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##  eISSN 0454-8124
pISSN 1225-6951

### Article

Kyungpook Mathematical Journal 2021; 61(3): 473-486

Published online September 30, 2021

### Lucas-Euler Relations Using Balancing and Lucas-Balancing Polynomials

Robert Frontczak, Taras Goy*

e-mail : robert.frontczak@lbbw.de

Faculty of Mathematics and Computer Science, Vasyl Stefanyk Precarpathian National University, Ivano-Frankivsk 76018, Ukraine
e-mail : taras.goy@pnu.edu.ua

Received: October 21, 2021; Revised: March 12, 2021; Accepted: March 23, 2021

We establish some new combinatorial identities involving Euler polynomials and balancing (Lucas-balancing) polynomials. The derivations use elementary techniques and are based on functional equations for the respective generating functions. From these polynomial relations, we deduce interesting identities with Fibonacci and Lucas numbers, and Euler numbers. The results must be regarded as companion results to some Fibonacci-Bernoulli identities, which we derived in our previous paper.

Keywords: Euler polynomials and numbers, Bernoulli numbers, balancing polynomials and numbers, Fibonacci numbers, generating function.

In 1975, Byrd  derived the following identity relating Lucas numbers to Euler numbers:

k=0 n/2n2k54kLn2kE2k=21n.

In , Wang and Zhang obtained a more general result valid for j≥ 1 as follows

k=0 n/2n2k54kFj2kLj(n2k)E2k=21nLjn.

Castellanos  found

k=0n2n2k22k1L2(nk)jLj2kE2k=(54)nFj2n,

which expresses even powers of Fibonacci numbers in terms of Lucas and Euler numbers.

Here, as usual, Fibonacci and Lucas numbers satisfy the recurrence relation un=un1+un2, n≥ 2, with initial conditions F0 = 0, F1 = 1 and L0 = 2, L1 = 1, respectively, whereas Euler numbers (En)n0 are given by the power series

n=0Enznn!=1coshz.

Fibonacci and Lucas numbers are entries A000045 and A000032 in the On-Line Encyclopedia of Integer Sequences , respectively.

The Lucas-Euler pair may be regarded as the twin of the Fibonacci-Bernoulli pair. In the last years, there has been a growing interest in deriving new relations for these two pairs of sequences. For example, Zhang and Ma  proved a relation between Fibonacci polynomials and Bernoulli numbers (Bn)n0 defined by

n=0Bnznn!=zez1.

The following identity is a special case of their result:

k=0nnk5nk2FkBnk=nβn1,

where β=(15)/2, or, equivalently,

k=0 n/2n2k5kFn2kB2k=nLn12.

See also [14, 18, 19, 20] for other results in this direction. Recently, Frontczak , Frontczak and Goy , and Frontczak and Tomovski  proved some generalizations of existing results. For instance, from  we have

k=0nnk(5Fj)nkFjkBnk=nFjβj(n1),

which holds for all j ≥ 1 and generalizes (1.4) to an arithmetic progression, and

k=0 n/2n2k(20k5k)F2j2kL2j(n2k)B2k=5n2F2jF2j(n1).

Note, since B2n+1=0 for n≥1, from (1.4) we get Kelisky's formula 

k=0 n/2n2k5kFj2kFj(n2k)B2k=n2FjLj(n1).

In this paper, we present new identities linking Lucas numbers to Euler numbers (polynomials). The results stated are polynomial generalizations of (1.4) and are complements of the recent discoveries from [5, 7].

Throughout the paper, we will work with different kind of polynomials of a complex variable x: Euler polynomials (En(x))n0, Bernoulli polynomials (Bn(x))n0, balancing polynomials (Bn*(x))n0, and Lucas-balancing polynomials (Cn(x))n0.

Euler and Bernoulli polynomials are famous mathematical objects and are fairly well understood. They are defined by [3, Chapter 24]

H(x,z)= n=0Bn(x)znn!=zexzez1  (|z|<2π)

and

I(x,z)= n=0En(x)znn!=2exzez+1  (|z|<π).

The numbers Bn(0)=Bn are the famous Bernoulli numbers. Bernoulli numbers are rational numbers starting with B0=1, B1=-1/2, B2=1/6, B4=-1/30, B6=1/42, and so on. Also, as already mentioned, B2n+1=0 for n≥ 1. Euler numbers En are obtained from I(1/2,2z) that is

En=2nEn(1/2).

In contrast to Bernoulli numbers, Euler numbers are integers where E0=1, E2=-1, E4=5 and E2n+1=0 for n≥ 0. Explicit formulas for the polynomials are

Bn(x)= k=0 nnkBkxnkandEn(x)= k=0 nnkEk2k(x12)nk.

