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On Recurrences in Generalized Arithmetic Triangle

  • Hacéne Belbachir EMAIL logo , Abdelkader Bouyakoub and Fariza Krim
Published/Copyright: March 31, 2023
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Abstract

In the present paper, we consider the generalized arithmetic triangle called GAT which is structurally identical to Pascal’s triangle for which we keep the Pascal’s rule of addition and we replace both legs by two sequences (an)n≥1 and (bn)n≥1 with a0 = b0 = Ω. Our goal is to describe the recurrence relation associated to the sum of elements lying along a finite ray in this triangle. As consequences, we obtain some combinatorial properties and we establish that the sum of elements lying along a main rising diagonal is a convolution of generalized Fibonacci sequence and another sequence which one will determine. We also precise the corresponding generating function. Further, we establish some nice identities by using the Morgan-Voyce phenomenon. Finally, we generalize the Golden ratio.

2020 Mathematics Subject Classification: Primary 11B37; 05A10; Secondary 11B65; 11B39; 05A15

1. Introduction

Pascal’s triangle appears in numerous situations and has many intriguing properties. Over the years, a number of Pascal-like triangular arrays have been developed. Koshy [20, 21] and Belbachir and Szalay [7] collected various generalizations. The generalization of Ensley [13] called Generalized Arithmetic Triangle, the Ensley’s GAT for short, changed the legs called generator sequences to an arbitrary sequences of real numbers (an)n≥0 and (bn)n≥0. Then the GAT depends on the generator sequences (an)n≥0 and (bn)n≥0. Ensley [13] studied the Fibonacci triangle, the case where an = bn = Fn, the Fibonacci numbers. The cases, where (an, bn) = (0, Fn), (an,bn)=(0,1n) and (an, bn) = (F2n−1, Fn−1), were treated by Dil and Mezo [12]. In [8], we can also find an interesting description of Fibonacci and Lucas triangles. As Fibonacci numbers can be generated from the rising diagonals of Pascal’s triangle, Feinberg, see [14], was motivated to develop a similar triangle that would generate Lucas numbers from its rising diagonal. This triangle is Lucas triangle which is the particular case of Ensley’s GAT when an = 1 and bn = 2. For other recent works on the subject, we refer to references [2,3]

In the present paper, we consider similar construction of Ensley’s GAT and our aim is to determine the recurrence relation associated to the sum of elements lying along a finite ray. Then, we establish the corresponding generating function. Also, we study the Morgan-Voyce phenomenon that leads us to establish new identities. Finally, we provide some interesting applications, among which one will establish that the sum of elements lying along a main rising diagonal is a convolution of generalized Fibonacci sequence and another sequence which one will determine.

1.1. Ensley’s Generalized Arithmetic Triangle

The following definition is given in [13].

Definition 1.

Let (an)n≥0 and (bn)n≥0 be real sequences such that a0 = b0 = Ω. The Ensley’s Generalized Arithmetic Triangle for (an)n≥0 and (bn)n≥0 contains elements C(n, k) in the nth row and kth column defined as follows: C(n, 0) = an, C(n, n) = bn and for n > k > 0,

C(n,k)=C(n1,k)+C(n1,k1).

Belbachir and Szalay, see [7], considered the Ensley’s GAT with suitable change of the rule of addition and the generator sequences. It is defined as follows.

Definition 2.

Let (an)n≥0 and (bn)n≥0 be two real sequences, A and B two real numbers. The GAT contains elements [ nk] in the nth row and kth column defined for n ≥ 2, as follows: [ n0]=Anan,[ nn]=Bnbn and for 1 ≤ kn − 1,

[nk]=A[n1k]+B[n1k1],

with the convention [ nk]=0 whenever k < 0 or k > n and [ 00] is denoted by Ω.

The convention certainly works also for the binomial coefficients: (nk)=0 whenever k < 0 or k > n.

In this paper, we keep the rule of addition in the triangle defined by Belbachir and Szalay [7] and the generator sequences of Ensley’s GAT. We call this triangle, generalized arithmetic triangle (GAT for short). It is defined as follows.

Definition 3.

Let (an)n≥0 and (bn)n≥0 be two real sequences, A and B two numbers. The GAT contains elements nk in the nth row and kth column defined for n ≥ 2, as follows: n0=an, nn=bn, and for 1 ≤ kn − 1,

nk=An1k+Bn1k1,

with the convention nk=0 whenever k < 0 or k > n and 00 is denoted by Ω.

Both definitions given in [13] and [7] are special cases of the above definition.

Figure 1 shows the rows 0 to 4 of the GAT generated by the sequences (an)n≥0 and (bn)n≥0 and the numbers A and B.

Clearly, a GAT depends only on the generator sequences (an)n≥0, (bn)n≥0 and the numbers A and B. Therefore, when necessary, we will denote by nk(A,B,an,bn)( nk for short) to emphasize the parameters of the triangle.

Figure 1. First rows of the GAT.
Figure 1.

First rows of the GAT.

1.2. GAT’S elements and binomial coefficients

The aim of this section is to evaluate nk the entry k of row n, of a GAT in terms of the sequences (an)n≥0, (bn)n≥0, the values A and B and the binomial coefficients (nk) of Pascal’s triangle. It is established in [7] with a slight modification, that:

Theorem 1.1.

Let (an)n∈ℕ and (bn)n∈ℕ be two sequences and A and B two numbers. The corresponding GAT has as entry the number nk given for (n, k) ≠ (0, 0), by the expression

nk=AnkBk(i=1nk(n1ik1)aiAi+i=1k(n1iki)biBi)+nknan+knbn.

As i=1nk(n1ik1)=(n1k) for k ≥ 1, n ≥ 1 and i=1k(n1iki)=(n1k1) for k < n, n ≥ 1, we get the following.

Corollary 1.1.1.

For an = ΩAn and a given sequence (bn)n, the corresponding GAT has as entry the number nk given for (n, k) ≠ (0, 0), by the expression

nk=AnkBk(Ω(n1k)+i=1k(n1iki)biBi)+knbn.

Corollary 1.1.2.

For bn = ΩBn and a given sequence (an)n, the corresponding GAT has as entry the number nk given for (n, k) ≠ (0, 0), by the expression

nk=AnkBk(i=1nk(n1ik1)aiAi+Ω(n1k1))+nknan.

Corollary 1.1.3.

For (an, bn) = (ΩAn, ΩBn), the corresponding GAT has as entry the number nk given for (n, k) ≠ (0, 0), by the expression

nk=ΩAnkBk(nk).

2. Quasi-symmetry and duality in a GAT

Note that in a GAT, we generally lose the symmetry. In fact, one observes that in general

nk(A,B,an,bn)nnk(A,B,an,bn).

However one has the quasi-symmetry property.

Quasi-symmetry property

Let (an)n≥0 and (bn)n≥0 be two sequences, A and B two numbers. Then

2.1 nk(A,B,an,bn)=nnk(B,A,bn,an).

Example 1.

Let A = B = 1. For an = bn = Fn, where (Fn)n is the Fibonacci sequence, we obtain the symmetrical GAT given in Table 1. Whereas, for an = Fn, bn = Jn, where (Jn)n is the Jacobsthal sequence, we obtain the asymmetrical GAT given in Table 2. The quasi-symmetry GAT are illustrated in Tables 3 and 4.

Table 1.

The (1,1,Fn, Fn) GAT.

Ω
1 1
1 2 1
2 3 3 2
3 5 6 5 3
5 8 11 11 8 5
Table 2.

The (1,1,Fn, Jn) GAT.

