Interaction geometry

Topic navigation; Research index lists all notes.

• Question — Research record, section 1: Question.

• Two different notions of encounter — Research record, section 2: Two different notions of encounter.

• Electron-electron scattering is therefore not the same as electron-electron full-depth contact — Research record, section 3: Electron-electron scattering is therefore not the same as electron-electron full-depth contact.

• General depth-mediated interaction rule — Research record, section 4: General depth-mediated interaction rule.

• First comparison with the observed interaction pattern — Research record, section 5: First comparison with the observed interaction pattern.

• Next proof obligations — Research record, section 11: Next proof obligations.

• Central full-depth dynamics does not by itself prove unobserved-visible coincidence — Research record, section 14: Central full-depth dynamics does not by itself prove unobserved-visible coincidence.

• A stronger invariant candidate from two complex structures — Research record, section 18: A stronger invariant candidate from two complex structures.

• Exchange symmetry and Pauli suppression of full-depth contact — Research record, section 19: Exchange symmetry and Pauli suppression of full-depth contact.

• Generalization to unequal particle depths — Research record, section 20: Generalization to unequal particle depths.

• Present verdict — Research record, section 24: Present verdict.

• Pair-invariant collapse on the electron sector — Research record, section 25: Pair-invariant collapse on the electron sector.

• Direct projection of the current V2 scalar quartic into a two-electron channel — Research record, section 26: Direct projection of the current V2 scalar quartic into a two-electron channel.

• Historical quadratic kernel as a candidate pre-contact force — Research record, section 28: Historical quadratic kernel as a candidate pre-contact force.

• First direct verdict on $K_{66}$ from presently written V2 — Research record, section 29: First direct verdict on $K_{66}$ from presently written V2.

• Electromagnetic pre-contact steering: a dimensional Green-function test — Research record, section 30: Electromagnetic pre-contact steering: a dimensional Green-function test.

• A useful decomposition of the electromagnetic problem — Research record, section 31: A useful decomposition of the electromagnetic problem.

• Can a pulled-back depth-two connection reduce unobserved transverse momentum? — Research record, section 32: Can a pulled-back depth-two connection reduce unobserved transverse momentum?.

• Consequence for the original electron-beam proposal — Research record, section 33: Consequence for the original electron-beam proposal.

• Updated verdict after testing the current scalar and electromagnetic sectors — Research record, section 34: Updated verdict after testing the current scalar and electromagnetic sectors.

• Projector-dynamics audit of the remaining unobserved-steering channel — Research record, section 35: Projector-dynamics audit of the remaining unobserved-steering channel.

• Next proof obligation — Research record, section 37: Next proof obligation.

• Nuclear radiation benchmark — Recoil does not cancel a neutral pair's relative electric dipole, while ordinary proton polarization gives a tiny fixed-radius cancellation benchmark rather than a universal V2 bound.

• Nuclear response feedback — A reciprocal electron–nuclear polarization model produces retarded feedback and coupled modes, with energy-checked evolution of circular and petalled preparations.

• Nuclear stability test — Coherent radiation and passivity impose a precise dark-mode condition for persistent dipole motion, while the ordinary proton benchmark falls far short of cancellation.

• Orbit current projection — A conserved electromagnetic source requires a specified current projection, not identification with the detector-averaged orbit image.

• Orbit electromagnetic spectrum — Circle, petalled, and detuned actual orbits give distinct conditional radiation diagnostics and finite-generator constraints on electromagnetic probes.

• Projected Dirac current — Varying a minimally gauged diagnostic action fixes the current form and normalization identities, while projection exposes missing-mode contributions.