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The QCD axion stands as one of the most promising candidates for resolving the strong CP problem. However, the value of the axion's decay constant $f_a$ and, by extension, its mass $m_a$, remain uncertain within the framework of effective…

High Energy Physics - Phenomenology · Physics 2024-11-01 Qiaoli Yang , Runchao Huang

The QCD Lagrangian contains a CP violating gluon density term with a physical coefficient $\bar{\theta}$. The upper bound on the electric dipole moment of neutron implies that the value of $\bar{\theta}$ should be extremely small rather…

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

We attempt to identify a phenomenologically viable solution to the strong $CP$ problem in which the axion is composed entirely out of Standard Model fermion species. The axion consists predominantly of the $\eta'$ meson with a minuscule…

High Energy Physics - Phenomenology · Physics 2021-08-09 Gia Dvali , Lena Funcke

We study finite density QCD in an approximation in which the interaction between quarks is modelled on that induced by instantons. We sketch the mechanism by which chiral symmetry restoration at finite density occurs in this model. At all…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. Alford , K. Rajagopal , F. Wilczek

The strong charge-parity (CP) problem has been a long-standing problem in particle physics since 1976, illustrating the small CP-violation phase in quantum chromodynamics (QCD). The axion, based on the Peccei-Quinn mechanism, is the most…

High Energy Physics - Phenomenology · Physics 2024-08-23 Qiuyue Liang , Risshin Okabe , Tsutomu T. Yanagida

We study the effect of a non-zero strange quark mass on the color-flavor-locked (CFL) phase of high density quark matter. We have previously shown that for a strange quark mass $m_s\sim m_u^{1/3}\Delta^{2/3}$ the CFL state becomes unstable…

High Energy Physics - Phenomenology · Physics 2008-11-26 Thomas Schaefer

We determine the model-independent component of the couplings of axions to electroweak gauge bosons, induced by the minimal coupling to QCD inherent to solving the strong CP problem. The case of the invisible QCD axion is developed first,…

High Energy Physics - Phenomenology · Physics 2019-03-27 G. Alonso-Álvarez , M. B. Gavela , P. Quilez

Several extensions of the standard model feature new colored states that besides modifying the running of the QCD coupling could even lead to the loss of asymptotic freedom. Such a loss would potentially diminish the Wilsonian fundamental…

High Energy Physics - Phenomenology · Physics 2015-12-15 Francesco Sannino

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

We find that there are three axions in standard--like superstring models in the four dimensional free fermionic formulation. These axions are either harmful or very heavy. Therefore, they cannot solve the strong CP problem. We show that…

High Energy Physics - Phenomenology · Physics 2009-10-22 Edi Halyo

The strong CP problem and its resolution through the existence of an axion are briefly reviewed. The constraints on the axion from accelerator searches, from the evolution of red giants and from supernova SN1987a combine to require $m_a < 3…

High Energy Physics - Phenomenology · Physics 2014-11-17 P. Sikivie

The axion particle is the outcome of the proposed Peccei-Quinn mechanism for solving the strong CP problem. Axion is also a popular dark matter candidate. Thus there is an increased interest in establishing its existence. Axions couple to…

High Energy Physics - Phenomenology · Physics 2022-04-06 A. Nicolaidis

The even light QCD axion called the $Z_{\mathcal N}$ axion can both solve the strong CP problem and account for the dark matter (DM). We point out that the single and double level crossings can naturally take place in the mass mixing…

High Energy Physics - Phenomenology · Physics 2024-01-05 Hai-Jun Li , Ying-Quan Peng , Wei Chao , Yu-Feng Zhou

We propose a minimal set of weak-basis invariants in an extension of the SM where one up-type isosinglet vector-like quark is introduced, which allows us to obtain all the physical content of the CKM matrix. We present CP-odd invariants of…

High Energy Physics - Phenomenology · Physics 2023-05-22 Francisco Albergaria , G. C. Branco , José Filipe Bastos , J. I. Silva-Marcos

We show that there are many candidates for the quintessence and/or the QCD axions in a class of chiral $U(1)$ gauge theories. Their qualities are high enough to serve as the dark energy and/or to solve the strong CP problem. Interestingly,…

High Energy Physics - Phenomenology · Physics 2023-08-17 Yu-Cheng Qiu , Jin-Wei Wang , Tsutomu T. Yanagida

It is difficult to construct a post-inflation QCD axion model that solves the axion quality problem (and hence the Strong CP problem) without introducing a cosmological disaster. In a post-inflation axion model, the axion field value is…

High Energy Physics - Phenomenology · Physics 2024-08-27 Qianshu Lu , Matthew Reece , Zhiquan Sun

In this lecture we review several cosmological issues associated with the axion. Axion solves the strong CP problem and is a good candidate for the dark matter. Limits, which are imposed by the value of isocurvature fluctuations fraction in…

High Energy Physics - Phenomenology · Physics 2007-05-23 Alexey Anisimov

Murayama proposed a GeV-scale axion theory where the up-quark mass term is generated dynamically by the QCD chiral condensate, spontaneously breaking a Peccei-Quinn symmetry. It predicts a too large mass splitting between neutral and…

High Energy Physics - Phenomenology · Physics 2026-02-25 Luca Di Luzio , Michele Redi , Alessandro Strumia , Andrea Tesi , Arsenii V. Titov

We study the mirror world with dark matter arising from the thermal freeze-out of the lightest, stable mirror particle -- the mirror electron. The dark matter abundance is achieved for mirror electrons of mass 225 GeV, fixing the mirror…

High Energy Physics - Phenomenology · Physics 2023-02-10 David I. Dunsky , Lawrence J. Hall , Keisuke Harigaya

It is shown that in the scheme with a rotating fermion mass matrix (i.e. one with a scale-dependent orientation in generation space) suggested earlier for explaining fermion mixing and mass hierarchy, the theta-angle term in the QCD action…

High Energy Physics - Phenomenology · Physics 2011-01-27 J. Bordes , H. M. Chan , S. T. Tsou