Unity under arithmetic refinement

Unity remains fixed as arithmetic resolution increases. The collision measure assigns every address a share of one total; larger addresses receive smaller shares. The finite clock space determines which descriptions of that whole are available. Its residual records what those clocks have not represented.

A remainder clock records the fractional position of an integer within a fixed period. The first such clock has period two. Doubling its values gives one at every odd address and zero at every even address. It reproduces unity on one part of the integer sequence and leaves the other part unresolved. Admitting further periods gives more freedom to account for what remains. All earlier clocks remain available, and the carry and dilation identities relate descriptions at different resolutions.

A reading of that unresolved part becomes useful when it supplies a combination of new clocks that reduces the approximation error. Several readings may see the same direction. Adding their individual gains can then count the same improvement twice. The cost of their combined correction is its squared norm, with those overlaps retained. Two prescribed families below have costs bounded independently of the number of refinement levels. Their complete readings give explicit coefficients for an improving clock combination.

The primitive collision kernel in Conservation and Profinite Dynamics in Digit-Collision Energy and Finite Generation of Collision Capacity [6, 7] supplies a natural observation measure at the integer origin. Its reciprocal address weights include every row, giving the approximation a fixed meaning as the clock cutoff changes. Proposition 2 derives these weights from the unit mass.

Binary refinement gives a place to look. It places unity on one chain of orthogonal currents, and the normal equations force a definite amount of residual energy onto an initial part of that chain. A visible current need not itself be a combination of admitted clocks. Making its reading admissible introduces a coarse component, which can cancel the visible detail. The response identities retain that cancellation and the part of the fit already made.

The distinction is between locating unresolved energy and capturing it with a permitted correction. The location theorem and the uniform cost bounds hold at every cutoff. They give a finite improvement whenever a complete reading survives. The final open problem asks whether enough of these improvements must accumulate through an unbounded sequence of refinements.

Use the real Hilbert space \mathcal H=\ell^2(\mathbb N,\omega),\qquad \omega_m=\frac1{m(m+1)},\qquad \phi_j(m)=\{m/j\}. Let V_N=\operatorname{span}(\phi_2,\ldots,\phi_N), let P_N be its orthogonal projection in the complete infinite norm, and put p_N=P_N\mathbf{1},\qquad r_N=\mathbf{1}-p_N. D_N=\|r_N\|^2=\langle r_N,\mathbf{1}\rangle,\qquad \mathcal C_N=D_N^{-1}. The space, clocks and constant target in (1) are the discrete Nyman–Beurling–Báez-Duarte approximation setting described by Bagchi [1]. In this setting, D_N\to0 is equivalent to the Riemann hypothesis. Conditioning primitive collision mass gives another route to these same weights. The question pursued here concerns specified finite observations, their admissible corrections and the gain they can certify within that established approximation problem.

We call \mathcal C_N the native approximation capacity. It measures recovery of unity in the conditioned collision norm. It is distinct from the aggregate affine collision capacity, which sums a prescribed family of rows before squaring. Both arise from the collision structure; their definitions and gains are different. The binary lift T copies a parent value to addresses 2m and 2m+1 and is zero at address one. Set U=\sqrt2\,T and d_1=\sqrt2\,\delta_1, where \delta_m is the point mass at m. The paired native weights determine this normalization. All depth indices are nonnegative integers.

The shallow horizon and eligible depths are fixed by H_N=\left\lceil\log_2(4/D_N)\right\rceil,\qquad M_h=\lfloor N/2^h\rfloor. I_N=\{h\in\mathbb Z:0\le h<H_N,\ M_h\ge2\}. Prescribe the detector family by g_M=(P_{4M}-P_M)d_1,\qquad w_{N,h}=(I-P_N)U^hg_{M_h}. Its response and complete cost are b_{N,h}=\langle r_N,w_{N,h}\rangle,\qquad K_{N,hk}=\langle w_{N,h},w_{N,k}\rangle. The joint capture is J_N=b_N^T K_N^\dagger b_N. Here K^\dagger denotes the Moore–Penrose inverse. The joint quotient computes projection onto the prescribed detector space.

Theorem 10 proves the forcing statement, Proposition 3 gives the capture certificate, and Theorem 14 proves the cost bounds. The horizon is intrinsic to the actual error. A shallow level is used by the prescribed family only when its clock cutoff is admissible.

The cost bound has a direct constructive consequence. With the exact readings, set \widetilde p_N=p_N+\frac12\sum_{h\in I_N}b_{N,h}w_{N,h}\in V_{4N}. Proposition 5, with C=2 and zero observation error, gives D_N-D_{4N}\ge D_N-\|\mathbf{1}-\widetilde p_N\|^2 \ge\frac12\sum_{h\in I_N}|b_{N,h}|^2. Thus any nonzero reading supplies an improvement, with the overlap between depths charged in the same bound. The right side depends on the complete signed readings; the forced spine energy cannot be substituted for it.

Orthogonal projection, generalized inverses and the Wold decomposition are classical [4, 5]. The shallow forcing argument uses the residual’s norm and mean; the finite correction rule is a general Hilbert-space estimate. The arithmetic content lies in the selected detectors and their complete clock responses. In particular, Proposition 13 exhibits exact cancellation of visible detail by a coarse component, and Theorem 17 retains the old fit in every descendant reading. For copied masks, a classical geometric Gram estimate supplies the upper cost; the arithmetic pattern determines the reading. The finite calculations in Section 9 illustrate these symbolic results.

Digit-ending closures supply the second family. Their geometry has three named operations. Palindromic reflection reverses the last two digits within an ending block. Torsional readings follow changes between neighboring residue spokes. A radial increment advances to the next address on the same spoke. Sections 13 and 14 define these operations and their weighted energies. The names describe the arithmetic geometry; telescoping and the weighted mean–difference identity give their elementary accounting.

