Abstract
Let \({p : \mathbb{C} \to \mathbb{R}}\) be a subharmonic, nonharmonic polynomial and \({\tau \in \mathbb{R}}\) a parameter. Define \(\bar{Z}_{\tau p} = \frac{\partial}{\partial\bar{z}} + \tau\frac{\partial p}{\partial \bar{z}} = e^{-\tau p}\frac{\partial}{\partial\bar{z}} e^{\tau p}\) , a closed, densely defined operator on \({L^2(\mathbb{C})}\) . If \({\square}_{\tau p}=\bar{Z}_{\tau p}\bar{Z}_{\tau p}^{*}\) and \({\square}_{\tau p}=\bar{Z}_{\tau p}^{*}\bar{Z}_{\tau p}\) , we solve the heat equations \({\partial_s u + \tilde{\square}_{\tau p} u=0}\) , u(0,z) = f(z) and \({\partial_s \tilde{u} + \tilde{\square}_{\tau p} \tilde{u}=0}\) , \({\tilde{u}(0,z) = \tilde{f}(z)}\) . We write the solutions via heat semigroups and show that the solutions can be written as integrals against distributional kernels. We prove that the kernels are C ∞ off of the diagonal {(s, z, w) : s = 0 and z = w} and find pointwise bounds for the kernels and their derivatives.
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Raich, A. Pointwise estimates for relative fundamental solutions of heat equations in \({\mathbb{R} \times \mathbb{C}}\) . Math. Z. 256, 193–220 (2007). https://doi.org/10.1007/s00209-006-0065-4
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DOI: https://doi.org/10.1007/s00209-006-0065-4
Keywords
- Gaussian decay
- Fundamental solution
- Heat semigroup
- Schrödinger operator
- Polynomial model
- Domains of finite type
- Unbounded weakly pseudoconvex domains