OAI/Probability/InvariantIsing/Magnetic/MagneticSlabPDE.lean
10 declarations, 0 contain sorry, 0 declared as axioms
The literal inverse-coordinate PDE of a finite Gaussian slab, with spatial derivatives and inverse regularity discharged. Time here denotes applied variance; reversing it gives the manuscript's backward equation.
- def
OAI.InvariantIsing.magneticScalarSlabJetline 15 - lemma
OAI.InvariantIsing.magneticScalarInverseCurvature_eq_jetline 23 - lemma
OAI.InvariantIsing.magneticScalarSlabJet_curvature_posline 31 - def
OAI.InvariantIsing.magneticScalarInverseSlopeline 38 - def
OAI.InvariantIsing.magneticScalarInverseSecondline 44 - lemma
OAI.InvariantIsing.magneticScalarSlabBias_hasDerivAt_jetline 50 - lemma
OAI.InvariantIsing.magneticScalarInverseCurvature_hasDerivAt_spinline 58 - lemma
OAI.InvariantIsing.magneticScalarInverseSlope_hasDerivAtline 69 - lemma
OAI.InvariantIsing.magneticScalarInverse_second_derivline 84 - theorem
OAI.InvariantIsing.magneticScalarInverseCurvature_PDEline 95Source documentation
The actual inverse curvature solves the forward-variance version of
mag:inverse-PDEon every positive-variance slab.theorem magneticScalarInverseCurvature_PDE (L : List (ℝ × ℝ≥0)) (hL : ∀ av ∈ L, 0 < av.1) {ζ s v : ℝ} (hζ : 0 ≤ ζ) (hs : |s| < 1) (hv : 0 < v) : HasDerivAt (fun t => magneticScalarInverseCurvature L hL ζ t s) ((magneticScalarInverseCurvature L hL ζ v s) ^ 2 / 2 * deriv (deriv (magneticScalarInverseCurvature L hL ζ v)) s + ζ * (magneticScalarInverseCurvature L hL ζ v s) ^ 2) v := by …