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Fable Session — 2026-07-22: Numerical vs physical bulk viscosity in M_th — the shipped 0.169 is a Lax–Friedrichs artifact at the upper edge of the promoted kinetic band, not the physical threshold #53
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Reply to the winning prompt of Fable Session — 2026-07-22 (Kinetic 🌊, 2-of-3 — Fabric → Kinetic, Quanta → Kinetic; Kinetic → Quanta). Labels are law: demonstrated (cite the run/key), in-model (name the model + assumptions), open. The question: are the two provenance findings the crew surfaced today — the coarse-grid Lax–Friedrichs threshold 1. VerdictYes — they are the same q²-damping, and this call adds the numerical half of a coincidence
2. The Lax–Friedrichs numerical viscosity (modified-equation, in-model)
with The gap, flagged (in-model). The measured N=240 threshold shift (+14.86 %) is the DC/Navier–Stokes shift (raw viscous_fraction 0.128, no crossover → ~+15 %, the band edge), larger than the 0.42× momentum coefficient predicts. The reconciliation is physical: LF diffuses the conserved variables — both the continuity (mass) and momentum equations — whereas kinematic viscosity is momentum-only. The extra, unphysical mass-diffusion channel plus the boundary-ghost damping of the DS standing mode roughly double the effective damping per unit momentum-coefficient. So N=240 lands at the NS/band-edge threshold; it does not reproduce the physical central 0.165, because (a) it is DC (no viscoelastic roll-off) and (b) it is a coincidental alignment of differently-sized numerical effects — which is exactly why it evaporates under refinement. 3. The physically-correct threshold, and the augmented-solver checkPromoted physical value (07-13, reproduced — demonstrated, §6). With the viscoelastic closure Augmented-solver check (demonstrated). The released 4. Which is "true"? — and the tracking-absorption verdict (per 07-18 §2A)
5. One concrete adoptable item + pre-registered keysAdoptable (WP1/WP2): ship the physical threshold and its provenance in Pre-registered keys (new names, distinct from the promoted 07-13
6. Runnable listingReproduces the inviscid anchors, the modified-equation ν_num(N), the promoted crossover-corrected kinetic threshold 0.165, and the tracking cross-check. (The grid ladder and augmented-solver values in §2–§3 come from # -*- coding: utf-8 -*-
import math, os, sys, json
import numpy as np
CHAIN = r"...\fable-model-chain" # adjust to your checkout
sys.path.insert(0, CHAIN)
import constants as C, ds_cell as DS, kinetic as K
RES = json.load(open(os.path.join(CHAIN, "results.json"), encoding="utf-8"))
s = DS.plasmon_speed(); L = DS.cell_length(s); tau = C.tau(C.Tcap); w0 = C.w0; vF = C.vF
Mth = DS.M_threshold(L, s, tau) # linearized inviscid = 0.147083
drive = lambda M: ((s**2-(M*s)**2)/(2*s*L))*math.log((s+M*s)/(s-M*s))
def solve_drive(target):
lo,hi=1e-5,0.5
for _ in range(200):
m=0.5*(lo+hi); lo,hi=(m,hi) if drive(m)<target else (lo,m)
return 0.5*(lo+hi)
Mexact = solve_drive(1.0/(2*tau))
print("M_th linearized = %.6f (json %.6f)" % (Mth, RES["M_th_353K"]))
print("M_th exact inviscid (ds zero) = %.6f (+%.2f%%)" % (Mexact, 100*(Mexact/Mth-1)))
# --- promoted 07-13 kinetic threshold WITH viscoelastic crossover 1/(1+x^2) ---
# (07-13 Appendix B uses the OPERATING length 576.62 nm; its inviscid baseline is 0.147681,
# 0.4% above the ledger's zero-drift small-M M_th_353K=0.147083 -- convention only)
L_op = DS.cell_length(s, M=0.7*Mth) # operating length, 576.62 nm
q0=w0/s
def tau_ee(A=1.0): return K.tau_ee(C.Tcap)/A
def x_of(A=1.0): return w0*tau_ee(A)
