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Applied Mathematics & Information Sciences – An International Journal c °2009 Dixie W Publishing Corporation, U. S. A. 3(1) (2009), 53–58 An Explicit Formula for the Euler Polynomials of Higher Order Qiu-Ming Luo1,2 1 Department of Mathematics, East China Normal University Dongchuan Road 500, Shanghai 200241, China 2 Department of Mathematics, Jiaozuo University, Henan Jiaozuo 454003, China Email Address: [email protected] Received March 23, 2008; Revised June 18, 2008 We obtain an explicit formula for the Euler polynomials of higher order in terms of the Gaussian hypergeometric function. The corresponding new formulas of the Euler polynimials and numbers are also deduced. Finally, we also remark some possible applications of these results in the number theory and information science fields. Keywords: Euler numbers of higher order, Euler polynomials of higher order, Gaussian hypergeometric function, Stirling numbers of the second kind, difference operator, coding theory and cryptography. 1 Introduction The classical Bernoulli polynomials Bn (x) and Euler polynomials En (x) together (α) (α) with their familiar generalizations Bn (x) and En (x) of (real or complex) order α, are usually defined by means of the following generating functions (see, for details, [1, 3, 8]): µ and z ez − 1 µ ¶α 2 ez + 1 exz = ∞ X Bn(α) (x) n=0 ¶α exz = ∞ X En(α) (x) n=0 zn n! (|z| < 2π; 1α := 1) , (1.1) zn n! (|z| < π; 1α := 1) , (1.2) respectively. The classical Bernoulli and Euler polynomials are respectively found from (1.1) and (1.2) as follows: Bn (x) := Bn(1) (x) and En (x) := En(1) (x) (n ∈ N0 ) . (1.3) 54 Qiu-Ming Luo Further the classical Bernoulli numbers Bn and Euler numbers En with their forms of higher order are µ ¶ 1 Bn := Bn (0) and En := 2n En , 2 (1.4) ³α´ , Bn(α) := Bn(α) (0) and En(α) := 2n En(α) 2 respectively. Recently, Luo et al. [6] gave certain new recursive formulas for the Euler numbers and polynomials of higher order; Luo [7] further obtained several formulas involving the Stirling numbers of the second kind. Srivastava and Todorov [9] gave some elegant formulas for the Bernoulli numbers and polynomials of higher order as follows Bn(α) = n X µ k (−1) k=0 ¶µ ¶µ ¶−1 α+n α+k−1 n+k S(n + k, k) n−k k k (1.5) and Bn(α) (x) = ¶ µ ¶ n µ ¶µ k X n α + k − 1 k! X k 2k (−1)j j (x + j)n−k k k (2k)! j=0 j k=0 h j i . × 2 F1 k − n, k − α; 2k + 1; x+j (1.6) Here 2 F1 [a, b; c; z] denotes the Gaussian hypergeometric function defined by (see [1, 15.1.1]) 2 F1 [a, b; c; z] = ∞ X (a)n (b)n z n , (c)n n! n=0 (1.7) where (λ)0 = 1, (λ)n = λ(λ + 1) · · · (λ + n − 1) = Γ(λ + n)/Γ(λ) (n ≥ 1). 2 An Explicit Formula of En(α) (x) in Terms of the Gaussian Hypergeometric Function In the present section, we will prove an explicit formula for the Euler polynomials of higher order which is an analogue of the formula (1.6). We need the following lemmas before proving main result. Lemma 2.1. For n = 0, 1, . . . , x ∈ R, α ∈ C, the following formulas are true En(α) (x) = n µ ¶ (α) ³ X n E k=0 k k 2k x− α ´n−k , 2 An Explicit Formula for the Euler Polynomials of Higher Order 55 En(α) (x) = (−1)n En(α) (α − x), n µ ¶ ³ ´ X n (−x)n−k (α) (α) x En = Ek (x). k 2 2n−k k=0 Proof. From (1.2), we can readily obtain above formulas. Clearly, by Lemma 2.1 we have En(α) (α) = (−1)n En(α) (0), n µ ¶ ³ ´ X n (−α)n−k (α) (α) α En Ek (α). = 2 2n−k k (2.1) k=0 Theorem 2.1. For n = 0, 1, . . . , x ∈ R, α ∈ C, the following formula in terms of the Gaussian hypergeometric function is true µ ¶µ ¶ k µ ¶ n X 1 n α+k−1 X j k En(α) (x) = (−1) j k (x + j)n−k 2k k k j j=0 k=0 (2.2) h j i × 2 F1 k − n, k; k + 1; . x+j Proof. By Taylor’s expansion and Leibniz’s rule, the generating relation (1.2) yields n µ ¶ X n n−s s n³ 2 ´α o¯¯ d (α) En (x) = x Dz . (2.3) ¯ , Dz = z s e +1 dz z=0 s=0 Since (1 + w)−α = ¶ ∞ µ X α+k−1 (−w)k k (|w| < 1), k=0 setting 1 + w = (ez + 1)/2 and applying the binomial theorem, we find from (2.3) that µ ¶ n µ ¶ s X n n−s X (−1)k α + k − 1 (α) x En (x) = Dzs {(ez − 1)k }|z=0 . (2.4) k s 2 k s=0 k=0 Now we make