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Mathematics
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5 April 2022

Various Types of q-Differential Equations of Higher Order for q-Euler and q-Genocchi Polynomials

and
1
Department of Mathematics, Hannam University, Daejeon 34430, Korea
2
Department of Mathematics Education, Silla University, Busan 46958, Korea
*
Author to whom correspondence should be addressed.
This article belongs to the Special Issue Advances in Differential and Difference Equations with Applications 2023

Abstract

One finds several q-differential equations of a higher order for q-Euler polynomials and q-Genocchi polynomials. Additionally, we have a few q-differential equations of a higher order, which are mixed with q-Euler numbers and q-Genocchi polynomials. Moreover, we investigate some symmetric q-differential equations of a higher order by applying symmetric properties of q-Euler polynomials and q-Genocchi polynomials.

1. Introduction

The Bernoulli equation is written as
d y d x + p ( x ) y g ( x ) y m = 0 ,
where m is any real number, and p ( x ) and g ( x ) are continuous functions; see [].
The above Bernoulli equation is one of the equations that can convert nonlinear equations into linear equations. The equation was first discussed in a work by Jacob Bernoulli in 1695, after whom it is named. For example, this Bernoulli equation can solve problems modeled by nonlinear differential equations and also solve equations about the population expressed in logistic equations or Verhulst equations.
In [,], we note
n = 0 E n t n n ! = 2 e t + 1 , n = 0 E n ( x ) t n n ! = 2 e t + 1 e t x ,
where E n is the Euler numbers and E n ( x ) is the Euler polynomials. If m = 0 in Equation (1), then the Bernoulli equation has the solution which is the generating function of the Euler polynomials. The equation is as follows.
d d x E n 1 ( x ) + E 0 ( 1 ) + 2 x E 1 ( 1 ) E n 1 ( x ) + 2 E 1 ( 1 ) E n ( x ) = 0 ,
where E n ( x ) is the Euler polynomials.
In q-calculus, we consider the first order of the q-Bernoulli equation D q y + p ( x ) y g ( x ) y m = 0 . When m = 0 in Equation (1), the q-Euler polynomials is the solution of the following q-differential equation of the first order.
D q E n 1 , q ( x ) + q ( E 0 , q ( 1 ) + 2 q x ) E 1 , q ( 1 ) E n 1 , q ( x ) + 2 q n 1 E 1 , q ( 1 ) E n , q ( q x ) = 0 ,
where D q is the derivative in q-calculus and E n , q ( x ) is the q-Euler polynomials. We note that Equation (3) becomes Equation (2) when q 1 .
Through Equation (3), the goal of this paper is to find out the form of differential equations of a higher order. We also find several symmetric properties of differential equations of a higher order, the structure of differential equations of a higher order, the properties of polynomials at q 1 , and so on. To introduce q-Euler polynomials and q-Genocchi polynomials, we will summarize the definitions and make the arrangements required in this paper as follows.
The q-number, which is important in q-calculus, was first introduced by Jackson, see [,]. From the discovery of the q-number, various useful results were considered and studied in q-series, q-special functions, quantum algebras, q-discrete distribution, q-differential equation, q-calculus, and so on; see [,,,,,,,,,,]. Here, we would like to briefly review several significant concepts of q-calculus, which we need for this paper.
Let n , q R with q 1 . The number
[ n ] q = 1 q n 1 q
