Hindawi Publishing Corporation Discrete Dynamics in Nature and Society Volume 2012, Article ID 840345, 11 pages doi:10.1155/2012/840345 Review Article Incomplete Bivariate Fibonacci and Lucas p-Polynomials Dursun Tasci,1 Mirac Cetin Firengiz,2 and Naim Tuglu1 1 2 Department of Mathematics, Faculty of Science, Gazi University, Teknikokullar, 06500 Ankara, Turkey Department of Mathematics, Faculty of Education, Başkent University, Baglica, 06810 Ankara, Turkey Correspondence should be addressed to Mirac Cetin Firengiz, mcetin@baskent.edu.tr Received 26 November 2011; Accepted 8 February 2012 Academic Editor: Gerald Teschl Copyright q 2012 Dursun Tasci et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. We define the incomplete bivariate Fibonacci and Lucas p-polynomials. In the case x 1, y 1, we obtain the incomplete Fibonacci and Lucas p-numbers. If x 2, y 1, we have the incomplete Pell and Pell-Lucas p-numbers. On choosing x 1, y 2, we get the incomplete generalized Jacobsthal number and besides for p 1 the incomplete generalized Jacobsthal-Lucas numbers. In the case x 1, y 1, p 1, we have the incomplete Fibonacci and Lucas numbers. If x 1, y 1, p 1, k n − 1/p 1, we obtain the Fibonacci and Lucas numbers. Also generating function and properties of the incomplete bivariate Fibonacci and Lucas p-polynomials are given. 1. Introduction Djordjević introduced incomplete generalized Fibonacci and Lucas numbers using explicit formulas of generalized Fibonacci and Lucas numbers in 1. In 2 incomplete Fibonacci and Lucas numbers are given as follows: Fn k k n−1−j j0 n−1 0≤k≤ , 2 , j k n Ln k n −j j0 n−j j , 0≤k≤ n 2 1.1 , where n 1, 2, 3, . . .. Note that for the case k n−1/2 incomplete Fibonacci numbers are reduced to Fibonacci numbers and for the case k n/2 incomplete Lucas numbers are 2 Discrete Dynamics in Nature and Society reduced to Lucas numbers in 2. Also the authors considered the generating functions of the incomplete Fibonacci and Lucas numbers in 3. In 4 Djordjević and Srivastava defined incomplete generalized Jacobsthal and Jacobsthal-Lucas numbers. The generalized Fibonacci and Lucas p-numbers were studied in 5, 6. Incomplete Fibonacci and Lucas p-numbers are defined by Fpk n k n − jp − 1 k n Lkp n n − jp j0 n−1 0≤k≤ , p1 , j j0 n − jp , n 0≤k≤ , p1 j 1.2 for n ≥ 1 in 7. In 8 the authors introduced incomplete Pell and Pell-Lucas p-numbers. The generalized bivariate Fibonacci p-polynomials Fp,n x, y and generalized bivariate Lucas p-polynomials Lp,n x, y are defined the recursion for p ≥ 1 Fp,n x, y xFp,n−1 x, y yFp,n−p−1 x, y , n > p, 1.3 with Fp,0 