Abstract :
In this paper we develop a theory of singular integral operators acting on function spaces over the measured
metric space (Rd,ρ,γ ), where ρ denotes the Euclidean distance and γ the Gauss measure. Our theory
plays for the Ornstein–Uhlenbeck operator the same rôle that the classical Calderòn–Zygmund theory plays
for the Laplacian on (Rd,ρ,λ), where λ is the Lebesgue measure. Our method requires the introduction of
two new function spaces: the space BMO(γ ) of functions with “bounded mean oscillation” and its predual,
the atomic Hardy space H1(γ ). We show that if p is in (2,∞), then Lp(γ ) is an intermediate space between
L2(γ ) and BMO(γ ), and that an inequality of John–Nirenberg type holds for functions in BMO(γ ).
Then we show that ifMis a bounded operator on L2(γ ) and the Schwartz kernels ofMand of its adjoint
satisfy a “local integral condition of Hörmander type,” thenMextends to a bounded operator from H1(γ )
to L1(γ ), from L∞(γ ) to BMO(γ ) and on Lp(γ ) for all p in (1,∞). As an application, we show that certain
singular integral operators related to the Ornstein–Uhlenbeck operator, which are unbounded on L1(γ )
and on L∞(γ ), turn out to be bounded from H1(γ ) to L1(γ ) and from L∞(γ ) to BMO(γ ).
© 2007 Elsevier Inc. All rights reserved.
Keywords :
Atomic Hardy space , Gauss measure , BMO , Imaginary powers , singular integrals , Riesz transform