is called the q-number. We note that lim q 1 [ n ] q = n . In particular, for k Z , [ k ] q is called the q-integer.
The q-Gaussian binomial coefficients are defined by
m r q = 0 if r > m ( 1 q m ) ( 1 q m 1 ) ( 1 q m r + 1 ) ( 1 q ) ( 1 q 2 ) ( 1 q r ) if r m ,
where m and r are non-negative integers. For r = 0 , the value is 1 since the numerator and the denominator are both empty products. One notes [ n ] q ! = [ n ] q [ n 1 ] q [ 2 ] q [ 1 ] q and [ 0 ] q ! = 1 .
Definition 1.
The q-derivative of a function f with respect to x is defined by
D q , x f ( x ) : = D q f ( x ) = f ( x ) f ( q x ) ( 1 q ) x , f o r x 0 ,
and D q f ( 0 ) = f ( 0 ) .
One can prove that f is differentiable at zero, and it is clear that D q x n = [ n ] q x n 1 . Let us point out that D q , x ( k ) f ( x ) converges to f ( k ) ( x ) as q goes to 1. From Definition 1, we can see some formulae for the q-derivative.
Theorem 1.
From Definition 1, we note that
( i ) D q ( f ( x ) g ( x ) ) = q ( x ) D q f ( x ) f ( q x ) D q g ( x ) = f ( x ) D q g ( x ) + g ( q x ) D q f ( x ) , ( i i ) D q f ( x ) g ( x ) = g ( q x ) D q f ( x ) f ( q x ) D q g ( x ) g ( x ) g ( q x ) = g ( x ) D q f ( x ) f ( x ) D q g ( x ) g ( x ) g ( q x ) , ( i i i ) f o r a n y c o n s t a n t s a a n d b , D q ( a f ( x ) + b g ( x ) ) = a D q f ( x ) + b D q g ( x ) .
Definition 2.
Let z be any complex numbers with | z | < 1 . We introduce the following two series, called q-exponential functions
e q ( z ) = n = 0 z n [ n ] q ! , E q ( z ) = n = 0 q n 2 z n [ n ] q ! .
We note that lim q 1 e q ( z ) = e z .
Theorem 2
([]). From Definition 2, we note that
( i ) e q ( x ) e q ( y ) = e q ( x + y ) , if y x = q x y . ( i i ) e q ( x ) E q ( x ) = 1 . ( i i i ) e q 1 ( x ) = E q ( x ) .
Due to the above two types of q-exponential functions, Euler, Bernoulli, and Genocchi polynomials are defined as new types of polynomials, and many mathematicians have studied their properties; see [,,,,,,]. In addition, it is studied in various fields, such as the structure of approximations of polynomials and their relevance to fractals by using computers; see [,,]. The definition of each polynomial used in this paper can be confirmed in Definitions 3 and 4.
Definition 3.
The q-Euler numbers and polynomials can be expressed as
n = 0 E n , q t n [ n ] q ! = 2 e q ( t ) + 1 , n = 0 E n , q ( x ) t n [ n ] q ! = 2 e q ( t ) + 1 e q ( t x ) , r e s p e c t i v e l y .
When q 1 in Definition 3, we can find the Euler numbers and polynomials.
Definition 4.
The q-Genocchi numbers and polynomials can be expressed as
n = 0 G n , q t n [ n ] q ! = 2 t e q ( t ) + 1 , n = 0 G n , q ( x ) t n [ n ] q ! = 2 t e q ( t ) + 1 e q ( t x ) , r e s p e c t i v e l y .
When q 1 in Definition 4, we can find the Genocchi numbers and polynomials as
n = 0 G n t n n ! = 2 t e t + 1 , n = 0 G n ( x ) t n n ! = 2 t e t + 1 e t x .
Based on the previous content, our purpose is to find various q-differential equations of higher order that contain q-Euler polynomials and q-Genocchi polynomials as solutions of the equation of a higher order. In Section 2, we find a q-differential equation of higher order that has q-Euler polynomials as the solution and check its associated properties. In Section 3, not only are we able to find a q-differential equation of a higher order that is the solution of q-Genocchi polynomials, but we can also address a q-differential equation of a higher order in combination with the q-Euler number or polynomials. Various properties can be identified based on these equations of a higher order.

