log-convexity controls only the monotonicity of $\Lambda_k$ and gives no control at all over the multiplicity $\mathfrak N_k$ — high spectral frequency can perfectly well coexist with unbounded multiplicity, so spectral cascade does not imply physical concentration, which is the core no-go of the all-order effective-volume route. Decomposing the direct-gate ratio into an order penalty $2^k$, a physical-multiplicity factor $\mathfrak N_k^{1/3}$, and a spectral-peak mismatch, it is shown that even under perfect single-cell concentration ($\mathfrak N_k\sim1$), the bare $2^k$ factor alone can still make the fixed-order gate fail at high order — direct failure at high order does not equate to packet multiplicity. Next, the more favorable chain scale from Theorem 3.14 is tested: **C5-H.3 Volume-Only Chain No-Go** uses the same wave-packet model to prove that — even for a chain theorem whose asymptotic-critical exponent genuinely tends to zero — closing it at high order via a coarse global volume certificate generally still fails (the theorem constant itself grows like $k^2$, overwhelming any gain from pure volume alone). §24–25 explain the geometric reason: what Theorem 3.14 actually exploits is component/sign one-dimensional micro-geometry (rapid sign alternation, filamentary geometry, directional oscillation), which global volume simply cannot see — small volume is a sufficient certificate of 1D sparseness, not the full geometry the theorem actually uses. The genuine positive fact that survives (**C5-H.4**): the gap between the chain and a priori exponents, $1/[(k+1)(2k+3)]\sim1/(2k^2)\to0$, does genuinely tend to zero — if a survivor could maintain any fixed positive concentration-gain exponent, and the theorem-constant burden were negligible, the chain spatial condition would eventually be crossed — but (**C5-H.5** and what follows) if the theorem constant or the multiplicity $\mathfrak N_k$ grows fast enough in step, it can completely overwhelm this vanishing exponential gap — a vanishing exponent gap does not imply automatic regularity. A multi-packet realization example (§36) further shows that $N$ mutually distant, approximately disjoint copies of the same wave packet let $\mathfrak N_k$ simply multiply by $N$ without changing the derivative spectral scale, continuing the "carrier multiplicity" theme that has run throughout C3/C4. **C5-H.6 Static All-Order Volume Closure No-Go** formally declares: a static all-order effective-volume closure scheme is a methodological dead end; the direct gate should remain a fixed-order "kill switch," not the main engine for automatic order escalation; the correct high-order asymptotic object must instead turn to what Grujić–Xu's paper genuinely relies on and C5 has not yet made rigorous: component/sign one-dimensional micro-geometry + Type-A/B derivative chains + harmonic-measure compatibility. Formally hands off to C5-I — Derivative Sign-Geometry Defects, Chain Sections, and Harmonic-Measure Compatibility, with 8 targets left to prove.">
← NS_O / 44 / C5-H: All-Order Effective-Volume Defects, Spectral–Multiplicity Ladders, and Asymptotic-Critical Compatibility
C5-G obtained the first theorem-ready fixed-order direct gate. C5-H asks: if a hypothetical survivor keeps $\mathfrak G_k^{dir}>1$ at every fixed $k$, can a purely volume-based argument push this all the way to $k\to\infty$ to force a contradiction? The answer is no — and not only does the fixed-order direct route fail, so does the asymptotically favorable chain route, on pure volume alone. First, an honest theorem audit: the spatial scale in Grujić–Xu's (2024) Theorem 3.5 carries a $2^{-k}$ factor, and the admissible later-time window carries a $4^{-k}$ factor — this is an exponential penalty built into the published theorem itself, not a product of C5's methodology. An explicit purely illustrative smooth single-scale analytic wave-packet model is constructed (explicitly stated to be not an N–S counterexample, only an illustrative no-go): **C5-H.1 All-Order Direct-Gate No-Go** proves that even for the most favorable smooth, single-scale data, the