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On approach regions for the conjugate Poisson integral and singular integrals

S. FerrandoR. JonesK. Reinhold — 1996

Studia Mathematica

Let ũ denote the conjugate Poisson integral of a function f L p ( ) . We give conditions on a region Ω so that l i m ( v , ε ) ( 0 , 0 ) ( v , ε ) Ω ũ ( x + v , ε ) = H f ( x ) , the Hilbert transform of f at x, for a.e. x. We also consider more general Calderón-Zygmund singular integrals and give conditions on a set Ω so that s u p ( v , r ) Ω | ʃ | t | > r k ( x + v - t ) f ( t ) d t | is a bounded operator on L p , 1 < p < ∞, and is weak (1,1).

Exponential sums with coefficients 0 or 1 and concentrated L p norms

B. AndersonJ. M. AshR. L. JonesD. G. RiderB. Saffari — 2007

Annales de l’institut Fourier

A sum of exponentials of the form f ( x ) = exp 2 π i N 1 x + exp 2 π i N 2 x + + exp 2 π i N m x , where the N k are distinct integers is called an (because the convolution of f with itself is f ) or, simply, an . We show that for every p &gt; 1 , and every set E of the torus 𝕋 = / with | E | &gt; 0 , there are idempotents concentrated on E in the L p sense. More precisely, for each p &gt; 1 , there is an constant C p &gt; 0 so that for each E with | E | &gt; 0 and ϵ &gt; 0 one can find an idempotent f such that the ratio E | f | p / 𝕋 | f | p 1 / p is greater than C p - ϵ . This is in fact a lower bound result and, though optimal, it is close to the...

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