Abstract

Current upper bounds of the neutron electric dipole moment constrain the physically observable quantum chromodynamic (QCD) vacuum angle θˉ1011|\bar\theta| \lesssim 10^{-11}. Since QCD explains vast experimental data from the 100 MeV scale to the TeV scale, it is better to explain this smallness of θˉ|\bar\theta| in the QCD framework, which is the strong \Ca\Pa problem. Now, there exist two plausible solutions to this problem, one of which leads to the existence of the very light axion. The axion decay constant window, $10^9\ {\gev}\lesssim F_a\lesssim 10^{12} \gevfora for a {\cal O}(1)initialmisalignmentangle initial misalignment angle \theta_1,hasbeenobtainedbyastrophysicalandcosmologicaldata.For, has been obtained by astrophysical and cosmological data. For F_a\gtrsim 10^{12}GeVwith GeV with \theta_1<{\cal O}(1)$, axions may constitute a significant fraction of dark matter of the universe. The supersymmetrized axion solution of the strong \Ca\Pa problem introduces its superpartner the axino which might have affected the universe evolution significantly. Here, we review the very light axion (theory, supersymmetrization, and models) with the most recent particle, astrophysical and cosmological data, and present prospects for its discovery.Comment: 47 pages with 32 figure

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    Last time updated on 02/01/2020