2. Several q -Differential Equations of Higher Order and Properties of q -Euler Polynomials

In this section, we show that the q-Euler polynomials are solutions to some q-differential equations of a higher order. Moreover, we introduce a special q-differential equation of a higher order which is related to a symmetric property for q-Euler polynomials.
Let
F q ( t , x ) : = 2 e q ( t ) + 1 e q ( t x ) = n = 0 E n , q ( x ) t n [ n ] q ! .
From Definition 3, we find the q-Euler numbers in Equation (4). From Table 1, we also can see a few q-Euler numbers E n , q and polynomials E n , q ( x ) as follows.
Lemma 1.
For 0 < q < 1 , we have
( i ) E n k , q ( x ) = [ n k ] q ! [ n ] q ! D q , x ( k ) E n , q ( x ) , ( i i ) E n k , q ( q 1 x ) = q k [ n k ] q ! [ n ] q ! D q , x ( k ) E n , q ( q 1 x ) .
Proof. 
(i) We will use induction to show the lemma. Applying q-derivative in (4), we have
D q , x ( 1 ) n = 0 E n , q ( x ) t n [ n ] q ! = 2 e q ( t ) + 1 D q , x ( 1 ) e q ( t x ) = n = 0 [ n ] q E n 1 , q ( x ) t n [ n ] q ! .
From the above equation, we find a relation such as
D q , x ( 1 ) E n , q ( x ) = [ n ] q E n 1 , q ( x ) .
In a similar way, we have
D q , x ( 2 ) E n , q ( x ) = [ n ] q [ n 1 ] q E n 2 , q ( x ) .
Therefore, we can find
D q , x ( k ) E n , q ( x ) = [ n ] q [ n 1 ] q [ n ( k 1 ) ] q E n k , q ( x ) ,
which is the desired result.
(ii) We omit the proof of (ii) in Lemma 1 because we can derive the required result if we use a similar method in the proof of (i) in Lemma 1. □
Theorem 3.
The q-Euler polynomials E n , q ( x ) is a solution of the following q-differential equation of a higher order.
E n 1 , q ( 1 ) 2 [ n 1 ] q ! D q , x ( n 1 ) E n 1 , q ( x ) + q E n 2 , q ( 1 ) 2 [ n 2 ] q ! D q , x ( n 2 ) E n 1 , q ( x ) + + q n 3 E 2 , q ( 1 ) 2 [ 2 ] q ! D q , x ( 2 ) E n 1 , q ( x ) + q n 2 E 1 , q ( 1 ) 2 D q , x ( 1 ) E n 1 , q ( x ) + ( q 1 E 0 , q ( 1 ) + 2 x ) q n 2 E n 1 , q ( x ) + E n , q ( q x ) = 0 .
Proof. 
Using the q-derivative, we can note
D q , t 2 e q ( t ) + 1 = 2 e q ( t ) ( e q ( t ) + 1 ) ( e q ( q t ) + 1 ) .
We consider the q-derivative after substituting q x instead of x in (4). From Equation (5), we have
D q , t F q ( t , q x ) = D q , t 2 e q ( t ) + 1 e q ( q t x ) = e q ( q t x ) 2 e q ( t ) ( e q ( t ) + 1 ) ( e q ( q t ) + 1 ) + 2 q x e q ( q t ) + 1 e q ( q t x ) = F q ( q t , x ) q x 1 e q ( t ) + 1 e q ( t ) = n = 0 q n + 1 x E n , q ( x ) 2 1 k = 0 n n q q n k E k , q ( 1 ) E n k , q ( x ) t n [ n ] q ! .
