theory badges

838 public concepts

This index is navigation only; assess each concept and its sources before use.

1. B16 pp/pep weak-screening baseline audit — A classical Debye-Hueckel field is reconstructed from authenticated B16 temperature, density, and 29-species composition profiles; pp enhancement and pep suppression are kept as baseline diagnostics.
2. B16 and Solar Fusion II local pep/pp ratio closure — A versioned audit compares the local ratio reconstructed from B16 source fluxes and PEANUTS-hosted radial profiles with Solar Fusion II Eq. (46), restricted to its stated temperature domain.
3. Bahcall–May pep integral replay — The original 1969 pep/pp tree-rate phase-space integral is evaluated directly over the solar 10≤T6≤16 range and compared in one density convention with its own uncentered Eq.32 approximation and the centered Solar Fusion II Eq.41 tree expression.
4. Published pep temperature-factor convention — Bahcall's authenticated 1996 neutrino-flux subroutine and Solar Fusion I Eq.19 use an uncentered 1+0.02T6 factor. Solar Fusion II Eq.41 attributes a centered 1+0.02(T6−16) factor to Solar Fusion I, then carries that factor through its radiative correction to Eq.46; Solar Fusion III retains it. A versioned replay compares both forms with BP00, BS05 and B23 author pp/pep source tables inside the later review temperature domain.
5. Author B23/SF-III pep/pp ratio replay — SHA-256-authenticated Herrera–Serenelli v1.1 and v1.2 archives supply later-model source fluxes and normalized radial production profiles for a local-ratio comparison with the SFII/SFIII recommended formula, including all six v1.2 composition alternatives.
6. Author B23/SF-III pp–pep source covariance — The SHA-256-authenticated v1.2 author flux files supply a published pp–pep correlation and marginal source-flux errors for each of six separately named solar composition states.
7. B23/SF-III conditional two-channel source response — Author-used B16-derived or interpolated S11 logarithmic derivatives act on named B23 baseline fluxes; an explicit first-order pep direct-rate replacement exposes separate pp and pep weak-rate inputs.
8. B23/SF-III conditional electron source-to-rate replay — A versioned operator joins one frozen electron-dipole benchmark to conditional pp/pep weak-rate fractions, each named B23 composition's own source flux and radial profile, source-weighted MSW, and full-recoil Born scattering rates.
9. B23 pep capture-weighted source and radial MSW rate — A versioned conditional operator applies the original point-Coulomb capture weight to the same frozen electron-dipole pep spinor trace on each authenticated B23 radial state, then separates source normalization and profile-only MSW/Born response.
10. B23 paired thermal pp and capture-weighted pep source rates — One frozen electron coefficient supplies a point-Coulomb thermal pp weak fraction and a capture-weighted pep weak fraction on each same B23 composition. The pp thermal mean replaces the pep surrogate's stationary pp structural input before both channels reach radial MSW/Born rates.
11. Historical positive-probe B23 paired pp/pep source-to-hit ledger — The original B23-GS98 pp/pep first-order source, MSW matter and detector recoil ledger used positive-only Wilson vector/input quotients on the public Borexino hit axis. Seven components and four unresolved detector Z/W sign scenarios remain explicit.
12. Signed-slope B23 paired pp/pep partial hit ledger — The charged-source VnueduLL slope and six detector Vnue contact slopes are replaced by signed finite-difference responses in one B23-GS98 pp/pep source, MSW, recoil and 859-bin hit state; all four direct detector sign scenarios remain explicit.
13. B23 paired-hit ideal information with source covariance — A versioned Fisher operator applies the B23-GS98 pp/pep source covariance to two fractional source nuisances on the paired selected-hit spectra, with fixed, source-prior, free-source, and oracle-label comparisons for every provisional Z/W detector sign.
14. B23 pp/pep recoil-response matrix numerical closure — The same B23-GS98 pp/pep baseline and signed-WET detector contact spectra are folded through a replaceable true-recoil-to-hit matrix and compared with direct Gaussian response quadrature.
15. B23 paired pp/pep held-out fixed-fit public residual projection — The same-state B23-GS98 pp/pep selected-hit shift is compared bin by bin with the authenticated Borexino 2018 public residual and error arrays under a fixed published total fit. Four unresolved detector-sign choices and separate electron branches remain explicit.
16. Signed-WET B23 paired pp/pep public fixed-fit residual check — The corrected B23-GS98 pp/pep hit spectra are scored against the same authenticated Borexino 2018 public residuals and diagonal errors, holding the collaboration total fit fixed for all four unresolved detector signs and separate electron branches.
