2015
DOI: 10.1007/s00041-015-9453-7
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$$L^{p}(\mu ) \rightarrow L^{q}(\nu )$$ L p ( μ ) → L q ( ν ) Characterization for Well Localized Operators

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Cited by 13 publications
(15 citation statements)
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“…Very interesting recent papers [20], [21] give necessary and sufficient conditions for the two weight estimates of the well localized operators and of the Haar shifts, but again the conditions were more restrictive than the Sawyer type ones: again, for each interval I one has to check the roundedness on infinitely many vector-valued functions.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…Very interesting recent papers [20], [21] give necessary and sufficient conditions for the two weight estimates of the well localized operators and of the Haar shifts, but again the conditions were more restrictive than the Sawyer type ones: again, for each interval I one has to check the roundedness on infinitely many vector-valued functions.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…The definition of a well localized operator depends on a parameter r which measures how "well" the operator is localized. The constant C in the two weight inequality proved in [14] and [17] depends on r and the constants in the Sawyer type testing conditions. In [7] the dyadic shifts were looked at from a little different perspective.…”
Section: Introductionmentioning
confidence: 98%
“…Operators of interest are the maximal function [S1, Moe, PzR, V], fractional and Poisson integrals [S2,Cr], the Hilbert transform [CS1,CS2,KP,NTV1,LSSU,L3] and general Calderón-Zygmund singular integral operators and their commutators [CrRV,CrMoe,CrMPz2,NRTV], the square functions [LLi1,LLi2,CLiX,HLi], paraproducts and their dyadic counterparts [M,HoLWic1,HoLWic2,IKP,Be3]. Necessary and sufficient conditions are only known for the maximal function, fractional and Poisson integrals [S1], square functions [LLi1] and the Hilbert transform [L3,LSSU], and among the dyadic operators for the martingale transform, the dyadic square functions, positive and well localized dyadic operators [Wil1,NTV1,NTV3,T,Ha,HaHLi,HL,LSU2,Ta,Vu1,Vu2]. If the weights u and v are assumed to be in A d 2 , then necessary and sufficient conditions for boundedness of dyadic paraproducts and commutators in terms of Bloom's BM O are known [HoLWic1,HoLWic2].…”
Section: Introductionmentioning
confidence: 99%