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Minimal recurrences for binomial power sums

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Abstract

For every positive integer rr, we prove that the least order of a polynomial-coefficient recurrence for Fr(n)=∑k=0n(nk)rF_r(n)=\sum_{k=0}^n\binom nk^r is ⌊(r+1)/2⌋\lfloor(r+1)/2\rfloor. This establishes the unrestricted minimal-order assertion arising from Franel's work of 1894–1895. We also determine the least order ⌊r/2⌋\lfloor r/2\rfloor, for r≥2r\geq2, of the alternating sums (−1)n∑k=02n(−1)k(2nk)r(-1)^n\sum_{k=0}^{2n}(-1)^k\binom{2n}{k}^r. The lower bounds follow from real moment representations: every nonzero singularity of the representing measure forces a root of the leading characteristic polynomial of the recurrence. A common reflection argument gives telescoping recurrences attaining both bounds. For the ordinary sums, we combine the deformation of Straub and Zudilin with a shifted prime-power congruence to prove that the minimal shift operator is irreducible over \C(n).

Introduction

For a positive integer rr, the sums

Fr(n)=∑k=0n(nk)r,n=0,1,2,…,(1)F_r(n)=\sum_{k=0}^{n}\binom{n}{k}^r,\qquad n=0,1,2,\ldots, \tag*{(1)}

form a classical family in the theory of polynomial-coefficient recurrences. The first two cases are F1(n)=2nF_1(n)=2^n and F2(n)=(2nn)F_2(n)=\binom{2n}{n}. Franel found second-order recurrences for F3F_3 and F4F_4 in 1894 and 1895 and proposed a general form for the recurrences [8, 9]. The order suggested by those examples is

mr=⌊r+12⌋.m_r=\left\lfloor\frac{r+1}{2}\right\rfloor.

The present paper proves that this order is minimal for every rr. It also determines the corresponding orders for alternating binomial power sums and proves irreducibility and arithmetic rigidity for the ordinary Franel recurrences.

This long-standing problem is supported by a rich history of ideas and prior work. Perlstadt [13] computed recurrences for r=5,6r=5,6, and McIntosh [10] treated r≤10r\le10. Cusick [5] proposed a general construction; Stoll [16] identified a gap in its nonvanishing argument and proved the upper bound mrm_r. Minimality is a separate question: a recurrence obtained from a given summand need not be the shortest recurrence of the sum. Earlier minimality results for r=3,4,5,6r=3,4,5,6 are attributed to Schmidt and Yuan (1995) by Yuan Jin and Dickinson [21 p. 350]. Yuan, Lu and Schmidt [22] ruled out first-order recurrences for every r≥3r\ge3. Straub and Zudilin [17, Theorem 1.1] proved the lower bound mrm_r for recurrences obtained by creative telescoping from (1). They also verified unrestricted minimality computationally for r≤20r\le20 [17 Remark 4.1]. Van Hoeij [19 §5, Remark 6] subsequently obtained the matching telescoping upper bound by polynomial reduction and reflection. For more information, see Tonien’s paper [18].

To state the results clearly, we use the following conventions throughout. A recurrence of order MM for a sequence uu is an identity

∑j=0Mpj(n)u(n+j)=0(n sufficiently large),pj∈C[n],p0pM≠0.(2)\sum_{j=0}^{M}p_j(n)u(n+j)=0\qquad(n\text{ sufficiently large}),\qquad p_j\in\mathbb{C}[n],\quad p_0p_M\ne0. \tag*{(2)}

Rational-function coefficients give the same notion after clearing denominators. Note that the order is the width of the shifts, not the degree of the coefficient polynomials. Two sequences define the same eventual germ if they agree for all sufficiently large indices. All solution spaces below are spaces of such germs.

For a nonzero recurrence, put

D=max⁡jdeg⁡pj,χ(X)=∑j[nD]pj(n)Xj.(3)D=\max_j \deg p_j,\qquad\chi(X)=\sum_j [n^D]p_j(n)X^j. \tag*{(3)}

We call χ\chi its leading characteristic polynomial. This definition refers to the highest degree in nn; its degree in XX can be smaller than the order of the recurrence.

The second family considered here is

Tr(n)=(−1)n∑k=02n(−1)k(2nk)r=∑k=−nn(−1)k(2nn+k)r,r≥2.(4)T_r(n)=(-1)^n\sum_{k=0}^{2n}(-1)^k\binom{2n}{k}^r=\sum_{k=-n}^{n}(-1)^k\binom{2n}{n+k}^r,\qquad r\ge2. \tag*{(4)}

Write ar=⌊r/2⌋a_r=\lfloor r/2\rfloor and define the monic polynomials

Hr(X)=∏0≤k<r/2(X−λr,k),λr,k=(−1)k(2cos⁡πkr)r,(5)H_r(X)=\prod_{0\le k<r/2}(X-\lambda_{r,k}),\qquad\lambda_{r,k}=(-1)^k\left(2\cos\frac{\pi k}{r}\right)^r, \tag*{(5)}
H~r(X)=∏h=0ar−1(X−νr,h),νr,h=(2cos⁡(2h+1)π2r)2r.(6)\widetilde{H}_r(X)=\prod_{h=0}^{a_r-1}(X-\nu_{r,h}),\qquad\nu_{r,h}=\left(2\cos\frac{(2h+1)\pi}{2r}\right)^{2r}. \tag*{(6)}

The formula for HrH_r also gives H1(X)=X−2H_1(X)=X-2.

Theorem 1.1. The least recurrence orders of FrF_r for r≥1r\ge1 and TrT_r for r≥2r\ge2 are respectively mrm_r and ara_r. Both bounds are attained over Q(n)\mathbb{Q}(n) by rational telescoping of the displayed binomial summands.

Moreover, the polynomials HrH_r and H~r\widetilde{H}_r belong to Z[X]\mathbb{Z}[X]. For every polynomial-coefficient recurrence of FrF_r, one has Hr∣χH_r\mid\chi; for every such recurrence of TrT_r, one has H~r∣χ\widetilde{H}_r\mid\chi.

In particular, at the minimum order the corresponding leading characteristic polynomial is a nonzero scalar multiple of HrH_r or H~r\widetilde{H}_r. The formula for HrH_r determines the characteristic polynomial discussed in [19 §7, Question 1]. The divisibility assertion applies to every recurrence, regardless of how it is obtained.

For the alternating sums, McIntosh [11, Theorem 1] gave a construction of recurrences of order at most ara_r and established sharpness when rr is prime or a power of 22 [11 Theorem 2]. His lower bound uses the algebraic degree of the dominant growth constant. The proof here uses every nonzero critical value of a real torus symbol, including values outside the Galois orbit of the dominant one. This gives the same conclusion for all rr.

Let SS denote the forward shift, Su(n)=u(n+1)Su(n)=u(n+1), and let

C(n)[S;σ],σ(c(n))=c(n+1),Sc(n)=c(n+1)S,\mathbb{C}(n)[S;\sigma],\qquad\sigma(c(n))=c(n+1),\qquad Sc(n)=c(n+1)S,

be the shift Ore ring. Let Lr∈Q(n)[S;σ]L_r\in\mathbb{Q}(n)[S;\sigma] be the monic minimal operator of FrF_r. Here monic means that the coefficient of SmrS^{m_r} is 11.

Theorem 1.2 (Irreducibility). For every r≥1r\ge1, the operator LrL_r is irreducible in C(n)[S;σ]\mathbb{C}(n)[S;\sigma].

Furthermore, one can show that every nonzero complex solution germ of LrL_r has the same monic minimal annihilator LrL_r, and every annihilator of that germ is a left multiple of LrL_r. For r≥3r\ge3, no nonzero solution germ is hypergeometric over C(n)\mathbb{C}(n).

We first establish minimality and then use the arithmetic congruence to deduce irreducibility. The coefficient field in Theorem 1.2 is C(n)\mathbb{C}(n); the automorphism fixes the complex constants and sends nn to n+1n+1. Hypergeometric means U(n+1)=a(n)U(n)U(n+1)=a(n)U(n) on a tail for some a(n)∈C(n)a(n)\in\mathbb{C}(n).

The arithmetic of the other solutions is also rigid. A rational sequence is globally bounded on a tail if there are positive integers B,CB,C such that BCnu(n)BC^n u(n) is integral for all sufficiently large nn. For a rational function R(x1,…,xd)R(x_1,\ldots,x_d) regular at the origin, its diagonal is

Diag⁡R(z)=∑n≥0[x1n⋯xdn]R(x1,…,xd)zn.\operatorname{Diag}R(z)=\sum_{n\ge0}[x_1^n\cdots x_d^n]R(x_1,\ldots,x_d)z^n.

