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Only irrational anchored necessity has independently reviewed local proof coverage on this page: bounded discrepancy for [0,b)[0,b), 0<b<10<b<1, forces b={jξ}b=\{j\xi\}. The review and distinct passing grade concern the historical reconstruction pinned in the verification record below. The present source-prose and standing corrections are mapped documentary changes, not a fresh mathematical review of later bytes. The arbitrary-translate/Bohl reduction, rational rotations and already accepted Ostrowski sufficiency proof are outside that review. The full published statement remains below.

Statement and source

Harry Kesten, On a conjecture of Erdős and Szüsz related to uniform distribution mod 1, Acta Arithmetica 12 (1966), 193–212, Theorem 4 on printed p. 193 (the right-hand leaf of PDF sheet 1). The selected journal header gives 1966; the “1966/67” form found in some citations is a bibliographic variant.

For ξ∈[0,1]\xi\in[0,1], 0≤a<b≤10\le a<b\le1, and b−a<1b-a<1, put

N(M,ξ,a,b)=#{m:1≤m≤M, a≤{mξ}<b},R(M,ξ,a,b)=N(M,ξ,a,b)−M(b−a).N(M,\xi,a,b)=\#\{m:1\le m\le M,\ a\le\{m\xi\}<b\}, \qquad R(M,\xi,a,b)=N(M,\xi,a,b)-M(b-a).

For fixed ξ,a,b\xi,a,b, Theorem 4 states that R(M,ξ,a,b)R(M,\xi,a,b) is bounded as MM ranges over the positive integers if and only if

b−a={jξ}for some j∈Z.b-a=\{j\xi\}\qquad\text{for some }j\in\mathbb Z.

The source includes rational ξ\xi (its footnote calls that case trivial). The application to E0998 concerns irrational α\alpha, with ξ={α}\xi=\{\alpha\}. This theorem constrains the length, not the separate endpoints, and permits every non-wrapping translate [a,b)⊆[0,1][a,b)\subseteq[0,1] of the given proper length.

Exact elementary transfers

For 0<ℓ<10<\ell<1, the condition ℓ={jα}\ell=\{j\alpha\} is equivalent to ℓ∈Zα+Z\ell\in\mathbb Z\alpha+\mathbb Z. One implication follows from {jα}=jα−⌊jα⌋\{j\alpha\}=j\alpha-\lfloor j\alpha\rfloor. Conversely, if ℓ=jα+k\ell=j\alpha+k with integers j,kj,k and 0<ℓ<10<\ell<1, then the unique representative of jαj\alpha modulo 11 in [0,1)[0,1) is ℓ\ell. For irrational α\alpha, the integer jj here is nonzero.

The full interval [0,1)[0,1), omitted by the theorem's strict length restriction, has N(M)=MN(M)=M and R(M)=0R(M)=0. Its length 11 belongs to Zα+Z\mathbb Z\alpha+\mathbb Z, but is never a fractional part. It must be treated separately when the theorem is restated using group membership. An empty interval similarly has identically zero discrepancy and lies outside the displayed hypothesis a<ba<b.

The imported problem asks for a uniform bound for all sufficiently large nn. Such a bound is equivalent to boundedness for all positive nn: if ∣R(n)∣≤C|R(n)|\le C for n≥n0n\ge n_0, replace CC by the maximum of CC and the finitely many values ∣R(1)∣,…,∣R(n0−1)∣|R(1)|,\ldots,|R(n_0-1)|. The reverse implication is immediate. Thus there is no eventual-versus-all-indices gap in applying the theorem.

For irrational α\alpha, if both endpoints are orbit points and 0<b−a<10<b-a<1, subtracting their two representations shows b−a∈Zα+Zb-a\in\mathbb Z\alpha+\mathbb Z. This proves that the endpoint condition is sufficient. Necessity for the endpoints does not follow.

Anchored necessity: selected subdirection

The proof below reconstructs only the following proper subdirection of Theorem 4. For irrational 0<ξ<10<\xi<1 and fixed 0<b<10<b<1, if

R(M)=#{1≤k≤M:{kξ}<b}−MbR(M)=\#\{1\le k\le M:\{k\xi\}<b\}-Mb

is bounded for all positive integers MM, then b={jξ}b=\{j\xi\} for some j∈Zj\in\mathbb Z. Braces denote fractional parts in [0,1)[0,1).

