2022/06/29 by Hu, ZhuoRan
#42A38 #42B20 #42B25 #Analysis of PDEs (math.AP) #FOS: Mathematics
paper · doi:10.48550/arxiv.2206.14586
For p>p0=(2λ)/(2λ+1) with λ>0, the Hardy space Hλp(ℝ+2) associated with the Dunkl transform Fλ and the Dunkl operator D on the real line ℝ, where Dxf(x)=f'(x)+\fracλx[f(x)-f(-x)], is the set of functions F=u+iv on the upper half plane ℝ2+=\(x, y): x∈ℝ, y>0\, satisfying λ-Cauchy-Riemann equations: Dxu-∂y v=0, ∂y u +Dxv=0, and supy>0∫ℝ|F(x+iy)|p|x|2λdx<∞ in [7]. Then it is proved in [11] that the real Dunkl-Hardy Spaces Hλp(ℝ) for (1)/(1+γλ)