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a89d282 | 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 62 63 64 65 66 67 68 69 70 71 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86 87 88 89 90 91 92 93 94 95 96 97 98 99 100 101 102 103 104 105 106 107 108 109 110 111 112 113 114 115 116 117 118 119 120 121 122 123 124 125 126 127 128 129 130 131 132 133 134 135 136 137 138 139 140 141 142 143 144 145 146 147 148 149 150 151 152 153 154 155 156 157 158 159 160 161 162 163 164 165 166 167 168 169 170 171 172 173 174 175 176 177 178 179 180 181 182 183 184 185 186 187 188 189 190 191 192 193 194 195 196 197 198 199 200 201 202 203 204 205 206 207 208 209 210 211 212 213 214 215 216 217 218 219 220 221 222 223 224 225 226 227 228 229 230 231 232 233 234 235 236 237 238 239 240 241 242 243 244 245 246 247 248 249 250 251 252 253 254 255 256 257 258 259 260 261 262 263 264 265 266 267 268 269 270 271 272 273 274 275 276 277 278 279 280 281 282 283 284 285 286 287 288 289 290 291 292 293 294 295 296 297 298 299 300 301 302 303 304 305 306 307 308 309 310 311 312 313 314 315 316 317 318 319 320 321 | import OAI.Probability.InvariantIsing.Pressure.RandomCoefficientIBP
import OAI.Probability.InvariantIsing.Arrays.ReplicaCovariance
import OAI.Probability.InvariantIsing.Core.GGErrorAlgebra
import OAI.Probability.IsingPerceptron.JointGGClosure
namespace OAI
/-! GG estimates for Haar-dependent Gaussian perturbation tensors. -/
noncomputable section
open MeasureTheory ProbabilityTheory IsingPerceptron
open scoped BigOperators
namespace InvariantIsing
variable {Ω X : Type*} [MeasurableSpace Ω] [MeasurableSpace X]
/-- Expectation over external disorder and independent Gaussian coordinates. -/
def randomCoefficientAverage (P : Measure Ω) (ν : Ω → Measure X)
(A : Ω → X → ℕ →₀ ℝ) (t : ℝ) {r : ℕ} (D : Ω → (Fin r → X) → ℝ) : ℝ :=
∫ z : Ω × (ℕ → ℝ), referenceReplicaMean (ν z.1)
(fun x => t * cylinderField (A z.1 x) z.2) (D z.1) ∂P.prod gaussianCoordinates
def randomCoefficientEnergy (P : Measure Ω) (ν : Ω → Measure X)
(A : Ω → X → ℕ →₀ ℝ) (t : ℝ) {r : ℕ} (D : Ω → (Fin (r + 1) → X) → ℝ) : ℝ :=
∫ z : Ω × (ℕ → ℝ), referenceReplicaMean (ν z.1)
(fun x => t * cylinderField (A z.1 x) z.2)
(fun σ => cylinderField (A z.1 (σ 0)) z.2 * D z.1 σ) ∂P.prod gaussianCoordinates
variable [Countable X] [MeasurableSingletonClass X]
{P : Measure Ω} [IsProbabilityMeasure P] {ν : Ω → Measure X}
[∀ ω, IsProbabilityMeasure (ν ω)]
lemma randomCoefficientAverage_abs_le (hν : Measurable ν)
(A : Ω → X → ℕ →₀ ℝ)
(hAm : Measurable (fun p : (Ω × (ℕ → ℝ)) × X => cylinderField (A p.1.1 p.2) p.1.2))
(t : ℝ) {r : ℕ} (D : Ω → (Fin r → X) → ℝ)
(hDm : Measurable (Function.uncurry D)) {c : ℝ} (hc : 0 ≤ c)
(hD : ∀ ω σ, |D ω σ| ≤ c) : |randomCoefficientAverage P ν A t D| ≤ c := by
apply abs_integral_le_const_of_bound
