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We review results from QCD axion string and domain wall simulations and propagate the associated uncertainties into the calculation of the axion relic density. This allows us to compare different results in the literature and, using cosmological constraints, to perform statistical inference on the axion mass window in the post-inflationary Peccei-Quinn symmetry breaking scenario. For dark matter axions, this leads to a median dark matter axion mass of 0.50 meV, while the 95% credible interval at highest posterior density is between 0.48 and 0.52 meV. For simulations including string-domain wall decays, these numbers are 0.22 meV and [0.16, 0.27] meV. Relaxing the condition that axions are all of the dark matter, the axion mass window is completed by an upper bound of around 80 meV, which comes from hot dark matter constraints. This demonstrates, at least from the statistical perspective, that the axion mass can be constrained rather precisely once it is possible to overcome the much larger systematic uncertainties.
The cosmological scenario where the Peccei-Quinn symmetry is broken after inflation is investigated. In this scenario, topological defects such as strings and domain walls produce a large number of axions, which contribute to the cold dark matter of
An axion-like particle (ALP) with mass $m_phi sim 10^{-15}$eV oscillates with frequency $sim$1 Hz. This mass scale lies in an open window of astrophysical constraints, and appears naturally as a consequence of grand unification (GUT) in string/M-theo
We present a new mechanism to deplete the energy density of the QCD axion, making decay constants as high as $f_a simeq 10^{17},rm{GeV}$ viable for generic initial conditions. In our setup, the axion couples to a massless dark photon with a coupling
We study the formation and evolution of topological defects in an aligned axion model with multiple Peccei-Quinn scalars, where the QCD axion is realized by a certain combination of the axions with decay constants much smaller than the conventional P
We study the topological susceptibility in 2+1 flavor QCD above the chiral crossover transition temperature using Highly Improved Staggered Quark action and several lattice spacings, corresponding to temporal extent of the lattice, $N_tau=6,8,10$ and