Theorem 1.3 (Rational solutions). Let VrV_r be the rational-valued solution space of LrL_r. The limit

L(U)=lim⁡n→∞U(n)Fr(n)\mathcal{L}(U)=\lim_{n\to\infty}\frac{U(n)}{F_r(n)}

exists for every U∈VrU\in V_r and gives a Q\mathbb{Q}-linear isomorphism

Vr→LQ⊕Qπ2⊕⋯⊕Qπ2mr−2.(7)V_r \xrightarrow{\mathcal{L}} \mathbb{Q}\oplus\mathbb{Q}\pi^2\oplus\cdots\oplus\mathbb{Q}\pi^{2m_r-2}. \tag*{(7)}

Note that within VrV_r, each of the following conditions describes exactly the line QFr\mathbb{Q}F_r: bounded denominators on a tail; denominators involving only a fixed finite set of primes; global boundedness; and a generating series which, modulo an element of Q[z]\mathbb{Q}[z], is the diagonal of a rational function over Q\mathbb{Q} regular at the origin. For r≥2r\ge2, the integer-valued solution germs form the group 12ZFr\frac{1}{2}\mathbb{Z}F_r.

The explicit deformation and the values underlying (7) are due to Straub and Zudilin [17 Theorem 1.3]. Together with van Hoeij’s order bound, their independence already makes these solutions a basis of the minimal telescoper. The unrestricted minimality proved here identifies that operator with LrL_r. A congruence at shifted prime powers then separates the basis vectors arithmetically. The denominator growth can be read from the limit itself: if a nonzero solution has L(U)=PU(π2)\mathcal{L}(U)=P_U(\pi^2), with PU∈Q[X]P_U\in\mathbb{Q}[X] of degree less than mrm_r, its common denominators through index NN have logarithm 2deg⁡(PU)N+o(N)2\deg(P_U)N+o(N) (Theorem 6.1). This yields the classification in Theorem 1.3. For r=3r=3, it also answers the integer-sequence question of Schulte, VanSchalkwyk and Yang [15 Conjecture 4.5]; a short independent proof is given in Corollary 6.2.

The two mechanisms

The analytic part begins with a general observation. If u(n)=∫xn dμ(x)u(n)=\int x^n\,\mathrm{d}\mu(x) for a compactly supported measure, then a recurrence for uu becomes a differential equation for μ\mu. Away from zero, each point where μ\mu fails to have a smooth density must be a zero of χ\chi (Proposition 2.1). Moment recurrences and differential equations have long been studied together; relevant forms appear in Batenkov’s work on piecewise DD-finite functions [1 Theorems 2.9 and 2.13] and in the work of Bostan, Elvey Price, Guttmann and Maillard on Stieltjes moment sequences [2 Theorem 3]. The distributional formulation used here applies directly to eventual recurrences and retains the exact polynomial χ\chi.

Franel already derived the r=3r=3 recurrence from a double integral [8 p. 46]. Here the measures are pushforwards of Haar measure under explicit real Laurent polynomials. Every critical point lying over a nonzero value is a nondegenerate extremum. At each such value the local density contributions have the same sign and orientation, so they cannot cancel. Counting these values proves the required lower bounds. Essam and Guttmann [7 §III B] developed the lattice-walk interpretation of FrF_r and related its generating function to Green functions of projected lattices. Our measure is the spectral measure at the origin of a symmetric lattice-walk operator. Its critical-value singularities are the density-of-states phenomenon studied by van Hove [20]. The recurrence consequence uses the interior critical values as well as the spectral edge.

The arithmetic part uses a different feature. After multiplication by a suitable power of pp, each deformation coefficient at p+bp+b reduces to a fixed nonzero multiple of Fr(b)F_r(b). An annihilating recurrence for any nonzero linear combination can therefore be transferred to FrF_r. A finite-dimensional descent over Q\mathbb{Q} makes this argument work for arbitrary complex coefficients (Proposition 5.4). It proves irreducibility without factoring the recurrence operator.

Organization

Sections 2–4 prove Theorem 1.1. Section 5 develops the congruence and proves Theorem 1.2; Section 6 proves the arithmetic classification. Appendix § 7 determines the exact dependence of a minimal telescoping certificate on its summation variable, resolving that part of the patterns recorded in [17 Remark 4.1].

A singular-support bound for moment recurrences

A distribution is smooth on an interval if it is given there by a C∞C^\infty function times Lebesgue measure. Its singular support is the complement of the largest open set on which it is smooth. For a compactly supported distribution μ\mu, its moments ⟨μ,xn⟩\langle\mu,x^n\rangle are well-defined by inserting any smooth cutoff equal to 1 near its support.

Proposition 2.1. Let μ\mu be a compactly supported distribution on R\mathbb{R} and put u(n)=⟨μ,xn⟩u(n)=\langle\mu,x^n\rangle. Suppose

∑j=0Mpj(n)u(n+j)=0(n≥N),pj∈C[n],(p0,…,pM)≠0.(8)\sum_{j=0}^{M}p_j(n)u(n+j)=0 \qquad(n\geq N), \qquad p_j\in\mathbb{C}[n], \qquad(p_0,\ldots,p_M)\ne0. \tag*{(8)}

Here N∈Z≥0N\in\mathbb{Z}_{\geq0}. With DD and χ\chi as in (3),

sing supp⁡μ∖{0}⊆{x∈R:χ(x)=0}.(9)\operatorname{sing\,supp}\mu\setminus\{0\}\subseteq\{x\in\mathbb{R}:\chi(x)=0\}. \tag*{(9)}

In particular, MM is at least the number of distinct nonzero points of sing supp⁡μ\operatorname{sing\,supp}\mu.

Proof. Use bilinear distribution pairing. The Euler operator E=x d/dxE=x\,d/dx has formal transpose E∗=−x d/dx−1E^*=-x\,d/dx-1. The compactly supported distribution

T=∑j=0Mpj(E∗)(xjμ)T=\sum_{j=0}^{M}p_j(E^*)(x^j\mu)

satisfies ⟨T,xn⟩=0\langle T,x^n\rangle=0 for n≥Nn\geq N, since Exn=nxnEx^n=nx^n. Every moment of xNTx^NT therefore vanishes. The Fourier–Laplace transform of a compactly supported distribution is entire, and its derivatives at zero are its moments, up to nonzero constants. Thus the transform of xNTx^NT vanishes identically, and uniqueness of the Fourier transform gives xNT=0x^NT=0. Consequently T=0T=0 away from 0.

The coefficient of μ(D)\mu^{(D)} in TT is

(−1)DxDχ(x).(-1)^D x^D\chi(x).

Indeed, the highest derivative in (E∗)D(xjμ)(E^*)^D(x^j\mu) has coefficient (−1)DxD+j(-1)^D x^{D+j}. By definition of DD, the polynomial χ\chi is nonzero. Near a point x0≠0x_0\ne0 where χ(x0)≠0\chi(x_0)\ne0, the equation T=0T=0 is a regular linear ordinary differential equation for μ\mu. Its distributional solutions are smooth: for D>0D>0, form the first-order system for (μ,μ′,…,μ(D−1))(\mu,\mu',\ldots,\mu^{(D-1)}) and multiply by the inverse of a smooth fundamental matrix. The resulting distributional vector has derivative zero and is constant. For D=0D=0, multiplication by a nonvanishing function forces μ\mu to vanish locally. This proves (9). The last assertion follows from deg⁡χ≤M\deg\chi\leq M. □

The exclusion of 0 is necessary: a distribution supported at 0 can have all sufficiently high moments equal to zero. Positivity is not required in the proposition. It enters through the following criterion for a critical value to belong to the singular support.

Lemma 2.2. Let PP be a smooth real function on a compact smooth manifold without boundary of dimension d≥1d\geq1, equipped with a positive smooth density. Let μ\mu be its pushforward under PP. Suppose that the critical points in the fiber P−1(λ)P^{-1}(\lambda) form a nonempty finite set, are all nondegenerate, and are all local maxima or all local minima. Then λ∈sing supp⁡μ\lambda\in\operatorname{sing\,supp}\mu.

Proof. Choose disjoint neighborhoods of these critical points and smooth nonnegative cutoffs equal to 1 near them. The Morse lemma gives coordinates in which P=λ+η∣y∣2P=\lambda+\eta|y|^2, with the same η∈{1,−1}\eta\in\{1,-1\} at every point. Polar integration shows that the local pushforward density, with t=η(x−λ)t=\eta(x-\lambda), has the form

1{t>0}td/2−1h(t),h∈C∞([0,ϵ)),h(0)>0.(10)\mathbf{1}_{\{t>0\}}t^{d/2-1}h(t), \qquad h\in C^\infty([0,\epsilon)), \qquad h(0)>0. \tag*{(10)}

The spherical average of the smooth coordinate density is a smooth even function of the radius, hence a smooth function of its square. This proves the asserted smoothness of hh. The contribution from the remainder of the manifold is smooth near λ\lambda, by integration along regular level sets. Compactness and nondegeneracy ensure that a sufficiently small neighborhood of λ\lambda contains no further critical points outside the chosen neighborhoods.

