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R E S E A R C H

Open Access

A note on type 2

q

-Bernoulli and type 2

q

-Euler polynomials

Dae San Kim

1

, Taekyun Kim

2

, Han Young Kim

2

and Jongkyum Kwon

3*

*Correspondence:

[email protected] 3Department of Mathematics Education and ERI, Gyeongsang National University, Jinju, Republic of Korea

Full list of author information is available at the end of the article

Abstract

As is well known, power sums of consecutive nonnegative integers can be expressed in terms of Bernoulli polynomials. Also, it is well known that alternating power sums of consecutive nonnegative integers can be represented by Euler polynomials. In this paper, we show that power sums of consecutive positive oddq-integers can be expressed by means of type 2q-Bernoulli polynomials. Also, we show that alternating power sums of consecutive positive oddq-integers can be represented by virtue of type 2q-Euler polynomials. The type 2q-Bernoulli polynomials and type 2q-Euler polynomials are introduced respectively as the bosonicp-adicq-integrals onZpand

the fermionicp-adicq-integrals onZp. Along the way, we will obtain Witt type

formulas and explicit expressions for those two newly introduced polynomials.

MSC: 11B83; 11S80; 05A30; 11B65

Keywords: Type 2q-Bernoulli polynomials; Type 2q-Euler polynomials;p-adic

q-integral; Power sums of consecutive positive oddq-integers

1 Introduction

Letpbe a fixed odd prime number. Throughout this paper,Zp,Qp, andCp will denote

the ring ofp-adic integers, the field ofp-adic rational numbers, and the completion of the algebraic closure ofQp, respectively. Let| · |pbe thep-adic norm which is normalized as

|p|p=1p. Letqbe an indeterminate such thatq∈Cpwith|1 –q|p<p– 1

p–1, and [x] q=1–q

x

1–q.

Note that [x]–q=1–(–q)

x

1+q .

The bosonicp-adicq-integrals onZpare defined by Kim as

Zp

f(x)dμq(x) = lim N→∞

1 [pN]

q pN–1

x=0

f(x)qx (see [7]), (1.1)

wheref is a uniformly differentiable function onZp.

In [1,2], Carlitz considered theq-Bernoulli numbers which are given by the recurrence relation:

β0,q= 1, q(qβq+ 1)nβn,q=

⎧ ⎨ ⎩

1, ifn= 1,

0, ifn> 1, (1.2)

with the usual convention about replacingβn q byβn,q.

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In [6,7], Kim gave the following Witt type formula:

Zp

[x]nqdμq(x) =βn,q (n≥0). (1.3)

Carlitz also defined theq-Bernoulli polynomials by

βn,q(x) =

qxβq+ [x]q

n

=

n

l=0

n l

[x]nqlqlxβl,q (see [1,2]), (1.4)

wherenis a nonnegative integer.

An integral representation forβn,q(x), (n≥0) was given by Kim as follows:

Zp

[x+y]nqdμq(y) =βn,q(x), (n≥0), (see [5,7]). (1.5)

In [6,8, 10], Kim introduced the modified q-Bernoulli polynomials as the p-adic q-integral onZpgiven by

Bn,q(x) =

Zp

qy[x+y]nqdμq(y) (n≥0). (1.6)

Forx= 0,Bn,q=Bn,q(0) are called the modifiedq-Bernoulli numbers.

From (1.1), we note that

B0,q=

q– 1

logq, (qBq+ 1)

nB n,q=

⎧ ⎨ ⎩

1, ifn= 1,

0, ifn> 1, (1.7)

with the usual convention about replacingBnqbyBn,q.

By (1.6), we easily get

Bn,q(x) = n

l=0

n l

[x]nqlqlxBl,q (n≥0),

= 1

(1 –q)n n

l=0

n l

(–1)lqlx l [l]q

(n≥0) (see [6,8,10]).

