The modulo-2 Hankel transform of 1−x+x2/r(x2)1-x+x^2/r(x^2)

At least 4 years old · documented by

Let r(x)r(x) be the generating function of the Rueppel sequence, and let the Hankel transform be reduced termwise modulo 22. Modulo-2 periodicity conjecture. The Hankel transform of the sequence with generating function 1−x+x2/r(x2)1-x+x^2/r(x^2), taken modulo 22, yields the periodic sequence with period

1,0,1,1,1,1,0,1‾.\overline{1,0,1,1,1,1,0,1}.

The conjecture follows observed initial terms in the paper's comparison of Rueppel and Catalan analogs; no proof or resolution is supplied.

References

Primary source

Paul Barry, “Conjectures and results on some generalized Rueppel sequences”, arXiv:2107.00442 (2021).

Progress summary

Refreshed
Claimed solved

A reader-written proof claims to establish the conjectured period-eight pattern, but no independent verification has been found.

Paul Barry’s 2021 paper poses the conjecture that the Hankel transform modulo 22 of the sequence generated by 1−x+x2/r(x2)1-x+x^2/r(x^2) is periodic with pattern 1,0,1,1,1,1,0,1‾\overline{1,0,1,1,1,1,0,1}. The paper bases this on computed initial terms and gives no proof.

Known results

  • Barry (2021): recorded the period-eight pattern as Conjecture 11, without a resolution.

August 2026 community proof claim

A submission dated August 25, 2026 claims a proof for all n≥0n\geq0. Its visible argument reduces the Rueppel series modulo 22 to Catalan generating-function identities and proposes an auxiliary determinant evaluation leading to the stated residue classes n≡1,6(mod8)n\equiv1,6\pmod 8 for zeros and n≡0,2,3,4,5,7(mod8)n\equiv0,2,3,4,5,7\pmod 8 for ones. The proof is unverified.

Current status (as of August 2026): the conjecture remains unverified; a dated community submission claims a complete proof, while the published source still records only the conjecture.

Sources

Solutions 1

ProofThis solution needs a summarySee full solutionHide full solution

Proof of the period-eight Rueppel Hankel conjecture

Let

r(x)=∑j≥0x2j−1,F(x)=1−x+x2r(x2)=∑j≥0fjxj,r(x)=\sum_{j\geq 0}x^{2^j-1}, \qquad F(x)=1-x+\frac{x^2}{r(x^2)} =\sum_{j\geq0}f_jx^j,

and write

hn=det⁡(fi+j)0≤i,j≤n.h_n=\det(f_{i+j})_{0\leq i,j\leq n}.

We prove, for every n≥0n\geq0, that

hn≡{0(mod2),n≡1,6(mod8),1(mod2),n≡0,2,3,4,5,7(mod8).(1)\boxed{ h_n\equiv \begin{cases} 0\pmod 2,&n\equiv1,6\pmod8,\\ 1\pmod 2,&n\equiv0,2,3,4,5,7\pmod8. \end{cases}} \tag{1}

This establishes Conjecture 11 of Paul Barry, Conjectures and results on some generalized Rueppel sequences.

Reduction to Catalan moments

Let

C(x)=∑j≥0Cjxj,Cj=1j+1(2jj),C(x)=\sum_{j\geq0}C_jx^j, \qquad C_j=\frac1{j+1}\binom{2j}{j},

be the Catalan generating function. Its defining identity is

C(x)=1+xC(x)2.(2)C(x)=1+xC(x)^2. \tag{2}

On the other hand,

r(x)=1+xr(x2).(3)r(x)=1+xr(x^2). \tag{3}

Over F2[[x]]\mathbb F_2[[x]], Frobenius gives r(x2)=r(x)2r(x^2)=r(x)^2. Thus (2) and (3), together with their common constant coefficient, imply

r(x)≡C(x)(mod2).(4)r(x)\equiv C(x)\pmod2. \tag{4}

Because both series have constant coefficient 11, inversion preserves this congruence. Consequently FF is coefficientwise congruent to the integral series