· simpa only [cylinderField_smul] using
measurable_randomCoefficient_mean hν (fun ω x => t • A ω x)
(by simpa only [cylinderField_smul] using hAm.const_mul t) D hDm
· intro z
exact referenceReplicaMean_abs_le _ _ _ (measurable_of_countable _) hc (hD z.1)
lemma randomCoefficientAverage_one (hν : Measurable ν)
(A : Ω → X → ℕ →₀ ℝ)
(hAm : Measurable (fun p : (Ω × (ℕ → ℝ)) × X => cylinderField (A p.1.1 p.2) p.1.2))
{B : ℝ} (hA : ∀ ω x, (A ω x).sum (fun _ c => c ^ 2) ≤ B) (t : ℝ) (r : ℕ) :
randomCoefficientAverage P ν A t (fun (_ : Ω) (_ : Fin r → X) => 1) = 1 := by
unfold randomCoefficientAverage
calc
_ = ∫ _z : Ω × (ℕ → ℝ), (1 : ℝ) ∂P.prod gaussianCoordinates := by
apply integral_congr_ae
filter_upwards [randomCoefficient_all_exp_ae (P := P) hν A hAm hA] with z hz
exact referenceReplicaMean_const _ _ (hz t) r 1
_ = 1 := by simp
lemma randomCoefficientAverage_add_bounded (hν : Measurable ν)
(A : Ω → X → ℕ →₀ ℝ)
(hAm : Measurable (fun p : (Ω × (ℕ → ℝ)) × X => cylinderField (A p.1.1 p.2) p.1.2))
{B : ℝ} (hA : ∀ ω x, (A ω x).sum (fun _ c => c ^ 2) ≤ B)
(t : ℝ) {r : ℕ} (D E : Ω → (Fin r → X) → ℝ)
(hDm : Measurable (Function.uncurry D)) (hEm : Measurable (Function.uncurry E))
{c d : ℝ} (hc : 0 ≤ c) (hd : 0 ≤ d)
(hD : ∀ ω σ, |D ω σ| ≤ c) (hE : ∀ ω σ, |E ω σ| ≤ d) :
randomCoefficientAverage P ν A t (fun ω σ => D ω σ + E ω σ) =
randomCoefficientAverage P ν A t D + randomCoefficientAverage P ν A t E := by
have ht : Measurable (fun p : (Ω × (ℕ → ℝ)) × X =>
cylinderField (t • A p.1.1 p.2) p.1.2) := by
simpa only [cylinderField_smul] using hAm.const_mul t
have hiD := integrable_randomCoefficient_mean (P := P) hν
(fun ω x => t • A ω x) ht D hDm hc hD
have hiE := integrable_randomCoefficient_mean (P := P) hν
(fun ω x => t • A ω x) ht E hEm hd hE
simp only [cylinderField_smul] at hiD hiE
unfold randomCoefficientAverage
calc
_ = ∫ z : Ω × (ℕ → ℝ),
referenceReplicaMean (ν z.1) (fun x => t * cylinderField (A z.1 x) z.2) (D z.1) +
referenceReplicaMean (ν z.1) (fun x => t * cylinderField (A z.1 x) z.2) (E z.1)
∂P.prod gaussianCoordinates := by
apply integral_congr_ae
filter_upwards [randomCoefficient_all_exp_ae (P := P) hν A hAm hA] with z hz
exact referenceReplicaMean_add_bounded _ _ (hz t) _ _ (hD z.1) (hE z.1)
_ = _ := integral_add hiD hiE
/-- Conditional Gaussian integration by parts, with the diagonal retained. -/
theorem randomCoefficientEnergy_full_identity (hν : Measurable ν)
(A : Ω → X → ℕ →₀ ℝ)
(hAm : Measurable (fun p : (Ω × (ℕ → ℝ)) × X => cylinderField (A p.1.1 p.2) p.1.2))
(hcross : Measurable (fun p : Ω × (X × X) => cylinderCross (A p.1 p.2.1) (A p.1 p.2.2)))
{B : ℝ} (hA : ∀ ω x, (A ω x).sum (fun _ c => c ^ 2) ≤ B)
(t : ℝ) {r : ℕ} (D : Ω → (Fin (r + 1) → X) → ℝ)
(hDm : Measurable (Function.uncurry D)) {c : ℝ} (hc : 0 ≤ c)
(hD : ∀ ω σ, |D ω σ| ≤ c) :
randomCoefficientEnergy P ν A t D = t *
