Research article

Asymptotics on a heriditary recursion

  • Received: 21 July 2024 Revised: 10 October 2024 Accepted: 16 October 2024 Published: 25 October 2024
  • MSC : 03D99, 11B37, 41A60, 65B15

  • The asymptotic behavior for a heriditary recursion

    x1>aandxn+1=1nsnk=1f(xkk) for every n1

    is studied, where f is decreasing, continuous on (a,) (a<0), and twice differentiable at 0. The result has been known for the case s=1. This paper analyzes the case s>1. We obtain an asymptotic sequence that is quite different from the case s=1. Some examples and applications are provided.

    Citation: Yong-Guo Shi, Xiaoyu Luo, Zhi-jie Jiang. Asymptotics on a heriditary recursion[J]. AIMS Mathematics, 2024, 9(11): 30443-30453. doi: 10.3934/math.20241469

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  • The asymptotic behavior for a heriditary recursion

    x1>aandxn+1=1nsnk=1f(xkk) for every n1

    is studied, where f is decreasing, continuous on (a,) (a<0), and twice differentiable at 0. The result has been known for the case s=1. This paper analyzes the case s>1. We obtain an asymptotic sequence that is quite different from the case s=1. Some examples and applications are provided.



    To the evaluation of sequences, which may be divergent, asymptotic expansions provide a way to compute sequences with arbitrarily high accuracy [4,11,12,17]. Many researchers have studied asymptotics of partial sums and related inequalities. One of the most famous examples is the harmonic sum [10,15], which has an asymptotic estimate

    Hn=nk=11k=lnn+γ+εn,

    where γ=limn(Hnlnn)=0.577 is the constant of Euler and εn0. Zhu [20] calculated the asymptotic expansion of the finite sum of some sequences

    Sn=nk=1(n2+k)1.

    Other well-known examples of asymptotic formulas include the Euler–Maclaurin formula [12], the Euler–Boole type summation formula [6] and the prime number theorem [1]. Grünberg [7] applied the Euler–Maclaurin formula to obtain the asymptotic expansions of the sums,

    nk=1(logk)pkq,nk=1kq(logk)p,nk=1(logk)p(nk)q,nk=11kq(logk)p

    in closed form to arbitrary order (p,qN). Wang and Wong [16] carried out the asymptotic estimation of the partial sum nk=0fn(k)qgn(k). Xu [19] provided an estimate for the partial sum

    γn(z)=nk=1zk1(1klnk+1k),where0<z<1.

    Blagouchine and Moreau [2] derived the complete asymptotic expansion of the finite sum

    Sn(φ,a)n1l=1csc(φ+aπln),nN{1},φ+aπlnπk,kZ.

    Some researchers have also given asymptotic estimates for some recurrences in combinatorial mathematics and algorithms. For example, Xu [18,19] studied the asymptotic series of the generalized Somos recurrence. Hwang, Janson, and Tsai [9] gave exact and asymptotic solutions of a divide-and-conquer recurrence. Heuberger, Krenn, and Lipnik [8] presented some asymptotic analysis of q-recursive sequences.

    However, due to computational complexity and lack of tools or methods, very few papers have investigated asymptotic expansions of heriditary recursions (refer to [5, Section 6.3, p. 291]). Recently, Popa [13] investigated a heriditary recursion

    x1>aandxn+1=1nnk=1f(xkk)for everyn1,

    where f:(a,)(0,) and a<0. He gave the first five terms of the asymptotic expansion of (xn)n1. The aim of this paper is to study the generalized form

    x1>aandxn+1=1nsnk=1f(xkk) for every n1, (1.1)

    where s>1. Using only elementary techniques, we establish an asymptotic estimate of (xn)n1 in (1.1). We obtain an asymptotic sequence for the case s>1 that is quite different from the case s=1. Some examples and applications are provided.

    In this section we first introduce the Euler–Maclaurin formula (see [3,6,14]), from which asymptotic expansions of many sequences and sums can be derived.

    Lemma 2.1 (Euler–Maclaurin formula). Suppose f is k-times continuously differentiable on the interval [a,b] with a<b,a,bZ. Then

    a<nbf(n)=ba{f(x)(1)kk!ψk(x)f(k)(x)}dx+k=1(1)!(f(1)(b)f(1)(a))B.

