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import OAI.Probability.RadialTransition.BoltzmannMeasure
namespace OAI
universe uX uI
noncomputable section
open MeasureTheory Filter Set
open scoped ContDiff BigOperators NNReal ENNReal
namespace RadialTransition
lemma cell_young {D G n : ℝ} (hD : 0 < D) : n * G ≤ D / 4 * n^2 + G^2 / D := by
have hh := sq_nonneg (D*n - 2*G)
have he : G^2 / D * D = G^2 := div_mul_cancel₀ _ hD.ne'
nlinarith
theorem one_cell_exponential_moment {X : Type uX} [TopologicalSpace X] [MeasurableSpace X]
[BorelSpace X] [SecondCountableTopology X] (ν : Measure X) [IsFiniteMeasure ν]
(z : ℝ) {β D B J G : ℝ} (hβ : 0 ≤ β) (hD : 0 < D) (hJ : J ≤ D)
{H : ParticleState X → ℝ} (hH : Measurable H)
(henergy : ∀ x, (D-J/2) * (particleCount x : ℝ)^2 - B*particleCount x -
(particleCount x : ℝ)*G ≤ H x - H particleVacuum) :
(∫⁻ x, ENNReal.ofReal (Real.exp (β*D/4*(particleCount x : ℝ)^2 - β*H x)) ∂particleBase ν z) ≤
ENNReal.ofReal (Real.exp ((ν univ).toReal * Real.exp (z+β*B))) *
ENNReal.ofReal (Real.exp (β*G^2/D)) *
∫⁻ x, ENNReal.ofReal (Real.exp (-β*H x)) ∂particleBase ν z := by
let A := Real.exp (β*G^2/D - β*H particleVacuum)
have hm : Measurable (fun x => ENNReal.ofReal (Real.exp (-β*H x))) :=
(Real.measurable_exp.comp (measurable_const.mul hH)).ennreal_ofReal
have hlower : ENNReal.ofReal (Real.exp (-β*H particleVacuum)) ≤
∫⁻ x, ENNReal.ofReal (Real.exp (-β*H x)) ∂particleBase ν z := by
calc
_ = ∫⁻ x, ENNReal.ofReal (Real.exp (-β*H x)) ∂Measure.dirac particleVacuum :=
(lintegral_dirac' _ hm).symm
_ ≤ _ := lintegral_mono' (dirac_vacuum_le_particleBase ν z) le_rfl
have hupper : (∫⁻ x, ENNReal.ofReal (Real.exp (β*D/4*(particleCount x : ℝ)^2 - β*H x)) ∂particleBase ν z) ≤
ENNReal.ofReal A * ENNReal.ofReal (Real.exp ((ν univ).toReal * Real.exp (z+β*B))) := by
calc
_ ≤ ∫⁻ x, ENNReal.ofReal A * ENNReal.ofReal (Real.exp (β*B*particleCount x)) ∂particleBase ν z := by
apply lintegral_mono
intro x
dsimp only [A]
rw [← ENNReal.ofReal_mul (Real.exp_pos _).le, ← Real.exp_add]
apply ENNReal.ofReal_le_ofReal
apply Real.exp_le_exp.mpr
have hy := cell_young (G := G) (n := (particleCount x : ℝ)) hD
have hj := mul_nonneg (sub_nonneg.mpr hJ) (sq_nonneg (particleCount x : ℝ))
have he := mul_le_mul_of_nonneg_left (henergy x) hβ
have hy' := mul_le_mul_of_nonneg_left hy hβ
have hj' := mul_nonneg hβ hj
have heq : β * (G^2/D) = β*G^2/D := by ring
nlinarith
_ = _ := by rw [lintegral_const_mul' _ _ ENNReal.ofReal_ne_top, lintegral_exp_particleCount]
calc
_ ≤ _ := hupper
_ = ENNReal.ofReal (Real.exp ((ν univ).toReal * Real.exp (z+β*B))) *
ENNReal.ofReal (Real.exp (β*G^2/D)) * ENNReal.ofReal (Real.exp (-β*H particleVacuum)) := by
dsimp [A]
rw [sub_eq_add_neg, Real.exp_add, ENNReal.ofReal_mul (Real.exp_pos _).le]
rw [neg_mul]
ac_rfl
_ ≤ _ := mul_le_mul' le_rfl hlower
section ProductCells
variable {I : Type uI} [Fintype I] {X : I → Type uX}
[∀ i, TopologicalSpace (X i)] [∀ i, MeasurableSpace (X i)]
[∀ i, BorelSpace (X i)] [∀ i, SecondCountableTopology (X i)]
def cellN (i : I) (x : ∀ j, ParticleState (X j)) : ℝ := particleCount (x i)
