Informal definitions and lemmas
See informal definitions and lemmas as a dependency graph.
This file is automatically generated using informal_lemma
and informal_definition
commands
appearing in the raw Lean code of HepLean.
There is an implicit invitation to the reader to contribute to the formalization of informal definitions and lemmas. You may also wish to contribute to HepLean by including informal definitions and lemmas in the raw Lean code, especially if you do not have a background in Lean.
HepLean.BeyondTheStandardModel.PatiSalam.Basic
Informal def: GaugeGroupI :=
The group SU(4) x SU(2) x SU(2)
.
- Physics description: The gauge group of the Pati-Salam model (unquotiented by ℤ₂).
- References: No references provided
- Dependencies:
Informal def: embedSM :=
The group homomorphism SU(3) x SU(2) x U(1) -> SU(4) x SU(2) x SU(2)
taking (h, g, α) to (blockdiag (α h, α ^ (-3)), g, diag(α ^ (3), α ^(-3))).
- Physics description: The embedding of the Standard Model gauge group into the Pati-Salam gauge group.
- References: Page 54 of https://math.ucr.edu/home/baez/guts.pdf
- Dependencies:
Informal def: gaugeGroupISpinEquiv :=
The equivalence between GaugeGroupI
and Spin(6) × Spin(4)
.
- Physics description: No physics description provided
- References: No references provided
- Dependencies:
Informal def: gaugeGroupℤ₂SubGroup := The ℤ₂-subgroup of ``GaugeGroupI with the non-trivial element (-1, -1, -1).
- Physics description: The ℤ₂-subgroup of the un-quotiented gauge group which acts trivially on all particles in the standard model.
- References: https://math.ucr.edu/home/baez/guts.pdf
- Dependencies:
Informal def: GaugeGroupℤ₂ :=
The quotient of ``GaugeGroupI by the ℤ₂-subgroup gaugeGroupℤ₂SubGroup
.
- Physics description: The gauge group of the Pati-Salam model with a ℤ₂ quotient.
- References: https://math.ucr.edu/home/baez/guts.pdf
- Dependencies:
Informal lemma: sm_ℤ₆_factor_through_gaugeGroupℤ₂SubGroup :=
The group StandardModel.gaugeGroupℤ₆SubGroup under the homomorphism
embedSM factors
through the subgroup ``gaugeGroupℤ₂SubGroup.
- Physics description: No physics description provided
- Proof description: No proof description provided
- References: No references provided
- Dependencies:
Informal def: embedSMℤ₆Toℤ₂ :=
The group homomorphism from StandardModel.GaugeGroupℤ₆ to
GaugeGroupℤ₂
induced by ``embedSM.
- Physics description: No physics description provided
- References: No references provided
- Dependencies:
HepLean.BeyondTheStandardModel.Spin10.Basic
Informal def: GaugeGroupI :=
The group Spin(10)
.
- Physics description: The gauge group of the Spin(10) model (aka SO(10)-model.)
- References: No references provided
- Dependencies:
Informal def: embedPatiSalam :=
The lift of the embedding SO(6) x SO(4) → SO(10)
to universal covers,
giving a homomorphism Spin(6) x Spin(4) → Spin(10)
. Precomposed with the isomorphism,
``PatiSalam.gaugeGroupISpinEquiv,
between SU(4) x SU(2) x SU(2)
and Spin(6) x Spin(4)
.
- Physics description: The embedding of the Pati-Salam gauge group into Spin(10).
- References: Page 56 of https://math.ucr.edu/home/baez/guts.pdf
- Dependencies:
HepLean.SpaceTime.LorentzGroup.Restricted
Informal def: Restricted := The subgroup of the Lorentz group consisting of elements which are proper and orthochronous.
- Physics description: No physics description provided
- References: No references provided
- Dependencies:
HepLean.SpaceTime.SL2C.Basic
Informal lemma: toLorentzGroup_det_one :=
The determinant of the image of SL(2, ℂ)
in the Lorentz group is one.