x, y 0, Fp,n x, y xn−1 for n 1, 2, . . . p, 1.4 and Lp,n x, y xLp,n−1 x, y yLp,n−p−1 x, y , n > p, 1.5 with Lp,0 x, y p 1, Lp,n x, y xn for n 1, 2, . . . p 1.6 in 5. When x y 1, Fp,n 1, 1 Fp n. In 5, the authors obtained some relations for these polynomials sequences. In addition, in 5, the explicit formula of bivariate Fibonacci p-polynomials is Fp,n x, y n−1/p1 n − jp − 1 j0 j xn−jp1−1 yj , n ≥ 0, p ≥ 1, 1.7 and the explicit formula of bivariate Lucas p-polynomials is Lp,n x, y n/p1 j0 n n − jp n − jp j xn−jp1 yj , n ≥ 0, p ≥ 1. 1.8 Discrete Dynamics in Nature and Society 3 In this paper, we defined incomplete bivariate Fibonacci and Lucas p-polynomials. We generalize incomplete Fibonacci and Lucas numbers, incomplete generalized Fibonacci numbers, incomplete generalized Jacobsthal numbers, incomplete Fibonacci and Lucas p-numbers, incomplete Pell and Pell-Lucas p-numbers. 2. Incomplete Bivariate Fibonacci and Lucas p-Polynomials Definition 2.1. For p ≥ 1, n ≥ 1, incomplete bivariate Fibonacci p-polynomials are defined as k Fp,n x, y k n − jp − 1 j0 xn−jp1−1 yj , j 0≤k≤ n−1 . p1 2.1 k For x 1, y 1, Fp,n x, y Fpk n, we get incomplete Fibonacci p-numbers 7. k If x 2, y 1, Fp,n x, y Ppk n, we obtained incomplete Pell p-numbers 8. k k x, y Jn,p1 , we have incomplete generalized On choosing x 1, y 2, Fp,n Jacobsthal numbers 4. k x, y Fn k, we get incomplete Fibonacci numbers 2. If x 1, y 1, p 1, Fp,n k x, y Fn , we obtained Fibonacci For x 1, y 1, p 1, k n − 1/p 1, Fp,n numbers 9. Definition 2.2. For p ≥ 1, n ≥ 1, incomplete bivariate Lucas p-polynomials are defined as Lkp,n k n x, y n − jp j0 n − jp j xn−jp1 yj , 0≤k≤ n . p1 2.2 If x 1, y 1, Lkp,n x, y Lkp n, we obtained incomplete Lucas p-numbers 7. For x 2, y 1, Lkp,n x, y Qpk n, we have incomplete Pell-Lucas p-numbers 8. k , we get incomplete generalized On choosing x 1, y 2, p 1, Lkp,n x, y jn,p1 Jacobsthal-Lucas numbers 4. If x 1, y 1, p 1, Lkp,n x, y Ln k, we obtained incomplete Lucas numbers 2. For x 1, y 1, p 1, k n/p 1, Lkp,n x, y Ln , we have Lucas numbers 9. Proposition 2.3. The incomplete bivariate Fibonacci p-polynomials satisfy the following recurrence relation: k1 k1 k Fp,n x, y xFp,n−1 x, y yFp,n−p−1 x, y , 0≤k≤ n−p−3 . p1 2.3 4 Discrete Dynamics in Nature and Society Proof. Using 2.1, we obtain k1 k x, y yFp,n−p−1 x, y xFp,n−1 x k1 n − jp − 2 k1 n − jp − 2 k1 n − jp − 2 k1 k n − p − pj − 2 xn−p−jp1−2 yj1 y j j0 n−jp1−1 j n−jp1−1 j y k1 n − pj − 2 n − jp − 2 j n − pj − 2 xn−jp1−1 yj j −1 j1 j0 x j j0 x j j0 x j j0 k n − p − pj − 2 xn−p−jp1−2 yj y y j j0 n−jp1−2 j j −1 x n−jp1−1 j y − 2.4 