omit [Fintype I] [∀ i, BorelSpace (X i)] [∀ i, SecondCountableTopology (X i)]
[∀ i, TopologicalSpace (X i)] [∀ i, MeasurableSpace (X i)] in
theorem cellN_nonneg (i : I) (x : ∀ j, ParticleState (X j)) : 0 ≤ cellN i x := Nat.cast_nonneg _
omit [Fintype I] [∀ i, BorelSpace (X i)] [∀ i, SecondCountableTopology (X i)]
[∀ i, MeasurableSpace (X i)] in
theorem measurable_cellN (i : I) : Measurable (cellN (X := X) i) :=
((show Measurable (fun n : ℕ => (n : ℝ)) from continuous_of_discreteTopology.measurable).comp
continuous_particleCount.measurable).comp (measurable_pi_apply i)
theorem integrable_exp_cell_total (ν : ∀ i, Measure (X i)) [∀ i, IsFiniteMeasure (ν i)]
(z c : ℝ) : Integrable (fun x => Real.exp (c * ∑ i, cellN i x))
(Measure.pi (fun i => particleBase (ν i) z)) := by
have hh := Integrable.fintype_prod_dep (fun i => integrable_exp_particleCount (ν i) z c)
convert hh using 1
ext x
rw [Finset.mul_sum, Real.exp_sum]
rfl
theorem cell_partition_pos (ν : ∀ i, Measure (X i)) [∀ i, IsFiniteMeasure (ν i)]
(z : ℝ) {E : (∀ i, ParticleState (X i)) → ℝ}
(hi : Integrable (fun x => Real.exp (-E x)) (Measure.pi (fun i => particleBase (ν i) z))) :
0 < boltzmannPartition (Measure.pi (fun i => particleBase (ν i) z)) E := by
apply (integral_pos_iff_support_of_nonneg (fun _ => (Real.exp_pos _).le) hi).mpr
have hs : Function.support (fun x => Real.exp (-E x)) = univ := by
ext x
simp [Function.support, Real.exp_ne_zero]
rw [hs]
rw [Measure.pi_univ]
apply pos_iff_ne_zero.mpr
apply Finset.prod_ne_zero_iff.mpr
intro i _
rw [particleBase_univ (measure_ne_top (ν i) univ)]
exact ENNReal.ofReal_ne_zero_iff.mpr (Real.exp_pos _)
theorem weighted_square_le {I : Type uI} [Fintype I] (w n : I → ℝ)
(hw : ∀ i, 0 ≤ w i) (hrow : ∑ i, w i ≤ 1) :
(∑ i, w i * n i)^2 ≤ ∑ i, w i * (n i)^2 := by
have hh := Finset.sum_sq_le_sum_mul_sum_of_sq_le_mul Finset.univ
(fun i _ => hw i) (fun i _ => mul_nonneg (hw i) (sq_nonneg (n i)))
(fun i (_ : i ∈ Finset.univ) => (show (w i * n i)^2 ≤ w i * (w i * (n i)^2) by nlinarith))
exact hh.trans (mul_le_of_le_one_left (Finset.sum_nonneg (fun i _ => mul_nonneg (hw i) (sq_nonneg (n i)))) hrow)
theorem integrable_cell_numerator (ν : ∀ i, Measure (X i)) [∀ i, IsFiniteMeasure (ν i)]
(z : ℝ) {D B : ℝ} {E f : (∀ i, ParticleState (X i)) → ℝ}
(hE : Measurable E) (hf : Measurable f)
(hstable : ∀ x, D/2 * ∑ i, (cellN i x)^2 - B * ∑ i, cellN i x ≤ E x)
(hfbound : ∀ x, f x ≤ D/2 * ∑ i, (cellN i x)^2) :
Integrable (fun x => Real.exp (f x - E x)) (Measure.pi (fun i => particleBase (ν i) z)) := by
apply (integrable_exp_cell_total ν z B).mono' (Real.measurable_exp.comp (hf.sub hE)).aestronglyMeasurable
filter_upwards [] with x
change |Real.exp (f x - E x)| ≤ Real.exp (B * ∑ i, cellN i x)
rw [abs_of_pos (Real.exp_pos _)]
exact Real.exp_le_exp.mpr (by linarith [hstable x, hfbound x])
theorem uniform_cell_exponential_moment [Nonempty I] [DecidableEq I]
(ν : ∀ i, Measure (X i)) [∀ i, IsFiniteMeasure (ν i)]
(z : ℝ) {D B V : ℝ} (hD : 0 < D) (hV : 0 ≤ V)
(hvol : ∀ i, (ν i univ).toReal ≤ V)
