30,755 research outputs found

    On lpl^p -multipliers of functions analytic in the disk

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    We consider bounded analytic functions in domains generated by sets that have Littlewood--Paley property. We show that each such function is an lpl^p -multiplier.Comment: 6 pages, minor modification on page 2 is made to improve clarit

    Thickness conditions and Littlewood--Paley sets

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    We consider sets in the real line that have Littlewood--Paley properties LP(p)\mathrm{LP}(p) or LP\mathrm{LP} and study the following question: How thick can these sets be?Comment: 15 pages, v2 has minor modifications to improve clarity, typos remove

    Absolutely convergent Fourier series. An improvement of the Beurling--Helson theorem

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    We consider the space A(T)A(\mathbb T) of all continuous functions ff on the circle T\mathbb T such that the sequence of Fourier coefficients f^={f^(k), kZ}\hat{f}=\{\hat{f}(k), ~k \in \mathbb Z\} belongs to l1(Z)l^1(\mathbb Z). The norm on A(T)A(\mathbb T) is defined by fA(T)=f^l1(Z)\|f\|_{A(\mathbb T)}=\|\hat{f}\|_{l^1(\mathbb Z)}. According to the known Beurling--Helson theorem, if ϕ:TT\phi : \mathbb T\rightarrow\mathbb T is a continuous mapping such that einϕA(T)=O(1), nZ,\|e^{in\phi}\|_{A(\mathbb T)}=O(1), ~n\in\mathbb Z, then ϕ\phi is linear. It was conjectured by Kahane that the same conclusion about ϕ\phi is true under the assumption that einϕA(T)=o(logn)\|e^{in\phi}\|_{A(\mathbb T)}=o(\log |n|). We show that if einϕA(T)=o((loglogn/logloglogn)1/12)\|e^{in\phi}\|_{A(\mathbb T)}=o((\log\log |n|/\log\log\log |n|)^{1/12}) then ϕ\phi is linear.Comment: A typo on page 14 line 4 is corrected. A typo on page 16 line 5 is corrected. Notation in the proof of Lemma 2 are replaced with more readable one

    B Decays as a Probe of Spontaneous CP-Violation in SUSY Models

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    We consider phenomenological implications of susy models with spontaneously broken CP-symmetry. In particular, we analyze CP-asymmetries in B decays and find that the predictions of these models are vastly different from those of the SM. These features are common to NMSSM-like models with an arbitrary number of sterile superfields and the MSSM with broken R-parity.Comment: Talk given at SUSY'99, 14-19 June, Fermilab, Batavia, I
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