It is well known that

0k+ 1k+ 2k+· · ·+ (n– 1)k= 1 k+ 1

Bk+1(n) –Bk+1

(n≥1,k≥0). (1.8)

HereBk(x) are the Bernoulli polynomials given by

t et– 1e

xt=

n=0

Bn(x)

tn

n! (see [1–17]), (1.9)

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In [8], Kim proved that the power sums of consecutive nonnegativeq-integers are given by

[0]kq+q[1]kq+q2[2]qk+· · ·+qn–1[n– 1]kq= 1 k+ 1

Bk+1,q(n) –Bk+1,q

(n≥1,k≥0).

Now, we consider the power sums of consecutive odd positiveq-integers and ask the following question:

q[1]kq+q3[3]kq+q5[5]qk+· · ·+q2n–1[2n– 1]kq=? (1.10)

In addition, we ask the following question:

[1]kqq[3]kq+q2[5]kq–· · ·+ (–1)n–1qn–1[2n– 1]kq=? (1.11)

We will see that (1.10) can be expressed in terms of type 2q-Bernoulli polynomials and (1.11) by virtue of type 2q-Euler polynomials. Here we note that the type 2q-Bernoulli polynomials are represented by bosonicp-adicq-integrals onZpand the type 2q-Euler

polynomials by fermionicp-adicq-integrals onZp.

2 Type 2q-Bernoulli polynomials and numbers

From (1.1), we have

Zp

qxf(x+ 1)dμq(x) =

Zp

qxf(x)dμq(x) +

q– 1 logqf

(0). (2.1)

By using (2.1) and induction, we get

Zp

qxf(x+n)dμq(x) =

Zp

qxf(x)dμq(x) +

q– 1 logq

n–1

l=0

f(l), (2.2)

wherenis a positive integer.

In view of (1.6), we consider the generating function of the type 2q-Bernoulli polyno-mials given by the followingp-adicq-integral onZp:

Zp

qye[2y+x+1]qtdμ

q(y) =

n=0

bn,q(x)

tn

n!. (2.3)

From (2.3), we have

Zp

qy[2y+x+ 1]nqdμq(y) =bn,q(x) (n≥0). (2.4)

Forx= 0,bn,q=bn,q(0) are called the type 2q-Bernoulli numbers.

By (2.4), we get

bn,q=

Zp

qy[2y+ 1]nqdμq(y) =

2 (1 –q)n

n

l=0

n l

(–1)lql l [2l]q

(4)

By (2.5), we easily get

bn,q=

2 (1 –q)n

n

l=0

n l

(–1)lql l [2l]q

= 2n (1 –q)n

n

l=1

n– 1 l– 1

(–1)lql(1 –q)

m=0

q2lm

= –2n

(1 –q)n–1

m=0

q2m+1

n–1

l=0

n– 1 l

(–1)lq(2m+1)l

= –2n ∞

m=0

q2m+1[2m+ 1]nq–1. (2.6)

Theorem 2.1 For n≥0,we have

bn,q=

2 (1 –q)n

n

l=0

n l

(–1)lql l [2l]q

= –2n ∞

m=0

q2m+1[2m+ 1]n–1

q . (2.7)

By (2.7), we can derive the generating function for the type 2q-Bernoulli numbers as follows:

n=0

bn,q

tn

n! = –2t ∞

m=0

q2m+1e[2m+1]qt. (2.8)

From (2.4), we note that

bn,q(x) = n

l=0

n l

qlxbl,q[x]nql, (2.9)

and that

q2bq+ 1 +q

n

bn,q= 2nq (n≥0). (2.10)

From (2.4), we easily get

bn,q(x) =

2 (1 –q)n

n

l=0

n l

(–1)lq(x+1)l l [2l]q

= –2n ∞

m=0

(5)

From (2.2), we note that

bm,q(2n) –bm,q=

Zp

qx[2x+ 1 + 2n]mq dμq(x) –

Zp

qx[2x+ 1]mq dμq(x)

= 2m

n–1

l=0

q2l+1[2l+ 1]mq–1. (2.12)

Therefore, by (2.12), we obtain the following theorem.

