The QCD axion couplings of various invisible axion models are presented. In particular, the exact global symmetry U(1)PQU(1)PQ in the superpotential is possible for the anomalous U(1) from string compactification, broken only by the gauge anomalies at one loop level, and is shown to have the resultant invisible axion coupling to photon, View the MathML sourcecaγγ≥83−caγγchbr where View the MathML sourcecaγγchbr≃2. However, this bound is not applicable in approximate U(1)PQU(1)PQ models with sufficiently suppressed U(1)PQU(1)PQ-breaking superpotential terms. We also present a simple method to obtain View the MathML sourcecaγγ0 which is the value obtained above the electroweak scale. ©2016 The Authors.1441sciescopu
The QCD axion solving the strong CP problem may originate from antisymmetric tensor gauge fields in ...
AbstractWe derive the necessary conditions to build a class of invisible axion models with Flavor Ch...
I describe how under favourable circumstances the invisible axion may manifest its existence at the ...
It is pointed out that there exist a few problems to be overcome toward an observable sub-meV QCD ax...
We study some of the novel effects that arise when the QCD axion is placed in the ``bulk'' of large ...
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The recent detection of the cosmic microwave background polarimeter experiment BICEP2 of tensor fluc...
The QCD axion solving the strong CP problem may originate from antisymmetric tensor gauge fields in ...
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AbstractThe QCD axion with fa at an intermediate scale, 109 GeV∼1012 GeV, seems in conflict with the...
The QCD axion solving the strong CP problem may originate from antisymmetric tensor gauge fields in ...
AbstractWe derive the necessary conditions to build a class of invisible axion models with Flavor Ch...
I describe how under favourable circumstances the invisible axion may manifest its existence at the ...
It is pointed out that there exist a few problems to be overcome toward an observable sub-meV QCD ax...
We study some of the novel effects that arise when the QCD axion is placed in the ``bulk'' of large ...
We reexamine the axion-photon couplings in various invisible axion models motivated by the recent pr...
We investigate the most interesting decay processes involving axions, photons and the lightest pseud...
The QCD axion with fafa at an intermediate scale, 109 GeV∼1012 GeV109 GeV∼1012 GeV, seems in conflic...
We study the cosmological evolution of the QCD axion coupled to hidden photons. For a moderately str...
We consider the renormalizable SO(5)/SO(4) sigma-model, in which the Higgs particle has a pseudo-Nam...
We consider the renormalizable SO(5)/SO(4) sigma-model, in which the Higgs particle has a pseudo-Nam...
The recent detection of the cosmic microwave background polarimeter experiment BICEP2 of tensor fluc...
The QCD axion solving the strong CP problem may originate from antisymmetric tensor gauge fields in ...
AbstractThe axion search experiments invite a plausible estimation of the axion–photon–photon coupli...
AbstractThe QCD axion with fa at an intermediate scale, 109 GeV∼1012 GeV, seems in conflict with the...
The QCD axion solving the strong CP problem may originate from antisymmetric tensor gauge fields in ...
AbstractWe derive the necessary conditions to build a class of invisible axion models with Flavor Ch...
I describe how under favourable circumstances the invisible axion may manifest its existence at the ...