To make the calculations easier, we multiply t in Equation (6). Then, we find
t D q , t F q ( t , q x ) = n = 0 [ n ] q q n x E n 1 , q ( x ) 2 1 k = 0 n 1 n 1 k q q n k 1 E k , q ( 1 ) E n k 1 , q ( x ) t n [ n ] q ! .
Additionally, we can obtain the following equation from (4).
t D q , t F q ( t , q x ) = n = 0 [ n ] q E n , q ( q x ) t n [ n ] q ! .
By comparing the coefficients of Equations (7) and (8), we find
2 1 k = 0 n 1 n 1 k q q n k 1 E k , q ( 1 ) E n k 1 , q ( x ) = q n x E n 1 , q ( x ) E n , q ( q x ) .
From (i) in Lemma 1, we consider the following equation.
E n k 1 , q ( x ) = [ n k 1 ] q ! [ n 1 ] q ! D q , x ( k ) E n 1 , q ( x ) .
Substituting the right hand side of (10) to the left hand side of (9), we obtain
2 1 k = 0 n 1 n 1 k q q n k 1 E k , q ( 1 ) E n k 1 , q ( x ) = 2 1 k = 0 n 1 q n k 1 E k , q ( 1 ) [ k q ! ] D q , x ( k ) E n 1 , q ( x ) .
Using Equations (9) and (11), we complete the required result. □
Table 1. q-Euler numbers and polynomials.
We can see Corollaries 1 and 2 when q 1 in Theorem 3.
Corollary 1.
The Euler polynomial E n ( x ) is a solution of the following differential equation of a higher order.
E n 1 ( 1 ) 2 ( n 1 ) ! d n 1 d x n 1 E n 1 ( x ) + E n 2 ( 1 ) 2 ( n 2 ) ! d n 2 d x n 2 E n 1 ( x ) + + E 2 ( 1 ) 4 d 2 d x 2 E n 1 ( x ) + E 1 ( 1 ) 2 d d x E n 1 ( x ) + E 0 ( 1 ) + 2 x 2 E n 1 ( x ) + E n ( x ) = 0 .
Corollary 2.
In (9), one holds
2 E n ( x ) = 2 x E n 1 ( x ) k = 0 n 1 n 1 k E n k 1 ( 1 ) E k ( x ) ,
where E n ( x ) is the Euler polynomials.
Theorem 4.
The q-Euler polynomial E n , q ( x ) satisfies the following q-differential equation of a higher order.
l = 0 n 1 E l , q 2 [ n l 1 ] q ! [ l ] q ! D q , x ( n 1 ) E n 1 , q ( x ) + l = 0 n 2 q E l , q 2 [ n l 2 ] q ! [ l ] q ! D q , x ( n 2 ) E n 1 , q ( x ) + + l = 0 2 q n 3 E l , q 2 [ 2 l ] q ! [ l ] q ! D q , x ( 2 ) E n 1 , q ( x ) + l = 0 1 q n 2 E l , q 2 [ 1 l ] q ! [ l ] q ! D q , x ( 1 ) E n 1 , q ( x ) + ( q 1 E 0 , q 2 x ) q n 2 E n 1 , q ( x ) + E n , q ( q x ) = 0 ,
where E n , q is the q-Euler numbers.
Proof. 
To find the q-differential equation of higher order including q-Euler numbers, we transform Equation (6) as follows.
D q , t F q ( t , q x ) = n = 0 q n + 1 x E n , q ( x ) 2 1 k = 0 n l = 0 k n k q k l q q n k E l , q E n k 1 , q ( x ) t n [ n ] q ! .
From the similar method in Theorem 3, we find
2 1 k = 0 n 1 l = 0 k n 1 k q k l q q n k 1 E l , q E n k 1 , q ( x ) = q n x E n 1 , q ( x ) E n , q ( q x ) .