F~(x)=1−x+x2C(x2).(5)\widetilde F(x) =1-x+\frac{x^2}{C(x^2)}. \tag{5}

By (2),

Q(x)=1C(x)=1−xC(x)=∑j≥0qjxj,(6)Q(x)=\frac1{C(x)}=1-xC(x)=\sum_{j\geq0}q_jx^j, \tag{6}

so

q0=1,qj=−Cj−1(j≥1).(7)q_0=1, \qquad q_j=-C_{j-1}\quad(j\geq1). \tag{7}

It therefore suffices to evaluate the Hankel determinants of

F~(x)=1−x+x2Q(x2)(8)\widetilde F(x)=1-x+x^2Q(x^2) \tag{8}

over the integers and then reduce the result modulo 22.

An auxiliary Catalan determinant

For k≥1k\geq1, let AkA_k be the size-kk Hankel determinant of

1+xQ(x)=1+x−x2C(x).1+xQ(x)=1+x-x^2C(x).

We claim that

Ak=(−1)k−1(1+∑j=1k−1j2).(9)A_k=(-1)^{k-1} \left(1+\sum_{j=1}^{k-1}j^2\right). \tag{9}

To see this, put m=k−1m=k-1 and introduce the Catalan moment matrix

Mm=(Ci+j)0≤i,j<m.M_m=(C_{i+j})_{0\leq i,j<m}.

Its standard ballot-triangle factorization is

Mm=LmLmT,Lm=(ℓi,j)0≤i,j<m,ℓi,j=(2ii−j)−(2ii−j−1)(0≤j≤i).(10)M_m=L_mL_m^{\mathsf T}, \qquad L_m=(\ell_{i,j})_{0\leq i,j<m}, \qquad \ell_{i,j} =\binom{2i}{i-j}-\binom{2i}{i-j-1} \quad(0\leq j\leq i). \tag{10}

Here out-of-range binomial coefficients are zero, and LmL_m is unit lower triangular. Define

v=(1,−C0,−C1,…,−Cm−2)T,zj=(−1)j(j+1).(11)v=(1,-C_0,-C_1,\ldots,-C_{m-2})^{\mathsf T}, \qquad z_j=(-1)^j(j+1). \tag{11}

The ballot generating function

∑i≥jℓi,jxi=xjC(x)2j+1(12)\sum_{i\geq j}\ell_{i,j}x^i =x^jC(x)^{2j+1} \tag{12}

shows that

∑i≥0(∑j=0i(−1)j(j+1)[(2ii−j)−(2ii−j−1)])xi=C(x)(1+xC(x)2)2=1C(x)=1−xC(x).(13)\begin{aligned} \sum_{i\geq0} \left(\sum_{j=0}^{i} (-1)^j(j+1) \left[ \binom{2i}{i-j}-\binom{2i}{i-j-1} \right] \right)x^i &=\frac{C(x)}{(1+xC(x)^2)^2}\\ &=\frac1{C(x)}\\ &=1-xC(x). \end{aligned} \tag{13}

Hence Lmz=vL_mz=v. The Hankel matrix defining AkA_k has the block form

(1vTv−Mm).\begin{pmatrix} 1&v^{\mathsf T}\\ v&-M_m \end{pmatrix}.

Since det⁡Mm=1\det M_m=1, its Schur complement gives

Ak=(−1)m(1+vTMm−1v)=(−1)m(1+zTz)=(−1)m(1+∑j=1mj2),\begin{aligned} A_k &=(-1)^m\left(1+v^{\mathsf T}M_m^{-1}v\right)\\ &=(-1)^m\left(1+z^{\mathsf T}z\right)\\ &=(-1)^m\left(1+\sum_{j=1}^{m}j^2\right), \end{aligned}

which proves (9).

The usual shifted Catalan Hankel evaluations are

det⁡(Ci+j)0≤i,j<t=det⁡(Ci+j+1)0≤i,j<t=1,det⁡(Ci+j+2)0≤i,j<t=t+1.(14)\det(C_{i+j})_{0\leq i,j<t} =\det(C_{i+j+1})_{0\leq i,j<t}=1, \qquad \det(C_{i+j+2})_{0\leq i,j<t}=t+1. \tag{14}

The first two identities follow from their respective unit ballot-triangle factorizations; the third follows from the first two by the Desnanot--Jacobi determinant identity.