(randomCoefficientAverage P ν A t (fun ω σ => D ω σ *
(∑ i : Fin (r + 1), cylinderCross (A ω (σ 0)) (A ω (σ i)))) -
(r + 1 : ℕ) * randomCoefficientAverage P ν A t
(fun ω (τ : Fin (r + 1 + 1) → X) => D ω (Fin.tail τ) *
cylinderCross (A ω ((Fin.tail τ) 0)) (A ω (τ 0)))) := by
have h := joint_randomCoefficient_cylinder_insertion (P := P) hν
(fun ω x => t • A ω x) A
(by simpa only [cylinderField_smul] using hAm.const_mul t) hAm
(by simpa only [cylinderCross_smul_right] using hcross.const_mul t)
(fun ω x => by rw [cylinder_norm_smul]; exact mul_le_mul_of_nonneg_left (hA ω x) (sq_nonneg t))
hA D hDm hc hD
simp only [cylinderField_smul, cylinderCross_smul_right] at h
have heq (ω : Ω) : (fun σ : Fin (r + 1) → X =>
D ω σ * (∑ i, t * cylinderCross (A ω (σ 0)) (A ω (σ i)))) =
(fun σ => t * (D ω σ * ∑ i, cylinderCross (A ω (σ 0)) (A ω (σ i)))) := by
funext σ
rw [← Finset.mul_sum]
ring
have hfresh (ω : Ω) : (fun τ : Fin (r + 1 + 1) → X =>
D ω (Fin.tail τ) * (t * cylinderCross (A ω ((Fin.tail τ) 0)) (A ω (τ 0)))) =
(fun τ => t * (D ω (Fin.tail τ) *
cylinderCross (A ω ((Fin.tail τ) 0)) (A ω (τ 0)))) := by
funext τ
ring
simp_rw [heq, hfresh, referenceReplicaMean_const_mul] at h
rw [integral_const_mul, integral_const_mul] at h
change randomCoefficientEnergy P ν A t D = _ at h
rw [h]
unfold randomCoefficientAverage
ring
/-- Energy fluctuation bounds remain valid for Haar-dependent tensors and
Haar-dependent replica tests. -/
theorem randomCoefficient_energy_covariance_bound (hν : Measurable ν)
(A : Ω → X → ℕ →₀ ℝ)
(hAm : Measurable (fun p : (Ω × (ℕ → ℝ)) × X => cylinderField (A p.1.1 p.2) p.1.2))
{B : ℝ} (hA : ∀ ω x, (A ω x).sum (fun _ c => c ^ 2) ≤ B)
(t b : ℝ) {r : ℕ} (D : Ω → (Fin (r + 1) → X) → ℝ)
(hDm : Measurable (Function.uncurry D)) {c : ℝ} (hc : 0 ≤ c)
(hD : ∀ ω σ, |D ω σ| ≤ c)
(hE : Integrable (fun z : Ω × (ℕ → ℝ) => ∫ x,
|cylinderField (A z.1 x) z.2 - b|
∂(ν z.1).tilted (fun x => t * cylinderField (A z.1 x) z.2))
(P.prod gaussianCoordinates)) :
|randomCoefficientEnergy P ν A t D - b * randomCoefficientAverage P ν A t D| ≤
c * (∫ z : Ω × (ℕ → ℝ), ∫ x, |cylinderField (A z.1 x) z.2 - b|
∂(ν z.1).tilted (fun x => t * cylinderField (A z.1 x) z.2)
∂P.prod gaussianCoordinates) := by
have ht : Measurable (fun p : (Ω × (ℕ → ℝ)) × X =>
cylinderField (t • A p.1.1 p.2) p.1.2) := by
simpa only [cylinderField_smul] using hAm.const_mul t
have hiU := integrable_randomCoefficient_insertion (P := P) hν
(fun ω x => t • A ω x) A ht hAm
(fun ω x => by rw [cylinder_norm_smul]; exact mul_le_mul_of_nonneg_left (hA ω x) (sq_nonneg t))
hA D hDm hc hD
have hiV := integrable_randomCoefficient_mean (P := P) hν
(fun ω x => t • A ω x) ht D hDm hc hD
simp only [cylinderField_smul] at hiU hiV
have he := randomCoefficient_all_exp_ae (P := P) hν A hAm hA
have hY : ∀ᵐ z : Ω × (ℕ → ℝ) ∂P.prod gaussianCoordinates,