Adding the local terms preserves the form (10) with positive h(0)h(0). A one-sided power with exponent d/2−1d/2-1 is not smooth at zero: for an integer exponent a derivative has a jump, and for a noninteger exponent a derivative is unbounded. A smooth remainder cannot remove this defect. Hence μ\mu is not smooth at λ\lambda. □\square

The real torus symbols and their critical values

Fix r≥2r \ge2 and put d=r−1d=r-1. On the torus Td\mathbb{T}^{d}, write zj=eiθjz_j=e^{i\theta_j}, Z=z1⋯zdZ=z_1\cdots z_d, and

A(z)=∏j=1d(1+zj),P=A+A(z−1)=A(1+Z−1),Q=A−A(z−1)i=A(1−Z−1)i.A(z)=\prod_{j=1}^{d}(1+z_j),\qquad P=A+A(z^{-1})=A(1+Z^{-1}),\qquad Q=\frac{A-A(z^{-1})}{i}=\frac{A(1-Z^{-1})}{i}.

Both PP and QQ are real-valued on the torus. With s=θ1+⋯+θds=\theta_1+\cdots+\theta_d, they become

P(θ)=2r∏j=1dcos⁡(θj/2)cos⁡(s/2),Q(θ)=2r∏j=1dcos⁡(θj/2)sin⁡(s/2).(11)P(\theta)=2^r\prod_{j=1}^{d}\cos(\theta_j/2)\cos(s/2),\qquad Q(\theta)=2^r\prod_{j=1}^{d}\cos(\theta_j/2)\sin(s/2). \tag*{(11)}

These products are periodic, despite the separate half-angle factors. Let μr\mu_r be the pushforward of normalized Haar measure under PP, and let μ~r\widetilde{\mu}_r be its pushforward under R=Q2R=Q^2.

Lemma 3.1. For every n≥0n \ge0,

Fr(n)=CT⁡Pn=∫xn dμr(x),Tr(n)=CT⁡Q2n=∫xn dμ~r(x).(12)F_r(n)=\operatorname{CT} P^n=\int x^n\,d\mu_r(x),\qquad T_r(n)=\operatorname{CT} Q^{2n}=\int x^n\,d\widetilde{\mu}_r(x). \tag*{(12)}

Proof. Expanding (1+Z−1)n(1+Z^{-1})^n gives

CT⁡Pn=∑k=0n(nk)CT⁡(AnZ−k)=∑k=0n(nk)r.\operatorname{CT} P^n=\sum_{k=0}^{n}\binom{n}{k}\operatorname{CT}(A^nZ^{-k})=\sum_{k=0}^{n}\binom{n}{k}^{r}.

Likewise,

CT⁡Q2n=(−1)n∑k=02n(−1)k(2nk)CT⁡(A2nZ−k)=Tr(n).\operatorname{CT} Q^{2n}=(-1)^n\sum_{k=0}^{2n}(-1)^k\binom{2n}{k}\operatorname{CT}(A^{2n}Z^{-k})=T_r(n).

Constant terms are torus integrals against normalized Haar measure. □\square

Lemma 3.2. The distinct nonzero critical values of PP are exactly λr,k\lambda_{r,k}, 0≤k<r/20 \le k < r/2. At each such value all critical points are nondegenerate extrema of the same type. The distinct nonzero critical values of R=Q2R=Q^2 are exactly νr,h\nu_{r,h}, 0≤h<ar0 \le h < a_r. All critical points at these values are nondegenerate local maxima.

Proof. At a point where P≠0P \ne0, all factors in (11) are nonzero, and

∂θjlog⁡∣P∣=−12tan⁡(θj/2)−12tan⁡(s/2).\partial_{\theta_j}\log|P|=-\frac{1}{2}\tan(\theta_j/2)-\frac{1}{2}\tan(s/2).

Thus all θj\theta_j at a nonzero critical point are equal modulo 2π2\pi, say to θ\theta, and rθ≡0(mod2π)r\theta\equiv0\pmod{2\pi}. The possible points are θj=2πk/r\theta_j=2\pi k/r, 0≤k<r0\le k<r; the point with θj=π\theta_j=\pi, when present, has value zero and is excluded. The value at every other point is

P=(−1)k(2cos⁡πkr)r.P=(-1)^k\left(2\cos\frac{\pi k}{r}\right)^r.

The indices kk and r−kr-k give the same value. The representatives 0≤k<r/20\le k<r/2 have strictly decreasing absolute values, so they give all the distinct nonzero critical values. At these points,

Hess⁡log⁡∣P∣=−14sec⁡2(πkr)(Id+Jd),(13)\operatorname{Hess}\log|P|=-\frac{1}{4}\sec^2\left(\frac{\pi k}{r}\right)(I_d+J_d), \tag*{(13)}

where JdJ_d is the all-ones matrix. This matrix is negative definite. Since Hess⁡P=PHess⁡log⁡∣P∣\operatorname{Hess}P=P\operatorname{Hess}\log|P| at a critical point, a positive critical value is a nondegenerate maximum and a negative one is a nondegenerate minimum. For Q≠0Q \ne0, the critical equations instead read

∂θjlog⁡∣Q∣=−12tan⁡(θj/2)+12cot⁡(s/2)=0.\partial_{\theta_j}\log|Q| = -\frac{1}{2}\tan(\theta_j/2) + \frac{1}{2}\cot(s/2) = 0.

They force θj=(2h+1)π/r\theta_j = (2h+1)\pi/r, 0≤h<r0 \le h < r. Writing α=(2h+1)π/(2r)\alpha= (2h+1)\pi/(2r), one obtains

Q=(−1)h(2cos⁡α)r,Hess⁡log⁡∣Q∣=−14sec⁡2α (Id+Jd).Q = (-1)^h(2\cos\alpha)^r,\qquad\operatorname{Hess}\log|Q| = -\frac{1}{4}\sec^2\alpha\,(I_d+J_d).

When rr is odd, the point with θj=π\theta_j=\pi has value zero and is excluded. Since ∇R=2Q∇Q\nabla R=2Q\nabla Q, there are no other nonzero critical points of RR. At every such point, Hess⁡R=2Q2Hess⁡log⁡∣Q∣\operatorname{Hess}R=2Q^2\operatorname{Hess}\log|Q| is negative definite. Pairing hh with r−1−hr-1-h leaves precisely the distinct values νr,h\nu_{r,h} in (6). □

Lemmas 2.2 and 3.2 show that each λr,k\lambda_{r,k} belongs to sing supp⁡μr\operatorname{sing\,supp}\mu_r and each νr,h\nu_{r,h} belongs to sing supp⁡μ~r\operatorname{sing\,supp}\widetilde{\mu}_r. Proposition 2.1 therefore proves the divisibilities in Theorem 1.1 and the lower bounds mrm_r and ara_r. The case r=1r=1 follows directly from F1(n)=2nF_1(n)=2^n: its recurrence implies ∑jpj(n)2j=0\sum_j p_j(n)2^j=0, hence χ(2)=0\chi(2)=0.

Lemma 3.3. One has Hr,H~r∈Z[X]H_r,\widetilde{H}_r\in\mathbb{Z}[X].

Proof. For zr=1z^r=1, the values (1+z)r(1+z)^r are precisely the critical values of PP, with the possible additional value zero. Inversion pairs the equal values; the value at z=1z=1 is unpaired. Thus the distinct nonzero values form the root set of HrH_r. They are algebraic integers and this set is stable under the Galois group of the cyclotomic field. The coefficients of HrH_r are consequently rational algebraic integers.

Similarly, for zr=−1z^r=-1, the values −(1+z)2r-(1+z)^{2r} are precisely the roots of H~r\widetilde{H}_r, with each nonzero value counted twice and the additional value zero when rr is odd. The same argument proves the assertion for H~r\widetilde{H}_r. □

Some small cases illustrate the two spectra:

rrHr(X)H_r(X)H~r(X)\widetilde{H}_r(X)
2X−4X-4X−4X-4
3(X−8)(X+1)(X-8)(X+1)X−27X-27
4(X−16)(X+4)(X-16)(X+4)X2−136X+16X^2-136X+16
5(X−32)(X2+11X−1)(X-32)(X^2+11X-1)X2−625X+3125X^2-625X+3125
6(X−64)(X+27)(X−1)(X-64)(X+27)(X-1)(X−64)(X2−2702X+1)(X-64)(X^2-2702X+1)

Table 3.

