Baryon Asymmetry, Dark Matter and Quantum Chromodynamics
David H. Oaknin, Ariel Zhitnitsky
TL;DR
The paper presents a cosmological scenario in which the baryon asymmetry and dark matter originate from a charge separation at the QCD phase transition, with dense color superconducting CS lumps (and anti-lumps) forming alongside ordinary hadrons. The global baryon number is taken to be zero, while net hadronic baryons arise in the visible phase and opposite charge is sequestered in CS dark-matter lumps; the observed ratio $\Omega_{DM}/\Omega_B$ and $n_B/n_{\gamma}$ emerge from the same QCD-scale physics. The authors analyze the microphysics of quark reflection at CS interfaces, demonstrating that low-energy quarks are strongly reflected (suppressing annihilation) while higher-energy modes can transmit, enabling charge exchange that drives phase separation. They outline the necessary conditions (Sakharov-like criteria) and spatial-scale hierarchies, provide rough estimates for the baryon-to-photon ratio, and discuss observational constraints and potential experimental tests (COSLAB) to validate or falsify the scenario. Overall, the work offers a QCD-based mechanism linking baryogenesis to dark matter via phase separation at the QCD transition, with testable implications for cosmology and astrophysics.
Abstract
We propose a novel scenario to explain the observed cosmological asymmetry between matter and antimatter, based on nonperturbative QCD physics. This scenario relies on a mechanism of separation of quarks and antiquarks in two coexisting phases at the end of the cosmological QCD phase transition: ordinary hadrons (and antihadrons), along with massive lumps (and antilumps) of novel color superconducting phase. The latter would serve as the cosmological cold dark matter. In certain conditions the separation of charge is C and CP asymmetric and can leave a net excess of hadrons over antihadrons in the conventional phase, even if the visible universe is globally baryon symmetric $B = 0$. In this case an equal, but negative, overall baryon charge must be hidden in the lumps of novel phase. Due to the small volume occupied by these dense lumps/antilumps of color superconducting phase and the specific features of their interaction with "normal" matter in hadronic phase, this scenario does not contradict the current phenomenological constrains on presence of antimatter in the visible universe. Moreover, in this scenario the observed cosmological ratio $Ω_{DM}\simΩ_{B}$ within an order of magnitude finds a natural explanation, as both contributions to $Ω$ originated from the same physics during the QCD phase transition. The baryon to entropy ratio $n_{B}/n_γ\sim 10^{-10}$ would also be a natural outcome, fixed by the temperature $T_f \simlt T_{QCD}$ at which the separation of phases is completed.
