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arXiv:1603.00681v2 [math.NT] 21 Mar 2016 h alyDcsnpoesta any that process Cayley-Dickson the eeta emty unu hsc,sga,clriaeprocess p 8]. sciences, [1, color analysis as signal, and such physics, quantum various , in ferential role important an play Introduction 1 ∗ Let mail: e h iproi ioac Fibonacci Bi-periodic The eateto ahmtc,Fclyo cec n Letters, and Science of Faculty , of Department hr a ena nraigitrs nqaenosadoctonion and on interest increasing an been has There rtn ucin,octonions. functions, erating s the give we paper, pro octonions. this some of Fibonacci investigated result bi-periodic main as for another well as as Also, derive octonions them. we these that, of After octonions. Fibonacci bi-periodic the eshrHc etsVl nvriy eshr Turkey Nevsehir, University, Veli Bektas Haci Nevsehir O m Classification: Ams Keywords: in we , Fibonacci bi-periodic using by paper, this In eteotno ler vrtera ubrfield real the over the be zimzslu.d.r yzi@eshreut,ntas [email protected], [email protected], eateto ahmtc,SineFaculty, Science Mathematics, of Department eateto ahmtc,SineFaculty, Science Mathematics, of Department eckUiest,Cmu,Kna Turkey Konya, Campus, University, Selcuk eckUiest,Cmu,Kna Turkey Konya, Campus, University, Selcuk iproi ioac eune ioac eune gen- , Fibonacci sequence, Fibonacci Bi-periodic amy Yilmaz Nazmiye 13,1R2 56,20G20. 15A66, 11R52, 11B39, eaiTaskara Necati a 9 2018 19, May ai Yazlik Yasin p = Abstract p p ′ 1 O ∈ + p ′′ a ewitnas written be can , e ∗ [email protected] h generating the R ete over perties ti nw,by known, is It . ummations n,geostatics ing, troduce yis dif- hysics, that s ′ ′′ 2 2 2 where p ,p ∈ H = a0 + a1i + a2j + a3k i = j = k = −1,ijk = −1, a0,a1,a2,a3 ∈ R the real algebra. The octonions in Clifford algebra C are a normed  with eight over the real numbers larger than the quater- nions. The field O =∼ C4 of octonions

7 p = pses, ps ∈ R, s=0 X is an eight-dimensional non-commutative and non-associative R-field generated by eight elements

e0 = 1, e1 = i, e2 = j, e3 = k, e4 = e, e5 = ie, e6 = je, e7 = ke .

The and of any two octonions, p = p′ + p′′e, q = q′ + q′′e, are defined by

′ ′ ′′ ′′ ′ ′ ′′ ′′ ′ ′′ p + q = p + q +(p + q )e and pq = p q − q′′p +(q p + p q′)e , where q′, q′′ denote the conjugates of the quaternions q′, q′′, respectively. The conju- gate and of p are denoted by

7 2 p = Re(p) − Im(p) and pp = ps , (1.1) s=0 X respectively [1, 8, 38, 42]. On the other hand, the literature includes many papers dealing with the special number such as Fibonacci, Lucas, Pell ([4, 9, 21, 25, 26, 30, 39, 40, 41]). One of these directions goes through to the bi-perodic Fibonacci (or, equivalently, gen- eralized Fibonacci) and the bi-periodic Lucas (or, equivalently, generalized Lucas). In fact bi-perodic Fibonacci sequences have been firstly defined by Edson and Yayenie in 2009 and then some important properties for these sequences have been investigated in the references [9, 39]. Also, bi-perodic Lucas sequences have been defined by Bilgici in 2014 and then some important properties for these sequences have been investigated in the reference [4]. For any two nonzero real numbers a and b, the bi-periodic Fibonacci ∞ ∞ {qn}n=0 and bi-periodic Lucas sequences {ln}n=0 are defined recursively by

aqn−1 + qn−2, if n is even q0 = 0, q1 = 1, qn = n ≥ 2 (1.2) bqn− + qn− , if n is odd  1 2 and bln−1 + ln−2, if n is even l0 = 2, l1 = a, ln = n ≥ 2 . (1.3) aln−1 + ln−2, if n is odd  In addition, the authors in the references [4],[9] and [39] expressed so many prop- erties on the bi-periodic Fibonacci and bi-periodic Lucas sequences. In fact some of the main outcomes (that depicted in these references) of these sequences can be summarized as in the following: • The Binet formulas are given by

− a1 ξ(n) αn − βn qn = (1.4) ⌊ n ⌋ α − β (ab) 2  

2 and ξ(n) a n n ln = n+1 (α + β ) , (1.5) (ab)⌊ 2 ⌋ n where the condition ξ (n)= n − 2 2 can be read as

 0, n is even ξ (n)= (1.6) 1, n is odd  and α, β are roots of of λ2 − abλ − ab = 0. • The generating functions for the bi-periodic Fibonacci and bi-periodic Lucas sequences with odd subscripted are

∞ 3 2m−1 x − x f(x)= q m− x , (1.7) 2 1 1 − (ab + 2)x2 + x4 m=1 X

and ∞ 3 2m+1 a + ax L (x)= l m x . (1.8) 1 2 +1 1 − (ab + 2)x2 + x4 m=0 X • The bi-perodic Fibonacci and bi-peridoic Lucas sequences satify the

(ab + 4)qn = ln−1 + ln+1 , (1.9)

ln = qn−1 + qn+1 (1.10) and n−1 q−n =(−1) qn , (1.11) n l−n =(−1) ln . (1.12) After all these above material on bi-periodicity, let us give our attention to the other classification parameters on these above special sequences, namely quaternions and octonions. We should note that, in the literature (see [2, 3, 5]-[7], [10]-[20],[22]- [24],[27]-[29], [31]-[37] and the references cited in them), it can be found some works on the quaternions and octonions for Jabosthal, Pell as well as the Fibonacci and Lucas numbers. For example, in [24], it is investigated some properties of the Fibonacci and Lucas octonions. It is natural to wonder whether there exits a connection between the parameters bi-periodicity and quaternions. Actually this was done in [35, 36]. The authors defined the bi-periodic Fibonacci and Lucas quaternions as

3 3

Qn = qn+ses and Pn = ln+ses , s=0 s=0 X X where n ≥ 0. In the light of all these above material (depicted as separate paragraphs), the main goal of this paper is to define bi-periodic Fibonacci octonions with a different viewpoint. To do that, by using bi-periodic Fibonacci numbers, we obtain the gen- erating function of these octonions. We also actually investigated some properties of bi-periodic Fibonacci octonions.

3 2 The bi-periodic Fibonacci octonions

As we indicated in the previous section, in this part, we introduce the bi-periodic Fibonacci octonions as a new generalization of Fibonacci octonions by considering the bi-periodic Fibonacci numbers.

Definition 2.1 The bi-periodic Fibonacci octonions On(a,b) are defined by

7

On(a,b)= qn+ses, (2.1) s=0 X where qn is the bi-periodic for n ∈ N = {0, 1, 2, 3,...}.

n−1 From the Equation (1.11), that is q−n = (−1) qn, the bi-periodic Fibonacci octonions with negative subscripts are defined by

7 n−s−1 O−n(a,b)= (−1) qn−ses, (2.2) s=0 X where n ∈ N = {0, 1, 2, 3,...}. After all, we present the following first proposition of this paper.

Proposition 2.1 For n ∈ N, we give the results related to bi-periodic Fibonacci octo- nions:

i) On(a,b)+ On(a,b) = 2qne0, 2 ii) On(a,b)+ On(a,b)On(a,b) = 2qne0On(a,b), 7 2 iii) On(a,b)On(a,b)= s=0 qn+s n−1 iv) O−n(a,b)+ O−n(a,bP)=2(−1) qne0

v) On(a,b)+ O−n(a,b)= lnO0(a,b), where n is even.

Proof. i) From Definition 2.1, we obtain

7 7

On(a,b)+ On(a,b) = qn+ses + qne0 − qn+ses s=0 s=1 X X = 2qne0 .

ii) By taking into account i), we have

2 On(a,b) = On(a,b)(2qne0 − On(a,b))

= 2qne0On(a,b) − On(a,b)On(a,b) .

iii) The proof is easily seen by using the Equation (1.1). iv) The proof is similar to i).

4 v) From the Equations (2.1) and (2.2), we write for n even

7 7 n−s−1 On(a,b)+ O−n(a,b) = qn+ses + (−1) qn−ses s=0 s=0 X X 7 s−1 = (qn+s +(−1) qn−s)es . s=1 X By taking into account the Equations (1.2) and (1.10), we obtain

7 On(a,b)+ O−n(a,b) = ln qses s=1 X = lnO0(a,b) .

Theorem 2.1 For n ≥ 0, the Binet formula for the bi-periodic Fibonacci octonions is ∗ ∗ 1 α αn − β βn n ( ), if n is even (ab)⌊ 2 ⌋ α − β O a,b ∗∗ n ∗∗ n n( )=  1 α α − β β  , n  n ( ) if is odd (ab)⌊ 2 ⌋ α − β  2 where α, β are roots of characteristic equation of λ − abλ − ab = 0 and ξ(t+1) ξ(t+1) ∗ 7 a t ∗ 7 a t α = t=0 t α et and β = t=0 t β et , (ab)⌊ 2 ⌋ (ab)⌊ 2 ⌋ P ξ(t) P ξ(t) ∗∗ 7 a t ∗∗ 7 a t α = t=0 t+1 α et and β = t=0 t+1 β et . (ab)⌊ 2 ⌋ (ab)⌊ 2 ⌋ P P Proof. It can easily seen by considering the Definition 2.1 and the Equation (1.4).

Theorem 2.2 For n, r ∈ Z+ and n ≥ r, the following is hold:

∗ ∗ 2r 4r ∗ ∗ 2r 4r 2 α β ((ab) − α )+ β α ((ab) − β ) O n− r (a,b)O n r (a,b) − O (a,b)= . 2 2 2 +2 2n (ab)2r(α − β)2

2 Proof. Let us take U = O2n−2r (a,b)O2n+2r (a,b) − O2n(a,b). Then, by using Teorem 2.1, we write

∗ − ∗ − ∗ ∗ 1 α α2n 2r − β β2n 2r 1 α α2n+2r − β β2n+2r U = 2n−2r ( ) 2n+2r ( ) (ab)⌊ 2 ⌋ α − β (ab)⌊ 2 ⌋ α − β ∗ 2n ∗ 2n 1 α α − β β 2 −( 2n ( )) (ab)⌊ 2 ⌋ α − β 1 ∗ ∗ − ∗ ∗ − = [α β (−ab)2n(1 − α4r (−ab) 2r)+ β α (−ab)2n(1 − β4r(−ab) 2r)] (ab)2n(α − β)2 ∗ ∗ ∗ ∗ α β ((ab)2r − α4r )+ β α ((ab)2r − β4r) = . (ab)2r(α − β)2

5 If we take r = 1 in Theorem 2.2, it is obtained in the following corollary. Corollary 2.1 For n ∈ Z+, we have the Cassini-like identity

∗ ∗ 2 4 ∗ ∗ 2 4 2 α β ((ab) − α )+ β α ((ab) − β ) O n− (a,b)O n (a,b) − O (a,b)= . 2 2 2 +2 2n (ab)2(α − β)2

Theorem 2.3 For n, r ∈ Z+, n ≥ r and r is even, we have

∗ ∗ r r ∗ ∗ r r α β ((ab) −α2 )+β α ((ab) −β2 ) 2 (ab)r(α−β)2 , if n is even O − a,b O a,b O a,b ∗∗ ∗∗ r 2r ∗∗ ∗∗ r 2r . n r( ) n+r( )− n( )= α β ((ab) −α )+β α ((ab) −β ) r− , n ( − (ab) 1(α−β)2 if is odd Proof. The proof is done similarly to the proof of Theorem 2.2.

Now, we present the generating function of the bi-periodic Fibonacci octonions in the following theorem. Theorem 2.4 For the bi-periodic Fibonacci octonions, we have the generating func- tion ∞ n O0(a,b)+ x(O1(a,b) − bO0(a,b))+(a − b)R(x) On(a,b)x = , 1 − bx − x2 n=0 X where 1 1 1 1 1 1 1 R(x)=(xe + e + e + e + e + e ++ e + e )f(x) − (xe + e +( + 0 1 x 2 x2 3 x3 4 x4 5 x5 6 x6 7 1 2 x 1 1 1 1 1 (ab+1)x)e +( +ab+1)e +( +(ab+1) +(a2b2 +3ab+1)x)e +( +(ab+1) + 3 x2 4 x3 x 5 x4 x2 1 1 1 (a2b2 +3ab+1))e +( +(ab+1) +(a2b2 +3ab+1) +(a3b3 +5a2b2 +6ab+1)x)e ) 6 x5 x3 x 7 x − x3 and f(x)= . 1 − (ab + 2)x2 + x4 Proof. Assume that G(x,a,b) is the generating function for the bi-periodic Fibonacci octonions. Then we have

2 n G(x,a,b)= O0(a,b)+ O1(a,b)x + O2(a,b)x + · · · + On(a,b)x + · · · . (2.3) If it is multiplying equation (2.3) with bx and x2, respectively, then we have

2 3 n+1 bxG(x,a,b)= bO0(a,b)x+bO1(a,b)x +bO2(a,b)x +· · ·+bOn(a,b)x +· · · . (2.4)

2 2 3 4 n+2 x G(x,a,b)= O0(a,b)x + O1(a,b)x + O2(a,b)x + · · · + On(a,b)x + · · · . (2.5) By considering the Equations (1.2), (2.3), (2.4), (2.5) and Definition 2.1, it is obtained the equation

2 (1 − bx − x )G(x) = O0(a,b)+ x(O1(a,b) − bO0(a,b)) ∞ n + (On(a,b) − bOn−1(a,b) − On−2(a,b))x n=2 X = O0(a,b)+ x(O1(a,b) − bO0(a,b)) ∞ 7 n + (qn+s − bqn+s−1 − qn+s−2)esx . n=2 s=0 X X

6 By considering again the Equations (1.2) and (1.7), we get

∞ 2 2n (1 − bx − x )G(x) = O0(a,b)+ x(O1(a,b) − bO0(a,b))+(a − b) q2n−1x e0 n=1 ∞ ∞ X 2n−1 2n−2 +(a − b) q2n−1x e1 +(a − b) q2n−1x e2 n=2 n=2 X∞ X∞ 2n−3 2n−4 +(a − b) q2n−1x e3 +(a − b) q2n−1x e4 n=3 n=3 X∞ X∞ 2n−5 2n−6 +(a − b) q2n−1x e5 +(a − b) q2n−1x e6 n=4 n=4 X∞ X 2n−7 +(a − b) q2n−1x e7 . n=5 X Consequently, we have

2 (1 − bx − x )G(x) = O0(a,b)+ x(O1(a,b) − bO0(a,b))+(a − b)xf(x)e0 −1 +(a − b)(f(x) − q1x)e1 +(a − b)x (f(x) − q1x)e2 −2 3 +(a − b)x (f(x) − q1x − q3x )e3 −3 3 +(a − b)x (f(x) − q1x − q3x )e4 −4 3 5 +(a − b)x (f(x) − q1x − q3x − q5x )e5 −5 3 5 +(a − b)x (f(x) − q1x − q3x − q5x )e6 −6 3 5 7 +(a − b)x (f(x) − q1x − q3x − q5x − q7x )e7

= O0(a,b)+ x(O1(a,b) − bO0(a,b))+(a − b)R(x) as required.

For bi-periodic Fibonacci octonions, we give the summations according to specified rules.

Theorem 2.5 For n ∈ Z+, there exist

n−1 On+1(a,b)+ On(a,b) − On−1(a,b) − On−2(a,b) i) Or(a,b)= r=0 ab α∗β − β∗α − α∗∗ab + β∗∗ab P+ , ab(α − β) ∗ ∗ n−1 O2n(a,b) − O2n−2(a,b) α β − β α ii) O r (a,b)= + , r=0 2 ab ab(α − β) P ∗∗ ∗∗ n−1 O2n+1(a,b) − O2n−1(a,b) α − β iii) O r (a,b)= − . r=0 2 +1 ab α − β P Proof. We will, now, just prove i), since the proofs of ii) and iii) can be done quite similarly with it. The main of the proof will be touched just the result Theorem 2.1(in other words the Binet formula of these octonions). We must note that the proof should be investigated for both cases of n.

7 n is odd : In this case, we get

n−1 n−3 n−1 2 2

Or(a,b) = O2r(a,b)+ O2r+1(a,b) r=0 r=0 r=0 X X X n−1 n−3 2 1 α∗α2r − β∗β2r 2 1 α∗∗α2r+1 − β∗∗β2r+1 = ( )+ ( ) (ab)r α − β (ab)r α − β r=0 r=0 X X n−1 n−1 n−3 α∗ 2 α2 β∗ 2 β2 α∗∗ 2 α2 = ( )r − ( )r + α( )r α − β ab α − β ab α − β ab r=0 r=0 r=0 Xn−3 X X β∗∗ 2 β2 − β( )r α − β ab r=0 X

2 2 α n−1 β n−1 n−1 ∗ ( ) 2 +1 − 1 ∗ ( ) 2 +1 − 1 α ab β ab Or(a,b) = − α − β α2 α − β β2 r=0 − 1 − 1 X ab ab 2 n− 2 n− α 3 +1 β 3 +1 α∗∗ ( ) 2 α − α β∗∗ ( ) 2 β − β + ab − ab . α − β α2 α − β β2 − 1 − 1 ab ab In here, simplifying the last equality, we imply the equality in i) as required. n is even : From Theorem 2.1, we know

n−2 n−2 n−1 2 2 Or(a,b) = O2r(a,b)+ O2r+1(a,b) r=0 r=0 r=0 X X X n−2 n−2 ∗ ∗ ∗∗ ∗∗ 2 1 α α2r − β β2r 2 1 α α2r+1 − β β2r+1 = ( )+ ( ) (ab)r α − β (ab)r α − β r=0 r=0 X X 2 n− 2 n− α 2 +1 β 2 +1 α∗ ( ) 2 − 1 β∗ ( ) 2 − 1 = ab − ab α − β α2 α − β β2 − 1 − 1 ab ab 2 n− 2 n− α 2 +1 β 2 +1 α∗∗ ( ) 2 α − α β∗∗ ( ) 2 β − β + ab − ab . α − β α2 α − β β2 − 1 − 1 ab ab As a result, by arranging the last equality, we have n−1 ∗ ∗ ∗∗ ∗∗ On+1(a,b)+ On(a,b) − On−1(a,b) − On−2(a,b) α β − β α − α ab + β ab Or(a,b)= + . ab ab(α − β) r=0 X

8 Corollary 2.2 In the all results of Section 2, to reveal the importance of this subject, we can express certain and immediate relationships as follows:

• If we replace a = b = 1 in qn, we obtain the same result in [24] for Fibonacci octonions.

• If we replace a = b = 2 in qn, we obtain the same result in [34] for Pell octonions.

• If we replace a = b = k in qn, we get the k-Fibonacci octonions.

Conclusion 2.1 In this paper, we define the octonions for bi-periodic Fibonacci se- quences and present some properties of these octonions. By the results in Sections 2 of this paper, we have a great opportunity to compare and obtain some new properties over these octonions. This is the main aim of this paper. Thus, we extend some recent result in the literature. In the future studies on the octonions for number sequences, we except that the following topics will bring a new insight. • It would be interesting to study the different summations and properties for bi- periodic Fibonacci octonions, • Also, it would be interesting to investigate the octonions for bi-periodic general- ized Fibonacci sequences.

Acknowledgement 2.1 This research is supported by TUBITAK and Selcuk Uni- versity Scientific Research Project Coordinatorship (BAP).

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