Leg 127 (exploration, reserve). Gate answer: YES, (i). Data:
writeup/data/p2_route_ngx_v1_general.json. Runner:
experiments/p2_route_ngx_v1_general.py. Figure: fig63_route_ngx_v1_general.png, rebuilt
from the curated JSON alone by experiments/p2_route_ngx_v1_general_evidence.py. Novelty
pass: writeup/novelty/leg_127.md, run and committed before any construction. Module
additions are append-only in solver/spectral_certificate.py; gates 32–37 in
test_spectral_certificate.py (37/37 pass).
Gate, in its pre-committed wording. Can the no-go be DECIDED on the full bounded class (either (i) a proof that
Z₁ ≥ 1for every boundedA(A₂₁free) at somes < 1, with hypotheses containing thea = 0CLM linearization, or (ii) an explicit admissibleAwithA₂₁ ≠ 0and measuredZ₁ < 1, grid-stable over ≥ 3 resolutions?) YES, (i). The yes-(i) branch fires: the theorem reaches its sharp form. Report it standalone; the scope-line upgrades across banked prose are pointer-block work for the orchestrator, not silent edits; fold into the publication-scoping question already with the user.THE SCOPE LINE IS LOAD-BEARING AND IT IS NEW. arXiv:2607.19762 (Xu, 2026), which post-dates leg 58's novelty pass, proves the same
a = 0CLM linearisation is invertible on origin-H²after the standard modulation, with a spectral gap of1/2. Everything below is therefore a statement about theℓ¹_wrealization ats < 1and about nothing else. No sentence in this leg says the operator "has no bounded approximate inverse".
0. What was open
Leg 58 proved Z₁ ≥ 1 on the class A₂₁ = 0 by evaluating I − A L on x = (0; h), where
h is the tail block's far-field kernel (T h = 0, h_m ∼ m⁻², hence h ∈ ℓ¹_w iff
s < 1). Then
(I − A L)(0; h) = ( −(A₁₁B + A₁₂T)h ; h − A₂₁Bh − A₂₂Th )
and T h = 0 kills the A₁₂ and A₂₂ terms, leaving ‖A₁₁Bh‖ + ‖h‖ ≥ ‖h‖. The argument
stops at A₂₁ ≠ 0 because h − A₂₁Bh becomes cancellable. For that class the repository had
leg 54's battery only: seven shapes, best admissible Z₁ = 8.9591 against a block-diagonal
baseline of 10.4584, and MM4c's rank-one construction driving the ĥ-column floor to
≈ 10⁻¹⁶ at a total Z₁ of 5.66 × 10⁵.
1. The pre-registered argument, carried out, and refuted (lesson 76)
DIRECTION.md pre-registered a two-direction argument: pair x = (0; h) with the
finite-block directions A₂₁ populates. Carried out, it reads as follows. For x = (z; 0)
with z_K = 0 the coupling C z vanishes (C is rank one and sees only z_K), so the
tail-row component of (I − A L)x is exactly −A₂₁ L₁₁ z, uncancellable. Writing
‖h − A₂₁Bh‖ = θ‖h‖ and optimising over θ gives
Z₁ ≥ max( θ , (1−θ)/η ) ≥ 1/(1+η), η = ‖G⁻¹Bh‖_w / ‖h‖_w.
Measured at K = 4, s = 0.3 (JSON NGX3_explicit_sequence, finite_correction_norm,
against a unit-normalised h): η = 14.45 → 13.66 across M − K = 128 … 2048, i.e. it
converges to ≈ 13.7 rather than decaying. The bound is therefore Z₁ ≥ 0.068, which is
vacuous. The pre-registered route does not close, and it is recorded here rather than
deleted.
2. The argument that does close, and it has no blocks in it
For every x, ‖x‖_w ≤ ‖(I − A L)x‖_w + ‖A‖_w‖Lx‖_w. Dividing by ‖x‖_w and minimising:
(T1) For every bounded
A:Z₁ ≥ 1 − ‖A‖_w · σ_min(L), whereσ_min(L) := inf_{x≠0} ‖Lx‖_w/‖x‖_w = 1/‖L⁻¹‖_w.
A is never decomposed, so A₂₁ never appears and there is no corner in which the argument
can stop. (T1) is folklore and is NOT claimed; it is the contrapositive-with-remainder of
the Z₁ < 1 ⟹ invertible hypothesis stated in arXiv:1503.06315, arXiv:2505.03091 and
arXiv:2411.18361. The novelty pass established this before construction and forbade the claim.
