OAI/Probability/InvariantIsing/Magnetic/MagneticImplicitBias.lean
3 declarations, 0 contain sorry, 0 declared as axioms
Parametric inversion of a strictly increasing physical mean spin. This supplies the finite-dimensional inverse-coordinate and envelope steps without assuming differentiability of the minimizing bias.
- lemma
OAI.InvariantIsing.parametric_bias_continuousAtline 16 - lemma
OAI.InvariantIsing.parametric_bias_hasDerivAtline 41Source documentation
The implicit bias derivative follows from the derivative of the actual mean-spin map and the local root equation.
lemma parametric_bias_hasDerivAt {A : ℝ × ℝ → ℝ} {b : ℝ → ℝ} {t s a c : ℝ} (hb : ContinuousAt b t) (hc : c ≠ 0) (hA : HasFDerivAt A (pairLinear a c) (t, b t)) (he : ∀ᶠ q in 𝓝 t, A (q, b q) = s) : HasDerivAt b (-a / c) t := by … - lemma
OAI.InvariantIsing.parametric_bias_envelopeline 74Source documentation
Envelope differentiation with the bias response derived, rather than postulated, from the physical mean-spin equation.
lemma parametric_bias_envelope {U A : ℝ × ℝ → ℝ} {b : ℝ → ℝ} {t s a c v : ℝ} (hb : ContinuousAt b t) (hc : c ≠ 0) (hA : HasFDerivAt A (pairLinear a c) (t, b t)) (he : ∀ᶠ q in 𝓝 t, A (q, b q) = s) (hU : HasFDerivAt U (pairLinear v s) (t, b t)) : HasDerivAt (fun q => U (q, b q) - b q * s) v t := by …