Abstract

We study the CP domain walls and the consequent gravitational waves induced by the spontaneous breaking of the CP symmetry in the complex singlet extension to the Standard Model. We impose the constraints from the unitarity, stability and the global minimal of the vacuum solutions on the model parameter space. The CP domain wall profiles and tensions are obtained by numerically solving the relevant field equations. The explicit CP violation terms are then introduced to the potential as biased terms to make the domain walls unstable and collapse, The BBN bound on the magnitude of the energy bias is taken into account. To achieve sufficiently strong gravitational wave signals, the domain wall tension σ is required to be at least σ/TeV3∼ mathcal{O} (103). We find that the gravitational wave spectrum can be probed in the future SKA and/or DECIGO programs, when the typical mass scale is at least ∼ mathcal{O} (10) TeV and the explicit CP violation terms are as small as mathcal{O} (10−24)− mathcal{O} (10−23). The gravitational waves from collapsing domain walls thus provide a complementarity to the probe of extremely small CP violation at high-energy scale.

Highlights

  • The new fields may mix very weakly to the SM fields, e.g. the SM Higgs doublet

  • We find that the gravitational wave spectrum can be probed in the future square kilometer arrays (SKA) and/or DECIGO programs, when the typical mass scale is at least ∼ O(10) TeV and the explicit CP violation terms are as small as O(10−24)−O(10−23)

  • We find that the GW spectrum can be probed in the future SKA and/or DECIGO programs, when the typical mass scales of the complex singlet extension to the Standard Model (cxSM) are ∼ O(10) − O(100) TeV

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Summary

The complex singlet extension to the SM

[65], to achieve the SCPV in the theory of one complex scalar field, the global U(1) symmetry must be explicitly broken by at least two U(1) breaking couplings with different U(1) charges. This is to say one needs to select U(1) symmetry breaking terms from at. If the parameter choices among four groups still retain the global discrete symmetry, for example the combination of (b1 , d1) still having a Z2 symmetry, the corresponding spontaneous symmetry breaking can lead to the other type of domain walls. It is possible to suppress the interaction between two types of domain walls with proper parameter choices, we will avoid such complication in the following discussions by introducing a term explicitly breaking the discrete symmetry

The mass spectrum with the SCPV and the broken Z2 symmetry
The perturbative unitarity
The stability of the tree-level potential
The global minimum condition
The CP domain wall solution
The biased terms in the cxSM
The constraints and predictions to the GW signals
The future probes of the GWs
Summary
A The stability of the potential
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