What this leg contributes is which side of (T1) the operator's ℓ¹_w realization falls on.
(T1) is sharp, not lossy. Taking A = L⁻¹ gives Z₁ = 0 and ‖A‖_w = 1/σ_min exactly,
so the right-hand side is 0 and the slack is 0. Measured over the exact-inverse checks:
max slack 1.24 × 10⁻⁸ (NGX1_max_slack_at_the_exact_inverse). A bound that is attained does
not leak, which is why the conclusion below carries no hidden constant.
3. The operator is not bounded below in ℓ¹_w at s < 1
σ_min(L) for the assembled bordered object (leg 53's assembly, leg 54's single-matrix form),
fitted as σ_min ∼ M^{−p} over M − K = 128 … 2048:
s |
class | fitted p (K = 4) |
predicted 1 − s |
|---|---|---|---|
| 0.0 | flat | 0.9925 | 1.00 |
| 0.3 | algebraic | 0.6985 | 0.70 |
| 0.7 | algebraic | 0.3202 | 0.30 |
| 1.0 | algebraic | 0.0788 | 0.00 |
| 1.5 | algebraic | 0.5000 | , (different mechanism, §6) |
Max deviation from 1 − s over all s < 1 and all K ∈ {2, 4, 8}: 0.0219. The relative
spread of σ_min across K at the top of the ladder is 0.29% for s < 1: the divergence
is a property of the tail, not of where the split is placed, which is why no choice of
finite block escapes it.
3.1 The sequence is constructed, not found (lesson 86)
explicit_far_field_direction builds v_M = (z_M ; h^{(M)}) with h^{(M)} the analytic tail
kernel and G z_M = −B h^{(M)}. Measured against the numerically-optimal direction from
l1_bounded_below_constant:
- ratio to the numerical optimum: 1.0000000000045 (max over the ladder);
- cosine with the numerical optimum: 0.9999999999999998;
- finite-block residual of
L v: at most1.22 × 10⁻¹⁴over every class andM(float zero); z_K = 0.0exactly, by the parity of the kernel recursion, this switches off one of the two finite-to-tail coupling columns,C[:,K−1](the(1 − K/2)entry); the other,C[:,K+1](the far-field column), is killed not byzbut because it is supported on a single row, the truncation edge (§6);- rows carrying the residual of
L v: 1, the truncation edgem = M.
The rate then follows analytically: the edge row has size |1 − M/2|·|h_M|·w_M ∼ M^{s−1}
(gate 35 measures the exponent as −0.6942 against a predicted −0.70), while
‖v_M‖_w is bounded because Σ m^{s−2} converges for s < 1 (gate 34: the norm rises 5.4%
over an 8× range of M with shrinking increments, against a 2.83× growth at s = 1.5 on the
identical vector).
3.2 It is not a truncation artifact (leg 58's NG2c, re-aimed)
The referee objection: the near-null vector is an artifact of stopping at M. Test: zero-pad
the M-optimal direction into truncations 2M and 4M and re-measure. Max degradation over
the audit: 1.3543× (bounded, not a return to O(1)) and the embedded ratios continue
falling along the ladder at the same rate.
4. The theorem
Theorem NGX. Let
X = ℓ¹_wwithw_k = (1+k)^s,s < 1, and letLbe the assembled bordereda = 0CLM steady linearisation in the compactified odd-sine coefficient basis, split at modeK, withμ = 0. LetAbe any bounded operator onX: admissible in leg 54's MM3 sense, i.e. the truncation of one fixed bounded operator, so that‖A‖_wis uniform inM, withA₂₁completely free andA₁₁, A₁₂, A₂₂arbitrary. Then
Z₁ = ‖I − A L‖_w ≥ 1.Quantitatively at truncation
M:Z₁ ≥ 1 − ‖A‖_w · σ_min(L_M)withσ_min(L_M) = c_s M^{−(1−s)} → 0.Proof. (1) (T1), folklore. (2)
σ_min(L) = 0, witnessed by the explicit sequence of §3.1. ∎
This supersedes leg 58's A₂₁ = 0 theorem (that class is the special case A₂₁ = 0) and
retires leg 54's "measured, not proved" scope line for this operator in this space.
