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Article

A Parametric Kind of Fubini Polynomials of a Complex Variable

by
Sunil Kumar Sharma
1,*,
Waseem A. Khan
2 and
Cheon Seoung Ryoo
3
1
College of Computer and Information Sciences, Majmaah University, Majmaah 11952, Saudi Arabia
2
Department of Mathematics and Natural Sciences, Prince Mohammad Bin Fahd University, P.O. Box 1664, Al Khobar 31952, Saudi Arabia
3
Department of Mathematics, Hannam University, Daejeon 34430, Korea
*
Author to whom correspondence should be addressed.
Mathematics 2020, 8(4), 643; https://doi.org/10.3390/math8040643
Submission received: 31 March 2020 / Revised: 15 April 2020 / Accepted: 16 April 2020 / Published: 22 April 2020
(This article belongs to the Special Issue Special Polynomials)

Abstract

:
In this paper, we propose a parametric kind of Fubini polynomials by defining the two specific generating functions. We also investigate some analytical properties (for example, summation formulae, differential formulae and relationships with other well-known polynomials and numbers) for our introduced polynomials in a systematic way. Furthermore, we consider some relationships for parametric kind of Fubini polynomials associated with Bernoulli, Euler, and Genocchi polynomials and Stirling numbers of the second kind.

1. Introduction

Mathematicians and other scientists have studied trigonometric functions, special numbers, and polynomials, and their applications because these functions have various mathematical usages which include derivative, integral and other algebraic properties. By using these functions with their functional equations and derivative equations, various properties of these special numbers and polynomials have been investigated (see [1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26]). By using these functions with a trigonometric function, we not only study some special families of polynomials and numbers including the Bernoulli, Euler, and Genocchi polynomials, but also derive some identities and relationships for these polynomials and numbers.
The classical Bernoulli polynomials B j ( u ) , the classical Euler polynomials E j ( u ) and the classical Genocchi polynomials G j ( u ) are usually defined by means of the following generating functions
z e z 1 e u z = j = 0 B j ( u ) z j j ! , ( z < 2 π )
2 e z + 1 e u z = j = 0 E j ( u ) z j j ! , ( z < π )
and
2 z e z + 1 e u z = j = 0 G j ( u ) z j j ! , ( z < π )
respectively. Each of these polynomials has been extensively studied in many recent works, (see [18,19]).
The Geometric (also known as Fubini) polynomials [1] are defined by
1 1 u ( e z 1 ) = j = 0 F j ( u ) z j j ! ,
so that
F j ( u ) = k = 0 j k ! S 2 ( j , k ) u k = k = 0 j j k k ! u k ,
where j k are called the Stirling numbers of second kind, (see [13,17]).
On setting u = 1 in (4), we obtain
1 2 e z = j = 0 F j z j j ! ,
where F j are called the jth Fubini numbers or ordered Bell numbers, (see [4,26])
A few numbers of these polynomials are
F 0 ( u ) = 1 , F 1 ( u ) = u , F 2 ( u ) = u + 2 u 2 ,
F 3 ( u ) = u + 6 u 2 + 6 u 3 , F 4 ( u ) = u + 14 u 2 + 36 u 3 + 24 u 4 ,
and
F 0 = 1 , F 1 = 1 , F 2 = 3 , F 3 = 13 , F 4 = 75 .
The Stirling numbers of the first kind are defined by the coefficients in the expansion of ( u ) j in terms of powers of u as follows, (see [14])
( u ) j = u ( u 1 ) ( u j + 1 ) = l = 0 j S 1 ( j , l ) u l , ( j 0 ) ,
and the Stirling numbers of the second kind are defined by (see [15,16])
( e z 1 ) j = j ! l = j S 2 ( l , j ) z l l ! , ( j 0 ) .
Recently, Masjed-Jamei et al. [6,7,8,9] and Srivastava et al. [23,24,25] introduced and studied the parametric kind of the two exponential generating functions e u z cos v z and e u z sin v z are defined by
e u z cos v z = k = 0 C k ( u , v ) z k k ! ,
and
e u z sin v z = k = 0 S k ( u , v ) z k k ! ,
where
C k ( u , v ) = j = 0 [ k 2 ] ( 1 ) j k 2 j u k 2 j v 2 j ,
and
S k ( u , v ) = j = 0 [ k 1 2 ] ( 1 ) j k 2 j + 1 u k 2 j 1 v 2 j + 1 .
In (2018), Kim and Ryoo [11] introduced the cosine-Bernoulli polynomials of a complex variable, the sine-Bernoulli polynomials of a complex variable and the cosine-Euler polynomials of a complex variable, the sine-Euler polynomials of a complex variable, respectively are defined as follows
z e z 1 e ( u + i v ) z = j = 0 B j ( u + i v ) z j j ! ,
and
2 e z + 1 e ( u + i v ) z = j = 0 E j ( u + i v ) z j j ! .
From (13) and (14), we get
z e z 1 e u z cos v z = j = 0 B j ( u + i v ) + B j ( u i v ) 2 z j j ! = j = 0 B j ( c ) ( u , v ) z j j ! ,
and
2 e z 1 e u z sin v z = j = 0 B j ( u + i v ) B j ( u i v ) 2 i z j j ! = j = 0 B j ( s ) ( u , v ) z j j ! ,
2 e z + 1 e u z cos v z = j = 0 E j ( u + i v ) + E j ( u i v ) 2 z j j ! = j = 0 E j ( c ) ( u , v ) z j j ! ,
and
2 e z + 1 e u z sin v z = j = 0 E j ( u + i v ) E j ( u i v ) 2 i z j j ! = j = 0 E j ( s ) ( u , v ) z j j ! .
The main object of this paper is as follows. In Section 2, we consider generating a function for the parametric type of Fubini numbers and polynomials of a complex variable and give some basic properties of these polynomials. In Section 3, we derive recurrence relations, differentiation, summation formulae of parametric Fubini-type polynomials. In Section 4, we construct relationships for parametric Fubini-type polynomials associated with Bernoulli, Euler, Genocchi polynomials and Stirling numbers of the second kind.