The positive roots of H~r\widetilde{H}_r also give a sparsity bound: every recurrence of TrT_r has at least ar+1a_r+1 coefficient polynomials of maximal degree. Indeed, a nonzero real or imaginary part of χ\chi has the ara_r distinct positive roots νr,h\nu_{r,h}, so Descartes’ rule of signs requires at least ar+1a_r+1 nonzero monomials. In particular, every coefficient of a minimum-order alternating recurrence has maximal degree. For a minimum-order ordinary recurrence, both endpoint coefficients have maximal degree, since HrH_r is monic and has nonzero constant coefficient.

Remark 3.4. The representation of TrT_r makes it a Stieltjes moment sequence with support exactly [0,νr,0][0,\nu_{r,0}]. Indeed, the continuous image of the connected torus under Q2Q^2 is this interval, and the inverse image of every open interval meeting it has positive Haar measure. Consequently, all its Hankel minors with strictly increasing row and column indices are positive. To see the strictness, the determinant integration identity expresses such a minor as

1s!∫det⁡[xℓai]i,ℓ=1sdet⁡[xℓbj]j,ℓ=1s∏ℓ=1sdμ~r(xℓ),\frac{1}{s!}\int\det[x_\ell^{a_i}]_{i,\ell=1}^{s}\det[x_\ell^{b_j}]_{j,\ell=1}^{s}\prod_{\ell=1}^{s}d\widetilde{\mu}_r(x_\ell),

where aia_i and bjb_j are strictly increasing nonnegative integers. Both generalized Vandermonde determinants are positive when 0<x1<⋯<xs0<x_1<\cdots<x_s, and their product is nonnegative everywhere. Full support gives strict positivity of the integral. In particular, the ratios Tr(n+1)/Tr(n)T_r(n+1)/T_r(n) increase strictly to νr,0\nu_{r,0}. These are standard consequences of the moment representation; the recurrence lower bound requires its additional interior singularities.

A common telescoping construction

We give a common proof of the matching upper bounds. The ordinary case follows the reduction and reflection argument of van Hoeij [19 §5, Remark 6]. The signed formulation below also treats the alternating sums and verifies the certificate boundary terms. In particular, a minimum-order recurrence of FrF_r telescopes the original summand, as required for the deformation theorem used in § 5. Write (x)j=x(x+1)⋯(x+j−1)(x)_j=x(x+1)\cdots(x+j-1), with (x)0=1(x)_0=1.

Lemma 4.1. Let r≥2r\ge2 and ε∈{1,−1}\varepsilon\in\{1,-1\}, and put

qε={1,ε=1,2,ε=−1,mε={⌊(r+1)/2⌋,ε=1,⌊r/2⌋,ε=−1.q_\varepsilon= \begin{cases} 1, & \varepsilon=1,\\ 2, & \varepsilon=-1, \end{cases} \qquad m_\varepsilon= \begin{cases} \lfloor(r+1)/2\rfloor, & \varepsilon=1,\\ \lfloor r/2\rfloor, & \varepsilon=-1. \end{cases}

There exist p0,…,pmε∈Q[n]p_0,\ldots,p_{m_\varepsilon}\in\mathbb{Q}[n], not all zero, and C∈Q(n,k)C\in\mathbb{Q}(n,k) such that, for fε(n,k)=εk(nk)rf_\varepsilon(n,k)=\varepsilon^k\binom{n}{k}^r,

∑a=0mεpa(n)fε(n+qεa,k)=C(n,k+1)fε(n,k+1)−C(n,k)fε(n,k).(14)\sum_{a=0}^{m_\varepsilon}p_a(n)f_\varepsilon(n+q_\varepsilon a,k)=C(n,k+1)f_\varepsilon(n,k+1)-C(n,k)f_\varepsilon(n,k). \tag*{(14)}

For all sufficiently large nonnegative integers nn, the certificate product has well-defined, finitely supported values on k∈Zk\in\mathbb{Z}, with removable singularities interpreted by continuation. Its bilateral forward difference therefore sums to zero.

Proof. Work over K=Q(n)K=\mathbb{Q}(n) and set

DεC(k)=ε(n−kk+1)rC(k+1)−C(k),Qj(k)=(n+1)jr(n−k+1)jr.D_\varepsilon C(k)=\varepsilon\left(\frac{n-k}{k+1}\right)^r C(k+1)-C(k), \qquad Q_j(k)=\frac{(n+1)_j^r}{(n-k+1)_j^r}.

Brackets denote classes modulo DεK(k)D_\varepsilon K(k). We will bound only the span of the selected shift classes [Qqεa][Q_{q_\varepsilon a}].

First remove the poles of QjQ_j from right to left. If the rightmost remaining pole is k=n+hk=n+h, write its principal part as A(k)/(n−k+h)rA(k)/(n-k+h)^r, with deg⁡kA<r\deg_k A<r. Since krk^r is invertible modulo (n−k+h)r(n-k+h)^r in K[k]K[k], choose H∈K[k]H\in K[k], deg⁡H<r\deg H<r, with

krH(k)≡A(k)(mod(n−k+h)r).k^rH(k)\equiv A(k)\pmod{(n-k+h)^r}.

For Vh(k)=krH(k)/(n−k+h)rV_h(k)=k^rH(k)/(n-k+h)^r one has

DεVh(k)=ε(n−k)rH(k+1)(n−k+h−1)r−krH(k)(n−k+h)r.D_\varepsilon V_h(k)=\varepsilon\frac{(n-k)^rH(k+1)}{(n-k+h-1)^r}-\frac{k^rH(k)}{(n-k+h)^r}.

Adding this expression cancels the pole at n+hn+h and introduces at most a pole at n+h−1n+h-1; for h=1h=1 its first term is polynomial. Thus Pj=Qj+DεUjP_j=Q_j+D_\varepsilon U_j is polynomial, where UjU_j is a finite sum of such VhV_h. For j=0j=0 take P0=1P_0=1 and U0=0U_0=0.

Each VhV_h is O(kr−1)O(k^{r-1}) at infinity. If ε(−1)r=1\varepsilon(-1)^r=1, the multiplier in DεD_\varepsilon is 1+O(k−1)1+O(k^{-1}), so the leading terms cancel and DεVh=O(kr−2)D_\varepsilon V_h=O(k^{r-2}). Otherwise it is −1+O(k−1)-1+O(k^{-1}), giving DεVh=O(kr−1)D_\varepsilon V_h=O(k^{r-1}). Since QjQ_j is proper for j≥1j\ge1, in both cases

deg⁡Pj<bε,bε=r−1{ε(−1)r=1}.\deg P_j<b_\varepsilon,\qquad b_\varepsilon=r-\mathbf{1}_{\{\varepsilon(-1)^r=1\}}.

Let JC(k)=C(n−k)JC(k)=C(n-k). Direct substitution gives

JDεC=DεC⋆,C⋆(k)=−ε(kn−k+1)rC(n−k+1).JD_\varepsilon C=D_\varepsilon C^\star, \qquad C^\star(k)=-\varepsilon\left(\frac{k}{n-k+1}\right)^r C(n-k+1).

Hence JJ induces an involution on the quotient. Moreover,

εjJQj−Qj=DεBj,Bj(k)=∑ℓ=0j−1εℓ(n+1)jr(k+1)ℓr(n−k+1)j−ℓr.\varepsilon^jJQ_j-Q_j=D_\varepsilon B_j, \qquad B_j(k)=\sum_{\ell=0}^{j-1}\frac{\varepsilon^\ell(n+1)_j^r}{(k+1)_\ell^r(n-k+1)_{j-\ell}^r}.

Indeed, after multiplication by fε(n,k)f_\varepsilon(n,k), this is the telescoping sum of the jj consecutive shifts in kk of fε(n+j,k)f_\varepsilon(n+j,k). For j=qεaj=q_\varepsilon a one has εj=1\varepsilon^j=1. Consequently

Sj=Pj+JPj2,Qj−Sj=−12Dε(Uj+Uj⋆+Bj).S_j=\frac{P_j+JP_j}{2}, \qquad Q_j-S_j=-\frac{1}{2}D_\varepsilon(U_j+U_j^\star+B_j).

The polynomial SjS_j is even in k−n/2k-n/2 and has degree less than bεb_\varepsilon. Such polynomials form a space of dimension ⌈bε/2⌉=mε\lceil b_\varepsilon/2\rceil=m_\varepsilon, with basis 1,(k−n/2)2,…,(k−n/2)2(mε−1)1,(k-n/2)^2,\ldots,(k-n/2)^{2(m_\varepsilon-1)}.

Thus the mε+1m_\varepsilon+1 representatives S0,Sqε,…,SqεmεS_0,S_{q_\varepsilon},\ldots,S_{q_\varepsilon m_\varepsilon} are linearly dependent over KK. The displayed certificate identity, followed by clearing denominators in nn, gives (14).

