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Numerical values of the planar microscopic radius-tail constants: C_*, whole-cluster split, C_2/C_0 and B_sign for the parent kernel (not certified; scientific effect NONE) #178
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Microscopic tail constants numerics: script, source map, README and r…
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Microscopic tail constants numerics: half-line quadrature for the eve…
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Microscopic tail constants numerics: RESULTS.json, NOTE.md and manifest
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Microscopic tail constants numerics: converged log-Z quadrature (ns =…
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Microscopic tail constants numerics: README run time; manifest
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Merge main (Math-#169, #176, #170 integrated; citation guide) into th…
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Microscopic tail numerics v3: pin merged [E], [Q]; check the exact cu…
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C6 planar tail numerics v3.1: apply R4/R5/R6 nonauthor reads (wording…
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Merge current main into PR178, preserving all seven reviewed packet f…
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| name: C6 microscopic tail numerics (replay) | ||
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| 'on': | ||
| pull_request: | ||
| paths: | ||
| - 'frontiers/c6_microscopic_tail_numerics_20260930/**' | ||
| - '.github/workflows/c6-microscopic-tail-numerics.yml' | ||
| - 'frontiers/two_scale_cluster_geometry_20260929/RADIAL_TAIL.md' | ||
| - 'frontiers/spectral_cluster_closure_20260929/PROOF.md' | ||
| - 'frontiers/c6_cluster_coefficients_numerics_20260930/RESULTS.json' | ||
| - 'frontiers/planar_cubic_cluster_20260929/PROOF.md' | ||
| - 'imports/lifetime_parent_20260925/UNIFORM_MATRIX_CAP_AND_LIFETIME.md' | ||
| - 'frontiers/extreme_cluster_sampling_20260930/PROOF.md' | ||
| - 'frontiers/radial_rate_20260930/PROOF.md' | ||
| workflow_dispatch: | ||
|
|
||
| permissions: | ||
| contents: read | ||
|
|
||
| jobs: | ||
| exact-controls-and-replay: | ||
| runs-on: ubuntu-latest | ||
| timeout-minutes: 20 | ||
| steps: | ||
| - uses: actions/checkout@11d5960a326750d5838078e36cf38b85af677262 | ||
| with: | ||
| persist-credentials: false | ||
| - uses: actions/setup-python@a26af69be951a213d495a4c3e4e4022e16d87065 | ||
| with: | ||
| python-version: '3.11.16' | ||
| - name: Verify manifest and main-resident pins, replay exact controls and sample kernels, reject mutants | ||
| env: | ||
| PYTHONDONTWRITEBYTECODE: '1' | ||
| run: | | ||
| set -euo pipefail | ||
| python -B -S - <<'PY' | ||
| import hashlib, json, pathlib, subprocess, sys | ||
| root = pathlib.Path('frontiers/c6_microscopic_tail_numerics_20260930').resolve() | ||
| manifest = json.loads((root / 'SOURCE_FILES.json').read_text())['files'] | ||
| present = sorted(p.name for p in root.iterdir()) | ||
| if present != sorted([e['path'] for e in manifest] + ['SOURCE_FILES.json']): | ||
| raise ValueError('packet tree differs from manifest: ' + repr(present)) | ||
| for entry in manifest: | ||
| path = root / entry['path'] | ||
| if pathlib.PurePosixPath(entry['path']).name != entry['path'] or path.is_symlink(): | ||
| raise ValueError('flat regular source required: ' + entry['path']) | ||
| data = path.read_bytes() | ||
| if len(data) != entry['bytes'] or hashlib.sha256(data).hexdigest() != entry['sha256']: | ||
| raise ValueError('source identity mismatch: ' + entry['path']) | ||
| pins = json.loads((root / 'SOURCE_MAP.json').read_text()) | ||
| for entry in pins['sources']: | ||
| if not entry['current_required']: | ||
| continue | ||
| data = pathlib.Path(entry['path']).read_bytes() | ||
| blob = hashlib.sha1(b'blob %d\0' % len(data) + data).hexdigest() | ||
| if len(data) != entry['bytes'] or hashlib.sha256(data).hexdigest() != entry['sha256'] or blob != entry['git_blob']: | ||
