Abstract

We investigate some interesting properties of the 𝑞-Euler polynomials. The purpose of this paper is to give some relationships between Bernstein and 𝑞-Euler polynomials, which are derived by the 𝑝-adic integral representation of the Bernstein polynomials associated with 𝑞-Euler polynomials.

1. Introduction

Let 𝑝 be a fixed odd prime number. Throughout this paper 𝑝, 𝑝, and 𝑝 denote the ring of 𝑝-adic integers, the field of 𝑝-adic numbers, and the field of 𝑝-adic completion of the algebraic closure of 𝑝, respectively (see [115]). Let be the set of natural numbers and +={0}. The normalized 𝑝-adic absolute value is defined by |𝑝|𝑝=1/𝑝. As an indeterminate, we assume that 𝑞𝑝 with |1𝑞|𝑝<1. Let UD(𝑝) be the space of uniformly differentiable function on 𝑝. For 𝑓UD(𝑝), the 𝑝-adic invariant integral on 𝑝 is defined by 𝐼1(𝑓)=𝑝𝑓(𝑥)𝑑𝜇1(𝑥)=lim𝑝𝑁𝑁1𝑥=0𝑓(𝑥)𝜇1𝑥+𝑝𝑁𝑝=lim𝑝𝑁𝑁1𝑥=0𝑓(𝑥)(1)𝑥,(1.1) (see [710]). For 𝑛, we can derive the following integral equation from (1.1):𝐼1𝑓𝑛=(1)𝑛𝑝𝑓(𝑥)𝑑𝜇1(𝑥)+2𝑛1𝑙=0(1)𝑛1𝑙𝑓(𝑙),(1.2) where 𝑓𝑛(𝑥)=𝑓(𝑥+𝑛) (see [711]). As well-known definition, the Euler polynomials are given by the generating function as follows:2𝑒𝑡𝑒+1𝑥𝑡=𝑒𝐸(𝑥)𝑡=𝑛=0𝐸𝑛(𝑡𝑥),𝑛!(1.3) (see [3, 5, 715]), with usual convention about replacing 𝐸𝑛(𝑥) by 𝐸𝑛(𝑥). In the special case 𝑥=0, 𝐸𝑛(0)=𝐸𝑛 are called the 𝑛th Euler numbers. From (1.3), we can derive the following recurrence formula for Euler numbers: 𝐸0=1,(𝐸+1)𝑛+𝐸𝑛=2if0𝑛=0,if𝑛>0,(1.4) (see [12]), with usual convention about replacing 𝐸𝑛 by 𝐸𝑛. By the definitions of Euler numbers and polynomials, we get 𝐸𝑛(𝑥)=(𝐸+𝑥)𝑛=𝑛𝑙=0𝑛𝑙𝑥𝑛𝑙𝐸𝑙,(1.5) (see [3, 5, 715]). Let 𝐶[0,1] denote the set of continuous functions on [0,1]. For 𝑓𝐶[0,1], Bernstein introduced the following well-known linear positive operator in the field of real numbers : 𝔹𝑛(𝑓𝑥)=𝑛𝑘=0𝑓𝑘𝑛𝑛𝑘𝑥𝑘(1𝑥)𝑛𝑘=𝑛𝑘=0𝑓𝑘𝑛𝐵𝑘,𝑛(𝑥),(1.6) where (𝑛𝑘)=𝑛(𝑛1)(𝑛𝑘+1)/𝑘!=𝑛!/𝑘!(𝑛𝑘)! (see [1, 2, 7, 11, 12, 14]). Here, 𝔹𝑛(𝑓𝑥) is called the Bernstein operator of order 𝑛 for 𝑓. For 𝑘,𝑛+, the Bernstein polynomials of degree 𝑛 are defined by𝐵𝑘,𝑛𝑛𝑘𝑥(𝑥)=𝑘(1𝑥)𝑛𝑘,for[].𝑥0,1(1.7) In this paper, we study the properties of 𝑞-Euler numbers and polynomials. From these properties, we investigate some identities on the 𝑞-Euler numbers and polynomials. Finally, we give some relationships between Bernstein and 𝑞-Euler polynomials, which are derived by the 𝑝-adic integral representation of the Bernstein polynomials associated with 𝑞-Euler polynomials.