Projection into a new clock band makes the polarity readings admissible. Their family is distinct from (4), whose definition and cost bound remain fixed. Proposition 5 uses either bound to turn the measured response into an improving clock combination. The update needs no inverse of the detector Gram and allows uncertainty in the readings. Constructing the band projections still uses the native clock geometry.

Collision measure and the native approximation

The unity slice

On ordered coprime positive pairs define \mathscr K(a,b)=\frac1{2ab(a+b)}.

The probability kernel and the period-weighted mass are different. For example, direct subtraction gives \mathscr K(a,b)-\mathscr K(a,a+b)-\mathscr K(a+b,b) =\frac3{2(a+b)(2a+b)(a+2b)}>0. Equation (1) is the native unity slice of collision mass. Its address weights differ from uniform Haar weights on a residue group. They also have a direct interval interpretation. The reciprocal intervals I_m=(1/(m+1),1/m] partition (0,1] and have length \omega_m. Assigning the value F(m) on I_m is an isometric embedding of \mathcal H into L^2(0,1). In particular \sum_{m\ge L}\omega_m=1/L. Large addresses occupy short intervals, while the full norm continues to account for all of them.

Normal equations and error increments

The clocks are linearly independent. Indeed, with \phi_j(0)=0, \phi_j(m)-\phi_j(m-1)=\frac1j-\mathbf{1}_{j\mid m}. If a finite clock combination vanishes, evaluate its difference first at m=1 and then successively at m=2,\ldots,N to recover every coefficient as zero. A finite combination is periodic and vanishes at common multiples of its clock periods, so it cannot equal \mathbf{1}. Consequently 0<D_N\le1 and the finite Gram matrix is positive definite.

The classical lower bound.

The reciprocal-interval embedding \mathcal I, extended by zero on (1,\infty), sends unity to \chi_{(0,1]} and satisfies \mathcal I\phi_j(x)=\{1/(jx)\}-j^{-1}\{1/x\}. Indeed, if 1/x=m+\theta with 0\le\theta<1, the two fractional parts on the right have the same \theta/j term. Let \mathcal B_\lambda be the span in L^2(0,\infty) of \{\vartheta/x\} for \lambda\le\vartheta\le1, and let d(\lambda) be the distance from \chi_{(0,1]} to that space. Since \mathcal IV_N\subset\mathcal B_{1/N}, Burnol’s theorem [2] gives D_N\ge d(1/N)^2,\qquad \liminf_{N\to\infty}D_N\log N \ge\sum_{\rho}\frac{m_\rho^2}{|\rho|^2}>0. The sum is over distinct nontrivial zeta zeros, with multiplicities m_\rho. The conclusion is unconditional; if RH fails, the limiting distance is positive and the left side is infinite. Thus D_N\ge c/\log N for all sufficiently large N, and \mathcal C_N=O(\log N). This constrains how fast the optimized error can disappear. It supplies neither convergence nor a lower bound for a selected reading.

The next estimate is a general consequence of a Gram ceiling. It supplies a correction rule once the arithmetic has supplied admissible readings.

With exact readings, the coefficients are simply b_i/C and the guaranteed gain is \|b\|_2^2/C. The proposition also gives a stopping rule for numerical observation. A reading norm no larger than its error allowance cannot certify a positive update through this bound. The joint error allowance and the proved cost bound determine how far the update can move. Correlated readings are charged together, so their overlap cannot inflate the certified gain.

Carry resolution and admitted refinement

A remainder can be read to increasing digit depth without admitting a new clock. These two operations have different effects. Carry resolution reduces the error in describing a fixed row. Admitted refinement enlarges the space in which unity is approximated.

For a signed combination v=\sum_{j=2}^M\alpha_j\phi_j, resolve row j with a word product B_j and put \varepsilon=\sum_j|\alpha_j|/B_j. The observation weights sum to one, so (18) gives \|\widetilde v-v\|\le\varepsilon,\qquad \big|\|\widetilde v\|^2-\|v\|^2\big| \le2\|v\|\varepsilon+\varepsilon^2. The first assertion follows from a uniform pointwise bound; the second expands \|v+(\widetilde v-v)\|^2. Thus every fixed signed energy can be resolved with a controlled error in the complete norm. The resolved vector need not belong to the original clock space. This estimate does not itself improve its approximation to unity.

To describe admitted refinement, extend a sequence by zero at zero and define, for an integer b\ge2, (T_bf)(n)=f(\lfloor n/b\rfloor),\qquad e_b=\mathbf{1}_{\{1,\ldots,b-1\}}.

For F,G\in\mathcal H, put \eta=G-TF. Expanding the square and using (20) with b=2 gives \|G\|^2=\tfrac12\|F\|^2+\|\eta\|^2+2\langle TF,\eta\rangle. The last two terms are the signed source work. Refinement retains the source square and its interaction with the copy. Halving the copied energy does not estimate their sum.

The transported old fit and the new optimum give a useful energy account without discarding their interaction.

The baseline in (23) is essential. A positive transported energy need not give an improvement of comparable size. Carry reconstruction can evaluate that energy more accurately; the signed excess over its baseline is a different quantity.

The dyadic current tree

Specialize to T=T_2, so (Tf)(1)=0,\qquad (Tf)(2m)=(Tf)(2m+1)=f(m),\qquad U=\sqrt2T. The paired weights satisfy \omega_{2m}+\omega_{2m+1}=\omega_m/2. Therefore U^*U=I, and (U^*F)(m)= \frac{(m+1)F(2m)+mF(2m+1)}{\sqrt2(2m+1)}. Write Q=I-UU^*. For odd q\ge3, put d_q=\frac{(q+1)\delta_q-(q-1)\delta_{q-1}}{\sqrt2}, \qquad d_1=\sqrt2\delta_1. For q\ge3 the vectors have unit norm, disjoint pair supports, and weighted mean zero in each pair. Together with d_1, they form an orthonormal basis of Q\mathcal H.

