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Flux measures and first hitting data on labelled wall sections

Definition
BianchiIX_AxisSectionMeasureData

by trppppp · Nov 6, 2026 · Mathlib 0df444a (Lean v4.33.1)

bianchi-ix-era-statisticsdynamical-systems

For real variables p,s,a,b,cp,s,a,b,cp,s,a,b,c, set

K=a2+b2+c2−2(ab+bc+ca),S=p2+s2,C=S+K.K=a^2+b^2+c^2-2(ab+bc+ca),\qquad S=p^2+s^2,\qquad C=S+K.K=a2+b2+c2−2(ab+bc+ca),S=p2+s2,C=S+K.

The shear components and wall rates are

P=Kp−2a2+b2+c2+ab−2bc+ac,P=Kp-2a^2+b^2+c^2+ab-2bc+ac,P=Kp−2a2+b2+c2+ab−2bc+ac, Q=Ks+3(−b2+c2+ab−ac),Q=Ks+\sqrt{3}(-b^2+c^2+ab-ac),Q=Ks+3​(−b2+c2+ab−ac), r1=−S+2p,r2=−S−p+3s,r3=−S−p−3s.r_1=-S+2p,\qquad r_2=-S-p+\sqrt{3}s,\qquad r_3=-S-p-\sqrt{3}s.r1​=−S+2p,r2​=−S−p+3​s,r3​=−S−p−3​s.

These functions define the normalized vacuum Bianchi IX vector field (P,Q,r1a,r2b,r3c)(P,Q,r_1a,r_2b,r_3c)(P,Q,r1​a,r2​b,r3​c).

Let X=R5X=\mathbb R^5X=R5 with coordinates x=(p,s,a,b,c)x=(p,s,a,b,c)x=(p,s,a,b,c) and the sup norm. Write

F(x)=(P,Q,r1a,r2b,r3c),C(x)=C(p,s,a,b,c),F(x)=(P,Q,r_1a,r_2b,r_3c),\qquad \mathcal C(x)=C(p,s,a,b,c),F(x)=(P,Q,r1​a,r2​b,r3​c),C(x)=C(p,s,a,b,c),

and let W={(p,s,a,b,c)∈X:a>0, b>0, c>0}W=\{(p,s,a,b,c)\in X:a>0,\ b>0,\ c>0\}W={(p,s,a,b,c)∈X:a>0, b>0, c>0}.

Write N1(x)=aN_1(x)=aN1​(x)=a, N2(x)=bN_2(x)=bN2​(x)=b, and N3(x)=cN_3(x)=cN3​(x)=c. For initial data (x0,t0)(x_0,t_0)(x0​,t0​), let Imax⁡(x0,t0)I_{\max}(x_0,t_0)Imax​(x0​,t0​) be the union of all open convex domains of solutions with these initial data, and let αx0,t0\alpha_{x_0,t_0}αx0​,t0​​ be their compatible curve. A solution SSS has such a domain ISI_SIS​, a curve αS\alpha_SαS​, and αS(t0)=x0\alpha_S(t_0)=x_0αS​(t0​)=x0​.

Let L(X,X)\mathcal L(X,X)L(X,X) be the continuous linear operators on XXX and set

A(x)=dFx,F~(x,J)=(F(x),A(x)∘J).A(x)=dF_x,\qquad \widetilde F(x,J)=(F(x),A(x)\circ J).A(x)=dFx​,F(x,J)=(F(x),A(x)∘J).

For a fixed initial time t0t_0t0​, put

Dt0={(x,t):t∈Imax⁡(x,t0)},Φt0(x,t)=αx,t0(t),Jx,t0(t)=dxΦt0(x,t).\mathcal D_{t_0}=\{(x,t):t\in I_{\max}(x,t_0)\},\qquad \Phi_{t_0}(x,t)=\alpha_{x,t_0}(t),\qquad J_{x,t_0}(t)=d_x\Phi_{t_0}(x,t).Dt0​​={(x,t):t∈Imax​(x,t0​)},Φt0​​(x,t)=αx,t0​​(t),Jx,t0​​(t)=dx​Φt0​​(x,t).

Write λx=dCx:X→R\lambda_x=d\mathcal C_x:X\to\mathbb Rλx​=dCx​:X→R for the constraint differential.