2. 𝑞-Euler Numbers and Polynomials

In this section, we assume that 𝑞𝑝 with |1𝑞|𝑝<1. Let 𝑓(𝑥)=𝑞𝑥𝑒𝑥𝑡. From (1.1) and (1.2), we have𝑝𝑓(𝑥)𝑑𝜇1(2𝑥)=𝑞𝑒𝑡.+1(2.1) Now, we define the 𝑞-Euler numbers as follows:2𝑞𝑒𝑡+1=𝑒𝐸𝑞𝑡=𝑛=0𝐸𝑛,𝑞𝑡𝑛,𝑛!(2.2) with the usual convention about replacing 𝐸𝑛𝑞 by 𝐸𝑛,𝑞.

By (2.2), we easily get𝐸0,𝑞=2𝐸𝑞+1,𝑞𝑞+1𝑛+𝐸𝑛,𝑞=2if0𝑛=0,if𝑛>0,(2.3) with usual convention about replacing 𝐸𝑛𝑞 by 𝐸𝑛,𝑞.

We note that2𝑞𝑒𝑡=2+1𝑒𝑡+𝑞12=21+𝑞1+𝑞𝑛=0𝐻𝑛𝑞1𝑡𝑛,𝑛!(2.4) where 𝐻𝑛(𝑞1) is the 𝑛th Frobenius-Euler numbers.

From (2.1), (2.2), and (2.4), we have𝑝𝑞𝑥𝑒𝑥𝑡𝑑𝜇1(𝑥)=𝐸𝑛,𝑞=2𝐻1+𝑞𝑛𝑞1,for𝑛+.(2.5) Now, we consider the 𝑞-Euler polynomials as follows:2𝑞𝑒𝑡𝑒+1𝑥𝑡=𝑒𝐸𝑞(𝑥)𝑡=𝑛=0𝐸𝑛,𝑞(𝑡𝑥)𝑛,𝑛!(2.6) with the usual convention 𝐸𝑛𝑞(𝑥) by 𝐸𝑛,𝑞(𝑥).

From (1.2), (2.1), and (2.6), we get𝑝𝑞𝑥𝑒(𝑥+𝑦)𝑡𝑑𝜇1(2𝑦)=𝑞𝑒𝑡𝑒+1𝑥𝑡=𝑛=0𝐸𝑛,𝑞(𝑡𝑥)𝑛.𝑛!(2.7) By comparing the coefficients on the both sides of (2.6) and (2.7), we get the following Witt's formula for the 𝑞-Euler polynomials as follows:𝑝𝑞𝑦(𝑥+𝑦)𝑛𝑑𝜇1(𝑦)=𝐸𝑛,𝑞(𝑥)=𝑛𝑙=0𝑛𝑙𝑥𝑛𝑙𝐸𝑙,𝑞.(2.8) From (2.6) and (2.8), we can derive the following equation:2𝑞𝑞𝑒𝑡𝑒+1(1𝑥)𝑡=21+𝑞1𝑒𝑡𝑒𝑥𝑡=𝑛=0𝐸𝑛,𝑞1(𝑥)(1)𝑛𝑡.𝑛!(2.9) By (2.6) and (2.9), we obtain the following reflection symmetric property for the 𝑞-Euler polynomials.

Theorem 2.1. For 𝑛+, one has (1)𝑛𝐸𝑛,𝑞1(𝑥)=𝑞𝐸𝑛,𝑞(1𝑥).(2.10)

From (2.5), (2.6), (2.7), and (2.8), we can derive the following equation: for 𝑛, 𝐸𝑛,𝑞𝐸(2)=𝑞+1+1𝑛=𝑛𝑙=0𝑛𝑙𝐸𝑙,𝑞(1)=𝐸0,𝑞+1𝑞𝑛𝑙=1𝑛𝑙𝑞𝐸𝑙,𝑞2(1)=11+𝑞𝑞𝑛𝑙=1𝑛𝑙𝐸𝑙,𝑞=2+21+𝑞1𝑞(1+𝑞)𝑞𝑛𝑙=0𝑛𝑙𝐸𝑙,𝑞=2𝑞1𝑞2𝑞𝐸𝑛,𝑞2(1)=𝑞+1𝑞2𝐸𝑛,𝑞,(2.11) by using recurrence formula (2.3). Therefore, we obtain the following theorem.