2. Two Parametric Kind of the Fubini Polynomials of Complex Variable

In this section, we introduce the cosine-Fubini polynomials and sine-Fubini polynomials by splitting complex Fubini polynomials into real and imaginary parts and present some basic properties. Now, we consider the Fubini polynomials that are given by the generating function
1 1 w ( e z 1 ) e ( u + i v ) z = j = 0 F j ( u + i v ; w ) z j j ! .
The well-known Euler’s formula is defined as follows (see [11])
e ( u + i v ) z = e u z e i v z = e u z ( cos v z + i sin v z ) .
Using (15) and (16), we have
j = 0 F j ( u + i v ; w ) z j j ! = 1 1 w ( e z 1 ) e ( u + i v ) z = 1 1 w ( e z 1 ) e u z ( cos v z + i sin v z ) ,
and
j = 0 F j ( u i v ; w ) z j j ! = 1 1 w ( e z 1 ) e ( u i v ) z = 1 1 w ( e z 1 ) e u z ( cos v z i sin v z ) .
From (17) and (18), we get
1 1 w ( e z 1 ) e u z cos v z = j = 0 F j ( u + i v ; w ) + F j ( u i v ; w ) 2 z j j ! ,
and
1 1 w ( e z 1 ) e u z sin v z = j = 0 F j ( u + i v ; w ) F j ( u i v ; w ) 2 i z j j ! .
Definition 1.
Two parametric kinds of Fubini polynomials or the cosine-Fubini polynomials F j ( c ) ( u , v ; w ) and sine-Fubini polynomials F j ( s ) ( u , v ; w ) for nonnegative integer j are defined by
1 1 w ( e z 1 ) e u z cos v z = j = 0 F j ( c ) ( u , v ; w ) z j j ! ,
and
1 1 w ( e z 1 ) e u z sin v z = j = 0 F j ( s ) ( u , v ; w ) z j j ! ,
respectively.
It is clear that
F n ( c ) ( u , 0 ; w ) = F n ( c ) ( u ; w ) , F n ( s ) ( u , 0 ; w ) = 0 , F n ( c ) ( 0 , v ; w ) = F n ( c ) ( v ; w ) ,
F n ( s ) ( 0 , v ; w ) = F n ( s ) ( v ; w ) , F n ( c ) ( 0 , 0 ; 1 ) = F n ( c ) , F n ( s ) ( 0 , 0 ; w ) = 0 .
The first few follow immediately from this generating function:
F 0 ( c ) ( u , v ; w ) = 1 , F 1 ( c ) ( u , v ; w ) = u + w , F 2 ( c ) ( u , v ; w ) = u 2 v 2 + w + 2 u w + 2 w 2 , F 3 ( c ) ( u , v ; w ) = u 3 3 u v 2 + w + 3 u w + 3 u 2 w 3 v 2 w + 6 w 2 + 6 u w 2 + 6 z 3 , F 4 ( c ) ( u , v ; w ) = u 4 6 u 2 v 2 + v 4 + w + 4 u w + 6 u 2 w + 4 u 3 w 6 v 2 w 12 u v 2 w + 14 w 2 + 24 u w 2 + 12 u 2 w 2 12 v 2 w 2 + 36 w 3 + 24 u w 3 + 24 w 4 ,
and
F 0 ( s ) ( u , v ; w ) = 0 , F 1 ( s ) ( u , v ; w ) = v , F 2 ( s ) ( u , v ; w ) = 2 u v + 2 v w , F 3 ( s ) ( u , v ; w ) = 3 u 2 v v 3 + 3 v w + 6 u v w + 6 v w 2 , F 4 ( s ) ( u , v ; w ) = 4 u 3 v 4 u v 3 + 4 v w + 12 u v w + 12 u 2 v w 4 v 3 w + 24 v w 2 + 24 u v w 2 + 24 v w 3 .
