Inequalities relative to two-parameter Vilenkin-Fourier coefficients
Ferenc Weisz (1991)
Studia Mathematica
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Ferenc Weisz (1991)
Studia Mathematica
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Ferenc Weisz (1995)
Studia Mathematica
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Martingale Hardy spaces and BMO spaces generated by an operator T are investigated. An atomic decomposition of the space is given if the operator T is predictable. We generalize the John-Nirenberg theorem, namely, we prove that the spaces generated by an operator T are all equivalent. The sharp operator is also considered and it is verified that the norm of the sharp operator is equivalent to the norm. The interpolation spaces between the Hardy and BMO spaces are identified by...
J. Chao, Lizhong Peng (1996)
Colloquium Mathematicae
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Rodrigo Bañuelos (1987)
Studia Mathematica
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María Jolis (1990)
Publicacions Matemàtiques
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We prove that the class m of continuous martingales with parameter set [0,1], bounded in L, is included in the class of semi-martingales S (L(P)) defined by Allain in [A]. As a consequence we obtain a compact Itô's formula. Finally we relate this result with the compact Itô formula obtained by Sanz in [S] for martingales of m .
D. Hun Hong, M. Ordóñez Cabrera, S. Hak Sung, A. I. Volodin (1999)
Extracta Mathematicae
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Richard Gundy (1969)
Studia Mathematica
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G. Blower (1995)
Studia Mathematica
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Let be a sequence of independent identically distributed random operators on a Banach space. We obtain necessary and sufficient conditions for the Abel means of to belong to Hardy and Lipschitz spaces a.s. We also obtain necessary and sufficient conditions on the Fourier coefficients of random Taylor series with bounded martingale coefficients to belong to Lipschitz and Bergman spaces.
F. Delbaen, W. Schachermayer (1996)
Annales de l'I.H.P. Probabilités et statistiques
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Ferenc Weisz (1996)
Studia Mathematica
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It is shown that the restricted maximal operator of the two-dimensional dyadic derivative of the dyadic integral is bounded from the two-dimensional dyadic Hardy-Lorentz space to (2/3 < p < ∞, 0 < q ≤ ∞) and is of weak type . As a consequence we show that the dyadic integral of a ∞ function is dyadically differentiable and its derivative is f a.e.