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Solving the Boundary Value Problems for Differential Equations with Fractional Derivatives by the Method of Separation of Variables

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Solving the Boundary Value Problems for Differential Equations with Fractional Derivatives by the Method of Separation of Variables mathematics Article Solving the Boundary Value Problems for Differential Equations with Fractional Derivatives by the Method of Separation of Variables Temirkhan Aleroev National Research Moscow State University of Civil Engineering (NRU MGSU), Yaroslavskoe Shosse, 26, 129337 Moscow, Russia; [email protected] Received: 16 September 2020; Accepted: 22 October 2020; Published: 29 October 2020 Abstract: This paper is devoted to solving boundary value problems for differential equations with fractional derivatives by the Fourier method. The necessary information is given (in particular, theorems on the completeness of the eigenfunctions and associated functions, multiplicity of eigenvalues, and questions of the localization of root functions and eigenvalues are discussed) from the spectral theory of non-self-adjoint operators generated by differential equations with fractional derivatives and boundary conditions of the Sturm–Liouville type, obtained by the author during implementation of the method of separation of variables (Fourier). Solutions of boundary value problems for a fractional diffusion equation and wave equation with a fractional derivative are presented with respect to a spatial variable. Keywords: eigenvalue; eigenfunction; function of Mittag–Leffler; fractional derivative; Fourier method; method of separation of variables In memoriam of my Father Sultan and my son Bibulat 1. Introduction Let j(x) L (0, 1). Then the function 2 1 x a d− 1 a 1 a j(x) (x t) − j(t) dt L1(0, 1) dx− ≡ G(a) − 2 Z0 is known as a fractional integral of order a > 0 beginning at x = 0 [1]. Here G(a) is the Euler gamma-function. As is known (see [1]), the function y(x) L (0, 1) is called the fractional derivative 2 1 of the function j(x) L (0, 1) of order a > 0 beginning at x = 0, if 2 1 a d− j(x) = a y(x), dx− which is written da y(x) = j(x). dxa Then da dxa denote the fractional integral for a < 0 and the fractional derivative for a > 0. Mathematics 2020, 8, 1877; doi:10.3390/math8111877 www.mdpi.com/journal/mathematics Mathematics 2020, 8, 1877 2 of 27 Let g n be a set of real numbers satisfying the condition 0 < g 1, (0 j n). We denote f kg0 j ≤ ≤ ≤ k sk = ∑ gj 1; j=0 − k mk = sk + 1 = ∑ gj (0 k n), j=0 ≤ ≤ and assume that 1 n = ∑ gj 1 = sn = mn 1 > 0. r j=0 − − Following M. M. Dzhrbashyan [1], we consider the integro-differential operators d (1 g0) D(s0) j(x) − − j(x), (1 g ) ≡ dx− − 0 d (1 g1) dg0 D(s1) j(x) − − j(x), (1 g ) g0 ≡ dx− − 1 dx d (1 g2) dg1 dg0 D(s2) j(x) − − j(x), (1 g ) g1 g0 ≡ dx− − 2 dx dx ············ d (1 gn) dgn 1 dg0 D(sn) j(x) − − − j(x). (1 gn) gn 1 g0 ≡ dx− − dx − ··· dx We denote Da the operator of fractional integro-differentiation of order a beginning at a R and ax 2 with end at x R of order [a]. By definition we have 2 x sign(x a) f(t)dt − a 1 , a < 0, f(t) L1[a, b], G( a) (x t) − 2 (a) 8 − a − Dax f(t) = R >f(t), a = 0, f(t) L1[a, b], <> 2[a]+1 a [a] 1 sign[a]+1(x a) ¶ D − − f(t), a > 0, f(t) L [a, b], ¶x[a]+1 ax 1 > − 2 > where [a] is the integer part: of a, which satisfies [a] a < [a] + 1, and x [a, b]. ≤ 2 Boundary Value Problems for Differential Equations of Fractional Order The paper is devoted to the method of separation of variables (the Fourier method). This method, which is so widely used in solving boundary value problems for partial differential equations of integer order, until recently remained unsuitable for solving boundary value problems for differential equations with fractional derivatives. The main reason, of course, is that the spectral theory of non-self-adjoint operators generated by the corresponding differential expressions of fractional order and boundary conditions of the Sturm–Liouville type has been supplemented with the necessary information quite recently. Almost all of the author’s papers, to varying degrees, are devoted to the study of the spectral structure of these operators, which constitute the theoretical basis of the method of separation of variables, and the author of this paper, in a sense, summarizes his work in this area. So, in this paper, a method of separation of variables is presented for solving boundary value problems for differential equations with fractional derivatives of the form 2 2 ¶ u ¶ u b = + C Da u + C D u, 0 < a, b < 2, (1) ¶t2 ¶x2 1 0x 0 0t Mathematics 2020, 8, 1877 3 of 27 and ¶u(x, t) = Da u(x, t). ¶t 0+ First