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International Journal of Mathematics and Mathematical Sciences Volume 2012, Article ID 689797,10pages

doi:10.1155/2012/689797

Research Article

Arithmetic Identities Involving Bernoulli and

Euler Numbers

H.-M. Kim

1

and D. S. Kim

2

1Department of Mathematics, Kookmin University, Seoul 136-702, Republic of Korea

2Department of Mathematics, Sogang University, Seoul 121-742, Republic of Korea

Correspondence should be addressed to D. S. Kim,[email protected]

Received 12 June 2012; Accepted 23 October 2012

Academic Editor: A. Bayad

Copyrightq2012 H.-M. Kim and D. S. Kim. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

The purpose of this paper is to give some arithmatic identities for the Bernoulli and Euler numbers. These identities are derived from the severalp-adic integral equations onZp.

1. Introduction

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

ring ofp-adic rational integers, the field ofp-adic rational numbers, and the completion of algebraic closure ofQp, respectively. Thep-adic norm is normalized so that|p|p1/p. LetN

be the set of natural numbers andZ N∪ {0}.

Let UDZpbe the space of uniformly differentiable functions onZp. Forf ∈UDZp,

the bosonicp-adic integral onZpis defined by

If

Zpfxdμx Nlim→ ∞

pN−1

x0

fxμxpNZp

lim

N→ ∞

1

pN

pN−1

x0

fx, 1.1

and the fermionicp-adic integral onZpis defined by Kim as followssee1–8:

I−1f

Zpfxdμ−1x Nlim→ ∞

pN−1

x0

(2)

The Euler polynomials,Enx, are defined by the generating function as followssee

1–16:

FEt, x 2

et1e

xt

n0

Enxtn

n!. 1.3

In the special case,x0,En0 Enis called thenth Euler number. By1.3and the definition of Euler numbers, we easily see that

Enx n

l0

n

l Elxn−l Ex

n

, 1.4

with the usual convention about replacingEl byEl see10. Thus, by1.3and1.4, we

have

E0 1, E1nEn2δ0,n, 1.5

whereδk,nis the Kronecker symbolsee9,10,17–19.

From1.2, we can also derive the following integral equation for the fermionicp-adic integral onZpas follows:

I−1f1−I−1f2f0, 1.6

see1,2. By1.3and1.6, we get

Zpe

xytdμ−1y 2

et1e

xt

n0

Enxtn

n!. 1.7

Thus, by1.7, we have

Zp

xyndμ−1yEnx, 1.8

see1–8,13–16.

The Bernoulli polynomials,Bnx, are defined by the generating function as follows:

FBt, x t

et1e

xt

n0

Bnxtn

n!, 1.9

see18. In the special case,x0,Bn0 Bnis called thenth Bernoulli number. From1.9 and the definition of Bernoulli numbers, we note that

Bnx n

l0

n

l x

n−lBl Bxn,

(3)

see1–19, with the usual convention about replacingBlbyBl. By1.9and1.10, we easily

see that

B01, B1nBnδ1,n, 1.11

see13.

From1.1, we can derive the following integral equation onZp:

If1Iff0, 1.12

wheref1x fx1andf0 dfx/dx|x0. By1.12, we have

Zpe

xyty t

et1e

xt

n0

Bnxtn

n!. 1.13

Thus, by1.13, we can derive the following Witt’s formula for the Bernoulli polynomials:

Zp

xyndμyBnx, forn∈Z. 1.14

In19, it is known that fork, m∈Z,

max{k,m}

j1

k

j −1

j1m

j

Bkm1−jx

km1−j x

kx1m −1m1

km1kmk , 1.15

wherekj0 ifj <0 orj > k.

The purpose of this paper is to give some arithmetic identities involving Bernoulli and Euler numbers. To derive our identities, we use the properties ofp-adic integral equations on Zp.

2. Arithmetic Identities for Bernoulli and Euler Numbers

Let us take the bosonicp-adic integral onZpin1.15as follows:

I1

Zpx

kx1mdμx −1m1

km1kmk

m

l0

m

l −1

l

Zpx

km−ldμx −1m1

km1kmk

m

l0

m

l −1

lBkm−l −1m1

km1kmk .

(4)

On the other hand, we get

I1

max{k,m}

j1

k

j −1

j1m

j

1

km1−j

ZpBkm1−jxdμx

max{k,m}

j1

k

j −1

j1m

j

1

km1−j

×km1−j

l0

km1−j

l Bkm1−j−lBl.

2.2

By2.1and2.2, we get

max{k,m}

j1

km1−j

l0

1

km1−j

k

j −1

j1m

j

×

km1−j

l Bkm1−j−lBl

m

l0

−1l

m

l Bkm−l

−1m1

km1kmk .

2.3

Therefore, by2.3, we obtain the following theorem.

