广义分数Hilfer积分及其导数

Pub Date : 2020-12-31 DOI:10.47443/cm.2020.0036
J. E. Valdés
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引用次数: 7

摘要

分数阶微积分是数学的一个分支,主要研究非整数阶的微分和积分算子及其应用。尽管分数阶微积分与经典微积分一样古老,但它仅在近40年才成为数学中最发达的领域之一,这不仅是因为该领域的出版物数量呈指数级增长,而且还因为它的不同应用以及与其他数学领域的重叠。近年来,该领域得到了大力发展,在各个领域都有广泛的应用。经典结果基本上在Riemann-Liouville分数阶导数和Caputo分数阶导数两个基本方向上进行了扩展。由于这一领域的进展,出现了许多分数(全局)和广义(局部)算子。这些新的操作符使研究人员有可能选择最适合他们研究的问题的操作符。读者可以参考论文[2],其中给出了一些理由来证明这些新算子的出现,并讨论了这些算子的应用和理论发展。这些算子是由许多数学家用一个几乎不具体的公式发展起来的,包括Riemann-Liouville (RL), Weyl, Erdelyi-Kober和Hadamard积分,以及Liouville和Katugampola的分数算子。许多作者甚至引入了由一般局部微分算子生成的新的分数算子。在这个方向上,在[19]中定义了广义局部导数,它将合形导数和非合形导数一般化,这是在[7]中提出的广义积分算子的基础,它作为特殊情况包含Riemann - Liouville分数积分(参见[31])。事实上,这些新的操作符需要分类,因为它们可能会引起研究人员的困惑。Baleanu和Fernandez[3]对这些分数型和广义算子进行了相当完整的分类,并提供了丰富的信息和参考资料。为了更完整的回顾,读者可以参考文献[1]的第1章,其中介绍了从Newton到Caputo的微分算子(局部和全局)的历史,并显示了算子之间的质的差异。[1]的1.4节包含了一些我们想要强调的结论:“因此,我们可以得出Riemann-Liouville和Caputo算子不是导数,因此它们不是分数阶导数,而是分数阶算子。”我们同意[27]的结果,即局部分数算子不是分数阶导数”(见[1]中的第24页)。本文给出了Hilfer型的k广义分数阶导数的一个新定义,并研究了它的基本性质。我们还提出了一个用sigmoid函数定义的核的特殊情况。定义gamma函数Γ(见[21,24,28,29])和k-广义gamma函数Γk(见[6])为:
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Generalized fractional Hilfer integral and derivative
Fractional calculus, a branch of mathematics, is focused on the study and applications of the differential and integral operators of non-integer order. Although the fractional calculus is as old as the classical calculus, it has become one of the most developed areas of mathematics only in the last 40 years, not only because of the exponential growth of the number of publications in this area, but also due to its different applications and its overlapping with other areas of mathematics. This area has been developed intensively in recent years and it has found multiple applications in various fields. The classical results were basically extended in two fundamental directions: Riemann–Liouville fractional derivative and Caputo fractional derivative. As a result of the progress made in this area, numerous fractional (global) and generalized (local) operators have been appeared. These new operators give researchers the possibility to choose the one that suits best with the problem they investigate. Readers can consult the paper [2] where some reasons are given to justify the appearance of these new operators and where the applications and theoretical developments of these operators are discussed. These operators, developed by many mathematicians with a hardly specific formulation, include the Riemann–Liouville (RL), Weyl, Erdelyi-Kober and Hadamard integrals, and the fractional operators of Liouville and Katugampola. Many authors have even introduced new fractional operators generated from the general local differential operators. In this direction, a generalized local derivative was defined in [19], which generalizes both the conformable and non-conformable derivatives and that is the basis for the generalized integral operator proposed in [7], which contains as a particular case the fractional integral of Riemann– Liouville (see [31]). In fact, these new operators require a classification as they can cause confusion in researchers. Baleanu and Fernandez [3] gave a fairly complete classification of these fractional and generalized operators together with abundant information and references. For a more complete review, the readers are referred to Chapter 1 of [1], where a history of differential operators (both local and global) from Newton to Caputo is presented and where the qualitative differences between the operators are shown. Section 1.4 of [1] contains some conclusions that we want to highlight: “Therefore, we can conclude that the Riemann–Liouville and Caputo operators are not derivatives and, therefore, they are not fractional derivatives, but fractional operators. We agree with the result [27] that the local fractional operator is not a fractional derivative” (see p.24 in [1]). In this work, we present a new definition of the k-generalized fractional derivative of the Hilfer type, and we study its fundamental properties. We also present a particular case with a kernel defined in terms of the sigmoid function. The gamma function Γ (see [21,24,28,29]) and k-generalized gamma function Γk (see [6]) are defined as:
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