of all, we note that anomalous diffusion or dispersion we can describe using the fractional space derivatives, and some processes with ‘memory’ effects-using the fractional time derivatives. It should be noted that depending on the modeled process, the fractional differentiation operators appearing in these equations can be both the Riemann–Liouville fractional differentiation operators and the fractional differentiation operators in the Caputo sense. One of the most important problems in modeling physical processes using differential equations with fractional derivatives is the problem of establishing in what sense the fractional derivative is taken and the identification of the order of this fractional derivative. Undoubtedly, the most significant, fundamental point in the study of boundary value problems for these equations by the method of separation of variables is the question of completeness of systems of eigenfunctions of boundary value problems for the equations L(u; g , g , g , q(x)) = D(s2)u [l + q(x)]u(x) = 0, (2) 0 1 2 − a X00(x) + C1D0xX = lX(x), (3) (these equations arise when the variables are separated in Equations (2) and (3)). Therefore, we present basic results from the spectral theory of operators generated by differential equations of the form (2) and boundary conditions of the Sturm–Liouville type. The relationship between eigenvalues and zeros of a Mittag–Leffler function is shown. The Green’s functions of boundary value problems for equations of the form (2) are considered in detail (it should be noted that these Green’s functions were first obtained by the author in his post-graduate student paper [2]), the study of which made it possible to approach problems of the distribution of zeros of a function of the Mittag type from completely new positions-Leffler and reveal the deeply hidden properties of these functions, which for many years have not been possible for specialists in the theory of functions. First of all, we note that the asymptotic properties of the Mittag–Leffler function have been sufficiently well studied [1], but the study of the non-asymptotic properties of the zeros of the Mittag–Leffler function or, similarly, the eigenvalues of operators generated by boundary value problems for Equation (2), is conjugate with large analytical difficulties (in particular, M. M. Dzhrbashian wrote in [1] that “the question about the completeness of the eigenfunctions of boundary value problems for Equation (2) or a finer question about whether these systems compose a basis in L2(0,1) has a certain interest. However, their solution is apparently associated with significant analytic difficulties”.). Therefore, the author gives these properties in sufficient detail. 2. Boundary Value Problems for the Fractional Order Diffusion Equation In this section we present the necessary information from the spectral theory of operators generated by differential equations of fractional order and boundary conditions of the Sturm–Liouville type. 2.1. Spectral Analysis of Operators, Generated by Fractional Differential Equations of Order More than 1 but Less than 2 and Boundary Conditions of Sturm–Liouville Type and on One Method for Identifying the Order of the Fractional Derivative We devote this subsection to the spectral analysis of two boundary value problems [3,4] x 1 d u0(z) L(u; 1, 1 a, 1, 0) = 1 a dz + lu(x) = 0 − G(a) dx (x z) − Z0 − Mathematics 2020, 8, 1877 4 of 27 u(0) = 0, u(1) = 0, and x 1 a 1 L(u; 1, 1, 1 a, 0) = (x z) − u00(z)dz + lu(x) = 0, − G(a) − Z0 u(0) = 0, u(1) = 0. These problems are the focus of many researchers. First, we note that in [4] (and references therein), the following problem was considered da u00 + l u = 0, 0 < a < 1, (4) dxa u(0) = 0, u(1) = 0. (5) with studying of the spectrum of the operator x a 2 (b) d− d 1 a 1 00 D u = a 2 u = (x z) − u (z)dz, (b = 2 a) dx− dx G(a) − − Z0 (the operator D(s2) transforms to the operator D(b) if g = g = 1 and g = 1 a). 0 1 2 − The operator D(b) arose great interest after F. Mainardi’s paper [3]. In this paper, the following equation was considered x 1 u00(z) g g 1 dz + w u(t) = 0 (6) G(2 g) (t z) − − Z0 − where w is a positive constant and 1 < g < 2, which Mainardi called a fractional oscillatory equation. This paper has been, without exaggeration, very interesting for a lot of researchers. First of all, note that: 1. If l = 0, then any solution u(x) S2[0, 1] (where S2[0, 1] is the class of summable (integrable) on 6 2 [0, 1] functions u(x) including their derivatives of first and second order) for the equation x (b) 1 a 1 D u = (x z) − u00(z)dz = lu (7) G(a) − − Z0 coincides with the solution for Equation (4); 2.
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