Abstract

In this manuscript, we present an explicit way to describe the violation of CP symmetry in the standard model (SM) of electroweak interactions. In such a way, complex Cabbibo-Kobayashi-Maskawa (CKM) matrices are achieved which stand for the violation of CP symmetry. At the beginning, two necessary but not sufficient conditions for yielding a complex CKM matrix are stated as criteria. Then we found an interesting condition between the real and imaginary parts of a Hermitian $3\times 3$ matrix may provide extra relations among its parameters and reduce the number of them from eighteen down to five. In previous investigations, this can be done only down to nine. With another assumption among some of those parameters, the mass-matrix pattern is further simplified so as to be diagonalized analytically and in consequence four matrices which reveal $S_N$ symmetries among or between quark generations are obtained. In some of such $S_N$-symmetric cases, the derived CKM matrices are complex which indicate that CP symmetry is violated accordingly. Taking the Jarlskog invariant as an estimate of the CPV strength, the value predicted by this model is orders stronger than the empirical value detected experimentally. However, that happens to fill partly the gap between the cosmologically observed amount of Baryon Asymmetry of the Universe (BAU) and that current Standard Model of particle physics predicts. It also proves the long suspected existence of BAU-productive eras in early universe if some fermions were indistinguishable, i.e., $S_N$-symmetric, under circumstances of extremely high temperatures.

Highlights

  • We present an explicit way to describe the violation of CP symmetry in the standard model (SM) of electrweak interactions

  • Two necessary but not sufficient conditions for yielding a complex CKM matrix are stated as criteria

  • For over fifty years, an explicit way to describe the violation of CP symmetry is still obscure

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Summary

Introduction

If we analyze the theoretical origin of CPV from its fundamental, considering only the quark sector here, the patterns of quark-mass matrices M are obviously the keys to ignite such a violation. After decades such a satisfactory Yukawa-coupling matrix is still obscure There is another way in SM to extract a complex phase from the vacuum expectation value (VEV) of its only Higgs doublet. An assumption =A A=1 A=2 A3 , where A1 , A2 and A3 are diagonal elements of the most general M matrix to be given, is employed to further simplify its pattern Such an assumption gives us four analytically diagonalizable M k matrices and correspondingly four complex Uk matrices, where k = 1 to 4 indicate to which case they correspond.

Analytically Diagonalizable M Matrices and Their U Matrices
B1 B2 0 C1 C2
CKM Matrix and the BAU Problem
Conclusions and Discussions
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