Baryogenesis

The placed census is one proton mass per tube, split evenly: under [M packaging]. Telescope counts stay [O residual]. In that package the global totals of baryon number, lepton number, and charge are zero. The figure is the retired external target, not this census. The sketch below is an older Chern–Simons estimate. It is not the placed account.

Drainage of the same half-filling

Thermodynamic drainage length is packaging of the half-filling above. It is not a second census. The neck depth is [E algebra] of the clothes lock [M]. Discrete survey containment in is [M packaging]. Local neutrality is [M packaging] of capture plus positron clearance. None of these rows writes . The census token stays unissued. Prospective telescope counts stay [O residual].

Chern-Simons Dynamics and Sakharov Conditions

During the nucleation of the S³ universe from a topological bubble, the Chern-Simons number undergoes rapid change. Since is not conserved during topology change, this naturally fulfills the first of Sakharov's conditions.

• Baryon number violation: Topological transitions on the S³ boundary violate baryon number.
• C and CP violation: While CPT is a discrete symmetry, C is broken by the Hopf orientation of the nucleating bubble.
• Out of equilibrium: The bubble nucleation event is rapid and far from thermal equilibrium.

The Rate Asymmetry

The CS term in the S³ action introduces a bias in the pair creation rate between matter and antimatter states during the rapid bubble growth phase. This leads to a rate asymmetry:

This leads to a numerical estimate for the baryon-to-photon ratio today:

The Asymmetry Carrier

While the rate asymmetry is established, the exact physical mechanism that converts this topological preference into a specific baryon orientation is the subject of the ongoing BN4 (Bubble Nucleation) programme.