Euler polynomials can be expressed in terms of Bernoulli polynomials via

En(x)=2n+1(Bn+1(x)2n+1Bn+1(x2)).

Particularly,

En(0)=2(12n+1)n+1Bn+1.

Balancing polynomials are of younger age and are introduced in the next section.

Balancing polynomials Bn*(x) and Lucas-balancing polynomials Cn(x) are generalizations of balancing and Lucas-balancing numbers . These polynomials satisfy the recurrence wn(x)=6xwn1(x)wn2(x), n≥ 2, but with the respectively initial conditions B0*(x)=0, B1*(x)=1 and C0(x)=1, C1(x)=3x. The Binet formulas for these polynomials are

Bn*(x)=λn(x)λn(x)29x21andCn(x)=λn(x)+λn(x)2,

where λ(x)=3x+9x21. Also, the following explicit formulas hold [15, 16]

Bn*(x)=k=0(n1)/2(1)kn1kk(6x)n12k,  n0,Cn(x)=n2k=0n/2(1)knknkk(6x)n2k,  n1.

Consult the papers [4, 6, 10, 11, 12, 13, 16] for more information about these polynomials. The numbers Bn*(1)=Bn* and Cn(1)=Cn are called balancing and Lucas-balancing numbers, respectively. These numbers are indexed in  under entries A001109 and A001541.

Balancing and Lucas-balancing polynomials possess interesting properties. They are related to Chebyshev polynomials by simple scaling [Lemma 2.1]. The exponential generating functions for balancing and Lucas-balancing polynomials are derived in [4, 6]. Here, however, we will only need the results from : Let b1(x,z) and b2(x,z) be the exponential generating functions of odd and even indexed balancing polynomials, respectively. Then

b1(x,z)=n=0B 2n+1*(x)znn!  =e (18x21)z 9x21(3xsinh(6x9x21z)+9x21cosh(6x9x21z))

and

b2(x,z)= n=0B2n*(x)znn!=e(18x21)z9x21sinh(6x9x21z).

Similarly, the exponential generating functions for Lucas-balancing polynomials are found to be

c1(x,z)=n=0C 2n+1(x)znn!  =e(18x21)z(3xcosh(6x9x21z)+9x21sinh(6x9x21z))

and

c2(x,z)= n=0C2n(x)znn!=e(18x21)zcosh(6x9x21z).

Connections between Bernoulli polynomials Bn(x) and balancing polynomials Bn*(x) have been established in the recent papers [5, 7]. They are interesting, as they instantly give relations between Bernoulli numbers and Fibonacci and Lucas numbers. The links are the following evaluations 

Bn*(ωsLs6)=ωsn1FsnFs,  Cn(ωsLs6)=ωsnLsn2,

where ωs=1, if s is even, and ωs=i=1, if s is odd. These links will be used to prove our results.

### 3. Relations Between Euler and Balancing (Lucas-Balancing) Polynomials

We start with the following result involving even indexed balancing and Lucas-balancing polynomials.

Theorem 3.1. For each n≥ 1 and x, we have

k=1n/2n12k1C2(n2k)(x)(144x2(9x21))kE2k1(0)              =12x(19x2)B2n2*(x).

Proof. Since tanhz=12e2z+1, from (1.8) we get

I(0,12x9x21z)=1tanh(6x9x21z)

and, by (2.2) and (2.4),

n=0(k=0nnkC2(nk)(12x9x21)kEk(0))znn!    =n=0(k=0n1nkC2k(12x9x21)nkEnk(0)+C2n(x))znn!    =c2(x,z)I(0,12x9x21z)    =e(18x21)z(cosh(6x9x21z)sinh(6x9x21z))    =c2(x,z)9x21b2(x,z)    =n=0(C2n(x)9x21B2n*(x))znn!.

Thus,

k=0nnkC2(nk)(12x9x21)kEk(0)=C2n(x)9x21B2n*(x).

Since E2n1=0 for n ≥ 1, after some algebra we have (3.1).

Corollary 3.2. For each n ≥ 1 and j ≥ 1,

k=0 n/2n12k15k1F2j2k1L2j(n2k)E2k1(0)=F2j(n1).

Proof. Evaluate (3.1) at the x=ωjLj/6 and use the links from (2.5). To simplify recall that Ln25Fn2=(1)n4 and F2n=FnLn.

Using (1.10), we can write (3.2) as

k=0 n/2n12k120k5kkF2j2k1L2j(n2k)B2k=5F2j(n1),

which is easily reduced to (1.6).

