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))
.
Equations
Instances For
The 2 x 2 complex matrices made up of components of the two Higgs fields.
Equations
- TwoHDM.fieldCompMatrix Φ1 Φ2 x = !![Φ1 x 0, Φ1 x 1; Φ2 x 0, Φ2 x 1]
Instances For
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
.
Instances For
An instance of NormedAddCommGroup
on Matrix (Fin 2) (Fin 2) ℂ
defined through
Matrix.normedAddCommGroup
.
Instances For
An instance of NormedSpace
on Matrix (Fin 2) (Fin 2) ℂ
defined through
Matrix.normedSpace
.
Instances For
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.
Equations
- TwoHDM.prodMatrix_invariant = { deps := [`TwoHDM.prodMatrix, `StandardModel.HiggsField.gaugeAction] }
Instances For
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