Abstract

Let L=−ΔHn+V be a Schrödinger operator on the Heisenberg group Hn, where ΔHn is the sublaplacian on Hn and the nonnegative potential V belongs to the reverse Hölder class RHs with s∈[Q/2,∞). Here Q=2n+2 is the homogeneous dimension of Hn. For given α∈(0,Q), the fractional integral operator associated with the Schrödinger operator L is defined by Iα=L−α/2. In this article, the author introduces the Morrey space Lρ,∞p,κ(Hn) and weak Morrey space WLρ,∞p,κ(Hn) associated with L, where (p,κ)∈[1,∞)×[0,1) and ρ(⋅) is an auxiliary function related to the nonnegative potential V. The relation between the fractional integral operator and the maximal operator on the Heisenberg group is established. From this, the author further obtains the Adams (Morrey-Sobolev) inequality on these new spaces. It is shown that the fractional integral operator Iα=L−α/2 is bounded from Lρ,∞p,κ(Hn) to Lρ,∞q,κ(Hn) with 0<α<Q, 1<p<Q/α, 0<κ<1−(αp)/Q and 1/q=1/p−α/Q(1−κ), and bounded from Lρ,∞1,κ(Hn) to WLρ,∞q,κ(Hn) with 0<α<Q, 0<κ<1−α/Q and 1/q=1−α/Q(1−κ). Moreover, in order to deal with the extreme cases κ≥1−(αp)/Q, the author also introduces the spaces BMOρ,∞(Hn) and Cρ,∞β(Hn), β∈(0,1] associated with L. In addition, it is proved that Iα is bounded from Lρ,∞p,κ(Hn) to BMOρ,∞(Hn) under κ=1−(αp)/Q, and bounded from Lρ,∞p,κ(Hn) to Cρ,∞β(Hn) under κ>1−(αp)/Q and β=α−(1−κ)Q/p.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.