Add Dissociated boring Energy le
AddDissociated.boringEnergy_le
Project documentation
If a finite set is additively dissociated, then its order- additive energy is at most , where is the project's Chang constant. This is the quantitative dissociated-set estimate used in the proof of Chang's lemma.
Exact Lean statement
lemma AddDissociated.boringEnergy_le [MeasurableSpace G] [DiscreteMeasurableSpace G] [DecidableEq G]
[Finite G] {s : Finset G} (hs : AddDissociated (s : Set G)) (n : ℕ) :
boringEnergy n s ≤ changConst ^ n * n ^ n * #s ^ nFormal artifact
Lean source
lemma AddDissociated.boringEnergy_le [MeasurableSpace G] [DiscreteMeasurableSpace G] [DecidableEq G] [Finite G] {s : Finset G} (hs : AddDissociated (s : Set G)) (n : ℕ) : boringEnergy n s ≤ changConst ^ n * n ^ n * #s ^ n := by cases nonempty_fintype G obtain rfl | hn := eq_or_ne n 0 · simp calc _ = (‖dft 𝟭_[(s : Set G)]‖ₙ_[↑(2 * n)] ^ (2 * n) : ℝ) := by rw [cLpNorm_dft_indicator_one_pow] _ ≤ (4 * rexp 2⁻¹ * sqrt ↑(2 * n) * ‖dft 𝟭_[(s : Set G)]‖ₙ_[2]) ^ (2 * n) := by gcongr refine rudin_ineq (le_mul_of_one_le_right zero_le_two <| Nat.one_le_iff_ne_zero.2 hn) (dft 𝟭_[(s : Set G), ℂ]) ?_ rwa [cft_dft, support_comp_eq_preimage, Set.support_indicator_one, Set.preimage_comp, Set.neg_preimage, addDissociated_neg, AddEquiv.addDissociated_preimage] _ = _ := by simp_rw [mul_pow, pow_mul, cL2Norm_dft_indicator_one] rw [← exp_nsmul, sq_sqrt (by positivity), sq_sqrt (by positivity)] simp_rw [← mul_pow] simp [changConst] ring_nf- Project
- Arithmetic Progressions Almost Periodicity
- License
- Apache-2.0
- Commit
- afafc42a5326
- Source
- APAP/Prereqs/Chang.lean:67-86
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