Theorem 2.2 For m≥0and n∈N,we have

1 m+ 1

bm+1,q(2n) –bm+1,q

= 2

n–1

l=0

q2l+1[2l+ 1]mq. (2.13)

From (2.13), we note that

n–1

l=0

q2l+1[2l+ 1]mq = 1 2m+ 2

m+1

l=0

m+ 1 l

q2nlbl,q[2n]qm+1–lbm+1,q

= 1

2m+ 2 m

l=0

m+ 1 l

q2nlbl,q[2n]mq+1–l

+ (q– 1)2n(m+ 1)qbm+1,q

. (2.14)

By (2.14), we get the following corollary.

Corollary 2.3 For n∈Nand m≥0,we have

n–1

l=0

q2l+1[2l+ 1]mq = 1 2m+ 2

m

l=0

m+ 1 l

q2nl[2n]mq+1–lbl,q

+(q– 1)[2n(m+ 1)]qbm+1,q

2m+ 2 . (2.15)

Example Here we check formula (2.15) form= 1. First, we observe that

[2n+ 1]2q– 1 =

n–1

l=0

[2l+ 3]2q– [2l+ 1]2q

=

n–1

l=0

[2l+ 1]q+q2l+1[2]q– [2l+ 1]q

×[2l+ 1]q+q2l+1[2]q+ [2l+ 1]q

= 2[2]q n–1

l=0

q2l+1[2l+ 1]q+

[2]2

qq2[4n]q

[4]q

(6)

By (2.16), we get

n–1

l=0

q2l+1[2l+ 1]q=

1 2[2]q

[2n+ 1]2q– 1 – [2]2qq2[4n]q [4]q

= 1

2(q+ 1)

1 –q2n+1

1 –q 2

– 1 –q2(q+ 1)21 –q

4n

1 –q4

= q(1 –q

2n)

(1 –q)(1 –q2)

q2(1 –q4n)

(1 –q)(1 –q4). (2.17)

We now show that (2.17) agrees with the result in (2.15). For this, we first note the fol-lowing from (2.7):

b0,q=

q– 1

logq, b1,q= – 1 logq

2q 1 –q2,

b2,q=

2 1 –q

1 2logq

2q 1 –q2+

2q2

1 –q4

.

Then, from (2.15), we have

n–1

l=0

q2l+1[2l+ 1]q=

1 4

[2n]2qb0,q+ 2q2n[2n]qb1,q+ (q– 1)[4n]qb2,q

=1 4

1 –q2n 1 –q

2

q– 1 logq+ 2q

2n1 –q2n

1 –q – 1 logq

2q 1 –q2

+ (q– 1)1 –q

4n

1 –q 2 1 –q

1 2logq

2q 1 –q2+

2q2

1 –q4

= q(1 –q

2n)

(1 –q)(1 –q2)

q2(1 –q4n) (1 –q)(1 –q4).

3 Type 2q-Euler polynomials and numbers

It is known that the fermionicp-adicq-integrals onZpare defined by Kim as

Iq(f) =

Zp

f(x)dμq(x) = lim N→∞

1 [pN]

q pN–1

x=0

f(x)(–q)x (see [11,14,17]), (3.1)

where [x]–q=1–(–q)

x

1+q .

From (3.1), we note that

qIq(f1) =q

Zp

f(x+ 1)q(x) = lim N→∞

q [pN]

q pN–1

x=0

f(x+ 1)(–q)x

= – lim

N→∞ 1 [pN]

q pN

x=1

f(x)(–q)x= –I–q(f) + [2]qf(0). (3.2)

By (3.2), we get

(7)

and

qnIq(fn) = (–1)nIq(f) + [2]q n–1

l=0

(–1)n–1–lqlf(l), (3.4)

wherefn(x) =f(x+n), withn∈N.

As is known, Carlitz consideredq-Euler numbers given by the recurrence relation

E0,q= 1, q(qEq+ 1)n+En,q=

⎧ ⎨ ⎩

[2]q, ifn= 0,

0, ifn> 0,

(3.5)

with the usual convention about replacingEl

qbyEl,q(see [1,2]).