This author-recorded reconstruction has independently reviewed proof coverage for exactly this selected direction, with the historical subject and subsequent documentary mapping recorded below. It excludes arbitrary starting endpoints, the Bohl reduction cited on p. 205, rational rotations, and the already reconstructed Ostrowski sufficiency direction. The full translated Theorem 4 remains a named published interface outside this selected proof.

The selected 1966 journal PDF is identified on the source card. The proof consumes the definitions on printed pp. 193–194, the needed parts of Theorem 1 on pp. 196–199, and Section 4 on pp. 204–212. The elementary inputs and the consumed partition geometry are proved below; no external continued-fraction theorem is left as an unproved premise. Labels (A)–(Q) below belong to this reconstruction, not to the source.

Continued-fraction identities

Apply the continued-fraction algorithm to ξ\xi: put T1=1/ξT_1=1/\xi, ai=⌊Ti⌋a_i=\lfloor T_i\rfloor, and Ti+1=1/(Ti−ai)T_{i+1}=1/(T_i-a_i). Irrationality makes every step defined, with ai≥1a_i\ge1 and Ti=ai+1/Ti+1>1T_i=a_i+1/T_{i+1}>1. Set

p−1=1,p0=0,q−1=0,q0=1,pn=anpn−1+pn−2,qn=anqn−1+qn−2(n≥1).p_{-1}=1,\quad p_0=0,\quad q_{-1}=0,\quad q_0=1, \qquad p_n=a_np_{n-1}+p_{n-2},\quad q_n=a_nq_{n-1}+q_{n-2}\quad(n\ge1).

Induction in these recurrences gives

pnqn−1−pn−1qn=(−1)n−1,ξ=pnTn+1+pn−1qnTn+1+qn−1.p_nq_{n-1}-p_{n-1}q_n=(-1)^{n-1},\qquad \xi=\frac{p_nT_{n+1}+p_{n-1}}{q_nT_{n+1}+q_{n-1}}.

For the first identity the determinant changes sign at each step. For the second, the case n=0n=0 is ξ=1/T1\xi=1/T_1; substituting Tn+1=an+1+1/Tn+2T_{n+1}=a_{n+1}+1/T_{n+2} gives the next case. In particular gcd⁡(pn,qn)=1\gcd(p_n,q_n)=1.

Write

σn=(−1)n,An=Tn+1,Qn=Anqn+qn−1,δn=Qn−1,εn=qnξ−pn=σnδn.\sigma_n=(-1)^n,\quad A_n=T_{n+1},\quad Q_n=A_nq_n+q_{n-1},\quad \delta_n=Q_n^{-1},\quad \varepsilon_n=q_n\xi-p_n=\sigma_n\delta_n.

The error formula follows by subtracting pn/qnp_n/q_n in the preceding fraction. Here AnA_n and QnQ_n are Kesten's an+1′a'_{n+1} and qn+1′q'_{n+1}, respectively. The local εn=qnξ−pn\varepsilon_n=q_n\xi-p_n is a signed convergent error, not Kesten's εn\varepsilon_n on p. 207: his symbol denotes the finite-prefix stability threshold called η\eta below. Since An=an+1+1/An+1A_n=a_{n+1}+1/A_{n+1}, direct substitution gives

Qn+1=An+1Qn,δn+1=δnAn+1,δn−1=an+1δn+δn+1.(A)Q_{n+1}=A_{n+1}Q_n,\qquad \delta_{n+1}=\frac{\delta_n}{A_{n+1}},\qquad \delta_{n-1}=a_{n+1}\delta_n+\delta_{n+1}. \tag{A}

For the last identity one can also use the recurrence for εn\varepsilon_n and their alternating signs. For n≥2n\ge2 we have 0<qn−1<qn0<q_{n-1}<q_n, qn+2≥2qnq_{n+2}\ge2q_n, and, with a=an+1a=a_{n+1},

qn+1<Qn<(a+2)qn.(B)q_{n+1}<Q_n<(a+2)q_n. \tag{B}

Thus qn→∞q_n\to\infty and δn→0\delta_n\to0. Telescoping (A) gives

∑j=s∞aj+1δj=δs−1+δs⟶0.(C)\sum_{j=s}^{\infty}a_{j+1}\delta_j =\delta_{s-1}+\delta_s\longrightarrow0. \tag{C}

Only these identities are needed, not existence or uniqueness of a general Ostrowski expansion of an arbitrary integer.