n−2 −1 xn−1 k1 n − jp − 1 xn−jp1−1 yj − 0 j j0 k1 Fp,n x, y . Taking x y 1 in 2.3, we could obtain a formula for incomplete Fibonacci pnumbers see 7, Proposition 3. Taking x y p 1 in 2.3, we could obtain a formula for incomplete Fibonacci numbers see 2, Proposition 1. Proposition 2.4. The nonhomogeneous recurrence relation of incomplete bivariate Fibonacci ppolynomials is k Fp,n x, y k xFp,n−1 x, y k yFp,n−p−1 x, y − n − pk 1 − 2 xn−pk1−k−2 yk1 . k 2.5 Proof. It is easy to obtain from 2.1 and 2.3. Proposition 2.5. For 0 ≤ k ≤ n − h − p − 1/p 1, one has h h j0 j kj yh−j xj Fp,np kh x, y Fp,n j−1 p1h−p x, y . 2.6 Discrete Dynamics in Nature and Society 5 Proof. Equation 2.6 clearly holds for h 0. Suppose that the equation holds for h > 0. We show that the equation holds for h 1. We have h1 h 1 j j0 h1 h h1 h j0 y j h j h y j−1 x, y x h x, y x, y j−1 h1 h j0 j −1 kj yh1−j xj Fp,np j−1 x, y h1 kh1 xh1 Fp,nph x, y 2.7 kj1 Fp,npj x, y h h kj1 yh−j xj Fp,npj x, y x, y x j j0 −1 kh yFp,n kj h−j j1 kh yFp,n p1h−p kj yh1−j xj Fp,np x Fp,np x, y h h1−j j h j−1 j−1 j −1 kh yFp,n p1h−p j j0 kj yh1−j xj Fp,np k yh1 Fp,n−p x, y kh1 x, y xFp,n x, y p1 h x, y . h1 p1h−p kh1 Fp,n p1 Proposition 2.6. For n ≥ kp 1 p 2, h−1 y j0 xj k Fp,n−pj x, y 1 xh−1 k1 k1 Fp,nh x, y − xFp,n x, y . 2.8 Proof. Equation 2.8 can be easily proved by using 2.3 and induction on h. We have the following proposition in which the relationship between the incomplete bivariate Fibonacci and Lucas p-polynomials is preserved as found in 5 before. Proposition 2.7. One has Lkp,n x, y k Fp,n1 x, y k−1 pyFp,n−p x, y , n 0≤k≤ . p1 2.9 6 Discrete Dynamics in Nature and Society Proof. By 2.1, rewrite the right-hand side of 2.9 as k Fp,n1 x, y k−1 pyFp,n−p x, y k n − jp k n − jp k j0 x j j0 x j j0 k−1 n − p − jp − 1 y py xn−p−jp1−1 yj j j0 n−jp1 j n−jp1 j y py k n − jp − 1 j −1 j1 n − jp j k n n − jp j0 n − jp − 1 n − jp j j −1 xn−jp1 yj−1 x n−jp1 j y − n−1 xn −1 xn−jp1 yj Lkp,n x, y . 2.10 Proposition 2.8. The incomplete bivariate Lucas p-polynomials satisfy the following recurrence relation: k1 k Lk1 p,n x, y xLp,n−1 x, y yLp,n−p−1 x, y , 0≤k≤ n−p−2 . p1 2.11 Proof. We write by using 2.3 and 2.9 k1 k Lk1 p,n x, y Fp,n1 x, y pyFp,n−p x, y k1 k k k−1 xFp,n x, y yFp,n−p x, y py xFp,n−p−1 x, y yFp,n−2p−1 x, y x k1 Fp,n x, y k pyFp,n−p−1 x, y y k Fp,n−p x, y k−1 pyFp,n−2p−1 x, y 2.12 k xLk1 p,n−1 x, y yLp,n−p−1 x, y . Proposition 2.9. The nonhomogeneous recurrence relation of incomplete bivariate Lucas ppolynomials is Lkp,n x, y xLkp,n−1 x, y yLkp,n−p−1 x, y n−p−1 − n − pk 1 − 1 n − pk 1 − 1 k Proof. The proof can be done by using 2.2 and 2.11. xn−p1k1 yk1 . 