Ω
1 1
1 2 1
2 3 3 3
3 5 6 6 5
5 8 11 12 11 11
Table 3.

The (1, 1, Fn+1, 1) GAT.

Ω
1 1
2 2 1
3 4 3 1
5 7 7 4 1
8 12 14 11 5 1
Table 4.

The (1, 1, 1, Fn+1) GAT.

Ω
1 1
1 2 2
1 3 4 3
1 4 7 7 5
1 5 11 14 12 8

Duality

Let n ∈ ℕ, r ∈ ℕ, q ∈ ℤ, p = 0,…, r − 1 such that r + q > 0. Then the grid point (n, p) and the direction (r, q) define a transversal ray of the GAT which contains the elements

nqkp+rk,k=0,1,,npr+q.

For a fixed direction (r, q) and a fixed value of p, the sequence (Gn(r,q,p))n0 defined by

Gn+1(r,q,p):=k=0(np)/(r+q)nqkp+rk,

and G0(r,q,p)=0, constitutes the sum of elements lying on the corresponding ray in the GAT. Note that (because a sum over empty set is zero)

2.2 G1(r,q,p)=Gp(r,q,p)=0andGn+1(r,q,p)=npforpn<p+r+q.

For more details concerning directions in Pascal’s triangle, see [6] and [7]. In the following, using the quasi-symmetry property, we prove that there exists a grid point (m, p′) and a direction (r′, −q), q > 0 which define a transversal ray of GAT containing the same elements in reverse order. More precisely, we have the result.

Proposition 2.1.

Let r ∈ ℕ, q < 0, p = 0,…, r − 1 such that r + q > 0. Then

k=0(np)/(r+q)nqkp+rk(A,B,an,bn)=k=0(np)/(r+q)mqkp+rk(B,A,bn,an),

with m = nq [(np)/(r + q)], q′ = −q, r′ = r + q, p′ = np − (r + q) [(np)/(r + q)].

Proof. We have r′ + q′ > 0 and p′ < r′. It is easy to see that

(mp)(r+q)=1r(p+r(np)(r+q))=(p/r)+(np)(r+q).

Since p < r, ⌊(mp′) / (r′ + q′)⌋ = ⌊(np) / (r + q)⌋ and

k=0(np)/(r+q)mqkp+rk(B,A,bn,an)=k=0(np)/(r+q)nq((np)/(r+q)k)np(r+q)((np)/(r+q)k)(B,A,bn,an)=k=0(np)/(r+q)nqlnp(r+q)lB,A,bn,an,

with l = ⌊(np)/(r + q)⌋ − k.

We conclude by (2.1).

According to the quasi-symmetry property in the GAT, we will consider in the sequel only directions (r, q) with q ≥ 0.

3. Sum of elements lying along a finite ray in GAT

In what follows, we shall use the following notation given in [15]. Let S be a statement that can be true or false. The bracketed notation [S] stands for 1 if S is true, 0 otherwise.

Ensley [13] discussed some GAT’s properties generated by the Fibonacci sequence and A = B = 1. He showed that the sum sn of the elements in the nth row

sn=k=0nnk(1,1,Fn,Fn)

satisfy the recurrence relation

sn=sn1+sn2+2n1.

Moreover (see for instance, [7]), the ascending diagonal sum

dn=k=0n/2nkk(1,1,Fn,Fn)

satisfies the recursion formula

dn=dn1+dn2+Fn2+Fn/22[neven].

In this section, we consider the GAT as defined in Definition 3. Our aim is to determine the sum of elements located in a finite ray of the GAT generated by any sequences (an)n≥0 and (bn)n≥0.

The case an = An and bn = Bn was treated in [7]. One can easily show the following.

Lemma 3.1.

For p ≥ 0 and α = (np)/(r + q), we have

k=0αnp(r+q)knqkanqk=an[p=0],k=0αp+rknqkbnqk=bp+αr[α].

Recall that the bracketed notation [S] stands for 1 if S is true, 0 otherwise.

Theorem 1.1 and Lemma 3.1 allow us to state the following result which gives the expression of Gn+1(r,p,q) in terms of (an)n≥0, (bn)n≥0, A, B and binomial coefficients.

Proposition 3.1.

For p ≥ 0 and α = (np)/(r + q), we have

Gn+1(r,p,q)=k=0αAnp(r+q)kBp+rk(i=1np(r+q)k(nqk1ip+rk1)aiAi+i=1p+rk(nqk1ip+rk1)biBi)+annPn+bp+αr[α].

Remark 1.

Note that for p = 0, the summation can starts at k = 1 as (n1)=0.

Remark 2.

Formula (3) in [6] is a special case of Proposition 3.1. Indeed, when an = An and bn = Bn for n ≥ 0, we get

3.1 Gn+1(r,p,q)=k=0α(nqkp+rk)Anp(r+q)kBp+rk.

To avoid some complication, we agree that a−n = b−n = 0 for n ≥ 1.

4. Recurrence relation associated to rays in the GAT

We deal now with the main result, establishing a recurrence relation associated to the sum of elements located in a finite ray of the GAT generated by any sequences (an)n≥0 and (bn)n≥0.

According to Proposition 2.1, we have to consider only the case q > 0. First, we set, for m ≥ 1,

λ0(m):=(1)m(r1m),

and for s ≥ 1,

λs(m):=(1)m1(rs1m1).

Note that the λs(m)'s, 1 ≤ srm, are the binomial coefficients given by the extension of Pascal’s triangle to negative rows. By induction, we have the following.

Lemma 4.1.

For r ≥ 2 and 1 ≤ mr − 1,

λ0(m)=s=1rmλs(m).

Let now αj:=n1jpr+q, 0 ≤ jr − 1. For αj ∈ ℕ and r ≥ 1 we define

4.1 M0:=bp+rα0+Brbp+rα0r,

and for j ≥ 1,

4.2 Mj:=Aj(λ0(j)bp+rαj+λ1(j)bp+rαj1B++λrj(j)bp+rαjr+jBrj).

Let us consider the expression of Gn(r,q,p) as given in Proposition 3.1. We denote by (Gn(p))n the sequence (Gn(r,q,p))n. We are now able to give our main result.

Theorem 4.1.

The terms of the sequence (Gn(p))n satisfy the recurrence relation

j=0r(A)j(rj)Gnj(p)Bpj=0r(A)j(rpj)anpj1+j=0r1Mj[αj]=BrGnqr(p).

Remark 3.

For the sake of clarity, the proof of Theorem 4.1 will be given at the end of this section in the case p = 0. A similar proof can easily be established in the case p ≥ 1.

From Lemma 4.1 and Theorem 4.1, we can deduce the following.

Corollary 4.1.1.

For bn = Bnb, b ∈ ℝ, the terms of the sequence (Gn(p))n satisfy the recurrence relation

j=0r(A)j(rj)Gnj(p)Bpj=0rp(A)j(rpj)anpj1=BrGnqr(p).

Corollary 4.1.2.

For an = Ana, a ∈ ℝ, the terms of the sequence (Gn(p))n satisfy the recurrence relation

j=0r(A)j(rj)Gnj(p)+j=0r1Mj[αj]=BrGnqr(p).

Remark 4.

[6: Theorem 1] is a special case of Theorem 4.1 with an = An and bn = Bn, n ≥ 0.

As the last result of this section, we express the sequence (Gn(0))n as the convolution of two well determined sequences.

Let (Xn)n be a sequence defined for n ≥ 0 by

Xn:=k=0n/(r+q)An(r+q)kBrk(n+r1qkr1+rk),

and (Yn)n a sequence defined by: Y0 := 0 and

Yn:={j=0n1(A)j(rj)anj1,for1n<r+q,j=0r(A)j(rj)anj1j=0r1Mj[αj]fornr+q.