- Physics description: No physics description provided
- Proof description: No proof description provided
- References: No references provided
- Dependencies:
Informal lemma: toLorentzGroup_timeComp_nonneg :=
The time coponent of the image of SL(2, ℂ)
in the Lorentz group is non-negative.
- Physics description: No physics description provided
- Proof description: No proof description provided
- References: No references provided
- Dependencies:
Informal lemma: toRestrictedLorentzGroup :=
The homomorphism from SL(2, ℂ)
to the restricted Lorentz group.
- Physics description: No physics description provided
- Proof description: No proof description provided
- References: No references provided
- Dependencies:
HepLean.SpaceTime.WeylFermion.Basic
Informal def: leftHandedWeylFermion := The vector space ℂ^2 carrying the fundamental representation of SL(2,C).
- Physics description: A Weyl fermion with indices ψ_a.
- References: https://particle.physics.ucdavis.edu/modernsusy/slides/slideimages/spinorfeynrules.pdf
- Dependencies:
Informal def: rightHandedWeylFermion := The vector space ℂ^2 carrying the conjguate representation of SL(2,C).
- Physics description: A Weyl fermion with indices ψ_{dot a}.
- References: https://particle.physics.ucdavis.edu/modernsusy/slides/slideimages/spinorfeynrules.pdf
- Dependencies:
Informal def: altLeftHandedWeylFermion := The vector space ℂ^2 carrying the representation of SL(2,C) given by M → (M⁻¹)ᵀ.
- Physics description: A Weyl fermion with indices ψ^a.
- References: https://particle.physics.ucdavis.edu/modernsusy/slides/slideimages/spinorfeynrules.pdf
- Dependencies:
Informal def: altRightHandedWeylFermion := The vector space ℂ^2 carrying the representation of SL(2,C) given by M → (M⁻¹)^†.
- Physics description: A Weyl fermion with indices ψ^{dot a}.
- References: https://particle.physics.ucdavis.edu/modernsusy/slides/slideimages/spinorfeynrules.pdf
- Dependencies:
Informal def: leftHandedWeylFermionAltEquiv :=
The linear equiv between leftHandedWeylFermion and altLeftHandedWeylFermion given
by multiplying an element of rightHandedWeylFermion by the matrix εᵃ⁰ᵃ¹ = !![0, 1; -1, 0]]
.
- Physics description: No physics description provided
- References: No references provided
- Dependencies:
Informal lemma: leftHandedWeylFermionAltEquiv_equivariant := The linear equiv leftHandedWeylFermionAltEquiv is equivariant with respect to the action of SL(2,C) on leftHandedWeylFermion and altLeftHandedWeylFermion.
- Physics description: No physics description provided
- Proof description: No proof description provided
- References: No references provided
- Dependencies:
Informal def: rightHandedWeylFermionAltEquiv :=
The linear equiv between rightHandedWeylFermion and altRightHandedWeylFermion given
by multiplying an element of rightHandedWeylFermion by the matrix εᵃ⁰ᵃ¹ = !![0, 1; -1, 0]]
- Physics description: No physics description provided
- References: No references provided
- Dependencies:
Informal lemma: rightHandedWeylFermionAltEquiv_equivariant := The linear equiv rightHandedWeylFermionAltEquiv is equivariant with respect to the action of SL(2,C) on rightHandedWeylFermion and altRightHandedWeylFermion.
- Physics description: No physics description provided
- Proof description: No proof description provided
- References: No references provided
- Dependencies:
Informal def: leftAltWeylFermionContraction := The linear map from leftHandedWeylFermion ⊗ altLeftHandedWeylFermion to ℂ given by summing over components of leftHandedWeylFermion and altLeftHandedWeylFermion in the standard basis (i.e. the dot product).
- Physics description: The contraction of a left-handed Weyl fermion with a right-handed Weyl fermion. In index notation this is ψ_a φ^a.
