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Theory and Modern Applications

Fractional order of Legendre-type matrix polynomials


Recently, special functions of fractional order calculus have had many applications in various areas of mathematical analysis, physics, probability theory, optimization theory, graph theory, control systems, earth sciences, and engineering. Very recently, Zayed et al. (Mathematics 8:136, 2020) introduced the shifted Legendre-type matrix polynomials of arbitrary fractional orders and their various applications utilizing Rodrigues matrix formulas. In this line of research, we use the fractional order of Rodrigues formula to provide further investigation on such Legendre polynomials from a different point of view. Some properties, such as hypergeometric representations, continuation properties, recurrence relations, and differential equations, are derived. Moreover, Laplace’s first integral form and orthogonality are obtained.

1 Introduction

The recent advances in fractional order calculus (FOC) are dominated by its multidisciplinary applications. Undoubtedly, fractional calculus has become an exciting new mathematical approach to solving various problems in mathematics, model physical, engineering, and many branches of science (see, for example, [27] and the references therein). The “special functions of fractional order calculus” (SF of FOC) as generalized fractional calculus operators of some classical special functions were found by Kiryakova [8, 9] and Agarwal [2]. Recently, there has been an increasing interest to use classes of special functions, referred to as (SF of FOC), that play most important role in the theory of differentiation and integration of arbitrary order (i.e. FC) and appear as solutions of fractional order differential equations and systems (see e.g. [1015]).

On the contrary, the mainstream and, perhaps, the most effective approach to the field of special functions of matrix argument is the fractional calculus approach, recently presented in the fundamental works (for instance, see [1619]). Analogous to the classical case, it is also noticed that Rodrigues matrix formula is a useful approach to define a sequence of orthogonal matrix polynomials (see [1, 2025]). This approach allows establishing many interesting properties of the matrix polynomials. Moreover, these generalized matrix formulas allow to define new classes of special matrix functions and matrix polynomials and to include fractional order differentiation.

The Legendre polynomials are used by mathematicians and engineers for a variety of mathematical and numerical solutions. For example, Legendre and associate Legendre polynomials are widely used in the determination of wave functions of electrons in the orbits of an atom [26] and in the determination of potential functions in the spherically symmetric geometry [27], etc. The Legendre polynomials are applicable in fluid dynamics to study the flow around the outside of a puff of hot gas rising through the air, see for details [28, 29]. For readers, they can find other applications of these polynomials in [3035]. Later on, a new kind of the Legendre matrix polynomials was introduced by Upadhyaya and Shehata [36, 37]. Within the frame, they discussed some fundamental properties and applications of these matrix polynomials. Motivated by certain recent extensions of the shifted Legendre-type matrix polynomials of arbitrary fractional orders utilizing Rodrigues matrix formulas [1], we introduce and examine some properties of the fractional order of Legendre-type matrix polynomials generated by fractional analogues of the Rodrigues-type formulas of these polynomials. The paper is organized, as follows: Sect. 2 includes the basic definitions and properties used in the following sections. In Sect. 3, we define the Legendre-type matrix polynomials of arbitrary fractional orders. The section also includes the hypergeometric matrix representations and establish that these Legendre-type matrix polynomials are continuous functions of arbitrary fractional orders. Recurrence relations and development of second-order matrix differential equations satisfied by these polynomials are provided in Sect. 4. Laplace’s first integral form and the orthogonality of Legendre-type matrix polynomials of arbitrary fractional orders are proved in Sect. 5. We reach the conclusion in Sect. 6.

2 Preliminaries

In this section, we recall some definitions and terminologies which will be used to prove the main results in the next sections.

Definition 2.1

A matrix D, in the space of complex matrices \(\mathbb{C}^{N\times N}\), is called positive stable [25] if

$$ \mathbf{Re}(z)>0, \quad z\in \sigma (D), $$

where \(\sigma (D)\) is the spectrum of matrix D.

Definition 2.2

Let D be a positive stable matrix in \(\mathbb{C}^{N\times N}\). The gamma matrix function \(\Gamma (D)\) is defined in [25] as follows:

$$ \Gamma (D)= \int _{0}^{\infty }e^{-z}z^{D-I} \,dz; \quad z^{D-I}= \exp \bigl((D-I)\ln {z}\bigr). $$

Definition 2.3


For all D in \(\mathbb{C}^{N\times N}\), we assume

$$ D+nI \text{ is invertible for all } n\in \mathbb{N}_{0}:= \mathbb{N}\cup \{0\}, $$

and the Pochhammer symbol (the shifted factorial) is defined by

$$ (D)_{n}=D(D+I)\cdots\bigl(D+(n-1)I\bigr)=\Gamma {(D+nI)}\Gamma ^{-1}{(D)};\qquad (D)_{0}\equiv I, $$

where I is an identity matrix in \(\mathbb{C}^{N\times N}\).

Lemma 2.1

(Lancaster [38])

Let D be a matrix in \(\mathbb{C}^{N\times N}\)such that \(\|D\| < 1\)and \(\|I\| = 1\), then \((I +D)^{-1}\)exists, and we have

$$ (I +D)^{-1}=I-D+D^{2}-D^{3}+D^{4}-D^{5}+ \cdots, $$

where \(\|D\|\)is denoted by

$$ \Vert D \Vert =\sup_{x\neq 0}\frac{ \Vert Dx \Vert _{2}}{ \Vert x \Vert _{2}} $$

for a vector y in \(\mathbb{C}^{N}\), \(\|y\|_{2}=(y^{H}y)^{\frac{1}{2}}\)is the Euclidean norm of y, and \(y^{H}\)denotes the Hermitian adjoint of y.