Theorem 2.2. For 𝑛, one has 𝑞𝐸𝑛,𝑞1(2)=2+𝑞𝐸𝑛,𝑞.(2.12)

By using (2.5) and (2.8), we get 𝑝𝑞𝑥(1𝑥)𝑛𝑑𝜇1(𝑥)=(1)𝑛𝑝𝑞𝑥(𝑥1)𝑛𝑑𝜇1(𝑥)=(1)𝑛𝐸𝑛,𝑞1(1)=𝑞𝑝(𝑥+2)𝑛𝑑𝜇1(2𝑥)=𝑞𝑞+1𝑞2𝐸𝑛,𝑞1=2+𝑞𝐸𝑛,𝑞1=2+𝑞𝑝𝑥𝑛𝑞𝑥𝑑𝜇1(𝑥),for𝑛>0.(2.13) Therefore, we obtain the following theorem.

Theorem 2.3. For 𝑛, one has 𝑝𝑞𝑥(1𝑥)𝑛𝑑𝜇1(1𝑥)=2+𝑞𝑝𝑥𝑛𝑞𝑥𝑑𝜇1(𝑥).(2.14)

By using Theorem 2.3, we will study for the 𝑝-adic integral representation on 𝑝 of the Bernstein polynomials associated with 𝑞-Euler polynomials in Section 3.

3. Bernstein Polynomials Associated with 𝑞-Euler Numbers and Polynomials

Now, we take the 𝑝-adic integral on 𝑝 for the Bernstein polynomials in (1.7) as follows:𝑝𝐵𝑘,𝑛(𝑥)𝑞𝑥𝑑𝜇1(𝑥)=𝑝𝑛𝑘𝑥𝑘(1𝑥)𝑛𝑘𝑞𝑥𝑑𝜇1=𝑛𝑘(𝑥)𝑛𝑘𝑗=0𝑗𝑛𝑘(1)𝑛𝑘𝑗𝑝𝑥𝑛𝑗𝑞𝑥𝑑𝜇1=𝑛𝑘(𝑥)𝑛𝑘𝑗=0𝑗𝑛𝑘(1)𝑛𝑘𝑗𝐸𝑛𝑗,𝑞=𝑛𝑘𝑛𝑘𝑗=0𝑗𝑛𝑘(1)𝑗𝐸𝑘+𝑗,𝑞,where𝑛,𝑘+.(3.1) By the definition of Bernstein polynomials, we see that𝐵𝑘,𝑛(𝑥)=𝐵𝑛𝑘,𝑛(1𝑥),where𝑛,𝑘+.(3.2) Let 𝑛,𝑘+ with 𝑛>𝑘. Then, by (3.2), we get 𝑝𝑞𝑥𝐵𝑘,𝑛(𝑥)𝑑𝜇1(𝑥)=𝑝𝑞𝑥𝐵𝑛𝑘,𝑛(1𝑥)𝑑𝜇1(=𝑛𝑥)𝑛𝑘𝑘𝑗=0𝑘𝑗(1)𝑘𝑗𝑝(1𝑥)𝑛𝑗𝑞𝑥𝑑𝜇1=𝑛𝑘(𝑥)𝑘𝑗=0𝑘𝑗(1)𝑘𝑗2+𝑞𝑝𝑥𝑛𝑗𝑞𝑥𝑑𝜇1=𝑛𝑘(𝑥)𝑘𝑗=0𝑘𝑗(1)𝑘𝑗2+𝑞𝐸𝑛𝑗,𝑞1=2+𝑞𝐸𝑛,𝑞1if𝑛𝑘𝑞𝑘=0,𝑘𝑗=0𝑘𝑗(1)𝑘𝑗𝐸𝑛𝑗,𝑞1if𝑘>0.(3.3) Thus, we obtain the following theorem.