For the boundary assertion, specialize n=Nn=N to a sufficiently large nonnegative integer, avoiding all parameter poles in the finitely many rational functions used above. Put δ=(1−ε)/2\delta=(1-\varepsilon)/2 and use the entire continuation in kk

fε(N,k)=eiπδk{Γ(N+1)Γ(k+1)Γ(N−k+1)}r.f_\varepsilon(N,k)=e^{i\pi\delta k}\left\{\frac{\Gamma(N+1)}{\Gamma(k+1)\Gamma(N-k+1)}\right\}^{r}.

It has zeros of order rr at every integer outside [0,N][0,N]. Therefore VhfεV_hf_\varepsilon has a removable singularity at its only possible pole k=N+hk=N+h, and its integer values have finite support. The reflected certificate is explicitly

Vh∗(k)=−εkrH(N−k+1)(k+h−1)r.V_h^*(k)=-\varepsilon\frac{k^rH(N-k+1)}{(k+h-1)^r}.

It is polynomial when h=1h=1; otherwise its sole possible pole is the negative integer 1−h1-h, again canceled by a zero of order rr. Finally,

Bj(k)fε(N,k)=∑ℓ=0j−1fε(N+j,k+ℓ),B_j(k)f_\varepsilon(N,k)=\sum_{\ell=0}^{j-1}f_\varepsilon(N+j,k+\ell),

whose integer values also have finite support. Every certificate in the construction is a finite linear combination of these products. Their bilateral forward differences consequently sum to zero. □

Completion of the proof of Theorem 1.1. For ε=1\varepsilon=1, bilateral summation in Lemma 4.1 gives a nonzero recurrence of order at most mrm_r for FrF_r. For ε=−1\varepsilon=-1, specialize the parameter to 2n2n and use

∑kf−1(2n+2j,k)=(−1)n+jTr(n+j).\sum_k f_{-1}(2n+2j,k)=(-1)^{n+j}T_r(n+j).

The resulting recurrence is ∑j=0αr(−1)jpj(2n)Tr(n+j)=0\sum_{j=0}^{\alpha_r}(-1)^jp_j(2n)T_r(n+j)=0 and has order at most αr\alpha_r. Nonzero polynomial coefficients remain nonzero under the substitution n↦2nn\mapsto2n. If either endpoint vanished, translating the index would give a recurrence of smaller width, contrary to the lower bounds proved in Section 3. The divisibility already proved then gives χ=cHr\chi=cH_r or cH~rc\widetilde{H}_r at the minimum order. For r=1r=1, the identity F1(n+1)=2F1(n)F_1(n+1)=2F_1(n) supplies the upper bound. Its normalized certificate is −k/(n−k+1)-k/(n-k+1), whose product with (nk)\binom{n}{k} is −(n−1k−1)-\binom{n-1}{k-1} and has finite support on the integer lattice. □

The deformation and its arithmetic

A deformation theorem

Define the even rational function

Ar(n,t)=∑k=0n(nk)r{∏h=1k(1−th)∏h=1n−k(1+th)}−r=∑j≥0Ar,j(n)t2j.(15)A_r(n,t)=\sum_{k=0}^{n}\binom{n}{k}^{r}\left\{\prod_{h=1}^{k}\left(1-\frac{t}{h}\right)\prod_{h=1}^{n-k}\left(1+\frac{t}{h}\right)\right\}^{-r} =\sum_{j\geq0}A_{r,j}(n)t^{2j}. \tag*{(15)}

Empty products are 1. Evenness follows by replacing kk by n−kn-k, and every Ar,j(n)A_{r,j}(n) is rational. In particular, Ar,0=FrA_{r,0}=F_r. We use the following result with its original attribution.

Theorem 5.1 (Straub–Zudilin, [17 Theorems 1.3 and 3.1]). Every recurrence over Q(n)\mathbb{Q}(n) obtained by rational telescoping from (nk)r\binom{n}{k}^{r} is solved, for all sufficiently large nn, by Ar,jA_{r,j} for 2j<r2j<r. For every j≥0j\geq0,

lim⁡n→∞Ar,j(n)Fr(n)=ϕr,jπ2j,ϕr,j=[t2j](tsin⁡t)r∈Q>0.(16)\lim_{n\to\infty}\frac{A_{r,j}(n)}{F_r(n)}=\phi_{r,j}\pi^{2j},\qquad\phi_{r,j}=[t^{2j}]\left(\frac{t}{\sin t}\right)^r\in\mathbb{Q}_{>0}. \tag*{(16)}

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The telescoping construction in § 4 and minimality show that Ar,0,…,Ar,mr−1A_{r,0},\ldots,A_{r,m_r-1} solve LrL_r. The case r=1r=1 is immediate from A1,0(n)=2nA_{1,0}(n)=2^n. Independence follows from these limits and the transcendence of π\pi, as in [17 proof of Theorem 1.1]. We give an arithmetic proof as part of a congruence that will control denominators and annihilators.

One congruence at shifted prime powers

Write vpv_p for the valuation normalized by vp(p)=1v_p(p)=1, with vp(0)=+∞v_p(0)=+\infty, and Z(p)={x∈Q:vp(x)≥0}\mathbb{Z}_{(p)}=\{x\in\mathbb{Q}:v_p(x)\geq0\}. Congruences of formal power series are coefficientwise. Put ℓn=lcm⁡(1,…,n)\ell_n=\operatorname{lcm}(1,\ldots,n) for n≥1n\geq1, and ℓ0=1\ell_0=1.

Lemma 5.2. For every r≥1r\geq1 and n≥0n\geq0,

Ar(n,ℓnt)∈Z[[t]].(17)A_r(n,\ell_n t)\in\mathbb{Z}[[t]]. \tag*{(17)}

For any prime pp and integers α≥1\alpha\geq1 and 0≤b<p0\leq b<p, the series Ar(pα+b,pαt)A_r(p^\alpha+b,p^\alpha t) lies in Z(p)[[t]]\mathbb{Z}_{(p)}[[t]] and

Ar(pα+b,pαt)≡Fr(b)((1−t)−r+(1+t)−r)(modp).(18)A_r(p^\alpha+b,p^\alpha t)\equiv F_r(b)\left((1-t)^{-r}+(1+t)^{-r}\right)\pmod p. \tag*{(18)}

Consequently, for every j≥0j\geq0,

ℓn2jAr,j(n)∈Z,p2jαAr,j(pα+b)≡Cr,jFr(b)(modp),Cr,j=2(r+2j−12j).(19)\ell_n^{2j}A_{r,j}(n)\in\mathbb{Z},\qquad p^{2j\alpha}A_{r,j}(p^\alpha+b)\equiv C_{r,j}F_r(b)\pmod p,\qquad C_{r,j}=2\binom{r+2j-1}{2j}. \tag*{(19)}

For fixed r,j,br,j,b, one has vp(Ar,j(pα+b))=−2jαv_p(A_{r,j}(p^\alpha+b))=-2j\alpha for all sufficiently large primes pp, uniformly in α≥1\alpha\geq1.

Proof. Replacing tt by ℓnt\ell_n t in (15) makes every factor (1±ℓnt/h)−r(1\pm\ell_n t/h)^{-r} an integral formal power series. This proves (17).

Put N=pα+b<2pαN=p^\alpha+b<2p^\alpha. For 1≤h≤N1\leq h\leq N one has vp(h)≤αv_p(h)\leq\alpha. The only index with valuation α\alpha is h=pαh=p^\alpha. After replacing tt by pαtp^\alpha t, every factor therefore lies in Z(p)[[t]]\mathbb{Z}_{(p)}[[t]], and every factor except the one with h=pαh=p^\alpha is congruent to 11 modulo pp. The identity

(1+x)N≡(1+xpα)(1+x)b(modp)(1+x)^N\equiv(1+x^{p^\alpha})(1+x)^b\pmod p

shows that the summands with b<k<pαb<k<p^\alpha vanish modulo pp. For 0≤k≤b0\leq k\leq b, the exceptional factor occurs in the second product and gives (1+t)−r(1+t)^{-r}, while (Nk)≡(bk)(modp)\binom{N}{k}\equiv\binom{b}{k}\pmod p. For k=pα+qk=p^\alpha+q, 0≤q≤b0\leq q\leq b, it occurs in the first product and gives (1−t)−r(1-t)^{-r}, while (Npα+q)≡(bq)(modp)\binom{N}{p^\alpha+q}\equiv\binom{b}{q}\pmod p. Summing proves (18). Coefficient extraction gives (19). Its right side is a fixed nonzero integer, so it is a unit at all sufficiently large primes. This proves the valuation assertion. □\square

Proposition 5.3. The eventual germs Ar,0,…,Ar,mr−1A_{r,0},\ldots,A_{r,m_r-1} form a basis of the rational solution space of LrL_r over Q\mathbb{Q} and of the complex solution space over C\mathbb{C}. The limit map in (7) is a Q\mathbb{Q}-linear isomorphism.