Definition 2.4

([24, 25])

Let s and r be finite positive integers, the generalized hypergeometric matrix function is defined by the matrix power series

$$ {}_{s}F_{r}(E;D;z)=\sum _{n=0}^{\infty }\prod^{s}_{i=1}(E_{i})_{n} \prod^{r}_{j=1}\bigl[(D_{j})_{n} \bigr]^{-1}\frac{z^{n}}{n!}, $$

where \(E_{i}\), \(1\leq i\leq s\), and \(D_{j}\), \(1\leq j\leq r\), are commutative matrices in \(\mathbb{C}^{N\times N}\) and

$$ D_{j}+n I \text{ are invertible for all integers } n\in \mathbb{N}_{0}. $$

Note that for \(s=2\), \(r=1\) we get the Gauss hypergeometric matrix function \({}_{2}F_{1}\) (see [25]).

Definition 2.5

([2, 8, 9])

The fractional order integral (Riemann–Liouville operator) of the function \(f(u)\) of order α is defined by

$$ \bigl(I^{\alpha }_{a} f\bigr) (u)= \frac{1}{\Gamma (\alpha )} \int ^{ \infty }_{a}(u-t)^{\alpha -1}f(t)\,dt, $$

where \(a\in \mathbb{R}\) and \(\alpha \in \mathbb{R}^{+}\).

Definition 2.6

([1, 17])

Let D be a positive stable matrix in \(\mathbb{C}^{{N}\times {N}}\) and \(\mu \in \mathbb{C}\) such that \(\mathbf{Re} (\mu )>0\), the Riemann–Liouville fractional integral of order μ is defined as follows:

$$ \mathbf{I}^{\mu }\bigl(\zeta ^{D}\bigr)= \frac{1}{\Gamma (\mu )} \int _{0}^{\zeta }( \zeta -z)^{\mu -1}\zeta ^{D} \,dz, \quad D\in \mathbb{C}^{N\times N}, $$

where \(\mathbf{Re}(z)>0\).

Lemma 2.2

([1, 18])

Let D be a positive stable matrix in \(\mathbb{C}^{{N}\times {N}}\)such that \(\mathbf{Re} (\mu )>0\). Then the Riemann–Liouville fractional integrals of order μ can be written as

$$ \mathbf{I}^{\mu }\bigl(\zeta ^{D-I}\bigr)= \Gamma (D)\Gamma ^{-1}(D+\mu I)\zeta ^{D+( \mu -1)I}. $$

For the fractional order derivative, we have the following definition.

Definition 2.7

([2, 9, 39])

The Liouville–Caputo fractional derivative of order \(\alpha \in (n-1,n)\) (\(n\in \mathbb{N}:={\{1,2,\ldots\}} \)) of \(f(\tau )\), \(\tau \geq a\) is given by

$$ D_{a}^{\alpha } f(\tau ) = I_{a}^{n-\alpha } D^{n} f(\tau ),\quad D= \frac{d}{d\tau }. $$

This definition is more convenient in many applications in physics, engineering, and applied sciences [3, 9, 14, 15, 39]. Moreover, it generalizes (interpolates) the definition of integer order derivative. The fractional derivative of the product functions \(g(\tau )f(\tau )\) is given by the Leibniz rule in the form (cf. [2, 15])

$$ D^{\alpha }\bigl[g(\tau )f(\tau )\bigr]=\sum ^{\infty }_{s=0}\binom{\alpha }{s} D^{s}g( \tau ) D^{\alpha -s}f(\tau ). $$

3 Fractional Legendre matrix polynomials and hypergeometric representation

Following [25, 36, 37], we adapt the Legendre-type matrix polynomials to the fractional setting as follows.

Definition 3.1

(Fractional Legendre matrix polynomial)

Let E be a positive stable matrix in \(\mathbb{C}^{N\times N}\), and let us denote \(\sqrt{E}=E^{\frac{1}{2}}=\exp (\frac{1}{2}\log E)\) the image of the function \(z^{\frac{1}{2}}=\exp (\frac{1}{2}\log \eta )\) by the Riesz–Dunford functional calculus, acting on the matrix E, where logη denotes the principal branch of the complex logarithm (cf. [25, 40]). We define the Legendre-type matrix functions (LTMFs) by the Rodrigues formula

$$ L_{\frac{1}{m}}(z,E)=\frac{1}{\Gamma (\frac{1}{m}+1)}D^{\frac{1}{m}}_{-1} (\sqrt{2E} )^{-\frac{1}{m}} \biggl\{ \biggl( \frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr\} ^{\frac{1}{m}},\quad m=1,2,3, \ldots , $$

and, for \(\alpha \in (-1,0)\), the Legendre-type matrix functions of order α are defined by

$$ L_{\alpha }(z, E)=\frac{1}{\Gamma (\alpha +1)} (\sqrt{2E} )^{-\alpha } I^{-\alpha }_{-1} \biggl[ \biggl( \frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr]^{\alpha }. $$

3.1 Hypergeometric representation

Theorem 3.1

The matrix polynomials \(L_{\frac{1}{m}}(z, E)\)have the following representations in terms of the Gauss hypergeometric function:

  1. (i)

    \(L_{\frac{1}{m}}(z,E)=\{\frac{1}{2}(\frac{z\sqrt{2E}}{2}-I)\}^{ \frac{1}{m}} \,{}_{2}F_{1} (-\frac{1}{m},-\frac{1}{m};1;( \frac{z\sqrt{2E}}{2}+I)(\frac{z\sqrt{2E}}{2}-I)^{-1} )\).

  2. (ii)

    \(L_{\frac{1}{m}}(z, E)=(-1)^{\frac{1}{m}} \,{}_{2}F_{1} (- \frac{1}{m},\frac{1}{m}+1; 1; \frac{2I+z\sqrt{2E}}{4} )\).