| raise ValueError('consumed source identity mismatch on this tree: ' + entry['path']) | ||
| script = str(root / 'tail_constants.py') | ||
| for flags in (['-B', '-S'], ['-B', '-O', '-S']): | ||
| out = subprocess.run([sys.executable, *flags, script, '--check'], cwd=root, capture_output=True, timeout=900) | ||
| if out.returncode != 0: | ||
| raise RuntimeError('check failed under ' + ' '.join(flags) + ': ' + out.stdout.decode()[-400:]) | ||
| for m in ['shape-integral', 'gamma-power', 'cusp-shift']: | ||
| rc = subprocess.run([sys.executable, *flags, script, '--check', '--mutant', m], cwd=root, capture_output=True, timeout=900).returncode | ||
| if rc != 1: | ||
| raise RuntimeError('mutant ' + m + ' not rejected') | ||
| print(json.dumps({'scientific_effect': 'NONE', 'certified': False})) | ||
| PY | ||
| git diff --exit-code | ||
177 changes: 177 additions & 0 deletions
177
frontiers/c6_microscopic_tail_numerics_20260930/NOTE.md
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| # Numerical values of the planar microscopic radius-tail constants for the parent kernel | ||
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| **Object:** `CL-C6-MICRO-TAIL-NUMERICS-20260930-v1`. **Author lane:** Anthropic / Claude. **Kind:** numerical note. | ||
| **Scientific effect:** NONE. **Certified:** no (deterministic Gauss quadrature with reported convergence; not an | ||
| enclosure). Third of the planar numerics notes after Math-#168 (near coefficients `alpha_1, alpha_2`) and | ||
| Math-#174 (remote coefficient `k integral_X Lambda`). | ||
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| ## 1. What is evaluated | ||
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| [R] (Math-#166, merged) proves for the already-formed limiting microscopic measure `M` (the `r -> 0` limit taken | ||
| first) the point-intensity radius tail | ||
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| F(t) = integral sum_i 1{R_i > t} dM ~ C_* t^(-11), | ||
| C_* = (216/11) k^7 (c_m/z_0) I J_cusp, I = 246528/35, (R13) | ||
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| with `J_cusp = integral H(h) gamma(a)^11 h_0(A_0, Rot_O tau_cusp) da dxi dh dO` (R12) and | ||
| `gamma(a) = sqrt(1 + (a/(12k))^2)`, and lists "no numerical value of its Gaussian integral" as a non-claim. The | ||
| companions Math-#169 ([E]) and Math-#176 ([Q]), both merged but still conditional (§5), express further constants of the same measure through | ||
| the same cusp integrals: the whole-cluster split of the tail (E6) and the second-order coefficient `C_2`, the | ||
| total-variation coefficient `kappa |C_2/C_0|` of the radial ratio and the signed constant `B_sign` ((13), (16), | ||
| (19)). This note evaluates all of them in the plane for the parent kernel `K(z) = exp(-|z|^2/2)` ([LP] §2). | ||
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| **Planar reduction.** In `d = 2` the spectral measure (17) of [SC] has `m = d - 1 = 1`, `c_1 = 1`, no hard | ||
| curvatures, and the Haar variable `O in O(1) = {±1}` averages trivially, because `p_odd` is invariant under | ||
| `(a, beta, c) -> (-a, beta, -c)`; `H(h) = 1`. Its density `h_0(A_0, tau)` at `A_0 = 0` is the raw contact density of | ||
| `(f_zz; f_xxz, f_xzz, f_zzz)` at `(0; a, beta, c)` given the contact pins `(f, f_x, f_z, f_xx, f_xz, f_xxx) = | ||
| (b, 0, 0, 0, 0, 12k)`, which by the exact regression of Math-#168 factors as `p_b(0) . p_odd(a, beta, c)` with | ||
| `p_b(0) = phi(b/sqrt2)/sqrt2` (the density of `f_zz | (f, f_xx, f_xz) = (b, 0, 0) ~ N(-b, 2)` at `0`) and | ||
| `p_odd = N(0, diag(2, 2, 6))`, for every `k, b`. These are the continuum jet covariances. For the periodized parent | ||
| kernel at side `L` they hold up to the lattice-moment deviation recorded by Math-#168 (`lattice_vs_continuum`: at | ||
| most `1.4e-13` at `L = 12, 24`; `L = 6` is not covered), so the values below are for the continuum covariance and | ||
| apply at `L >= 12`. Hence | ||