Proof. In fact, every finite collection Ar,0,…,Ar,JA_{r,0},\ldots,A_{r,J} is linearly independent over Q\mathbb{Q} as eventual germs. In a nonzero proposed relation, let JJ be the highest index with nonzero coefficient. For every sufficiently large prime pp, all its nonzero rational coefficients are pp-adic units, and Lemma 5.2 with b=0b=0, α=1\alpha=1 gives distinct valuations −2j-2j for the summands at index pp. The term with smallest valuation, at j=Jj=J, cannot cancel.

Choose NN beyond the poles and the zeros of the endpoint coefficients of LrL_r, and beyond the index from which all Ar,jA_{r,j} with j<mrj<m_r satisfy that recurrence. Its order mrm_r recurrence determines a solution on this tail from mrm_r consecutive values. The matrix

[Ar,j(N+i)]0≤i,j<mr\left[A_{r,j}(N+i)\right]_{0\leq i,j<m_r}

is nonsingular over Q\mathbb{Q}: otherwise a nonzero rational combination would have mrm_r consecutive zero values and would vanish on a tail, contradicting independence. Its inverse has rational entries. Thus the same sequences give both asserted bases.

For U=∑jcjAr,jU=\sum_j c_jA_{r,j}, cj∈Qc_j\in\mathbb{Q}, Theorem 5.1 gives L(U)=∑jcjϕr,jπ2jL(U)=\sum_j c_j\phi_{r,j}\pi^{2j}. The numbers ϕr,j\phi_{r,j} are nonzero rationals, and the powers 1,π2,…,π2mr−21,\pi^2,\ldots,\pi^{2m_r-2} are linearly independent over Q\mathbb{Q} by the transcendence of π\pi. This proves the isomorphism. □\square

Transferring annihilators

The shifted congruence supplies more than independence. It transfers an annihilator of any nonzero combination of the deformation coefficients to the undeformed sequence. The following proof treats complex constants directly.

Proposition 5.4. Fix r≥1r \ge1 and suppose, on a tail,

U=∑j=0JcjAr,j,cj∈C,cJ≠0.U = \sum_{j=0}^{J} c_j A_{r,j}, \qquad c_j \in\mathbb{C}, \quad c_J \ne0.

If Q=∑ℓ=0dqℓ(n)SℓQ = \sum_{\ell=0}^{d} q_\ell(n)S^\ell, qℓ∈C[n]q_\ell\in\mathbb{C}[n], annihilates UU eventually, then

∑ℓ=0dqℓ(b)Fr(b+ℓ)=0(b∈Z≥0).(20)\sum_{\ell=0}^{d} q_\ell(b)F_r(b+\ell)=0 \qquad(b \in\mathbb{Z}_{\ge0}). \tag*{(20)}

Every annihilator of UU in C(n)[S;σ]\mathbb{C}(n)[S;\sigma] therefore also annihilates FrF_r eventually.

Proof. The case Q=0Q=0 is immediate. Otherwise choose a Q\mathbb{Q}-basis β1,…,βt\beta_1,\ldots,\beta_t of the finite-dimensional Q\mathbb{Q}-vector space spanned by all products cj[nh]qℓ(n)c_j[n^h]q_\ell(n). Write

cjqℓ(n)=∑i=1tβiqi,j,ℓ(n),qi,j,ℓ∈Q[n].c_jq_\ell(n)=\sum_{i=1}^{t}\beta_i q_{i,j,\ell}(n), \qquad q_{i,j,\ell}\in\mathbb{Q}[n].

For every sufficiently large integer nn, the identity QU(n)=0QU(n)=0 becomes

∑i=1tβi(∑j=0J∑ℓ=0dqi,j,ℓ(n)Ar,j(n+ℓ))=0.\sum_{i=1}^{t}\beta_i\left(\sum_{j=0}^{J}\sum_{\ell=0}^{d}q_{i,j,\ell}(n)A_{r,j}(n+\ell)\right)=0.

Each parenthesized expression is rational. Independence of the βi\beta_i over Q\mathbb{Q} makes each expression zero separately.

Fix b≥0b\ge0. Evaluate these rational identities at n=p+bn=p+b, where p>b+dp>b+d is a sufficiently large prime avoiding all coefficient denominators. Multiply by p2Jp^{2J} and reduce modulo pp. By (19), the terms with j<Jj<J vanish, leaving

Cr,J∑ℓ=0dqi,J,ℓ(b)Fr(b+ℓ)≡0(modp).C_{r,J}\sum_{\ell=0}^{d}q_{i,J,\ell}(b)F_r(b+\ell)\equiv0 \pmod p.

Here qi,j,ℓ(p+b)≡qi,j,ℓ(b)(modp)q_{i,j,\ell}(p+b)\equiv q_{i,j,\ell}(b)\pmod p. The displayed rational number is independent of pp and is divisible by infinitely many primes, so it is zero. Multiplying by βi\beta_i and summing over ii, then canceling Cr,JcJ≠0C_{r,J}c_J\ne0, gives (20). For rational-function coefficients, first clear their polynomial denominators in nn, which preserves annihilation on a tail. □

Proof of Theorem 1.2. Suppose that Lr=BRL_r=BR in C(n)[S;σ]\mathbb{C}(n)[S;\sigma] with 0<ord⁡R<mr0<\operatorname{ord}R<m_r. The constant coefficient of RR is nonzero, because the constant coefficient of LrL_r is nonzero. Beyond the finitely many poles and endpoint zeros of RR, nonzero initial data give a nonzero solution germ UU of RR: forward and backward uniqueness prevent it from vanishing eventually. Then LrU=0L_rU=0, so Proposition 5.3 expresses UU as a nonzero complex combination of Ar,0,…,Ar,mr−1A_{r,0},\ldots,A_{r,m_r-1}. Proposition 5.4 gives RFr=0RF_r=0, contrary to the minimal order mrm_r. This proves irreducibility.

For any nonzero solution germ UU of LrL_r and any annihilator QQ of UU, Proposition 5.4 gives QFr=0QF_r=0. Right division by the monic operator LrL_r writes Q=HLr+RQ=HL_r+R with ord⁡R<mr\operatorname{ord}R<m_r; this is the usual division algorithm in the shift Ore ring [12]. Since RFr=0RF_r=0, minimality forces R=0R=0. Finally, a nonzero hypergeometric germ has an annihilator S−a(n)S-a(n) with a(n)∈C(n)a(n)\in\mathbb{C}(n), impossible when r≥3r\ge3 and $m_r\ge 2. □

The rate of convergence of solution ratios

The characteristic roots also give a uniform exponential rate for the limits. This concerns complex solutions as well as rational ones.

Corollary 5.5. For r≥3r \ge3 and every complex solution germ UU of LrL_r, the limit L(U)=lim⁡U(n)/Fr(n)\mathcal{L}(U) = \lim U(n)/F_r(n) exists and

lim sup⁡n→∞∣U(n)Fr(n)−L(U)∣1/n≤cos⁡r(πr).(21)\limsup_{n\to\infty}\left|\frac{U(n)}{F_r(n)}-\mathcal{L}(U)\right|^{1/n}\le\cos^r\left(\frac{\pi}{r}\right). \tag*{(21)}

For r=1,2r=1,2, every solution germ is a constant multiple of FrF_r.

Proof. After clearing denominators, divide a minimum-order recurrence by its coefficient of SmrS^{mr}. Theorem 1.1 shows that the resulting coefficients tend to those of HrH_r, and the trailing coefficient is nonzero on a sufficiently late tail. The roots λr,k\lambda_{r,k} are nonzero with distinct absolute values. Perron’s theorem [14], in the form stated in [4 §4], therefore gives a basis of solutions with successive ratios tending to λr,k\lambda_{r,k}. The elementary bounds

2rn(n+1)r−1≤Fr(n)≤2rn\frac{2^{rn}}{(n+1)^{r-1}}\le F_r(n)\le2^{rn}

show that Fr(n)1/n→2r=λr,0F_r(n)^{1/n}\to2^r=\lambda_{r,0}, so FrF_r has a nonzero component in the dominant basis direction. Subtracting the corresponding multiple of FrF_r from UU leaves only the other directions, whose largest exponential modulus is (2cos⁡(π/r))r(2\cos(\pi/r))^r. This proves (21). □

Denominators, diagonals and integer solutions

Exact denominator growth

For x∈Qx\in\mathbb{Q}, let den⁡(x)\operatorname{den}(x) be its positive denominator in lowest terms, with den⁡(0)=1\operatorname{den}(0)=1. Fix an initial index N0≥1N_0\ge1 from which the displayed basis expansion of the rational germ holds, and put

DU(N)=lcm⁡{den⁡(U(n)):N0≤n≤N}.(22)D_U(N)=\operatorname{lcm}\{\operatorname{den}(U(n)):N_0\le n\le N\}. \tag*{(22)}

Changing finitely many terms changes log⁡DU(N)\log D_U(N) by at most a constant for all sufficiently large NN, and hence does not affect its exponential growth rate. Write ψ(N)=log⁡ℓN=∑pα≤Nlog⁡p\psi(N)=\log\ell_N=\sum_{p^\alpha\le N}\log p.

