Artian's HVP Source-Access Reference Framework
When an HVP row matches the area better than the shape, the next object is the camera. Version: 41.01 Concept DOI: 10.5281/zenodo.20732034 Author: Ali Attar Website: quantumtraction.org Main book anchor: Quantum Traction Theory: Main Book v10.01 For the BaBar \(e^+e^-\to\pi^+\pi^-\) row, the same full covariance packet splits the comparison into an integrated \(a_\mu\) direction and a shape-orthogonal line-shape direction: \[ \boxed{ \chi^2_{\rm full} = z_{a_\mu}^{2}+\chi^2_{\rm sh}. } \] In the primary window \(0.600<\sqrt{s}<0.880\,{\rm GeV}\), the scalar row is moderately pulled, \[ \boxed{ z_{a_\mu}=-1.9753069836215, \qquad p_{a_\mu}=0.04823332120278627, } \] while the identity-camera line-shape sector is severely stressed: \[ \boxed{ \chi^2_{\rm sh}(I)=58495.38442559397, \qquad \nu_{\rm sh}=139, \qquad \chi^2_{\rm sh}(I)/\nu_{\rm sh}=420.8301037812516. } \] Version 41.01 defines the legal BaBar access-camera object \[ \boxed{ \mathcal C_{\rm BaBar}^{\rm QTT}: R_{2\pi}^{\rm src,QTT}(s) \longmapsto R_{2\pi}^{\rm lab/BaBar}(s), } \] with the source held fixed: \[ \boxed{ {\partial R_{2\pi}^{\rm src,QTT}\over \partial\mathcal C_{\rm BaBar}^{\rm QTT}}=0. } \] The new v41.01 witness is the family-transfer gate: \[ \boxed{ \mathfrak W_{\rm cam}^{41.01} \left( \mathcal C_{\rm BaBar}^{\rm QTT} \right) = \left( Q_{\rm family}, Q_{\rm no\ row\ rescue}, Q_{\rm source\ frozen}, Q_{\rm direct\ scan\ block}, Q_{\rm blinded\ transfer} \right). } \] For same-family ISR/radiative-return rows, the camera must transfer through row metadata and declared correction conventions, not through the row residual: \[ \boxed{ d\in\mathcal F_{\rm ISR} \Longrightarrow \mathcal C_{d}^{\rm QTT} = \mathcal T_{d\leftarrow{\rm BaBar}}^{\rm cam} \mathcal C_{\rm BaBar}^{\rm QTT}, \qquad {\delta\mathcal T_{d\leftarrow{\rm BaBar}}^{\rm cam}\over \delta\{\mathbf y_d,\mathbf r_d\}}=0. } \] Direct-scan rows are not allowed to inherit the BaBar ISR camera without their own camera theorem: \[ \boxed{ d\in\mathcal F_{\rm scan} \Longrightarrow \mathcal C_{d}^{\rm QTT}\ne \mathcal T_{d\leftarrow{\rm BaBar}}^{\rm cam} \mathcal C_{\rm BaBar}^{\rm QTT}. } \] The green condition remains strict: \[ \boxed{ Q_{\rm green}=1 \iff \mathcal C_{\rm BaBar}^{\rm QTT}\in\mathfrak K_{\rm BaBar}^{\rm QTT}, \quad \mathfrak W_{\rm cam}^{41.01}=1, \quad \chi^2_{\rm sh}(\mathcal C_{\rm BaBar}^{\rm QTT}) \le \chi^2_{0.95}(139). } \] A map that only rescues BaBar is not a QTT access theorem; it is a row-local correction. The next executable step is to derive the bounded BaBar ISR camera, run the same covariance statistic, and test a blinded same-family transfer before assigning the remaining stress to the source. Main status labels: SIGMA-HVP-BABAR-ACCESS-CAMERA-MAP-CLOSURE-THEOREM-CLOSED SIGMA-HVP-CAMERA-TRANSFER-WITNESS-THEOREM-CLOSED SIGMA-HVP-BABAR-ONE-ROW-RESCUE-FIREWALL-CLOSED SIGMA-HVP-DIRECT-SCAN-NONTRANSFER-GUARDRAIL-CLOSED SIGMA-HVP-CAMERA-SYSTEMATIC-DOUBLE-COUNT-FIREWALL-CLOSED SIGMA-HVP-BABAR-ACCESS-CAMERA-NUMERICAL-DROP-PENDING SIGMA-HVP-CAMERA-TRANSFER-NUMERICAL-EXECUTION-PENDING Included files: PDF paper, Version 41.01 Release ZIP containing LaTeX source, verifier scripts, CSV/JSON certificates, figures, render audit, and SHA-256 manifest
Authors
- Attar Ali (ORCID: https://orcid.org/0009-0008-9931-2691)
Institutions
- Oldham Council (GB)
Publication Details
- Journal
- Zenodo (CERN European Organization for Nuclear Research)
- Published
- 2026-06-29
- DOI
- https://doi.org/10.5281/zenodo.21031423
- Primary Topic
- Image Processing Techniques and Applications
- Type
- preprint