Using (i) in Lemma 1 in the left hand side of (12), we can find the desired result. □
From Theorem 4, we can find Corollaries 3 and 4 when q 1 .
Corollary 3.
The Euler polynomials E n ( x ) satisfy the following differential equation of a higher order.
l = 0 n 1 E l 2 ( n l 1 ) ! l ! d n 1 d x n 1 E n 1 ( x ) + l = 0 n 2 E l 2 ( n l 2 ) ! l ! d n 2 d x n 2 E n 1 ( x ) + + l = 0 2 E l 2 ( 2 l ) ! l ! d 2 d x 2 E n 1 ( x ) + l = 0 1 E l 2 ( 1 l ) ! l ! d d x E n 1 ( x ) + E 0 2 x 2 E n 1 ( x ) + E n ( x ) = 0 ,
where E n is the Euler numbers.
Corollary 4.
In Equation (12), the following holds:
2 1 k = 0 n 1 l = 0 k n 1 k k l E l E n k 1 ( x ) = x E n 1 ( x ) E n ( x ) ,
where E n is the Euler numbers and E n ( x ) is the Euler polynomials.
From Theorems 3 and 4, we obtain Corollary 5.
Corollary 5.
Let 0 < q < 1 . Then, one holds
k = 0 n 1 n 1 k q q n k 1 E k , q ( 1 ) E n k 1 , q ( x ) = k = 0 n 1 l = 0 k n 1 k q k l q q n k 1 E l , q E n k 1 , q ( x ) .
Theorem 5.
The q-Euler polynomials E n , q ( x ) are a solution of the following q-differential equation of a higher order.
E n 1 , q ( 1 ) 2 [ n 1 ] q ! D q , x ( n 1 ) E n 1 , q ( q 1 x ) + E n 2 , q ( 1 ) 2 [ n 2 ] q ! D q , x ( n 2 ) E n 1 , q ( q 1 x ) + + E 3 , q ( 1 ) 2 [ 3 ] q ! D q , x ( 3 ) E n 1 , q ( q 1 x ) + E 2 , q ( 1 ) 2 [ 2 ] q ! D q , x ( 2 ) E n 1 , q ( q 1 x ) + E 1 , q ( 1 ) 2 D q , x ( 1 ) E n 1 , q ( q 1 x ) + ( E 0 , q ( 1 ) 2 x ) 2 E n 1 , q ( q 1 x ) + q 1 n E n , q ( x ) = 0 .
Proof. 
Using the q-derivative in Equation (4), we have
t D q , t F q ( q t , x ) = n = 0 [ n ] q q n E n , q ( x ) t n [ n ] q ! .
Replacing q t instead of t and applying the q-derivative in (4), we also find
t D q , t F q ( q t , x ) = n = 0 [ n ] q q 2 n 1 x E n 1 , q ( q 1 x ) 2 1 k = 0 n 1 n 1 k q q 2 n k 1 E k , q ( 1 ) E n k 1 , q ( q 1 x ) t n [ n ] q ! .
Comparing the coefficients of Equations (12) and (13), we obtain
2 1 k = 0 n 1 n 1 k q q 2 n k 1 E k , q ( 1 ) E n k 1 , q ( q 1 x ) = q 2 n 1 x E n 1 , q ( q 1 x ) q n E n , q ( x ) .
From (ii) in Lemma 1, we note
E n k 1 , q ( q 1 x ) = q k [ n k 1 ] q ! [ n 1 ] q ! D q , x ( k ) E n 1 , q ( q 1 x ) .
Using (16) in the left hand side of (15), we derive
k = 0 n 1 n 1 k q q 2 n k 1 E k , q ( 1 ) E n k 1 , q ( q 1 x ) = k = 0 n 1 q 2 n 1 E k , q ( 1 ) [ k ] 1 ! D q , x ( k ) E n 1 , q ( q 1 x ) .
We can find a equation combining the right hand side of (17) and (15), which shows the required result. □
We find Corollary 6 when q 1 in Theorem 5.
Corollary 6.