Theorem 6.1. Let

U(n)=∑j=0JcjAr,j(n),cj∈Q,cJ≠0,U(n)=\sum_{j=0}^{J}c_jA_{r,j}(n),\qquad c_j\in\mathbb{Q},\quad c_J\ne0,

on the chosen tail. There are a finite set of primes SS and an integer B≥1B\ge1 such that

vp(U(pα))=−2Jα(p∉S, α≥1).(23)v_p(U(p^\alpha))=-2J\alpha\qquad(p\notin S,\ \alpha\ge1). \tag*{(23)}
vp(DU(N))=2J⌊log⁡pN⌋(p∉S, N≥N0).(24)v_p(D_U(N))=2J\lfloor\log_pN\rfloor\qquad(p\notin S,\ N\ge N_0). \tag*{(24)}

and

DU(N)∣BℓN2J,log⁡DU(N)=2Jψ(N)+OU,N0(log⁡N).(25)D_U(N)\mid B\ell_N^{2J},\qquad\log D_U(N)=2J\psi(N)+O_{U,N_0}(\log N). \tag*{(25)}

In particular,

lim⁡N→∞log⁡DU(N)N=2J.(26)\lim_{N\to\infty}\frac{\log D_U(N)}{N}=2J. \tag*{(26)}

Proof. Choose BB with Bcj∈ZBc_j\in\mathbb{Z} for every jj. By (17), Bℓn2JU(n)B\ell_n^{2J}U(n) is integral, which gives the divisibility in (25). Let SS contain all primes at most N0N_0, the divisors of BB and Cr,JC_{r,J}, and the prime divisors of the numerator of cJc_J in lowest terms. Outside this finite set, cJc_J is a unit and the other cjc_j are integral. At n=pαn=p^\alpha, the term with j=Jj=J has valuation exactly −2Jα-2J\alpha by (19); every lower term has strictly larger valuation. This proves (23).

For p∉Sp\notin S, the divisibility bound gives vp(DU(N))≤2J⌊log⁡pN⌋v_p(D_U(N))\le2J\lfloor\log_pN\rfloor. If p≤Np\le N, choose α=⌊log⁡pN⌋\alpha=\lfloor\log_pN\rfloor. Then N0<p≤pα≤NN_0<p\le p^\alpha\le N, so (23) gives the matching lower bound. If p>Np>N, both sides are zero. This proves (24). Only the fixed exceptional primes can contribute to log⁡DU(N)−2Jlog⁡ℓN\log D_U(N)-2J\log\ell_N, and each contributes O(log⁡N)O(\log N). Finally, the prime number theorem gives ψ(N)∼N\psi(N)\sim N. □`

For the solution space of LrL_r, Proposition 5.3 shows that the possible nonzero-solution rates in (26) are exactly 0,2,…,2mr−20,2,\ldots,2m_r-2. More precisely, the solutions with rate at most 2J2J form

span⁡Q{Ar,0,…,Ar,J},0≤J<mr.\operatorname{span}_{\mathbb{Q}}\{A_{r,0},\ldots,A_{r,J}\},\qquad0\le J<m_r.

Equivalently, write the Apéry limit uniquely as L(U)=PU(π2)\mathcal{L}(U)=P_U(\pi^2), where PU∈Q[X]P_U\in\mathbb{Q}[X] and deg⁡PU<mr\deg P_U<m_r. For every nonzero U∈VrU\in V_r,

lim⁡N→∞log⁡DU(N)N=2deg⁡PU.(27)\lim_{N\to\infty}\frac{\log D_U(N)}{N}=2\deg P_U. \tag*{(27)}

Indeed, (16) gives PU(X)=∑jcjϕr,jXjP_U(X)=\sum_j c_j\phi_{r,j}X^j, and each ϕr,j\phi_{r,j} is nonzero. Thus the arithmetic filtration agrees with the polynomial degree of the Apéry limit.

The globally bounded direction

Proof of the arithmetic assertions in Theorem 1.3. Write a nonzero rational solution in the basis of Proposition 5.3, and let JJ be its highest nonzero index. If J=0J=0, it is a rational multiple of FrF_r and has bounded denominators. If J>0J>0, equation (23) with α=1\alpha=1 shows that its denominator at index pp is divisible by p2Jp^{2J} for every sufficiently large prime pp. It therefore has neither bounded denominators nor a fixed finite set of denominator primes. It cannot be globally bounded, since for p∤BCp\nmid BC multiplication by BCpBC^p does not change this negative valuation.

Every diagonal of a rational function over Q\mathbb{Q} regular at the origin is globally bounded. For completeness, write that function as P(x)/Q(x)P(x)/Q(x) with integral polynomials and Q(0)=a≠0Q(0)=a\ne0. The series H=1−Q/aH=1-Q/a has zero constant term, and

PQ=Pa∑q≥0Hq.\frac{P}{Q}=\frac{P}{a}\sum_{q\ge0}H^q.

A monomial of total degree hh receives terms only from q≤hq\le h, so its coefficient has denominator dividing ah+1a^{h+1}. A diagonal in dd variables is consequently made integral by multiplying its nnth coefficient by a(ad)na(a^d)^n; absolute values may be used to make these scaling integers positive. A polynomial change affects only a finite common denominator. Hence a diagonal solution germ belongs to QFr\mathbb{Q}F_r. Conversely,

∑n≥0Fr(n)zn=Diag⁡1(1−x1)⋯(1−xr)−x1⋯xr.(28)\sum_{n\ge0}F_r(n)z^n=\operatorname{Diag}\frac{1}{(1-x_1)\cdots(1-x_r)-x_1\cdots x_r}. \tag*{(28)}

Indeed, geometric expansion gives ∑k≥0(x1⋯xr)k∏i(1−xi)−k−1\sum_{k\ge0}(x_1\cdots x_r)^k\prod_i(1-x_i)^{-k-1}, whose diagonal coefficient is ∑k=0n(nk)r\sum_{k=0}^n\binom{n}{k}^r. Rational multiples are again rational diagonals.

It remains to determine the integer lattice for r≥2r\ge2. For every N≥1N\ge1,

gcd⁡{Fr(n):n≥N}=2.(29)\gcd\{F_r(n):n\ge N\}=2. \tag*{(29)}

Pairing the summands with indices kk and n−kn-k shows that Fr(n)F_r(n) is even for n≥1n\ge1: when n=2hn=2h, the unpaired coefficient (2hh)=2(2h−1h−1)\binom{2h}{h}=2\binom{2h-1}{h-1} is also even. For every prime pp, all interior coefficients (pαk)r\binom{p^\alpha}{k}^r are divisible by pp. Thus Fr(pα)≡2(modp)F_r(p^\alpha)\equiv2\pmod p, excluding all odd primes from the gcd, and Fr(2α)≡2(mod4)F_r(2^\alpha)\equiv2\pmod4 because r≥2r\ge2. This proves (29). An integer-valued solution germ is already a rational multiple cFrcF_r; the gcd says exactly that the denominator of cc divides 22.

Theorem 1.3 has an equivalent interpretation for binomial sums. Bostan, Lairez and Salvy [3 Theorem 3.5] characterize univariate multiple binomial sums over Q\mathbb{Q} as diagonals of rational power series. Within their class, the solution germs of LrL_r are therefore exactly QFr\mathbb{Q}F_r. The secondary deformation solutions cannot be rewritten as multiple binomial sums in that class. This conclusion concerns rational functions and sums over Q\mathbb{Q}; these hypotheses specify the class of diagonals used here.

The classical integer-sequence question

The preceding theorem classifies eventual integer solutions for r≥2r \ge2. In the classical case r=3r = 3, a much shorter argument answers the question about entire integer sequences. This is the converse asked in [15 Conjecture 4.5], where the initial values were assumed positive, and in the conclusion of [18]. The Casoratian formula used in the proof is also present in [18 proof of Theorem 6].

Corollary 6.2. An integer sequence U(0),U(1),…U(0), U(1), \ldots satisfies

(n+1)2U(n+1)=(7n2+7n+2)U(n)+8n2U(n−1),n≥1,(30)(n+1)^2 U(n+1) = (7n^2 + 7n + 2)U(n) + 8n^2 U(n-1), \qquad n \ge1, \tag*{(30)}

if and only if U(n)=cF3(n)U(n) = cF_3(n) for some c∈Zc \in\mathbb{Z}. More generally, a rational solution of (30) with bounded denominators on a tail is a rational multiple of F3F_3 on the entire sequence.