The consumed partition geometry, with both parities

Fix n≥2n\ge2 and abbreviate q=qnq=q_n, v=qn−1v=q_{n-1}, Q=QnQ=Q_n, A=AnA=A_n, δ=δn\delta=\delta_n, σ=σn\sigma=\sigma_n. Use the oriented circle coordinate

yn(k)={σkξ}.y_n(k)=\{\sigma k\xi\}.

For r=0,…,q−1r=0,\ldots,q-1, let λr\lambda_r be the unique integer in [1,q][1,q] such that σpnλr≡r(modq)\sigma p_n\lambda_r\equiv r\pmod q. The error formula gives

Yr:=yn(λr)=rq+λrqQ∈(rq,r+1q).(D)Y_r:=y_n(\lambda_r)=\frac rq+\frac{\lambda_r}{qQ} \in\left(\frac rq,\frac{r+1}{q}\right). \tag{D}

Indeed 0<λr/(qQ)<1/q0<\lambda_r/(qQ)<1/q by (B). These are exactly the first qq orbit points, in increasing oriented order. Put Yq=Y0+1Y_q=Y_0+1 when measuring the interval that crosses zero.

The determinant identity implies σpnv≡−1(modq)\sigma p_nv\equiv-1\pmod q. Consequently the label of the next point, including the cyclic last-to-first pair, satisfies

λr+1={λr−v,λr>v,λr+q−v,λr≤v.(E)\lambda_{r+1}= \begin{cases} \lambda_r-v,&\lambda_r>v,\\ \lambda_r+q-v,&\lambda_r\le v. \end{cases} \tag{E}

Here λq=λ0\lambda_q=\lambda_0; representatives are always in [1,q][1,q]. Subtracting the two instances of (D), using the lift at the cyclic pair, shows that the interval from YrY_r to Yr+1Y_{r+1} has length

Lr={Aδ,λr>v(short),(A+1)δ,λr≤v(long).(F)L_r= \begin{cases} A\delta,&\lambda_r>v\quad\text{(short)},\\ (A+1)\delta,&\lambda_r\le v\quad\text{(long)}. \end{cases} \tag{F}

This proves the needed long/short classification for odd as well as even nn: reflection is built into yny_n, rather than left as an omitted case. All these lengths are less than 2/q2/q, and hence tend uniformly to zero.

Now include all indices through qn+1=aq+vq_{n+1}=aq+v, where a=an+1a=a_{n+1}. Every such index has a unique form λr+sq\lambda_r+sq, with

0≤s≤mr,mr={a−1,λr>v,a,λr≤v.0\le s\le m_r,\qquad m_r= \begin{cases} a-1,&\lambda_r>v,\\ a,&\lambda_r\le v. \end{cases}

Since λr+sq≤qn+1<Q\lambda_r+sq\le q_{n+1}<Q, the same calculation as (D) yields

yn(λr+sq)=Yr+sδ<r+1q.(G)y_n(\lambda_r+sq)=Y_r+s\delta <\frac{r+1}{q}. \tag{G}

Thus there are no additional points between consecutive displayed points in a column, or between its last displayed point and Yr+1Y_{r+1}. The column interval is split into mrm_r pieces of length δn\delta_n and a last piece of length

Lr−mrδn=(An−an+1+1)δn=δn+δn+1.(H)L_r-m_r\delta_n =(A_n-a_{n+1}+1)\delta_n =\delta_n+\delta_{n+1}. \tag{H}

At level n+1n+1 the orientation reverses. Its short length is An+1δn+1=δnA_{n+1}\delta_{n+1}=\delta_n, and its long length is δn+δn+1\delta_n+\delta_{n+1}. Hence the regular pieces in (G) become short intervals and the last piece becomes a long interval. This proves all the refinement information used from Theorem 1; its other general-NN statements and corollaries are not required.

Locating the endpoint and deriving the counting identity

Assume for contradiction that bb is not {jξ}\{j\xi\} for any integer jj. In particular no positive orbit point is bb or zero. Put

zn={b,n even,1−b,n odd.z_n= \begin{cases} b,&n\ \text{even},\\ 1-b,&n\ \text{odd}. \end{cases}

Choose nn sufficiently large that the partition interval containing znz_n does not cross zero; this is possible by (F) and min⁡(b,1−b)>0\min(b,1-b)>0. Write its index as rnr_n, its initial label as λn=λrn\lambda_n=\lambda_{r_n}, its length as LnL_n, and

hn=zn−Yrn,0<hn<Ln.h_n=z_n-Y_{r_n},\qquad 0<h_n<L_n.