Theorem 4.2.

For n ≥ 1, we have

Gn(0)=k=0n1XkYnk.

Proof. We use the induction on the non negative integer n.

For nr + q, assume that Gm(0)=k=0m1XkYmk, mn − 1. We have from Theorem 4.1,

Gn(0)=j=1r(A)j(rj)Gnj(0)+BrGnqr(0)+Yn=j=1r(A)j(rj)k=0nj1XkYnjk+Brk=0nrq1XkYnrqk+Yn.

Letting s = k + j and t = k + r + q, we get

Gn(0)=j=1r(A)j(rj)s=jn1XsjYns+Brt=r+qn1XtrqYnt+Yn.

Since Xn = 0 for n < 0, we can write

Gn(0)=j=1r(A)j(rj)s=1n1XsjYns+Brt=1n1XtrqYnt+Yn=s=1n1Yns(j=1r(A)j(rj)Xsj)+Brt=1n1XtrqYnt+Yn=s=1n1Yns(j=1r(A)j(rj)Xsj+BrXsrq)+Yn.

We know that (Xn)n satisfies the recurrence relation, (see [6])

j=0r(A)j(rj)Xnj=BrXnqr.

Therefore, Gn(0)=s=1n1YnsXs+Yn=s=0n1YnsXs as X0 = 1.

We now assume that 1 ≤ nr + q − 1. So, we have Xn=(n+r1r1)An and from (2.2), Gn(0)= n10 =an1.

Then, we have to prove that k=0n1XkYnk=an1.

We have

k=0n1XkYnk=X0Yn+k=1n1XkYnk.

Since X0 = 1 and Yn=j=0n1(A)j(rj)anj1, we obtain that

k=0n1XkYnk=an1+j=1n1(A)j(rj)anj1+k=1n1XkYnk.

Therefore, we aim to prove that for 1 ≤ nr + q − 1,

4.3 k=1n1XkYnk=j=1n1(A)j(rj)anj1,

by considering two cases.

1. If 1 ≤ nr + 1.

k=1n1XkYnk=k=1n1Ak(k1+rr1)j=0nk1(A)j(rj)ankj1,k=1n1XkYnk=k=1n1i=0nk1(1)n1kiAnk(r+ir1)(rn1ki)ak1.

For each 1 ≤ kn − 1, we set j = n − 1 − ki . Then, we get

k=1n1XkYnk=k=1n1Ankj=0nk1(1)j(rj)(r+n1kjr1)ak1.

By putting in (9.3), t = n − 1 − k for k ≥ 1, tr − 1 since nr + 1, one has

k=1n1XkYnk=k=1n1(1)n1kAnk(rnk)ak1.

If we put j = nk, we get (4.3).

2. If r + 2 ≤ nr + q − 1. In this case, Yn=j=0r(1)jAj(rj)an1j since n − 1 > r. So,

k=1n1XkYnk=k=1n1Ak(k1+rr1)j=0r(A)j(rj)ankj1.

Now, we separate the sum following the index k in three parts; 1 ≤ kr, k = r + 1 and r + 2 ≤ kn − 1 to obtain

k=1n1XkYnk=k=1rj=0k1(1)kj1Ak(rk1j)(r+jr1)ank1+j=0r(1)rjAr+1(rrj)(r+jr1)anr2+k=r+2n1j=0n2(1)kj2Ak(rrj)(k1+jr1)ank1.

We set s = k − 1 − j, t = rj and we get

k=1n1XkYnk=k=1rAks=0k1(1)s(rs)(r+k1sr1)ank1+Ar+1t=0r(1)t(rt)(2rtr1)anr2+k=r+2n1(1)k2rAkt=0r(1)t(rt)(k1+rtr1)ank1.

By putting in (9.3), t = k − 1 ≤ r − 1 in the first sum of the right hand side, one has

k=1rAks=0k1(1)s(rs)(r+k1sr1)ank1=k=1r(1)k1Ak(rk)ank1.

From Lemma 9.3,

t=0r(1)t(rt)(2rtr1)=0andt=0r(1)t(rt)(k1+rtr1)=0.

Therefore, we get (4.3). The proof is complete.

5. The generating function

In this section, we give the generating function associated to the sum of GAT’s elements lying along a finite ray. But first, we will need the following lemmas and theorem.

Lemma 5.1.

For ar ≥ 1,

j=0r(A)j(rj)nja=Brnrar.

Proof. Let Ir=j=0r(A)j(rj) nja . We use induction on the positive integer r. From Definition 3,

I1naAn1a=Bn1a1.

Assume now that Ir=Br nrar We have

Ir+1=j=0r(A)j(rj)nja+j=0r(A)j(rj1)nja=j=0r(A)j(rj)njaAj=0r(A)j(rj)nj1a=BrnrarABrnr1ar.

We conclude by Definition 3.

Lemma 5.2.

Let Zn:=k=0p(n+pkpk)bk. The following identity holds true

n0Zntn=(1t)p1k=0p(1t)kbk.

Proof.

n0(k=0p(n+pkpk)bk)tn=k=0pn0(n+pkpk)tnbk=k=0p(1t)kp1bk

as

m0(m+ss)tm=(1t)s1.

For fixed r and p, we now set

5.1 Ck(t):=np+rknp+rktnandH(t):=n0antn.

Lemma 5.3.

For r ∈ ℕ, 0 ≤ pr, q ∈ ℤ and the sequences (an)n and (bn)n, the generating function Ck(t) verifies the relation, for k ≥ 0,

5.2 Ck(t)=(Bt1At)rkC0(t),

with

5.3 C0(t)=bptp+(Bt1At)p(H(t)Ω+At1Atk=1p(1AtB)kbk).

Proof. For k ≥ 0,

(1At)rCk+1(t)=j=0r(A)j(rj)np+rk+rnp+rk+rtn+j=j=0r(A)j(rj)np+rk+r+jnjp+rk+rtn.

So,

(1At)rCk+1(t)=j=0r(A)j(rj)(np+rk+rnjp+rk+rtn),

as njp+rk+r =0 for p + rk + rn < p + rk + r + j.

From Lemma 5.1, we get

(1At)rCk+1(t)=np+rk+rBrnrp+rktn=Brtrnp+rknp+rktn.

Thus from (5.1), (1 − At)r Ck+1 (t) = BrtrCk(t). It follows that Ck(t)=(Bt1At)rkC0(t).

For p = 0, C0(t)=n0 n0tn=n0antn=H(t).

For p ≥ 1 and using Theorem 1.1,

C0(t)=pptp+np+1AnpBp(i=1np(n1ip1)aiAi+i=1p(n1ipi)biBi)tn,

as npn = pn =0.

Let us set C0 (t) = bptp + T1 + T2 with

T1:=np+1AnpBpi=1np(n1ip1)aiAitn

and

T2:=np+1AnpBpi=1p(n1ipi)biBitn.

We have

T1=tpBpm1[i=1m(mi+p1p1)Amiai]tm,withm=np,=tpBp(m1amtm)(m0(m+p1p1)(At)m)=tpBp(H(t)Ω)(1At)P.T2=tpBpm0[i=1p(m+p1pi)biBi](At)m+1,withm=np1,=Atp+1Bp(1At)p1i=1p(1AtB)ibi.

By replacing, the proof is complete.

Remark 5.

We can easily deduce the following special cases:

  • For bn = ΩBn, C0(t)=(Bt1At)pH(t).

