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Project-declaredLean 4.32.0 · mathlib@81a5d257c8e4

Mul Operator has Dense Domain

QuantumMechanics.SpaceDHilbertSpace.mulOperator_hasDenseDomain

Plain-language statement

The multiplication operator corresponding to a μ-a.e. strongly measurable function is densely defined.

Exact Lean statement

lemma mulOperator_hasDenseDomain
    {μ : Measure (Space d)} {f : Space d → ℂ} (hf : AEStronglyMeasurable f μ) :
    (𝓜 μ f).HasDenseDomain

Formal artifact

Lean source

Canonical source
Full Lean sourceLean 4
lemma mulOperator_hasDenseDomain    {μ : Measure (Space d)} {f : Space d  ℂ} (hf : AEStronglyMeasurable f μ) :    (𝓜 μ f).HasDenseDomain := by  intro ψ  apply mem_closure_iff_seq_limit.mpr  obtain u, hu, hfu := hf.aemeasurable  let s :   Set (Space d) := fun n  u ⁻¹' (Metric.closedBall 0 n)  let φ :   SpaceDHilbertSpace d μ := fun n     mk ((memHS_coe ψ).indicator (Ω := s n) (by measurability))  have hφ :  n, φ n =ᵐ[μ] (s n).indicator ψ := fun n  coeFn_mk _  use φ  constructor  · intro n    refine memHS_iff.mpr by measurability, by measurability, ?_    refine HasFiniteIntegral.mono (memHS_iff.mp <| memHS_coe (n • φ n)).2.2 ?_    filter_upwards [hfu, coeFn_smul n (φ n), hφ n] with x h₁ h₂ h₃    by_cases hx : x  s n    · simp_rw [norm_pow, norm_norm, sq_le_sq, abs_norm]      calc        _ = ‖u x‖ * ‖φ n x‖ := by simp [h₁]        _  n * ‖φ n x‖ := mul_le_mul_of_nonneg_right (by simp_all [s]) (norm_nonneg _)        _ = ‖(n • φ n) x‖ := by simp [h₂,  Nat.cast_smul_eq_nsmul ℂ]    · simp [h₃, hx]  · apply tendsto_sub_nhds_zero_iff.mp    apply tendsto_zero_iff_tendsto_zero_lintegral_enorm_sq.mpr    have h :  n, ∫⁻ x, ‖(φ n - ψ) x‖ₑ ^ 2 ∂μ = ∫⁻ x, ‖(s n)ᶜ.indicator ψ x‖ₑ ^ 2 ∂μ := by      intro n      refine lintegral_congr_ae ?_      filter_upwards [coeFn_sub (φ n) ψ, hφ n] with x h₁ h₂      by_cases hx : x  s n <;> simp [hx, h₁, h₂]    simp_rw [h]    rw [ MeasureTheory.lintegral_zero:= Space d) (μ := μ)]    refine tendsto_lintegral_of_dominated_convergence' (fun x  ‖ψ x‖ₑ ^ 2) ?_ ?_ ?_ ?_    · measurability    · intro n      filter_upwards with x      by_cases hx : x  s n <;> simp [hx]    · have : ∫⁻ x, ‖‖ψ x‖ ^ 2‖ₑ ∂μ := (memHS_iff.mp <| memHS_coe ψ).2.2.ne      simp_all    · filter_upwards with x      rw [ zero_pow two_ne_zero,  enorm_zero (E := ℂ)]      refine ENNReal.Tendsto.pow (Tendsto.enorm (tendsto_nhds_of_eventually_eq ?_))      refine eventually_atTop.mpr ⌈‖u x‖⌉₊, fun n hn  ?_      suffices ‖u x‖  n by simp [s, this]      exact (Nat.le_ceil _).trans (by exact_mod_cast hn)
Project
Physlib
License
Apache-2.0
Commit
dd43e9e65791
Source
Physlib/QuantumMechanics/Operators/Multiplication.lean:133-177

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Project-declaredLean 4.32.0

Adiabatic relation log

adiabatic_relation_log

Plain-language statement

Adiabatic relation in logarithmic form: If S(Ua,Va,N) = S(Ub,Vb,N) with N fixed, then c * log (Ua/Ub) + log (Va/Vb) = 0.

physicsquantum field theoryrelativity

Source project: Physlib

Person-level attribution pending.

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Project-declaredLean 4.32.0

Adiabatic relation Ua Ub Va Vb

adiabatic_relation_UaUbVaVb

Plain-language statement

Adiabatic relation in product form: If S(Ua,Va,N) = S(Ub,Vb,N) with N fixed, then (Ua/Ub)^c * (Va/Vb) = 1.

physicsquantum field theoryrelativity

Source project: Physlib

Person-level attribution pending.

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