    Suppose f and all its derivatives go to zero as x. Then we obtain by letting b (and adding f(a) to both sides),

    n=af(n)=af(x)dx+12f(a)k=2(1)!f(1)(a)B(1)kk!af(k)(x)ψk(x)dx,

    where B(x)'s are Bernoulli polynomials, B=B(0)'s are Bernoulli numbers, and ψk(x)=Bk({x}).

    For convenience, let (k1)i be Pochhammer's symbol defined as

    (k1)0:=1,(k1)i:=(k1)k(k+1)(k+2)(k+i2),fori1.

    Put ci(α)=(α1)ii!.

    For α>1, let ζ(α) denote the Riemann zeta function, namely,

    ζ(α)=k=11kα.

    In order to compute the asymptotic expansion, we need the following asymptotic estimate of sums and sequences.

    Lemma 2.2. Let α>1. Then

    (i)

    k=n1kα=1(α1)nα1+12nα+o(1nα),n.

    (ii)

    n1k=11kα=ζ(α)1(α1)nα112nα+o(1nα),n.

    (iii)

    1(n1)α11nα1=i=0ci+1(α)nα+i,

    where ci(α)=(α1)ii!.

    Proof. (ⅰ) By the Euler–Maclaurin formula, f(k)=1kα, α>1, we obtain

    k=n1kα=n1yαdy+12nα+i=2Bii!(α)i1nα+i1=1(α1)nα1+12nα+o(1nα).

    (ⅱ) It is clear that

    n1k=11kα=k=11kαk=n1kα.

    Then the result (ⅱ) immediately follows from (ⅰ).

    (ⅲ) Using the Maclaurin series (1+x)β=1+(β1)x+(β2)x2+o(x2), we have

    1(n1)α11nα1=1nα1(1(11n)α11)=1nα1i=1(α1)ii!ni=i=0ci+1(α)nα+i.

    We first give some asymptotic estimates of the sequence (xn)n1, which is defined by (1.1).

    Lemma 3.1. Suppose that the sequence (xn)n1 is defined by (1.1), f is decreasing, continuous on (a,), a<0, and twice differentiable at 0 with a Taylor series f(x)=f(0)+f(0)x+f(0)x2+o(x2). Then the following results hold:

    (i)limnxn=0,

    (ii)limnns1xn=f(0),

    (iii) the finite sum

    n1k=1(f(xkk)f(0))=f(0)f(0)(ζ(s)1(s1)ns112ns)+o(1ns),n.

    Proof. (ⅰ) Since f takes positive real numbers, we get xn>0 for all n2. Since the inequality xkk>0 for all k2 and f is decreasing, we get f(xkk)f(0), and

    nk=1f(xkk)=f(x1)+nk=2f(xkk)f(x1)+(n1)f(0).

    We deduce that for every n1

    0<xn+1=1nsnk=1f(xkk)f(x1)+(n1)f(0)ns. (3.1)

    Since s>1, it follows from the squeeze theorem that limnxn=0.

    (ⅱ) Moreover, by (ⅰ), we have limnxn/n=0. From the Stolz–Cesàro theorem, and the continuity at 0, we obtain

    limn1nn1k=1f(xkk)=limnf(xnn)=f(0).

    Let n2. It follows from (1.1) that xn=1(n1)sn1k=1f(xkk). Then

    limnns1xn=limnxn1ns1=limn1(n1)sn1k=1f(xkk)1ns1=limnn(n1)s1nn1k=1f(xkk)1ns1=f(0).

    (ⅲ) Since f is differentiable at 0, we have

    limkf(xkk)f(0)xkk=f(0).

    It follows from (ii) and f(x)=f(0)+f(0)x+f(0)x2+o(x2) that

    f(xkk)f(0)=f(0)xkk+f(0)(xkk)2+o((xkk)2)=f(0)f(0)ks+f2(0)f(0)k2s+o(1k2s).

    By Lemma 2.2 (ⅱ), we have

    n1k=1(f(xkk)f(0))=n1k=1(f(0)f(0)ks+f2(0)f(0)k2s+o(1k2s))=f(0)f(0)(ζ(s)1(s1)ns112ns)+o(1ns),n.

    The following theorem gives the first three terms of the asymptotic expansion of xn.

