot)}(\mathbb R^n), and the BMO-type space BMOp(β‹…),L(Rn){\mathrm{BMO}}_{p(\cdot),L}(\mathbb R^n). By means of tent spaces with variable exponents, the authors then establish the molecular characterization of HLp(β‹…)(Rn)H_L^{p(\cdot)}(\mathbb R^n) and a duality theorem between such a Hardy space and a BMO-type space. As applications, the authors study the boundedness of the fractional integral on these Hardy spaces and the coincidence between HLp(β‹…)(Rn)H_L^{p(\cdot)}(\mathbb R^n) and the variable exponent Hardy spaces Hp(β‹…)(Rn)H^{p(\cdot)}(\mathbb R^n).Comment: 47 pages, Ann. Acad. Sci. Fenn. Math. (to appear

    Generation of pure, ionic entangled states via linear optics

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    In this paper, we propose a novel scheme to generate two-ion maximally entangled states from either pure product states or mixed states using linear optics. Our new scheme is mainly based on the ionic interference. Because the proposed scheme can generate pure maximally entangled states from mixed states, we denote it as purification-like generation scheme. The scheme does not need a Bell state analyzer as the existing entanglement generation schemes do, it also avoids the difficulty of synchronizing the arrival time of the two scattered photons faced by the existing schemes, thus the proposed new entanglement generation scheme can be implemented more easily in practice.Comment: 6 pages, 4 figure
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