Proof. The Casoratian Wn=F3(n)U(n+1)−F3(n+1)U(n)W_n = F_3(n)U(n+1) - F_3(n+1)U(n) satisfies

Wn=−8n2(n+1)2Wn−1=(−8)n(n+1)2(U(1)−2U(0)).W_n = -\frac{8n^2}{(n+1)^2}W_{n-1} = \frac{(-8)^n}{(n+1)^2}(U(1)-2U(0)).

If b=U(1)−2U(0)≠0b = U(1)-2U(0) \ne0, choose arbitrarily large odd primes dividing neither the numerator nor denominator of bb nor a common denominator for the tail of UU. At n=p−1n = p-1, the formula gives vp(Wn)=−2v_p(W_n) = -2, contradicting bounded denominators of WnW_n. Thus U(1)=2U(0)U(1) = 2U(0). The recurrence uniquely propagates these initial values, giving U=U(0)F3U = U(0)F_3. Integrality at n=0n = 0 forces U(0)∈ZU(0) \in\mathbb{Z}; the converse follows from the defining binomial sum. □

Further questions

The minimal orders and the leading characteristic polynomials leave several finer questions. Straub and Zudilin [17 Remark 4.1] record experimental formulas for the degree in nn of a primitive minimum-order Franel recurrence, and additional factorization patterns in its certificate. Appendix A settles the denominator and degree in the summation variable kk. The degree in nn and the possible factors depending only on nn require further arguments.

The analytic method applies more broadly to constant terms u(n)=CT⁡Pnu(n) = \operatorname{CT} P^n of real Laurent polynomials on a torus. To prove minimality, it is enough to exhibit sufficiently many distinct nonzero values at which the pushforward measure is not smooth and to construct a matching recurrence. Extrema of a common type give a direct noncancellation criterion. For symbols with saddle points or several types of critical points in the same fiber, the local contributions must be compared more carefully.

Related extensions of the Straub–Zudilin deformation to other binomial sums were studied by Dougherty-Bliss and Zeilberger [6]. The arithmetic method here requires a rational basis whose scaled reductions at p+bp+b all recover the same distinguished sequence at bb, with distinct scaling exponents. Establishing an analogous deformation and congruence for the alternating family would give information about its entire solution space. The moment argument alone determines its minimal order and characteristic roots, but does not supply that arithmetic structure.

The summation variable in a minimal certificate

We determine the kk-dependent denominator and numerator-degree patterns observed in Remark 4.1 of Straub and Zudilin [17]. It does not address possible denominator factors depending only on nn, the predicted degree in nn, or the further factorization patterns in that remark.

Every minimum-order recurrence is a scalar multiple over Q(n)\mathbb{Q}(n) of the telescoper constructed in Section 4: after normalizing the leading coefficients, the difference of two such operators would be an annihilator of smaller order. Hence every recurrence in the following proposition has a rational certificate.

Proposition A.1. Let r≥1r \ge1, m=⌊(r+1)/2⌋m = \lfloor(r + 1)/2 \rfloor, and let ∑j=0mpj(n)Sj\sum_{j=0}^{m} p_j(n)S^j be a minimal-order Franel recurrence, with pj∈Q[n]p_j \in\mathbb{Q}[n] and p0pm≠0p_0p_m \ne0. Its rational certificate C∈Q(n,k)C \in\mathbb{Q}(n,k) is characterized by

DC=∑j=0mpj(n)Qj(n,k),DC=(n−k)r(k+1)rC(n,k+1)−C(n,k),Qj=(n+1)jr(n−k+1)jr.DC = \sum_{j=0}^{m} p_j(n)Q_j(n,k), \qquad DC = \frac{(n-k)^r}{(k+1)^r} C(n,k+1) - C(n,k), \qquad Q_j = \frac{(n+1)_j^r}{(n-k+1)_j^r}.

Put K=Q(n)K = \mathbb{Q}(n) and Bm(k)=∏h=1m(n−k+h)rB_m(k) = \prod_{h=1}^{m}(n-k+h)^r. Then the reduced denominator of CC in K[k]K[k] is BmB_m, up to a unit of KK. Equivalently,

C(n,k)=A(n,k)Bm(k),A∈K[k],gcd⁡K[k](A,Bm)=1.C(n,k) = \frac{A(n,k)}{B_m(k)}, \qquad A \in K[k], \qquad\gcd_{K[k]}(A,B_m) = 1.

Moreover,

kr∣A(n,k),deg⁡kA=rm+1{r even}.k^r \mid A(n,k), \qquad\deg_k A = rm + 1_{\{r\ \mathrm{even}\}}.

For a fixed recurrence its rational certificate is unique.

Proof. Write T=∑jpjQjT = \sum_j p_jQ_j. Its only possible finite poles in kk are n+1,…,n+mn+1,\ldots,n+m, each of order at most rr. Work over an algebraic closure of KK and group the finitely many poles of CC into orbits under integer translation. In each occupied orbit choose a pole α\alpha for which none of α−1,α−2,…\alpha-1,\alpha-2,\ldots is a pole. At k=α−1k=\alpha-1, the function C(k+1)C(k+1) has a pole and C(k)C(k) is regular. The multiplier (n−k)r/(k+1)r(n-k)^r/(k+1)^r cannot remove this pole unless α−1=n\alpha-1=n; its pole at −1-1 only increases the order. Otherwise α−1\alpha-1 must be a pole of TT. Thus every occupied orbit is n+Zn+\mathbb{Z}, and its leftmost pole has the form n+hn+h with h≥1h \ge1. At the rightmost pole n+hn+h, the shifted term is regular, so TT has a pole there. Hence h≤mh \le m. Descending from this rightmost pole in DC=TDC=T shows that every pole of CC has order at most rr. Therefore BmC∈K[k]B_mC \in K[k].

There is no pole of CC at −1-1 or 00, and TT is regular at −1-1. The order-rr pole of the multiplier there forces C(k+1)C(k+1) to vanish to order at least rr. Hence kr∣BmCk^r \mid B_mC, since Bm(0)≠0B_m(0) \ne0 in KK.

It remains to show that no factor of BmB_m cancels. By Theorem 1.1,

deg⁡pm=D:=max⁡jdeg⁡pj.\deg p_m = D := \max_j \deg p_j.

For r=1r=1, the same equality follows directly from p0+2p1=0p_0+2p_1=0. For a sufficiently large nonnegative integer NN, interpret f(N,k)=(Nk)rf(N,k)=\binom{N}{k}^r by gamma-function continuation, as in the telescoping construction. The pole bounds just proved imply that b(N,k)=C(N,k)f(N,k)b(N,k)=C(N,k)f(N,k) is finite at every integer kk and has finite support there. Summing its forward difference from k=N+hk=N+h to infinity gives

b(N,N+h)=−∑j=hmpj(N)∑ℓ=0j−h(N+jℓ)r,1≤h≤m.(31)b(N,N+h)=-\sum_{j=h}^{m}p_j(N)\sum_{\ell=0}^{j-h}\binom{N+j}{\ell}^{r}, \qquad1 \le h \le m. \tag*{(31)}

The right side is a nonzero polynomial in NN: its j=mj=m summand has degree D+r(m−h)D+r(m-h), with leading coefficient −[nD]pm/((m−h)!)r-[n^D]p_m/((m-h)!)^r, whereas every j<mj<m summand has smaller degree. Since f(N,k)f(N,k) has a zero of exact order rr at k=N+hk=N+h, equation (A.1) is incompatible with a pole of order less than rr for CC at k=n+hk=n+h. This proves the exact denominator assertion.

Finally, let C=c(n)ka(1+O(k−1))C=c(n)k^a(1+O(k^{-1})) at infinity, where a∈Za \in\mathbb{Z} and c≠0c \ne0. Since Q0=1Q_0=1 and Qj=O(k−rj)Q_j=O(k^{-rj}) for j≥1j \ge1, one has T=p0+O(k−r)T=p_0+O(k^{-r}). Direct expansion gives

DC={−2c(n)ka(1+O(k−1)),r odd,c(n)(a−r(n+1))ka−1(1+O(k−1)),r even.DC = \begin{cases} -2c(n)k^a(1+O(k^{-1})), & r\ \mathrm{odd},\\ c(n)(a-r(n+1))k^{a-1}(1+O(k^{-1})), & r\ \mathrm{even}. \end{cases}

The displayed leading coefficients are nonzero in KK. It follows that a=0a=0 for odd rr and a=1a=1 for even rr, proving the numerator degree. The same expansion shows that ker⁡D=0\ker D=0 on K(k)K(k), which proves uniqueness of the rational certificate.

Remark A.2. The argument proves the same conclusion for any polynomial-coefficient telescoping relation of width mm satisfying p0pm≠0p_0p_m \ne0 and deg⁡pm=max⁡jdeg⁡pj\deg p_m=\max_j\deg p_j. Minimality is used only to supply this last degree equality. All denominator statements above are in K[k]K[k]; elements of K×K^\times are units and are not controlled by this proposition.

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