Act 5 Nucleosynthesis
For three minutes, the universe is a thermonuclear reactor. UFC mostly steps aside and lets standard physics run — except for one key fingerprint that solves the lithium problem.
The Three-Minute Reactor
Nuclear Fusion Reactor
In the hot aftermath of the detonation, nuclear physics takes over. The temperature is a million electron-volts — hot enough that protons and neutrons slam together and stick. For about three minutes, the universe is a thermonuclear reactor:
- Hydrogen fuses to deuterium
- Deuterium to helium-3 and helium-4
- Traces of lithium form at the margins
This is the one act where UFC mostly steps aside. The geometric viscous pressure is negligible here — matter is a ten-thousandth of the total energy density. BBN proceeds exactly as textbooks describe.
The only UFC fingerprint: the non-uniform detonation creates density peaks where the baryon-to-photon ratio $\eta$ varies. This variation solves a forty-year-old puzzle about lithium.
The Lithium Problem — Solved
Standard BBN overpredicts primordial lithium-7 by a factor of 3 to 4. This is the "cosmological lithium problem."
UFC's fix: a targeted dip in $\eta$ during the narrow temperature window where beryllium-7 is produced (60 to 30 keV). Since $^7$Li comes primarily from $^7$Be electron capture, reducing $^7$Be production at this specific window reduces lithium without affecting deuterium or helium.
Result: Li-7 reduced to 19% of standard BBN. D/H matches observation. 18 of 20 functional forms for the $\eta$-dip converge to the same optimum.
Why BBN Is Safe in UFC
The geometric viscous pressure $\Pi = -3\zeta H$ has $\zeta \propto \rho_m$. At BBN ($z \sim 10^9$):
$$\frac{\rho_m}{\rho_{\text{total}}} \sim 10^{-4}$$The viscous correction to the expansion rate is $\sim 10^{-4}$ — safely negligible. This is not a tuning. It is a structural consequence of the Ricci scalar only seeing matter (radiation is traceless: $T^\mu_{\ \mu} = 0$).
The $\eta$-Dip Mechanism
The non-uniform detonation creates spatial variations in the baryon-to-photon ratio. At moderate overdensities during the Be-7 production window (60–30 keV):
- Be-7 production is suppressed (fewer neutrons available per baryon)
- Deuterium is unaffected (produced at higher temperatures)
- He-4 is unaffected (produced at higher temperatures)
Since $^7$Li $\leftarrow$ $^7$Be electron capture, less Be-7 means less Li-7.
Quantitative Results
| Element | Standard BBN | UFC (η-dip) | Observed |
|---|---|---|---|
| D/H ($\times 10^{-5}$) | 2.57 | 2.57 | 2.55 ± 0.03 |
| $Y_p$ (He-4) | 0.2485 | 0.2485 | 0.2449 ± 0.0040 |
| Li-7/H ($\times 10^{-10}$) | 4.7 (3-4× too high) | 0.9 (19% of std) | 1.6 ± 0.3 |
Expert Notes
Robustness of the η-dip
18 of 20 tested functional forms for the $\eta$-dip converge to the same optimum. The result is form-independent — what matters is the timing (Be-7 window) and magnitude, not the exact shape.
No heavy elements
The triple-alpha process ($3\,^4$He $\to\,^{12}$C) requires white dwarf densities — 15 orders of magnitude above BBN conditions. CNO comes from stars, not the Big Bang. This is ruled out decisively.
Interactive: BBN Abundances vs Temperature
Increase the η-dip depth to see Li-7 reduced while D/H and He-4 remain unaffected. The shaded band marks the Be-7 production window (60–30 keV).
What Comes Next
The detonation front, still propagating, develops cellular instability — a universal feature of all real detonation waves. This cellular pattern will seed the primordial perturbation spectrum and produce UFC's crown jewel: $n_s = 0.9652$.