The inequalities are strict because its endpoints are orbit points. Define dnd_n as the largest integer dd with 0≤d≤mrn0\le d\le m_{r_n} and dδn<hnd\delta_n<h_n. Call the case dn=mrnd_n=m_{r_n} terminal. If it is not terminal, then

dnδn<hn<(dn+1)δn.(I)d_n\delta_n<h_n<(d_n+1)\delta_n. \tag{I}

The partition refinement gives the exact transition rules. In the nonterminal case the next interval is short and

λn+1=λn+(dn+1)qn,hn+1=(dn+1)δn−hn.(J)\lambda_{n+1}=\lambda_n+(d_n+1)q_n,\qquad h_{n+1}=(d_n+1)\delta_n-h_n. \tag{J}

In the terminal case it is long; its initial point in the reversed orientation is the far endpoint of the old interval. Thus

λn+1={λn−qn−1,old interval short,λn+qn−qn−1,old interval long,hn+1=Ln−hn.(K)\lambda_{n+1}= \begin{cases} \lambda_n-q_{n-1},&\text{old interval short},\\ \lambda_n+q_n-q_{n-1},&\text{old interval long}, \end{cases} \qquad h_{n+1}=L_n-h_n. \tag{K}

These are statements about positive integer labels, not a choice of fractional-part representatives.

For a nonterminal d=dnd=d_n, set t=d+1t=d+1 and Mn=tqnM_n=tq_n. Then 1≤t≤an+11\le t\le a_{n+1}, so Mn<qn+1M_n<q_{n+1}. The first MnM_n points have exactly tt representatives in each grid cell (r/qn,(r+1)/qn)(r/q_n,(r+1)/q_n), namely those in (G) with 0≤s<t0\le s<t. By (I), all tt points in cell rnr_n are below znz_n. Moreover

zn<Yrn+tδn=rnqn+λn+tqnqnQn<rn+1qn,z_n<Y_{r_n}+t\delta_n =\frac{r_n}{q_n} +\frac{\lambda_n+tq_n}{q_nQ_n} <\frac{r_n+1}{q_n},

where nonterminality ensures λn+tqn≤qn+1<Qn\lambda_n+tq_n\le q_{n+1}<Q_n. All earlier cells contribute tt points and all later cells contribute none. Consequently

Dn(Mn):=σnR(Mn)=t(rn+1)−tqnzn=t(1−λnQn−qnhn).(L)D_n(M_n):=\sigma_nR(M_n) =t(r_n+1)-tq_nz_n =t\left(1-\frac{\lambda_n}{Q_n}-q_nh_n\right). \tag{L}

For odd nn this uses the exact identity

#{1≤k≤M:{−kξ}<1−b}=M−#{1≤k≤M:{kξ}<b}.\#\{1\le k\le M:\{-k\xi\}<1-b\} =M-\#\{1\le k\le M:\{k\xi\}<b\}.

It holds because neither equality kξ∈Zk\xi\in\mathbb Z nor {kξ}=b\{k\xi\}=b occurs. Thus (L) includes the sign and endpoint conventions in the source's even and odd counting formulas.

Why separated discrepancy blocks add

For every fixed positive integer MM there is η(M)>0\eta(M)>0 such that moving each of the first MM orbit points by any circle distance less than η(M)\eta(M) leaves its membership in [0,b)[0,b) unchanged. Take less than the minimum of their positive circle distances to the two boundary points 0,b0,b. This is a finite positive minimum.

Suppose infinitely many indices nn have block lengths Mn=cnqnM_n=c_nq_n, where cnc_n is an integer with 1≤cn≤an+11\le c_n\le a_{n+1}, and σnR(Mn)≥c\sigma_nR(M_n)\ge c for one fixed c>0c>0. One parity contains infinitely many of them. Choose increasing indices n1,n2,…n_1,n_2,\ldots of that parity, so separated that

δni+1−1+δni+1<η(Mni).\delta_{n_{i+1}-1}+\delta_{n_{i+1}}<\eta(M_{n_i}).

This is possible by (C). For any finite terminal index u>iu>i, put Si=∑j=i+1uMnjS_i=\sum_{j=i+1}^uM_{n_j}. Its rotation differs from an integer by the signed sum ∑j=i+1ucnjεnj\sum_{j=i+1}^u c_{n_j}\varepsilon_{n_j}, whose absolute value is at most the tail in (C). Hence

N(Si+Mni,ξ,0,b)−N(Si,ξ,0,b)=N(Mni,ξ,0,b).N(S_i+M_{n_i},\xi,0,b)-N(S_i,\xi,0,b) =N(M_{n_i},\xi,0,b).

