论文标题

Octonionic Kerzman-Stein操作员

Octonionic Kerzman-Stein operators

论文作者

Constales, Denis, Kraußhar, Rolf Sören

论文摘要

在本文中,我们考虑了与任意Lipschitz域相关的八元离子设置中的广义强化空间,在这些环境中,单位正常场几乎到处都存在。首先,我们讨论一些基本属性,并解释关联Clifford分析设置的结构差异。非缔合性需要特别注意适当的内部产品,因此在广义szegö投影的定义中。每当我们想从复制内核希尔伯特空间中应用经典定理时,我们首先需要切换到RIESZ表示定理所拥有的实用值的内部产品。然后,我们引入了对八元离子单基因函数的双重cauchy变换的概括,该函数代表了相对于实值的内部产品$ \ langle \ cdot,\ cdot \ rangle_0 $以及关联的八元电动的kerzman-stein操作员和相关的核功能。 同样在Octonionic设置中,我们引入的Kerzman-Stein操作员证明是一个紧凑的操作员。这种方法背后的一种动机是找到一种近似方法来计算八元离子单基因函数的szegö投影,从而在八元元素中解决了BVP的可能性,而没有明确了解Octonionicszegökernel的明确了解,这通常很难确定。我们还讨论了八元离子单位球和半空间的特殊情况。最后,我们将我们的八世代Kerzman-Stein操作员与希尔伯特的转型联系起来,尤其是在半空间中的希尔伯特·里兹变换。

In this paper we consider generalized Hardy spaces in the octonionic setting associated to arbitrary Lipschitz domains where the unit normal field exists almost everywhere. First we discuss some basic properties and explain structural differences to the associative Clifford analysis setting. The non-associativity requires special attention in the definition of an appropriate inner product and hence in the definition of a generalized Szegö projection. Whenever we want to apply classical theorems from reproducing kernel Hilbert spaces we first need to switch to the consideration of real-valued inner products where the Riesz representation theorem holds. Then we introduce a generalization of the dual Cauchy transform for octonionic monogenic functions which represents the adjoint transform with respect to the real-valued inner product $\langle \cdot, \cdot \rangle_0$ together with an associated octonionic Kerzman-Stein operator and related kernel functions. Also in the octonionic setting, the Kerzman-Stein operator that we introduce turns out to be a compact operator. A motivation behind this approach is to find an approximative method to compute the Szegö projection of octonionic monogenic functions offering a possibility to tackle BVP in the octonions without the explicit knowledge of the octonionic Szegö kernel which is extremely difficult to determine in general. We also discuss the particular cases of the octonionic unit ball and the half-space. Finally, we relate our octonionic Kerzman-Stein operator to the Hilbert transform and particularly to the Hilbert-Riesz transform in the half-space case.

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