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| c_1 h_0(0, tau)/z_0 = [p_b(0)/z_0] p_odd(a, beta, c), p_b(0)/z_0 = phi(b/sqrt2) / (sqrt2 . 36 k^2 m_(2,b)), | ||
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| the prefactor of Math-#168, and `J_cusp(k) = integral gamma(a)^11 p_odd(a, a^2/(12k), a^3/(144k^2)) da` is a | ||
| one-dimensional Gaussian integral, `b`-free; all `b`-dependence of the constants sits in the prefactor. | ||
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| **Near-mass identity (control).** The same root-resolved integral (R11) without the radius indicator is the near | ||
| point mass `integral n dM = a_1 + 2 a_2`, `a_j = integral 1{n = j} dM` ([SC] (18), (20); `n <= 2` by the classifier of | ||
| [SC] §6), which at `d = 2` are Math-#168's `alpha_j` (the near part of `Lambda_1` in [CL] (1.6), Math-#159, not | ||
| pinned here): | ||
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| alpha_1 + 2 alpha_2 = 108 k^7 [p_b(0)/z_0] integral_S Q(u, v) integral_(Z != 0) |Z|^(-12) | ||
| integral p_odd(a, beta(u, v, Z, a), c(u, v, Z, a)) da dZ du dv, (N) | ||
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| with `beta = a^2/(12k) + k b_0(u)/Z^2`, `c = a^3/(144k^2) + a b_0(u)/(4Z^2) + 2k(v - b_0(u) u)/Z^3`. This | ||
| four-dimensional integral is evaluated independently here and compared with the merged Math-#168 values; agreement | ||
| is a consistency check between the [SC]/[R] parametrization (jet Jacobian `2`, root Jacobian `6`, weight `9`, multiplicity by the map) and the | ||
| [CL]/[CUB] parametrization of Math-#168, which integrates the classifier over the jets directly. | ||
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| ## 2. Exact structure | ||
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| - Shape integrals over `S = {-3/2 < u < 1/2, |b_0|/2 < v < 3 - 6u}` with `Q = (4v^2 - b_0^2)(b_0 - 4uv)`, in rational | ||
| arithmetic: `I = 246528/35`, `U_2 = integral u^2 Q = 240192/35`, `B = integral b_0 Q = -428544/7 = 3I - 12 U_2`, | ||
| `U_abs = integral |u| Q = 5898627/880` ([Q] (12)); `E eta = 5771/7062` under `Q/I` ([R] H3); the outer doublet | ||
| integral `J = 1083417/280` ([E] (E5), derived from the primitive (E20)); `11 U_2/(2I) = 4587/856`, `11 U_abs/(2I) = 4587821/876544` (author-side | ||
| corollary in Math-#176 comment 5903080058, not part of the pinned [Q] bytes). The inner doublet integral `D = 27066286003/223205220 - (79298560/4782969) log 2 = 109.7699503...` | ||
| ([E] E21) is quoted, not recomputed exactly (it was confirmed to `1e-13` by quadrature in the Slice C read). | ||
| - `kappa = (2/13)(11/13)^(11/2) = q_0^(-11) - q_0^(-13)` at `q_0 = sqrt(13/11)` ([Q] (16)). | ||
| - With the aligned planar cusp density ([Q] (21)–(22), `v_a = v_beta = 2`, `v_c = 6` for the continuum kernel): | ||
| `D_a G_0 = -[a^2/24 + a^4/(3456 k^2)] G_0 <= 0`, so `C_2 > 0`. | ||
| - Assembly (`K_0 = 108 k^7 p_b(0)/z_0`; `C_0` below is [E]'s per-shape amplitude, `C_* = C_0 I` is [Q]'s `C_0`): | ||
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| C_0 = (216/11) k^7 [p_b(0)/z_0] J_cusp, C_* = C_0 I, | ||
| G_max ~ C_0 (I - D), G_2 ~ C_0 J, B_2 ~ C_0 D, singleton ~ C_0 (I - D - J), | ||
| C_2 = K_0 [ U_2 T_1 + (2B/13) T_2 ], T_1 = integral gamma^9 (1 + 12A^2) G_0 da, T_2 = integral gamma^13 D_a G_0 da, | ||
| c = C_2/C_*, d_TV(R/t, Pareto_11) = kappa c t^(-2) + O(t^(-4)), | ||
| B_sign = (K_0/C_*) U_abs integral |A| gamma^10 G_0 da, A = a/(12k). | ||
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| Every integrand in `a` is even, so the integrals are taken on `[0, 14]` and doubled (this also removes the kink of | ||
| `|A|` at `0`); 96-point Gauss–Legendre, checked against 48 points. | ||
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| ## 3. Values | ||
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| **Cusp integrals** (`b`-free): | ||
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| | `k` | `J_cusp` | `T_1` | `T_2` | `integral |A| gamma^10 G_0` | max rel. dev. 48 vs 96 points | | ||
