Linear finite functional in the weighted Sobolev space

IF 0.3 Q4 MECHANICS
Igor K. Korytov
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引用次数: 0

Abstract

In this paper, a representation of a linear functional in the weighted Sobolev space is obtained. The space is normed without use of pseudodifferential operators. The norm contains partial derivatives of all intermediate orders of the test function. The Sobolev space is considered to be of non-Hilbert type. First, we deduce the representation of linear functional via a boundary element of the test space. The boundary element corresponds to the given functional. This way, referring to Clarkson’s inequalities, we prove the uniqueness of the boundary element. Then, to obtain a condition for the boundary element, we differentiate the function built based on the norm. The result leads to a representation of an arbitrary linear functional via the boundary element. When considering the boundary element as unknown, the representation performs as a nonlinear differential equation. Second, we consider a finite linear functional. The extreme function of such a functional was built in our earlier papers. The extreme function is expressed via convolution of the fundamental solution of a linear partial differential equation with a given functional. The functional performs as a distribution in the convolution. Convolution exists if the linear functional is finite. Using this fact, we prove that the representation of a finite linear functional via the boundary element is identical to the representation via the extreme function.
加权Sobolev空间中的线性有限泛函
本文给出了加权Sobolev空间中线性泛函的表示形式。该空间在不使用伪微分算子的情况下归范。范数包含测试函数所有中间阶的偏导数。Sobolev空间被认为是非hilbert型的。首先,我们通过测试空间的边界元素推导出线性泛函的表示。边界元对应于给定的泛函。这样,参考克拉克森不等式,我们证明了边界元的唯一性。然后,对基于范数建立的函数进行微分,得到边界元存在的条件。结果导致通过边界元素的任意线性泛函的表示。当考虑边界元素为未知时,表示为非线性微分方程。其次,我们考虑一个有限线性泛函。这种泛函的极值函数在我们以前的文章中已经建立了。极值函数是通过线性偏微分方程的基本解与给定泛函的卷积来表示的。函数在卷积中表现为一个分布。如果线性泛函是有限的,则存在卷积。利用这一事实,我们证明了有限线性泛函的边界元表示与极值函数表示是相同的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
CiteScore
0.90
自引率
66.70%
发文量
0
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