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The [[research/leads/totient_binary_series/integer_interpolation/phase_transference|phase comparison]] equates a small odd-kernel cost with a large phase error on a specified family. Its reverse implications from irrationality on other supports do not, by themselves, give a reverse implication on [J,2J][J,2J]. Here the identity φ(3k)=2φ(2k)\varphi(3k)=2\varphi(2k) for odd kk coprime to 33 supplies the missing arithmetic on that short support.

The result is an equivalence along a subsequence of powers of two, and an exact finite sufficient test for phase separation. It proves no unbounded sequence of successful tests and does not resolve Problem 249. These are author-recorded, unreviewed arguments. The eventual structural assertions use the fixed-modulus prime number theorem at the disclosed standing below.

Notation and the structural hypotheses

Let J=2m≥4J=2^m\ge4, use all indices J≤n≤2JJ\le n\le2J, and put

H=3J+2,at=φ(t)/2(t≥3),An=Φn/2,Vn=UJ(n)/2,wn=n+J+2.H=3J+2,\quad a_t=\varphi(t)/2\quad(t\ge3),\quad A_n=\Phi_n/2,\quad V_n=U_J(n)/2,\quad w_n=n+J+2.

Here Φn\Phi_n, UJ(n)U_J(n) and the complete positive tail TnT_n are defined on the [[research/leads/totient_binary_series/integer_interpolation/two_depth_carries|two-depth page]]. In particular

2JTn=UJ(n)+Tn+J,0<Tn+J≤wn,0<Vn<2J−1(n+2).(1)2^JT_n=U_J(n)+T_{n+J},\qquad 0<T_{n+J}\le w_n,\qquad 0<V_n<2^{J-1}(n+2). \tag{1}

Write ∥x∥=dist⁡(x,Z)\|x\|=\operatorname{dist}(x,\mathbb Z), and let $\epsilon_J=\min_\theta\max_{J\le n\le2J} |\theta V_n-A_n/2|/w_n$. This minimum is attained, as on the phase comparison page. Define the finite set

KJ={k: k odd, 3∤k, J<2k<3k≤2J},Dk=a3k+J−2a2k+J.\mathcal K_J=\{k:\ k\text{ odd},\ 3\nmid k,\ J<2k<3k\le2J\}, \quad D_k=a_{3k+J}-2a_{2k+J}.

The two structural hypotheses used below are

gcd⁡J<t≤2Jat=1,G:=gcd⁡k∈KJDk>0 and odd.(2)\gcd_{J<t\le2J}a_t=1,\qquad G:=\gcd_{k\in\mathcal K_J}D_k>0\ \hbox{and odd}. \tag{2}

The gcd is taken positive, ignoring zero entries; (2) requires a nonzero entry. Set D∗=max⁡k∈KJ∣Dk∣D_*=\max_{k\in\mathcal K_J}|D_k|, so 1≤G≤D∗≤H1\le G\le D_*\le H. Also a∗:=max⁡J<t≤2Jat≥a2J=J/2a_*:=\max_{J<t\le2J}a_t\ge a_{2J}=J/2, hence H/a∗≤8H/a_*\le8.

Lemma 1. Conditions (2) hold for every sufficiently large power of two JJ. They also give the odd feasibility and row-rank hypotheses of Theorem 4 on the phase comparison page.

Proof. The integer a2J=J/2a_{2J}=J/2 is a power of two. A prime p∈(J,2J)p\in(J,2J) with p≡3(mod4)p\equiv3\pmod4 supplies the odd value ap=(p−1)/2a_p=(p-1)/2, proving the first gcd assertion. For the second, choose a prime

5J/2<P<3J,P≡3(mod4),P≡J+3(mod9).5J/2<P<3J,\qquad P\equiv3\pmod4,\qquad P\equiv J+3\pmod9.

These congruences specify a reduced class modulo 3636, since JJ is coprime to 33. Then k=(P−J)/3k=(P-J)/3 is odd, is 11 modulo 33, and belongs to KJ\mathcal K_J. Its Dk=aP−2a2k+JD_k=a_P-2a_{2k+J} is odd.