  • For an = ΩAn, C0(t)=bptp+Atp+1k=0p(1At)kp1Bpkbk.

  • For an = ΩAn and bn = ΩBn, C0 (t) = Ω(Bt)p (1 − At)p−1.

Now, we are able to give the generating function of (Gn(p))n.

Theorem 5.1.

For r ∈ ℕ, 0 ≤ p < r, q ∈ ℤ and B ≠ 0, the generating function G(t):=n0Gn+1(p)tn associated to (Gn(p))n is given by

G(t)=(1At)r(1At)rBrtr+qC0(t),

with C0 (t) as given by (5.3).

Proof. We have

G(t)=n0Gn+1(p)tn=k0n0nqkp+rktn,

as nk=0 for n < k. According to (5.1) and (5.2),

G(t)=k0tqkCk(t)=C0(t)k0(Brtr+q(1At)r)k=(1At)r(1At)rBrtr+qC0(t).

Corollary 5.1.1.

For r ∈ ℕ, 0 ≤ p < r, q ∈ ℤ and B ≠ 0, the generating function associated to (Gn(p))n is given for bn = ΩBn by

5.4 G(t)=(Bt)pH(t)(1At)rP(1At)rBrtr+q,

and for an = ΩAn by

G(t)=(1At)rbptp+Atp+1k=0p(1At)r+kp1Bpkbk(1At)rBrtr+q,

and for an = ΩAn and bn = ΩBn by

G(t)=Ω(Bt)p(1At)rp1(1At)rBrtr+q.

Remark 6.

For an = An and bn = Bn, we get Theorem 2 given in [6] which holds not only for q > 0, but for q ≤ 0 as well.

6. Morgan-Voyce and Fibonacci numbers

In [6], the authors established that the sequence (υn) associated to different directions of the ray in Pascal’s triangle, defined for r ∈ ℕ, q ∈ ℤ, pr − 1 such that r + q > 0, by

υn+1=k=0(np)/(r+q)(nqkp+rk)xnp(r+q)yp+rk,

satisfies the linear recurrence relation

υnx(r1)υn1++(x)r(rr)υnr=yrυnrq.

Thus, the sequence (υn) is of order r for q ≤ 0 and we can write

υnx(r1)υn1++((x)r+q(rr+q)yr)υnrq++(x)r(rr)υnr=0.

This is what we call the Morgan-Yoyce phenomenon. For more details, see [[22,[24,[25]. Using this phenomenon, we can infer remarkable identities for Fibonacci numbers.

Let δ0 = Ω, δ1 be two parameters and (δn)n be a sequence defined by

6.1 δn=2Aδn1A2δn2,n2.

In this section, we consider the GAT generated by the sequences (an)n and (bn)n such that

6.2 a1=Aδ1,anδn,n2,bn=Bn,n1.

By setting in Corollary 4.1.1, r = 2, p = 0 and q = −1, we get for n ≥ 3,

Gn(2A+B2)Gn1+A2Gn2=an12Aan2+A2an3.

Assume that A = i, B2 = 1 − 2i, with i2 = −1. It follows from (6.1) and (6.2) that

Gn=Gn1+Gn2.

However, Gn+1=k=0n n+k2k , so G1= 00=Ω, G2 = 1 + i(δ1 − 2). If we write Gn = αFn + βFn+1, then from G1 and G2 it follows that

Gn=(2Ω1)Fn+(1Ω)Fn+1+i(δ12)Fn1.

Thus

6.3 (2Ω1)Fn+(1Ω)Fn+1=Re(Gn)and(δ12)Fn1=Im(Gn).

For δ1 = 2,

Gn=(2Ω1)Fn+(1Ω)Fn+1,

and for δ1 = 2, Ω = 0,

Gn=Fn1.

For Ω = δ1 = 1, using some combinatorial computations, Proposition 3.1 and (6.3) give for m ≥ 0,

F2m+1=k=02ms=0k/2(1)m+k+s2k2s(k2s)(2m+k2k),F2m+2=k=02m+1s=0(k1)/2(1)1+m+k+s2k2s1(k2s+1)(2m+1+k2k).

As a last result in this section, we quote an application of Theorem 5.1. Recall that the Morgan-Voyce polynomials Bn (x) are defined by

B0(x)=1,B1(x)=2+t,Bn(x)=(2+x)Bn1(x)Bn2(x),n2.

They have been widely studied (see [[4,[22,[24,[25]). In [24], the author gives a closed form expression and a generating function

Bn(x)=k=0n(n+K+11+2k)xk,n0Bn(x)tn=11(x+2)tt2.

Using (5.4), we are able to express Bn (x) in descending powers of x. Indeed, if we put A = x + 2, B = −1, r = q = 1, an = An for n ≥ 0, we deduce

n0Gn+1(0)tn=n0Bn(x)tn.

So, from (3.1) we get for n ≥ 0,

Bn(x)=k=0n(nkk)(1)k(x+2)n2k.

We get also, n0Gn+1(0)tn=n0Bn(x)tn by setting A = 1, B=x(x0), r = 2, q = −1, an = n + 1. Therefore, for x ≥ 0 and n ≥ 0,

Bn(x)=k=0nn+k2k(1,x,n+1,xn).

7. Some illustrations

We present some examples to illustrate Theorem 4.1 for p = 0. The sequence (Gn(0))n is denoted for short by (Gn)n.

Example 2.

Consider (bn)n = (Bn)n and an=An(n+kk)Bk for a fixed k, kr. From Corollary 4.1.1, the terms of the sequence (Gn)n satisfy the recurrence relation

7.1 j=0r(A)j(rj)Gnjj=0r(A)j(rj)anj1=BrGnqr.

From Lemma 9.3,

j=0r(A)j(rj)anj1=An1j=0r(1)j(rj)(n+k1jk)Bk=An1(n+k1rkr)Bk.

Then (7.1) becomes

7.2 j=0r(A)j(rj)GnjBrGnqr=An1(n+k1rkr)Bk.

For (r, q) = (1,1), we obtain

GnAGn1BGn2=An1(n+k2k1)Bk,

which is the nonhomogeneous recurrence relation of (Fn(k)), the bivariate hyper-Fibonacci polynomials given in [5]. More precisely,

Gn=Fn(k),whereFn+1(k)=j=0n/2An2jBj+k(n+kjj+k).

For (r, q) = (1, q), q > 0, we obtain

GnAGn1BGnq1=An1(n+k2k1)Bk,

which is the recurrence relation of (Un(k)), the hyper q-Fibonacci polynomials given in [1]:

Gn=Un+2(k),whereUn+1(k)=j=0n/(q+2)An(q+1)jBj+k(n+kqjj+k).

Example 3.

The direction (r, q) = (1,1). It concerns the sequence Wn+1=Gn+1(1,1,0) given by

Wn+1=k=0n/(r+q)nkk(A,B,an,bn).

From Theorem 5.1, (Wn) satisfies, for n ≥ 2,

7.3 WnAWn1BWn2=(an1Aan2)+(bn12Bbn32)[nodd].

We give the following examples.

an bn Wn
AnF2n−1 BnFn−1 Wn=AWn1+BWn2+An1F2n4+Bn12Fn72[ nodd ]
AnFn BnFn Wn=AWn1+BWn2+An1Fn3+Bn12Fn52[ nodd ]

Remark 7.

The recurrence relation associated to (Wn) in the last example of the above table, is given in [7] for A = B = 1.