  3. (iii)

    \(L_{\alpha }(z,E)=(-1)^{\alpha } \,{}_{2}F_{1} (-\alpha , \alpha +1; 1; \frac{2I+z\sqrt{2E}}{4} )\); \(\alpha \in (-1,0)\).


(i) According to Definition 3.1, we can write

$$ L_{\frac{1}{m}}(z,E)=\frac{1}{\Gamma (\frac{1}{m}+1)}D^{ \frac{1}{m}}_{-1} (\sqrt{2E} )^{-\frac{1}{m}} \biggl\{ \frac{z\sqrt{2E}}{2}-I \biggr\} ^{\frac{1}{m}} \biggl\{ \frac{z\sqrt{2E}}{2}+I \biggr\} ^{\frac{1}{m}}. $$

Using the Leibniz rule for fractional derivative, we obtain

$$\begin{aligned} L_{\frac{1}{m}}(z,E) =& \frac{ (\sqrt{2E} )^{-\frac{1}{m}}}{\Gamma (\frac{1}{m}+1)} \sum ^{\infty }_{k=0}C^{\frac{1}{m}}_{k}D^{k} \biggl( \frac{z\sqrt{2E}}{2}-I \biggr)^{\frac{1}{m}}D^{\frac{1}{m}-k}_{-1} \biggl(\frac{z\sqrt{2A}}{2}+I \biggr)^{\frac{1}{m}} \\ =& \biggl\{ \frac{1}{2} \biggl(\frac{z\sqrt{2E}}{2}-I \biggr) \biggr\} ^{ \frac{1}{m}} \\ &{}\times\sum^{\infty }_{k=0} \frac{\{\Gamma (\frac{1}{m}+1)\}^{2}}{\{\Gamma (\frac{1}{m}-k+1)\}^{2}\{\Gamma (k+1)\}^{2}} \biggl(\frac{z\sqrt{2E}}{2}+I \biggr)^{k} \biggl(\frac{z\sqrt{2E}}{2}-I \biggr)^{-k}. \end{aligned}$$


$$\begin{aligned} L_{\frac{1}{m}}(z,E)= \biggl\{ \frac{1}{2} \biggl( \frac{z\sqrt{2E}}{2}-I \biggr) \biggr\} ^{\frac{1}{m}} \,{}_{2}F_{1} \biggl(-\frac{1}{m},-\frac{1}{m};1; \biggl( \frac{z\sqrt{2E}}{2}+I \biggr) \biggl(\frac{z\sqrt{2E}}{2}-I \biggr)^{-1} \biggr). \end{aligned}$$

(ii) Since

$$\begin{aligned} L_{\frac{1}{m}}(z,E) =&\frac{1}{\Gamma (\frac{1}{m}+1)}D^{ \frac{1}{m}}_{-1} (\sqrt{2E} )^{-\frac{1}{m}} \biggl\{ \biggl(\frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr\} ^{\frac{1}{m}} \\ =&\frac{D^{\frac{1}{m}}_{-1} (\sqrt{2E} )^{-\frac{1}{m}}}{\Gamma (\frac{1}{m}+1)} \biggl\{ (-1)^{\frac{1}{m}} \biggl( \frac{z\sqrt{2E}}{2}+I \biggr)^{ \frac{1}{m}} \biggl(I-\frac{x\sqrt{2E}}{2} \biggr)^{\frac{1}{m}} \biggr\} \\ =&\frac{1}{\Gamma (\frac{1}{m}+1)}D^{-\frac{1}{m}}_{-1} (\sqrt{2E} )^{\frac{1}{m}} \biggl\{ (-2)^{\frac{1}{m}} \biggl( \frac{z\sqrt{2E}+2I}{2} \biggr)^{\frac{1}{m}}\cdot \biggl(I- \frac{z\sqrt{2E}+2I}{4} \biggr)^{\frac{1}{m}} \biggr\} . \end{aligned}$$

To make use of Lemma 2.1, we observe that

$$ \biggl(I-\frac{z\sqrt{2E}+2I}{4} \biggr)^{\frac{1}{m}}= \sum ^{ \infty }_{k=0}(-1)^{k}C^{\frac{1}{m}}_{k} \biggl( \frac{z\sqrt{2E}+2I}{4} \biggr)^{k}=\sum ^{\infty }_{k=0} \frac{(-1)^{k}}{2^{k}}C^{\frac{1}{m}}_{k} \biggl( \frac{z\sqrt{2E}+2I}{2} \biggr)^{k}. $$

Therefore, we get

$$\begin{aligned} L_{\frac{1}{m}}(z,E)&= \frac{(-2)^{\frac{1}{m}} (\sqrt{2E} )^{-\frac{1}{m}}}{ \Gamma (\frac{1}{m}+1)\cdot 2^{\frac{1}{m}}} \sum ^{\infty }_{k=0}\frac{(-1)^{k}}{2^{2k}}C_{k}^{\frac{1}{m}}D^{ \frac{1}{m}}_{-1} (z\sqrt{2E}+2I )^{\frac{1}{m}+k} \\ &=(-1)^{k} (\sqrt{2E} )^{-\frac{1}{m}} (\sqrt{2E} )^{\frac{1}{m}}\sum^{\infty }_{k=0} \frac{(-\frac{1}{m})_{k}(\frac{1}{m}+1)_{k}}{(\Gamma (k+1))^{2}} \biggl(\frac{2I+z\sqrt{2E}}{4} \biggr)^{k} \\ &=(-1)^{k}\sum^{\infty }_{k=0} \frac{(-\frac{1}{m})_{k}(\frac{1}{m}+1)_{k}}{(1)_{k}k!} \biggl( \frac{2I+z\sqrt{2E}}{4} \biggr)^{k} \\ &=(-1)^{\frac{1}{m}} \,{}_{2}F_{1} \biggl(- \frac{1}{m}, \frac{1}{m}+1; 1; \frac{z\sqrt{2E}+2I}{4} \biggr). \end{aligned}$$

(iii) Similarly, in proof (ii), we obtain the required relationship. □

3.2 Property of continuity

Theorem 3.2

If \(m=1,2,3,\ldots \)and \(\alpha \in (-1,0)\), then

  1. (i)

    \(\lim_{\frac{1}{m}\to 0^{+}} L_{\frac{1}{m}}(z,E)=\lim_{\alpha \to 0^{-}} L_{\alpha }(z,E)=1\).

