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Threshold-free reciprocal transfer at prime-power section orders

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4 Threshold-free reciprocal transfer at prime-power section orders

The completion of Nishibuchi's conjecture fixes the requested eventual congruence. The stronger question is whether the sufficient starting row can be removed, and how much precision the difference order and the step actually provide. This section answers the first question at every prime-power section order. Subsequent sections give a factorial improvement and exact results at section order four.

Throughout these sections, the normalized source and its reciprocal are

\[ G_{N,j}(t)=j!\sum_{n\geq0}\frac{t^{Nn}}{(Nn+j)!},\qquad F_{N,j}(t)=G_{N,j}(t)^{-1} =\sum_{n\geq0}C_{N,j}(n)\frac{t^{Nn}}{(Nn)!}, \]
(4.1)

where \(N\geq1\) and \(0\leq j<N\). In particular, \(C_{N,j}(0)=1\). The coefficients in the original convention satisfy

\[ E_{Nn}^{(N,j)}=j!C_{N,j}(n),\qquad E_d^{(N,j)}=0\quad(N\nmid d). \]
(4.2)

Thus every valuation of a nonzero difference gains \(v_p(j!)\) on returning to the original coefficients. This factor must be retained when stating optimal periods or the final congruence.

Write \(S f(n)=f(n+1)\) and \(\Delta_H=S^H-1\). A mixed difference \(\Delta_{H_1}\cdots\Delta_{H_k}\) acts on the row variable \(n\), rather than on the full Euler subscript. We use \(v_p(0)=+\infty\). Orders and starting rows are nonnegative integers; steps are positive integers unless stated otherwise. An empty mixed difference is the original value, and a zero ordinary step makes every nonempty product containing it zero.

4.1 The Hurwitz lattice and translated differential flatness

Definition 4.1: Hurwitz integral series

For a prime \(p\), let

\[ \mathcal H_p=\left\{\sum_{d\geq0}f_d\frac{t^d}{d!}: f_d\in\mathbb Z_p\right\} \subset\mathbb Q_p[[t]]. \]

For \(N=p^a\) and \(\lambda\in\mathbb Z_p\), put

\[ D=\frac{d}{dt},\qquad L_\lambda=\frac{D^N-\lambda}{p}. \]

A series \(A\) is \(\lambda\)-flat if \(L_\lambda^k A\in\mathcal H_p\) for every \(k\geq0\).

Products preserve \(\mathcal H_p\) because the coefficient at factorial degree \(d\) is

\[ (AB)_d=\sum_{i=0}^d\binom di a_i b_{d-i}. \]

The derivative \(D\) acts by the coefficient shift \((DA)_d=a_{d+1}\). Consequently every nonnegative power of \(D\) preserves the lattice. If \(A\in\mathcal H_p\) has unit constant term, its reciprocal belongs to the same lattice: with \(B=A^{-1}\),

\[ b_0=a_0^{-1},\qquad b_d=-a_0^{-1}\sum_{i=1}^d\binom di a_i b_{d-i}. \]
(4.3)

If \(A\) is supported at degrees divisible by \(N\), this recurrence also proves that \(B\) has the same support.

Lemma 4.2: Translated product formula

For \(N=p^a\), \(a\geq1\), and \(\lambda,\mu\in\mathbb Z_p\),

\[ L_{\lambda+\mu}(AB) =(L_\lambda A)B+A(L_\mu B) +\sum_{i=1}^{N-1}c_i(D^iA)(D^{N-i}B), \qquad c_i=\frac1p\binom Ni\in\mathbb Z. \]
(4.4)

Flatness types add under multiplication.

Proof of Lemma 4.2

The identity \((1+X)^{p^a}=1+X^{p^a}\) over \(\mathbb F_p\) shows that every interior binomial coefficient \(\binom Ni\) is divisible by \(p\). Subtract \((\lambda+\mu)AB\) from the ordinary \(N\)th derivative product formula and divide by \(p\) to obtain (4.4).