The coordinates read the boundary current through \langle F,d_q\rangle=\frac{F(q)-F(q-1)}{\sqrt2\,q}\quad(q\ge3\text{ odd}). For s=2^h the exact pullback is ((U^*)^hF)(m)= \sqrt{s}\,m(m+1) \sum_{n=sm}^{s(m+1)-1}\frac{F(n)}{n(n+1)}. Repeated pullback expresses the same current through weighted blocks. The affine denominators record their boundaries. At the next level, the current reads the difference of the normalized neighboring blocks.

Unity forces shallow spine energy

Directly, Q\mathbf{1}=\delta_1 and U^*\mathbf{1}=2^{-1/2}\mathbf{1}. More explicitly, U^hd_1 equals 2^{(h+1)/2} on [2^h,2^{h+1})\cap\mathbb N and is zero elsewhere. Hence \boxed{\mathbf{1}=\sum_{h\ge0}s_hU^hd_1,\qquad s_h=2^{-(h+1)/2}.} Unity has no transverse coordinate q>1. Its spine is the closed span of the U^hd_1.

The theorem forces D_N^2-scale energy correlated with unity onto the shallow spine. The full residual has energy D_N. The intrinsic horizon satisfies 4/D_N\le2^{H_N}<8/D_N. No estimate relating D_N to N is used here. For h<H_N, M_h>ND_N/4-1. Thus ND_N\ge8 is a sufficient condition for every shallow depth to be eligible. All subsequent detector statements retain the definition of I_N whether or not this condition holds.

Visible detail and canceled admissible readings

The odd-divisor shifts approximate the root in the wandering space. Their admissible lifts show how visible detail can be canceled by a coarse response. For odd j set R_jd_q=d_{jq} and define z=\sum_{q\ {\rm odd}}\frac{d_q}{\sqrt2q},\qquad \kappa=\frac{\pi^2}{16},\qquad A_M^{\rm ar}=\sum_{\substack{m\le M\\m\ {\rm odd}}} \frac{\mu(m)^2}{J_2(m)}, where \mu is the Möbius function and J_2(m)=m^2\prod_{p\mid m}(1-p^{-2}). For odd j\le M put a_j=\frac{j}{A_M^{\rm ar}} \sum_{\substack{m\le M,\ m\ {\rm odd}\\j\mid m}} \frac{\mu(m/j)\mu(m)}{J_2(m)},\qquad q_M=\sqrt2\sum_{j\le M,\ j\ {\rm odd}}a_jR_jz.

The affine collision covariance therefore gives the transverse arithmetic form at each depth, with the displayed normalization. Transfer between depths is governed by the moving clock projection. The covariance identity does not identify native dilation with translation on the profinite completion.

For L\ge N, H=H_N and M_h=\lfloor L/2^h\rfloor\ge2 at every 0\le h<H, set d_h^{\rm read}=\langle r_N,U^h q_{M_h}\rangle and c_h=c_{h,1}(r_N). Write M_{\min}=\min_{0\le h<H}M_h. The errors U^h(q_{M_h}-d_1) are mutually orthogonal and perpendicular to the full unity spine. The projection of r_N onto that spine has energy at least D_N^2, since \langle r_N,\mathbf{1}\rangle=D_N and \|\mathbf{1}\|=1. Bessel’s inequality therefore yields \|d^{\rm read}-c\|_2^2 \le\frac{\zeta(2)}{M_{\min}}D_N(1-D_N). Thus M_{\min}\ge16\zeta(2)/D_N implies \|d^{\rm read}\|_2\ge D_N/4.

The exact lift identity is U^h\phi_j=\sqrt{s}\,(\phi_{sj}-j^{-1}\phi_s), \qquad s=2^h,\qquad\phi_1=0. It follows by writing each address as sm+r, 0\le r<s. For L=4N, all lifts U^hF_{M_h} are therefore admissible in V_{4N}. The sufficient visibility conditions can be written entirely in the native variables, ND_N\ge2,\qquad ND_N^2\ge32\zeta(2). Indeed M_{\min}>ND_N-1\ge ND_N/2 under the first condition, and the second then gives M_{\min}\ge16\zeta(2)/D_N. The detail part remains only one component of the lift.

The lift F_M exhibits cancellation within the admitted clock space. We retain (4) as the prescribed new-clock family.

Admissible detectors with uniformly bounded cost

The new-clock family removes the part of each probe already represented by the old clock space. What remains is available for an actual correction. Its reading still contains the terminal contribution omitted by a spine-only observation. By (41), w_{N,h}\in V_{4N}\cap V_N^\perp for each eligible depth. Also f_h=(U^*)^hr_N\perp V_{M_h}, so b_{N,h}=\langle f_h,g_{M_h}\rangle =c_{h,1}(r_N)-\tau_{N,h},\qquad \tau_{N,h}=\langle f_h,(I-P_{4M_h})d_1\rangle. The tail remains in the signed response. Proposition 3 gives J_N\le D_N-D_{4N}.

When the cost trace vanishes, that fact leaves recovery of unity unresolved. The estimate uses convergence of the root projection, which does not determine the limit of D_N.

The joint Gram retains the cross terms between readings. Adding individual gains would lose them. Equation (46) also allows a single surviving depth to furnish the lower bound.

Logarithmic conditioning and transported response

The native moments are \mu_j=\langle \mathbf{1},\phi_j\rangle=\frac{\log j}{j},\qquad \sigma_j=\langle d_1,\phi_j\rangle=\frac1{\sqrt2j},\qquad \mu=\sqrt2 L\sigma. For the first identity, summation by parts with (11) reduces the cutoff sum to j^{-1}(\mathsf H_K-\mathsf H_{\lfloor K/j\rfloor}) and a vanishing endpoint. The second is the origin coordinate. Here L is diagonal with entries \log j.

