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Dong-Ping Fu

Publications and source records attributed to Dong-Ping Fu.

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Quark masses and mixing in the D_5 model under spontaneous CP violation

It is known that CP violation occurs in flavor physics, and the CKM matrix is complex. We investigate the Yukawa sector of a four-Higgs model based on D_5 symmetry. To understand all possible sources of CP violation in the Yukawa sector, we systematically analyze the impact of all possible representation assignments of the left-handed and right-handed quark fields under the D_5 group. After imposing the conditions of non-block-diagonal CKM matrix and the absence of massless quarks, we find that the only viable representation consists of one D_5 doublet and one singlet. In this case, two distinct types of quark mass models emerge in the quark sector. For each model, we introduce the most general vacuum that allows spontaneous CP violation (SCPV) into the mass matrices. Due to the specific structure of the D_5 symmetry, the vacuum expectation values (vevs) satisfy particular relations such that, for both quark models, the up- and down-quark mass squared matrices (i.e., M_d M_d^\dagger and M_u M_u^\dagger) can be simultaneously block-diagonalized by the same unitary transformation, forcing the CKM matrix to be block-diagonal and thus yielding vanishing mixing angles and CP violation. This result rules out the possibility of explaining experimental observations within the D_5 4HDM under the SCPV framework.

hep-ph

A D_5 Model of Quarks with Explicit CP Violation

We investigate the quark sector of a four-Higgs-doublet model with an exact D_5 symmetry. In the framework of explicit CP violation, we considered the most general real vacuum, derived the quark mass matrices, and performed a numerical fit to the quark masses and the CKM mixing matrix at the scale mu = 1 TeV using a differential evolution algorithm, based on the 2024 PDG experimental data.The results show that the model simultaneously fits the quark mass spectrum and the CKM mixing angles with an excellent overall chi^2 = 6.97, accurately reproducing the six-quark mass hierarchy and perfectly matching the nine squared moduli of the CKM matrix. The resulting Jarlskog invariant J_CP = 3.144 \times 10^{-5} agrees with the experimental value 3.12 \times 10^{-5} within 0.19\sigma, indicating that the new source of CP violation from the complex phases in the quark Yukawa couplings alone is sufficient to generate the observed CP violation. Moreover, the hierarchical structures of the vacuum expectation values and the quark Yukawa couplings naturally explain the observed quark mass hierarchy through their interplay.

hep-ph

Spontaneous CP violation in the D_5-symmetric four-Higgs-doublet models

We constructed a four-Higgs-doublet model (4HDM) invariant under D_5 symmetry and investigated its complete neutral vacuum structure in detail. Assuming explicit CP conservation in the scalar potential, we examined whether CP symmetry can be spontaneously broken. We provided a complete list of all possible real and complex vacua, along with the constraints on the potential parameters required for each vacuum solution to exist. We also discussed the positive-definiteness conditions that the Hessian must satisfy for each vacuum to be a local minimum of the potential. The results show that, after spontaneous symmetry breaking, some complex vacua lead to spontaneous CP violation in the potential, whereas the remaining complex vacua still preserve CP conservation. Among these CP-violating complex vacua, one can be regarded as the most general form. Furthermore, we discussed the relationship between real and complex vacua.

hep-ph