For completeness, the iterated formula is an integral multinomial formula, rather than a product rule with unspecified remainders. On the tensor of the two factors use the mutually commuting operators

\[ L_\lambda\otimes1,\quad 1\otimes L_\mu,\quad c_iD^i\otimes D^{N-i}\quad(1\leq i<N). \]

Applying multiplication after the \(k\)th power of their sum gives exactly \(L_{\lambda+\mu}^k(AB)\). Expanding it yields terms indexed by \(a,b,e_1,\ldots,e_{N-1}\geq0\), with \(a+b+\sum_i e_i=k\):

\[ \frac{k!}{a!b!\prod_i e_i!}\prod_i c_i^{e_i} (D^\alpha L_\lambda^a A)(D^\beta L_\mu^b B), \quad \alpha=\sum_i i e_i,\quad \beta=\sum_i(N-i)e_i. \]
(4.5)

Every scalar is integral. If \(A\) and \(B\) have the stated flatness types, both factors in every term belong to \(\mathcal H_p\), as does their product.

Lemma 4.3: Reciprocal transfer

If \(A\) is \(\lambda\)-flat and has unit constant term, then \(A^{-1}\) is \((-\lambda)\)-flat.

Proof of Lemma 4.3

Set \(B=A^{-1}\). Its order-zero integrality was established in (4.3). Assume by induction that \(L_{-\lambda}^bB\in\mathcal H_p\) for \(b<k\). Since \(AB=1\),

\[ L_0^k(AB)=\left(\frac{D^N}{p}\right)^k1=0\qquad(k>0). \]

Use (4.5) with \(\mu=-\lambda\). Exactly one term has inverse order \(b=k\): it has \(a=0\) and all \(e_i=0\), and is \(A L_{-\lambda}^k B\). In every other term \(b<k\), so its second factor is integral by induction and derivative-shift integrality. Its first factor is integral by the flatness of \(A\), and its scalar is integral. Hence \(A L_{-\lambda}^k B\in\mathcal H_p\). Multiplying by the already integral \(B\) proves \(L_{-\lambda}^k B\in\mathcal H_p\). This induction takes place in the entire Hurwitz lattice. It places no restriction on the coefficient degree or the starting row.

4.2 The actual Euler source

The packed factorial coefficient of \(G_{N,j}\) is

\[ g_{N,j}(n)=\frac{j!(Nn)!}{(Nn+j)!} =\prod_{i=1}^j\left(1+\frac Ni n\right)^{-1}. \]
(4.6)

The empty product is one. If \(N=p^a\) and \(1\leq i<N\), then \(v_p(i)<a\), so \(N/i\in p\mathbb Z_p\). Every affine denominator in (4.6) is therefore a unit on \(\mathbb Z_p\).

For \(s\in p\mathbb Z_p\), an exact finite-difference identity is

\[ \Delta_1^k\frac1{1+sn} =\frac{(-s)^k k!}{\prod_{h=0}^k(1+s(n+h))}. \]
(4.7)

It follows by induction, subtracting adjacent rational functions; each successive subtraction adds the factor \(-(k+1)s\) in the numerator. Its denominator is a unit, so it belongs to \(p^k\mathbb Z_p\). The discrete Leibniz formula

\[ \Delta_1^k(fg)(n) =\sum_{r=0}^k\binom kr (\Delta_1^r f)(n)(\Delta_1^{k-r}g)(n+r) \]
(4.8)

then proves \(\Delta_1^k g_{N,j}(n)\in p^k\mathbb Z_p\) for every \(k,n\). The coefficient at degree \(Nn\) of \(L_1^kG_{N,j}\) is precisely \(p^{-k}\Delta_1^k g_{N,j}(n)\), and the other residue classes vanish. Thus the actual source is \(1\)-flat.

