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Related papers: Strong CP-Problem in Superstring Theory

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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

We examine the possibility that the strong CP problem is solved by string-theoretic axions in strong-coupling limit of the E_8 x E_8 heterotic string theory (M-theory). We first discuss some generic features of gauge kinetic functions in…

High Energy Physics - Theory · Physics 2014-11-18 Kiwoon Choi

We present a study of dark matter and the strong CP problem within a globally consistent framework of Type IIA string theory, compactified on a $T^6/(\mathbb{Z}_2 \times \mathbb{Z}_2)$ orientifold with intersecting D6-branes (Model A), for…

High Energy Physics - Theory · Physics 2026-04-22 Yang Liu

In the context of a Coleman-Weinberg mechanism for the Higgs boson mass, we address the strong CP problem. We show that a DFSZ-like invisible axion model with a gauge-singlet complex scalar field S, whose couplings to the Standard Model are…

High Energy Physics - Phenomenology · Physics 2015-01-09 Kyle Allison , Christopher T. Hill , Graham G. Ross

I propose a new axionic solution to the strong CP problem which involves a hypothetical vector-like quark(s) in a high-colour representation of the conventional QCD. There are two distinct scenarios. If the current mass of the exotic quark…

High Energy Physics - Phenomenology · Physics 2016-02-23 Archil Kobakhidze

We suggest a new solution to the strong CP problem. The solution is based on the proper use of the boundary conditions for the QCD generating functional integral. We expand the perturbative boundary conditions to both perturbative and…

High Energy Physics - Phenomenology · Physics 2023-12-19 S. A. Larin

Solutions to the strong CP problem typically introduce new scales associated with the spontaneous breaking of symmetries. Absent any anthropic argument for small $\bar\theta$, these scales require stabilization against ultraviolet…

High Energy Physics - Phenomenology · Physics 2016-01-27 Abdelhamid Albaid , Michael Dine , Patrick Draper

The Supersymmetric Standard Model is a benchmark theoretical framework for particle physics, yet it suffers from a number of deficiencies, chief among which is the strong CP problem. Solving this with an axion in the context of selected new…

High Energy Physics - Phenomenology · Physics 2015-05-13 Ernest Ma

We consider 5 dimensional gauge theories where the 5th direction is compactified on an interval. The Chern-Simons (CS) terms (favored by naive dimensional analysis) are discussed. A simple scenario with an extra U(1)_X gauge field that…

High Energy Physics - Phenomenology · Physics 2009-04-21 Bohdan Grzadkowski , Jose Wudka

String theoretic axion is a prime candidate for the QCD axion solving the strong CP problem. For a successful realization of the QCD axion in string theory, one needs to stabilize moduli including the scalar partner (saxion) of the QCD…

High Energy Physics - Theory · Physics 2010-10-27 Kiwoon Choi , Kwang Sik Jeong

I describe how the QCD vacuum structure, necessary to resolve the $U(1)_A$ problem, predicts the presence of a P, T and CP violating term proportional to the vacuum angle $\bar{\theta}$. To agree with experimental bounds, however, this…

High Energy Physics - Phenomenology · Physics 2011-04-11 R. D. Peccei

We analyze the strong CP problem and the implications for axion physics in the context of $U_1$ vector leptoquark models, recently put forward as an elegant solution to the hints of lepton flavor universality violation in B-meson decays. It…

High Energy Physics - Phenomenology · Physics 2019-12-25 Javier Fuentes-Martin , Mario Reig , Avelino Vicente

A non-axion solution to the Strong CP Problem is proposed that works even in the context of gravity-mediated supersymmetry breaking. Both $\epsilon'/\epsilon$ and indirect CP violation in the $B-\bar{B}$ are predicted to be unobservably…

High Energy Physics - Phenomenology · Physics 2014-11-17 S. B. Barr

We discuss conditions that should be satisfied by axion models for solving the strong CP problem. It has been observed that Planck scale effects may render the axion models ineffective if there are gauge invariant operators of dimension…

High Energy Physics - Phenomenology · Physics 2016-08-24 Bogdan A. Dobrescu

We present a new mechanism to solve the strong CP problem using $N\geq2$ axions, each dynamically relaxing part of the $\bar\theta$ parameter. At high energies $M\gg\Lambda_{QCD}$ the $SU(3)_{c}$ group becomes the diagonal subgroup of an…

High Energy Physics - Phenomenology · Physics 2018-12-26 Prateek Agrawal , Kiel Howe

It is emphasized that the existence of a very light axion is consistent with the strong CP invariance and cosmological and astrophysical constraints. The attempt to embed the very light axion in superstring models is discussed.

Astrophysics · Physics 2016-11-03 Jihn E. Kim

The physical origin of the strong CP problem in QCD, rooted in the structures of the vacuum of the standard model, is reviewed. The chiral solution to this problem, with its accompanying axion, is explained and various characteristics of…

High Energy Physics - Phenomenology · Physics 2011-04-11 R. D. Peccei

Theory of superstrings on Calabi-Yau manifolds is applied to investigate catalysis of proton decay.

High Energy Physics - Phenomenology · Physics 2023-05-24 Yuri M. Malyuta

We propose a new solution to the strong CP problem based on supersymmetric non-renormalization theorems. CP is broken spontaneously and it's breaking is communicated to the MSSM by radiative corrections. The strong CP phase is protected by…

High Energy Physics - Phenomenology · Physics 2014-11-17 G. Hiller , M. Schmaltz

We propose a new solution to the strong-CP problem. It involves the existence of an unbroken gauged $U(1)_X$ symmetry whose gauge boson gets a Stuckelberg mass term by combining with a pseudoscalar field $\eta (x)$. The latter has…

High Energy Physics - Phenomenology · Physics 2009-11-07 G. Aldazabal , L. E. Ibanez , A. M. Uranga
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