- References: No references provided
- Dependencies:
Informal lemma: leftAltWeylFermionContraction_invariant := The contraction leftAltWeylFermionContraction is invariant with respect to the action of SL(2,C) on leftHandedWeylFermion and altLeftHandedWeylFermion.
- Physics description: No physics description provided
- Proof description: No proof description provided
- References: No references provided
- Dependencies:
Informal def: altLeftWeylFermionContraction := The linear map from altLeftHandedWeylFermion ⊗ leftHandedWeylFermion to ℂ given by summing over components of altLeftHandedWeylFermion and leftHandedWeylFermion in the standard basis (i.e. the dot product).
- Physics description: The contraction of a left-handed Weyl fermion with a right-handed Weyl fermion. In index notation this is φ^a ψ_a .
- References: No references provided
- Dependencies:
Informal lemma: leftAltWeylFermionContraction_symm_altLeftWeylFermionContraction := The linear map altLeftWeylFermionContraction is leftAltWeylFermionContraction composed with the braiding of the tensor product.
- Physics description: No physics description provided
- Proof description: No proof description provided
- References: No references provided
- Dependencies:
Informal lemma: altLeftWeylFermionContraction_invariant := The contraction altLeftWeylFermionContraction is invariant with respect to the action of SL(2,C) on leftHandedWeylFermion and altLeftHandedWeylFermion.
- Physics description: No physics description provided
- Proof description: No proof description provided
- References: No references provided
- Dependencies:
Informal def: rightAltWeylFermionContraction := The linear map from rightHandedWeylFermion ⊗ altRightHandedWeylFermion to ℂ given by summing over components of rightHandedWeylFermion and altRightHandedWeylFermion in the standard basis (i.e. the dot product).
- Physics description: The contraction of a right-handed Weyl fermion with a left-handed Weyl fermion. In index notation this is ψ_{dot a} φ^{dot a}.
- References: No references provided
- Dependencies:
Informal lemma: rightAltWeylFermionContraction_invariant := The contraction rightAltWeylFermionContraction is invariant with respect to the action of SL(2,C) on rightHandedWeylFermion and altRightHandedWeylFermion.
- Physics description: No physics description provided
- Proof description: No proof description provided
- References: No references provided
- Dependencies:
Informal def: altRightWeylFermionContraction := The linear map from altRightHandedWeylFermion ⊗ rightHandedWeylFermion to ℂ given by summing over components of altRightHandedWeylFermion and rightHandedWeylFermion in the standard basis (i.e. the dot product).
- Physics description: The contraction of a right-handed Weyl fermion with a left-handed Weyl fermion. In index notation this is φ^{dot a} ψ_{dot a}.
- References: No references provided
- Dependencies:
Informal lemma: rightAltWeylFermionContraction_symm_altRightWeylFermionContraction := The linear map altRightWeylFermionContraction is rightAltWeylFermionContraction composed with the braiding of the tensor product.
- Physics description: No physics description provided
- Proof description: No proof description provided
- References: No references provided
- Dependencies:
Informal lemma: altRightWeylFermionContraction_invariant := The contraction altRightWeylFermionContraction is invariant with respect to the action of SL(2,C) on rightHandedWeylFermion and altRightHandedWeylFermion.
- Physics description: No physics description provided
- Proof description: No proof description provided
- References: No references provided
- Dependencies:
HepLean.StandardModel.Basic
Informal def: gaugeGroupℤ₆SubGroup :=
The ℤ₆-subgroup of ``GaugeGroupI with elements (α^2 * I₃, α^(-3) * I₂, α), where α
is a sixth complex root of unity.
- Physics description: The subgroup of the un-quotiented gauge group which acts trivially on all particles in the standard model.
- References: https://math.ucr.edu/home/baez/guts.pdf
- Dependencies:
Informal def: GaugeGroupℤ₆ :=
The quotient of ``GaugeGroupI by the ℤ₆-subgroup gaugeGroupℤ₆SubGroup
.
- Physics description: The smallest possible gauge group of the Standard Model.