Both prime choices follow separately from the fixed-modulus theorem π(x;q,r)∼x/(φ(q)log⁡x)\pi(x;q,r)\sim x/(\varphi(q)\log x) for fixed coprime q,rq,r. The counts in these intervals are asymptotic to J/(2log⁡J)J/(2\log J) and J/(24log⁡J)J/(24\log J), respectively. Only six reduced classes modulo 3636 arise, so their thresholds can be made common. No growing modulus or simultaneous prime pair is used.

More generally, (2) implies that some DkD_k is odd and some ata_t is odd. For such kk, since it is odd and 3∤k3\nmid k, a3k=2a2ka_{3k}=2a_{2k} is even, while a3k+Ja_{3k+J} is odd. Together with an odd ata_t from the first gcd assertion this gives an odd minor of the two rows (at)(a_t) and (at+J)(a_{t+J}). Thus they have rank two. For n≥4n\ge4, An≡an(mod2)A_n\equiv a_n\pmod2 and Vn≡an+J(mod2)V_n\equiv a_{n+J}\pmod2. The same two columns have an odd minor and include an odd VnV_n. Dividing their scalar cross-product by their odd gcd produces an odd kernel vector. □\square

The external prime-theorem statement was inspected in NIST DLMF §27.11, closing paragraph, version 1.2.8 (2026-09-15), and the introductory fixed-qq formula in Tao's 2009 exposition. Its analytic proof is neither reconstructed nor independently reviewed here. This use changes the fixed moduli from the earlier 2020 to 44 and 3636; it makes no uniformity assertion for unbounded moduli. At an individual JJ, (2) can instead be checked directly without this asymptotic input.

Localizing a small phase

Proposition 2. Assume (2). Suppose δ>0\delta>0, 18δH3<118\delta H^3<1, and some real θ\theta satisfies

∥θVn−An/2∥≤δwn(J≤n≤2J).(3)\|\theta V_n-A_n/2\|\le\delta w_n \qquad(J\le n\le2J). \tag{3}

Then there is a nonzero odd integer qq with

∣q∣≤26δ2JH,∥qVn2J+1−An2∥≤31δHwn(J≤n≤2J).(4)|q|\le26\delta2^JH,\qquad \left\|\frac{qV_n}{2^{J+1}}-\frac{A_n}{2}\right\| \le31\delta H w_n\quad(J\le n\le2J). \tag{4}

There is also an integer pp such that

∥q2J−2S∥≤38δH22−J,∣S−pq2J−2∣≤152δH2∣q∣22J.(5)\left\|q2^{J-2}S\right\|\le38\delta H^2 2^{-J},\qquad \left|S-\frac{p}{q2^{J-2}}\right| \le\frac{152\delta H^2}{|q|2^{2J}}. \tag{5}

Proof. Choose integers mnm_n so that the errors in (3) have absolute value at most δwn\delta w_n. The recurrences give, for J<t≤2JJ<t\le2J,

θ(at+J−2Jat)−at/2−ℓt=et,ℓt=mt−2mt−1∈Z,∣et∣≤3δH.(6)\theta(a_{t+J}-2^Ja_t)-a_t/2-\ell_t=e_t, \quad \ell_t=m_t-2m_{t-1}\in\mathbb Z, \quad |e_t|\le3\delta H. \tag{6}

Subtract twice the relation at 2k2k from the one at 3k3k. The terms involving ata_t cancel, so integers hkh_k satisfy ∣θDk−hk∣≤9δH|\theta D_k-h_k|\le9\delta H. If ss realizes ∣Ds∣=D∗|D_s|=D_*, every integer Dkhs−DshkD_kh_s-D_sh_k has absolute value at most 18δHD∗<118\delta HD_*<1, and is zero. Thus hk/Dkh_k/D_k has one common value on the nonzero entries. Because all hkh_k are integers and their corresponding DkD_k have gcd GG, this value is r/Gr/G for some integer rr. Consequently

∣θ−r/G∣≤E,E=9δH/D∗.(7)|\theta-r/G|\le E,\qquad E=9\delta H/D_*. \tag{7}

This integer-minor argument includes the small-error threshold; a gcd assertion alone would not give a quantitative approximation.