From (19)–(22), we find
F j ( c ) ( u , v ; w ) = F j ( u + i v ; w ) + F j ( u i v ; w ) 2 ,
F j ( s ) ( u , v ; w ) = F j ( u + i v ; w ) F j ( u i v ; w ) 2 i .
Remark 1.
Taking u = 0 in (21) and (22), we get new type of polynomials as follows
1 1 w ( e z 1 ) cos v z = j = 0 F j ( c ) ( 0 , v ; w ) z j j ! ,
and
1 1 w ( e z 1 ) sin v z = j = 0 F j ( s ) ( 0 , v ; w ) z j j ! ,
respectively.
Remark 2.
For w = 1 2 in (19) and (20), we have
2 e z + 1 e u z cos v z = j = 0 E j ( u + i v ) + E j ( u i v ) 2 z j j ! ,
and
2 e z + 1 e u z sin v z = j = 0 E j ( u + i v ) E j ( u i v ) 2 i z j j ! ,
(see [11]).
Remark 3.
For w = 1 2 in (21) and (22), we get
j = 0 F j ( c ) u , v ; 1 2 z j j ! = 2 e z + 1 e u z cos v z = j = 0 E j ( c ) ( u , v ) z j j ! ,
and
j = 0 F j ( s ) u , v ; 1 2 z j j ! = 2 e z + 1 e u z sin v z = j = 0 E j ( s ) ( u , v ) z j j ! ,
(see [6]).
Now, we start some basic properties of these polynomials.
Theorem 1.
Let j 0 , we have
F j ( c ) ( 0 , v ; w ) = r = 0 [ j 2 ] j 2 r ( 1 ) r v 2 r F j 2 r ( w ) ,
and
F j ( s ) ( 0 , v ; w ) = r = 0 [ j 1 2 ] j 2 r + 1 ( 1 ) r v 2 r + 1 F j 2 r 1 ( w ) .
Proof. 
From (23) and (24), we have
j = 0 F j ( c ) ( 0 , v ; w ) z j j ! = 1 1 w ( e z 1 ) cos v z
= j = 0 F j ( w ) z j j ! r = 0 ( 1 ) r v 2 r z 2 r ( 2 r ) ! .
= j = 0 r = 0 [ j 2 ] j 2 r ( 1 ) r v 2 r F j 2 r ( w ) z j j ! ,
and
j = 0 F j ( s ) ( 0 , v ; w ) z j j ! = 1 1 w ( e z 1 ) sin v z
= j = 0 r = 0 [ j 1 2 ] j 2 r + 1 ( 1 ) r v 2 m + 1 F j 2 r 1 ( w ) z j j ! .
Therefore, by (27) and (28), we get the results (25) and (26). □
Theorem 2.
Let j 0 , we have
F j ( u + i v ; w ) = r = 0 j j r ( u + i v ) j r F r ( w )
= r = 0 j j r ( i v ) j r F r ( u ; w ) ,
and
F j ( u i v ; w ) = r = 0 j j r ( u i v ) j r F r ( w )
= r = 0 j j r ( 1 ) j r ( i v ) j r F r ( u ; w ) .
Proof. 
By using (17) and (18), we can easily get. So we omit the proof. □
Theorem 3.
Let j 0 and v 0 . Then
F j ( c ) ( u , v ; w ) = H j ( c ) u , v ; 1 + w w ,
and
F j ( s ) ( u , v ; w ) = H j ( s ) u , v ; 1 + w w ,
where H j ( u ) are called the Frobenius–Euler polynomials, (see [10,12]).
Proof. 
By (21), we have
j = 0 F j ( c ) ( u , v ; w ) z j j ! = 1 1 w ( e z 1 ) e u z cos v z
