3.1. Big Bang Nucleosynthesis (BBN)
It is reassuring that the same baryon abundance b h2 = 0.0214 ± 0.0020 implied by the deuterium abundance D/H in low-metallicity Lyman limit systems in quasar spectra  agrees with that implied by the relative heights of the first two peaks in the WMAP angular power spectrum , giving b h2 = 0.0224 ± 0.0009. This is also in agreement with the baryon abundance deduced from clusters  and with the lower limit from the opacity of the Lyman alpha forest . However, there are uncertainties in the measured deuterium abundance evolution , and potential problems - or perhaps clues to new physics - in discrepancies between the observed helium and lithium abundances and the predictions of BBN.
The abundance by mass of 4He measured in low-metallicity ionized regions in nearby galaxies implies an extrapolated primordial abundance Yp = 0.2421 ± 0.0021 according to the latest published data , which corresponds according to standard BBN to a baryon abundance b h2 = 0.012+0.003-0.002, lower by about 3 than the value just mentioned from D/H and CMB measurements. It remains to be seen whether this could be remedied by improved analyses (for example, based on more realistic models of these low-metallicity galaxies or of their HII regions), or alternatively whether it is perhaps an indication of problems with standard BBN.
The D/H  b in standard BBN implies a primordial 7Li/H 3.3 - 6.0 × 10-10, in serious disagreement with the value of 7Li/H = 1.23+0.34-0.16 × 10-10 measured in atmospheres of galactic halo metal-poor stars in the "Spite plateu" (i.e. with metallicity [Fe/H] less than about -2) . It disagrees even with the puzzlingly higher value 7Li/H = 2.19+0.30-0.27 × 10-10 from a sample of globular cluster stars . It is possible that some of the 7Li in such stars is destroyed by astration, consistent with the small range of 7L abundance in the Spite plateau stars , but this may not resolve the discrepancy.
These disagreements call into question the usual assumptions of standard BBN, for example, the assumption of no significant electron neutrino asymmetry and N = 3 light neutrino species . However, an alternative possibility that might neatly account for the 7Li discrepancy is the injection of energetic nucleons around 1000 s after the big bang, for example due to decay of the next-to-lightest supersymmetric partner particle into the lightest one .