Theorem 2.1. Fork, m∈Z, one has

max{k,m}

j1

km1−j

l0

1

km1−j

k

j −1

j1m

j

×

km1−j

l Bkm1−j−lBl

−1m1

km1kmk

m

l0

−1l

m

l Bkm−l.

2.4

Now we consider the fermionicp-adic integral onZpin1.15as follows:

I2

max{k,m}

j1

k

j −1

j1m

j

1

km1−j

km1−j

l0

km1−j

l

×Bkm1−j−l

Zpx

(5)

max{k,m} j1

k

j −1

j1m

j

1

km1−j

km1−j

l0

km1−j

l

×Bkm1−j−lEl.

2.5

On the other hand, we get

I2

m

l0

−1l

m

l

Zpx

m−lkdμ−1x −1m1

km1kmk

m

l0

−1l

m

l Ekm−l

−1m1

km1kmk .

2.6

By2.5and2.6, we get

max{k,m}

j1

km1−j

l0

1

km1−j

k

j −1

j1m

j

km1−j

l

×Bkm1−j−lEl

m

l0

−1l

m

l Ekm−l

−1m1

km1kmk .

2.7

Therefore, by2.7, we obtain the following theorem.

Theorem 2.2. Fork, m∈Z, one has

max{k,m}

j1

km1−j

l0

1

km1−j

k

j −1

j1m

j

km1−j

l

×Bkm1−j−lEl− −1

m1

km1kmk

m

l0

−1l

m

l Ekm−l.

2.8

Replacingxby1−xin1.15, we have the identity:

max{k,m}

j1

k

j −1

j1m

j

Bkm1−j1−x

km1−j

−1kmxm1xk −1m1

km1kmk .

(6)

Let us take the bosonicp-adic integral onZpin2.9as follows:

I3

max{k,m}

j1

k

j −1

j1m

j

1

km1−j

×km1−j

l0

km1−j

l Bkm1−j−l

Zp1−x

ldμx

max{k,m}

j1

k

j −1

j1m

j

1

km1−j

×

km1−j

l0

km1−j

l Bkm1−j−lBl

max{k,m}

j1

k

j −1

j1m

j

1

km1−j

×km1−j

l0

km1−j

l Bkm1−j−ll

max{k,m}

j1

k

j −1

j1m

j

1

km1−j

×km1−j

l0

km1−j

l Bkm1−j−lδ1,l

max{k,m}

j1

km1−j

l0

1

km1−j

k

j −1

j1m

j

×

km1−j

l Bkm1−j−lBl

max{k,m}

j1

k

j −1

j1m

j 2Bkm−jδ1,km−j

max{k,m}

j1

km1−j

l0

1

km1−j

k

j −1

j1m

j

×

km1−j

l Bkm1−j−lBl2

maxk,m

j1

k

j −1

j1m

j

×Bkm−j

k

km−1 −1

km m

km−1 .

(7)

On the other hand, we see that

I3 −1km

k

l0

−1l

k

l Bkm−l

−1m1

km1kmk . 2.11

By2.10and2.11, we get

max{k,m}

j1

km1−j

l0

1

km1−j

k

j −1

j1m

j

×

km1−j

l Bkm1−j−lBl2

max{k,m}

j1

k

j −1

j1m

j

×Bkm−j

k

km−1 −1

km m

km−1

−1km

k

l0

−1l

k

l Bkm−l

−1m1

km1kmk .

2.12

Therefore, by2.12, we obtain the following theorem.

Theorem 2.3. Fork, m∈Z, one has

max{k,m}

j1

km1−j

l0

1

km1−j

k

j −1

j1m

j

×

km1−j

l Bkm1−j−lBl2

max{k,m}

j1

k

j −1

j1m

j

×Bkm−j

k

km−1 −1

km m

km−1 −

−1m1

km1kmk

−1km

k

l0

−1l

k

l Bkm−l.

2.13

We consider the fermionicp-adic integral onZpin2.9as follows:

I4

max{k,m}

j1

k

j −1

j1m

j

1

km1−j

×km1−j

l0

km1−j

l Bkm1−j−l

Zp1−x

(8)

max{k,m} j1

k

j −1

j1m

j

1

km1−j

×km1−j

l0

km1−j

l Bkm1−j−lEl

2

max{k,m}

j1

k

j −1

j1m

j

1

km1−j

×km1−j

l0

km1−j

l Bkm1−j−l

−2

max{k,m}

j1

k

j −1

j1m

j

1

km1−j

×km1−j

l0

km1−j

l Bkm1−j−lδ0,l

max{k,m}

j1

km1−j

l0

1

km1−j

k

j −1

j1m

j

×km1−j

l Bkm1−j−lEl

2

max{k,m}

j1

1

km1−j

k

j −1

j1m

j δ1,km1−j

max{k,m}

j1

km1−j

l0

1

km1−j

k

j −1

j1m

j

×

km1−j

l Bkm1−j−lEl2

k

km −1

km1 m

km .