  2. (ii)

    \(L_{\frac{1}{m}}(-z, E)=(-1)^{\frac{1}{m}} L_{\frac{1}{m}}(z,E) \).


(i) According to relation (ii) in Theorem 3.1, we have

$$\begin{aligned} \lim_{\frac{1}{m}\to 0^{+}} L_{\frac{1}{m}}(z, E) =& \lim_{\frac{1}{m}\to 0^{+}}(-1)^{\frac{1}{m}} \,{}_{2}F_{1} \biggl(- \frac{1}{m},\frac{1}{m}+1; 1; \frac{2I+z\sqrt{2E}}{4} \biggr) \\ =&\lim_{\frac{1}{m}\to 0^{+}} (-1)^{\frac{1}{m}} \biggl\{ \frac{(-\frac{1}{m})_{0}(\frac{1}{m}+1)_{0}}{(1)_{0}}+ \frac{(-\frac{1}{m})_{1}(\frac{1}{m}+1)_{1}}{(1)_{1}} \frac{2I+z\sqrt{2E}}{4}+\cdots \biggr\} , \end{aligned}$$

where \((\varsigma )_{0}=1\), \((0)_{s}=0\), then we obtain the required result as follows:

$$ \lim_{\frac{1}{m}\to 0^{+}} L_{\frac{1}{m}}(z, E)=1. $$


$$ \lim_{\alpha \to 0^{-}} L_{\alpha }(z,E)=1. $$

(ii) From relation (i) in Theorem 3.1, we can write

$$\begin{aligned} L_{\frac{1}{m}}(-z,E) =& \biggl\{ \frac{1}{2} \biggl( \frac{-z\sqrt{2E}}{2}-I \biggr) \biggr\} ^{\frac{1}{m}} \,{}_{2}F_{1} \biggl(- \frac{1}{m},-\frac{1}{m};1; \biggl(I-\frac{z\sqrt{2E}}{2} \biggr) \biggl(\frac{-z\sqrt{2E}}{2}-I \biggr)^{-1} \biggr) \\ =& (-1)^{\frac{1}{m}} \biggl\{ \frac{1}{2} \biggl( \frac{z\sqrt{2E}}{2}+I \biggr) \biggr\} ^{\frac{1}{m}} \\ &{}\times {}_{2}F_{1} \biggl(-\frac{1}{m},- \frac{1}{m};1; \biggl( \frac{z\sqrt{2E}}{2}-I \biggr) \biggl( \frac{z\sqrt{2E}}{2}+I \biggr)^{-1} \biggr). \end{aligned}$$


$$ L_{\frac{1}{m}}(-z,E)= (-1)^{\frac{1}{m}} L_{ \frac{1}{m}}(z,E). $$


4 Recurrence relations and matrix differential equations

Two main results are given in this section. The first one is concerned with the Legendre-type matrix polynomials of arbitrary fractional orders \(L_{\frac{1}{m}}(z,E)\), which generalizes its counterpart given in [36]. The second main result provides a differential equation related to \(L_{\frac{1}{m}}(z,E)\).

Theorem 4.1

The matrix polynomials \(L_{\frac{1}{m}}(z,E)\)have the following recurrence relations:

  1. (i)

    \(2L'_{\frac{1}{m}+1}(z, E)-2L'_{\frac{1}{m}-1}(z, E)=(\frac{2}{m}+1) \sqrt{2E}L_{\frac{1}{m}}(z, E)\).

  2. (ii)

    \(2L'_{\frac{1}{m}+1}(z, E)=(\frac{1}{m}+1)\sqrt{2E}L_{\frac{1}{m}}(z, E)+z\sqrt{2E}L'_{\frac{1}{m}}(z, E)\).

  3. (iii)

    \(z\sqrt{2E}L'_{\frac{1}{m}}(z,E)-\frac{1}{m}\sqrt{2E}L_{ \frac{1}{m}}(z,E)=2L'_{\frac{1}{m}-1}(z,E)\).


(i) Since

$$ L_{\frac{1}{m}}(z, E)=\frac{1}{\Gamma (\frac{1}{m}+1)}D^{\frac{1}{m}}_{-1} (\sqrt{2E} )^{-\frac{1}{m}} \biggl\{ \biggl( \frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr\} ^{\frac{1}{m}}, $$


$$ L_{\frac{1}{m}+1}(z, E)=\frac{1}{\Gamma (\frac{1}{m}+2)}D^{ \frac{1}{m}+1}_{-1} (\sqrt{2E} )^{-(\frac{1}{m}+1)} \biggl\{ \biggl(\frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr\} ^{\frac{1}{m}+1}. $$