Put λ=2J+1Gθ\lambda=2^{J+1}G\theta. Multiplying (6) by 2G2G and using (7) yields integers

qt=2rat+J−Gat−2Gℓt,∣λat−qt∣≤η,η=GH(E+6δ).(8)q_t=2r a_{t+J}-Ga_t-2G\ell_t, \qquad |\lambda a_t-q_t|\le\eta, \qquad \eta=GH(E+6\delta). \tag{8}

For any t,ut,u, the integer auqt−atqua_uq_t-a_tq_u has absolute value at most HηH\eta. Moreover

Hη=9δ(G/D∗)H3+6δGH2≤15δH3<1.H\eta=9\delta(G/D_*)H^3+6\delta GH^2 \le15\delta H^3<1.

These integers vanish. The first gcd assertion in (2) now gives an integer QQ with qt=Qatq_t=Qa_t for every tt. Hence ∣λ−Q∣≤η/a∗|\lambda-Q|\le\eta/a_*. Since qt≡Gat(mod2)q_t\equiv Ga_t\pmod2 and some ata_t is odd, QQ is odd. Set q=Q−2J+1rq=Q-2^{J+1}r, also odd. Then

∣q∣≤2J+1GE+η/a∗≤18δ2JH+120δH≤26δ2JH,|q|\le2^{J+1}GE+\eta/a_* \le18\delta2^JH+120\delta H \le26\delta2^JH,

where J≥4J\ge4, G≤D∗≤HG\le D_*\le H and H/a∗≤8H/a_*\le8 were used.

The dyadic phase q/2J+1q/2^{J+1} differs from Gθ−rG\theta-r by at most η/(a∗2J+1)\eta/(a_*2^{J+1}). Because GG is odd, multiplying (3) by GG preserves the half-integer target modulo integers. Equation (1) gives

∥qVn2J+1−An2∥≤(Gδ+η4a∗)wn≤(13Gδ+2GE)wn≤31δHwn.\left\|\frac{qV_n}{2^{J+1}}-\frac{A_n}{2}\right\| \le\left(G\delta+\frac{\eta}{4a_*}\right)w_n \le(13G\delta+2GE)w_n\le31\delta H w_n.

This proves (4), including its parity requirement. Oddness of GG cannot be dropped from this step.

For any odd integer qq, the exact complete-tail identity (1) implies

qVn2J+1−An2≡q2n−2S−qTn+J2J+2(mod1).(9)\frac{qV_n}{2^{J+1}}-\frac{A_n}{2} \equiv q2^{n-2}S-\frac{qT_{n+J}}{2^{J+2}}\pmod1. \tag{9}

The omitted algebraic term is (q+1)Φn/4∈Z(q+1)\Phi_n/4\in\mathbb Z. Thus (1) and (4) give ∥q2n−2S∥≤38δH2\|q2^{n-2}S\|\le38\delta H^2 throughout the window. This bound is less than 1/31/3, since 18δH3<118\delta H^3<1 and H≥14H\ge14. Choose the nearest-integer residuals fnf_n for these quantities. Each fn+1−2fnf_{n+1}-2f_n is an integer of absolute value less than 11, hence zero. Therefore ∣fJ∣=2−J∣f2J∣≤38δH22−J|f_J|=2^{-J}|f_{2J}|\le38\delta H^2 2^{-J}. Dividing by ∣q∣2J−2|q|2^{J-2} proves (5). □\square

The subsequence equivalence on the short support

Theorem 3. Along the powers of two JJ, the following statements are equivalent:

  1. SS is irrational.
  2. lim sup⁡J→∞, J=2mϵJ2J=∞\limsup_{J\to\infty,\ J=2^m}\epsilon_J2^J=\infty.
  3. On some unbounded subsequence of those JJ, there are odd kernel vectors supported on [J,2J][J,2J] with cost o(2J)o(2^J).

