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Project-declaredLean 4.32.0 · mathlib@81a5d257c8e4

Two sided metric carleson has Lorentz Type

two_sided_metric_carleson_hasLorentzType

Plain-language statement

Assume the phase space is countable, a4a\ge4, 1<q<21<q<2, and every truncated Calderón-Zygmund operator TrT_r has the required uniform strong L2L^2 bound. Then the two-sided metric Carleson operator is bounded from Lorentz Lq,1L^{q,1} to weak Lorentz Lq,L^{q,\infty}, with the explicit project constant 4C(a,q)/q4C(a,q)/q.

Exact Lean statement

theorem two_sided_metric_carleson_hasLorentzType [Countable (Θ X)] (ha : 4 ≤ a)
  (hq : q ∈ Ioo 1 2)
  (hT : ∀ r > 0, HasBoundedStrongType (czOperator K r) 2 2 volume volume (C_Ts a)) :
    HasLorentzType (carlesonOperator K) q 1 q ⊤ volume volume (4 * (C10_0_1 a q) / q)

Formal artifact

Lean source

Canonical source
Full Lean sourceLean 4
theorem two_sided_metric_carleson_hasLorentzType [Countable (Θ X)] (ha : 4  a)  (hq : q  Ioo 1 2)  (hT :  r > 0, HasBoundedStrongType (czOperator K r) 2 2 volume volume (C_Ts a)) :    HasLorentzType (carlesonOperator K) q 1 q ⊤ volume volume (4 * (C10_0_1 a q) / q) := by  have hqq' := NNReal.HolderConjugate.conjExponent hq.1  rename_i m kernel cf cancel count  have : IsOneSidedKernel a K := by infer_instance  set kpd : KernelProofData a K := KernelProofData.mk d ha cf this  apply (two_sided_metric_carleson_hasRestrictedWeakType ha (mem_Ioc_of_Ioo hq) hqq' hT).hasLorentzType    (by simpa) (by simp) (by simp) (C10_0_1_pos hq.1)  · intro f hf    apply (carlesonOperator_measurable _).aestronglyMeasurable    apply (hf.memLp _).locallyIntegrable <;> simp [hq.1.le]  · intro f g hf hg    filter_upwards with x    apply carlesonOperator_add_le_add_carlesonOperator    · apply (hf.memLp _).locallyIntegrable <;> simp [hq.1.le]    · apply (hg.memLp _).locallyIntegrable <;> simp [hq.1.le]  · intro a f    filter_upwards with x    rw [carlesonOperator_const_smul']    exact le_of_eq rfl  · intro f fs hf h_meas h_norm_monotone h_lim G    have hf : LocallyIntegrable f volume := by      apply (hf.memLp _).locallyIntegrable <;> simp [hq.1.le]    have bound {n : } : ᵐ (a : X), ‖fs n a‖  ‖f a‖ := by      filter_upwards with x using (h_norm_monotone x).ge_of_tendsto (h_lim x).norm _    calc _      _  eLpNorm (fun x  Filter.liminf (fun n  carlesonOperator K (fs n) x) Filter.atTop) 1 (volume.restrict G) := by        apply eLpNorm_mono_enorm        intro x        apply carlesonOperator_le_liminf_carlesonOperator_of_tendsto (norm ∘ f)          (Filter.Eventually.of_forall h_meas) _ hf.norm (Filter.Eventually.of_forall h_lim)        filter_upwards; simpa      _  Filter.liminf (fun n  eLpNorm (carlesonOperator K (fs n)) 1 (volume.restrict G)) Filter.atTop := by        rw [eLpNorm_one_eq_lintegral_enorm]        simp_rw [eLpNorm_one_eq_lintegral_enorm, enorm_eq_self]        apply lintegral_liminf_le        intro n        exact carlesonOperator_measurable (hf.mono (h_meas _) bound)    exact Filter.liminf_le_limsup  · simp  · intro f g hfg    filter_upwards with x    rw [carlesonOperator_congr_ae hfg]
Project
Carleson formalization
License
Apache-2.0
Commit
74ef907d6bdb
Source
Carleson/TwoSidedCarleson/RestrictedWeakType.lean:49-93

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Related declarations

Project-declaredLean 4.32.0

Ae tendsto zero of distribution le

ae_tendsto_zero_of_distribution_le

Plain-language statement

Suppose that, for every error threshold δ>0\delta>0 and every measure tolerance ε>0\varepsilon>0, one can choose N0N_0 so that the set where supN>N0f(x)FN(x)\sup_{N>N_0}\lVert f(x)-F_N(x)\rVert exceeds δ\delta has measure at most ε\varepsilon. Then FN(x)F_N(x) converges to f(x)f(x) for almost every xx.

harmonic analysisFourier analysismeasure theory

Source project: Carleson formalization

Person-level attribution pending.

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Project-declaredLean 4.32.0

Antichain operator

antichain_operator

Plain-language statement

For an antichain A\mathfrak{A} of pairwise incomparable tiles, and measurable functions ff and gg bounded by the indicators of FF and GG, the pairing of gg with the Carleson sum over A\mathfrak{A} is controlled by the L2L^2 norms of ff and gg and by positive powers of the two tile-density parameters. Concretely, the bound is

C(a,q)dens1(A)(q1)/(8a4)dens2(A)1/q1/2f2g2.C(a,q)\,\mathrm{dens}_1(\mathfrak{A})^{(q-1)/(8a^4)}\,\mathrm{dens}_2(\mathfrak{A})^{1/q-1/2}\,\lVert f\rVert_2\lVert g\rVert_2.

harmonic analysisFourier analysismeasure theory

Source project: Carleson formalization

Person-level attribution pending.

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