A DETERMINANTAL EXPRESSION AND A RECURRENCE RELATION FOR THE EULER POLYNOMIALS
FENG QI
Institute of Mathematics, Henan Polytechnic University, Jiaozuo 454010, Henan Province, China; College of Mathematics, Inner Mongolia University for
Nationalities, Tongliao 028043, Inner Mongolia Autonomous Region, China; Department of Mathematics, College of Science, Tianjin Polytechnic University,
Tianjin 300387, China
BAI-NI GUO
School of Mathematics and Informatics, Henan Polytechnic University, Jiaozuo 454010, Henan Province, China
Abstract. In the paper, by a very simple approach, the author establishes an expression in terms of a lower Hessenberg determinant for the Euler polyno-mials. By the determinantal expression, the author finds a recurrence relation for the Euler polynomials. By the way, the author derives the corresponding expression and recurrence relation for the Euler numbers.
1. Main results
It is known that a matrix H = (hij)n×n is called a lower (or an upper, respec-tively) Hessenberg matrix if hij = 0 for all pairs (i, j) such that i+ 1 < j (or
j + 1 < i, respectively). Correspondingly, we can define a lower (or an upper, respectively) Hessenberg determinant.
It is general knowledge that the Bernoulli numbers and polynomials Bk and
Bk(u) can be generated respectively by
z ez−1 =
∞ X
k=0
Bk
zk k! = 1−
z
2 +
∞ X
k=1
B2k
z2k
(2k)!
E-mail addresses:[email protected], [email protected], [email protected], [email protected].
2010 Mathematics Subject Classification. Primary 11B68, Secondary 11C20, 11Y55, 15A15, 26A06, 33B10, 65F40.
Key words and phrases. determinantal expression; recurrence relation; Euler polynomial; Euler number; Hessenberg determinant.
This paper was typeset usingAMS-LATEX.
and
zeuz
ez−1 =
∞ X
k=0
Bk(u)
zk
k!
for |z| < 2π. Because the function x
ex−1 −1 +
x
2 is odd in x ∈ R, all of the Bernoulli numbersB2k+1 fork ∈Nequal 0. The first six Bernoulli numbers B2k for− ≤k≤5 are
B0= 1, B2= 1
6, B4=− 1
30, B6= 1
42, B8=− 1
30, B10= 5 66. In [4, Section 21.5] and [5, p. 1], it was listed that
Bk=k!
1 0 0 · · · 0 0 1
1
2! 1 0 · · · 0 0 0
1 3!
1
2! 1 · · · 0 0 0
..
. ... ... . .. ... ... ... 1
(k−1)! 1 (k−2)!
1
(k−3)! · · · 1 0 0 1
k!
1 (k−1)!
1 (k−2)! · · ·
1
2! 1 0 1
(k+1)! 1 k!
1 (k−1)! · · ·
1 3!
1 2! 0
.
In [7, Theorem 1.2], the Bernoulli polynomialsBk(u) fork∈Nwere expressed by
a lower Hessenberg determinant
Bk(u) = (−1)k
1
`+ 1 `+ 1
m
(1−u)`−m+1−(−u)`−m+1 1
≤`≤k,0≤m≤k−1 and, consequently, the Bernoulli numbersBkfork∈Nwere represented by a lower
Hessenberg determinant
Bk = (−1)k
1
`+ 1 `+ 1
m
1
≤`≤k,0≤m≤k−1
.
It is common knowledge that the Euler numbersEk and the Euler polynomials
Ek(x) can be generated respectively by
(1) 2e
t/2
et+ 1 =
∞ X
k=0
Ek
k! t
2 k
and
(2) 2e
xt
et+ 1 =
∞ X
k=0
Ek(x)
k! t k
which converge uniformly with respect to t ∈ (−π, π). By these definitions, it is easy to see that
(3) Ek= 2kEk
1 2
.
Since the generating function 2eett/+12 of the Euler numbers Ek is even on (−π, π), thenE2k−1= 0 for allk∈N. The first nine Euler numbersE2k for 0≤k≤8 are
1, −1, 5, −61, 1385, −50521, 2702765, −199360981
and the first six Euler polynomialsEk(x) for 0≤k≤5 are
1, x−1 2, x
2−x, x3−3 2x
2+1 4, x
4−2x3+x, x5−5 2x
4+5 2x
At the website [9], the Euler numbersE2kwere represented by a lower Hessenberg determinant
E2k= (−1)k(2k)!
1
2! 1 0 · · · 0 0
1 4!
1
2! 1 · · · 0 0
..
. ... ... . .. ... ... 1
(2k−2)! 1 (2k−4)!
1
(2k−6)! · · · 1 2! 1 1
(2k)! 1 (2k−2)!
1
(2k−4)! · · · 1 4! 1 2!
, k∈N.
In [8, Theorem 1.1], the Euler numbersE2k fork∈Nwere represented by a lower
Hessenberg and sparse determinant
E2k = (−1)k
i
j−1
cos
(i−j+ 1)π 2 (2k) ×(2k) .