The complete clock Gram is explicit. For \ell=\operatorname{lcm}(i,j) and \Psi=\Gamma'/\Gamma, G_{ij}=\frac1{ij\ell}\sum_{r=1}^{\ell}(r\bmod i)(r\bmod j) \left[\Psi\!\left(\frac{r+1}{\ell}\right)- \Psi\!\left(\frac r\ell\right)\right]. The bracket divided by \ell equals the full residue weight \sum_{t\ge0}1/[(r+t\ell)(r+t\ell+1)]. The residue sum therefore includes the full infinite observation tail.

Let \Phi_N\alpha=\sum_{j=2}^N\alpha_j\phi_j be clock synthesis. With a_N=G_N^{-1}\mu_N, the actual squared error is D_N=1-\mu_N^Ta_N. For arbitrary raw columns F_h, set v_h=\Phi_N^*F_h. Their conditioned Gram and residual response are \langle F_h,F_k\rangle-v_h^TG_N^{-1}v_k,\qquad \langle \mathbf{1},F_h\rangle-a_N^Tv_h. Taking F_h=U^hg_{M_h} recovers (5) with every signed cross term retained. The finite interval calculations in Section 9, performed with nfield [12], evaluate the rational digamma arguments with controlled analytic remainder [8] and enclose the positive Gram solves.

At a coarse cutoff M, partition the clocks through 4M into O=\{2,\ldots,M\} and B=\{M+1,\ldots,4M\}. Let G_{ij}=\langle \phi_i,\phi_j\rangle and set \begin{aligned} A_M&=G_{BO}G_O^{-1},& S_M&=G_{BB}-G_{BO}G_O^{-1}G_{OB},\\ v_M&=\sigma_B-A_M\sigma_O,& u_M&=\mu_B-A_M\mu_O,\\ C_M&=L_BA_M-A_ML_O. \end{aligned} The Schur complement S_M is positive definite by clock independence.

In (56), conditioning changes the logarithmic relation through C_M. Descent also transports the admitted approximation, contributing \mathfrak t_{N,h}. Replacing that descendant by a newly optimized r_M would change the source.

Nor does positive definiteness force \mathfrak m_M to be positive by algebra alone. For example, W=\begin{pmatrix}1&-3/4\\-3/4&9/16+1/100\end{pmatrix},\quad L=(\log2)\operatorname{diag}(1,2),\quad v=(1,1)^T has \det W=1/100>0 but (Lv)^TWv=-21\log2/200<0. This matrix refutes a positivity inference from positive definiteness alone. It is not a native Schur inverse.

Finite response illustrations

The following calculations illustrate the response identity and gain bounds. They were performed with nfield [12]; the uniform theorems above follow from their symbolic proofs. Five cutoffs N=25,35,42,48,89 were separately enclosed with 192-bit ball arithmetic and independently regenerated complete analytic Grams. At N=25,h=1, with s=2 and M=12, the enclosures give the signs shown below.

The sum of the first two terms is positive, whereas the actual response is negative. The transported old fit changes the sign at this cutoff. The displayed decimals abbreviate interval enclosures; the sign comparison is a finite computation.

The prescribed panel consists of N=25,\ldots,400,\quad512,\quad800,\quad969,\quad1388,\quad1600. It has 381 cutoffs, 2675 eligible depth rows, and 19211 ordered joint Gram entries. Complete native Grams were evaluated before projection; the infinite observation space was not truncated. Floating joint capture ranged from 89.19\% to 99.19\% of the actual N to 4N error decrease.

At the first cutoff, the interval calculation gives D_{25}-D_{100}\ge J_{25}>19D_{25}^2. The larger panel uses floating arithmetic. The added logarithmic splits reproduced the original depth, summary and full Gram outputs without changing the detectors. Their maximum floating discrepancies were 1.78\times10^{-16} for the native split and 3.67\times10^{-15} after lifting.

The calculations in nfield [12] also include 147620 exact integer or rational checks of the spine, detail and transfer identities and 113633 checks of the cutoff, cost and commutator identities. These finite checks supplement the proofs. They do not establish the uniform lower constant in Problem 24.

The moving projection and the limits of conservation

Let \mathcal W be the unitary Wold coordinate map, let \mathsf S be the forward depth shift, and let \Phi_L synthesize clocks through L. Let e_{0,1} denote the unit vector at depth zero and odd address one. In those coordinates the actual clock projection is \mathcal P_L=\mathcal A_LG_L^{-1}\mathcal A_L^*,\qquad \mathcal A_L=\mathcal W\Phi_L. The exact residual recurrence is \boxed{\mathcal Wr_{2N}=(I-\mathcal P_{2N}) \left(2^{-1/2}\mathsf S\mathcal Wr_N+ 2^{-1/2}e_{0,1}\right).} Indeed \mathbf{1}=T\mathbf{1}+\delta_1 and TV_N\subset V_{2N} by (41), so r_{2N}=(I-P_{2N})(Tr_N+\delta_1). Conjugation gives (61). Raw pullback shifts depth; the moving projection uses the full clock columns and couples depth to the transverse odd-address coordinates. There is no uniform finite bandwidth even for a fixed small clock space. Indeed P_2d_1=(\sqrt2/\log2)\phi_2, whose root coordinate is positive at every depth. A depth-zero input therefore acquires arbitrarily deep coordinates in one projection.

