2022/04/07 by Jacek Dziubański, Agnieszka Hejna, Dziubański, Jacek +1
Mathematics · #33C52 #35J10 #35K08 #39A70 #43A32 #44A20 #FOS: Mathematics #Functional Analysis (math.FA) #Mathematical Analysis and Transform Methods #Spectral Theory in Mathematical Physics #advanced mathematical theories
paper · pdf · doi:10.48550/arxiv.2204.03443
openalex publication_date 2022/04/07 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
On \mathbb RN equipped with a normalized root system R, a multiplicity function k(α) > 0, and the associated measure dw(\mathbf x)=∏α∈ R|⟨ \mathbf x,α⟩|k(α) d\mathbf x, we consider a Dunkl Schrödinger operator L=-Δk+V, where Δk is the Dunkl Laplace operator and V∈ L1\rm loc (dw) is a non-negative potential. Let ht(\mathbf x,\mathbf y) and k^\V\t(\mathbf x,\mathbf y) denote the Dunkl heat kernel and the integral kernel of the semigroup generated by -L respectively. We prove that k^\V\t(\mathbf x,\mathbf y) satisfies the following heat kernel lower bounds: there are constants C, c>0 such that hct(\mathbf x,\mathbf y)≤ C k^\V\t(\mathbf x,\mathbf y) if and only if sup\mathbf x∈\mathbb RN ∫0^∞ ∫\mathbb RN V(\mathbf y)w(B(\mathbf x,√(t)))-1e-‖\mathbf x-\mathbf y‖2/t dw(\mathbf y) dt