The Euler polynomials E n ( x ) are a solution of the following differential equation of a higher order.
E n 1 ( 1 ) 2 ( n 1 ) ! d n 1 d x n 1 E n 1 ( x ) + E n 2 ( 1 ) 2 ( n 2 ) ! d n 2 d x n 2 E n 1 ( x ) + + E 3 ( 1 ) 2 ( 3 ) ! d 3 d x 3 E n 1 ( x ) + E 2 ( 1 ) 4 d 2 d x 2 E n 1 ( x ) + E 1 ( 1 ) 2 d d x E n 1 ( x ) + ( E 0 ( 1 ) 2 x ) 2 E n 1 ( x ) + E n ( x ) = 0 .
Theorem 6.
The q-Euler polynomials E n , q ( x ) are a solution of the following q-differential equation of a higher order.
l = 0 n 1 E l , q 2 [ n l 1 ] q ! [ l ] q ! D q , x ( n 1 ) E n 1 , q ( q 1 x ) + l = 0 n 2 E l , q 2 [ n l 2 ] q ! [ l ] q ! D q , x ( n 2 ) E n 1 , q ( q 1 x ) + + l = 0 2 E l , q 2 [ 2 l ] q ! [ l ] q ! D q , x ( 2 ) E n 1 , q ( q 1 x ) + l = 0 1 E l , q 2 [ 1 l ] q ! [ l ] q ! D q , x ( 1 ) E n 1 , q ( q 1 x ) + ( E 0 , q 2 x ) 2 E n 1 , q ( q 1 x ) + q 1 n E n , q ( x ) = 0 .
Proof. 
Substituting q 2 n , q 1 x instead of q n and x, respectively, in Corollary 3, we have
k = 0 n 1 n 1 k q q 2 n k 1 E k , q ( 1 ) E n k 1 , q ( q 1 x ) = k = 0 n 1 l = 0 k n 1 k q k l q q 2 n k 1 E l , q E n k 1 , q ( q 1 x ) .
Replacing (18) instead of (14), we derive
2 1 k = 0 n 1 l = 0 k n 1 k q k l q q k E l , q E n k 1 , q ( q 1 x ) = x E n 1 , q ( q 1 x ) q 1 n E n , q ( x ) .
From (16), the left hand side of (19) is changed as
2 1 k = 0 n 1 l = 0 k n 1 k q k l q q k E l , q E n k 1 , q ( q 1 x ) = 2 1 k = 0 n 1 l = 0 k E l , q [ k l ] q ! [ l ] q ! D q , x ( k ) E n 1 , q ( q 1 x ) .
Therefore, we have
2 1 k = 0 n 1 l = 0 k E l , q [ k l ] q ! [ l ] q ! D q , x ( k ) E n 1 , q ( q 1 x ) = x E n 1 , q ( q 1 x ) q 1 n E n , q ( x ) ,
which obtains the desired result by using the similar method in Theorem 4. □
Here, we have Corollary 7 when q 1 in Theorem 6.
Corollary 7.
The Euler polynomials E n ( x ) are a solution of the following differential equation of a higher order.
l = 0 n 1 E l 2 ( n l 1 ) ! l ! d n 1 d x n 1 E n 1 ( x ) + l = 0 n 2 E l 2 ( n l 2 ! l ! d n 2 d x n 2 E n 1 ( x ) + + l = 0 2 E l 2 ( 2 l ) ! l ! d 2 d x 2 E n 1 ( x ) + l = 0 1 E l 2 ( 1 l ) ! l ! d d x E n 1 ( x ) + ( E 0 2 x ) 2 E n 1 ( x ) + E n ( x ) = 0 .
Theorem 7.
Let a b 0 , x , X R and 0 < q < 1 . Then, we have
E n , q ( b x ) [ n ] q ! D q , X ( n ) E n , q ( a X ) + b E n 1 , q ( b x ) [ n 1 ] q ! D q , X ( n 1 ) E n , q ( a X ) + + b n 2 E 2 , q ( b x ) [ 2 ] q ! D q , X ( 2 ) E n , q ( a X ) + b n 1 E 1 , q ( b x ) D q , X ( 1 ) E n , q ( a X ) + b n E 0 , q ( b x ) E n , q ( a X ) = E n , q ( a x ) [ n ] q ! D q , X ( n ) E n , q ( b X ) + a E n 1 , q ( a x ) [ n 1 ] q ! D q , X ( n 1 ) E n , q ( b X ) + + a n 2 E 2 , q ( a x ) [ 2 ] q ! D q , X ( 2 ) E n , q ( b X ) + a n 1 E 1 , q ( a x ) D q , X ( 1 ) E n , q ( b X ) + a n E 0 , q ( a x ) E n , q ( b X ) .