From (7.3) and Theorem 4.2, we are able to write (Wn) as the convolution of two sequences. One has for n ≥ 2,

7.4 Wn=k=0n1XkYnk,

with X0 = 1, X1 = A, Xn = AXn−1 + BXn−2, n ≥ 2 and Y0 = 0, Y1 = Ω, Yn=(an1Aan2)+(bn12Bbn32)[ nodd ], n ≥ 2.

For A = B = 1 and (an)n, (bn)n two given sequences, (Wn) is the convolution of the Fibonacci sequence and the sequence (Yn)n.

In the following, some examples are given, where (Fn) is the Fibonacci sequence, (ln) is the Lucas sequence and (Hn(k)) the hyper harmonic sequence defined by Hn(0)=1n for k ≥ 1. For more details, see [9,11].

an bn Wn Wn =
Fn + 1 1 Wn = Wn−1 + Wn−2 + Fn−2. k=0n1Fk+1Fnk2
ln+1 1 Wn = Wn−1 + Wn−2 + ln−2. k=0n1Fk+1lnk2
1n 1 Wn=Wn1+Wn2+1n(n+1). k=0n1Fk+1(nk)(nk+1)
Hn(k) 1 Wn=Wn1+Wn2+Hn1(k1). k=0n1Fk+1Hnk1(k1)
1 Fn+1 Wn=Wn1+Wn2+Fn32[ nodd ] k=1 (n1)/2 Fk1Fn2k
1 ln+1 Wn=Wn1+Wn2+ln32[ nodd ] ln+k=1 (n1)/2 lk1ln2k
1 1n+1 Wn=Wn1+Wn2+4n21[ nodd ] Fnk=1 (n1)/2 4Fn2k(2k+1)21

Example 4.

As a consequence of (7.4), we infer an expression for the sum of hyper harmonic numbers in terms of Fibonacci numbers. Indeed, in the last case of the above table, it is easy to see that nk(1,1,11n+1)=Hk+1(nk). So one has the following.

Proposition 7.1.

For any n ≥ 2, we have

k=1n/2Hk+1(n2k)=Fnk=2(n1)/24Fn2k(2k+1)21.

Example 5.

The case A = 0, bn = Bn, p = 0. From Corollary 4.1.1, this case deals with the sequence (Vn(r,q))n satisfying for nr + q the recurrence

7.5 Vn(r,q)BrVnrq(r,q)=an1.

The arrays in Tables 1 and 2 were studied by Bruckman [10] and Hoggatt [16], respectively. The column 0 consists of the Fibonacci numbers F2n−2 and F2n+1, respectively. Each of the remaining columns j, j ≥ 1, is obtained by lowering the previous column j − 1 by one level. Note that these tables are the particular case of the GAT when A = 0, B = 1 and, respectively, (an)n≥1 = (F2n)n≥0, (an)n≥0 = (F2n+1)n≥0.

In the Table 5, the n-th row sum is Vn+1(1,0)=F2n+1 and the rising diagonal sum is Vn+1(1,1)=Fn+12. Indeed, from relation (7.5), the sequence (Vn(1,0))n satisfies the recurrence

Vn(1,0)Vn1(1,0)=F2n2,

and the sequence (Vn(1,1))n satisfies the recurrence

Vn(1,1)Vn2(1,1)=F2n2.

Also, in the Table 6, Vn+1(1,0)=F2n+2 and Vn+1(1,1)=Fn+1Fn.

Some examples, with tn the triangular number and Tn the tetrahedral number, corresponding to this case are given as follows:

Table 5.

The (0,1,F2n, 1) GAT.

1
1 1
3 1 1
8 3 1 1
21 8 3 1 1
55 21 8 3 1 1
Table 6.

The (0,1,F2n+1, 1) GAT.

1
2 1
5 2 1
13 5 2 1
34 13 5 2 1
89 34 13 5 2 1
an B r q Vn(r,q)
n + 1 1 1 0 tn
tn + 1 1 1 0 tn
F2n+3 −1 1 0 Fn+12
ln+1 −1 1 1 Fn + 1
F2n + 2 1 1 1 Fn+12
ln −1 1 1 Fn
5Fn + 1 1 1 3 Fn + 2
ln−1 1 1 3 Fn

8. The generalized golden ratio

Given two initial terms u0 and u1 not both zero, we consider the recurrence relation un = un− 1 + un−2. It is a well-known property of such sequences that limnun+1un=ϕ, where ϕ, called the golden ratio, is the greatest root of t2t − 1 = 0. Raab [23] extended this result to the sequences defined by the recurrence

wn=xwn1+ywnm1,

given m + 1 initial terms. He proves that limnwn+1wn exists and is a root of tm+1xtmy = 0.

In this section, we establish the existence of similar limits for more general sequences. For that, let us consider the sequence (Tn)n defined for nr + q by

8.1 TnA(r1)Tn1++(A)r(r1)Tnr=BrTnqr.

Note that, from Corollary 4.1.2 and Corollary 4.1.1, Tn is the sum of elements lying on the corresponding ray in the GAT generated by the sequences (an)n = (An)n and (bn)n = (Bn)n. The characteristic polynomial of (Tn)n is

8.2 tq(tA)rBr=0,

and, from (2.2) and Theorem 1.1, initial conditions are

Tn+1=(np)AnpBp,pn<p+r+q.

Let us set

Tn:=i=1r+qcitin,

where ti, i = 1,…, r + q, are the roots of (8.2) and g(t) = tq (tA)rBr.

We have g(t) = tq−1 (tA)r−1 [(r + q)tAq]. or B ≠ 0, no root of g′(t) is a root of g(t). It follows that g(t) has no multiple root. Moreover, the determinant of the coefficients ci of the linear system in ci,i = 1,…, r + q,

8.3 i=1r+qcitin+1=(np)AnPBp,pnp+r+q1,

is not zero. Indeed, by writing (8.3) as

8.4 {i=1r+qcitip+1=(pp)A0Bpi=1r+qcitip+2=(p+1p)A1Bpi=1r+qcitip+r+q=(p+r+11p)Ar+q1Bp,

the determinant which is

D=|(t1p+1t1p+2t1p+r+qt2p+1t2p+2t2p+r+qtr+qp+1tr+qp+2tr+qp+r+q)|=k=1r+qtkp+11i<jr+qr+q(tj=ti).

Since all the roots are simple, then D ≠ 0 and the system (8.4) can be solved uniquely in c1,…, cr+1. Let now t* be such that for each i, |t*| > |ti|. We have the following.

Proposition 8.1.

If A > 0 and B > 0, then

limnTn+1Tn=t.

Proof. Let g(t) = tq (tA)rBr. We have, g (A) = −Br < 0 and limtg(t)=+. It follows that g admits a real root t* such that t* > A > 0. Furthermore, we have for 1 ≤ ir + q, |t*| > |t*| with ti a root of g.

Indeed, suppose that ti is a root of g such that |ti| > t*. Thus,

|tiA|||ti|A||ti|A>tA>0.

So,

|tiA|r>|tA|r

and it follows that

|tiq(tiA)r|>|t|q|(tA)|r=Br.

This is a contradiction.

Consider now the ratio

Tn+1Tn=i=1r+qcitin+1i=1r+qcitin=tn(c1t1(t1t)n++ct++cr+qtr+q(tr+qt)n)tn(c1(t1t)n+c++cr+q(tr+qt)n).

Since t* > 0 and t* > |ti|, we get limnTn+1Tn=t*. (We suppose without loss of generality that c* ≠ 0).

Example 6.

For (r, q) = (1,1), we have Tn = ATn−1 + BTn−2, T0 = 0, T1 = 1 (see relation (8.1)).