Integrable (fun x => cylinderField (A z.1 x) z.2)
((ν z.1).tilted (fun x => t * cylinderField (A z.1 x) z.2)) := by
filter_upwards [he] with z hz
exact (memLp_tilted_mul (mem_interior_integrableExpSet_of_all hz t) (1 : NNReal)).integrable
(by norm_num)
exact random_replica_energy_covariance_bound (ν := fun z : Ω × (ℕ → ℝ) => ν z.1)
(H := fun p => t * cylinderField (A p.1.1 p.2) p.1.2)
(Y := fun p => cylinderField (A p.1.1 p.2) p.1.2)
(fun p => D p.1.1 p.2)
(hDm.comp (measurable_fst.fst.prodMk measurable_snd)) hc (fun z => hD z.1) b
(he.mono fun _ hz => hz t) hY hiU hiV hE
/-- The finite GG comparison for the actual type of perturbations used here:
both coefficients and tests may depend on the external Haar disorder, and
the spectral self-overlap covariance remains an explicit error. -/
theorem randomCoefficient_gaussian_gg_bound (hν : Measurable ν)
(A : Ω → X → ℕ →₀ ℝ)
(hAm : Measurable (fun p : (Ω × (ℕ → ℝ)) × X => cylinderField (A p.1.1 p.2) p.1.2))
(hcross : Measurable (fun p : Ω × (X × X) => cylinderCross (A p.1 p.2.1) (A p.1 p.2.2)))
{B : ℝ} (hA : ∀ ω x, (A ω x).sum (fun _ c => c ^ 2) ≤ B)
(t b : ℝ) {r : ℕ} (D : Ω → (Fin (r + 1) → X) → ℝ)
(hDm : Measurable (Function.uncurry D)) {c : ℝ} (hc : 0 ≤ c)
(hD : ∀ ω σ, |D ω σ| ≤ c)
(hE : Integrable (fun z : Ω × (ℕ → ℝ) => ∫ x,
|cylinderField (A z.1 x) z.2 - b|
∂(ν z.1).tilted (fun x => t * cylinderField (A z.1 x) z.2))
(P.prod gaussianCoordinates)) :
|t| * |(r + 1 : ℕ) * randomCoefficientAverage P ν A t
(fun ω (τ : Fin (r + 1 + 1) → X) => D ω (Fin.tail τ) *
cylinderCross (A ω ((Fin.tail τ) 0)) (A ω (τ 0))) -
randomCoefficientAverage P ν A t D * randomCoefficientAverage P ν A t
(fun ω (τ : Fin 2 → X) => cylinderCross (A ω (τ 1)) (A ω (τ 0))) -
randomCoefficientAverage P ν A t
(fun ω σ => D ω σ * ∑ l : Fin r, cylinderCross (A ω (σ 0)) (A ω (σ l.succ)))| ≤
2 * c * (∫ z : Ω × (ℕ → ℝ), ∫ x, |cylinderField (A z.1 x) z.2 - b|
∂(ν z.1).tilted (fun x => t * cylinderField (A z.1 x) z.2)
∂P.prod gaussianCoordinates) +
|t| * |randomCoefficientAverage P ν A t
(fun ω σ => D ω σ * cylinderCross (A ω (σ 0)) (A ω (σ 0))) -
randomCoefficientAverage P ν A t D * randomCoefficientAverage P ν A t
(fun ω (σ : Fin 1 → X) => cylinderCross (A ω (σ 0)) (A ω (σ 0)))| := by
let V := randomCoefficientAverage P ν A t D
let U := randomCoefficientEnergy P ν A t D
let M := randomCoefficientEnergy P ν A t (fun (_ : Ω) (_ : Fin 1 → X) => 1)
let E := ∫ z : Ω × (ℕ → ℝ), ∫ x, |cylinderField (A z.1 x) z.2 - b|
∂(ν z.1).tilted (fun x => t * cylinderField (A z.1 x) z.2)
∂P.prod gaussianCoordinates
let L := randomCoefficientAverage P ν A t
(fun ω σ => D ω σ * cylinderCross (A ω (σ 0)) (A ω (σ 0)))
let L₀ := randomCoefficientAverage P ν A t
(fun ω (σ : Fin 1 → X) => cylinderCross (A ω (σ 0)) (A ω (σ 0)))
have hEn : 0 ≤ E := integral_nonneg (fun _ => integral_nonneg (fun _ => abs_nonneg _))
