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Related papers: A simple Solution to the Strong CP Problem

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We investigate origin of three features that are often assumed in analysis of two-Higgs doublet models: (i) softly broken Z2 symmetry, (ii) CP invariant Higgs potential, and (iii) degenerated mass spectra. We extend electroweak gauge…

High Energy Physics - Phenomenology · Physics 2016-08-24 Tomohiro Abe , Yuji Omura

We propose an alternative to the axion mechanism for addressing the charge parity (CP) problem in quantum chromodynamics (QCD). Our approach involves imposing CP as an inherent symmetry of the Lagrangian, which is then spontaneously broken.…

High Energy Physics - Phenomenology · Physics 2025-10-08 Rodolfo Ferro-Hernandez , Stefano Morisi , Eduardo Peinado

We study spontaneous CP violation as a solution to the strong CP problem in left-right symmetric theories. The discrete CP symmetry is broken by a complex vacuum expectation value of a right-handed Higgs doublet. Heavy vectorlike down-type…

High Energy Physics - Phenomenology · Physics 2019-07-03 Sebastian Ohmer

The most general Higgs potential of the two-Higgs-doublet model (2HDM) contains three squared-mass parameters and seven quartic self-coupling parameters. Among these, one squared-mass parameter and three quartic coupling parameters are…

High Energy Physics - Phenomenology · Physics 2009-11-11 John F. Gunion , Howard E. Haber

When new CP-violating interactions are dominated by flavor changing neutral particle exchanges, that may occur in many extensions of the standard model. We examine a type 3 two Higgs doublet model and find that direct CP asymmetries can be…

High Energy Physics - Phenomenology · Physics 2015-06-25 Yue-Liang Wu

Models of spontaneous CP violation can solve the Strong CP problem without the need of an anomalous Peccei-Quinn symmetry. In this work we review the Nelson-Barr approach, quantifying a peculiar coincidence between unrelated mass scales…

High Energy Physics - Phenomenology · Physics 2022-05-10 Alessandro Valenti

We discuss CP-violation in a model with a real and a complex isospin triplet Higgs fields without introducing any symmetries except for the electroweak gauge symmetry. This corresponds to the minimal extension of the Higgs sector with the…

High Energy Physics - Phenomenology · Physics 2023-06-16 Ting-Kuo Chen , Cheng-Wei Chiang , Kei Yagyu

The strong CP problem can be solved if the laws of nature are invariant under a space-time parity exchanging the Standard Model with its mirror copy. We review and extend different realizations of this idea with the aim of discussing Dark…

High Energy Physics - Phenomenology · Physics 2023-10-23 Michele Redi , Andrea Tesi

We show that in a Complementary two-Higgs doublet model(C2HDM) the CP violating phase in the CKM matrix can be generated spontaneously, dangerous FCNC can be naturally suppressed and the strong CP problem can also be avoided. The two Higgs…

High Energy Physics - Phenomenology · Physics 2017-05-31 Wei Liao

The CP violation gives rise to severe restriction of soft breaking terms in supersymmetric standard models. Among them, constraints on the holomorphic soft mass of Higgs doublets (the B parameter) are difficult to satisfy due to the other…

High Energy Physics - Phenomenology · Physics 2010-04-05 Masahiro Yamaguchi , Koichi Yoshioka

We discuss the formalism of two Higgs doublet model type III with CP violation from CP-even CP-odd mixing in the neutral Higgs bosons. The flavor changing interactions among neutral Higgs bosons and fermions are presented at tree level in…

High Energy Physics - Phenomenology · Physics 2015-06-18 R. Gaitán , R. Martinez , J. H. Montes de Oca Y. , S. Rodriguez Romo

We consider the two-Higgs-doublet model with explicit CP-violation, where the effective Higgs potential is not CP-invariant at the tree-level. Three neutral Higgs bosons of the model are the mixtures of CP-even and CP-odd bosons which exist…

High Energy Physics - Phenomenology · Physics 2009-11-07 M. N. Dubinin , A. V. Semenov

We show that a recently proposed solution to the Hierarchy Problem simultaneously solves the Strong CP Problem, without requiring an axion or any further new physics. Consistency of black hole physics implies a non-trivial relation between…

High Energy Physics - Theory · Physics 2008-11-26 Gia Dvali , Glennys R. Farrar

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

A model of quark mass matrices from six dimensions, which is nearly democatic in nature and which is previously constructed by two of us (PQH and MS), is studied in detail in this manuscript. We found that not only it fits all the six quark…

High Energy Physics - Phenomenology · Physics 2014-11-17 P. Q. Hung , M. Seco , A. Soddu

We show that a class of parity based solutions to the strong CP problem predicts new colored particles with mass at the TeV scale, due to constraints from Planck suppressed operators. The new particles are copies of the Standard Model…

High Energy Physics - Phenomenology · Physics 2016-10-07 Raffaele Tito D'Agnolo , Anson Hook

The charged fermion mass matrices are invariant under $U(1)^3$ symmetry linked to the fermion number transformation. Under the condition that the definition of this symmetry in arbitrary weak basis does not depend upon Higgs parameters such…

High Energy Physics - Phenomenology · Physics 2015-05-20 Anjan S. Joshipura , Bhavik P. Kodrani

We present a solution to the strong CP problem based on the identification of the theta angle with twice the CP violating phase present in the CKM quark matrix. This solution washes out all the unwanted issues stemming form the strong CP…

High Energy Physics - Phenomenology · Physics 2018-02-23 Renata Jora

We present a natural solution to the strong CP problem in the context of split fermions. By assuming CP is spontaneously broken in the bulk, a weak CKM phase is created in the standard model due to a twisting in flavor space of the bulk…

High Energy Physics - Phenomenology · Physics 2010-02-03 Roni Harnik , Gilad Perez , Matthew D. Schwartz , Yuri Shirman

The standard model does not provide an explanation of the observed alignment of quark flavors i.e. why are the up and down quarks approximately aligned in their weak interactions according to their masses? We suggest a resolution of this…

High Energy Physics - Phenomenology · Physics 2018-10-17 Abhish Dev , Rabindra N. Mohapatra