In [11], Kim obtained the Witt type formula for Carlitz’sq-Euler numbers which is rep-resented by the fermionicp-adicq-integrals onZp

Zp

[x]nqq(x) =En,q (n≥0). (3.6)

From (3.6), we note that

En,q=

[2]q

(1 –q)n n

l=0

n l

(–1)l 1

1 +ql+1 = [2]q

m=0

(–1)mqm[m]nq. (3.7)

By (3.7), we readily see that the generating function for Carlitz’sq-Euler numbers is given by

Fq(t) =

n=0

En,q

tn

n!= [2]q

m=0

(–1)mqme[m]qt. (3.8)

It is known that

qnEm,q(n) +Em,q= [2]q n–1

l=0

(–1)lql[l]mq (see [1,2]), (3.9)

wheren∈Nwithn≡1(mod 2). Note that equation (3.9) is an alternating sum of powers of consecutive positiveq-integers.

Now, we consider an alternating sum of powers of consecutive positive oddq-integers which are given by

n–1

l=0

(–1)lql[2l+ 1]mq = [1]mqq[3]mq +q2[5]mq –· · ·+ (–1)n–1qn–1[2n– 1]mq. (3.10)

Let us define the type 2q-Euler polynomials which are given by

Zp

[2y+x+ 1]mq q(y) =Em,q(x) (m≥0). (3.11)

(8)

From (3.11), we note that

Em,q(x) =

[2]q

(1 –q)m m

l=0

m l

(–1)lql(1+x) 1 1 +q2l+1

= [2]q

k=0

(–1)kqk[2k+ 1 +x]mq (m≥0). (3.12)

By (3.12), we get the following generating function for theq-Euler polynomials:

m=0

Em,q(x)

tm m!= [2]q

k=0

(–1)kqke[2k+1+x]qt. (3.13)

Theorem 3.1 For m≥0,we have

Em,q(x) =

[2]q

(1 –q)m m

l=0

m l

(–1)lql(1+x) 1 1 +q2l+1

= [2]q

k=0

(–1)kqk[2k+ 1 +x]mq. (3.14)

From (3.11), we have

En,q(x) =

Zp

[2y+ 1 +x]nqq(y)

=

n

l=0

n l

[x]nqlqlx

Zp

[2y+ 1]lqq(y)

=

n

l=0

n l

[x]nqlqlxEl,q (n≥0). (3.15)

Also, by (3.3), we get

qEm,q(2) +Em,q= [2]q (n≥0). (3.16)

Therefore, by (3.15) and (3.16), we obtain the following theorem.

Theorem 3.2 For m≥0,we have

Em,q(x) = m

l=0

m l

[x]mqlqlxEl,q. (3.17)

In particular,

(9)

Letnbe a positive integer withn≡1(mod 2). From (3.4), we have

qn

Zp

[2y+ 2n+ 1]mq q(y) +

Zp

[2y+ 1]mq q(y)

= [2]q n–1

l=0

(–1)lql[2l+ 1]mq. (3.19)

By (3.11) and (3.19), we get

qnEm,q(2n) +Em,q= [2]q n–1

l=0

(–1)lql[2l+ 1]mq. (3.20)

Therefore, by (3.20), we obtain the following theorem.

Theorem 3.3 For n∈Nwith n≡1(mod 2)and m≥0,we have

qnEm,q(2n) +Em,q= [2]q n–1

l=0

(–1)lql[2l+ 1]mq. (3.21)

4 Conclusions

In an introductory calculus class, the following formulas are proved by mathematical in-duction and used in Riemann sum evaluations of some definite integrals:

n

k=0

k= 1 + 2 +· · ·+n=n(n+ 1)

2 =

n+ 1 2

,

n

k=0

k2= 12+ 22+· · ·+n2=n(n+ 1)(2n+ 1)

6 ,

n

k=0

k3= 13+ 23+· · ·+n3= n+ 1 2

2

= n(n+ 1) 2

2

.

