Manuscript Em02-B@1 · Em02-B-v1.tex · 1347253e
Em02-B Computational Evaluation of Simulated Crossed Families Weighted atomic cone integrals, localization audits, and one simulated non-tip adjoint
Records simulated quadrature of the Em02-A formulas on declared crossed families. The cutoff constants, the weighted atomic cone integral, and one scalar non-tip adjoint are numerical values of this simulated data. Gauss and Sobol agreement is an independent quadrature of a closed-form atomic integrand. That agreement is not the seven-dimensional seed integral. The isolated 5a seed integral changes sign under refinement, so no row value is released. Those numbers are not the physical smoothing scale and not a physical coefficient. Target I isolation is not Target II coincidence and is not this quadrature. Em01-G's isolated failure is not imported. The identification ledger, the seven-row physical pairing, S2, and authorization remain unresolved. The stops at H2, I3, and J2 remain unresolved. XV-B is not opened. No quantum coefficient is admitted. No compilation is asserted. No symbolic execution is claimed.
Front matter
abstractAbstractFront matter · lines 42–82
Open as its own pageThis note records the audit in
results/tables/audit_manifest.json, source identifier1eeba3536183. Fifteen unit tests passed. The runner label issingular_diagnostic; the admission field isnot_claimed. A configuration labelledphysical_identifiedis rejected byrequire_simulated.For the cutoff in the package, and . The chart formula agrees to . At fixed , the mesh residual falls from at nodes to at nodes, which supports a grid-bias reading of the earlier stable residual. The amplitude probe has exact target , independent of .
The weighted atomic integral at is by a Gauss cap rule and by a scrambled Sobol rule on nodes. The relative gap is . These quadratures do not share nodes. A scalar simulated integral on equals . No inherited physical coefficient is claimed. The subsequent isolated-row run, source
05485aec7a9a, builds the specialized vertex and both adjoint constructions. They agree termwise to . The seven-dimensional seed integral changes sign from to to as the -node count goes from 5 to 7, so no row value is released. The later overlap reduction separates that failure from the inner integral. At the factored inner value is , and a 16-node overlap-box rule agrees to0.28\%. The outer cone rules do not: Gauss gives and Sobol stays near . The row remains unreleased.
Scope
sectionScopeScope · Em02-B@1#conv:simulated · lines 86–100
Open as its own pageThe physical ledger of Em02-A-v6 remains open. The package evaluates simulated data only. The obsolete shared-node value is not a result of this revision: that sum used an inserted null node and a single panel width. It is not in the manifest.
Every stored run carries
smooth_benchmark,singular_diagnostic, ormanufactured_cancellation.physical_identifiedraisesRuntimeError.
Localization
sectionLocalizationLocalization · lines 101–134
Open as its own pageThe five-cone mass at fixed rescaled resolution, not a refinement in , gives residual against at .
The chart residual at those scales stays near on an -node mesh. Holding and refining the mesh gives
nodes scaled integral residual against The residual shrinks as the mesh is refined. That supports grid bias. It does not by itself prove the bias model; it is the check the previous note lacked.
For , the scaled probe equals exactly, before quadrature error. The trapezoidal values are , , and . The drift is consistent with amplification of a small cone-mass error after subtraction, not with failure of the localization identity.
Weighted atomic integral
sectionWeighted atomic integralWeighted atomic integral · Em02-B@1#eq:atomic · lines 135–169
Open as its own pageThe passive -cone is weighted by , and . The angular factor on that cone is the sphere probability. The dynamical integral is
with the translated atomic profile and . The site is , , so is future null. Route B is a Gauss rule on the cap containing the mollifier support: nodes. Route A is a scrambled Sobol rule of length on the same cap and does not call Route B.
profile Gauss Sobol Absolute gaps are and . Relative gaps are about
0.11\%and0.14\%. A coarser Gauss rule, , differs from a rule by1.5\%relative. This is an independent quadrature check of a closed-form integrand. It is not the seven-row pairing: the vertex and the component adjoint are not in .
Simulated non-tip adjoint
sectionSimulated non-tip adjointSimulated non-tip adjoint · lines 170–182
Open as its own pageWith and unit scalar -factors, the displayed reduces to for . Derivatives are taken before the chart evaluation. On and transverse radius at most , with density at ,
dblquadreturns , error estimate . This is simulated scalar data, not the inherited component map.
Ledger
sectionLedgerLedger · lines 183–210
Open as its own pageResult Status , , chart twin Values of this Mesh residuals shrinking at fixed Supports grid bias Probe against the exact -free target Quadrature check Gauss/Sobol atomic integral Independent quadrature of S1 Scalar non-tip Simulated adjoint, one row Seven-row physical pairing, S2, authorization Not executed boundary. Numbers are tied to the named manifest and to fifteen passed tests. No physical admission is claimed.
Package boundary
remarkRemarkPackage boundary · Em02-B@1#conv:package · lines 212–228
Open as its own pageThe Python package that wrote the named manifest is archived from
https://github.com/cheungngo/Em02-B. That archive is package evidence. It is not a theorem of this note, and it is not a certificate.require_simulatedrejectsphysical_identified. The later filerow5a_05485aec7a9a.jsonrecords that the seven-dimensional seed integral changes sign, sorow_value_releasedstays false. The Gauss–Sobol statusindependent_quadrature_of_closed_form_atomic_integrandis not that seed integral. The outer cone rules do not agree. No physical admission is claimed. No compilation is asserted.bibliographyReferencesPackage boundary · lines 230–233
Open as its own pageEm02A
N. Cheung, Em02-A, version 6. Formula source.