Gauge orbits for the 2HDM #
The main reference for material in this section is https://arxiv.org/pdf/hep-ph/0605184.
For two Higgs fields Φ₁ and Φ₂, the map from space time to 2 x 2 complex matrices
defined by ((Φ₁^†Φ₁, Φ₂^†Φ₁), (Φ₁^†Φ₂, Φ₂^†Φ₂)).
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The 2 x 2 complex matrices made up of components of the two Higgs fields.
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- TwoHDM.fieldCompMatrix Φ1 Φ2 x = !![Φ1 x 0, Φ1 x 1; Φ2 x 0, Φ2 x 1]
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The matrix prodMatrix Φ1 Φ2 x is equal to the square of fieldCompMatrix Φ1 Φ2 x.
An instance of PartialOrder on ℂ defined through Complex.partialOrder.
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An instance of NormedAddCommGroup on Matrix (Fin 2) (Fin 2) ℂ defined through
Matrix.normedAddCommGroup.
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An instance of NormedSpace on Matrix (Fin 2) (Fin 2) ℂ defined through
Matrix.normedSpace.
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The matrix prodMatrix is positive semi-definite.
The matrix prodMatrix is hermitian.
The map prodMatrix is a smooth function on spacetime.
The map prodMatrix is invariant under the simultaneous action of gaugeAction on the two
Higgs fields.
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Given any smooth map f from spacetime to 2-by-2 complex matrices landing on positive
semi-definite matrices, there exist smooth Higgs fields Φ1 and Φ2 such that f is equal to
prodMatrix Φ1 Φ2.
See https://arxiv.org/pdf/hep-ph/0605184