There have been many explicit expressions for the Euler numbers Bk and the Euler polynomials Ek(x). See, for example, the recently-published papers [2, 3, 8] and plenty of references therein.
In this paper, by a very simple approach, we will establish a new expression in terms of a lower Hessenberg determinant for the Euler polynomialsEk(x). By the new determinantal expression, we will find a recurrence relation for the Euler poly-nomials. By the way, we will derive the corresponding expression and recurrence relation for the Euler numbersEk.
Our main results can be summarized up as two theorems below.
Theorem 1. Fork≥0, the Euler polynomials Ek(x)can be expressed as
(4) Ek(x) = (−1)k 2k
1 2 0 0 · · · 0 0 0
x 10 2 0 · · · 0 0 0
x2 20 21 2 · · · 0 0 0
x3 3
0 3 1 3 2
· · · 0 0 0
..
. ... ... ... . .. ... ... ...
xk−2 k−2 0
k−2 1
k−2 2
· · · kk−−23
2 0
xk−1 k−01 k−11 k−21 · · · kk−−13 k−1 k−2
2
xk k
0 k 1 k 2
· · · k k−3
k
k−2
k
k−1
and, consequently, the Euler numbers Ek can be expressed as
(5) Ek = (−1)k
1 2 0 0 · · · 0 0 0
1 2
1 0
2 0 · · · 0 0 0
1 22 2 0 2 1
2 · · · 0 0 0
1 23 3 0 3 1 3 2
· · · 0 0 0
..
. ... ... ... . .. ... ... ... 1
2k−2 k−2
0
k−2 1
k−2 2
· · · kk−−23
2 0
1 2k−1
k−1 0
k−1 1
k−1 2
· · · kk−−13 k−1 k−2
2 1 2k k 0 k 1 k 2
· · · k k−3
k
k−2
k
k−1
.
Theorem 2. The Euler polynomials and numbersEk(x)andEk satisfy the recur-rence relations
(6) Ek(x) =−
1 2
k−1
X
`=0
k
`
E`(x) +xk
and, consequently,
(7) Ek=−2k−1
k−1
X
`=0 1 2`
k
`
E`+ 1.
2. Proofs of Theorems 1 and 2
Now we start out to prove our main results.
Proof of Theorem 1. In [6, Section 2.2, p. 849], [7, p. 94], and [8, Lemma 2.1], Exercise 5) in [1, p. 40] was reformulated as the following conclusion. Let u(x) and v(x) 6= 0 be two differentiable functions. LetU(n+1)×1(x) be an (n+ 1)×1 matrix whose elementsuk,1(x) = u(k−1)(x) for 1≤k≤n+ 1, let V(n+1)×n(x) be an (n+ 1)×nmatrix whose elements
vi,j(x) =
i−1
j−1
v(i−j)(x), i−j ≥0
0, i−j <0
for 1≤i≤n+ 1 and 1≤j ≤n, and let|W(n+1)×(n+1)(x)|denote the determinant of the (n+ 1)×(n+ 1) matrix
W(n+1)×(n+1)(x) = U(n+1)×1(x) V(n+1)×n(x)
.
Then thenth derivative of the ratio u(x)v(x) can be computed by
(8) d
n
dxn
u(x)
v(x)
= (−1)n
W(n+1)×(n+1)(x)
vn+1(x) .
Letu(t) =ext andv(t) =et+ 1. Then, by virtue of the formula (8),
dk dtk
ext
et+ 1
= (−1)
k
×
ext et+ 1 0 · · · 0 0 0
xext 1
0
et et+ 1 · · · 0 0 0
x2ext 20et 21et · · · 0 0 0
x3ext 30et 31et · · · 0 0 0 ..
. ... ... . .. ... ... ...
xk−2ext k−02et k−12et · · · kk−−23
et et+ 1 0
xk−1ext k−1 0
et k−1 1
et · · · k−1 k−3
et k−1 k−2
et et+ 1
xkext k 0
et k
1
et · · · k k−3
et k
k−2
et k
k−1
et →(−1) k 2k+1
1 2 0 0 · · · 0 0 0
x 10
2 0 · · · 0 0 0
x2 20 21 2 · · · 0 0 0
x3 3
0 3 1 3 2
· · · 0 0 0
..
. ... ... ... . .. ... ... ...
xk−2 k−02 k−12 k−22 · · · kk−−23
2 0
xk−1 k−1 0
k−1 1
k−1 2
· · · kk−−13 k−1 k−2
2
xk k
0 k 1 k 2
· · · k k−3
k
k−2
k
k−1
ast→0 fork≥0. By the equation (2), the formula (4) is thus proved.
Considering the relation (3) and taking x = 12 in (4) lead to the formula (5)
readily. The proof of Theorem 1 is complete.
