Download lean/OAI/Probability/InvariantIsing/Magnetic/MagneticBlockError.lean from roseking/openAI-math-dataset: direct link, hf CLI and curl.
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https://huggingface.co/datasets/roseking/openAI-math-dataset/resolve/main/lean/OAI/Probability/InvariantIsing/Magnetic/MagneticBlockError.lean
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hf download hf://datasets/roseking/openAI-math-dataset/lean/OAI/Probability/InvariantIsing/Magnetic/MagneticBlockError.lean
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curl -L -o MagneticBlockError.lean https://huggingface.co/datasets/roseking/openAI-math-dataset/resolve/main/lean/OAI/Probability/InvariantIsing/Magnetic/MagneticBlockError.lean
3.26 kB
| import OAI.Probability.InvariantIsing.Magnetic.ConstrainedBlockMagneticEstimate | |
| import OAI.Probability.InvariantIsing.Magnetic.MagneticFieldParameter | |
| import Mathlib.Analysis.SpecificLimits.Basic | |
| namespace OAI | |
| /-! The finite block error vanishes uniformly over field partitions with | |
| bounded final height and magnetizations in a fixed interior interval. -/ | |
| noncomputable section | |
| open MeasureTheory ProbabilityTheory IsingPerceptron Filter | |
| open scoped BigOperators NNReal Topology | |
| namespace InvariantIsing | |
| def magneticUniformBiasBound (H r : ℝ) : ℝ := (Real.log 2 + H / 2) / (1 - r) | |
| lemma magneticBias_uniform_bound (h : FieldStep) {H r m : ℝ} | |
| (hr : r < 1) (hm : |m| ≤ r) (hH : h.height (Fin.last h.depth) ≤ H) : | |
| |magneticBias h m| ≤ magneticUniformBiasBound H r := by | |
| have hi := hm.trans_lt hr | |
| have hb := magneticBias_minimum_bound h hi hH (magneticBias_minimizes h hi) | |
| have hH0 := (h.nonneg (Fin.last h.depth)).trans hH | |
| exact hb.trans (div_le_div_of_nonneg_left (by positivity) (sub_pos.mpr hr) (by linarith)) | |
| lemma normalized_magneticBlockError {N : ℕ} (hN : 0 < N) (C A ε t : ℝ) : | |
| (N : ℝ)⁻¹ * (ε * (N * C) + (ε⁻¹ + t) * (A * Real.sqrt N) + | |
| N * Real.log (1 + Real.exp (-t))) = | |
| ε * C + (ε⁻¹ + t) * A / Real.sqrt N + Real.log (1 + Real.exp (-t)) := by | |
| have hn : (N : ℝ) ≠ 0 := by exact_mod_cast hN.ne' | |
| have hs : Real.sqrt (N : ℝ) ≠ 0 := (Real.sqrt_pos.mpr (by exact_mod_cast hN)).ne' | |
| have hs2 := Real.sq_sqrt (Nat.cast_nonneg N : (0 : ℝ) ≤ N) | |
| field_simp | |
| linear_combination (ε⁻¹ + t) * A * hs2 | |
| lemma log_one_add_exp_neg_tendsto : | |
| Tendsto (fun t : ℝ => Real.log (1 + Real.exp (-t))) atTop (𝓝 0) := by | |
| have he := Real.tendsto_exp_atBot.comp tendsto_neg_atTop_atBot | |
| have hh := (tendsto_const_nhds.add he).log (by norm_num : (1 : ℝ) + 0 ≠ 0) | |
| simpa only [add_zero, Real.log_one, Function.comp_apply] using hh | |
| theorem tendsto_zero_of_magneticBlockError (N : ℕ → ℕ) (hN : Tendsto N atTop atTop) | |
| (f : ℕ → ℝ) (hf : ∀ n, 0 ≤ f n) (C A : ℝ) (hC : 0 < C) | |
| (hb : ∀ ε : ℝ, 0 < ε → ∀ t : ℝ, 0 ≤ t → ∀ n, | |
| f n ≤ ε * C + (ε⁻¹ + t) * A / Real.sqrt (N n) + Real.log (1 + Real.exp (-t))) : | |
| Tendsto f atTop (𝓝 0) := by | |
| apply tendsto_order.2 | |
| constructor | |
| · intro a ha | |
| exact Eventually.of_forall (fun n => ha.trans_le (hf n)) | |
| · intro a ha | |
| let ε := a / (4 * C) | |
| have hε : 0 < ε := div_pos ha (by positivity) | |
| have hεC : ε * C = a / 4 := by dsimp [ε]; field_simp | |
| obtain ⟨t, ht, htl⟩ := ((eventually_ge_atTop (0 : ℝ)).and | |
| (log_one_add_exp_neg_tendsto.eventually (gt_mem_nhds (by linarith : (0 : ℝ) < a / 4)))).exists | |
| have hi : Tendsto (fun n => (Real.sqrt (N n : ℝ))⁻¹) atTop (𝓝 0) := | |
| tendsto_inv_atTop_zero.comp (Real.tendsto_sqrt_atTop.comp (tendsto_natCast_atTop_atTop.comp hN)) | |
| have hm : Tendsto (fun n => (ε⁻¹ + t) * A / Real.sqrt (N n)) atTop (𝓝 0) := by | |
| simpa only [div_eq_mul_inv, mul_zero] using hi.const_mul ((ε⁻¹ + t) * A) | |
| filter_upwards [hm.eventually (gt_mem_nhds (by linarith : (0 : ℝ) < a / 4))] with n hn | |
| have h := hb ε hε t ht n | |
| rw [hεC] at h | |
| linarith | |
| end InvariantIsing | |
| end | |
| end OAI | |