Abstract

We find that a Z-string is stable in a wide range of parameter space of the two Higgs doublet model due to a split into a pair of two topological Z-strings with fractional Z fluxes. This configuration, a bound state of the two strings connected by a domain wall, is called a vortex molecule. Although the vortex molecule has no net topological charge, the locally induced topological charge density is polarized, namely distributed positively around one constituent string and negatively around the other constituent string, leading to the stability of the molecule. We numerically show that the vortex molecule is indeed a stable solution of the equation of motions in a much wider parameter space of the model than the usual axially symmetric Z-string in the Standard Model and the two Higgs doublet model, although it is not the case for experimental values of the parameters.

Highlights

  • In cosmology, they were expected to contribute to the anisotropy of the cosmic microwave background [1, 5, 6] and galaxy structure formation [1, 7, 8]

  • We find that a Z-string is stable in a wide range of parameter space of the two Higgs doublet model due to a split into a pair of two topological Z-strings with fractional Z fluxes

  • We numerically show that the vortex molecule is a stable solution of the equation of motions in a much wider parameter space of the model than the usual axially symmetric Z-string in the Standard Model and the two Higgs doublet model, it is not the case for experimental values of the parameters

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Summary

The Lagrangian and Higgs potential

We introduce two SU(2) doublets of Higgs scalar fields, Φ1 and Φ2, both with the hypercharge Y = 1. Dμ represents the covariant derivative acting on the Higgs fields, and the index i runs i = 1, 2. The most generic quartic potential V (Φ1, Φ2) for the two Higgs doublets is given by. We rewrite the Higgs fields in a two-by-two matrix form [80], H, defined by. The matrix scalar field H transforms under the electroweak SU(2)W × U(1)Y symmetry as i i. The VEV of H is expressed by a diagonal matrix H = diag(v1, v2), and the Higgs potential can be rewritten by using H as follows:. The parameter sets in the Higgs potential in eqs.

Custodial symmetry and CP symmetry
Basis transformation
Higgs mass spectrum with custodial symmetry
Electroweak strings in 2HDM: a review
Non-topological Z-string
Topological Z-strings
Asymptotics of topological Z-strings
Interaction between topological Z-strings
Analytic argument on vortex molecule
Conditions to avoid shrinking
Polarization of topological charge
Numerical analysis
Vortex molecule solution
Summary and discussion
A Difference of conventions from previous works
B Stability of Z-string in SM
C Derivation of interaction between topological Z-strings
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