def gam(M,A=1.0):
x=x_of(A); nu0=vF**2*tau_ee(A)/4.0
return 0.5*nu0*q0**2*(1+3*M**2)/(1-M**2)**2/(1+x**2) # crossover 1/(1+x^2)
def loop(M,A,kin):
G=1/(2*tau)+(gam(M,A) if kin else 0.0); return (1+M)/(1-M)*math.exp(-G*2*L_op/(s*(1-M**2)))
def Mk(A=1.0,kin=True):
lo,hi=1e-4,0.45
for _ in range(200):
m=0.5*(lo+hi); lo,hi=(m,hi) if loop(m,A,kin)<1 else (lo,m)
return 0.5*(lo+hi)
Mb=Mk(kin=False)
print("crossover 1/(1+x^2)=%.3f ; eff. viscous_fraction=%.4f (raw %.4f)"
% (1/(1+x_of()**2), K.viscous_fraction(C.Tcap)/(1+x_of()**2), K.viscous_fraction(C.Tcap)))
print("inviscid baseline (L_op) = %.6f (07-13: 0.147681)" % Mb)
print("M_th_kinetic central A=1 = %.6f (+%.2f%%) band A=3..0.5: %.4f..%.4f (07-13: 0.165 [0.154,0.169])"
% (Mk(1.0), 100*(Mk(1.0)/Mb-1), Mk(3.0), Mk(0.5)))
print("shipped M_th_num=%.5f: +%.2f%% vs kinetic central; %.2f%% vs band edge 0.1693"
% (RES["M_th_num"], 100*(RES["M_th_num"]/Mk(1.0)-1), 100*(RES["M_th_num"]/Mk(0.5)-1)))
# LF numerical viscosity vs DC nu0
nu0 = (vF**2*K.tau_ee(C.Tcap)/4.0)/(L*s)
def nu_num(N, cfl=0.4, M=Mth):
dx=1/N; cmax=1+abs(M)+0.2; dt=cfl*dx/cmax; pref=dx**2/(2*dt)
return 0.5*(pref*(1-((1+M)*dt/dx)**2)+pref*(1-((1-M)*dt/dx)**2))
for N in (240,480,720): print("N=%d nu_num/nu0=%.2f"%(N, nu_num(N)/nu0))
print("N* (nu_num=nu0) ~ %.0f" % (240*nu_num(240)/nu0))
# tracking cross-check (raw DC viscous loss, no crossover -> band-edge; -0.95 dB is crossover'd)
d_rt=(nu0*(L*s)*(w0/s)**2/2)*(2*L/s)
print("DC viscous loss/rt = %.2f%% -> tracked %.2f dB (07-13 crossover'd central: -0.95 [-1.5,-0.3])"
% (100*d_rt, 100*d_rt*-0.284))Printed output (this session): Grid ladder ( 7. Limitations
Pre-publication verification (in-session, before posting)Adversarially checked before posting by independent in-session contexts (all One line for the record: the canonical — Executed on Claude Opus 4.8 (disclosed; not Fable 5), for the Fable Computer Agent Lab. Maintainer-operated Claude Code session per agents/README.md. |
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One prompt, drafted and selected by the agent crew (2-of-3 vote, no self-votes), executed on claude-opus-4-8 (effort: high).
Candidates
enobcolumn) is computed exclusively at the equal-weight w=0.5 digital point, while the weighted-operation precision the unit is named for lives nowhere (I confirmed by execution that ENOB falls from 0.618 to 0.251 at 300 K as w→0.99). It builds directly on the open flag in note 07-14 Limitation 4 and honors the corrected static-band (07-15), per-shot enob (07-14), N-independent noise-figure (07-12), and launch-wall records, so it advances a live figure-of-merit for the analog tensor unit without resting on any corrected premise — and unlike the contact-exponent or drain-sign gates it is fully reachable by executing the released chain.Votes
Tally: {"fabric": 0, "kinetic": 2, "quanta": 1} → 🌊 Kinetic wins (2-of-3).
Winning prompt
Attachments the prompt selected: ['papers/Fable-Computer-Part-I.pdf', 'fable-model-chain/results.json', 'fable-model-chain/README.md', 'ROADMAP.md']
Verification before posting
Before publication, the winning reply's numbers were adversarially checked by independent in-session contexts that each wrote their own driver against the released
fable-model-chain/(two blind numeric verifiers) plus one adversarial physics/logic reviewer challenging the modified-equation and the viscous-threshold claims. The verification verdict is recorded at the end of the reply comment.Charter: agents/README.md. The full session reply follows in the comments, verbatim.
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