= 1 1 + w w e z 1 + w w e u z cos v z
= j = 0 H j ( c ) u , v ; 1 + w w z j j ! .
Comparing the coefficients of t n n ! on both sides, we obtain (31). The proof of (32) is similar. □
Theorem 4.
Let j 0 , we have
F j ( c ) ( u , v ; w ) = k = 0 n j k F k ( w ) C j k ( u , v ) ,
F j ( s ) ( u , v ; w ) = k = 0 j j k F k ( w ) S j k ( u , v ) .
Proof. 
Using Equations (9), (10), (21) and (22), we can easily obtain the results (33) and (34). We omit the proof. □
Theorem 5.
Let j 0 , we have
C j ( u , v ) = F j ( c ) ( u , v ; w ) w F j ( c ) ( u + 1 , v ; w ) + w F j ( c ) ( u , v ; w ) ,
S j ( u , v ) = F j ( s ) ( u , v ; w ) w F j ( s ) ( u + 1 , v ; w ) + w F j ( s ) ( u , v ; w ) .
Proof. 
From (21), we have
e u z cos v z = 1 w ( e z 1 ) 1 w ( e z 1 ) e u z cos v z
= e u z cos v z 1 w ( e z 1 ) w ( e z 1 ) 1 w ( e z 1 ) e u z cos v z .
By using (9) and (21), we have
j = 0 C j ( u , v ) z j j !
= j = 0 F j ( c ) ( u , v ; w ) w F j ( c ) ( u + 1 , v ; w ) + w F j ( c ) ( u , v ; w ) z j j ! ,
which proves the desired result (35). The proof of (36) is similar. □
Theorem 6.
Let j 0 , we have
w F j ( c ) ( u + 1 , v ; w ) = ( 1 + w ) F j ( c ) ( u , v ; w ) C j ( u , v ) ,
w F j ( s ) ( u + 1 , v ; w ) = ( 1 + w ) F j ( s ) ( u , v ; w ) S j ( u , v ) .
Proof. 
From (21), we see
j = 0 F j ( c ) ( u + 1 , v ; w ) F j ( c ) ( u , v ; w ) z j j !
= e u z cos v z 1 w ( e z 1 ) ( e z 1 )
= 1 w e u z cos v z 1 w ( e z 1 ) e u z cos v z
= 1 w j = 0 F j ( c ) ( u , v ; w ) C j ( u , v ) z j j ! ,
which yields the obtained result (37). The proof of (38) is similar. □
Theorem 7.
For every j N , we have
u F j ( c ) ( u , v ; w ) = j F j 1 ( c ) ( u , v ; w ) ,
v F j ( c ) ( u , v ; w ) = j F j 1 ( s ) ( u , v ; w ) ,
and
u F j ( s ) ( u , v ; w ) = j F j 1 ( s ) ( u , v ; w ) ,
v F j ( s ) ( u , v ; w ) = j F j 1 ( c ) ( u , v ; w ) .
Proof. 
From (21), we have
j = 1 u F j ( c ) ( u , v ; w ) z j j ! = u e u z cos v z 1 w ( e z 1 ) = j = 0 F j ( c ) ( u , v ; w ) z j + 1 j !
= j = 0 F j 1 ( c ) ( u , v ; w ) z j ( j 1 ) ! = j = 1 j F j 1 ( c ) ( u , v ; w ) z j j ! ,
proving (39). Other (40)–(42) can be similarly derived. □
Theorem 8.
Let j 0 , we have
F j ( c ) ( 1 + u , v ; w ) = r = 0 j j r F j r ( c ) ( u , v ; w ) ,