use of the well-know formula (see [1, 24.1.4]) (ez − 1)k = ∞ X zr r=k r! ∆k 0r , S(r, k) = 1 k r ∆ 0 , k! (2.5) where S(r, k) denotes the Stirling number of the second kind defined by r µ ¶ X x xr = k!S(r, k). k k=0 For convenience we write ∆k ar = ∆k xr |x=a = µ ¶ k X k (−1)k−j (a + j)r , j j=0 (2.6) 56 Qiu-Ming Luo where ∆ is the difference operator defined by (see [1, pp. 822, III]) ∆f (x) = f (x + 1) − f (x). So, in general (see [1, pp. 823, 24.1.1]), k ∆ f (x) = k X k−j (−1) j=0 µ ¶ k f (x + j). j From (2.5) we find that Dzs {(ez − 1)k }|z=0 = ∆k 0s = k!S(s, k). Substituting this value into (2.4) yields µ ¶ n µ ¶ s X n n−s X (−1)k k! α + k − 1 (α) En (x) = x S(s, k), s 2k k s=0 (2.7) (2.8) k=0 or En(α) (x) = µ ¶ n µ ¶ s X n n−s X (−1)k α + k − 1 x ∆ k 0s . k s 2 k s=0 (2.9) k=0 If we rearrange the resulting duple series (2.9), we have ¶ µ ¶ n−k µ n X n (−1)k α + k − 1 X xn−s−k ∆k 0s+k . En(α) (x) = s + k 2k k s=0 (2.10) k=0 Further substituting for ∆k 0s+k from the definition (2.6) with a = 0 into (2.10), we get that µ ¶µ ¶ µ ¶ n k X 1 n α + k − 1 n−k X j k En(α) (x) = x (−1) jk 2k k k j j=0 k=0 (2.11) h i −j × 2 F1 k − n, 1; k + 1; . x Finally, we apply the known transformation [1, 15.3.4] h z i −a 2 F1 [a, b; c; z] = (1 − z) 2 F1 a, c − b; c; z−1 and (2.11) leads immediately to the desired (2.2). 3 Further Remarks Remark 3.1. Taking α = 1 in (2.2), we obtain the following new formula for the Euler polynomials µ ¶ k µ ¶ n h X 1 n X j i j k k n−k . En (x) = (−1) j (x + j) F k − n, k; k + 1; 2 1 2k k j=0 x+j j k=0 An Explicit Formula for the Euler Polynomials of Higher Order 57 Remark 3.2. By [1, 15.1.20], we have 2 F1 [a, b; c; 1] = Γ(c)Γ(c − a − b) Γ(c − a)Γ(c − b) (c 6= 0, −1, −2, . . . , <(c − a − b) > 0), which (for a = k − n, b = k, and c = k + 1) readily yields 2 F1 [k − n, k; k + 1; 1] = µ ¶−1 n , k (0 ≤ k ≤ n). (3.1) In view of (3.1) and the special case when x = 0 in formula (2.2), we get that En(α) (0) µ ¶ k µ ¶ n X 1 α+k−1 X j k (−1) = jn, 2k k j j=0 (3.2) µ ¶ n X (−1)k k! α + k − 1 S(n, k). = 2k k (3.3) k=0 or equivalently, En(α) (0) k=0 (α) Moreover, we note that, with En order can be written as En(α) = n µ ¶ X n k=0 k (α) := 2n En (α/2) and (2.1), the Euler numbers of higher 2k αn−k µ ¶ k X (−1)j j! α + j − 1 S(k, j). 2j j j=0 (3.4) Further, setting α = 1 in formula (3.4), we deduce easily the following formula for the Euler numbers n µ ¶ k X n k X (−1)j j! En = S(k, j). (3.5) 2 2j k j=0 k=0 Acknowledgements This research was supported, in part, by the Henan Innovation Project For University Prominent Research Talents, China under Grant 2007KYCX0021; Natural Science Foundation of Henan Province, China under Grant 0511015500; and Natural Science for Basic Research of Education Office of Henan Province, China under Grant 2007110022. References [1] M. Abramowitz and I. A. Stegun (Eds), Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables, National Bureau of Standards, Applied Mathematics Series 55, 4th printing, Washington, 1965. 58 Qiu-Ming Luo [2] C. Berge, Principles of Combinatorics, Academic Press, 1971. [3] A. Erdélyi, W. Magnus, F. Oberhettinger and F. G. Tricomi, Higher Transcendental Functions, Volume I, McGraw-Hill, New York, 1953. [4] P. Garrett, The Mathematics of Coding Theory, Prentice Hall, 2003. [5] K. Knopp, Infinite Sequences and Series, Dover, 1956. [6] Q.-M. Luo, Y. Zheng and F. Qi, Euler numbers of higher order and Euler polynomials of higher order, Henan Science, 21 (2003), 1–6 (in Chinese). [7] Q.-M. Luo. The Euler polynomials of higher order involving the Stirling numbers of the second kind, Austral. Math. Soc. Gaz. 31 (2004), 194–196. [8] W. Magnus, F. Oberhettinger and R. P. Soni, Formulas and Theorems for the Special Functions of Mathematical Physics, Third Enlarged Edition, Springer-Verlag, New York, 1966. [9] H. M. Srivastava and P. G. Todorov, An explicit formula for the generalized Bernoulli polynoaials, J. Math. Anal. Appl. 130 (1988), 509–513. [10] Y. Wang, H. Li and C. Liang, Information and coding theory, Higher Education Publishing Company, Beijing, 2005 (in Chinese).