2015
DOI: 10.1007/s10587-015-0226-x
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Atomic decomposition of predictable martingale Hardy space with variable exponents

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Cited by 7 publications
(3 citation statements)
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“…Remark 3. If θ = 0, then we obtain the definitions of [10,12,27]). If we consider the special case θ = 1 and pð•Þ ≡ p with the notations above, we obtain the definitions of H * pÞ , H S pÞ , H s pÞ , Q pÞ , and D pÞ , respectively (see [26]).…”
Section: Martingale Grand Hardy Spaces Via Variable Exponentsmentioning
confidence: 99%
See 1 more Smart Citation
“…Remark 3. If θ = 0, then we obtain the definitions of [10,12,27]). If we consider the special case θ = 1 and pð•Þ ≡ p with the notations above, we obtain the definitions of H * pÞ , H S pÞ , H s pÞ , Q pÞ , and D pÞ , respectively (see [26]).…”
Section: Martingale Grand Hardy Spaces Via Variable Exponentsmentioning
confidence: 99%
“…Since then, the study of martingale Hardy spaces associated with various functional spaces has attracted a steadily increasing interest. For instance, martingale Orlicz-type Hardy spaces were investigated in [3][4][5][6], martingale Lorentz Hardy spaces were studied in [7][8][9], and variable martingale Hardy spaces were developed in [10][11][12][13][14].…”
Section: Introductionmentioning
confidence: 99%
“…In martingale theory, Chao and Ombe [26] introduced the fractional integrals for dyadic martingales. The fractional integrals in this section are defined for more general martingale setting as in [13,14] (see also [15,[27][28][29][30][31][32]).…”
Section: The Fractional Integral Operatormentioning
confidence: 99%