The terminal current cancels the head

Put \psi=2\delta_1-\mathbf{1} and \rho=2^{-1/2}. Its spine coefficients and generating function are p_0=\rho,\quad p_j=-\rho^{j+1}\ (j\ge1),\qquad P(z)=\rho\,\frac{1-\sqrt2z}{1-\rho z}. For the lower triangular H by H convolution matrix P_H, the inverse coefficients are \sqrt2 at zero and 2^{(j-1)/2} at j\ge1. Its first column and its Frobenius norm give 2^{H-1}+1\le\|P_H^{-1}\|^2\le2^H+H-1. For F\in\mathcal H and c_h=\langle F,U^hd_1\rangle the full readings satisfy (\langle F,U^h\psi\rangle)_{h<H} =P_H^Tc_{<H}-v_Ht_H,\qquad (v_H)_h=\rho^{-h},\quad t_H=\sum_{k\ge H}\rho^{k+1}c_k. This follows by splitting \rho c_h-\sum_{j\ge1}\rho^{j+1}c_{h+j} at H. For F=\mathbf{1}, every reading is zero, although c_h=\rho^{h+1} and t_H=2^{-H}. The terminal column exactly cancels the head. In fact ((P_H^T)^{-1}v_H)_h=2^H\rho^{h+1}. The inverse cost in (62) leaves this terminal response uncontrolled.

Root visibility and admissibility

For any finite L, e=(I-P_L)d_1 is nonzero, since d_1 is not a periodic finite clock combination. It is orthogonal to every clock through L, yet \langle e,d_1\rangle=\|e\|^2>0. A statement for arbitrary Hilbert vectors cannot infer admissible visibility just from a nonzero root coordinate. Proposition 13 gives the stronger old-clock cancellation statement for the actual residual.

There is also a conditional obstruction within the actual optimizer sequence. Let V_\infty=\overline{\bigcup_NV_N}, let P_\infty be its orthogonal projection, and set D_\infty=\lim_ND_N. Suppose D_\infty>0. Nested projections then give r_N\to r_\infty=(I-P_\infty)\mathbf{1} in norm. Equation (41) puts U^hg_M in V_\infty. Since \|g_M\|\le1, |b_{N,h}|\le\|r_N-r_\infty\|\longrightarrow0. If D_\infty>0, the number of eligible depths stays bounded, so their readings vanish jointly while Theorem 10 retains positive shallow energy. This is consistent with the normal equations and with the cost theorem. It is not an assertion that D_\infty>0 occurs. The missing arithmetic theorem must exclude precisely such persistent signed cancellation.

Transport of the same admissible probe

Fourfold refinement admits a direct comparison without selecting new detector coefficients. An eligible probe at depth h and cutoff N has the same coarse source as the probe at depth h+2 and cutoff 4N. Conditioning changes, but the source is held fixed.

Since H_{4N}\ge H_N, all eligible old depths h<H_N-2 have a paired successor. The last two shallow depths require explicit boundary bookkeeping; no new depth is admitted to avoid that boundary. Equation (65) places the change in reading in the signed optimizer drift. A block estimate must control that drift together with the boundary readings. Their costs descend by (67); a lower bound on their combined response is still required.

The optimal cost of copied signed masks

Copying an observation to finer scales creates a family of readings that may overlap. The useful estimate bounds the cost of the whole family independently of how many copies are made. It applies to any signed indicator pattern, using the native dilation of Proposition 7 and the identity |f|=|f|^2 for a mask with values in \{-1,0,1\}. Digit endings will supply one such family.

The extremal Gram is the Kac–Murdock–Szegő matrix [\rho^{|k-l|}], a classical covariance form [3]. The calculation above includes its norm argument and identifies a native mask attaining the limiting bound. It does not assert that each particular mask, or its projection onto a clock band, has norm C_q.

For three fourfold copies of unity, the Gram and the equal-coefficient cost are already explicit: \begin{pmatrix} 1&1/2&1/4\\1/2&1&1/2\\1/4&1/2&1 \end{pmatrix}, \qquad \frac{\|h_0+h_1+h_2\|^2}{3}=\frac{11}{6}. The ratio tends to three as more copies are admitted. Other scale ratios give \begin{array}{c|cccc} q&2&4&9&16\\ C_q&3+2\sqrt2&3&2&5/3. \end{array} Larger separation reduces this universal cost by reducing overlap between copies. It also omits intermediate scales; the table supplies no claim of improved capture.

For r prescribed masks with these normalizations, Cauchy–Schwarz across the r families gives the common bound rC_q. Projection of every vector into the same admissible band can only decrease its synthesis norm. Proposition 5 therefore gives a finite improvement of at least (\|\widehat b\|_2-\varepsilon)_+^2/(rC_q) from uncertain readings. The arithmetic patterns determine the readings, while the copying theorem supplies their cost.

Palindromic blocks and carry polarity

Digit endings give signed masks whose changes are tied to carry resets. Their signs depend on the whole integer prefix as well as the final two digits. Retaining that prefix keeps the observation aligned with successive ending blocks.

Fix an integer base b\ge2 and write n=b^2h+bu+v, where 0\le u,v<b and h is the whole integer prefix. At fixed prefix and ending sum t=u+v, the complete ending block is \{b^2h+t+(b-1)u:\ \max(0,t-b+1)\le u\le\min(b-1,t)\}. Reversing the last two digits reverses this block. We call this its palindromic reflection. The block is symmetric under digit reversal; its individual addresses need not be palindromic numbers. Its reflection constant is 2b^2h+(b+1)t. The spoke of an address is its residue modulo b-1, namely h+t\pmod{b-1}. Consecutive addresses move between neighboring spokes, and an advance of b-1 returns to the same spoke at a new address. The polarity retaining this prefix is \begin{split} \varsigma_b(n)&=(-1)^{\lfloor(h+u+v)/(b-1)\rfloor}\\ &=(-1)^{\lfloor n/(b-1)\rfloor-\lfloor n/b\rfloor-\lfloor n/b^2\rfloor}. \end{split} Indeed n=(b-1)((b+1)h+u)+(h+u+v) proves the floor identity. On canonical spoke r, the number of preceding blocks at prefix h is 2h+\lfloor(h+b-2-r)/(b-1)\rfloor. Adding the within-prefix ordinal \lfloor t/(b-1)\rfloor gives the parity in (70). Successive complete blocks therefore alternate. The canonical spokes are the b-1 residue classes. Their seam advances to the next address on the first spoke; it does not repeat the starting address. The shifts b^2(b-1) and 2b^2(b-1) reverse and restore the polarity; in decimal they are 900 and 1800.