Hence, it follows

$$\begin{aligned} L_{\frac{1}{m}+1}(z,E)&= \frac{ (\sqrt{2E} )^{-(\frac{1}{m}+1)}}{\Gamma (\frac{1}{m}+2)} \biggl\{ I^{1-\frac{1}{m}}_{-1}D^{2} \biggl( \biggl(\frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr)^{\frac{1}{m}+1} \biggr\} \\ &= \frac{ (\sqrt{2E} )^{-(\frac{1}{m}+1)}}{\Gamma (\frac{1}{m}+2)} \biggl\{ I^{1-\frac{1}{m}}_{-1}D \biggl[ \biggl(\frac{1}{m}+1 \biggr) \biggl( \biggl(\frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr)^{\frac{1}{m}} \frac{2z(\sqrt{2E})^{2}}{4} \biggr] \biggr\} \\ &= \frac{ (\sqrt{2E} )^{1-\frac{1}{m}}}{2\Gamma (\frac{1}{m}+1)} \\ &\quad {}\times\biggl\{ I^{1-\frac{1}{m}}_{-1} \biggl[ \biggl( \biggl( \frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr)^{\frac{1}{m}}+ \frac{2(z\sqrt{2E})^{2}}{4m} \biggl( \biggl( \frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr)^{\frac{1}{m}-1} \biggr] \biggr\} \\ &= \frac{ (\sqrt{2E} )^{1-\frac{1}{m}}}{2\Gamma (\frac{1}{m}+1)} \\ &\quad {}\times\biggl\{ I^{1-\frac{1}{m}}_{-1} \biggl[ \biggl(\frac{2}{m}+1 \biggr) \biggl( \biggl(\frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr)^{\frac{1}{m}}+ \frac{2}{m} \biggl( \biggl(\frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr)^{ \frac{1}{m}-1} \biggr] \biggr\} . \end{aligned}$$

We now have

$$\begin{aligned} L_{\frac{1}{m}+1}(z,E) =&\frac{ (\sqrt{2E} )^{1-\frac{1}{m}}}{2\Gamma (\frac{1}{m}+1)}I^{1- \frac{1}{m}}_{-1} \biggl\{ \biggl(\frac{2}{m}+1 \biggr) \biggl( \biggl( \frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr)^{\frac{1}{m}} \biggr\} \\ &{}+\frac{(\sqrt{2E})^{1-\frac{1}{m}}}{\Gamma (\frac{1}{m})}I^{1- \frac{1}{m}}_{-1} \biggl( \biggl( \frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr)^{\frac{1}{m}-1}. \end{aligned}$$

Differentiating both sides, we get

$$\begin{aligned} L'_{\frac{1}{m}+1}(z,E) =& \biggl( \frac{2}{m}+1 \biggr) \biggl(\frac{\sqrt{2E}}{2} \biggr) \frac{D^{\frac{1}{m}}_{-1}(\sqrt{2E})^{-\frac{1}{m}}}{\Gamma (\frac{1}{m}+1)} \biggl\{ \biggl(\frac{x\sqrt{2A}}{2} \biggr)^{2}-I \biggr\} ^{\frac{1}{m}} \\ &{}+\frac{D D^{\frac{1}{m}-1}_{-1}(\sqrt{2E})^{-(\frac{1}{m}-1)}}{\Gamma (\frac{1}{m})} \biggl\{ \biggl(\frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr\} ^{ \frac{1}{m}-1} \\ =& \biggl(\frac{2}{m}+1 \biggr) \biggl(\frac{\sqrt{2E}}{2} \biggr)L_{ \frac{1}{m}}(z,E)+L'_{\frac{1}{m}-1}(z,E). \end{aligned}$$

Thus the proof of (i) in Theorem 4.1 is completed.

(ii) Also we have

$$\begin{aligned} L_{\frac{1}{m}+1}(z, E) =&\frac{D^{\frac{1}{m}+1}_{-1} (\sqrt{2E})^{-(\frac{1}{m}+1)}}{\Gamma (\frac{1}{m}+2)} \biggl\{ \biggl(\frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr\} ^{ \frac{1}{m}+1} \\ =&\frac{(\sqrt{2E})^{-(\frac{1}{m}+1)}}{\Gamma (\frac{1}{m}+2)}D^{ \frac{1}{m}}_{-1}D \biggl\{ \biggl( \frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr\} ^{\frac{1}{m}+1} \\ =&\frac{2(\frac{1}{m}+1)(\sqrt{2E})^{-(\frac{1}{m}+1)}(\sqrt{2E})^{2}}{4\Gamma (\frac{1}{m}+2)}D^{ \frac{1}{m}}_{-1} \biggl\{ z \biggl( \biggl(\frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr)^{\frac{1}{m}} \biggr\} \\ =&\frac{(\sqrt{2E})^{1-\frac{1}{m}}}{2\Gamma (\frac{1}{m}+1)}D^{ \frac{1}{m}}_{-1} \biggl\{ z \biggl( \biggl(\frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr)^{\frac{1}{m}} \biggr\} . \end{aligned}$$

Using the Leibniz rule for fractional derivative, we have

$$\begin{aligned} L_{\frac{1}{m}+1}(z, E) =&\frac{(\sqrt{2E})^{1-\frac{1}{m}}}{2\Gamma (\frac{1}{m}+1)} \Biggl\{ \sum^{\infty }_{k=0}C^{\frac{1}{m}}_{k}D^{k}x D^{\frac{1}{m}-k}_{-1} \biggl( \biggl(\frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr)^{\frac{1}{m}} \Biggr\} \\ =&\frac{(\sqrt{2E})^{1-\frac{1}{m}}}{2\Gamma (\frac{1}{m}+1)} \biggl\{ zD^{ \frac{1}{m}}_{-1} \biggl( \biggl(\frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr)^{\frac{1}{m}}+ \frac{1}{m}D^{\frac{1}{m}-1}_{-1} \biggl( \biggl( \frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr)^{\frac{1}{m}} \biggr\} . \end{aligned}$$

Multiplying it by 2 and differentiating it, we obtain

$$\begin{aligned} 2L'_{\frac{1}{m}+1}(z,E) =&\sqrt{2E} \biggl\{ zL'_{\frac{1}{m}}(z, E)+L_{\frac{1}{m}}(z, E)+ \frac{1}{m}L_{\frac{1}{m}}(z, E)\biggr\} \\ =& \biggl(\frac{1}{m}+1 \biggr)\sqrt{2E}L_{\frac{1}{m}}(z,E)+z \sqrt{2E}L'_{ \frac{1}{m}}(z,E), \end{aligned}$$

which is the required result in (ii).