For any series P(x)=∑j≥0pjxjP(x)=\sum_{j\geq0}p_jx^j with p0=1p_0=1 and reciprocal P(x)−1=∑j≥0bjxjP(x)^{-1}=\sum_{j\geq0}b_jx^j, formal-series inversion gives

det⁡(bi+j)0≤i,j<t=(−1)t−1det⁡(pi+j+2)0≤i,j<t−1.(15)\det(b_{i+j})_{0\leq i,j<t} =(-1)^{t-1} \det(p_{i+j+2})_{0\leq i,j<t-1}. \tag{15}

Applying this to P=CP=C, equations (7), (14), and (15) yield

Bt:=det⁡(qi+j)0≤i,j<t=(−1)t−1t,Dt:=det⁡(qi+j+1)0≤i,j<t=(−1)t,Et:=det⁡(qi+j+2)0≤i,j<t=(−1)t.(16)\begin{aligned} B_t &:=\det(q_{i+j})_{0\leq i,j<t} =(-1)^{t-1}t,\\ D_t &:=\det(q_{i+j+1})_{0\leq i,j<t} =(-1)^t,\\ E_t &:=\det(q_{i+j+2})_{0\leq i,j<t} =(-1)^t. \end{aligned} \tag{16}

Every determinant of size zero is understood to be 11.

The complete determinant evaluation

Let

H~N=det⁡(f~i+j)0≤i,j<N,F~(x)=∑j≥0f~jxj.\widetilde H_N =\det(\widetilde f_{i+j})_{0\leq i,j<N}, \qquad \widetilde F(x)=\sum_{j\geq0}\widetilde f_jx^j.

By (8),

f~0=1,f~1=−1,f~2j+2=qj,f~2j+3=0.(17)\widetilde f_0=1, \qquad \widetilde f_1=-1, \qquad \widetilde f_{2j+2}=q_j, \qquad \widetilde f_{2j+3}=0. \tag{17}

Reorder both rows and columns by even and odd indices. For

e=⌈N2⌉,o=⌊N2⌋,e=\left\lceil\frac N2\right\rceil, \qquad o=\left\lfloor\frac N2\right\rfloor,

the even-even block is the size-ee matrix defining AeA_e, the odd-odd block is the size-oo matrix defining BoB_o, and both off-diagonal blocks have their only nonzero entry, −1-1, in the upper-left corner. Expansion in these two entries gives

H~N=AeBo−De−1Eo−1(N≥2).(18)\widetilde H_N=A_eB_o-D_{e-1}E_{o-1} \qquad(N\geq2). \tag{18}

Substitution from (9) and (16) yields the stronger exact formulas

H~2m=m(1+∑j=1m−1j2)−1,H~2m+1=1−m(1+∑j=1mj2)(m≥1),(19)\boxed{ \begin{aligned} \widetilde H_{2m} &=m\left(1+\sum_{j=1}^{m-1}j^2\right)-1,\\ \widetilde H_{2m+1} &=1-m\left(1+\sum_{j=1}^{m}j^2\right) \end{aligned} \qquad(m\geq1),} \tag{19}

together with H~1=1\widetilde H_1=1.

Since j2≡j(mod2)j^2\equiv j\pmod2, we have

∑j=1tj2≡⌈t2⌉(mod2).(20)\sum_{j=1}^{t}j^2\equiv \left\lceil\frac t2\right\rceil \pmod2. \tag{20}

Equations (19)--(20) now show that, by matrix size NN, the determinant parities are

(H~N mod 2)N≥1=1,0,1,1,1,1,0,1‾.(21)(\widetilde H_N\bmod2)_{N\geq1} =\overline{1,0,1,1,1,1,0,1}. \tag{21}

Finally, (4)--(5) give

hn≡H~n+1(mod2),h_n\equiv\widetilde H_{n+1}\pmod2,

so (21) proves the asserted period-eight pattern (1) for every index.