Define the clock bits by \vartheta_j(n)=2\phi_{2j}(n)-\phi_j(n) =\lfloor n/j\rfloor-2\lfloor n/(2j)\rfloor\in\{0,1\}, \qquad \phi_1=0. Then \varsigma_b=(1-2\vartheta_{b-1})(1-2\vartheta_b) (1-2\vartheta_{b^2}). With x=\vartheta_{b-1}, y=\vartheta_b and z=\vartheta_{b^2}, the pair and triple interactions combine into the binary carry c_b=xy+xz+yz-2xyz =\left\lfloor\frac{x+y+z}{2}\right\rfloor =\mathbf{1}_{\{x+y+z\ge2\}}. Checking the four possible values of x+y+z proves this identity. Consequently \begin{split} \varsigma_b&=1-2(x+y+z)+4c_b,\\ \langle r_N,\varsigma_b\rangle&=D_N+4\langle r_N,c_b\rangle\qquad(N\ge2b^2). \end{split} The second equality is the actual normal equation. A positive carry does not impose a sign on its pairing with the residual.

This estimate does not force D_N to vanish. Since \varsigma_b(n)=1 for n<b-1, the polarity itself approaches unity in the native norm as the base grows. Its reading can approach D_N while that error remains positive.

Palindromic pair energy

For observations u,v at reflected addresses, their palindromic pair energy is the complete weighted sum on the left below. The standard weighted mean–difference identity separates its shared mean from its disagreement. For p,q>0, pu^2+qv^2=\frac{(pu+qv)^2}{p+q} +\frac{pq}{p+q}(u-v)^2. Here the native choices of p,q are the weights of the two addresses. They are generally unequal even though the ending block is symmetric. Let R reverse the last two decimal digits, and let M be a positive multiple of 100. If v is supported on n\ge M and v(Rn)=-v(n), then |\langle \mathbf{1},v\rangle|\le81M^{-3/2}\|v\|. For a pair n\le m=Rn, its displacement is at most 81, and |\omega_n-\omega_m|/(\omega_n+\omega_m)\le(m-n)/n\le81/M. Cauchy–Schwarz over the pairs, with \sum_{n\ge M}\omega_n=1/M, proves (78). The complementary weighted means in (77) remain.

Torsional readings and radial energy

Use the native dilation T_a of Proposition 7, with T_1=I and zero extension at address zero. In this section put a_k=a_0\,4^k. Polarization and the clock identity give \langle T_af,T_ag\rangle=a^{-1}\langle f,g\rangle,\qquad T_a\vartheta_j=\vartheta_{aj}. The copied carry c_{a,b}=T_ac_b therefore satisfies \|c_{a,b}\|^2=\frac{m_b}{a}\le\frac1{ab}, \qquad m_b=\|c_b\|^2>0. Here c_b vanishes before b, and is nonzero at b for b\ge3 and at 3 for b=2. Once the two shorter bits are admitted, \begin{gathered} (I-P_N)T_a\eta_b=-2(I-P_N)c_{a,b},\\ \|(I-P_N)c_{a,b}\|^2\le\frac{B_b}{4a}\qquad(N\ge2ab). \end{gathered} Thus carry and disagreement yield the same conditioned direction; they must not be counted as independent probes.

The normalized carries \xi_k=\sqrt{a_kb}\,c_{a_k,b} also have the exact interaction law \langle \xi_k,\xi_l\rangle =b\,2^{l-k}\langle c_b,T_{4^{l-k}}c_b\rangle\qquad(l\ge k). This follows from T_aT_d=T_{ad} and (79). It depends only on scale separation; (68) applies with B=1/b.

Neighboring spokes and the advancing seam

For decimal polarity define the nine torsional readings \psi_s(n)=\frac{\varsigma_{10}(n+s+1)-\varsigma_{10}(n+s)}2, \qquad 0\le s\le8. Each reading is half the signed polarity change between neighboring spokes. After nine address steps, the spoke is the same and the address has advanced by nine. This gives the radial increment along that spoke. Telescoping yields 2\sum_{s=0}^8\psi_s(n)=\varsigma_{10}(n+9)-\varsigma_{10}(n). This identity holds for any sequence in place of the polarity. The specific arithmetic lies in which carry boundaries cause the signed changes. Figure 1 shows the address path without identifying its two endpoints.

Write \Delta_{\rm rad}(n) for the right-hand side of (85). Define the torsional energy of these readings and the radial energy of their total by \begin{split} E_{\rm tor}&=\sum_{s=0}^8\|\psi_s\|^2,\\ E_{\rm rad}&=\|\Delta_{\rm rad}\|^2 =4\sum_{s,t=0}^8\langle \psi_s,\psi_t\rangle. \end{split} Both use the complete native norm. Radial energy retains the interactions between torsional readings; it is not an additional orthogonal portion of their energy. The radial direction is already in their span.

In every base the signed reset formula is \begin{split} \epsilon_b(m)&= (\mathbf{1}_{b-1\mid m}+\mathbf{1}_{b\mid m}+\mathbf{1}_{b^2\mid m})\bmod2,\\ \varsigma_b(m)-\varsigma_b(m-1)&=-2\varsigma_b(m-1)\epsilon_b(m). \end{split} Thus \psi_s takes values in \{-1,0,1\}; a product of two readings keeps both reset indicators and their signs.