Theorem 3.1. For 𝑛,𝑘+ with 𝑛>𝑘, one has 𝑝𝑞1𝑥𝐵𝑘,𝑛(𝑥)𝑑𝜇1(𝑥)=2𝑞+𝐸𝑛,𝑞if𝑛𝑘𝑘=0,𝑘𝑗=0𝑘𝑗(1)𝑘𝑗𝐸𝑛𝑗,𝑞if𝑘>0.(3.4)

By (3.1) and Theorem 3.1, we get the following corollary.

Corollary 3.2. For 𝑛,𝑘+ with 𝑛>𝑘, one has 𝑛𝑘𝑗=0𝑗(𝑛𝑘1)𝑗𝐸𝑘+𝑗,𝑞1=12+𝑞𝐸𝑛,𝑞if𝑘=0,𝑘𝑗=0𝑘𝑗(1)𝑘𝑗1𝑞𝐸𝑛𝑗,𝑞if𝑘>0.(3.5)

For 𝑚,𝑛,𝑘+ with 𝑚+𝑛>2𝑘. Then, we get 𝑝𝐵𝑘,𝑛(𝑥)𝐵𝑘,𝑚(𝑥)𝑞𝑥𝑑𝜇1(=𝑛𝑘𝑚𝑘𝑥)2𝑘𝑗=0𝑗2𝑘(1)𝑗+2𝑘𝑝𝑞𝑥(1𝑥)𝑛+𝑚𝑗𝑑𝜇1=𝑛𝑘𝑚𝑘(𝑥)2𝑘𝑗=0𝑗2𝑘(1)𝑗+2𝑘𝑞𝑝(𝑥+2)𝑛+𝑚𝑗𝑞𝑥𝑑𝜇1=𝑛𝑘𝑚𝑘(𝑥)2𝑘𝑗=0𝑗2𝑘(1)𝑗+2𝑘𝑞2𝑞+1𝑞2𝐸𝑛+𝑚𝑗,𝑞=12+𝑞𝐸𝑛+𝑚,𝑞if𝑛𝑘𝑚𝑘𝑘=0,2𝑘𝑗=0𝑗2𝑘(1)𝑗+2𝑘1𝑞𝐸𝑛+𝑚𝑗,𝑞if𝑘>0.(3.6) Therefore, we obtain the following theorem.

Theorem 3.3. For 𝑚,𝑛,𝑘+ with 𝑚+𝑛>2𝑘, one has 𝑝𝐵𝑘,𝑛(𝑥)𝐵𝑘,𝑚(𝑥)𝑞1𝑥𝑑𝜇1(𝑥)=2𝑞+𝐸𝑛+𝑚,𝑞if𝑛𝑘𝑚𝑘𝑘=0,2𝑘𝑗=0𝑗2𝑘(1)𝑗+2𝑘𝐸𝑛+𝑚𝑗,𝑞if𝑘>0.(3.7)

By using binomial theorem, for 𝑚,𝑛,𝑘+, we get𝑝𝐵𝑘,𝑛(𝑥)𝐵𝑘,𝑚(𝑥)𝑞1𝑥𝑑𝜇1(𝑥)(3.8)=𝑛𝑘𝑚𝑘𝑛+𝑚2𝑘𝑗=0𝑗𝑛+𝑚2𝑘(1)𝑗𝑝𝑥𝑗+2𝑘𝑞1𝑥𝑑𝜇1𝑛𝑘𝑚𝑘(𝑥)=𝑞𝑛+𝑚2𝑘𝑗=0𝑗𝑛+𝑚2𝑘(1)𝑗𝐸𝑗+2𝑘,𝑞1.(3.9) By comparing the coefficients on the both sides of (3.8) and Theorem 3.3, we obtain the following corollary.

Corollary 3.4. Let 𝑚,𝑛,𝑘+ with 𝑚+𝑛>2𝑘. Then, we get 𝑛+𝑚2𝑘𝑗=0𝑗𝑛+𝑚2𝑘(1)𝑗𝐸𝑗+2𝑘,𝑞1=12+𝑞𝐸𝑛+𝑚,𝑞if1𝑘=0,𝑞2𝑘𝑗=0𝑗2𝑘(1)𝑗+2𝑘𝐸𝑛+𝑚𝑗,𝑞if𝑘>0.(3.10)