We also have the following interesting identity.

Theorem 3.3. For each n0 and x, we have the relation

k=0 n/2n2kC2(n2k)(x)(36x2(9x21))kE2k=(18x21)n.

Proof. The result is a consequence of the fact that

c2(x,z)I(1/2,12x9x21z)=e(18x21)z.

Corollary 3.4. For each n ≥ 0 and j ≥ 1,

k=0 n/2n2k(54)kF2j2kL2j(n2k)E2k=21nL2jn.

Proof. Evaluate (3.3) at the point x=ωjLj/6 and use the links from (2.5). When simplifying you will also need the formula Ln2L2n=(1)n2.

Interestingly, if j=1/2 from (3.4) we obtain Byrd's result (1.4). Also, when j=1 and j=2, from (3.4) we obtain the following Lucas-Euler relations:

k=0n/2n2k(54)kL2(n2k)E2k=2(32)n,k=0n/2n2k(454)kL4(n2k)E2k=2(72)n,

respectively. The first example appears as equation (31) in .

A different expression for the sum on the left of (3.3) is stated next.

Theorem 3.5. For each n0 and x, we have

k=0n/2n2kC2(n2k)(x)(36x2(9x21))kE2k        =k=0nnk(C2k(x)9x21B2k*(x))(6x9x21)nk.

Proof. We use the identity

I(1/2,2z)=ez(1tanhz),

from which the functional equation follows

c2(x,z)I(1/2,12x9x21z)=e(6x9x21)z(c2(x,z)9x21b2(x,z)).

Thus,

k=0nnkC2k(x)(6x9x21)nkEnk      =k=0nnk(C2k(x)9x21B2k*(x))(6x9x21)nk,

that is equivalent to (3.6).

Theorem 3.4. For each n≥ 0 and x, it is true that

k=0nnkC2(nk)(x)12x 9x21kEk(x)=(18x21+6x(2x1)9x2 1)n.

Proof. The functional relation cosh(z/2)I(x,z)=e(x1/2)z produces immediately

c2(x,z)I(x,12x9x21z)=e18x21+6x(2x1)9x2 1z.

Comparing the coefficients of z in the power series expansions on both sides gives the identity.

When x=1/2, then we recover (3.5), by (1.9).

The following result appears as Theorem 13 in : For each n ≥ 0, j ≥ 1, and x, we have

k=0nnkFjk(5Fj)nkBnk(x)=nFj((5x+β)Fj+Fj1)n1, k=0nnkFjk(5Fj)nkBnk(x)=nFj((α5x)Fj+Fj1)n1,

where α=(1+5)/2 is the golden ratio and β=(15)/2=1/α.

Now, we present the analogue result for the Lucas-Euler pair:

Theorem 4.1. The following polynomial identity is valid for all n ≥ 0, j ≥ 1, and x:

k=0nnkLjk(5Fj)nkEnk(x)=2((5x+β)Fj+Fj1)n, k=0nnkLjk(5Fj)nkEnk(x)=2((α5x)Fj+Fj1)n.

Proof. Let L(z) be the exponential generating function for (Ljn)n0, j ≥ 1. Then, using the Binet formula for Ln, we get

L(z)=2e(1/2Fj+Fj1)zcosh(5Fj2z).

Thus, it follows that

n=0(k=0nnkLjk(5Fj)nkEnk(x))znn!=L(z)I(x,5Fjz)              =2e((x1/2)5Fj+1/2Fj+Fj1)z              =2e((5x+β)Fj+Fj1)z.

This proves the first equation. The second follows upon replacing x by 1-x and using En(1x)=(1)nEn(x) and αβ=5.

Note that the relations (4.1) and (4.2) provide a generalization of (3.4).

To see this, notice that they can be written more compactly as

k=0nnkLjk(±5Fj)nkEnk(x)=21n(Lj±5Fj(2x1))n.

Now, if x=1/2, we get

k=0nnk(±5Fj)nk2kLjkEnk=2Ljn,

which is equivalent to (3.4). We also mention the nice and curious identities

k=0nnk(±5Fj)nkLjkEnk(α)=2(±1)nLj±1n, k=0nnk(±5Fj)nkLjkEnk(β)=2(1)nLj1n,

which can be deduced from (3.4) and 5Fn=Ln+1+Ln1.

We conclude this presentation with the following interesting corollary.

Corollary 4.2. Let n, j and q be integers with n, j ≥ 1 and q odd. Then it holds that

k=0nnk(5Fj)nk(q(nk)1)LjkEnk(0)=2qn r=1 q1(1)r(rαj+(qr)βj)n.

