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We introduce a natural origin of the Peccei-Quinn (PQ) symmetry with a sufficiently good precision. In the standard model, the baryon number symmetry U(1)_B arises accidentally due to the SU(3)_C color gauge symmetry, and it protects the…

High Energy Physics - Phenomenology · Physics 2019-02-06 Hye-Sung Lee , Wen Yin

Because the Peccei-Quinn (PQ) symmetry has to be anomalous to solve the strong CP puzzle, some colored and chiral fermions have to transform non-trivially under this symmetry. But when the SM fermions are charged, as in the PQ or DFSZ…

High Energy Physics - Phenomenology · Physics 2020-11-04 Jérémie Quevillon , Christopher Smith

The Peccei-Quinn (PQ) solution to the Strong CP Problem is expected to fail unless the global symmetry U(1)${}_{\rm PQ}$ is protected from Planck-scale operators up to high mass dimension. Suitable protection can be achieved if the PQ…

High Energy Physics - Phenomenology · Physics 2018-04-05 Michael Duerr , Kai Schmidt-Hoberg , James Unwin

We introduce a class of composite axion models that provide a natural solution to the strong CP problem, and possibly account for the observed dark matter abundance. The QCD axion arises as a composite Nambu-Goldstone boson (NGB) from the…

High Energy Physics - Phenomenology · Physics 2022-05-13 Roberto Contino , Alessandro Podo , Filippo Revello

Axion models generically suffer from a severe quality problem when coupled to gravity. In this article we provide a very simple model with a high quality axion. The axion is a pseudo-Nambu-Goldstone boson of the baryon number symmetry,…

High Energy Physics - Phenomenology · Physics 2025-10-10 Prateek Agrawal , Anson Hook , Vazha Loladze , Mario Reig

A $SU(N)_L\times SU(N)_R$ gauge theory for a scalar multiplet $Y$ transforming in the bi-fundamental representation $(N,\bar N)$ preserves, for $N>4$, an accidental $U(1)$ symmetry firstly broken at operator dimension $N$. Two…

High Energy Physics - Phenomenology · Physics 2017-07-12 Luca Di Luzio , Enrico Nardi , Lorenzo Ubaldi

We argue that the axion arising in the solution of the strong CP problem can be identified with the Majoron, the (pseudo-)Goldstone boson of spontaneously broken lepton number symmetry. At low energies, the associated $U(1)_L$ becomes, via…

High Energy Physics - Phenomenology · Physics 2011-02-08 Adam Latosinski , Krzysztof A. Meissner , Hermann Nicolai

In the first part of this talk, after a brief presentation of the strong CP puzzle, the construction of axion models and their main phenomenological features are described. In the second part, the possibility to mix the Peccei-Quinn…

High Energy Physics - Phenomenology · Physics 2024-11-15 Christopher Smith

The axion solution to the strong CP problem requires an anomalous global U(1) symmetry. We show that the existence of such a symmetry is a natural consequence of an extra dimension in which a gauged U(1) is spontaneously broken on one of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Hsin-Chia Cheng , David Elazzar Kaplan

The possible discovery of proton decay, neutron-antineutron oscillation, neutrinoless beta decay in low energy experiments, and exotic signals related to the violation of the baryon and lepton numbers at collider experiments will change our…

High Energy Physics - Phenomenology · Physics 2015-09-28 Pavel Fileviez Perez

Although the axion is the most compelling solution to the strong CP problem, the ad hoc introduced global Peccei-Quinn symmetry suffers from a severe fine-tuning problem known as the quality problem. In this Letter, we show that the…

High Energy Physics - Phenomenology · Physics 2026-03-05 Jie Sheng , Tsutomu T. Yanagida

In this report we discuss the main theories to understand the origin of baryon and lepton number violation in physics beyond the Standard Model. We present the theoretical predictions for rare processes such as neutrinoless double beta…

We consider extensions of the Standard Model in which a spontaneously broken global chiral Peccei-Quinn (PQ) symmetry arises as an accidental symmetry of an exact $Z_N$ symmetry. For $N = 9$ or $10$, this symmetry can protect the accion -…

High Energy Physics - Phenomenology · Physics 2016-04-27 Andreas Ringwald , Ken'ichi Saikawa

We construct explicit models that solve the axion quality problem originating from quantum gravitational effects. The general strategy we employ is to supplement the Standard Model and its grand unified extensions by an anomaly-free axial…

High Energy Physics - Phenomenology · Physics 2025-02-20 K. S. Babu , Bhaskar Dutta , Rabindra N. Mohapatra

We present detailed arguments and calculations in support of our recent proposal to identify the axion arising in the solution of the strong CP problem with the Majoron, the (pseudo-)Goldstone boson of spontaneously broken lepton number…

High Energy Physics - Phenomenology · Physics 2015-06-04 Adam Latosinski , Krzysztof A. Meissner , Hermann Nicolai

It is firmly believed that the axion for solving the strong CP problem must come from the spontaneous breaking of an anomalous Peccei-Quinn global symmetry. Here we show a new possibility that the axion can be induced by a pseudo Goldstone…

High Energy Physics - Phenomenology · Physics 2023-07-11 Pei-Hong Gu

The effects of possible explicit violation of the Peccei-Quinn symmetry responsible for the solution of the strong CP problem are studied in supersymmetric models. It is shown that automatic models with an abelian $U(1)$ gauge symmetry are…

High Energy Physics - Phenomenology · Physics 2010-11-01 E. A. Dudas

We present a dynamical (composite) axion model where the Peccei-Quinn (PQ) symmetry arises automatically as a consequence of chirality and gauge symmetry. The Standard Model is simply extended by a confining and chiral $SU(5)$ gauge…

High Energy Physics - Phenomenology · Physics 2022-10-19 M. B. Gavela , M. Ibe , P. Quilez , T. T. Yanagida

We present several models where the QCD axion arises accidentally. Confining gauge theories can generate axion candidates whose properties are uniquely determined by the quantum numbers of the new fermions under the Standard Model. The…

High Energy Physics - Phenomenology · Physics 2017-03-15 Michele Redi , Ryosuke Sato

The smallness of the quark and lepton parameters and the hierarchy between them could be the result of selection rules due to a horizontal symmetry broken by a small parameter. The same selection rules apply to baryon number violating…

High Energy Physics - Phenomenology · Physics 2011-04-08 Valerie Ben-Hamo , Yosef Nir
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