    Theorem 3.1. Suppose that the sequence (xn)n1 is defined by (1.1), f is decreasing, continuous on (a,), a<0, and twice differentiable at 0 with a Taylor series f(x)=f(0)+f(0)x+f(0)x2+o(x2). Then there exists a constant CR such that

    C=limnns(xnf(0)ns1)=ζ(s)+(s1)f(0).

    Moreover, the sequence (xn)n1 of (1.1) has the following asymptotic expansion:

    xn=f(0)ns1+Cns+o(1ns).

    Proof. For every n2, we have

    xnf(0)ns1=1(n1)sn1k=1(f(xkk)f(0))+(1(n1)s11ns1)f(0).

    From Lemma 2.2 (ⅲ) and Lemma 3.1 (ⅲ), we can obtain

    xnf(0)ns1=1(n1)sn1k=1(f(xkk)f(0))+(1(n1)s11ns1)f(0)ζ(s)+c1(s)f(0)ns.

    It follows that

    ns(xnf(0)ns1)C:=ζ(s)+c1(s)f(0)=ζ(s)+(s1)f(0).asn.

    This completes the proof.

    The following theorem gives the first four terms of the asymptotic expansion.

    Theorem 3.2. Suppose that the sequence (xn)n1 is defined by (1.1), f is decreasing, continuous on (a,), a<0, and twice differentiable at 0 with a Taylor series f(x)=f(0)+f(0)x+f(0)x2+o(x2). Let C be defined by Theorem 3.1. Then the sequence (xn)n1 of (1.1) has the following asymptotic expansion:

    (i) If 1<s<2, then

    xn=f(0)ns1+Cns1s11n2s1+o(1n2s1).

    (ii) If s=2, then

    xn=f(0)ns1+Cns+(s1)sf(0)22(s1)ns+1+o(1ns+1).

    (iii) If s>2, then

    xn=f(0)ns1+Cns+(s1)sf(0)2ns+1+o(1ns+1).

    Proof. From Lemma 2.2 (ⅲ) and Lemma 3.1 (ⅲ), we deduce that

    xnf(0)ns1Cns=1(n1)s(n1k=1f(xkk)f(0))+(1(n1)s11ns1)f(0)Cns=1ns(C11(s1)ns112ns)+(c1(s)ns+c2(s)ns+1)f(0)Cns+o(1n2s)=1(s1)n2s1+c2(s)f(0)ns+112n2s+o(1n2s).

    Case 1. Let 1<s<2. Then 2s1<s+1, and

    xnf(0)ns1Cns1(s1)n2s1.

    Thus

    xn=f(0)ns1+Cns1s11n2s1+o(1n2s1).

    Case 2. Let s=2. Then 2s1=s+1<2s, and

    xnf(0)ns1Cns=1(s1)n2s1+c2f(0)ns+1+o(1ns+1)Dns+1,

    where D=c2f(0)1(s1). Thus

    xn=f(0)ns1+Cns+Dns+1+o(1ns+1).

    Case 3. Let s>2. Then s+1<2s1<2s. Hence, we have

    xn=f(0)ns1+Cns+c2f(0)ns+1+o(1ns+1).

    Below is our main theorem, which gives the first five terms of the asymptotic expansion.

    Theorem 3.3. Suppose that the sequence (xn)n1 is defined by (1.1), f is decreasing, continuous on (a,), a<0, and twice differentiable at 0 with a Taylor series f(x)=f(0)+f(0)x+f(0)x2+o(x2). Let C be defined by Theorem 3.1. Then the sequence (xn)n1 of (1.1) has the following asymptotic expansion:

    (i) If 1<s<2, then

    xn=f(0)ns1+Cns1s11n2s1+(s1)sf(0)2ns+1+o(1ns+1).

    (ii) If s=2, then

    xn=f(0)ns1+Cns+(s1)sf(0)22(s1)ns+1+(s1)s(s+1)f(0)36ns+2+o(1ns+2).

    (iii) If 2<s<3, then

    xn=f(0)ns1+Cns+(s1)sf(0)2ns+11s11n2s1+o(1n2s1).

    (iv) If s=3, then

    xn=f(0)ns1+Cns+(s1)sf(0)2ns+1+(s1)s(s+1)f(0)36ns+2+o(1n2s1).