2.13 Discrete Dynamics in Nature and Society 7 Proposition 2.10. For 0 ≤ k ≤ n − p − h/p 1, one has h h j j0 kj xj yh−j Lp,np x, y . 2.14 k1 Lk1 p,nh x, y − xLp,n x, y . 2.15 x, y Lkh p,n j−1 p1h−p Proof. Proof is similar to the proof of Proposition 2.5. Proposition 2.11. For n ≥ k 1p 1, one has h−1 y j0 Lkp,n−pj x, y xj 1 xh−1 Proof. Proof is obtained immediately by using 2.11 and induction h. Proposition 2.12. One has n/p1 k0 Lkp,n x, y n n 1 Lp,n x, y xFp,n x, y − Lp,n x, y . p1 p1 2.16 Proof. We can write from 2.2 n/p1 k0 n/p1 Lkp,n x, y L0p,n x, y L1p,n x, y L2p,n x, y · · · Lp,n x, y n−p n n n n n−p1 x x x y n 0 n−p 0 1 n−p n − 2p n n n n n n−p1 n−2p1 2 x x x y y ··· n 0 n−p n − 2p 1 2 n n n ⎡ ⎢n ⎢ ⎣n n n 0 xn · · · n n − n/ p 1 p ⎞ ⎤ n ⎜n − p 1 p⎟ n−p1n/p1 n/p1 ⎥ ⎥ ⎟x ×⎜ y ⎝ ⎠ ⎦ n p1 ⎛ 8 Discrete Dynamics in Nature and Society n n−p n n n n n 1 x 1 − 1 xn−p1 y p1 n 0 p1 n−p 1 n − 2p n n xn−2p1 y2 · · · 1−2 p1 n − 2p 1 ⎞ n p⎟ n − ⎜ n p 1 ⎟xn−p1n/p1 yn/p1 ⎜ ⎠ n n − n/ p 1 p ⎝ p1 n/p1 n n − jp n 1−j xn−jp1 yj p 1 n − jp j j0 ⎛ − n/p1 n − jp n n 1 xn−jp1 yj p1 n − jp j j0 n − jp n xn−jp1 yj . j n − jp j n/p1 j0 2.17 Equation 2.17 is calculated using the formula Lp,n x, y and ∂Lp,n x, y/∂x nFp,n x, y 5 n/p1 k0 Lkp,n x, y n/p1 n − jp n n xn−jp1 yj 1 p1 n − jp j j0 nFp,n x, y − nx−1 Lp,n x, y p 1 x−1 n n 1 Lp,n x, y xFp,n x, y − Lp,n x, y . p1 p1 2.18 Then we have the following conclusion. Conclusion 1. When x y p 1 in 2.16, we obtain n/2 Ln k k0 which is Proposition 11 in 2. ! n " n 1 Ln Fn − Ln 2 2 2.19 Discrete Dynamics in Nature and Society 9 3. Generating Functions of the Incomplete Bivariate Fibonacci and Lucas p-Polynomials Lemma 3.1 see 3. Let {sn }∞ n0 be a complex sequence satisfying the following nonhomogeneous recurrence relation: sn xsn−1 ysn−p−1 rn , n > p, 3.1 where {rn } is a given complex sequence. Then the generating function Skp x, y; t of the sequence {sn } is Skp p −1 i x, y; t s0 − r0 si − xsi−1 − ri t Gt 1 − xt − ytp1 , 3.2 i1 where Gt denotes the generating function of {rn }. Theorem 3.2. The generating function of the incomplete bivariate Fibonacci p-polynomials is Rkp x, y; t t kp11 p Fp,kp11 x, y ti Fp,kp11i x, y − xFp,kp1i x, y yk1 tp1 1 − xtk1 i1 3.3 −1 1 − xt − ytp1 . k Proof. From 2.1 and 2.5, Fp,n x, y 0 for 0 ≤ n < kp 1 1, k Fp,k p11 k Fp,k p12 x, y Fp,kp11 x, y , x, y Fp,kp12 x, y , 3.4 .. . k Fp,k p1p1 x, y Fp,kp1p1 x, y , and for n ≥ kp 1 p 2 k Fp,n x, y k xFp,n−1 x, y k yFp,n−p−1 x, y − n − pk 1 − 2 xn−pk1−k−2 yk1 . 