| |---|---|---|---|---|---| | ||
| | `0.5` | 0.0569758 | 0.0933384 | -0.0077782 | 0.0115205 | `1e-14` | | ||
| | `1.0` | 0.0485522 | 0.0561351 | -0.00467793 | 0.00468021 | `1e-15` | | ||
| | `2.0` | 0.0465858 | 0.0483768 | -0.0040314 | 0.0022051 | `2e-15` | | ||
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| **Tail constants** (`F(t) ~ C_* t^(-11)` is the `r^(-3)`-scaled expected number of near points at scaled radius | ||
| `R > t`; the split rows are values of [E] (E6); `c`, `kappa c`, `B_sign` of [Q] (13), (16), (19) (conditional on [E]/[Q]; see §5)): | ||
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| | `k` | `b` | `C_*` | `G_max` | `G_2` | `B_2` | singleton | `c = C_2/C_*` | `kappa c` | `B_sign` | | ||
| |---|---|---|---|---|---|---|---|---|---| | ||
| | `0.5` | `0.0` | 1.9297 | 1.8996 | 1.0601 | 0.030073 | 0.83957 | 9.7826 | 0.6 | 1.058 | | ||
| | `1.0` | `0.0` | 52.621 | 51.801 | 28.907 | 0.82006 | 22.894 | 6.9042 | 0.424 | 0.5045 | | ||
| | `2.0` | `0.0` | 1615.7 | 1590.5 | 887.55 | 25.179 | 702.95 | 6.2011 | 0.381 | 0.2477 | | ||
| | `0.5` | `1.0` | 0.55249 | 0.54388 | 0.30351 | 0.0086102 | 0.24038 | 9.7826 | 0.6 | 1.058 | | ||
| | `1.0` | `1.0` | 15.066 | 14.831 | 8.2763 | 0.23479 | 6.5549 | 6.9042 | 0.424 | 0.5045 | | ||
| | `2.0` | `1.0` | 462.58 | 455.37 | 254.11 | 7.209 | 201.26 | 6.2011 | 0.381 | 0.2477 | | ||
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| `c` and `B_sign` are `b`-free (the prefactor cancels); the ratios `G_max/C_* = (I-D)/I = 0.98442`, `G_2/C_* = J/I | ||
| = 0.54934`, `B_2/C_* = D/I = 0.015584` are universal. In `RESULTS.json`, `C2_over_C0` uses [Q]'s `C_0 = C_*`; | ||
| `C0_per_shape` is [E]'s `C_0`. The numbers satisfy the bounds of the Math-#176 author-side corollary (comment 5903080058; not in the | ||
| pinned [Q] blob): `c > 4587/856 = 5.3586` | ||
| and `0 < B_sign < 4587821/876544 = 5.2340`. Reading: at `k = 1`, `b = 0` the near point mass is `1.380` and `C_* = 52.6`, so the asymptotic law puts `C_* 2^(-11) = 0.026` (about `1.9%` of it) beyond twice the pin distance and `3e-4` beyond | ||
| three; the radial ratio's total-variation distance from Pareto(11) at threshold `t` is `0.42/t^2` to leading order | ||
| (`4.7%` at `t = 3`), and the signed-mark distance decays only like `0.50/t`. | ||
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| **Near-mass identity** (`alpha_1 + 2 alpha_2` from (N) at three shape-grid levels, against Math-#168): | ||
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| | `k` | (N) at 32/64/96 shape points (`ns = 160`) | (N), `b = 0` | Math-#168 GH60 | Math-#168 MC (s.e. of `alpha_1`) | rel. dev. vs GH60 / MC | | ||
| |---|---|---|---|---|---| | ||
| | `0.5` | 37.9952 / 37.871 / 37.8825 | 1.1874 | 1.1877 | 1.1844 (0.0027) | -2.67e-04 / +2.48e-03 | | ||
| | `1.0` | 175.923 / 176.071 / 176.082 | 1.3798 | 1.3801 | 1.3786 (0.0022) | -2.22e-04 / +8.33e-04 | | ||
| | `2.0` | 1119.62 / 1120.53 / 1120.7 | 2.1954 | 2.196 | 2.1948 (0.0033) | -2.34e-04 / +2.87e-04 | | ||
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| The shape-grid refinement at fixed `ns = 160` moves the integral by at most `3e-04` relative between the 64- and | ||
| 96-point levels (the sequence is monotone with observed order about 2 at `k = 2` and about 3.5 at `k = 1`, and is not | ||
| monotone at `k = 1/2`, so no order is claimed; the integrand has an integrable singularity at the corner | ||
| `(u, v) = (-1/2, 0)` of `S`, where the `|Z|`-scale of the Gaussian cutoff diverges), and the log-`Z` order is converged: at `32 x 32` shape points, | ||
| `ns = 64, 96, 160, 256` give `175.6152`, `175.9278`, `175.9235`, `175.9235` at `k = 1` (an under-resolved `ns = 64`, the order of the | ||
| first version of this note, biased the identity low by `1.8e-3`, exactly the deviation then reported; the `a`-order | ||
| `32` and `48` agree to all digits). At the finest level the identity lies within `1.1`, `0.5` and `0.2` Monte Carlo | ||