- References: https://math.ucr.edu/home/baez/guts.pdf
- Dependencies:
Informal def: gaugeGroupℤ₂SubGroup :=
The ℤ₂-subgroup of ``GaugeGroupI derived from the ℤ₂ subgroup of gaugeGroupℤ₆SubGroup
.
- Physics description: The ℤ₂subgroup of the un-quotiented gauge group which acts trivially on all particles in the standard model.
- References: https://math.ucr.edu/home/baez/guts.pdf
- Dependencies:
Informal def: GaugeGroupℤ₂ :=
The quotient of ``GaugeGroupI by the ℤ₂-subgroup gaugeGroupℤ₂SubGroup
.
- Physics description: The guage group of the Standard Model with a ℤ₂ quotient.
- References: https://math.ucr.edu/home/baez/guts.pdf
- Dependencies:
Informal def: gaugeGroupℤ₃SubGroup :=
The ℤ₃-subgroup of ``GaugeGroupI derived from the ℤ₃ subgroup of gaugeGroupℤ₆SubGroup
.
- Physics description: The ℤ₃-subgroup of the un-quotiented gauge group which acts trivially on all particles in the standard model.
- References: https://math.ucr.edu/home/baez/guts.pdf
- Dependencies:
Informal def: GaugeGroupℤ₃ :=
The quotient of ``GaugeGroupI by the ℤ₃-subgroup gaugeGroupℤ₃SubGroup
.
- Physics description: The guage group of the Standard Model with a ℤ₃-quotient.
- References: https://math.ucr.edu/home/baez/guts.pdf
- Dependencies:
Informal def: GaugeGroup :=
The map from GaugeGroupQuot
to Type
which gives the gauge group of the Standard Model
for a given choice of quotient.
- Physics description: The (global) gauge group of the Standard Model given a choice of quotient.
- References: https://math.ucr.edu/home/baez/guts.pdf
- Dependencies:
HepLean.StandardModel.HiggsBoson.Basic
Informal lemma: zero_is_zero_section :=
The HiggsField zero
defined by ofReal 0
is the constant zero-section of the bundle HiggsBundle
.
- Physics description: The zero Higgs field is the zero section of the Higgs bundle.
- Proof description: No proof description provided
- References: No references provided
- Dependencies:
HepLean.StandardModel.HiggsBoson.GaugeAction
Informal lemma: stability_group_single :=
The stablity group of the action of rep
on ![0, Complex.ofReal ‖φ‖]
,
for non-zero ‖φ‖
is the SU(3) x U(1)
subgroup of
gaugeGroup := SU(3) x SU(2) x U(1)
with the embedding given by
(g, e^{i θ}) ↦ (g, diag (e ^ {3 * i θ}, e ^ {- 3 * i θ}), e^{i θ})
.
- Physics description: The Higgs boson breaks electroweak symmetry down to the electromagnetic force.
- Proof description: No proof description provided
- References: No references provided
- Dependencies:
Informal lemma: stability_group :=
The subgroup of gaugeGroup := SU(3) x SU(2) x U(1)
which preserves every HiggsVec
by the action of ``StandardModel.HiggsVec.rep is given by SU(3) x ℤ₆
where ℤ₆
is the subgroup of SU(2) x U(1)
with elements (α^(-3) * I₂, α)
where
α is a sixth root of unity.
- Physics description: No physics description provided
- Proof description: No proof description provided
- References: No references provided
- Dependencies:
HepLean.StandardModel.HiggsBoson.Potential
Informal lemma: isBounded_iff_of_𝓵_zero :=
For P : Potential
then P.IsBounded if and only if P.μ2 ≤ 0.
That is to say - P.μ2 * ‖φ‖_H ^ 2 x
is bounded below if and only if P.μ2 ≤ 0
.
- Physics description: When there is no quartic coupling, the potential is bounded iff the mass squared is non-positive.
- Proof description: No proof description provided
- References: No references provided
- Dependencies: