Before electron-positron annihilation in cosmology, photons and electron-positron pairs share a temperature. Their effective entropy degrees of freedom areAfter annihilation the electromagnetic plasma contains only the two photon polarizations, so . The already decoupled neutrinos receive none of this entropy and simply cool as . Applying cosmological entropy conservation separately to the coupled electromagnetic plasma giveswhereas . Division yields the Cosmic neutrino background temperature
The energy density from a phase-space distribution function with internal states isIn the ultrarelativistic limit , set . The Fermi-Dirac distribution then givesSince ,
When , the Fermi-Dirac distribution approaches the step function for and zero for . For one internal state and negligible mass, the degenerate relic neutrino energy density is thereforeso .
At thermal equilibrium, the antineutrino chemical potential is . Its occupation is approximately , givingIt is exponentially smaller than the neutrino density; this particle-antiparticle imbalance is a cosmological lepton asymmetry.
Write the neutrino degeneracy parameter as . Requiring one degenerate species not to exceed today's critical density givesUsing ,Several equally degenerate species would strengthen the bound by the fourth root of their number.
A large neutrino degeneracy parameter raises the relativistic energy density and therefore the expansion rate. Big Bang nucleosynthesis tests this through primordial light-element abundances; an electron-neutrino chemical potential also shifts neutron--proton chemical equilibrium directly. The Cosmic microwave background power spectrum tests the changed expansion rate, matter-radiation equality, sound horizon, damping scale, and neutrino anisotropic stress. Finally, large-scale structure of the universe and the matter power spectrum test the altered equality scale and neutrino free streaming. These observables distinguish a degenerate-neutrino cosmology from the standard thermal relic scenario in complementary epochs.
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