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838 public concepts

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  1. Conditional pp/pep tensor-null rate contrast — One linear combination of the provisional pp and pep electron-dipole rate shifts cancels their common allowed tensor-to-axial ratio at first order, with separate selected-hit and full-recoil weights.
  2. Fixed-fit projection of the electron template onto public Borexino residuals — The authenticated published standardized residuals and bin errors are compared with the provisional pp/pep hit shift while holding the collaboration's published total fit fixed.
  3. Independent-electron uncertainty in the public fixed-fit score — Separate conditional Gaussian Rb and Cs coefficient distributions are propagated through each detector-sign scenario's fixed-fit public-bin quadratic score, retaining their shared electron-input covariance without pooling them.
  4. Conditional ideal information in Borexino pp/pep hit bins — A background-free Poisson model computes local information in the currently included electron-dipole pp/pep hit templates at fixed tensor ratio, across detector-sign choices, and after profiling a formal unrestricted tensor amplitude within each sign scenario.
  5. Conditional ideal hit information with separate pp/pep tensor slopes — Versioned background-free Poisson operators project the provisional frozen-coupling hit intercept away from independent pp and pep tensor-current slopes in the same selected Borexino hit bins, including four unresolved direct detector-sign alternatives.
  6. Flat 5D electroweak Pauli operators retain two independent dipoles — In a specified flat S1/Z2 electroweak field content, two independent gauge-invariant 5D Pauli terms reduce to independent 4D Warsaw eW and eB zero-mode coefficients. Their map has rank two; compactification does not fix their signed ratio.
  7. Candidate five-dimensional parent for the electron weak dipole — A compact 5D electroweak field content and its independent Pauli zero-mode terms are specified, but a predictive parent still needs fixed boundary data and a signed full 4D Warsaw loop match with correlated independent observables.
  8. LSND electron-neutrino electron total-cross-section precision — LSND reported a nu_e e total-cross-section slope of 10.1 with 1.1 statistical and 1.0 systematic uncertainties in units of 10^-45 cm²/MeV.
  9. Frozen electron weak-dipole direct-term LSND reach screen — Across a sampled 18–52.8 MeV neutrino-energy grid, the included direct Z/W scattering terms give at most a 6.37e-12 fractional total-cross-section shift at the largest primary electron-only coefficient endpoint, over four unresolved sign cases.
  10. XENONnT and PandaX-4T 2026 solar pp-equivalent fit inputs — XENONnT reported a 1–140 keV recoil ROI and a 10.2±2.0e10 cm^-2 s^-1 pp-equivalent flux; PandaX-4T reported a 20–1000 keV ROI and an 8.5±3.5e10 cm^-2 s^-1 combined pp-equivalent flux.
  11. Frozen direct Z/W pp free-electron recoil-window contrast — At kappaW(1 TeV)=1e-12 GeV^-2 and kappaB=0, the conditional direct detector fractional pp shifts are -1.879219473e-12 for 1–140 keV and -1.549871522e-12 for 20–1000 keV, giving an ideal pure-pp flux-ratio contrast of -3.293479519e-13.
  12. Electron-centered cross-scale weak/dipole theory gate — A new common mechanism requires an explicit Lorentz- and gauge-consistent term that predicts independent neutrino and magnetic observables from one frozen coupling.
  13. Independent CeB charged massless gauge matching column — A zero charged tree branch generates a separately calculated one-loop charged coefficient through its neutral/scalar source diagrams and off-diagonal source renormalization.
  14. Bounded independent EW CeW/CeB charged and photon source matrix — The two EW Wilson inputs map into the charged gauge component and tree photon source with distinct columns; the mixed-accuracy source map does not supply a full physical transport vector.
  15. Electron-photon dipole and Fermi bilocal charged soft kernel — The neutral photon component of the same CeW action is a second tree LEFT source whose product with the Fermi operator supplies a separately calculated local charged derivative counterterm.
  16. Ordered massless charged gauge finite block with explicit hard-soft matching — Calculated boxes and covariant source contacts cancel the retained gauge dependence and admit a bounded finite physical-D gauge projection in the fixed scheme.
  17. Internal-vector source triangle resolves the charged UV inventory failure — A previously absent proper lepton triangle has an independently calculated tensor and charge factor; it removes the retained local UV residual in the declared mass-independent gauge projection.
  18. Open-line charged UV audit with unresolved cancellation failure — Routed d-dimensional lepton triple and contact contractions, alongside a provisional current/field ledger, expose a residual requiring reconciliation before finite matching can be admitted.