F j ( s ) ( 1 + u , v ; w ) = r = 0 j j r F j r ( s ) ( u , v ; w ) .
Proof. 
Using the generating function (21), we have
j = 0 F j ( c ) ( 1 + u , v ; w ) z j j ! j = 0 F j ( c ) ( u , v ; w ) z j j !
= 1 1 w ( e z 1 ) ( e z 1 ) e u z cos v z
= j = 0 F j ( c ) ( u , v ; w ) z j j ! r = 0 z r r ! 1
= j = 0 F j ( c ) ( u , v ; w ) z j j ! r = 0 z r r ! j = 0 F j ( c ) ( u , v ; w ) z j j !
= j = 0 r = 0 j j r F j r ( c ) ( u , v ; w ) z j j ! j = 0 F j ( c ) ( u , v ; w ) z j j ! ,
which gives the claimed result (43). The proof of (44) is similar. □
Theorem 9.
For j 0 and u 1 u 2 . Then
k = 0 j j k F j k ( c ) ( u 1 , v 1 ; w 1 ) F k ( c ) ( u 2 , v 2 ; w 2 )
= w 2 F j ( c ) ( u 1 + u 2 , v 1 + v 2 ; w 2 ) w 1 F j ( c ) ( u 1 + u 2 , v 1 + v 2 ; w 1 ) w 2 w 1 ,
and
k = 0 j j k F j k ( s ) ( u 1 , v 1 ; w 1 ) F k ( s ) ( u 2 , v 2 ; w 2 )
= w 2 F j ( s ) ( u 1 + u 2 , u 1 + u 2 ; w 2 ) w 1 F j ( s ) ( u 1 + u 2 , v 1 + v 2 ; w 1 ) w 2 w 1 .
Proof. 
Equation (21) can be written as
j = 0 k = 0 F j ( c ) ( u 1 , v 1 ; w 1 ) F k ( c ) ( u 2 , v 2 ; w 2 ) z j j ! z k k !
= e u 1 z cos ( v 1 z ) 1 w 1 ( e z 1 ) e u 2 z cos ( v 2 z ) 1 w 2 ( e z 1 )
j = 0 k = 0 j j k F j k ( c ) ( u 1 , v 1 ; w 1 ) F k ( c ) ( u 2 , v 2 ; w 2 ) z j j !
= w 2 w 2 w 1 e ( u 1 + u 2 ) z cos [ ( v 1 + v 2 ) z ] 1 w 1 ( e z 1 ) w 1 w 2 w 1 e ( u 1 + u 2 ) z cos [ ( v 1 + v 2 ) z ] 1 w 2 ( e z 1 )
= j = 0 w 2 F j ( c ) ( u 1 + u 2 , v 1 + v 2 ; w 2 ) w 1 F j ( c ) ( u 1 + u 2 , v 1 + v 2 ; w 1 ) w 2 w 1 z j j ! .
By equating the coefficients of z j j ! on both sides, we get (45). The proof of (46) is similar. □
Theorem 10.
For j 0 , we have
( 1 + w ) F j ( c ) ( u , v ; w ) = w k = 0 j j k F j k ( c ) ( u , v ; w ) + C j ( u , v ) ,
and
( 1 + w ) F j ( s ) ( u , v ; w ) = w k = 0 j j k F j k ( s ) ( u , v ; w ) + S j ( u , v ) .
Proof. 
Consider the following identity
1 + w ( 1 w ( e z 1 ) ) w e z = 1 1 w ( e z 1 ) + 1 w e z .
Using above identity by partial fraction, we find
( 1 + w ) e u z cos v z ( 1 w ( e z 1 ) ) w e z = e u z cos v z 1 w ( e z 1 ) + e u z cos v z w e z
( 1 + w ) j = 0 F j ( c ) ( u , v ; w ) z j j !
= w j = 0 F j ( c ) ( u , v ; w ) z j j ! k = 0 z k k ! + j = 0 C j ( u , v ) z j j ! ,
which implies the desired result (47). The proof of (48) is similar. □

