We propose a QCD axion model where the origin of PQ symmetry and suppression of axion isocurvature perturbations are explained by introducing an extra dimension. Each extra quark–antiquark pair lives on branes separately to suppress PQ breaking operators. The size of the extra dimension changes after inflation due to an interaction between inflaton and a bulk scalar field, which implies that the PQ symmetry can be drastically broken during inflation to suppress undesirable axion isocurvature fluctuations
Motivated by multi-throat considerations, we study the phenomenological implications of a bulk axion...
The QCD axion solving the strong CP problem may originate from antisymmetric tensor gauge fields in ...
The mass of the axion and its decay rate are known to depend only on the scale of Peccei-Quinn symme...
We propose a QCD axion model where the origin of PQ symmetry and suppression of axion isocurvature p...
AbstractWe propose a QCD axion model where the origin of PQ symmetry and suppression of axion isocur...
Although QCD axion models are widely studied as solutions to the strong CP problem, they generically...
Although QCD axion models are widely studied as solutions to the strong CP problem, they generically...
Although QCD axion models are widely studied as solutions to the strong CP problem, they generically...
Although QCD axion models are widely studied as solutions to the strong CP problem, they generically...
We study some of the novel effects that arise when the QCD axion is placed in the ``bulk'' of large ...
We propose a new mechanism to suppress the axion isocurvature perturbation, while producing the righ...
AbstractWe propose a new mechanism to suppress the axion isocurvature perturbation, while producing ...
The mass of the axion and its decay rate are known to depend only on the scale of Peccei-Quinn symme...
AbstractThe BICEP2 experiment determined the Hubble parameter during inflation to be about 1014 GeV....
The mass of the axion and its decay rate are known to depend only on the scale of Peccei-Quinn symme...
Motivated by multi-throat considerations, we study the phenomenological implications of a bulk axion...
The QCD axion solving the strong CP problem may originate from antisymmetric tensor gauge fields in ...
The mass of the axion and its decay rate are known to depend only on the scale of Peccei-Quinn symme...
We propose a QCD axion model where the origin of PQ symmetry and suppression of axion isocurvature p...
AbstractWe propose a QCD axion model where the origin of PQ symmetry and suppression of axion isocur...
Although QCD axion models are widely studied as solutions to the strong CP problem, they generically...
Although QCD axion models are widely studied as solutions to the strong CP problem, they generically...
Although QCD axion models are widely studied as solutions to the strong CP problem, they generically...
Although QCD axion models are widely studied as solutions to the strong CP problem, they generically...
We study some of the novel effects that arise when the QCD axion is placed in the ``bulk'' of large ...
We propose a new mechanism to suppress the axion isocurvature perturbation, while producing the righ...
AbstractWe propose a new mechanism to suppress the axion isocurvature perturbation, while producing ...
The mass of the axion and its decay rate are known to depend only on the scale of Peccei-Quinn symme...
AbstractThe BICEP2 experiment determined the Hubble parameter during inflation to be about 1014 GeV....
The mass of the axion and its decay rate are known to depend only on the scale of Peccei-Quinn symme...
Motivated by multi-throat considerations, we study the phenomenological implications of a bulk axion...
The QCD axion solving the strong CP problem may originate from antisymmetric tensor gauge fields in ...
The mass of the axion and its decay rate are known to depend only on the scale of Peccei-Quinn symme...