have hU : |U - b * V| ≤ c * E :=
randomCoefficient_energy_covariance_bound hν A hAm hA t b D hDm hc hD hE
have hM : |M - b| ≤ E := by
have h := randomCoefficient_energy_covariance_bound (P := P) hν A hAm hA t b
(fun (_ : Ω) (_ : Fin (0 + 1) → X) => 1) measurable_const (c := 1) (by norm_num)
(fun _ _ => by norm_num) hE
change |M - b * randomCoefficientAverage P ν A t (fun (_ : Ω) (_ : Fin 1 → X) => 1)| ≤ 1 * E at h
simpa only [randomCoefficientAverage_one hν A hAm hA, mul_one, one_mul] using h
have hV : |V| ≤ c := randomCoefficientAverage_abs_le hν A hAm t D hDm hc hD
have hm : M = t * (L₀ - randomCoefficientAverage P ν A t
(fun ω (τ : Fin 2 → X) => cylinderCross (A ω (τ 1)) (A ω (τ 0)))) := by
have h := randomCoefficientEnergy_full_identity (P := P) (r := 0) hν A hAm hcross hA t
(fun (_ : Ω) (_ : Fin (0 + 1) → X) => 1) measurable_const (c := 1) (by norm_num)
(fun _ _ => by norm_num)
simpa only [Fin.sum_univ_succ, Fin.sum_univ_zero, add_zero, one_mul, Fin.tail,
Fin.succ_zero_eq_one, Nat.cast_one, Nat.zero_add] using h
have hdiagM : Measurable (Function.uncurry (fun ω (σ : Fin (r + 1) → X) =>
D ω σ * cylinderCross (A ω (σ 0)) (A ω (σ 0)))) := by
have hp : Measurable (fun p : Ω × (Fin (r + 1) → X) => (p.1, (p.2 0, p.2 0))) :=
measurable_fst.prodMk
(((measurable_pi_apply 0).comp measurable_snd).prodMk
((measurable_pi_apply 0).comp measurable_snd))
exact hDm.mul (hcross.comp hp)
have hoffM : Measurable (Function.uncurry (fun ω (σ : Fin (r + 1) → X) =>
D ω σ * ∑ l : Fin r, cylinderCross (A ω (σ 0)) (A ω (σ l.succ)))) := by
apply hDm.mul
apply Finset.measurable_sum
intro l _
have hp : Measurable (fun p : Ω × (Fin (r + 1) → X) => (p.1, (p.2 0, p.2 l.succ))) :=
measurable_fst.prodMk
(((measurable_pi_apply 0).comp measurable_snd).prodMk
((measurable_pi_apply l.succ).comp measurable_snd))
exact hcross.comp hp
have hdiag (ω : Ω) (σ : Fin (r + 1) → X) :
|D ω σ * cylinderCross (A ω (σ 0)) (A ω (σ 0))| ≤ c * |B| := by
rw [abs_mul]
exact mul_le_mul (hD ω σ) (cylinderCross_bound (A ω) (hA ω) _ _) (abs_nonneg _) hc
have hoff (ω : Ω) (σ : Fin (r + 1) → X) :
|D ω σ * ∑ l : Fin r, cylinderCross (A ω (σ 0)) (A ω (σ l.succ))| ≤ c * (r * |B|) := by
rw [abs_mul]
apply mul_le_mul (hD ω σ) _ (abs_nonneg _) hc
calc
_ ≤ ∑ l : Fin r, |cylinderCross (A ω (σ 0)) (A ω (σ l.succ))| :=
Finset.abs_sum_le_sum_abs _ _
_ ≤ ∑ _l : Fin r, |B| := Finset.sum_le_sum (fun _ _ => cylinderCross_bound (A ω) (hA ω) _ _)
_ = _ := by simp
have hu : U = t * (L + randomCoefficientAverage P ν A t
(fun ω σ => D ω σ * ∑ l : Fin r, cylinderCross (A ω (σ 0)) (A ω (σ l.succ))) -
(r + 1 : ℕ) * randomCoefficientAverage P ν A t
(fun ω (τ : Fin (r + 1 + 1) → X) => D ω (Fin.tail τ) *
cylinderCross (A ω ((Fin.tail τ) 0)) (A ω (τ 0)))) := by
have h := randomCoefficientEnergy_full_identity (P := P) hν A hAm hcross hA t D hDm hc hD