3. Relationship between Appell-Type Polynomials

In this section, we prove some relationships for parametric Fubini-type polynomials related to Bernoulli, Euler, and Genocchi polynomials and Stirling numbers of the second kind. We start the following theorem.
Theorem 11.
For j 0 , we have
F j ( c ) ( u , v ; w ) = r = 0 j + 1 j + 1 r k = 0 r r k B r k ( u ) B r ( u ) F j + 1 r ( c ) ( 0 , v ; w ) j + 1 ,
and
F j ( s ) ( u , v ; w ) = r = 0 j + 1 j + 1 r k = 0 r r k B r k ( u ) B r ( u ) F j + 1 r ( s ) ( 0 , v ; w ) j + 1 .
Proof. 
From (1) and (21), we have
1 1 w ( e z 1 ) e u z cos v z = 1 1 w ( e z 1 ) z e z 1 e z 1 z e u z cos v z = 1 z j = 0 k = 0 s s k B s k ( u ) z s s ! j = 0 F j ( c ) ( 0 , v ; w ) z j j ! 1 z s = 0 B s ( u ) z s s ! j = 0 F j ( c ) ( 0 , v ; w ) z j j ! = 1 z j = 0 r = 0 j j r k = 0 r r k B r k ( u ) F j r ( c ) ( 0 , v ; w ) z j j ! 1 z j = 0 r = 0 j j r B r ( v ) F j r ( c ) ( 0 , v ; w ) z j j ! ,
which gives the required result (49). The proof of (50) is similar. □
Theorem 12.
For j 0 , we have
F j ( c ) ( u , v ; w ) = r = 0 j j r k = 0 r r k E r k ( u ) + E r ( u ) F j r ( c ) ( 0 , v ; w ) 2 ,
and
F j ( s ) ( u , v ; w ) = r = 0 j j r k = 0 r r k E r k ( u ) + E r ( u ) F j r ( s ) ( 0 , v ; w ) 2 .
Proof. 
By using (2) and (21), we have
1 1 w ( e z 1 ) e u z cos v z = 1 1 w ( e z 1 ) 2 e z + 1 e z + 1 2 e u z cos v z = 1 2 j = 0 k = 0 j j k E j k ( u ) z j j ! + j = 0 E j ( u ) z j j ! × j = 0 F j ( c ) ( 0 , v ; w ) z j j ! = 1 2 j = 0 r = 0 j j r k = 0 r r k E r k ( u ) + r = 0 j j r E r ( u ) × F j r ( c ) ( 0 , v ; w ) z j j ! ,
which arrives the desired result (51). The proof of (52) is similar. □
Theorem 13.
For j 0 , we have
F j ( c ) ( u , v ; w ) = 1 2 r = 0 j + 1 j + 1 r k = 0 r r k G r k ( u ) + G r ( u ) F j + 1 r ( c ) ( 0 , v ; w ) j + 1 ,
and
F j ( s ) ( u , v ; w ) = 1 2 r = 0 j + 1 j + 1 r k = 0 r r k G r k ( u ) + G r ( u ) F j + 1 r ( s ) ( 0 , v ; w ) j + 1 .
Proof. 
From (3) and (21), we have
1 1 w ( e z 1 ) e u z cos v z = 1 1 w ( e z 1 ) 2 z e z + 1 e z + 1 2 z e u z cos v z = 1 2 z j = 0 k = 0 j j k G j k ( u ) z j j ! + j = 0 G j ( u ) z j j ! × j = 0 F j ( c ) ( 0 , v ; w ) z j j ! ,
yields the asserted result (53). The proof of (54) is similar. □
Theorem 14.
For j 0 , we have
F j ( c ) ( u , v ; w ) = r = 0 j j r C j r ( u , v ) k = 0 r z k k ! S 2 ( r , k ) ,
and
F j ( s ) ( u , v ; w ) = r = 0 j j r S j r ( u , v ) k = 0 r z k k ! S 2 ( r , k ) .
Proof. 
From (8) and (21), we have
j = 0 F j ( c ) ( u , v ; w ) z j j ! = 1 1 w ( e z 1 ) e u z cos v z
= e u z cos v z k = 0 z k ( e z 1 ) k
= e u z cos v z k = 0 z k r = k k ! S 2 ( r , k ) z r r !
= j = 0 C j ( u , v ) z j j ! r = 0 z k k = 0 r k ! S 2 ( r , k ) z r r ! .
Replacing j by j r in above equation, we get
j = 0 F j ( c ) ( u , v ; w ) z j j !
= j = 0 r = 0 j j r C j r ( u , v ) k = 0 r z k k ! S 2 ( r , k ) z j j ! ,
which gives the asserted result (55). The proof of (56) is similar. □
Theorem 15.
Let j 0 , we have