2.14

On the other hand, we get

I4 −1km

k

l0

−1l

k

l Ekm−l

−1m1

km1kmk . 2.15

(9)

Theorem 2.4. Fork, m∈Z, one has

max{k,m}

j1

km1−j

l0

1

km1−j

k

j −1

j1m

j

km1−j

l

×Bkm1−j−lEl2

k

km −1

km1 m

km

− −1m1

km1kmk −1

kmk

l0

−1l

k

l Ekm−l.

2.16

Acknowledgment

This Research was supported by Basic Science Research Program through the National Research Foundation of Korea NRF funded by the Ministry of Education, Science, and Technology2012R1A1A2003786.

References

1 T. Kim, “Some identities on the q-Euler polynomials of higher order and q-Stirling numbers by the fermionic p-adic integral onZp,” Russian Journal of Mathematical Physics, vol. 16, no. 4, pp. 484–491, 2009.

2 T. Kim, “Symmetry of power sum polynomials and multivariate fermionic p-adic invariant integral onZp,” Russian Journal of Mathematical Physics, vol. 16, no. 1, pp. 93–96, 2009.

3 T. Kim, “q-Bernoulli numbers and polynomials associated with Gaussian binomial coefficients,”

Russian Journal of Mathematical Physics, vol. 15, no. 1, pp. 51–57, 2008.

4 T. Kim, “q-Volkenborn integration,” Russian Journal of Mathematical Physics, vol. 9, no. 3, pp. 288–299, 2002.

5 T. Kim, B. Lee, S. H. Lee, and S.-H. Rim, “Identities for the Bernoulli and Euler numbers and polynomials,” Ars Combinatoria. In press.

6 S.-H. Rim and J. Jeong, “On the modified q-Euler numbers of higher order with weight,” Advanced

Studies in Contemporary Mathematics, vol. 22, no. 1, pp. 93–98, 2012.

7 S.-H. Rim and T. Kim, “Explicit p-adic expansion for alternating sums of powers,” Advanced Studies in

Contemporary Mathematics, vol. 14, no. 2, pp. 241–250, 2007.

8 C. S. Ryoo, “Some relations between twisted q-Euler numbers and Bernstein polynomials,” Advanced

Studies in Contemporary Mathematics, vol. 21, no. 2, pp. 217–223, 2011.

9 L. Carlitz, “Some arithmetic properties of generalized Bernoulli numbers,” Bulletin of the American

Mathematical Society, vol. 65, pp. 68–69, 1959.

10 L. Carlitz, “Note on the integral of the product of several Bernoulli polynomials,” Journal of the London

Mathematical Society Second Series, vol. 34, pp. 361–363, 1959.

11 J. Choi, D. S. Kim, T. Kim, and Y. H. Kim, “Some arithmetic identities on Bernoulli and Euler numbers arising from the p-adic integrals onZp,” Advanced Studies in Contemporary Mathematics, vol. 22, no. 2, pp. 239–247, 2012.

12 D. V. Dolgy, T. Kim, B. Lee, and C. S. Ryoo, “On the q-analogue of Euler measure with weightα,”

Advanced Studies in Contemporary Mathematics, vol. 21, no. 4, pp. 429–435, 2011.

13 D. S. Kim, T. Kim, D. V. Dolgy, S. H. Lee, and S.-H. Rim, “Some properties and identities of Bernoulli and Euler polynomials associated with p-adic integral onZp,” Abstract and Applied Analysis, vol. 2012, Article ID 847901, 12 pages, 2012.

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15 H.-M. Kim, D. S. Kim, T. Kim, S. H. Lee, D. V. Dolgy, and B. Lee, “Identities for the Bernoulli and Euler numbers arising from the p-adic integral onZp,” Proceedings of the Jangjeon Mathematical Society, vol. 15, no. 2, pp. 155–161, 2012.

16 Y. Simsek, “Generating functions of the twisted Bernoulli numbers and polynomials associated with their interpolation functions,” Advanced Studies in Contemporary Mathematics, vol. 16, no. 2, pp. 251– 278, 2008.

17 S. Araci, D. Erdal, and J. J. Seo, “A study on the fermionic p-adic q-integral onZpassociated with weighted q-Bernstein and q-Genocchi polynomials,,” Abstract and Applied Analysis, vol. 2011, Article ID 649248, 10 pages, 2011.

18 A. Bayad and T. Kim, “Identities involving values of Bernstein, q-Bernoulli, and q-Euler polynomials,”

Russian Journal of Mathematical Physics, vol. 18, no. 2, pp. 133–143, 2011.

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