The characteristic polynomial of (Tn) is t2AtB = 0, whose roots are t1=(A+A2+4B)/2 and t2=(AA2+4B)/2. Then:

  • For (A, B) = (1,1), we obtain Tn = Fn, the Fibonacci number and

    limnFn+1Fn=(1+5)/2.
  • For (A, B) = (2, 1), we obtain Tn = Pn, the Pell number and

    limnPn+1Pn=1+2.
  • For (A, B) = (1, 2), we obtain Tn = Jn, the Jacobsthal number and

    limnJn+1Jn=2.
  • For (A, B) = (3, 2), we obtain Tn = ϕn, the Fermat number and

    limnϕn+1ϕn=(3+17)/2.

Remark 8.

For (r, q) = (1, q), the result is given in [23].

9. Lemmata

In this section, we establish some intermediate lemmata which will play a key role in the proof of the recurrence relation associated with the sum of elements along a transversal ray in a GAT.

Lemma 9.1.

Let (dn)n∈ℕ be a sequence. Then for r ≥ 1, 1 ≤ tr, cr − 1, all natural numbers,

j=0r(1)j(rj)i=1c+2jt(cji+1t1)di=j=0rt(1)j(rtj)dc+2tj.

Proof. Let Sr=j=0r(1)j(rj)i=1c+2jr(cij+1r1)di. Using induction on the nonnegative integer r, we will prove first that

9.1 Sr=dcr+2.S1=j=01(1)j(1j)i=1cj+t(cij+10)di=i=1c+1dii=1cdi=dc+1.

Assume now that Sr = dcr+2 and prove that Sr+1 = dcr+1.

Sr+1=j=0r+1(1)j(r+1j)i=1cjr+1(cij+1r)di=j=0r+1(1)j(rj)i=1cjr+1(cij+1r)di+j=1r+1(1)j(rj1)i=1cjr+1(cij+1r)di=j=0r(1)j(rj)i=1cjr+1(cij+1r)di+j=0r(1)j(rj)i=1cjr(cijr)di=j=0r(1)j(rj)i=1cjr+1(cijr1)di+dcr+1.

Let now

Tr=j=0r(1)j(rj)i=1cjrt+1(cij+1t1)di.Tr=j=0r(1)jm=0t(rtjm)(tm)i=1cjrt+1(cij+1t1)di,Tr=m=0tj=0r(1)j(rtjm)(tm)i=1cjrt+1(cij+1t1)di.

Let k = jm. Since (nk)=0 if k < 0, we get,

Tr=m=0tk=0rm(1)k+m(rtk)(tm)i=1c+2kmt(cikm+1t1)di.

Note first, that the coefficient (rtk) in the summation with index k is zero for all k > rt and rmrt since mt. So, we can write the summation up to rt instead of rm without changing the total sum. Therefore

Tr=m=0tk=0rt(1)k+m(rtk)(tm)i=1c+2kmt(cikm+1t1)di,Tr=m=0rt(1)k(rtk)m=0t(1)m(tm)i=1c+2kmt(ckmi+1t1)di.

But according to (9.1),

m=0t(1)m(tm)i=1c+2kmt(ckmi+1t1)di=dckt+2,

then the proof is complete.

Lemma 9.2.

Let (dn)n∈ℕ be a sequence. Then for tr ≥ 1, c ≥ 0, all non negative integers

j=0r(1)j(rj)i=1cjt+1(cji+1t)di=i=1ct+1(cir+1tr)di.

Proof. We use induction on the non negative integer r. For r =1,

j=01(1)j(1j)i=1cjt+1(cji+1t)di=i=1ct+1(ci+1t)dii=1ct(cit)di=(tt)dct+1+i=1ct((ci+1t)(cit))di=(tt)dct+1+i=0ct(cit1)di=i=1ct+1(cit1)di.

Let now, Xr=j=0r(1)j(rj)i=1cjt+1(cij+1t)di and assume that

Xr=i=1ct+1(cir+1tr)di.

Xr+1=j=0r(1)j(rj)i=1cjt+1(cij+1t)di+j=0r+1(1)j(rj1)i=1cjt+1(cij+1t)di=i=1ct+1(cir+1tr)dij=0r(1)j(rj)i=1cjt(cijt)di=i=1ct+1(cir+1tr)dii=1ct(cirtr)di=(trtr)dct+1i=1ct((cir+1tr)(cirtr))di=(trtr)dct+1i=1ct((cirtr1))di=i=1ct+1((cirtr1))di.

Lemma 9.3.

Let a, b and r be non-negative integers. Then

j=0r(1)j(rj)(ajb)={ (arbr)forrba,0forr>b.

Proof. In case where rba, the proof can be found in [6].

Let now r > b and

Xr=j=0r(1)j(rj)(ajr1).

By using induction on r, it is easily seen that Xr = 0 for a ≥ 2r − 1. Moreover, one has (rj)=m=0b+1(rb1jm)(b+1m), so

j=0r(1)j(rj)(ajb)=j=0r(1)jm=0b+1(rb1jm)(b+1m)(ajb)=k=0rb1(1)k(rb1k)m=0b+1(1)m(b+1m)(akmb).

According to the above, m=0b+1(1)m(b+1m)(akmb)=0, then the proof is complete.

Lemma 9.4.

Let r ≥ 1. Then for 0 ≤ mr, 0 ≤ sr − 1,

j=0m(1)j(rj)(s+mjs)=(1)m(rs1m).

Proof. We again use induction on r. It is easy to verify the formula for r = 1. So assume it true for r.

j=0m(1)j(r+1j)(s+mjs)=j=0m(1)j(rj)(s+mjs)+j=1m(1)j(rj1)(s+mjs)=j=0m(1)j(rj)(s+mjs)j=0m1(1)j(rs)(s+mj1s)=(1)m(rs1m)(1)m1(rs1m1)=(1)m(rsm).

Especially for s = 0, one has for r ≥ 1 and 0 ≤ mr,

9.2 j=0m(1)j(rj)=(1)m(r1m),

and for s = r − 1, one has for r ≥ 1 and 0 ≤ tr − 1,

9.3 j=0t(1)j(rj)(r+tjr1)=(1)t(rt+1).

The proof of the principal theorem of this paper is essentially based on the following result.

Lemma 9.5.

Let r ∈ ℕ, q ∈ ℤ+ and nr + q + 1 and for j = 0,…, r, αj = (n − 1 − j) / (r + q).

Then only two possibilities hold.

  • αj ∈ ℕ for j = 0,…, r. In this case, ⌊αj⌋ = ⌊α0⌋, for j = 0, …, r.

  • There is a unique j0 ∈ {0,…, r} such that αj0 ∈ ℕ. In such case,

    αj ={ αj0forjj0,αj01forj0+1.

Proof. Let nr + q + 1. Then, there exist k ∈ ℕ and β < r + q such that n − 1 = k(r + q) + β. Let us define, for j ∈ ℕ, f(j) = (βj)/(r + q). Then for j0 = β, f (j0) = 0 and so αj0 = k. But β < r + q and q > 0, so the two following cases arise.

  1. βr. In this case, there exist a unique j0r such that αj0 ∈ ℕ.

  2. r < β < r + q. In this case, 0 < f (j) < 1 since 0 ≤ jr. It follows that 0 < αjk < 1 and so αj ∈ ℕ for 0 ≤ jr.

Lemma 9.6.

Let r ∈ ℕ, q ∈ ℤ+, (dn)n a sequence and let

T1:=j=0r(1)j(rj)k=1 βj As+2(r+q)kBrki=1s+2j(r+q)k(sjqki+1rk1)di,T2:=k=1 β01 As+2(r+q)(k+1)Br(k+1)i=1s+2(r+q)(k+1)(sq(k+1)ir+1rk1)di,

with βj=s+2jr+q. Then T1 = T2.