17. Corrected B23 public-bin fixed-fit influence audit — The corrected pp/pep model shift and the authenticated Borexino 2018 fit-derived residual are decomposed into per-bin contributions to the frozen diagonal score for all four detector-sign scenarios.
18. B23 pp joint-kernel Standard Model spectrum control — A point-Coulomb Maxwell–Gamow pp entrance distribution and allowed Standard Model lepton trace are mixed on the authenticated B23-GS98 radial state, then compared with Bahcall's separately calculated solar pp spectrum table.
19. B23 pp thermal mean-energy versus endpoint convention audit — Bahcall 1991's source-temperature formula is a mean-neutrino-energy change, while Bahcall 1997 applies a slightly different coefficient as an effective pp endpoint increment. A same-grid B23 allowed-current replay measures the actual mean change caused by that endpoint increment.
20. B23 pp Standard Model spectrum-choice hit control — The published pp neutrino spectrum and the independently modeled, unretuned B23 joint Standard Model spectrum are normalized on the same energy grid and folded through the same B23-GS98 flux, radial MSW state and approximate hit response.
21. B23 pp Solar Fusion III S-factor derivative shape control — The recommended total pp S-factor derivatives are divided by the lepton phase-space energy dependence already in the B23 joint kernel, and the residual entrance factor is propagated through the same B23-GS98 source mixture and pp energy grid.
22. B23 pp center-of-mass Doppler Standard Model spectrum control — The existing B23-GS98 conditional pp entrance and static allowed-current source kernel is convolved with its radius-dependent longitudinal proton-pair center-of-mass Maxwell velocity, then compared with the separately calculated Bahcall pp spectrum table.
23. B23 pp on-shell deuteron-recoil Standard Model spectrum control — The same B23-GS98 pp entrance state and allowed Standard Model current are recomputed with an on-shell recoiling deuteron, final-state phase space, and the energy-conservation Jacobian, then compared with Bahcall's separately calculated effective-endpoint spectrum.
24. B23 pp recoil plus center-of-mass Doppler Standard Model control — The on-shell deuteron recoil pp spectrum is boosted by the Gaussian proton-pair center-of-mass velocity while retaining its radius-dependent B23-GS98 recoil entrance probabilities.
25. B23 pp recoil-aware direct electron-dipole source term — Historical B23-GS98 pp recoil calculation of the frozen eW charged-W derivative interference and Standard Model allowed trace. Its direct charged-W vertex sign was superseded by the later action audit.
26. B23 pp recoil and CM Doppler direct electron-dipole shape — The frozen direct charged-W interference and Standard Model pp densities use the same analytic allowed trace, on-shell recoil solution, B23 radial entrance state, and leading center-of-mass energy boost.
27. B23 pp recoil-direct conditional MSW/Born rate — Historical B23 direct charged-W pp source projection through solar-flux normalization, radial production, MSW, and Born scattering. The direct source sign in its input was superseded by the charged-W action audit.
28. Action-repaired B23 pp direct source in true-recoil bins — Integrates the same conditional B23-GS98 pp flavor-energy kernels into arbitrary true-electron-recoil bins and reverses only the historical direct charged-W vertex sign verified by the action audit.
29. One-coefficient B23 pp direct source and detector true-recoil join — On the same frozen B23-GS98 pp flavor-energy state, the corrected direct-W source shift and action-defined direct Z/W detector shifts are integrated into identical true-electron-recoil bins.
30. Factorized B23 pep direct source and detector true-recoil join — The frozen electron coefficient and B23-GS98 radial state drive a Bahcall-May point-Coulomb pep source-energy distribution and action-defined direct Z/W detector shifts on one true-electron-recoil axis.
31. B23 on-shell pp tensor source column per unknown charged transition ratio — The frozen induced JMS tensor coefficient is multiplied by the exact leading allowed pp angular interference kernel and propagated through the same B23 entrance state, radius, adiabatic MSW map, true recoil and approximate selected hits as the direct pp source.
32. Factorized B23 pep tensor capture and pp-feedback hit columns — The same B23-GS98 factorized pep electron kernel as the saved direct source gives separate induced tensor columns for the unknown pep charged transition and for pp weak-rate feedback through the pep S11 flux response.