For 𝑠, let 𝑛1,𝑛2,,𝑛𝑠, 𝑘+ with 𝑛1+𝑛2++𝑛𝑠>𝑠𝑘. By induction, we get 𝑝𝐵𝑘,𝑛1(𝑥)𝐵𝑘,𝑛𝑠(𝑥)𝑞𝑥𝑑𝜇1(=𝑥)𝑠𝑖=1𝑛𝑖𝑘𝑝𝑥𝑠𝑘(1𝑥)𝑛1++𝑛𝑠𝑠𝑘𝑞𝑥𝑑𝜇1=(𝑥)𝑠𝑖=1𝑛𝑖𝑘𝑠𝑘𝑗=0𝑗𝑠𝑘(1)𝑠𝑘+𝑗𝑝(1𝑥)𝑛1++𝑛𝑠𝑗𝑞𝑥𝑑𝜇1=(𝑥)𝑠𝑖=1𝑛𝑖𝑘𝑠𝑘𝑗=0𝑗𝑠𝑘(1)𝑠𝑘+𝑗𝑞𝑝(𝑥+2)𝑛1++𝑛𝑠𝑗𝑞𝑥𝑑𝜇1=(𝑥)𝑠𝑖=1𝑛𝑖𝑘𝑠𝑘𝑗=0𝑗𝑠𝑘(1)𝑠𝑘+𝑗𝑞2𝑞+1𝑞2𝐸𝑛1++𝑛𝑠𝑗,𝑞=12+𝑞𝐸𝑛1++𝑛𝑠,𝑞if𝑘=0,𝑠𝑖=1𝑛𝑖𝑘1𝑞𝑠𝑘𝑗=0𝑗𝑠𝑘(1)𝑠𝑘+𝑗𝐸𝑛1++𝑛𝑠𝑗,𝑞if𝑘>0.(3.11) Therefore, we obtain the following theorem.

Theorem 3.5. Let 𝑠. For 𝑛1,𝑛2,,𝑛𝑠,𝑘+ with 𝑛1+𝑛2++𝑛𝑠>𝑠𝑘, one has 𝑝𝑠𝑖=1𝐵𝑘,𝑛𝑖𝑞(𝑥)1𝑥𝑑𝜇1(𝑥)=2𝑞+𝐸𝑛1+𝑛2++𝑛𝑠,𝑞if𝑘=0,𝑠𝑖=1𝑛𝑖𝑘𝑠𝑘𝑗=0𝑗𝑠𝑘(1)𝑠𝑘+𝑗𝐸𝑛1+𝑛2++𝑛𝑠𝑗,𝑞if𝑘>0.(3.12)

For 𝑛1,𝑛2,,𝑛𝑠,𝑘+ by binomial theorem, we get𝑝𝑠𝑖=1𝐵𝑘,𝑛𝑖𝑞(𝑥)𝑥𝑑𝜇1=𝑛(𝑥)1𝑘𝑛𝑠𝑘𝑛1++𝑛𝑠𝑠𝑘𝑗=0𝑛1++𝑛𝑠𝑗𝑠𝑘(1)𝑗𝑝𝑥𝑗+𝑠𝑘𝑞𝑥𝑑𝜇1=𝑛(𝑥)1𝑘𝑛𝑠𝑘𝑛1++𝑛𝑠𝑠𝑘𝑗=0𝑛1++𝑛𝑠𝑗𝑠𝑘(1)𝑗𝐸𝑗+𝑠𝑘,𝑞1.(3.13)

By using (3.13) and Theorem 3.5, we obtain the following corollary.

Corollary 3.6. Let 𝑠. For 𝑛1,𝑛2,,𝑛𝑠,𝑘+ with 𝑛1+𝑛2++𝑛𝑠>𝑠𝑘, one has 𝑛1++𝑛𝑠𝑠𝑘𝑗=0𝑛1++𝑛𝑠𝑗(𝑠𝑘1)𝑗𝐸𝑗+𝑠𝑘,𝑞1=12+𝑞𝐸𝑛1+𝑛2++𝑛𝑠,𝑞if1𝑘=0,𝑞𝑠𝑘𝑗=0𝑗𝑠𝑘(1)𝑠𝑘+𝑗𝐸𝑛1+𝑛2++𝑛𝑠𝑗,𝑞if𝑘>0.(3.14)