Abstract:In this paper we develop a time-fractional operator calculus in fractional Clifford analysis. Initially we study the Lp-integrability of the fundamental solutions of the multi-dimensional time-fractional diffusion operator and the associated time-fractional parabolic Dirac operator. Then we introduce the time-fractional analogues of the Teodorescu and Cauchy-Bitsadze operators in a cylindrical domain, and we investigate their main mapping properties. As a main result, we prove a time-fractional version of the … Show more
“…Throughout the paper, we show that we can always re-obtain the results of the classical function theory for the Dirac operator when switching to the limit case when = (1, … , 1). The analogous of the results presented in this paper for the case of the time-fractional parabolic Dirac operator can be found in Ferreira et al 21 The structure of the paper reads as follows. In the Section 2, we recall some basic definitions from the fractional calculus, special functions, and Clifford analysis.…”
Section: Introductionmentioning
confidence: 52%
“…We give a direct proof of the theorem in order to confirm that (34) is indeed the solution of (21). The proof uses the fact that C a + 1 1+ 1…”
Section: Theorem 4 a Family Of Eigenfunctions Of The Fractional Laplmentioning
confidence: 97%
“…Throughout the paper, we show that we can always re‐obtain the results of the classical function theory for the Dirac operator when switching to the limit case when α = (1,…,1). The analogous of the results presented in this paper for the case of the time‐fractional parabolic Dirac operator can be found in Ferreira et al…”
In this paper, we develop a fractional integro‐differential operator calculus for Clifford algebra‐valued functions. To do that, we introduce fractional analogues of the Teodorescu and Cauchy‐Bitsadze operators, and we investigate some of their mapping properties. As a main result, we prove a fractional Borel‐Pompeiu formula based on a fractional Stokes formula. This tool in hand allows us to present a Hodge‐type decomposition for the fractional Dirac operator. Our results exhibit an amazing duality relation between left and right operators and between Caputo and Riemann‐Liouville fractional derivatives. We round off this paper by presenting a direct application to the resolution of boundary value problems related to Laplace operators of fractional order.
“…Throughout the paper, we show that we can always re-obtain the results of the classical function theory for the Dirac operator when switching to the limit case when = (1, … , 1). The analogous of the results presented in this paper for the case of the time-fractional parabolic Dirac operator can be found in Ferreira et al 21 The structure of the paper reads as follows. In the Section 2, we recall some basic definitions from the fractional calculus, special functions, and Clifford analysis.…”
Section: Introductionmentioning
confidence: 52%
“…We give a direct proof of the theorem in order to confirm that (34) is indeed the solution of (21). The proof uses the fact that C a + 1 1+ 1…”
Section: Theorem 4 a Family Of Eigenfunctions Of The Fractional Laplmentioning
confidence: 97%
“…Throughout the paper, we show that we can always re‐obtain the results of the classical function theory for the Dirac operator when switching to the limit case when α = (1,…,1). The analogous of the results presented in this paper for the case of the time‐fractional parabolic Dirac operator can be found in Ferreira et al…”
In this paper, we develop a fractional integro‐differential operator calculus for Clifford algebra‐valued functions. To do that, we introduce fractional analogues of the Teodorescu and Cauchy‐Bitsadze operators, and we investigate some of their mapping properties. As a main result, we prove a fractional Borel‐Pompeiu formula based on a fractional Stokes formula. This tool in hand allows us to present a Hodge‐type decomposition for the fractional Dirac operator. Our results exhibit an amazing duality relation between left and right operators and between Caputo and Riemann‐Liouville fractional derivatives. We round off this paper by presenting a direct application to the resolution of boundary value problems related to Laplace operators of fractional order.
“…This implies that ⃗ T 1,Ω is a right inverse of the divergence operator and has vanishing rotational (see proposition 3.2 in Delgado and Porter [11]). In the next result, we will apply the above solution to four specific div-curl systems derived from (20). Moreover, we will construct functions in ker D +…”
In this manuscript, we characterize the kernel of the parabolic Dirac operator in an explicit way. More precisely, we will show that the members of this kernel equivalently satisfy a generalized div‐curl system. Furthermore, it will be established that it is sufficient to know four scalar solutions of the heat equation to construct explicitly a
‐valued function with 16 components belonging to the kernel of the parabolic Dirac operator. Some additional inherited properties of the heat equation are derived in this work along with concrete examples.
“…Fractional hyperholomorphic function theory is a very recent topic of research, see [4,6,7,10,11,16,20,28] for more details. In particular, the interest for considering fractional Laplace and Dirac type operators is devoted in [1,2,8,9,21].…”
Quaternionic analysis offers a function theory focused on the concept of ψ−hyperholomorphic functions defined as null solutions of the ψ−Fueter operator, where ψ is an arbitrary orthogonal base (called structural set) of H 4 .The main goal of the present paper is to extend the results given in [12], where a fractional ψ−hyperholomorphic function theory was developed. We introduce a quaternionic perturbed fractional ψ−Fueter operator calculus, where Stokes and Borel-Pompeiu formulas in this perturbed fractional ψ−Fueter setting are presented.
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