(iii) Subtracting (i) and (ii), we get

$$ z\sqrt{2E}L'_{\frac{1}{m}}(z,E)- \frac{1}{m}\sqrt{2E}L_{ \frac{1}{m}}(z,E)=2L'_{\frac{1}{m}-1}(z,E), $$

which is the required result in (iii). □

Theorem 4.2

For each natural number \(m\geq 1\), the Legendre-type matrix polynomials \(L_{\frac{1}{m}}(z,E)\)will satisfy the following matrix differential equation:

$$\begin{aligned}& \bigl(4I-(z\sqrt{2E})^{2} \bigr)L''_{\frac{1}{m}}(z,E) -2x( \sqrt{2E})^{2}L'_{ \frac{1}{m}}(z,E) \\& \quad {} +\frac{1}{m} \biggl(\frac{1}{m}+1 \biggr) ( \sqrt{2E})^{2}L_{ \frac{1}{m}}(z,E)=\mathbf{0},\quad \vert z \vert \leq 1. \end{aligned}$$


From (ii) in Theorem 4.1, we have

$$ 2L'_{\frac{1}{m}+1}(z,E)=\biggl( \frac{1}{m}+1\biggr)\sqrt{2E}L_{ \frac{1}{m}}(z,E)+z \sqrt{2E}L'_{\frac{1}{m}}(z,E). $$

Replacing \(\frac{1}{m}\) by \(\frac{1}{m}-1\) to get

$$ 2L'_{\frac{1}{m}}(z,E)= \frac{1}{m}\sqrt{2E}L_{ \frac{1}{m}-1}(z,E)+z\sqrt{2E}L'_{\frac{1}{m}-1}(z,E). $$

Differentiating (18) with respect to z, we have

$$ 2L''_{\frac{1}{m}}(z,E)= \frac{1}{m}\sqrt{2E}L'_{ \frac{1}{m}-1}(z,E)+ \sqrt{2E}L'_{\frac{1}{m}-1}(z,E)+z\sqrt{2E}L''_{ \frac{1}{m}-1}(z,E), $$


$$ 2L''_{\frac{1}{m}}(z,E)= \biggl(\frac{1}{m}+1\biggr)\sqrt{2E}L'_{ \frac{1}{m}-1}(z,E)+z \sqrt{2E}L''_{\frac{1}{m}-1}(z,E). $$

Also, from (iii) in Theorem 4.1, we have

$$ z\sqrt{2E}L'_{\frac{1}{m}}(z,E)- \frac{1}{m}\sqrt{2E}L_{ \frac{1}{m}}(z,E)=2L'_{\frac{1}{m}-1}(z,E). $$

Differentiating (21) with respect to z, we have

$$ \sqrt{2E}L'_{\frac{1}{m}}(z,E)+z \sqrt{2E}L''_{ \frac{1}{m}}(z,E)- \frac{1}{m}\sqrt{2E}L'_{\frac{1}{m}}(z,E)=2L''_{ \frac{1}{m}-1}(z,E), $$


$$ \biggl(1-\frac{1}{m} \biggr) \sqrt{2E}L'_{\frac{1}{m}}(z,E)+x \sqrt{2E}L''_{\frac{1}{m}}(z,E)=2L''_{\frac{1}{m}-1}(z,E). $$

Multiplying (22) by 2, we get

$$ 4L''_{\frac{1}{m}}(z,E)=2 \biggl(\frac{1}{m}+1 \biggr) \sqrt{2E}L'_{\frac{1}{m}-1}(z,E)+2z \sqrt{2E}L''_{\frac{1}{m}-1}(z,E). $$

From (21) and (23) in (24), we obtain

$$\begin{aligned} 4L''_{\frac{1}{m}}(z,E) =& \biggl(\frac{1}{m}+1 \biggr) \sqrt{2E}\biggl\{ z\sqrt{2E}L'_{\frac{1}{m}}(z,E)- \frac{1}{m}\sqrt{2E}L_{ \frac{1}{m}}(z,E)\biggr\} \\ &{}+x\sqrt{2E} \biggl\{ \biggl(1-\frac{1}{m}\biggr)\sqrt{2E}L'_{\frac{1}{m}}(z,E)+z \sqrt{2E}L^{\prime \prime }_{ \frac{1}{m}}(z,E)\biggr\} . \end{aligned}$$

Therefore, the proof Theorem 4.2 is completed. □

Corollary 4.1

For \(m=1, 2,3,\ldots\) , \(W(\cos \phi ,E)=L_{\frac{1}{m}}(\cos \phi ,E)\)satisfying the following differential equation:

$$ \frac{(\sqrt{2E})^{2}}{\sin \phi }\frac{d}{d\phi } \biggl( \sin \phi \frac{d W}{d\phi } \biggr)+\frac{1}{m} \biggl( \frac{1}{m}+1 \biggr) (\sqrt{2E})^{2} W=\mathbf{0}. $$


Replacing \(\frac{z\sqrt{2E}}{2}\) by \(I\cos \phi \) in equation (18), we have the required result. □

5 Laplace’s first integral form and orthogonality property

Two more basic properties of the Legendre-type matrix polynomials of arbitrary fractional orders \(L_{\frac{1}{m}}(z,E)\) are developed in this section. That they enjoy an integral form is obtained in Theorem 5.1 in Sect. 5.1 through exploitation of their Definition 3.1 in terms of the hypergeometric matrix function. Orthogonality as an integral over \([-1,1]\) is also the subject of Theorem 5.2 in Sect. 5.2.