simp only [Fin.sum_univ_succ, mul_add] at h
rw [randomCoefficientAverage_add_bounded hν A hAm hA t _ _ hdiagM hoffM
(mul_nonneg hc (abs_nonneg _)) (by positivity) hdiag hoff] at h
exact h
exact gaussianGG_of_energy_identities hEn hU hM hV hu hm
/-- Gaussian mean logpartition bounds remain valid when the coefficient
vectors depend on the external rotation disorder. -/
lemma randomCoefficient_cgf_mean_bounds (hν : Measurable ν)
(A : Ω → X → ℕ →₀ ℝ)
(hAm : Measurable (fun p : (Ω × (ℕ → ℝ)) × X => cylinderField (A p.1.1 p.2) p.1.2))
{B : ℝ} (hA : ∀ ω x, (A ω x).sum (fun _ c => c ^ 2) ≤ B) (t : ℝ) :
0 ≤ (∫ z : Ω × (ℕ → ℝ), cgf (fun x => cylinderField (A z.1 x) z.2) (ν z.1) t
∂P.prod gaussianCoordinates) ∧
(∫ z : Ω × (ℕ → ℝ), cgf (fun x => cylinderField (A z.1 x) z.2) (ν z.1) t
∂P.prod gaussianCoordinates) ≤ t ^ 2 * B / 2 := by
have hi := integrable_randomCoefficient_cgf (P := P) hν A hAm hA t
rw [integral_prod _ hi]
refine ⟨integral_nonneg (fun ω => (cylinder_cgf_mean_bounds (ν ω) (A ω) (hA ω) t).1), ?_⟩
calc
_ ≤ ∫ _ : Ω, t ^ 2 * B / 2 ∂P := integral_mono hi.integral_prod_left
(integrable_const _) (fun ω => (cylinder_cgf_mean_bounds (ν ω) (A ω) (hA ω) t).2)
_ = _ := by simp
/-- The local-minimum fluctuation estimate applies to the actual
Haar-dependent Gaussian fields, rather than requiring fixed coefficients. -/
theorem randomCoefficient_energy_at_minimum (hν : Measurable ν)
(A : Ω → X → ℕ →₀ ℝ)
(hAm : Measurable (fun p : (Ω × (ℕ → ℝ)) × X => cylinderField (A p.1.1 p.2) p.1.2))
{B : ℝ} (hA : ∀ ω x, (A ω x).sum (fun _ c => c ^ 2) ≤ B)
{v c a s δ K : ℝ} (hs : 0 < s) (hK : 0 < K)
(hmin : ∀ t ∈ Set.Icc (v - s) (v + s),
-(∫ z : Ω × (ℕ → ℝ), cgf (fun x => cylinderField (A z.1 x) z.2) (ν z.1) v
∂P.prod gaussianCoordinates) + c * (v - a) ^ 2 ≤
-(∫ z : Ω × (ℕ → ℝ), cgf (fun x => cylinderField (A z.1 x) z.2) (ν z.1) t
∂P.prod gaussianCoordinates) + c * (t - a) ^ 2)
(hconc : ∀ t ∈ ({v - s, v, v + s} : Set ℝ),
(∫ z : Ω × (ℕ → ℝ), |cgf (fun x => cylinderField (A z.1 x) z.2) (ν z.1) t -
(∫ z' : Ω × (ℕ → ℝ), cgf (fun x => cylinderField (A z'.1 x) z'.2) (ν z'.1) t
∂P.prod gaussianCoordinates)| ∂P.prod gaussianCoordinates) ≤ δ) :
let E := fun z : Ω × (ℕ → ℝ) => ∫ x,
|cylinderField (A z.1 x) z.2 - 2 * c * (v - a)|
∂(ν z.1).tilted (fun x => v * cylinderField (A z.1 x) z.2)
Integrable E (P.prod gaussianCoordinates) ∧
(∫ z, E z ∂P.prod gaussianCoordinates) ≤ (2 * c + K ^ 2) / (2 * K) + c * s + 4 * δ / s := by
exact expected_tilted_energy_at_minimum (μ := P.prod gaussianCoordinates)
(ν := fun z : Ω × (ℕ → ℝ) => ν z.1)
(Y := fun p : (Ω × (ℕ → ℝ)) × X => cylinderField (A p.1.1 p.2) p.1.2)
(hν.comp measurable_fst) hAm hs hK
(randomCoefficient_all_exp_ae hν A hAm hA)
(integrable_randomCoefficient_cgf hν A hAm hA) hmin hconc
end InvariantIsing
end
end OAI
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