Proof. 
To find the q-differential equation of a higher order using a symmetric property of q-Euler polynomials, we can construct form A, such as
A : = 4 e q ( a b t x ) e q ( a b t X ) ( e q ( a t ) + 1 ) ( e q ( b t ) + 1 ) .
Using the generating function of q-Euler polynomials and Cauchy products, form A is transformed as
A = n = 0 k = 0 n n k q a k b n k E k , q ( b x ) E n k , q ( a X ) t n [ n ] q !
and
A = n = 0 k = 0 n n k q b k a n k E k , q ( a x ) E n k , q ( b X ) t n [ n ] q ! .
Applying the coefficient comparison method on Equations (20) and (21), we find a symmetric property such as
k = 0 n n k q a k b n k E k , q ( b x ) E n k , q ( a X ) = k = 0 n n k q b k a n k E k , q ( a x ) E n k , q ( b X ) .
From (ii) in Lemma 1, we can remark
E n k , q ( α X ) = [ n k ] q ! α k [ n ] q ! D q , X ( k ) E n , q ( α X ) , for α 0 .
Using (23) in the both sides of (22), we obtain
k = 0 n b n k [ k ] q ! E k , q ( b x ) D q , X ( k ) E n , q ( a X ) = k = 0 n a n k [ k ] q ! E k , q ( a x ) D q , X ( k ) E n , q ( b X ) .
From the above equation, we express the required result and complete the proof of Theorem 7. □
Corollary 8.
Setting a = 1 in Theorem 7, we have
E n , q ( b x ) [ n ] q ! D q , X ( n ) E n , q ( X ) + b E n 1 , q ( b x ) [ n 1 ] q ! D q , X ( n 1 ) E n , q ( X ) + + b n 2 E 2 , q ( b x ) [ 2 ] q ! D q , X ( 2 ) E n , q ( X ) + b n 1 E 1 , q ( b x ) D q , X ( 1 ) E n , q ( X ) + b n E 0 , q ( b x ) E n , q ( X ) = E n , q ( x ) [ n ] q ! D q , X ( n ) E n , q ( b X ) + E n 1 , q ( x ) [ n 1 ] q ! D q , X ( n 1 ) E n , q ( b X ) + + E 2 , q ( x ) [ 2 ] q ! D q , X ( 2 ) E n , q ( b X ) + E 1 , q ( x ) D q , X ( 1 ) E n , q ( b X ) + E 0 , q ( x ) E n , q ( b X ) .
Corollary 9.
Let a b 0 , 0 < q < 1 and q 1 in Theorem 7. Then, the following holds
E n ( b x ) n ! d n d X n E n ( a X ) + b E n 1 ( b x ) ( n 1 ) ! d n 1 d X n 1 E n ( a X ) + + b n 2 E 2 ( b x ) 2 ! d 2 d X 2 E n ( a X ) + b n 1 E 1 ( b x ) d d X E n ( a X ) + b n E 0 ( b x ) E n ( a X ) = E n ( a x ) n ! d n d X n E n ( b X ) + a E n 1 ( a x ) ( n 1 ) ! d n 1 d X n 1 E n ( b X ) + + a n 2 E 2 ( a x ) 2 ! d 2 d X 2 E n ( b X ) + a n 1 E 1 ( a x ) d d X E n ( b X ) + a n E 0 ( a x ) E n ( b X ) .

