$A_4$ modular invariance and the strong CP problem
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arXiv
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| Format: | Preprint |
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2024
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| author | Petcov, S. T. Tanimoto, M. |
| author_facet | Petcov, S. T. Tanimoto, M. |
| contents | We present simple effective theory of quark masses, mixing and CP violation with level $N=3$ ($A_4$) modular symmetry, which provides solution to the strong CP problem without the need for an axion. The vanishing of the strong CP-violating phase $\bar θ$ is ensured by assuming CP to be a fundamental symmetry of the Lagrangian of the theory. The CP symmetry is broken spontaneously by the vacuum expectation value (VEV) of the modulus $τ$. This provides the requisite large value of the CKM CP-violating phase while the strong CP phase $\bar θ$ remains zero or is tiny. Within the considered framework we discuss phenomenologically viable quark mass matrices with three types of texture zeros, which are realized by assigning both the left-handed and right-handed quark fields to $A_4$ singlets ${\bf 1}$, ${\bf 1'}$ and ${\bf 1''}$ with appropriate weights. The VEV of $τ$ is restricted to reproduce the observed CKM parameters. We discuss cases in which the modulus VEV is close to the fixed points $i$, $ω$ and $i\infty$. In particular, we focus on the VEV of $τ$, which gives the absolute minima of the supergravity-motivated modular- and CP-invariant potentials for the modulus $τ$, so called, modulus stabilisation. We present a successful model, which is consistent with the modulus stabilisation close to $τ=ω$. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2404_00858 |
| institution | arXiv |
| publishDate | 2024 |
| record_format | arxiv |
| spellingShingle | $A_4$ modular invariance and the strong CP problem Petcov, S. T. Tanimoto, M. High Energy Physics - Phenomenology We present simple effective theory of quark masses, mixing and CP violation with level $N=3$ ($A_4$) modular symmetry, which provides solution to the strong CP problem without the need for an axion. The vanishing of the strong CP-violating phase $\bar θ$ is ensured by assuming CP to be a fundamental symmetry of the Lagrangian of the theory. The CP symmetry is broken spontaneously by the vacuum expectation value (VEV) of the modulus $τ$. This provides the requisite large value of the CKM CP-violating phase while the strong CP phase $\bar θ$ remains zero or is tiny. Within the considered framework we discuss phenomenologically viable quark mass matrices with three types of texture zeros, which are realized by assigning both the left-handed and right-handed quark fields to $A_4$ singlets ${\bf 1}$, ${\bf 1'}$ and ${\bf 1''}$ with appropriate weights. The VEV of $τ$ is restricted to reproduce the observed CKM parameters. We discuss cases in which the modulus VEV is close to the fixed points $i$, $ω$ and $i\infty$. In particular, we focus on the VEV of $τ$, which gives the absolute minima of the supergravity-motivated modular- and CP-invariant potentials for the modulus $τ$, so called, modulus stabilisation. We present a successful model, which is consistent with the modulus stabilisation close to $τ=ω$. |
| title | $A_4$ modular invariance and the strong CP problem |
| topic | High Energy Physics - Phenomenology |
| url | https://arxiv.org/abs/2404.00858 |