Proof. Let sr + q − 2. We will prove that T1T2 = 0 by using Lemma 9.5. There are two cases.

Case 1. βj ∈ ℕ. So, ⌊βj⌋ = ⌊β0⌋ for 0 ≤ jr and

T1T2=k=2 β0 As+2(r+q)kBrkj=0r(1)j(rj)i=1s+2j(r+q)k(sjqki+1rk1)dik=1 β0 1As+2(r+q)(k+1)Br(k+1)i=1s+2(r+q)(k+1)(sq(k+1)ir+1rk1)di.

By putting c = sqk and t = rk − 1 in Lemma 9.2, we infer

T1T2=k=2 β0 As+2(r+q)kBrki=1s+2j(r+q)k(sqkir+1r(k1)1)dik=1 β0 1As+2(r+q)(k+1)Br(k+1)i=1s+2(r+q)(k+1)(sq(k+1)ir+1rk1)di.

So,

9.4 T1T2=0.

Case 2. There is a unique j0, 0 ≤ j0r such that βj0 ∈ ℕ and βj ∈ ℕ for jj0 with βj ={ βj0forjj0,βj01forjj0+1. .

Let us write T1 as three sums by separating the sum indexed by j following 0 ≤ jj0 − 1, j = j0 and j0 + 1 ≤ jr.

T1=k=2βj0As+2(r+q)kBrkj=0j01(1)j(rj)i=1s+2j(r+q)k(sjqki+1rk1)di+(1)j0(rj0)k=2βj0As+2(r+q)kBrki=1s+2j0(r+q)k(sjqki+1rk1)di+k=2βj01As+2(r+q)kBrkj=j0+1r(1)j(rj)i=1s+2j(r+q)k(sjqki+1rk1)di.

Separating now, by including βj0 value, the sums indexed by k in two parts following 2 ≤ kβj0 − 1 and k = βj0. We get by noting that (sj0qβj0i+1rβj01)=0 as s − j0j0i + 1 < j0 − 1,

T1=k=2βj01As+2(r+q)kBrkj=0j0(1)j(rj)i=1s+2j(r+q)k(sjqki+1rk1)di+Aj0Brβj0j=0j01(1)j(rj)i=1s+2j(r+q)k(sjqβj0i+1rβj01)di+(1)j0(rj0)k=2βj0As+2(r+q)kBrki=1s+2j(r+q)k(sj0qki+1rk1)di+k=2βj01As+2(r+q)kBrkj=j0+1r(1)j(rj)i=1s+2j(r+q)k(sjqki+1rk1)di.

Then,

T1=Aj0Brβj0j=0j0(1)j(rj)i=1s+2j(r+q)βj0(sjqβj0i+1rβj01)di+k=2βj01As+2(r+q)kBrkj=0r(1)j(rj)i=1s+2j(r+q)k(sjqki+1rk1)di.

If we put in Lemma 9.2, c = sqk and t = rk − 1, we get

T1=Aj0Brβj0j01j=0(1)j(rj)s+2j(r+q)βj0i=1(sjqβj0i+1rβj01)di+βj01k=2As+2(r+q)kBrks+2j(r+q)ki=1(sqkir+1r(k1)1)di=Aj0Brβj0j01j=0(1)j(rj)s+2j(r+q)βj0i=1(sjqβj0i+1rβj01)di+βj01k=2As+2(r+q)(k+1)Br(k+1)s+2j(r+q)(k+1)i=1(sq(k+1)ir+1rk1)di.

Similarly writing T2 following 1 ≤ kβj0 − 2 and k = βj0 − 1. Noting that ⌊β0 − 1⌋ = βj0 − 1, we obtain

T2=k=1βj02As+2(r+q)(k+1)Br(k+1)i=1s+2(r+q)(k+1)(sq(k+1)ir+1rk1)di+Aj0Brαj0i=1s+2(r+q)βj0(sqβj0ir+1r(βj01)1)di.

Therefore

9.5 T1T2=Aj0Brαj0j=0j0(1)j(rj)i=1s+2j(r+q)βj0(sjqβj0i+1rβj01)dii=1s+2(r+q)βj0(sqβj0ir+1r(βj01)1)di.

For jj0, (sjqβj0i+1rβj0)=0 as sjj0i+1 < j0 −1 when 1 ≤ is + 2−j − (r=q)βj0. Then

T1T2=Aj0Brαj0j=0r(1)j(rj)i=1s+2j(r+q)βj0(sjqβj0i+1rβj01)dii=1s+2(r+q)βj0(sqβj0ir+1r(βj01)1)di.

Applying Lemma 9.2 for c = sj0 and t = j0 − 1, we get T1T2 = 0.

We set for r ≥ 1, q ∈ ℤ+, βj=s+2jr+q for 0 ≤ jr. Let then T3 and T4 be

T3:=j=0r(1)j(rj)k=2 βj As+2(r+q)kBrki=1rk(sjqki+1rki)di,T4:=k=2 β01 As+2(r+q)k+1Br(k+1)i=1rk(sjq(k+1)ir+1rki)di,

Lemma 9.7.

Let r ≥ 1, q ∈ ℤ+, (dn)n a sequence. Then, only one of the two possibilities holds.

  • For any j, 0 ≤ jr, βj ∈ ℕ and T3 = T4.

  • There is a unique j0 ∈ {0,…, r} such that βj0 ∈ ℕ. In which case,

    T3T4=Aj0Brαj0[ j=0j01(1)j(rj)i=1rβj0(sjqβj0i+1rβj0i)dii=1rβj0(sqβj0ir+1r(βj01)i)di ].

Proof. We follow the same steps as in the proof of Lemma 9.6 by using Lemma 9.3 instead of Lemma 9.2.

Remark 9.

Note that in the second case of Lemma 9.7, as the sum over an empty set is zero and (nk)=0 when n < k, then

T3T4=0for j0=0.

10. Proof of Theorem 4.1

Without loss of generality, we will prove Theorem 4.1 for p = 0. The sequence (Gn(0))n will be written (Gn)n for short.

We set

Z:=j=0r(A)j(rj)Gnjj=0r(A)j(rj)anj1+j=0r1Mj[ αj ],

and prove that for nr + q, Z = BrGn−q−r. So, replacing Gn − j by relation (4.3) and taking account of Remark 1, we obtain

Z=j=0r(1)j(rj)k=1 αj An1(r+q)kBrk( i=1n1j(r+q)k(nj2qkirk1)aiAi+i=1rk(nj2qkirki)biBi)+j=0r(A)j(rj)brαj[αj]+j=0r1Mj[αj].

Let us set,

U=j=0r(1)j(rj)k=1 αj An1(r+q)kBrki=1n1j(r+q)k(nj2qkirk1)aiAi

and

V=j=0r(1)j(rj)k=1 αj An1(r+q)kBrki=1rk(nj2qkirk1)biBi.

If we separate the sum in the right-hand side of U isolating the term with k = 1, we get

U=An1(r+q)Brj=0r(1)j(rj)i=1n1j(r+q)(nj2qir1)aiAi+j=0r(1)j(rj)k=2 αj An1(r+q)kBrki=1n1j(r+q)(nj2qkirk1)aiAi.

Lemma 9.1 gives

U=Bran1qr+j=0r(1)j(rj)k=2 αj An1(r+q)kBrki=1n1j(r+q)(nj2qkirk1)aiAi.