Proof. The known multiplication formula for Euler polynomials for odd q [3, Chapter 24]

qn r=0 q1(1)rEn(x+rq)=En(qx)

yields

r=1 q1(1)rEn(rq)=(qn1)En(0).

Therefore,

k=0nnkLjk(5Fj)nk(q(nk)1)Enk(0)      =2r=1q1(1)r((5rq+β)Fj+Fj1)n      =2qnr=1q1(1)r(5rFj+q(βFj+Fj1))n      =2qnr=1q1(1)r(rαj+(qr)βj)n.

The special instances for j=1, and q=3 and q=5, respectively, take the form

k=0nnk(5)nk(3(nk)1)Enk(0)=253nF2n

and

k=0nnk(5)nk(5(nk)1)LkEnk(0)=25 (1n)/2 (F 2n F n ),ifniseven;25 n/2 (L 2n L n ),ifnisodd.

In this section, we derive some mixed identities involving Bernoulli (Euler) polynomials and Bernoulli, Fibonacci and Lucas numbers.

Theorem 5.1. For each n,j0 and x,

k=0nnk(±5Fj)kLj(nk)Bk(x)    =21nk=0n/2n2k20kFj2k(±5Fj(2x1)+Lj)n2kB2k.

Proof. The result follows from the functional relation

H(x,±5Fjz)L(z)=5Fje(±(x1/2)5Fj+1/2Lj)zzcoth(5Fj2z)

and the well-known power series cothz= n=04nB 2n(2n)!z2n1.

If x=1/2, from (5.1) using Bn(1/2)=(21n1)Bn, we obtain the following result.

Corollary 5.2. For each n,j0,

k=0 n/2n2k5k(212k1)Fj2kLj(n2k)B2k=21nLjn k=0 n/2n2k20k( Fj Lj )2kB2k.

For example,

k=0 n/2n2k(212k1)5kB2kLn2k=21n k=0 n/2n2k20kB2k

and

k=0 n/2n2k(212k1)20kB2kL3(n2k)=21+n k=0 n/2n2k5kB2k.

If x = α and x=β, where α=(1+5)/2 is the golden ratio and β=-1/α, from (5.1) we have the following corollary.

Corollary 5.3. For each n,j0,

k=0nnk(5Fj)kLj(nk)Bk(α)=2Lj+1n k=0 n/2 n2k5k(FjL j+1)2kB2k, k=0nnk(5Fj)kLj(nk)Bk(α)=2(1)nLj1n k=0 n/2 n2k5k(FjL j1)2kB2k

and

k=0nnk(5Fj)kLj(nk)Bk(β)=2(1)nLj1n k=0 n/2 n2k5k(FjL j1)2kB2k,[2pt] k=0nnk(5Fj)kLj(nk)Bk(β)=2Lj+1n k=0 n/2 n2k5k(FjL j+1)2kB2k.

Finally, we present the theorem for Fibonacci-Euler pair.

Theorem 5.4. or each n ≥ 0 and j ≥ 1,

(n+1)k=0nnk(5Fj)kFj(nk)Ek(x)=4k=0n+12n+12k5k1(4k1)Fj2k1Fj2+Fj1+5Fj(x12)n+12kB2k

and

(1)n(n+1)k=0nnk(5Fj)kFj(nk)Ek(x)=4k=0n+12n+12k5k1(4k1)Fj2k1Fj2+Fj15Fj(x12)n+12kB2k.

Proof. Let F(z) be the exponential generating function for (Fjn)n0 with j ≥1. Then, using the Binet formula for Fn, we get

F(z)=25e1/2Fj+Fj1zsinh(5Fj2z).

The relations follows from

I(x,±5Fjz)F(z)=25eFj/2+Fj1+(x1/2)5Fjztanh(5Fj2z)

and power series

tanhz= n=04n(4n1)B 2n(2n)!z2n1.

In particularly, from Theorem 5.4 we have the following Euler-Bernoulli-Fibonacci-Lucas identity:

(n+1)k=1nnk(±5Fj2)kFj(nk)Ek=Ljn2n2k=0n+12n+12k5k1(4k1)2FjLj2k1B2k.

In this paper, we have documented identities relating Euler numbers (polynomials) to balancing and Lucas-balancing polynomials. We have also derived a general identity involving Euler polynomials and Lucas numbers in arithmetic progression. All results must be seen as companion results to the Fibonacci-Bernoulli pair from . In the future, we will work on more identities connecting Bernoulli/Euler numbers (polynomials) with Fibonacci/Lucas numbers (polynomials).

We would like to thank the referee for valuable suggestions.

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