2017
DOI: 10.1103/physrevd.95.095009
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Minimal axion model from flavor

Abstract: We show that solving the flavor problem of the Standard Model with a simple Uð1Þ H flavor symmetry naturally leads to an axion that solves the strong CP problem and constitutes a viable Dark Matter candidate. In this framework, the ratio of the axion mass and its coupling to photons is related to the SM fermion masses and predicted within a small range, as a direct result of the observed hierarchies in quark and charged lepton masses. The same hierarchies determine the axion couplings to fermions, making the f… Show more

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Cited by 189 publications
(210 citation statements)
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References 58 publications
(51 reference statements)
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“…In consequence, the Axiflavon is more sensitive to the scale of new physics than the MFV axion. To satisfy the present bounds on K and B decays, the axion scale f a needs to be of the order of 10 10 GeV [82], that approximatively coincides with the values necessary to pass the very stringent bounds on the aγγ and aee couplings. The Axiflavon is therefore an example of visible QCD axion, as it predicts lowenergy flavour effects, despite of the very large value of the axion scale f a .…”
Section: Jhep10(2017)168mentioning
confidence: 99%
See 1 more Smart Citation
“…In consequence, the Axiflavon is more sensitive to the scale of new physics than the MFV axion. To satisfy the present bounds on K and B decays, the axion scale f a needs to be of the order of 10 10 GeV [82], that approximatively coincides with the values necessary to pass the very stringent bounds on the aγγ and aee couplings. The Axiflavon is therefore an example of visible QCD axion, as it predicts lowenergy flavour effects, despite of the very large value of the axion scale f a .…”
Section: Jhep10(2017)168mentioning
confidence: 99%
“…The Axiflavon [81,82] is the axion arising in the context of the FN mechanism and has flavour violating couplings, in the mass basis for fermions, predicted in terms of the FN charges, up to O(1) uncertainties. This represents a major difference with respect to the MFV axion: the presence of flavour violating couplings induces tree-level flavour changing neutral current processes, such as the meson decays described in the previous section.…”
Section: Jhep10(2017)168mentioning
confidence: 99%
“…and Z F 4 invariant conditions in the Yukawa couplings are shown as 4 . The small hierarchies between neutrino masses are explained with a choice of O(1) Yukawa couplings since a neutrino mass squared is proportional to fourth power of the Yukawa couplings.…”
Section: An Example: N = 4 Casementioning
confidence: 99%
“…A discrete symmetry Z F N allows a self-coupling of the flavon in the superpotential, W S N /Λ N −3 , and the coupling stabilizes flavon. 4 This model also provides a solution for the µ-problem in the MSSM. The Higgsino mass term in the superpotential, the so-called µ-parameter, is written by W (S m /Λ m−1 )H u H d .…”
Section: Introductionmentioning
confidence: 99%
“…They rely on an extended scalar and fermionic heavy sector and on an additional spontaneously broken symmetry. Their study has recently been revived by the focus on flavourful axions which arise in FN-like setups [5][6][7][8] and whose EFT is very much constrained by flavour physics [9][10][11]. Such flavourful axions can also be linked with dark matter studies [12].…”
Section: Introductionmentioning
confidence: 99%