  19. Bosonic W two-point function with Rxi and FJ pole checks — The full bosonic transverse W diagram and one-point set has an independently checked momentum-dependent function, a UV-finite two-point subtraction and bounded massive-gauge pole tests.
  20. Bosonic charged finite-part projection with explicit UV remainder — Calculated W/input and covariant-source functions supply a finite-part slice whose nonzero local UV/scale residue and gauge dependence remain explicit requirements on the missing amplitude classes.
  21. Explicit GF-MW-alphabar electroweak input and tadpole map — A declared hybrid input scheme supplies dependent parameters and bare-parameter counterterm identities while retaining the archive's unspecified finite conversion and independent Wilson boundary.
  22. Charged dipole closed-fermion two-point and input completion — The declared hybrid scheme has a computed closed-fermion W/H/source/input class with UV, tadpole and corresponding Wilson-running cancellations; remaining bosonic and open-line finite EW classes are uncomputed.
  23. Charged D7 one-loop EW/LEFT hard and soft subblocks — The direct EW-scale eW source has a calculated zero pure-QCD hard remainder and a selected heavy-top W-bubble hard amplitude; the complete finite EW coefficient and input conversion remain unresolved.
  24. Charged D7 genuine derivative-EV finite insertion block — Six independent d-dimensional rank-chain derivative sources have calculated finite physical insertions and three executed mixed-gauge domains; higher input ranks, non-Abelian/source closure and finite EW matching remain open.
  25. Charged D7 finite mass-current evanescent insertion subblock — D-dimensional ordered chains give checked finite evanescent-to-physical current rows and a defined comparison-basis conversion; genuine derivative and finite EW/source matching remain explicit unknowns.
  26. Charged D7 QCD derivative mixing and fixed-order physical logarithms — Calculated one-gluon poles and mass-source factors preserve the previous EOM quotient and protect the complete D source, while a separate conditional EW boundary projection leaves finite and d-dimensional matching open.
  27. Charged D7 photon poles and physical derivative/mass basis — Direct external-photon insertions and unshelled four-point tensors close a ten-direction physical basis; five EOM directions yield a checked one-loop physical logarithm, with d-dimensional and finite/source closure open.
  28. Charged derivative one-loop QED projected UV subblock — A convention-pinned partonic charged operator, all six photon topologies and field factors yield a checked simple-pole projection; evanescent, full off-shell and physical matching/radiation closure remain open.
  29. Installed charged-vector matching precision and derivative-origin inventory — Signed W/B scans, high-precision Standard Model subtraction, separate running controls and analytic dependency tracing qualify an installed dimension-six vector map while preserving strict-order zeros and open dimension-seven/radiative terms.
  30. Neutron leading scalar and tensor charge admission with marginal uncertainty — Primary three-flavor MSbar QCD lattice charges at 2 GeV are substituted in the frozen finite-mass tree matrix; marginal endpoint maps and a declared Cartesian scenario retain missing covariance and symbolic current terms.
  31. Neutron charged low-energy operator response matrix — Finite-mass tree spectrum and electron-direction correlation relative to neutron spin are calculated for charged vector, scalar, pseudoscalar, tensor and derivative structures, with one-nucleon scalar/tensor form factors left symbolic.
  32. Inclusive neutron SM electron-track radiative kernel with independent axial matching — An additive Coulomb, inclusive virtual/real outer-radiative and first-recoil SM kernel gives finite electron-energy bins and a rate family depending on an unresolved lattice-to-decay axial/vector matching parameter.
  33. Free-neutron SM and direct leptonic-dipole benchmark — A spin-resolved covariant constant-form-factor amplitude yields a finite-mass electron spectrum, total tree rate and electron-direction asymmetry relative to neutron spin, with independent real 1 TeV eW/eB response columns.
  34. Beta-decay mass, charge and spin-sector controls — Sourced masses allow neutron, pp and pep conversion but forbid free-proton beta-plus decay and both deuteron beta breakups; number-conserving magnetic precession cannot create their final particles.
  35. Geometric origin of beta conversion remains open — The diagnostic calculation assumes the SM charged current. A common-spinor construction must still supply a charge-conserving transition Hamiltonian, changing-particle-number state space and independently fixed couplings before it can explain weak decay.
  36. Distance-normalized solar irradiance and 7Be detector-rate overlap — Join real TSI and published solar-neutrino detector-rate bins on their common dates, and remove the shared Earth-distance factor before inspecting a residual association.
  37. GP bulk sound speed — Squared long-wavelength sound speed of a uniform contact-interacting condensate.
  38. GP bulk healing length — Squared healing length under the conventional GP factor-of-two definition.

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