We do the same for V,

V=An1(r+q)Brj=0r(1)j(rj)i=1r(nj2qiri)biBi+j=0r(1)j(rj)k=1 αj An1(r+q)kBrki=1rk(nj2qkirki)biBi.

Lemma 9.3 gives

V=j=0r(1)j(rj)k=2 αj An1(r+q)kBrki=1rk(nj2qkirki)biBi.

Moreover, replacing Gn−q−r by relation (4.3), we get

BrGnqr=k=1 α01 An1(r+q)(k+1)Br(k+1)( i=1n1(r+q)(k+1)(n2q(k+1)irrk1)aiAi +i=1rk(n2q(k+1)irrki)biBj )+Branqr1+Branqr1+Brb(α01)[ α01 ].

Let us set now,

U*=k=1 α01 An1(r+q)(k+1)Br(k+1)i=1n1(r+q)(k+1)(n2q(k+1)irrk1)aiAi+Branqr1,V*=k=1 α01 An1(r+q)(k+1)Br(k+1)i=1rk(n2q(k+1)irrk1)biBi.

Then,

10.1 ZBrGnqr=(UU*)+(VV*)+W,

with

UU*=j=0r(1)j(rj)k=2 αj An1(r+q)kBrki=1n1j(r+q)k(nj2qkirk1)aiAik=1 α01 An1(r+q)(k+1)Br(k+1)i=1n1(r+q)(k+1)(n2q(k+1)irrk1)aiAi,VV*=j=0r(1)j(rj)k=2 αj An1(r+q)kBrki=1rk(nj2qkirki)biBik=1 α01 An1(r+q)(k+1)Br(k+1)i=1rk(n2q(k+1)irrki)biBi,

and

W=j=0r(A)j(rj)brαj[ αj ]+j=0r1Mj[ αj ]Brbr(α01)[ α01 ].

We aim to prove that ZBrGn−q−r, given by formula (10.1), is zero by Lemma 9.5. So, we will consider the two cases for each of the terms UU*, VV* and W.

Case 1. If αj ∈ ℕ, ⌊αj⌋ = ⌊α0⌋ for 0 ≤ jr, then W = 0 and by replacing s by n α 3 in Lemmata 9.6 and 9.7, we get

UU*=T1T2=0,VV*=T3T4=0.

Therefore ZBrGn−q−r = 0.

Case 2. There exists j0, 0 ≤ j0r such that αj0 ∈ ℕ and for j = j0, αj ∈ ℕ. So, we are dealing with two alternatives: j0 = 0 and j0 = 0.

  1. Suppose that j0 = 0. So from Lemma 9.5, α0 ∈ ℕ and αj ∈ ℕ with ⌊αj⌋ = α0 − 1 for j ≠ 0.

    From relation (4.1), W = 0 and by replacing s by n − 3 in Lemmata 9.6 and 9.7, we get

    UU*=T1T2=0,VV*=T3T4.

    From Remark 9, VV* = 0. Therefore ZBrGn−q−r = 0.

  2. Suppose now that j0 ≠ 0. From Lemma 9.5, αj0 ∈ ℕ and for jj0, αj ∈ ℕ with αj ={ αj0forjj0,αj01forjj0+1 . In this case, by relation (4.2),

    W=(A)j0(rj0)brαj0+Mj0.

Replacing s by n − 3 in Lemmata 9.6 and 9.7, we get, UU* = T1T2 = 0 and

VV*=T3T4=Aj0Brαj0[ j=0j01(1)j(rj)i=1rαj0(n2jqαj0irαj0i)biBii=1rαj0r(n2qαj0irr(αj01)i)biBi ].

Introducing the value of αj0, we rewrite VV* as

VV*=Aj0Brαj0(j=0j01(1)j(rj)i=1rαj0(rαj01+j0ijj0j1)biBii=1rαj0r(rαj01+j0irj01)biBi).

By replacing UU*, VV*, W in (10.1), we get

ZBrGnqr=Aj0Brαj0j=0j01(1)j(rj)i=1rαj0(rαj01+j0ijj0j1)biBiAj0Brαj0i=1rαj0r(rαj01+j0irj01)biBi+(A)j0(rj0)brαj0+Mj0.

Now, we write the first sum in the right-hand side of ZBrGn−q−r by isolating i = j0 to obtain

ZBrGnqr=Aj0Brαj0j=0j01(1)j(rj)i=1rαj01(rαj01+j0ijj0j1)biBi+Aj0j=0j01(1)j(rj)(j0j1j0j1)brαj0Aj0Brαj0i=1rαj0r(rαj01+j0irj01)biBi+(A)j0(rj0)brαj0+Mj0.

From relation (4.2) and (9.2)

Mj0=Aj0(s=0j0(1)s(rs)brαj0+t=1rj0Btλt(j0)brαj0t).

Then

ZBrGnqr=Aj0Brαj0(j=0j01(1)j(rj))i=1rαj01(rαj01+j0ijj0j1)biBii=1rαj0r (rαj01+j0irj01)biBi )Aj0t=1rj0Btλt(j0)brαj0t.

Now, we separate the first sum in ZBrGnqr0 following the index i in three parts; 1 ≤ ij0r, j0r + 1 ≤ ij0r 1 + j0 and j0r + j0ij0 − 1 to obtain

ZBrGnqr=Aj0Brαj0(Z1+Z2+Z3Z4Aj0t=1rj0Btλt(j0)brαj0t),

with

Z1=j=0j01(1)(rt)i=1rαj0r(rαj01+j0ijj0j1)biBi,Z2=j=0j01(1)j(rj)i=rαj0r+1rαj0r1+j0(rαj01+j0ijj0j1)biBi,Z3=j=0j01(1)j(rj)i=rαj0r+j0rαj01(rαj01+j0ijj0j1)biBiZ4=i=1rαj0r(rαj01+j0irj01)biBi.

Since (rαj01+j0ijj0j1)=0 for jj0, Z1 becomes

Z1=j=0r(1)j(rj)i=1rαj0r(rαj01+j0ijj0j1)biBi=j=0r(1)j(rj)i=1rαj0r(rαj01+j0ijeαj01)biBias(nk)=(nnk).

Then Lemma 9.3 gives

Z1=i=1rαj0r(rαj01+j0irj01)biBi.

So,

Z1Z4=0.

Otherwise, by setting k = ij0 + r, it is easy to see that

Z2=j=0r(1)j(rj)k=1j01(r1+j0kjrk)bk+rαj0rBk+rαj0r=k=1j01jbk+rαj0rBk+rαj0rj=0r(1)j(rj)=(r1+j0kjrk).

Then according to Lemma 9.3, Z2 = 0. So,

ZBrGnqr=Aj0Brαj0Z3Aj0t=1rj0Btλt(j0)brαj0t,

with

Z3=j=0j01j=1rj0(1)j01(rj)(s+j0j1s)brαj0sBrαj0s

by setting s = j0i, and from Lemma 9.4,

Z3=s=1rj0(1)j01(rs1j01)brαj0sBrαj0s=s=1rj0λs(j0)brαj0sBrαj0s.

Therefore, ZBrGn−q−r = 0 and the proof is complete.


(Communicated by István Gaál)


Funding statement: For Hacéne Belbachir and Fariza Krim, the paper was partially supported by the DGRSDT grant C0656701.

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Received: 2021-07-04
Accepted: 2022-05-17
Published Online: 2023-03-31
Published in Print: 2023-04-01

© 2023 Mathematical Institute Slovak Academy of Sciences

This work is licensed under the Creative Commons Attribution 4.0 International License.

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