The choice B_s=1 is valid. The same theorem applies to address indicators, so it does not favor polarity masks. It is an upper cost bound, not a lower detection bound. If \psi_s^{\rm per} is the period-1800 extension of (84), the zero extension used by dilation gives T_a\psi_s(n)=\psi_s^{\rm per}(\lfloor n/a\rfloor) -\psi_s^{\rm per}(0)\mathbf{1}_{\{1\le n<a\}}. Only s=8 has \psi_s^{\rm per}(0)\ne0. This initial correction belongs to the complete vector.

Directional clock interactions and capture

To use a mask for recovery, take the part that the newly admitted clocks can express. Computing that projection requires the complete weighted overlap of the mask with each clock. Initial boundaries and unfinished periods contribute to that overlap.

For a bounded periodic probe f with period P, put L=\operatorname{lcm}(P,j). Its complete native clock pairing is \langle f,\phi_j\rangle=\sum_{r=1}^Lf(r)\frac{r\bmod j}{j}\Omega_{L,r}, \qquad \Omega_{L,r}=\sum_{t\ge0}\frac1{(tL+r)(tL+r+1)}. Absolute convergence justifies grouping, and (49) evaluates the residue masses. Copied masks use period 1800a and the finite subtraction in (91).

Finite intervals also retain unfinished cycles. If g is L-periodic, set \bar g=L^{-1}\sum_{n=1}^Lg(n) and A(t)=\sum_{n=1}^t(g(n)-\bar g)=A(t\bmod L). For integer endpoints 1\le u\le v, summation by parts gives \begin{split} \sum_{n=u}^v w_ng(n) ={}&\bar g\sum_{n=u}^v w_n+w_vA(v)-w_uA(u-1)\\ &+\sum_{n=u}^{v-1}(w_n-w_{n+1})A(n). \end{split} The cutoff residues and moving weights remain together. For N<p\le2N prime and 2\le d\le2N, d\ne p, one has \operatorname{lcm}(p,d)=pd>2N. There is no completed common period through address 2N for this pair; its unfinished overlap cannot be replaced by a completed-period mean.

For a finite selection of the normalized masks, put \begin{gathered} v_i=(P_M-P_N)h_i,\qquad d_i=\langle r_N,v_i\rangle,\\ \mathsf K_{ij}=\langle v_i,v_j\rangle,\qquad \mathcal J_{N,M}=d^T\mathsf K^\dagger d. \end{gathered} This is a second detector family; it does not redefine the fixed J_N in (6).

The exact middle quantity must be retained. If v=\varepsilon u with \|u\|=1 and \varepsilon\ne0, then |\langle r_N,v\rangle|^2/\|v\|^2=|\langle r_N,u\rangle|^2 even as the raw reading tends to zero. The Schur construction in (50) implements these corrections. For a raw probe f, let h_j=\langle f,\phi_j\rangle. On the chosen old and new index sets, t=h_B-G_{BO}G_{OO}^{-1}h_O gives coefficients S^{-1}t in the conditioned new clocks. The response is u^TS^{-1}t and its cost is t^TS^{-1}t. No product probe has been added as a free clock.

Finite directional controls

The reported calculations use double precision and the complete native Gram. Entries are percentages of the available gain D_N-D_M captured by the projected nine masks, the address indicators \delta_1,\ldots,\delta_9, and their joint span. Every probe uses the same band projection P_M-P_N.

At the last band, the masks reduce the error from 0.010201919284 to 0.009383196948, while the full optimum is 0.008930777788. The address probes are projected into the same clock band using the complete norm; the observation space is not restricted to nine addresses. The joint span has up to eighteen directions.

These are floating diagnostics without interval certification. They concern the unscaled masks, not the multiscale family of Corollary 21. The equal-dimension comparison favors the address probes at each tested band. Adding the masks after them contributes only 0.1333 percentage points on the last band. Neither a favorable gain fraction nor bounded cost proves that the remaining error tends to zero.

Signed capture across scales

A bounded cost turns measured responses into usable gains at each cutoff. Recovery of unity depends on their accumulation. The remaining question is whether the prescribed shallow readings can stay too small relative to their full costs through an unbounded sequence of refinements.

Fix an integer N_*\ge2 and set N_k=N_*4^k. The following implication expresses cumulative recovery entirely in native approximation variables.

A concrete sufficient rate is described by F(N)=(1+\log N)[1+\log(1+\log N)].

This lower bound remains open. On the fixed fourfold chain, the series \sum_k1/F(N_k) diverges by comparison with \sum_{k\ge2}1/(k\log k). The rate is one choice of a divergent budget; no particular logarithmic rate is necessary in Theorem 23. The problem concerns the prescribed detector family. Its affirmative resolution would imply the Riemann hypothesis through the classical approximation criterion [1]. The divergence criterion and the finite cost bounds do not assert that this particular rate holds.

With \mathcal T_N>0, a stronger sufficient response estimate is \sum_{h\in I_N}|b_{N,h}|^2\ge\frac{a\mathcal T_N D_N^2}{F(N)}. Here each b_{N,h} retains all three terms of (56). Corollary 15 proves the implication to (99). The raw costs remain in the denominator even when they decrease. The full joint quotient may give a larger gain than this scalar estimate. A single depth may suffice, or the response may survive only when several depths are read together.

A further sufficient relaxation permits recovery over adjacent scales. For a fixed integer L\ge1, it is enough to prove \sum_{j=k}^{k+L-1}\frac{J_{N_j}}{D_{N_j}^2} \ge\frac{a}{(k+1)\log(k+2)} at all sufficiently large k=k_0,k_0+L,k_0+2L,\ldots. The disjoint block series diverges. This condition is also open and retains every within-step cross term.

Fractions of the remaining error

The preceding reciprocal budget and a multiplicative ledger give two ways to account for admissible gain. The latter also applies to the directional family, with no requirement that each band contribute a fixed share.