The problem of finding formulas for power sums of consecutive nonnegative integers has captivated mathematicians for many centuries. Even since generalized formulas for the power sums,Sk(n) =

n

l=0lk, were established, the various representations and

number-theoretic properties have been studied by Faulhaber. In this paper, we studied the q-analogues of Faulhaber’s well-known formula expressing the power sums in terms of Bernoulli polynomials. Indeed, we showed that power sums of consecutive positive odd q-integers can be expressed by means of type 2q-Bernoulli polynomials. Also, we showed that alternating power sums of consecutive positive oddq-integers can be represented by virtue of type 2q-Euler polynomials. The type 2q-Bernoulli polynomials and type 2 q-Euler polynomials were introduced respectively as the bosonicp-adicq-integrals onZp

and the fermionicp-adicq-integrals onZp. Along the way, we also obtained Witt type

formulas and explicit expressions for those two newly introduced polynomials.

Funding

(10)

Competing interests

The authors declare that they have no competing interests.

Authors’ contributions

All authors contributed equally to the manuscript and typed, read, and approved the final manuscript.

Author details

1Department of Mathematics, Sogang University, Seoul, Republic of Korea.2Department of Mathematics, Kwangwoon

University, Seoul, Republic of Korea.3Department of Mathematics Education and ERI, Gyeongsang National University,

Jinju, Republic of Korea.

Publisher’s Note

Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Received: 22 April 2019 Accepted: 10 June 2019

References

1. Carlitz, L.:q-Bernoulli numbers and polynomials. Duke Math. J.15, 987–1000 (1948) 2. Carlitz, L.:q-Bernoulli and Eulerian numbers. Transl. Am. Math. Soc.76, 332–350 (1954)

3. Jang, G.-W., Kim, T.: A note on type 2 degenerate Euler and Bernoulli polynomials. Adv. Stud. Contemp. Math. (Kyungshang)29(1), 147–159 (2019)

4. Jeong, J.-H., Jin, J.-H., Park, J.-W., Rim, S.-H.: On the twisted weakq-Euler numbers and polynomials with weight 0. Proc. Jangjeon Math. Soc.16(2), 157–163 (2013)

5. Kim, D.S., Kim, T.: A note on type 2 Changhee and Daehee polynomials. Rev. de la Real Acad. De Cien. Exac. Fis. Nat. Series A. Mate., 1–9 (2019).https://doi.org/10.1007/s13398-019-00656-x

6. Kim, T.: On explicit formulas ofp-adicq-integral L-functions. Kyushu J. Math.48(1), 73–86 (1994) 7. Kim, T.:q-Volkenborn integration. Russ. J. Math. Phys.9(3), 288–299 (2002)

8. Kim, T.: Sums of powers of consecutiveq-integers. Adv. Stud. Contemp. Math. (Kyungshang)9(1), 15–18 (2004) 9. Kim, T.: Analytic continuation of multipleq-zeta functions and their values at negative integers. Russ. J. Math. Phys.

11(1), 71–76 (2004)

10. Kim, T.: A note on exploring the sums of powers of consecutiveq-integers. Adv. Stud. Contemp. Math. (Kyungshang) 11(1), 137–140 (2005)

11. Kim, T.:q-Euler numbers and polynomials associated withp-adicq-integrals. J. Nonlinear Math. Phys.14(1), 15–27 (2007)

12. Kim, T., Rim, S.-H., Simsek, Y.: A note on the alternating sums of powers of consecutiveq-integers. Adv. Stud. Contemp. Math. (Kyungshang)13(2), 159–164 (2006)

13. Ozden, H., Cangul, I.N., Simsek, Y.: Multivariate interpolation functions of higher-orderq-Euler numbers and their applications. Abstr. Appl. Anal.2008, Article ID 390857 (2008)

14. Rim, S.-H., Kim, T., Ryoo, C.S.: On the alternating sums of powers of consecutiveq-integers. Bull. Korean Math. Soc. 43(3), 611–617 (2006)

15. Rim, S.-H., Park, J.-W., Kwon, J., Pyo, S.-S.: On the modifiedq-Euler polynomials with weight. Adv. Differ. Equ.2013, 356 (2013)

16. Ryoo, C.S., Kim, T.: Exploring theq-analogues of the sums of powers of consecutive integers with mathematica. Adv. Stud. Contemp. Math. (Kyungshang)18(1), 69–77 (2009)

References

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