33. Paired B23 pp/pep action terms in an approximate common hit response — Each channel's source-W, detector-Z and detector-W true-recoil bins are folded by the same independently reconstructed Gaussian hit rule and then added on the public N_h axis.
34. Signed WET detector contact on the B23 512-bin pp/pep state — The pinned one-loop signed WET neutrino-electron vector coefficients generate separate pp and pep first-order detector-contact recoil bins, folded through the same approximate 859-hit response as the newer direct-action parent.
35. Independent electron coefficient in paired B23 pp/pep hit terms — The saved one-coefficient electron magnetic slope and separate Rb/Cs residuals scale the same 512-bin B23 pp and pep source-plus-direct-detector hit templates without consulting solar counts.
36. Frozen electron coefficient in paired B23 pp/pep two-tensor affine hit map — The saved direct pp/pep hit intercept and disjoint pp and pep tensor-source columns form an affine first-order hit prediction in two unassigned charged-transition ratios, scaled by each independent Rb/Cs electron coefficient.
37. B23 pp/pep two-tensor rate null and ideal hit-shape profile — The saved B23 paired hit columns admit an exact two-rate cancellation with two free tensor ratios, while a background-free Poisson projection leaves a nonzero 859-bin shape residual at the frozen electron coefficient.
38. B23 pp/pep same-current covariance transfer — An exact Jacobian transfers a caller-supplied six-coordinate axial/tensor current covariance into correlated pp/pep ratios, then into the frozen two-ratio B23 selected rates and hit shape.
39. B23 pep contact-cell partial hit derivative — A scalar pep-contact reweight, the common-current ratio derivative and the frozen B23 pep tensor hit column compose into a partial selected-hit derivative per radial cell weight.
40. B23 recoil-direct pp source in reconstructed Borexino hit bins — Historical B23 on-shell recoil pp direct source folded into approximate Borexino hit bins. Its direct charged-W source sign was superseded by the later action audit; the separate calculated-table Standard Model comparison remains a conditional control.
41. Historical positive-probe charged vector source term in B23 pp hit bins — The original positive-only JMS charged-vector quotient was propagated through the identical allowed Standard Model pp current and B23's pp S11 response to the recoil-aware hit spectrum.
42. B23 recoil pp source and detector first-order sign envelope — The frozen recoil-direct B23 pp source hit spectrum is added once to matched dimension-six detector contact and project-action direct Z/W recoil templates; direct detector signs remain a four-case convention envelope.
43. Independent electron branches in B23 pp source-detector hit predictions — Each separate Rb or Cs electron magnetic coefficient scales every frozen B23 pp source-plus-detector sign scenario and is added to its unperturbed absolute hit spectrum without a solar fit.
44. Held-out public-bin fixed-fit score for B23 partial pp branches — The frozen recoil-aware B23 pp source-plus-detector shift for each independent electron coefficient and detector-sign case is evaluated against the published 2018 total-fit residuals and diagonal errors on the exact public hit axis.
45. Independent electron coefficient in B23 pp recoil-direct hit bins — Each independently inferred electron magnetic Rb or Cs coefficient branch scales the same frozen direct one-W pp source hit template, with its signed 95% coefficient endpoints retained bin by bin.
46. B23 pp/pep direct electron-dipole pair — One frozen charged-W derivative coefficient drives the B23 pp recoil source and a point-Coulomb factorized pep capture source through the paired solar flux rule, radial MSW, and energy-dependent Born total scattering.
47. Historical positive-probe paired B23 pp/pep charged vector response — The original positive-only Wilson JMS charged left-vector probe was treated as a coefficient slope and propagated through the same leading allowed Standard Model current in pp and pep to 1-AU flux and ideal MSW/Born rates.
48. Signed-probe B23 pp/pep charged-vector source response — Three signed Wilson probes replace the historical positive-only VnueduLL quotient and carry its evaluated slope spread through the same leading allowed-current B23 pp/pep flux and ideal-rate state.
49. Held-out Borexino marginal rate-scale screen for B23 direct pair — The frozen B23-GS98 direct-only pp/pep total-scatter shifts are placed beside Borexino Phase-II high-Z-CNO-conditioned fitted-rate central values and separate marginal statistical errors, with no coefficient fit to those observations.
50. B23 pp static allowed-current energy-shape response — A zero-mean allowed spinor weight perturbs the published pp neutrino spectrum at the frozen electron coefficient and is projected with the authenticated B23 pp flux and radial MSW state into the public hit axis.

Diagnostic context only. Cite independent evidence for claims about the world.