The proposition applies to \Gamma_j=\mathcal J_{N_j,N_{j+1}} for any chosen finite selection of the copied masks. For a detector subfamily this is a sufficient condition only. For L=1 and \Gamma_j=J_{N_j}, its premise implies the reciprocal-budget premise in (98), since 0<D_N\le1. The fractional formulation does not strengthen that earlier convergence criterion. When \Gamma_j is the entire band gain, the product is exact and divergence of the fractional sum is also necessary. Indeed a finite sum makes \gamma_j\to0, and eventually -\log(1-\gamma_j)\le2\gamma_j, so the product stays positive.

The uniform cost bound (90) supplies no divergence in (102). Quiet bands are permitted, but the actual signed readings must still give a divergent fractional budget. The unresolved task concerns this response, with the original weights, initial boundary and all later addresses retained.

Complete energy under refinement

The capture criteria ask whether the residual produces enough admissible gain. The copy identity from Section 3 leads to a complementary approach. Prescribe the clock coefficients arithmetically, follow their signed response under refinement, and bound the energy of that response. This uses the same clocks and observation norm. The coefficients are fixed by a divisor identity, so the packet energy and the optimized error D_N require separate estimates.

The construction below first reproduces unity on an expanding prefix. Combining its copies leaves a fixed boundary and a packet supported beyond that prefix. We bound the packet in the complete observation norm, then determine how much stronger that bound would need to be to force recovery.

Coefficients, copying and the boundary

Let \mu be the Möbius function, characterized by \sum_{d\mid n}\mu(d)=\mathbf{1}_{n=1}, and put A(m)=\sum_{j\le m}\frac{\mu(j)}j,\qquad M(m)=\sum_{j\le m}\mu(j),\qquad A(0)=0. For an integer s\ge2, set \begin{aligned} \tau_s(j)&=\min\{1,\max\{0,(2s-j)/s\}\},\\ \beta_{s,j}&=-j[\tau_s(j)A(j)-\tau_s(j-1)A(j-1)] \quad(2\le j\le2s), \end{aligned} with all other coefficients zero. Define F_s=\sum_{j=2}^{2s}\beta_{s,j}\phi_j,\qquad \varepsilon_s(n)=F_s(n)-1\ (n\ge1),\qquad\varepsilon_s(0)=0. Telescoping gives \sum_j\beta_{s,j}/j=1. For 2\le j\le s, \beta_{s,j}=-\mu(j), and the divisor identity gives \sum_{j\le n}\mu(j)\lfloor n/j\rfloor=1. Hence F_s(n)=1\quad(1\le n\le s),\qquad F_s(0)=0. Using the copy operator T from Section 3, put a_t=3T\varepsilon_{2t}-2T^2\varepsilon_t-\varepsilon_{4t}, \qquad E_t=\|a_t\|^2\qquad(t\ge2). The finite clock combination \pi_t=3TF_{2t}-2T^2F_t-F_{4t} belongs to V_{8t}. The exact prefixes above show \pi_t=b+a_t,\qquad b=-\delta_1+2\delta_2+2\delta_3,\qquad a_t(n)=0\quad(n\le4t). All these sequences have zero extension at address zero. In particular, the fixed boundary has not been discarded from the clock identity.

The whole observation norm

Define the infinite arithmetic envelope and its transfer by \begin{aligned} d_s&=\sup_{m\ge s}\max\{|A(m)|,|M(m)|/m\},\\ \alpha_s&=d_s(1+\log(1/d_s)),\qquad U_s=54s\alpha_s^{4/3}+9\alpha_s^{2/3}. \end{aligned} The floor identity gives |A(m)|\le1, and |M(m)|\le m, so 0<d_s\le1. The supremum covers every later integer.

The growth still needed

The complete norm is now controlled. To determine whether that control can force recovery, we use the fixed boundary in (104). A hypothetical zeta zero to the right of the critical line would pair nontrivially with that boundary, forcing the packet energy to grow at a positive power rate. The following implication makes this comparison precise.

Condition (110) remains open. The bound in Proposition 26 does not imply it: along a doubling chain, its logarithm still has a term of order k.

Signed capture under continued refinement

Refinement changes the admitted descriptions of unity while retaining the complete observation measure. The prescribed readings have joint cost at most two, independently of the number of eligible levels. Equation (9) turns their complete signed response into an improvement from N to 4N, retaining the old fit and every overlap.

The shallow-spine theorem locates unresolved energy within a finite initial range of resolutions. Making that energy admissible introduces a terminal pairing that can cancel it. The response identity keeps that pairing, including the transported approximation. Visibility and capture remain distinct.

Copied signed masks have optimal universal cost (\sqrt q+1)/(\sqrt q-1) at scale ratio q. Palindromic blocks supply one arithmetic family, with every cross term retained in the radial energy. Projection into a common clock band preserves the cost bound. The finite comparisons favor simpler address probes in the tested bands; the geometry alone supplies no general capture advantage.

The prescribed packet gives a second way to use the same clocks. Proposition 26 bounds its complete energy, including the mean and infinite observation tail. For every fixed B>0, E_t\le C_B\frac{t}{(\log t)^B}\qquad(t\ge2). Here C_B may depend on the fixed B. Packet energy E_t, optimized error D_N and selected detector gain J_N are different quantities. This estimate and Burnol’s lower bound (12) do not squeeze one quantity to zero.

The packet route needs growth slower than every positive power along one fixed doubling chain (Proposition 27). Bound (111) still permits t^\alpha for 0<\alpha<1. A quantitative comparison with J_N also remains open. Complete-energy upper bounds are established; the remaining problem is a sufficient packet growth rate or accumulation of signed capture.

For the detector family, the needed accumulation is expressed on a fixed fourfold chain. Divergence of the normalized capture sum in (98) forces the unresolved error to vanish. Problem 24 gives one sufficient rate, while (101) permits weak scales followed by stronger ones. The proved construction locates energy and bounds the cost of reading it. Whether the prescribed signed readings must capture enough through continued refinement is the open arithmetic problem.

References