F j ( c ) ( u + α , v ; w ) = r = 0 j j r C j r k = 0 r w k k ! S 2 ( r + α , k + α ) ,
and
F j ( s ) ( u + α , v ; w ) = r = 0 j j r S j r k = 0 r w k k ! S 2 ( r + α , k + α ) .
Proof. 
Replacing u by u + α in (21) and using the result ([2], p. 250, Theorem 16), we have
j = 0 F j ( c ) ( u + α , v ; w ) z j j ! = 1 1 w ( e z 1 ) e ( u + α ) z cos v z
= e u z cos v z e α z k = 0 w k ( e z 1 ) k
= e u z cos v z e α z k = 0 w k r = k k ! S 2 ( r , k ) z r r !
= j = 0 C j ( u , v ) z j j ! r = 0 w k k = 0 r k ! S 2 ( r + α , k + α ) z r r ! .
Replacing j by j r in above equation, we get
j = 0 F j ( c ) ( u + α , v ; w ) z j j !
= j = 0 r = 0 j j r C j r ( u , v ) k = 0 r w k k ! S 2 ( r + α , k + α ) z j j ! .
Equating the coefficients of z j on both sides, we get (57). The proof of (58) is similar. □
Theorem 16.
Let j 0 , we have
F j ( c ) ( u , v ; w ) = r = 0 i = r j j i ( u ) r S 2 ( i , r ) F j i ( c ) ( 0 , v ; w ) ,
and
F j ( s ) ( u , v ; w ) = r = 0 i = r j j i ( u ) r S 2 ( i , r ) F j i ( s ) ( 0 , v ; w ) .
Proof. 
From (7) and (21), we find
j = 0 F j ( c ) ( u , v ; w ) z j j ! = 1 1 w ( e z 1 ) ( ( e z 1 ) + 1 ) u cos v z
= Li k ( 1 e z ) e z 1 j = 0 u r ( e z 1 ) l
= r = 0 ( u ) r ( e z 1 ) r r ! 1 1 w ( e z 1 ) cos v z
= r = 0 ( u ) r i = 0 S 2 ( i , r ) z i i ! j = 0 F j ( c ) ( 0 , v ; w ) z j j !
= j = 0 r = 0 i = r j j i ( u ) r S 2 ( i , r ) F j i ( c ) ( 0 , v ; w ) z j j ! ,
which provides the claimed result (59). The proof of (60) is similar. □
Theorem 17.
For j 0 , we have
F j ( c ) ( u + α , v ; w ) = r = 0 j k = 0 j j r F j r ( c ) ( u , v ; w ) S 2 ( r , k ) ( α ) k ,
and
F j ( s ) ( u + α , v ; w ) = r = 0 j k = 0 j j r F j r ( s ) ( u , v ; w ) S 2 ( r , k ) ( α ) k .
Proof. 
From (8) and (21), we see
j = 0 F j ( c ) ( u , v ; w ) z j j ! = 1 1 w ( e z 1 ) e u z cos v z e α z
= j = 0 F j ( c ) ( u , v ; w ) z j j ! r = 0 α r z r r !
= j = 0 r = 0 j j r F j r ( c ) ( u , v ; w ) α r z r r !
= j = 0 r = 0 j j r F j r ( c ) ( u , v ; w ) z j j ! k = 0 r S 2 ( r , k ) ( α ) k
= j = 0 r = 0 j k = 0 j j r F j r ( c ) ( u , v ; w ) S 2 ( r , k ) ( α ) k z j j ! .
Equating the coefficients z j on both sides, we get (61). The proof of (62) is similar. □
Theorem 18.
For j 0 , we have
F j ( c ) ( u , v ; w ) = k = 0 l = k j j l F j l ( c ) ( k , v ; w ) S 2 ( l , k ) ( u ) ( k ) ,
and
F j ( s ) ( u , v ; w ) = k = 0 l = k j j l F j l ( s ) ( k , v ; w ) S 2 ( l , k ) ( u ) ( k ) .
Proof. 
From Equations (8) and (21), we determine
j = 0 F j ( c ) ( u , v ; w ) z j j ! = cos v z 1 w ( e z 1 ) e u z
= cos v z 1 w ( e z 1 ) ( e z ) u = cos v z 1 w ( e z 1 ) k = 0 u + k 1 k ( 1 e z ) k
= cos v z 1 w ( e z 1 ) k = 0 ( u ) ( k ) ( e z 1 ) k k ! e k z
= k = 0 ( u ) ( k ) j = 0 F j ( c ) ( k , v ; w ) z j j ! l = 0 S 2 ( l , k ) z l l !
= k = 0 ( u ) ( k ) j = 0 l = 0 j j l F j l ( c ) ( k , v ; w ) S 2 ( l , k ) z j j ! .
Comparing the coefficients z j on both sides, we get (63). The proof of (64) is similar. □