4. Conclusions

In this paper, we find several q-differential equations for q-Euler polynomials and q-Genocchi polynomials. This work obtains symmetric properties of the q-differential equation, which is related to q-Euler and q-Genocchi polynomials. Based on this paper, we believe that many readers can generate and visualize new concepts for special polynomials.

Author Contributions

Conceptualization, J.-Y.K.; Formal analysis, J.-Y.K.; Investigation, C.-S.R.; Project administration, C.-S.R. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Institutional Review Board Statement

Not applicable.

Data Availability Statement

The data presented in this study is available on request from the corresponding author.

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Bijay, K.S. Fluid Mechanics and Turbomachinery; CRC Press: London, UK; New York, NY, USA, 2021. [Google Scholar]
  2. Bayad, A.; Hamahata, Y. Identities involving two kinds of q-Euler polynomials and numbers. J. Integer Seq. 2012, 15, 14. [Google Scholar]
  3. Mahmudov, N.I. On a class of generalized q-Bernoulli and q-Euler polynomials. Adv. Differ. Equ. 2013, 2013, 1–10. [Google Scholar] [CrossRef] [Green Version]
  4. Jackson, H.F. q-Difference equations. Am. J. Math. 1910, 32, 305–314. [Google Scholar] [CrossRef]
  5. Jackson, H.F. On q-functions and a certain difference operator. Earth Environ. Sci. Trans. R. Soc. Edinb. 2013, 46, 253–281. [Google Scholar] [CrossRef]
  6. Bangerezako, G. An Introduction to q-Difference Equations; Preprint; Bujumbura, Burundi. 2007. Available online: https://perso.uclouvain.be/alphonse.magnus/gbang/qbook712.pdf (accessed on 22 February 2022).
  7. Carmichael, R.D. The general theory of linear q-qifference equations. Am. J. Math. 1912, 34, 147–168. [Google Scholar] [CrossRef]
  8. Charalambides, C.A. On the q-differences of the generalized q-factorials. J. Statist. Plann. Inference 1996, 54, 31–43. [Google Scholar] [CrossRef]
  9. Floreanini, R.; Vinet, L. q-orthogonal polynomials and the oscillator quantum group. Lett. Math. Phys. 1991, 22, 45–54. [Google Scholar] [CrossRef]
  10. Hajli, M. On a formula for the regularized determinant of zeta functions with application to some Dirichlet series. Q. J. Math. 2020, 71, 843–865. [Google Scholar] [CrossRef]
  11. Mason, T.E. On properties of the solution of linear q-difference equations with entire function coefficients. Am. J. Math. 1915, 37, 439–444. [Google Scholar] [CrossRef]
  12. Rawlings, D. Limit formulas for q-exponetial functions. Discrete Math. 1994, 126, 379–383. [Google Scholar] [CrossRef] [Green Version]
  13. Kemp, A. Certain q-analogues of the binomial distribution. Sankhyā Indian J. Stat. Ser. A 2002, 64, 293–305. [Google Scholar]
  14. Konvalina, J. A unified interpretation of the binomial coefficients, the Stirling numbers, and the Gaussian coefficients. Ame. Math. Mon. 2000, 107, 901–910. [Google Scholar] [CrossRef]
  15. Victor, K.; Pokman, C. Quantum Calculus Universitext; Springer: New York, NY, USA, 2002; ISBN 0-387-95341-8. [Google Scholar]
  16. Luo, Q.M.; Srivastava, H.M. q-extension of some relationships between the Bernoulli and Euler polynomials. Taiwan. J. Math. 2011, 15, 241–257. [Google Scholar] [CrossRef]
  17. Milovanovic, G.V.; Rassias, M.T. Analytic Number Theory, Approximation Theory and Special Functions; Springer: New York, NY, USA, 2016; ISBN 978-1-4939-0258-3. [Google Scholar]
  18. Ostrovska, S. q-Bernstein polynomials and their iterates. J. Approx. Theory 2003, 123, 232–255. [Google Scholar] [CrossRef] [Green Version]
  19. Phillips, G.M. Bernstein polynomials based on q-integers. Ann. Numer. Anal. 1997, 4, 511–518. [Google Scholar]
  20. Ryoo, C.S. A note on the zeros of the q-Bernoulli polynomials. J. Appl. Math. Inform. 2010, 28, 805–811. [Google Scholar]
  21. Ryoo, C.S.; Kim, T.; Agarwal, R.P. A numerical investigation of the roots of q-polynomials. Inter. J. Comput. Math. 2006, 83, 223–234. [Google Scholar] [CrossRef]
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