coarse volume certificate still forces $\mathfrak G_k^{dir}$ to diverge exponentially in $k$; §8 further proves the admissible time window itself undergoes exponential Zeno-type contraction, which cannot be made to vanish simply by raising the order. To study the all-order spectral ladder, the $L^2$ Fourier moment $M_k=\||\xi|^ku\|_2^2$ is introduced, and **C5-H.2** (Cauchy–Schwarz) proves $M_k^2\le M_{k-1}M_{k+1}$, forcing the spectral frequency $\Lambda_k$ to be monotonically increasing. But then comes the round's central no-go: using the Agmon inequality to decompose the effective volume exactly into "spectral-cell scale × physical multiplicity" $r_{eff,k}=\mathfrak N_k^{1/3}\Lambda_k^{-1}$, log-convexity controls only the monotonicity of $\Lambda_k$ and gives no control at all over the multiplicity $\mathfrak N_k$ — high spectral frequency can perfectly well coexist with unbounded multiplicity, so spectral cascade does not imply physical concentration, which is the core no-go of the all-order effective-volume route. Decomposing the direct-gate ratio into an order penalty $2^k$, a physical-multiplicity factor $\mathfrak N_k^{1/3}$, and a spectral-peak mismatch, it is shown that even under perfect single-cell concentration ($\mathfrak N_k\sim1$), the bare $2^k$ factor alone can still make the fixed-order gate fail at high order — direct failure at high order does not equate to packet multiplicity. Next, the more favorable chain scale from Theorem 3.14 is tested: **C5-H.3 Volume-Only Chain No-Go** uses the same wave-packet model to prove that — even for a chain theorem whose asymptotic-critical exponent genuinely tends to zero — closing it at high order via a coarse global volume certificate generally still fails (the theorem constant itself grows like $k^2$, overwhelming any gain from pure volume alone). §24–25 explain the geometric reason: what Theorem 3.14 actually exploits is component/sign one-dimensional micro-geometry (rapid sign alternation, filamentary geometry, directional oscillation), which global volume simply cannot see — small volume is a sufficient certificate of 1D sparseness, not the full geometry the theorem actually uses. The genuine positive fact that survives (**C5-H.4**): the gap between the chain and a priori exponents, $1/[(k+1)(2k+3)]\sim1/(2k^2)\to0$, does genuinely tend to zero — if a survivor could maintain any fixed positive concentration-gain exponent, and the theorem-constant burden were negligible, the chain spatial condition would eventually be crossed — but (**C5-H.5** and what follows) if the theorem constant or the multiplicity $\mathfrak N_k$ grows fast enough in step, it can completely overwhelm this vanishing exponential gap — a vanishing exponent gap does not imply automatic regularity. A multi-packet realization example (§36) further shows that $N$ mutually distant, approximately disjoint copies of the same wave packet let $\mathfrak N_k$ simply multiply by $N$ without changing the derivative spectral scale, continuing the "carrier multiplicity" theme that has run throughout C3/C4. **C5-H.6 Static All-Order Volume Closure No-Go** formally declares: a static all-order effective-volume closure scheme is a methodological dead end; the direct gate should remain a fixed-order "kill switch," not the main engine for automatic order escalation; the correct high-order asymptotic object must instead turn to what Grujić–Xu's paper genuinely relies on and C5 has not yet made rigorous: component/sign one-dimensional micro-geometry + Type-A/B derivative chains + harmonic-measure compatibility. Formally hands off to C5-I — Derivative Sign-Geometry Defects, Chain Sections, and Harmonic-Measure Compatibility, with 8 targets left to prove.
Relationship to the rest of the series, stated as closely as possible in the document's own words, not my interpretation.
'high spectral frequency does not imply physical concentration — volume-only certificate is too coarse, even to certify Theorem 3.14's chain scale in general.' — excerpted from Sections 16 and 23 of this paper.
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