5. The consequence, as a magnitude (NGX6)
Any A reaching Z₁ ≤ 1 − δ needs ‖A‖_w ≥ δ/σ_min(L_M) ∼ δ·M^{1−s}. Measured floors at
s = 0.3, target Z₁ = 0.99: 1.555 → 10.778 across M − K = 128 … 2048; growth per
doubling 1.99× (flat) and 1.62× (s = 0.3), i.e. exactly 2^{1−s}.
The honest reading. At any fixed M the floor is finite and modest, so a finite-M
counterexample is not excluded, and leg 54 already exhibited one, exact_inv, whose
‖A‖_w equals 1/σ_min to the printed digits (662.58 at M − K = 1024, s = 0.3). That
is precisely why MM3 ruled it inadmissible. What Theorem NGX excludes is a single bounded
A working uniformly in M, which is the only sense the radii-polynomial method has.
Cross-check against leg 54's banked battery: 196/196 rows satisfy (T1); minimum slack
7.73 × 10⁻¹⁰, attained at exact_inv (K = 64, s = 0.3), where the bound is tight.
6. Controls, both able to report the other answer (lesson 90)
Positive control, μ > 0. Dissipation gives the tail a diagonal and destroys the kernel.
σ_min then saturates: fitted exponent ≤ 2.62 × 10⁻³ in absolute value across every
μ > 0 and both arms, against 0.6985 at μ = 0 in the same code path.
Second control, the s-scan. The exponent must vanish at s = 1, where the kernel leaves
ℓ¹_w. It does (0.079, consistent with a logarithm rather than a power). At s = 1.5
σ_min diverges again, at exponent 0.500, but that is the cokernel side of
fredholm_sides (the dual functional entering the space), a different mechanism, and it is
reported separately rather than folded in (lesson 75). Note also that the K-spread jumps from
0.29% (s < 1) to 2.14 at s = 1.5: the second obstruction lives at the split, the first
does not. Two mechanisms, two K-sensitivities.
A coincidence that had to be interrogated. At μ = 0 the bordered and unbordered objects
give σ_min identical to 5.7 × 10⁻¹⁵ relative. Lesson 90 says identical numbers are a bug
until proven otherwise, so the same two arms were compared at μ = 0.1, where they differ by
6.1 × 10⁻² relative: the code path does distinguish them. The μ = 0 coincidence is
therefore a finding, but not for the reason first assumed: the far-field-amplitude
component z[K+1] is not zero (it is 6.5–6.8% of ‖v‖₁ and grows slowly with M) so bordering with that amplitude does reach the singular sequence. What actually blocks it is
that the far-field column C[:,K+1] is supported on a single row, the truncation edge:
bordering has nowhere else to couple into, so it (leg 52's repair, the entire purpose of the
assembled object) does not move the obstruction at all. This independently re-answers NG2c's
split-placement objection in the general class: the wall is not where the far-field unknown
is put.
7. What this is a statement about, and what it is not
Xu (arXiv:2607.19762) proves this operator is invertible on origin-H² after modulation, with
a spectral gap of 1/2; our gauge row performs exactly that modulation (the dilation zero mode
is exactly e₂, gated). The two results do not conflict: they separate two realizations of
one operator. The content of Theorem NGX is therefore:
The obstruction is a property of the certificate's space, not of the
a = 0CLM linearisation. The radii-polynomial method needs weightedℓ¹of Fourier coefficients in order to control its tail; in that space, at everys < 1, this operator is not bounded below, and no bounded approximate inverse exists at all: let alone a good one.
And the space is squeezed from both sides: at s < 1 the kernel is in the space; at s ≥ 1
the cokernel functional is in the dual; and s = 1, the one exponent where σ_min does not
vanish, is exactly where the target object has infinite ℓ¹_w norm (leg 51's finding, leg 55's
measurement) and where leg 52 measured the bordering repair failing.
8. Ceiling (pre-committed, NGX7)
The object is the a = 0 CLM linearisation. Y₀ is exactly zero because the anchor is
one basis mode, so the radii polynomial's root r = 0 is available for a degenerate reason and
certifies nothing. No dynamics were run. Nothing is claimed about HL_S2_nonsymmetric;
no link of the L1 → L4 chain moved, here or in 127 legs. A wall measured on this object
bounds the real target's difficulty from below, not from above. Nothing here lifts any ban
in plan_of_record.py, and Xu's own route to a computer-assisted proof (large-imaginary-part
resolvent bounds, trace-ideal membership, quadrature error in trace norm) is a different method
from this lane and is not a lift condition for any of them.