Use the empty-count convention N(0,ξ,0,b)=R(0)=0N(0,\xi,0,b)=R(0)=0. The same equality is trivial for i=ui=u, with Su=0S_u=0. Subtracting MnibM_{n_i}b and summing in reverse block order gives

R(∑i=1uMni)=∑i=1uR(Mni).(M)R\left(\sum_{i=1}^uM_{n_i}\right) =\sum_{i=1}^uR(M_{n_i}). \tag{M}

The common parity makes all summands have the same sign and magnitude at least cc. Thus ∣R∣|R| is unbounded. Under our boundedness hypothesis, every class of blocks with such a uniform positive signed discrepancy is finite. This proves the accumulation step (4.19)–(4.20) without assuming arbitrary blocks add. In the preceding tail estimate on p. 207, the printed braces cannot literally mean fractional parts: for odd jj, {qjξ}=1−δj\{q_j\xi\}=1-\delta_j, not a small positive error. The intended quantity is distance to the nearest integer, ∥⋅∥\|\cdot\|, which Kesten defines in footnote 4 on p. 196. This is a notational slip, not a mathematical gap. The local argument uses signed errors and the exact tail (C), so it does not import the printed fractional-part inequality.

Excluding all nonterminal digits

In this paragraph abbreviate a=an+1a=a_{n+1}, B=an+2B=a_{n+2}, q=qnq=q_n, v=qn−1v=q_{n-1}, Q=QnQ=Q_n, A=AnA=A_n, and t=dn+1t=d_n+1. Whenever dn≤a−2d_n\le a-2 it is nonterminal. From (I), (L) and λn≤q\lambda_n\le q,

Dn(Mn)>tQ((A−dn−2)q+v).(N)D_n(M_n)> \frac{t}{Q}\bigl((A-d_n-2)q+v\bigr). \tag{N}

If dn≤a−3d_n\le a-3, then a≥3a\ge3 and 1≤t≤a−21\le t\le a-2. Using (B) and A>aA>a gives

Dn(Mn)>t(a−1−t)a+2≥a−2a+2≥15.D_n(M_n)> \frac{t(a-1-t)}{a+2} \ge\frac{a-2}{a+2}\ge\frac15.

The middle inequality follows by minimizing the concave quadratic on the integer interval 1≤t≤a−21\le t\le a-2, whose two endpoint values are a−2a-2. If dn=a−2≥0d_n=a-2\ge0 and B≤6B\le6, then A−a=1/An+1>1/7A-a=1/A_{n+1}>1/7, so

Dn(Mn)>a−17(a+2)≥128.D_n(M_n)> \frac{a-1}{7(a+2)}\ge\frac1{28}.

The accumulation argument therefore excludes both cases for all sufficiently large nn. After enlarging the starting index, every nn satisfies

dn≥an+1−1ordn=an+1−2≥0,an+2≥7.(O)d_n\ge a_{n+1}-1 \quad\text{or}\quad d_n=a_{n+1}-2\ge0,\quad a_{n+2}\ge7. \tag{O}

For any nonterminal digit, (J) and hn+1>dn+1δn+1h_{n+1}>d_{n+1}\delta_{n+1} give a stronger bound than (N):

Dn(Mn)>tQ(Q−λn−tq+dn+1qAn+1).(P)D_n(M_n)> \frac{t}{Q} \left(Q-\lambda_n-tq+ \frac{d_{n+1}q}{A_{n+1}}\right). \tag{P}

In the second case of (O), t=a−1t=a-1, a≥2a\ge2, B≥7B\ge7, and (O) at the next index gives dn+1≥B−2d_{n+1}\ge B-2. Since Q=(a+1/An+1)q+vQ=(a+1/A_{n+1})q+v and λn≤q\lambda_n\le q, the parenthesis in (P) is at least (B−2)q/An+1(B-2)q/A_{n+1}. Hence

Dn(Mn)>a−1a+2B−2B+1≥1458=532.D_n(M_n)> \frac{a-1}{a+2}\frac{B-2}{B+1} \ge\frac14\frac58=\frac5{32}.

This class is also finite by (M). We have therefore proved that eventually dn≥an+1−1d_n\ge a_{n+1}-1 at every index, not merely at one parity.