(θ : I → I → ℝ) (hθ : ∀ i j, 0 ≤ θ i j) (hθdiag : ∀ i, θ i i = 0)
(hrow : ∀ i, ∑ j, θ i j ≤ 1)
{E : (∀ i, ParticleState (X i)) → ℝ} (hE : Measurable E)
(hstable : ∀ x, D/2 * ∑ i, (cellN i x)^2 - B * ∑ i, cellN i x ≤ E x)
(hconditional : ∀ i x s, D/2 * (particleCount s : ℝ)^2 - B * particleCount s -
(particleCount s : ℝ) * (D/8 * ∑ j, θ i j * cellN j x) ≤
E (Function.update x i s) - E (Function.update x i particleVacuum)) :
∀ i, (∫ x, Real.exp (D/4 * (cellN i x)^2)
∂boltzmannMeasure (Measure.pi (fun j => particleBase (ν j) z)) E) ≤
Real.exp (16/15 * V * Real.exp (z+B)) := by
classical
let μ := Measure.pi (fun j => particleBase (ν j) z)
let F (i : I) (x : ∀ j, ParticleState (X j)) := D/4 * (cellN i x)^2
let g (i : I) (x : ∀ j, ParticleState (X j)) := (1/16:ℝ) * ∑ j, θ i j * F j x
let C := Real.exp (V * Real.exp (z+B))
have hFmeas (i : I) : Measurable (F i) := measurable_const.mul ((measurable_cellN i).pow_const 2)
have hF0 (i : I) (x : ∀ j, ParticleState (X j)) : 0 ≤ F i x := mul_nonneg (by positivity) (sq_nonneg _)
have hθ1 (i j : I) : θ i j ≤ 1 :=
(Finset.single_le_sum (fun k _ => hθ i k) (Finset.mem_univ j)).trans (hrow i)
have hFbound (i : I) (x : ∀ j, ParticleState (X j)) : F i x ≤ D/2 * ∑ j, (cellN j x)^2 := by
have hh := Finset.single_le_sum (s := Finset.univ) (f := fun j => (cellN j x)^2)
(fun _ _ => sq_nonneg _) (Finset.mem_univ i)
dsimp [F]
nlinarith [sq_nonneg (cellN i x)]
have hgmeas (i : I) : Measurable (g i) :=
measurable_const.mul (Finset.measurable_sum _ (fun j _ => measurable_const.mul (hFmeas j)))
have hgBound (i : I) (x : ∀ j, ParticleState (X j)) : g i x ≤ D/2 * ∑ j, (cellN j x)^2 := by
have hh := Finset.sum_le_sum (s := Finset.univ)
(fun j (_ : j ∈ Finset.univ) => mul_le_of_le_one_left (hF0 j x) (hθ1 i j))
have hsum : ∑ j, F j x = D/4 * ∑ j, (cellN j x)^2 := by simp only [F, Finset.mul_sum]
have hn : 0 ≤ ∑ j, (cellN j x)^2 := Finset.sum_nonneg (fun _ _ => sq_nonneg _)
dsimp only [g]
rw [hsum] at hh
nlinarith
have hiE : Integrable (fun x => Real.exp (-E x)) μ := by
simpa using integrable_cell_numerator ν z hE measurable_const hstable
(f := fun _ => 0) (fun x => mul_nonneg (by positivity) (Finset.sum_nonneg (fun _ _ => sq_nonneg _)))
have hp := cell_partition_pos ν z hiE
let := boltzmannMeasure_probability hiE hp
have hiF (i : I) := integrable_cell_numerator ν z hE (hFmeas i) hstable (hFbound i)
have hig (i : I) := integrable_cell_numerator ν z hE (hgmeas i) hstable (hgBound i)
have hif (i : I) : Integrable (fun x => Real.exp (F i x)) (boltzmannMeasure μ E) := by
apply integrable_boltzmann hE _ hp
convert hiF i using 1
ext x
rw [← Real.exp_add]
congr 1
ring
have hC1 : 1 ≤ C := Real.one_le_exp_iff.mpr (mul_nonneg hV (Real.exp_pos _).le)
have hint (i : I) : (∫ x, Real.exp (F i x) ∂boltzmannMeasure μ E) ≤
C*(∫ x, Real.exp (g i x) ∂boltzmannMeasure μ E) := by
have hfmeas : Measurable (fun x => ENNReal.ofReal (Real.exp (F i x - E x))) :=
(Real.measurable_exp.comp ((hFmeas i).sub hE)).ennreal_ofReal
have hgmeas' : Measurable (fun x => ENNReal.ofReal C * ENNReal.ofReal (Real.exp (g i x - E x))) :=