5.1 Laplace’s first integral form

Theorem 5.1

The Legendre-type matrix polynomials of arbitrary (fractional) orders \(L_{\frac{1}{m}}(z,E)\)have the following Laplace’s first integral form:

$$ L_{\frac{1}{m}}(z,E)=\frac{1}{\pi } \int ^{\pi }_{0} \biggl[ \frac{z\sqrt{2E}}{2}+ \biggl( \biggl(\frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr)^{\frac{1}{2}}\cos \varphi \biggr]^{\frac{1}{m}}\,d\varphi . $$


According to Theorem 3.2, we can write

$$\begin{aligned} \begin{aligned}[b] L_{\frac{1}{m}}(z,E)&=(-1)^{\frac{1}{m}} \,{}_{2}F_{1} \biggl(-\frac{1}{m}, \frac{1}{m}+1; 1; \frac{2I+z\sqrt{2E}}{4} \biggr) \\ &= {}_{2}F_{1} \biggl(-\frac{1}{m}, \frac{1}{m}+1;1; \frac{2I-z\sqrt{2E}}{4} \biggr) \\ &= {}_{2}F_{1} \biggl(-\frac{1}{m}, \frac{1}{m}+1;1; \frac{I-\frac{z\sqrt{2E}}{2}}{2} \biggr). \end{aligned} \end{aligned}$$

Therefore, we obtain

$$ \begin{aligned} L_{\frac{1}{m}}(z,E)&= {}_{2}F_{1} \biggl(-\frac{1}{m}, \frac{1}{m}+1;1;\frac{I-\frac{z\sqrt{2E}}{2}}{2} \biggr) \\ &= \biggl(\frac{z\sqrt{2E}}{2} \biggr)^{\frac{1}{m}} \,{}_{2}F_{1} \biggl(-\frac{1}{2m},-\frac{1}{2m}+\frac{1}{2};1; \biggl\{ \biggl( \biggl(\frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr) \biggl( \biggl( \frac{z\sqrt{2E}}{2} \biggr)^{-1} \biggr)^{2} \biggr\} \biggr) \\ &= \biggl(\frac{z\sqrt{2E}}{2} \biggr)^{\frac{1}{m}}\sum ^{\infty }_{k=0} \frac{(-\frac{1}{2m})_{k} (-\frac{1}{2m}+\frac{1}{2} )_{k}}{(1)_{k}k!} \biggl\{ \biggl( \biggl(\frac{z\sqrt{2E}}{2} \biggr)^{2}-I \biggr) \biggl( \biggl( \frac{z\sqrt{2E}}{2} \biggr)^{-1} \biggr)^{2} \biggr\} ^{k}. \end{aligned} $$

Note that

$$ \biggl(-\frac{1}{2m} \biggr)_{k} \biggl(- \frac{1}{2m}+\frac{1}{2} \biggr)_{k}= \frac{(-\frac{1}{m})_{2k}}{2^{2k}}= \frac{(-1)^{2k}\Gamma (\frac{1}{m}+1)}{2^{2k}\Gamma (\frac{1}{m}-2k+1)}. $$

Now, we see that

$$ L_{\frac{1}{m}}(z,E)=\sum ^{\infty }_{k=0} \biggl\{ \frac{\Gamma (\frac{1}{m}+1) (\frac{z\sqrt{2E}}{2})^{\frac{1}{m}-2k}((\frac{z\sqrt{2E}}{2})^{2}-I)^{k}}{2^{2k}(k!)^{2}\Gamma (\frac{1}{m}-2k+1)} \biggr\} , $$

where \((\frac{1}{2})_{k}=\frac{\Gamma (2k+1)}{2^{2k}k!}= \frac{(2k)!}{2^{2k}k!}\Rightarrow 2^{2k}k!= \frac{(2k)!}{(\frac{1}{2})_{k}}\), then

$$ L_{\frac{1}{m}}(z,E)=\sum ^{\infty }_{k=0} \biggl\{ \frac{\Gamma (\frac{1}{m}+1)(\frac{1}{2})_{k} (\frac{z\sqrt{2E}}{2})^{\frac{1}{m}-2k}((\frac{z\sqrt{2E}}{2})^{2}-I)^{k}}{k!(2k)!\Gamma (\frac{1}{m}-2k+1)} \biggr\} . $$

But we have \(\frac{(\frac{1}{2})_{k}}{k!}=\frac{1}{\pi }\int ^{\pi }_{0}\cos ^{2k} \varphi \,d\varphi \) and \(\int ^{\pi }_{0}\cos ^{s}\varphi \,d\varphi =0\) for odd s. Hence,

$$ L_{\frac{1}{m}}(z,E)=\frac{1}{\pi }\sum ^{\infty }_{k=0} \biggl\{ \frac{\Gamma (\frac{1}{m}+1) (\frac{z\sqrt{2E}}{2})^{\frac{1}{m}-k}((\frac{z\sqrt{2E}}{2})^{2}-I)^{\frac{1}{2}k}}{k!\Gamma (\frac{1}{m}-k+1)} \biggr\} \int ^{\pi }_{0}\cos ^{k}\varphi \,d\varphi , $$

in which each term involving an odd k is zero, yields the desired result of Theorem 5.1. □