The only remaining nonterminal possibility is dn=a−1d_n=a-1 in a long interval: a short interval has maximal permitted digit a−1a-1. For a long interval λn≤v\lambda_n\le v. At sufficiently large indices, dn+1≥B−1d_{n+1}\ge B-1. Now (P), with t=at=a, gives

Dn(aq)>aQ(v−λn+(1+dn+1)qAn+1)≥aqBQAn+1>aa+2BB+1≥16.D_n(aq)> \frac{a}{Q} \left(v-\lambda_n+\frac{(1+d_{n+1})q}{A_{n+1}}\right) \ge\frac{aqB}{QA_{n+1}} >\frac{a}{a+2}\frac{B}{B+1}\ge\frac16.

This last class is finite too. This combines the transition and counting steps of source (4.24)–(4.31) in the common oriented coordinates; it does not leave the reversed-parity calculation implicit.

Thus eventually every digit is terminal. By (K), a terminal step is followed by a long interval. At all sufficiently large indices the interval is consequently long and its terminal digit is

dn=an+1.(Q)d_n=a_{n+1}. \tag{Q}

The terminal label forces an orbit endpoint

In (Q) the long-interval case of (K) applies at every step:

λn+1=λn+qn−qn−1.\lambda_{n+1}=\lambda_n+q_n-q_{n-1}.

Therefore λn−qn−1=j\lambda_n-q_{n-1}=j is one fixed integer once nn is sufficiently large. The initial point of the interval containing bb in the original circle is Pn={λnξ}P_n=\{\lambda_n\xi\}. Its distance from bb tends to zero by (F). Since λnξ=jξ+pn−1+εn−1\lambda_n\xi=j\xi+p_{n-1}+\varepsilon_{n-1} and εn−1→0\varepsilon_{n-1}\to0, the circle distance from b−jξb-j\xi to an integer is zero. Thus b−jξ∈Zb-j\xi\in\mathbb Z, and 0<b<10<b<1 implies b={jξ}b=\{j\xi\}. This contradicts the assumed absence of such an orbit point and proves the selected anchored necessity direction.

The integer-label invariant is an equivalent presentation of the final telescoping argument on pp. 211–212. Kesten's alternating half-unit terms compensate the oscillation of the convergent fractional parts, so his printed limit is justified. The invariant avoids the final representative check that the source leaves unstated; it does not repair an unjustified limit.

Current proof coverage and remaining obligations

The independent whole-claim review returned refutation-failed for exactly the anchored irrational necessity reconstruction. The distinct grade passed the report contract and independence, with documentary corrections. This discharges the literature-compilation proof-coverage review obligation for that proper subdirection only. The reviewed historical theorem text is retained as the opaque asset reviewed_theorem_4.md.txt, together with the reviewed digest.

The source-reading and correction record pins those subjects and maps the three source-prose corrections and the standing reconciliation in the present page. The original proof's mathematics is unchanged. The review is of the historical subject, not a fresh review of the later prose and standing edits. The source-delta and transformation review of this filing was completed and accepted before it was filed; it changed no mathematics.

The continued-fraction identities, consumed Theorem 1 geometry, parity transfer, finite-prefix stability, block accumulation, digit exclusions and final consequence have reviewed coverage within the selected proof. The signed coordinates and integer-label invariant are local reorganizations, not an author-issued erratum or a claim of a new theorem. The source's (4.27)–(4.31) and cases (i)/(ii)/(iii) were read but are bypassed, not reconstructed, by the direct nonterminal long-cell exclusion.

No mathematical code, Lean proof, numerical tier or new resolution of the endpoint problem is claimed. Theorem 1 outside the consumed geometry, the paper's Farey and metric results, rational rotations and the Bohl arbitrary-translate reduction are not reconstructed here. This partial direction is not full local proof coverage of Theorem 4.

The retained independent review and distinct grade cover the previously recorded Theorem 4 statement, exact domains and elementary transfers, not the anchored proof reviewed in the records above. That review read this page as it stood. The reconstruction filed on 2026-09-10T09:12:21Z added the anchored necessity sections above and removed the earlier proof-scope paragraph, which said the necessity argument was not reconstructed; the statement, exact domains and elementary transfers it read are otherwise unchanged apart from citation wording tidied on 2026-09-17. The endpoint disproof does not depend on the necessity direction. Those completed earlier scopes and their acceptance are unchanged.