The impact of new d(p,γ)3 rates on Big Bang Nucleosynthesis
We consider the effect on Big Bang Nucleosynthesis (BBN) of new measurements of the d(p,γ) 3 cross section by the LUNA Collaboration. These have an important effect on the primordial abundance of D/H which is also sensitive to the baryon density at the time of BBN. We have re-evaluated the thermal r...
Gespeichert in:
Veröffentlicht in: | Journal of cosmology and astroparticle physics 2021-03, Vol.2021 (3), p.46 |
---|---|
Hauptverfasser: | , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | We consider the effect on Big Bang Nucleosynthesis (BBN) of new measurements of the
d(p,γ)
3
cross section by the LUNA Collaboration. These have an important effect on the primordial abundance of D/H which is also sensitive to the baryon density at the time of BBN.
We have re-evaluated the thermal rate for this reaction, using
a world average of cross section data, which we describe with
model-independent polynomials; our results are in good agreement with a similar
analysis by LUNA.
We then perform a full likelihood analysis
combining BBN and
Planck
cosmic microwave background (CMB) likelihood chains
using the new rate combined with previous measurements and compare with the results using previous rates. Concordance between BBN and CMB measurements of the anisotropy spectrum using the old rates was excellent. The predicted deuterium abundance at the Planck value of the baryon density was (D/H)
BBN+CMB
old
= (2.57 ± 0.13) × 10
−5
which can be compared with the value determined from quasar absorption systems (D/H)
obs
= (2.55 ± 0.03) × 10
−5
. Using the new rates we find (D/H)
BBN+CMB
= (2.51 ± 0.11) × 10
−5
.
We thus find consistency among BBN theory, deuterium and 4 observations, and the CMB, when using reaction rates fit in our data-driven approach. We also find that the new reaction data tightens the constraints on the number of relativistic degrees of freedom during BBN, giving the effective number of light neutrino species N
ν
= 2.880 ± 0.144 in good agreement with the Standard Model of particle physics.
Finally, we note that the observed deuterium abundance continues to be more precise than the BBN+CMB prediction, whose error budget is now
dominated by d(d,n)
3
and d(d,p)
3
H.
More broadly, it is clear that the details of
the treatment of nuclear reactions and their uncertainty have become critical for BBN. |
---|---|
ISSN: | 1475-7516 1475-7516 |
DOI: | 10.1088/1475-7516/2021/03/046 |