| standard errors of `alpha_1` of the Math-#168 values at `k = 1/2, 1, 2`, and within `2.7e-04`, `2.2e-04`, `2.3e-04` relative of the GH60 | ||
| values. This is the check that the two parametrizations agree; it is not a certification of either. | ||
| The deviations from GH60 are all negative and of the size of the remaining shape-grid movement of (N), which still | ||
| increases between the two finest levels; at `k = 2` the GH60 reference is itself not settled at this level (Math-#168 | ||
| §4: `J_2(2)` GH60 lies 3.2 MC s.e. below MC and the third digit of `alpha_2(2)` is not established, about `4e-4` | ||
| relative in `alpha_1 + 2 alpha_2`). | ||
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| ## 4. Precision (empirical, not bounds) | ||
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| - The one-dimensional cusp integrals agree between 48 and 96 Gauss–Legendre points to the relative deviations in | ||
| the table (all at most `1.3e-14`); the constants inherit that precision and the exact prefactor. | ||
| - Three exact identities stated in Math-#190 (elementary: `G_0 = exp(-12 k^2 (gamma^6 - 1)) / sqrt(192 pi^3)` on the | ||
| cusp, and `(a gamma^11)' = 12 gamma^11 - 11 gamma^9`) hold in this quadrature at machine precision and are | ||
| `--check` rules since v3: `T_2 = -T_1/12` (`< 3e-18` absolute at every `k`), `T_b sqrt(192 pi^3) = (12k^2 + 1)/(36k^3)` | ||
| (`8/9`, `13/36`, `49/288`; `< 6e-16`), and the rational factor `(11/2)(U_2 - B/78)/I = 66451/11128` of | ||
| `c = C_2/C_* = (66451/11128) T_1/J_cusp` (exact). Since `T_1/J_cusp = 12 - 11 I_9/I_11 in (1, 12)`, Math-#190 | ||
| reports (information only, not consumed here) the bounds `5.9715 < c(k) < 71.658`, which would sharpen the corollary | ||
| `c > 4587/856`; the floating-point values here (`9.78`, `6.90`, `6.20`) lie inside. | ||
| - Math-#190 (reviews/c6_tail_constant_certified_20260930, other Claude session; merged 2026-10-01 at `77b854c` as a review | ||
| record filed as certified-arithmetic information, not a promotion; not consumed here) | ||
| reports certified interval enclosures of every constant of this table and finds each value of `RESULTS.json` | ||
| (blob `0b5ce76f`) within `9e-16` relative of its enclosure. That record is information for the reader; it is not a | ||
| certification of this note, which stays floating point. | ||
| - The near-mass integral moves by at most `3e-04` relative between the 64- and 96-point shape levels at `ns = 160`, | ||
| and by `4e-09` between `ns = 160` and `256`; its remaining error is of the former order, below the Math-#168 Monte | ||
| Carlo standard error. | ||
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| ## 5. What the numbers are not | ||
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| Not a proof and not an enclosure. `C_*` is a value of the reviewed formula (R13) of the merged [R]; the split and the | ||
| second-order/signed constants are values of formulas of [E] (Math-#169) and [Q] (Math-#176). Both are merged on main | ||
| after scoped nonauthor review, but their pinned bytes keep the disposition 'author-side conditional proof candidate' | ||
| and their source hypotheses remain. These values are therefore conditional on [E] and [Q] and their sources, | ||
| evaluated at their stated scope (planar, `r -> 0` first), with continuum spectral moments and no finite-`L` | ||
| periodization correction. Planar only (`d = 2`), parent | ||
| kernel only, aligned frame; no rate for `r -> 0`, no finite-`r` statement, no statement about the remote singleton | ||
| population. No register, catalog or STATUS change. Same GitHub account as every lane; zero | ||
| organizational-independence credit. The author will not merge. | ||
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| ## 6. Provenance | ||
|
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| `tail_constants.py` (standard library; `--check` replays the exact controls, the cusp integrals and the complete | ||
| constants table for each `k` and both `b`, the low-level near-mass integral for each `k` with its log-`Z` study | ||