Proof of Theorem 2. Let
Dk+1(x) =
1 2 0 0 · · · 0 0 0
x 10 2 0 · · · 0 0 0
x2 2
0
2
1
2 · · · 0 0 0
x3 3
0 3 1 3 2
· · · 0 0 0
..
. ... ... ... . .. ... ... ...
xk−2 k−2 0
k−2 1
k−2 2
· · · kk−−23
2 0
xk−1 k−01 k−11 k−21 · · · kk−−13 k−1 k−2
2
xk k
0 k 1 k 2
· · · k−k3 k k−2
k
k−1
for k ≥ 0. Expanding Dk+1(x) according to the last column consecutively and inductively reveals
Dk+1(x) =
k
k−1
1 2 0 0 · · · 0 0
x 10 2 0 · · · 0 0
x2 2
0
2
1
2 · · · 0 0
x3 3
0 3 1 3 2
· · · 0 0
..
. ... ... ... . .. ... ...
xk−2 k−2 0
k−2 1
k−2 2
· · · k−2 k−3
2
xk−1 k−01 k−11 k−21 · · · kk−−13 k−1 k−2
−2
1 2 0 0 · · · 0 0
x 10
2 0 · · · 0 0
x2 2
0
2
1
2 · · · 0 0
x3 3
0 3 1 3 2
· · · 0 0
..
. ... ... ... . .. ... ...
xk−2 k−2 0
k−2 1
k−2 2
· · · k−2 k−3
2
xk k
0 k 1 k 2
· · · k−k3 k k−2
= k k−1
1 2 0 0 · · · 0 0
x 10
2 0 · · · 0 0
x2 20 21 2 · · · 0 0
x3 3
0 3 1 3 2
· · · 0 0
..
. ... ... ... . .. ... ...
xk−2 k−02 k−12 k−22 · · · kk−−23 2
xk−1 k−01 k−11 k−21 · · · kk−−13 k−1 k−2
−2 k
k−2
1 2 0 0 · · · 0 0
x 10
2 0 · · · 0 0
x2 2
0
2
1
2 · · · 0 0
x3 30 31 32 · · · 0 0
..
. ... ... ... . .. ... ...
xk−3 k−3 0
k−3 1
k−3 2
· · · kk−−34 2
xk−2 k−2 0
k−2 1
k−2 2
· · · k−2 k−4
k−2 k−3
+ 22
k
k−3
1 2 0 0 · · · 0 0
x 10 2 0 · · · 0 0
x2 2
0
2
1
2 · · · 0 0
x3 3
0 3 1 3 2
· · · 0 0
..
. ... ... ... . .. ... ...
xk−4 k−4 0
k−4 1
k−4 2
· · · kk−−45 2
xk−3 k−03 k−13 k−23 · · · kk−−35 k−3 k−4
−23
1 2 0 0 · · · 0 0
x 10
2 0 · · · 0 0
x2 2
0
2
1
2 · · · 0 0
x3 30 31 32 · · · 0 0
..
. ... ... ... . .. ... ...
xk−4 k−4 0
k−4 1
k−4 2
· · · kk−−45 2
xk k
0 k 1 k 2
· · · k k−5
k
k−4
= m X `=0 (−1)`2`
k
k−`−1
×
1 2 0 · · · 0 0
x 10
2 · · · 0 0
x2 2
0
2
1
· · · 0 0
x3 3
0
3
1
· · · 0 0
..
. ... ... . ... ...
xk−m−2 k−m−2 0
k−m−2 1
· · · k−m−2 k−m−3
2
xk k
0
k
1
· · · k−mk−3 k k−m−2
= k−2
X
`=0 (−1)`2`
k
k−`−1
Dk−`(x) + (−1)k−12k−1
1 2
xk k
0
= k−2
X
`=0 (−1)`2`
k
k−`−1
Dk−`(x) + (−1)k−12k−1
k
0
−2xk
= k−1
X
`=0 (−1)`2`
k
k−`−1
Dk−`(x) + (−1)k2kxk
= k−1
X
`=0 (−1)`2`
k
k−`−1
2k−`−1 (−1)k−`−1
(−1)k−`−1
2k−`−1 Dk−`(x)
+ (−1)k2kxk
= (−1)k−12k−1 k−1
X
`=0
k
k−`−1
Ek−`−1(x) + (−1)k2kxk.
Accordingly, it follows that
Ek(x) = (−1)k
2k Dk+1(x) =− 1 2
k−1
X
`=0
k
k−`−1
Ek−`−1(x) +xk
=−1 2
k−1
X
`=0
k `
E`(x) +xk.
The relation (6) is thus proved.
Takingx= 12 in (6) and making use of the relation (3) result in the relation (7).
The proof of Theorem 2 is complete.
Remark 1. The expression (5) can also be obtained by applying the formula (8) to the functionsu(t) =et/2andv(t) =et+ 1 and considering the generating function
2et/2
et+1 in the equation (1).
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URL:https://qifeng618.wordpress.com