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Volume 2009, Article ID 357349,5pages doi:10.1155/2009/357349

Research Article

A Note on H ¨older Type Inequality for the Fermionic

p

-Adic Invariant

q

-Integral

Lee-Chae Jang

Department of Mathematics and Computer Science, KonKuk University, Chungju 380-701, South Korea

Correspondence should be addressed to Lee-Chae Jang,[email protected]

Received 11 February 2009; Accepted 22 April 2009

Recommended by Kunquan Lan

The purpose of this paper is to find H ¨older type inequality for the fermionicp-adic invariantq -integral which was defined by Kim2008.

Copyrightq2009 Lee-Chae Jang. 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.

1. Introduction

Letpbe a fixed odd prime. Throughout this paperZp, Qp,Q,C,and Cpwill, respectively, denote the ring ofp-adic rational integers, the field ofp-adic rational numbers, the rational number field, the complex number field, and the completion of algebraic closure ofQp. For a fixed positive integerdwithp, d 1, let

XXdlim N

Z/dpNZ, X1Zp,

X

0<a<dp

a,p1

adpZp,

adpNZpxX |xa moddpN,

1.1

wherea∈Zlies in 0≤a < dpNcf.124.

LetNbe the set of natural numbers. In this paper we assume thatq∈Cp,with|1−q|p< p−1/p−1, which implies thatqxexpxlogqfor|p|

p≤1. We also use the notations

xq 1−q

x

1−q, xq

1−−qx

(2)

for allx∈Zp. For any positive integerN,the distribution is defined by

µq

adpNZp qa

dpN q

. 1.3

We say thatfis a uniformly differentiable function at a pointa∈Zpand denote this property byfUDZp, if the difference quotients Ffx, y fxfy/xyhave a limit

lfaasx, ya, a cf.1–24.

For fUDZp, the above distribution µq yields the bosonic p-adic invariant

q-integral as follows:

Iq

f

Zp

fxdµqx lim N→ ∞

1 pN

q pN1

x0

fxqx, 1.4

representing thep-adicq-analogue of the Riemann integral forf. In the sense of fermionic, let us define the fermionicp-adic invariantq-integral onZpas

Iq

f

Zp

fxdµqx lim N→ ∞

1 pN

q pN1

x0

fxqx, 1.5

forfUDZp see16. Now, we consider the fermionicp-adic invariantq-integral onZp as

I1

flim

q→1Iq

f

Zp

fxdµ1x. 1.6

From1.5we note that

I−1

fI−1

f2f0, 1.7

wheref1x fx1 see16.

We also introduce the classical H ¨older inequality for the Lebesgue integral in25.

Theorem 1.1. Letm, m∈Qwith1/m1/m1. IffLmandgLm, thenf·g L1and

fgdxfmgm 1.8

wherefLm|f|mdx <andgLm |g|mdx <andf m{

|f|mdx}1/m.

(3)

2. H ¨older Type Inequality for Fermionic

p

-Adic Invariant

q

-Integrals

In order to investigate the H ¨older type inequality forI1, we introduce the new concept of

the inequality as follows.

Definition 2.1. Forf, gUDZp, we define the inequality onUDZp resp.,Cpas follows. For f, gUDZp resp.,x, y ∈ Cp,fpgresp.,xp yif and only if |f|p ≤ |g|p resp.,

|x|p≤ |y|p.

Letm, m∈Qwith 1/m1/m1. By substitutingfx qxandgx extinto1.3, we obtain the following equation:

Zp

fxgxµ−1x

Zp

qetxdµ−1x 2

qet1, 2.1

Zp

fxmµ1x

Zp

qmx −1x

2

qm1, 2.2

Zp

gxmµ1x

Zp

emxtdµ1x

2

emt1. 2.3

From2.1,2.2, and2.3, we derive

Zpfxgxdµ−1x

Zpfx m

−1

1/m Zpgx

m −1

1/m

emt11/mqm11/m

qet1

n0

n

l0

⎛ ⎜ ⎝ 1 m

l ⎞ ⎟ ⎠elmt

⎛ ⎜ ⎝

1 m

nl ⎞ ⎟

⎠qnlm 1

qet1

n0

n

l0

⎛ ⎜ ⎝ 1 m

l ⎞ ⎟ ⎠

⎛ ⎜ ⎝

1 m

nl ⎞ ⎟

⎠qnlm elmt

qet1.

2.4

We remark that thenth Frobenius-Euler numbersHnqand thenth Frobenius-Euler

polynomialsHnq, xattached to algebraic numberq/1may be defined by the exponential

generating functionssee16:

1−q etq

n0

Hn

qt

n

n!, 2.5

1−q etqe

xt

n0

Hn

q, xt

n

(4)

Then, it is easy to see that

2qemlt

qex1

k0

Hn

q−1, mlt

k

k!. 2.7

From2.4and2.7, we have the following theorem.

Theorem 2.2. Letm, m∈Qwith1/m1/m1. If one takesfx qxandgx ext, then one

has

Zpfxgxdµ−1x

Zpfx m

−1

1/m Zpgx

m −1

1/m

1

2q

n0

n

l0

⎛ ⎜ ⎝ 1 m l ⎞ ⎟ ⎠ ⎛ ⎜ ⎝ 1 m

nl ⎞ ⎟

qnlmk0

Hk

q−1, mltk

k!.

2.8

We note that form, m, k, l∈Qwith 1/m1/m1,

max ⎧ ⎪ ⎪ ⎨ ⎪ ⎪ ⎩ 1

2q p , ⎛ ⎜ ⎝ 1 m l ⎞ ⎟ ⎠ p , ⎛ ⎜ ⎝ 1 m

nl ⎞ ⎟ ⎠ p

,qml−1

p, k!1 p ⎫ ⎪ ⎪ ⎬ ⎪ ⎪

⎭≤1, 2.9

ByTheorem 2.2and2.7and the definition ofp-adic norm, it is easy to see that

Zpfxgxdµ−1x

Zpfx m

−1

1/m Zpgx

m −1 1/m p

≤maxHkq−1, ml p

, 2.10

for allm, m, k, l ∈ Q with 1/m1/m 1. We note that M max{|Hkq−1, ml|p} lies

in0,∞. Thus byDefinition 2.1and2.10, we obtain the following H ¨older type inequality theorem for fermionicp-adic invariantq-integrals.

Theorem 2.3. Letm, m∈Qwith1/m1/m1andMmax{|Hkq−1, ml|p}. If one takes

fx qxandgx ext, then one has

Zp

fxgxdµ−1xpM

Zp

fxmdµ−1

1/m

Zp

gxmdµ−1 1/m

. 2.11

Acknowledgment

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