Proof. By Lemma 1 and Corollary 5 of the phase comparison page, 2 implies 3. The complete-tail criterion on the two-depth page, with lower cutoff B=J→∞B=J\to\infty, shows that 3 implies 1.

For the remaining implication, suppose 2 fails. Choose a fixed M≥1M\ge1 such that ϵJ≤M2−J\epsilon_J\le M2^{-J} for every sufficiently large power of two. Apply Proposition 2 with δ=M2−J\delta=M2^{-J}, which eventually meets its threshold, and write

rJ=pJqJ2J−2,0<∣qJ∣≤26MHJ,∣S−rJ∣≤152MHJ2∣qJ∣23J,HJ=3J+2.r_J=\frac{p_J}{q_J2^{J-2}},\qquad 0<|q_J|\le26MH_J,\qquad |S-r_J|\le\frac{152MH_J^2}{|q_J|2^{3J}}, \quad H_J=3J+2.

If rJ≠r2Jr_J\ne r_{2J}, their common dyadic factors give ∣rJ−r2J∣≥1/(∣qJq2J∣22J−2)|r_J-r_{2J}|\ge1/(|q_Jq_{2J}|2^{2J-2}). Multiplying the sum of their approximation errors by that denominator would imply

1≤988M2(HJ2H2J2J+HJH2J224J),(10)1\le988M^2\left( \frac{H_J^2H_{2J}}{2^J} +\frac{H_JH_{2J}^2}{2^{4J}}\right), \tag{10}

which is false for every sufficiently large JJ. Thus consecutive powers eventually give the same rational number. Their errors tend to zero, forcing SS to equal that rational number. This proves the contrapositive of 1 implying 2. □\square

The dyadic factors in the denominator comparison are essential: using the product of the two denominators loses a factor 2J2^J. This proves a subsequence assertion, not ϵJ2J→∞\epsilon_J2^J\to\infty along all powers of two and not an all-depth polynomial cost bound. The earlier wider-support shadow construction still has its original scope; it was not restricted to the short support to obtain this theorem.

A finite exact sufficient test

Fix an integer M≥1M\ge1 and a power of two J≥4J\ge4 satisfying (2) and 18MH3<2J18MH^3<2^J. If, for each positive odd integer q≤26MHq\le26MH, there is an n∈[J,2J]n\in[J,2J] such that

dist⁡(qUJ(n)−2JΦn,2J+2Z)>124MH(n+J+2),(11)\operatorname{dist}\left(qU_J(n)-2^J\Phi_n, 2^{J+2}\mathbb Z\right) >124MH(n+J+2), \tag{11}

then ϵJ>M2−J\epsilon_J>M2^{-J}. Indeed otherwise Proposition 2 supplies an odd qq in this range satisfying the opposite inequality at every index, by multiplying (4) by 2J+22^{J+2}. Negative qq gives the same phase distances as positive qq because AnA_n is integral, so positive qq suffice.

This is a finite test on exact integers using totients only through 3J3J, with O(MJ)O(MJ) candidate numerators and O(J)O(J) coordinates for each. All the infinite-tail reasoning is in Proposition 2, not in a truncation of (11). A failure of this sufficient test says nothing decisive about the optimal phase error. Successful tests for a finite set of parameters prove no asymptotic claim. An unbounded sequence of successful pairs with M→∞M\to\infty would establish Theorem 3(2); no such sequence is proved here.

For a small structural check, at J=32J=32 one has KJ={17,19}\mathcal K_J=\{17,19\}, D17=41−2⋅10=21D_{17}=41-2\cdot10=21 and D19=44−2⋅12=20D_{19}=44-2\cdot12=20, hence G=1G=1. Also a64=16a_{64}=16 and a43=21a_{43}=21 give the other gcd in (2). These exposed computations check the index and parity conventions; they are not a phase certificate or evidence for the required growth.

The new finite test offers a concrete way to examine the arithmetic left by the phase comparison. Proving its success in a growing family, or obtaining separation by a different arithmetic argument, remains open. Neither this equivalence nor its connection with runs of binary digits rules out Fourier, lattice, signed-multiplier or other methods.