Theorem 4.4: All-row prime-power transfer

Let \(p\) be prime, \(a\geq1\), \(N=p^a\), and \(0\leq j<N\). The coefficients \(C_{N,j}(n)\) belong to \(\mathbb Z_p\) for all \(n\geq0\). Set \(A_{N,j}(n)=(-1)^n C_{N,j}(n)\) and \(T_H=S^H-(-1)^H\). For \(k\geq1\) and positive \(H_1,\ldots,H_k\),

\[\begin{aligned} v_p(\Delta_{H_1}\cdots\Delta_{H_k}A_{N,j}(n)) &\geq k+\sum_{\nu=1}^k v_p(H_\nu), \\ v_p(T_{H_1}\cdots T_{H_k}E_{Nn}^{(N,j)}) &\geq v_p(j!)+k+\sum_{\nu=1}^k v_p(H_\nu). \end{aligned}\]
(4.9), (4.10)

At \(p=2\), the ordinary differences of \(C_{N,j}\) and of the original coefficients satisfy the same bounds. These dyadic statements also hold for \(N=1\).

Proof of Theorem 4.4

Reciprocal transfer gives \(L_{-1}^kF_{N,j}\in\mathcal H_p\). Extraction of the packed coefficient gives \((S+1)^k C_{N,j}(n)\in p^k\mathbb Z_p\). Moreover,

\[ \Delta_1^k A_{N,j}(n)=(-1)^{n+k}(S+1)^k C_{N,j}(n), \]

so \(A_{N,j}\) has the ordinary \(p^k\) difference property. At \(p=2\), \(L_1=L_{-1}-1\); its integral binomial expansion on \(F_{N,j}\) gives \(\Delta_1^k C_{N,j}(n)\in2^k\mathbb Z_2\) directly. For \(N=1\) the interior sum in the product formula is empty, so the same argument applies without change; equivalently, \(F_{1,0}(t)=e^{-t}\).

To retain the valuation of a step, let \(B\) be any sequence satisfying \(\Delta_1^m B\in p^m\mathbb Z_p\) at every order and row. Use the finite operator identity

\[ \Delta_H=\sum_{i=1}^H\binom Hi\Delta_1^i. \]

The relation \(i\binom Hi=H\binom{H-1}{i-1}\) implies

\[ v_p\left(p^i\binom Hi\right) \geq i+v_p(H)-v_p(i)\geq1+v_p(H). \]

Multiplying these identities for the \(k\) steps, every term of total order \(M\) has its scalar multiplied by \(p^M\), and is divisible by \(p^{k+\sum_\nu v_p(H_\nu)}\). This proves the mixed-step bound. Finally,

\[ \Delta_H A_{N,j}(n)=(-1)^{n+H}T_H C_{N,j}(n). \]

Iteration contributes only a global sign. Multiplying by \(j!\) proves (4.10).

Corollary 4.5: Threshold-free dyadic congruence

For \(N=2^a\), \(a\geq0\), all permitted \(j\), and \(n\geq0\),

\[ v_2(\Delta_{H_1}\cdots\Delta_{H_k}E_{Nn}^{(N,j)}) \geq v_2(j!)+k+\sum_{\nu=1}^k v_2(H_\nu). \]
(4.11)

In particular, \(\Delta_H^k\) gains \(k(1+v_2(H))\) bits before normalization. For \(r>v_2(j!)\), the row displacement \(H=2^{\max(0,r-v_2(j!)-1)}\) is a sufficient period modulo \(2^r\) from row zero. If \(r\leq v_2(j!)\), all original coefficients vanish modulo \(2^r\).

Remark 4.6: Necessary boundaries

At an odd prime the ordinary step-one difference cannot replace the sign-twisted operator in the general theorem. For \(j=0\), \(C_{N,0}(0)=1\) and \(C_{N,0}(1)=-1\), so their ordinary difference is \(-2\), a unit at every odd prime. The proof also does not extend unchanged to non-prime-power \(N\), whose interior binomial coefficients need not be divisible by the chosen prime. Neither observation is a counterexample to Nishibuchi's original eventual congruence.

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