measurable_const.mul (Real.measurable_exp.comp ((hgmeas i).sub hE)).ennreal_ofReal
have hlocal : lmarginal (fun j => particleBase (ν j) z) {i}
(fun x => ENNReal.ofReal (Real.exp (F i x - E x))) ≤
lmarginal (fun j => particleBase (ν j) z) {i}
(fun x => ENNReal.ofReal C * ENNReal.ofReal (Real.exp (g i x - E x))) := by
rw [lmarginal_singleton, lmarginal_singleton]
intro x
have hginv (s : ParticleState (X i)) : g i (Function.update x i s) = g i x := by
dsimp only [g, F, cellN]
congr 1
apply Finset.sum_congr rfl
intro j _
by_cases hj : j = i
· subst j
simp [hθdiag]
· simp [Function.update_of_ne hj]
have hcur := one_cell_exponential_moment (ν i) z (β := 1) (D := D) (B := B) (J := D)
(G := D/8 * ∑ j, θ i j * cellN j x) (by norm_num) hD le_rfl
(H := fun s => E (Function.update x i s))
(hE.comp (measurable_update x (a := i))) (fun s => by
convert hconditional i x s using 1; ring)
have hG : (D/8 * ∑ j, θ i j * cellN j x)^2 / D ≤ g i x := by
have hh := weighted_square_le (θ i) (fun j => cellN j x) (hθ i) (hrow i)
have hs : ∑ j, θ i j * F j x = D/4 * ∑ j, θ i j * (cellN j x)^2 := by
dsimp only [F]
rw [Finset.mul_sum]
apply Finset.sum_congr rfl
intro j _
ring
dsimp only [g]
rw [hs]
apply (div_le_iff₀ hD).mpr
nlinarith [mul_nonneg (sq_nonneg D) (sub_nonneg.mpr hh)]
have hCi : Real.exp ((ν i univ).toReal * Real.exp (z+B)) ≤ C :=
Real.exp_le_exp.mpr (mul_le_mul_of_nonneg_right (hvol i) (Real.exp_pos _).le)
simp only [one_mul, neg_one_mul] at hcur
calc
_ = ∫⁻ s, ENNReal.ofReal (Real.exp (D/4*(particleCount s : ℝ)^2 -
E (Function.update x i s))) ∂particleBase (ν i) z := by
apply lintegral_congr
intro s
simp only [F, cellN, Function.update_self]
_ ≤ _ := hcur
_ ≤ ENNReal.ofReal C * ENNReal.ofReal (Real.exp (g i x)) *
∫⁻ s, ENNReal.ofReal (Real.exp (-E (Function.update x i s))) ∂particleBase (ν i) z := by
gcongr
_ = _ := by
rw [mul_assoc, ← lintegral_const_mul' _ _ ENNReal.ofReal_ne_top,
← lintegral_const_mul' _ _ ENNReal.ofReal_ne_top]
apply lintegral_congr
intro s
rw [hginv, Real.exp_sub]
simp only [div_eq_mul_inv, Real.exp_neg, ENNReal.ofReal_mul (Real.exp_pos _).le]
have htotal := lintegral_le_of_lmarginal_le {i} hfmeas hgmeas' hlocal
rw [lintegral_const_mul' _ _ ENNReal.ofReal_ne_top,
← ofReal_integral_eq_lintegral_ofReal (hiF i) (Eventually.of_forall (fun _ => (Real.exp_pos _).le)),
← ofReal_integral_eq_lintegral_ofReal (hig i) (Eventually.of_forall (fun _ => (Real.exp_pos _).le)),
← ENNReal.ofReal_mul (by linarith [hC1])] at htotal
have hr := (ENNReal.ofReal_le_ofReal_iff (mul_nonneg (by linarith [hC1])
(integral_nonneg (fun _ => (Real.exp_pos _).le)))).mp htotal
rw [integral_boltzmann hE, integral_boltzmann hE]
simp_rw [← Real.exp_add, neg_add_eq_sub]
have hh := mul_le_mul_of_nonneg_left hr (inv_nonneg.mpr hp.le)
nlinarith
have hc := occupation_moment_closure F θ hC1 (by norm_num : 0 ≤ (1/16:ℝ))
(by norm_num : (1/16:ℝ) < 1) hFmeas hF0 hif hθ hrow hint
intro i
convert hc i using 1
congr 1
dsimp [C]
rw [Real.log_exp]
ring
end ProductCells
end RadialTransition
end
end OAI