    (v) If s>3, then

    xn=f(0)ns1+Cns+(s1)sf(0)2ns+1+(s1)s(s+1)f(0)6ns+2+o(1n2s1).

    Proof. Case 1. Let 1<s<2. Then 2s1<s+1<2s. By Lemma 2.2 and Lemma 3.1, we have

    xnf(0)ns1Cns+1(s1)1n2s1=1(n1)s(n1k=1f(xkk)f(0))+(f(0)(n1)s1f(0)ns1)Cns+1(s1)1n2s1=1ns(ζ(s)1(s1)ns112ns)+(c1ns+c2ns+1+c3ns+2)f(0)Cns+1(s1)1n2s1+o(1n2s)=c2f(0)ns+112n2s+c3f(0)ns+2+o(1n2s)c2f(0)ns+1.

    Thus

    xn=f(0)ns1+Cns1s11n2s1+c2f(0)ns+1+o(1ns+1).

    Case 2. Let s=2. Then s+2=2s, and

    xnf(0)ns1CnsDns+1=12n2s+c3f(0)ns+2+o(1n2s)Ens+2,

    where

    D=c2f(0)1(s1),E=c3f(0)12.

    Case 3. Let 2<s<3. Then s+1<2s1<s+2<2s, and

    xnf(0)ns1Cnsc2f(0)ns+11(s1)1n2s1.

    Case 4. Let s=3. Then 2s1=s+2<2s, and

    xnf(0)ns1Cnsc2f(0)ns+1=1(s1)1n2s1+c3f(0)ns+2+o(1n2s)Fns+2,

    where

    F=c3f(0)1(s1).

    Case 5. Let s>3. Then s+2<2s1<2s, and

    xnf(0)ns1Cnsc2f(0)ns+1c3f(0)ns+2.

    In this section, we give some applications of our results to several specific examples and a comparison with Popa's results.

    Example 4.1. Let (xn)n1 be a sequence of the real numbers defined by

    xn+1=1nsnk=1exkk,x1R,n1.

    Note that f(x)=ex and f(0)=1.

    When s=32, it follows from Theorem 3.3 (i) that limnxn=0. Moreover,

    nxn=1+Cn1n32+38n2+o(1n2).

    When s=1, it follows from in [13, Theorem 5] that

    xn=1lnnn+An2lnnn2+2A1n2+o(1n2),

    since f(0)=1.

    This example corrects some printing errors in [13, Corollary 6]. And it is easy to see that when s>1, the asymptotic sequence for the case s>1 is completely different from the case s=1.

    Example 4.2. Let (xn)n1 be a sequence of the real numbers defined by x1>1e2 and

    xn+1=1nsnk=11ln(e2+xkk),n1.

    Note that f(x)=1ln(e2+x), and f(0)=12.

    When s=32, by Theorem 3.3 (i), we have limnxn=0, and

    2nxn=1+2Cn4n3/2+38n2+o(1n2).

    When s=4, by Theorem 3.3 (v), we have limnxn=0, and

    2n3xn=1+2Cn+6n2+10n3+o(1n3).

    Our analysis shows that this heriditary recursion can be further expanded according to the residual terms. By comparing asymptotic sequences, depending on the value of s, more and more terms of the asymptotic expansion are obtained.

    Our results show that, for the case s>1, Eq (1.1) has the asymptotic expansion of the form

    xn=kj=0ajnj+o(1nk), as n,

    while, for the case s=1, Eq (1.1) has the asymptotic expansion of the form

    xn=kj=1allnpjnnqj+o(lnpknnqk),

    where qj[0,),pjR and where some of the constants aj may depend on the initial values.

    Yong-Guo Shi: writing original draft, methodology, proof of conclusions; Xiaoyu Luo: writing original draft, methodology, proof of conclusions; Zhi-jie Jiang: validation, writing review, editing, proof of conclusions. The authors contributed equally to this work. All the authors have read and approved the final version of the manuscript for publication.

    We would like to thank the reviewers for having read this manuscript very carefully and for their many constructive and valuable comments, which have enhanced the final version of this paper.

    Yong-Guo Shi is supported by NSF of Sichuan Province (2023NSFSC0065). Xiaoyu Luo is Supported by The Innovation Fund of Postgraduate, Sichuan University of Science & Engineering.

    The authors declare no conflicts of interest.



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