4. Conclusions

In our present investigation, we have introduced and studied systematically two parametric families of Fubini polynomials F j ( c ) ( u , v ; w ) and F j ( s ) ( u , v ; w ) , which are defined using two specific generating functions. We have derived several fundamental properties of these parametric kinds of Fubini polynomials and such other polynomials as the parametric kind Bernoulli, Euler, and Genocchi polynomials. Lastly, we show that complex cosine-Fubini polynomials and complex sine-Fubini polynomials can be bespoke in terms of first- and second-form Stirling numbers.

Author Contributions

Conceptualization, S.K.S.; formal analysis, W.A.K.; investigation, S.K.S., W.A.K. and C.S.R.; project administration, W.A.K.; supervision, C.S.R.; funding acquisition, S.K.S; writing—original draft, S.K.S. and W.A.K. All authors contributed equally to the manuscript and all authors have read and agreed to the published version of the manuscript.

Funding

Sunil Kumar Sharma would like to thank Deanship of Scientific Research at Majmaah University for supporting this work under the Project No. R-1441-113.

Acknowledgments

Sunil Kumar Sharma would like to acknowledge Mohammed Alshehri, College of Computer and Information Sciences, Majmaah University for his encouragement. The authors would like to thank the referees for their valuable comments and suggestions.

Conflicts of Interest

The authors declare no conflict of interest.

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Sharma, S.K.; Khan, W.A.; Ryoo, C.S. A Parametric Kind of Fubini Polynomials of a Complex Variable. Mathematics 2020, 8, 643. https://doi.org/10.3390/math8040643

AMA Style

Sharma SK, Khan WA, Ryoo CS. A Parametric Kind of Fubini Polynomials of a Complex Variable. Mathematics. 2020; 8(4):643. https://doi.org/10.3390/math8040643

Chicago/Turabian Style

Sharma, Sunil Kumar, Waseem A. Khan, and Cheon Seoung Ryoo. 2020. "A Parametric Kind of Fubini Polynomials of a Complex Variable" Mathematics 8, no. 4: 643. https://doi.org/10.3390/math8040643

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