s和s型空间中某些微分算子方程的非定域时间问题

S. Bodnaruk, V. Gorodetskyi, R. Kolisnyk, N. Shevchuk
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引用次数: 0

摘要

在分数阶积分微分理论中,经常使用算子$A := \displaystyle \Big(I-\frac{\partial^2}{\partial x^2}\Big)$。这个算子叫做分数阶微分的贝塞尔算子$ 1/2 $的阶。本文研究了算子$B := \displaystyle \Big(I-\frac{\partial^2}{\partial x^2}+\frac{\partial^4}{\partial x^4}\Big)$的性质,它可以理解为算子$A$的某种类似物。建立了$B$是Hilbert空间$L_2(\mathbb{R})$中的自共轭算子,将其缩小到某个$S$类型的空间(这种空间在\cite{lit_bodn_2}中介绍)与由函数符号$a(\sigma) = (1+\sigma^2+\sigma^4)^{1/4}$、$\sigma \in \mathbb{R}$(这里$F$、$F^{-1}$是傅里叶变换)构造的伪微分算子$F_{\sigma \to x}^{-1}[a(\sigma) F_{x\to \sigma}]$相匹配。这种方法使我们能够有效地应用傅里叶变换方法来研究具有特定算子的演化方程的非局部随时间问题的正确可解性。当给定非局部条件的初始函数是Gevrey超分布型广义函数空间中的一个元素时,建立了给定方程的正确可解性。研究了该问题的基本解的性质,给出了其解的卷积形式。
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NONLOCAL BY TIME PROBLEM FOR SOME DIFFERENTIAL-OPERATOR EQUATION IN SPACES OF S AND S TYPES
In the theory of fractional integro-differentiation the operator $A := \displaystyle \Big(I-\frac{\partial^2}{\partial x^2}\Big)$ is often used. This operator called the Bessel operator of fractional differentiation of the order of $ 1/2 $. This paper investigates the properties of the operator $B := \displaystyle \Big(I-\frac{\partial^2}{\partial x^2}+\frac{\partial^4}{\partial x^4}\Big)$, which can be understood as a certain analogue of the operator $A$. It is established that $B$ is a self-adjoint operator in Hilbert space $L_2(\mathbb{R})$, the narrowing of which to a certain space of $S$ type (such spaces are introduced in \cite{lit_bodn_2}) matches the pseudodifferential operator $F_{\sigma \to x}^{-1}[a(\sigma) F_{x\to \sigma}]$ constructed by the function-symbol $a(\sigma) = (1+\sigma^2+\sigma^4)^{1/4}$, $\sigma \in \mathbb{R}$ (here $F$, $F^{-1}$ are the Fourier transforms). This approach allows us to apply effectively the Fourier transform method in the study of the correct solvability of a nonlocal by time problem for the evolution equation with the specified operator. The correct solvability for the specified equation is established in the case when the initial function, by means of which the nonlocal condition is given, is an element of the space of the generalized function of the Gevrey ultradistribution type. The properties of the fundamental solution of the problem was studied, the representation of the solution in the form of a convolution of the fundamental solution of the initial function is given.
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