5.2 Orthogonality property

Theorem 5.2

Let \(\mu , \nu =1,2,3,\ldots\) . Then the Legendre-type matrix polynomials of arbitrary (fractional) orders \(L_{\frac{1}{\mu }}(z,E)\)and \(L_{\frac{1}{\nu }}(z,E)\)satisfy the following property:

$$ \int ^{1}_{-1}L_{\frac{1}{\mu }}(z,E) L_{\frac{1}{\nu }}(z,E)\,dz=0;\quad \mu \neq \nu . $$


From Theorem 4.2, for any two numbers \(\mu \neq \nu \), we have

$$ \bigl(4I-(z\sqrt{2E})^{2} \bigr)L''_{\frac{1}{\mu }}(z,E)-2z( \sqrt{2E})^{2}L'_{ \frac{1}{\mu }}(z,E)+ \frac{1}{\mu } \biggl(\frac{1}{\mu }+1 \biggr) ( \sqrt{2E})^{2}L_{ \frac{1}{\mu }}(z,E)=\mathbf{0} $$


$$ \bigl(4I-(z\sqrt{2E})^{2} \bigr)L''_{\frac{1}{\nu }}(z,E)-2z( \sqrt{2E})^{2}L'_{ \frac{1}{\nu }}(z,E)+ \frac{1}{\nu } \biggl(\frac{1}{\nu }+1 \biggr) ( \sqrt{2E})^{2}L_{ \frac{1}{\nu }}(z,E)=\mathbf{0}. $$

By multiplying (33) by \(L_{\frac{1}{\nu }}(z,E)\) and (34) by \(L_{\frac{1}{\mu }}(z,E)\), subtracting the resulting equations, we have

$$\begin{aligned} &\bigl(4I-(z\sqrt{2E})^{2}\bigr) \bigl[L''_{\frac{1}{\mu }}(z,E)L_{\frac{1}{\nu }}(z,E)-L''_{ \frac{1}{\nu }}(z,E)L_{\frac{1}{\mu }}(z,E) \bigr] \\ &\qquad {}-2z(\sqrt{2E})^{2}\bigl[L'_{\frac{1}{\mu }}(z,E)L_{\frac{1}{\nu }}(z,E)-L'_{ \frac{1}{\nu }}(z,E)L_{\frac{1}{\mu }}(z,E) \bigr] \\ &\qquad {}+(\sqrt{2E})^{2} \biggl[\frac{1}{\mu } \biggl( \frac{1}{\mu }+1 \biggr)- \frac{1}{\nu } \biggl( \frac{1}{\nu }+1 \biggr) \biggr]P_{\frac{1}{\mu }}(z,E)L_{ \frac{1}{\nu }}(z,E)= \mathbf{0} \\ &\quad =\frac{d}{dz}\bigl(4I-(z\sqrt{2E})^{2}\bigr) \bigl[L'_{\frac{1}{\mu }}(z,E)L_{ \frac{1}{\nu }}(z,E)-L'_{\frac{1}{\nu }}(z,E)L_{\frac{1}{\mu }}(z,E) \bigr] \\ &\qquad {}+(\sqrt{2E})^{2} \biggl[\frac{1}{\mu } \biggl( \frac{1}{\nu }+1 \biggr)- \frac{1}{\nu } \biggl( \frac{1}{\nu }+1 \biggr) \biggr]L_{\frac{1}{\mu }}(z,E)L_{ \frac{1}{\nu }}(z,E)= \mathbf{0}. \end{aligned}$$

Integrating from −1 to 1, we obtain the result in (32). □

6 Conclusion

The Legendre polynomials \(\mathbb{P}_{n}(z)\) are given by the following Rodrigues’ formula [41]:

$$ \mathbb{P}_{n}(z)={\frac{1}{2^{n}n!}} {\frac{d^{n}}{dz^{n}}}\bigl(z^{2}-1\bigr)^{n},\quad n\in \mathbb{N}_{0}. $$

These polynomials satisfy the second order linear differential equation

$$ {\frac{d}{dz}} \biggl[ \bigl(1-z^{2} \bigr){ \frac{d\mathbb{P}_{n}(z)}{dz}} \biggr]+n(n+1)\mathbb{P}_{n}(z)=0;\quad \vert z \vert \leq 1. $$

Legendre polynomial is an important orthogonal polynomial with interval of orthogonality between −1 and 1, in the form

$$ \int ^{1}_{-1}\mathbb{P}_{m}(z) \mathbb{P}_{n}(z)\,dz= \textstyle\begin{cases} 0 &\mbox{if }n\neq m, \\ \frac{2}{2n+1} &\mbox{if }m=n. \end{cases} $$

Because of their orthogonal properties, Legendre polynomials have been used for solving other integral equations such as Fredholm integral equations [31], Bagley–Torvik equations [33], and Volterra integral equations [34]. Recently, orthogonal matrix polynomials and their generalizations in different ways have been a focus of increasing attention leading to new and interesting problems. In this perspective, this manuscript is a continuation of the recent authors’ paper [1], where we have discussed the Legendre-type matrix polynomials via fractional orders, starting from the Rodrigues matrix formula. This study is assumed to be a generalization of the scalar case [39] to the matrix setting. This approach allows us to derive several new integral and differential representations that can be used in theoretical and applicable aspects and for some numerical methods.


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The authors extend their appreciation to the Deanship of Scientific Research at King Khalid University for funding this work through research groups program under grant (R.G.P.1/184/41). The authors also would like to thank Prof. N. Saad for his valuable suggestions and comments to improve this paper.

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Zayed, M., Hidan, M., Abdalla, M. et al. Fractional order of Legendre-type matrix polynomials. Adv Differ Equ 2020, 506 (2020).

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