| entry, the assembly of the identity from the stored numbers, the identity tolerance against `RESULTS.json`, and the | ||
| three exact identities of §4; mutants `shape-integral`, | ||
| `gamma-power`, `cusp-shift` exit 1), `RESULTS.json` (full run, about fifteen minutes), `SOURCE_MAP.json` | ||
| (pins [R], [SC], [NUM], [CUB], [LP], [E], [Q] on `main` `3e0a91b`, all workflow-checked; [E] and [Q] were unmerged | ||
| companions in v1/v2 and were promoted to pins in v3 with their blobs unchanged), | ||
| `SOURCE_FILES.json`, workflow `c6-microscopic-tail-numerics.yml`. | ||
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| Revision v3.1 (Slice C review 5974193134 on Math-#178, findings F1–F8, wording only): [E]/[Q] values are stated as | ||
| conditional although both are merged; the corollary bounds are attributed to Math-#176 comment 5903080058, not to the | ||
| pinned [Q]; Math-#190 is recorded as merged at `77b854c` and its bounds as information only; precision `1.3e-14`; | ||
| near point mass `1.380` (`C_* 2^(-11)` about `1.9%` of it); the two `C_0` conventions in `RESULTS.json` named; | ||
| continuum spectral moments stated. With the Slice A review 5974218952 (F1–F3): the planar regression is stated as the | ||
| continuum covariance, valid at `L >= 12` by the Math-#168 lattice control; the trivial `O(1)` average is named; `J` | ||
| is cited at [E] (E5). With the Slice B review 5974449197 (F1–F4): no convergence order is claimed for the shape grid; | ||
| the sign and size of the GH60 deviations are explained; the `±` is the MC standard error of `alpha_1`; the identity is | ||
| derived from the pinned [SC], with [CL] (1.6) cited as context only. `RESULTS.json` and `tail_constants.py` unchanged. |
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| # Planar microscopic radius-tail constants (parent kernel, d = 2) | ||
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| **Object:** `CL-C6-MICRO-TAIL-NUMERICS-20260930-v1`. **Author lane:** Anthropic / Claude. **Kind:** numerical note | ||
| (deterministic Gauss quadrature with reported convergence; no proof, no enclosure). **Scientific effect:** NONE. | ||
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| Evaluates, for the parent kernel `exp(-|z|^2/2)` in the plane, the point-intensity tail constant `C_*` of the | ||
| already-formed microscopic measure ([R] (R13); `F(t) ~ C_* t^-11`), the whole-cluster split of that tail | ||
| (Math-#169, merged; values conditional on it), the second-order coefficient `C_2/C_0`, the TV coefficient `kappa |C_2/C_0|` and | ||
| the signed constant `B_sign` (Math-#176, merged; values conditional on it), for `k in {1/2, 1, 2}` and `b in {0, 1}`. In `d = 2` | ||
| the [SC] measure reduces to the exact contact regression of Math-#168, so every constant is a one-dimensional | ||
| Gaussian integral; the four-dimensional near-mass identity `alpha_1 + 2 alpha_2 = K_0 int Q |Z|^-12 p_odd` is | ||
| evaluated as a control against the merged Math-#168 values. | ||
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| - `NOTE.md` — what is evaluated, exact structure, values, precision, non-claims. | ||
| - `tail_constants.py` — standard-library script (Python `>= 3.11`): `--check` (exact controls and replay against | ||
| `RESULTS.json`, including the exact cusp identities `T_2 = -T_1/12`, `T_b sqrt(192 pi^3) = (12k^2+1)/(36k^3)`), full run regenerates `RESULTS.json` (about fifteen minutes); `--mutant {shape-integral, gamma-power, | ||
| cusp-shift}` must exit 1. | ||
| - `RESULTS.json`, `SOURCE_MAP.json` (seven main-resident pins: [R], [SC], [NUM], [CUB], [LP], [E], [Q]), `SOURCE_FILES.json`. | ||
| - Workflow `.github/workflows/c6-microscopic-tail-numerics.yml` replays manifest, pins, both check modes and the | ||
| mutants. | ||
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| Same GitHub account as every other lane; zero organizational-independence credit. The author will not merge. |
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