Abstract
Hadronic inhomogeneities are formed after the quark hadron phase transition. The nature of the phase transition dictates the nature of the inhomogeneities formed. Recently some scenarios of inhomogeneities have been discussed where the strange quarks are in excess over the up and down quarks. The hadronization of these quarks will give rise to a large density of hyperons and kaons in addition to the protons and neutrons which are formed after the phase transition. These unstable hyperons decay into pions, muons and their respective neutrinos. Hence the plasma during this period consists of neutrons, protons, electrons, muons and neutrinos. Due to the decay of the hyperons, the muon component of the inhomogeneities will be very high. We study the diffusion of neutrons and protons in the presence of a large number of muons immediately after the quark hadron phase transition. We find that the presence of the muons enhances the diffusion coefficient of the neutrons/protons. As the diffusion coefficient is enhanced, the inhomogeneities will decay faster in the regions where the muon density is higher. Hence smaller muon rich inhomogeneities will be completely wiped out. The decay of the hyperons will also generate muon neutrinos. Since the big bang nucleosynthesis provides constraints on the neutrino degeneracies, we revisit the effect of non zero degeneracies on the primordial elements.
Highlights
The quark hadron phase transition in the early universe resulted in the formation of hadrons at around 200 MeV
We have shown that baryonic inhomogeneities which have a larger number of muons decay faster compared to an inhomogeneities that are produced by a first order phase transition
It is quite possible that the muon density would be higher than the electron density in some of the inhomogeneities which are formed by the collapse of Z (3) domain walls
Summary
The quark hadron phase transition in the early universe resulted in the formation of hadrons at around 200 MeV. There have been discussions of antimatter domains formed after the quark hadron transition which produce a large number of pions [20,21]. We use the diffusion coefficient to study the decay of inhomogeneities in the era after the quark hadron phase transition. Since our basic starting point is the baryon overdense regions, we briefly discuss the formation of baryon overdensities and derive the diffusion coefficients of the nucleons through a plasma consisting of neutrons, protons, electrons and muons.
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