Forall reduced exists not potential Is Stable
TwoHiggsDoublet.forall_reduced_exists_not_potentialIsStable
Project documentation
A lemma invalidating the step in https://arxiv.org/pdf/hep-ph/0605184 leading to equation (4.4).
Exact Lean statement
lemma forall_reduced_exists_not_potentialIsStable :
∃ P, ¬ PotentialIsStable P ∧ (∀ k : EuclideanSpace ℝ (Fin 3), ‖k‖ ^ 2 ≤ 1 →
0 ≤ quarticTermReduced P k ∧ (quarticTermReduced P k = 0 → 0 ≤ massTermReduced P k))Formal artifact
Lean source
lemma forall_reduced_exists_not_potentialIsStable : ∃ P, ¬ PotentialIsStable P ∧ (∀ k : EuclideanSpace ℝ (Fin 3), ‖k‖ ^ 2 ≤ 1 → 0 ≤ quarticTermReduced P k ∧ (quarticTermReduced P k = 0 → 0 ≤ massTermReduced P k)) := by /- Construction of the explicit counter example. The reason that this counter example works is that: - There is a zero of the quartic term `z` on the boundary. - The quartic term is equal to `((k - z) · z)²`, as `k - z` approaches orthogonal to `z`, this becomes small on two accounts: the abs of `k - z` has to become small as `z` is on the boundary, and the angle between `k - z` and `z` also becomes small. - The mass term is of the form `-(k - z) · w` for some `w` orthogonal to `z`, so as `k - z` approaches orthogonal to `z`, the mass term becomes small only on the account that the abs of `k - z` becomes small. -/ refine ⟨.stabilityCounterExample, stabilityCounterExample_not_potentialIsStable, fun k hk => ⟨quarticTermReduced_stabilityCounterExample_nonneg k, fun hq => ?_⟩⟩ simp [quarticTermReduced_stabilityCounterExample] at hq simp only [PiLp.norm_sq_eq_of_L2, Real.norm_eq_abs, sq_abs, Fin.sum_univ_three, Fin.isValue] at hk have hk1 : k 1 = 0 := by nlinarith rw [massTermReduced_stabilityCounterExample, hk1]- Project
- Physlib
- License
- Apache-2.0
- Commit
- dd43e9e65791
- Source
- Physlib/Particles/BeyondTheStandardModel/TwoHDM/Potential.lean:889-907
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