3.5 n−k p1 −p−2 Now let k s0 Fp,k p11 x, y , k s1 Fp,k p12 x, y , . . . , k sp Fp,k p1p1 x, y , 3.6 10 Discrete Dynamics in Nature and Society and k sn Fp,nk x, y . p11 3.7 Also r0 r1 · · · rp 0, nk−p−1 rn n−p−1 xn−p−1 yk1 . 3.8 We obtained that Gt yk1 tp1 /1 − xtk1 is the generating function of the sequence {rn }. From Lemma 3.1, we get that the generating function Skp x, y; t of sequence {sn } is Skp k x, y; t Fp,k p k x, y ti Fp,k p11 yk1 tp1 1 − xtk1 i1 1 − xt − yt p11i p1 −1 k x, y − xFp,k p1i x, y 3.9 . Therefore, Rkp x, y; t tkp11 Skp x, y; t . 3.10 Theorem 3.3. The generating function of the incomplete bivariate Lucas p-polynomials is Wpk x, y; t t kp1 Lp,kp1 p x, y ti Lp,kp1i x, y − xLp,kp1i−1 x, y i1 tp1 yk1 p1 − xt 1 1 − xtk1 1 − xt − ytp1 −1 3.11 . Proof. From 2.9 and 3.3, ∞ Lkp,n x, y tn Wpk x, y; t n0 ∞ k k−1 Fp,n1 x, y pyFp,n−p x, y tn n0 ∞ ∞ k k−1 Fp,n1 x, y tn py Fp,n−p x, y tn n0 n0 t−1 Rkp x, y; t pytp Rk−1 x, y; t . p 3.12 Discrete Dynamics in Nature and Society 11 For the general case in Theorems 3.2 and 3.3, we find the generating functions of some special numbers by the special cases x, y, p. For example, x y 1 in 3.3 we obtain the generating function of incomplete Fibonacci p-numbers. References 1 G. B. Djordjević, “Generating functions of the incomplete generalized Fibonacci and generalized Lucas numbers,” The Fibonacci Quarterly, vol. 42, no. 2, pp. 106–113, 2004. 2 P. Filipponi, “Incomplete Fibonacci and Lucas numbers,” Rendiconti del Circolo Matematico di Palermo. Serie II, vol. 45, no. 1, pp. 37–56, 1996. 3 Á. Pintér and H. M. Srivastava, “Generating functions of the incomplete Fibonacci and Lucas numbers,” Rendiconti del Circolo Matematico di Palermo. Serie II, vol. 48, no. 3, pp. 591–596, 1999. 4 G. B. Djordjević and H. M. Srivastava, “Incomplete generalized Jacobsthal and Jacobsthal-Lucas numbers,” Mathematical and Computer Modelling, vol. 42, no. 9-10, pp. 1049–1056, 2005. 5 N. Tuglu, E. G. Kocer, and A. Stakhov, “Bivariate Fibonacci like p-polynomials,” Applied Mathematics and Computation, vol. 217, no. 24, pp. 10239–10246, 2011. 6 E. G. Kocer and N. Tuglu, “The Binet formulas for the Pell and Pell-Lucas p-numbers,” Ars Combinatoria, vol. 85, pp. 3–17, 2007. 7 D. Tasci and M. C. Firengiz, “Incomplete Fibonacci and Lucas p-numbers,” Mathematical and Computer Modelling, vol. 52, no. 9-10, pp. 1763–1770, 2010. 8 D. Tasci, M. Cetin Firengiz, and G. B. Djordjević, “Incomplete Pell and Pell-Lucas p-numbers,” Submit. 9 T. Koshy, Fibonacci and Lucas Numbers with Applications, Pure and Applied Mathematics, Wiley, New York, NY, USA, 2001. 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