For x=(p,s,a,b,c)x=(p,s,a,b,c)x=(p,s,a,b,c), define

H(x)=(abc)2/3,w(x)=abc(1+4H(x)),δ(x)=2K−3S,δˉ(x)=2(K+4H(x))1+4H(x),H(x)=(abc)^{2/3},\quad w(x)=abc(1+4H(x)),\quad \delta(x)=2K-3S,\quad \bar\delta(x)=\frac{2(K+4H(x))}{1+4H(x)},H(x)=(abc)2/3,w(x)=abc(1+4H(x)),δ(x)=2K−3S,δˉ(x)=1+4H(x)2(K+4H(x))​, V(x,t0,t)=w(x)det⁡Jx,t0(t)w(αx,t0(t)).V(x,t_0,t)=\frac{w(x)\det J_{x,t_0}(t)}{w(\alpha_{x,t_0}(t))}.V(x,t0​,t)=w(αx,t0​​(t))w(x)detJx,t0​​(t)​.

Write [L][L][L] for the matrix of a continuous linear operator L:X→XL:X\to XL:X→X in the standard basis. Set Ω(v0,…,v4)=det⁡(v0,…,v4)\Omega(v_0,\ldots,v_4)=\det(v_0,\ldots,v_4)Ω(v0​,…,v4​)=det(v0​,…,v4​),

ωx(v0,…,v3)=Ω(x/2,v0,…,v3)w(x),φx(v0,v1,v2)=ωx(F(x),v0,v1,v2).\omega_x(v_0,\ldots,v_3)=\frac{\Omega(x/2,v_0,\ldots,v_3)}{w(x)},\qquad \varphi_x(v_0,v_1,v_2)=\omega_x(F(x),v_0,v_1,v_2).ωx​(v0​,…,v3​)=w(x)Ω(x/2,v0​,…,v3​)​,φx​(v0​,v1​,v2​)=ωx​(F(x),v0​,v1​,v2​).

A normalized symmetry is a continuous linear equivalence L:X→XL:X\to XL:X→X satisfying

C(Lx)=C(x),Lx∈W ⟺ x∈W,F(Lx)=LF(x),w(Lx)=w(x),det⁡L=1.\mathcal C(Lx)=\mathcal C(x),\quad Lx\in W\ \Longleftrightarrow\ x\in W, \quad F(Lx)=LF(x),\quad w(Lx)=w(x),\quad\det L=1.C(Lx)=C(x),Lx∈W ⟺ x∈W,F(Lx)=LF(x),w(Lx)=w(x),detL=1.

These symmetries include the identity, composition, inverse, and the two maps

R(p,s,a,b,c)=((−p+3s)/2,(−3p−s)/2,b,c,a),S0(p,s,a,b,c)=(p,−s,a,c,b).R(p,s,a,b,c)=((-p+\sqrt3s)/2,(-\sqrt3p-s)/2,b,c,a),\qquad S_0(p,s,a,b,c)=(p,-s,a,c,b).R(p,s,a,b,c)=((−p+3​s)/2,(−3​p−s)/2,b,c,a),S0​(p,s,a,b,c)=(p,−s,a,c,b).

Transforming a solution replaces its curve α\alphaα by LαL\alphaLα and keeps its time domain.

Write Φts(x)=αx,s(t)\Phi^s_t(x)=\alpha_{x,s}(t)Φts​(x)=αx,s​(t), with domain I(x,s)I(x,s)I(x,s), and X={x:C(x)=1, Ni(x)>0 (i=1,2,3)}\mathcal X=\{x:\mathcal C(x)=1,\ N_i(x)>0\ (i=1,2,3)\}X={x:C(x)=1, Ni​(x)>0 (i=1,2,3)}. For y=(v,l,r)∈R3y=(v,l,r)\in\mathbb R^3y=(v,l,r)∈R3 and a wall height hhh, put

b=e−l,c=e−r,d=1−v2−K(h,b,c),Uh={y:d>0},ch(y)=(−d,v,h,b,c).b=e^{-l},\quad c=e^{-r},\quad d=1-v^2-K(h,b,c),\quad U_h=\{y:d>0\},\quad c_h(y)=(-\sqrt d,v,h,b,c).b=e−l,c=e−r,d=1−v2−K(h,b,c),Uh​={y:d>0},ch​(y)=(−d​,v,h,b,c).

For a normalized axis symmetry AAA, the chart is cA,h=A−1chc_{A,h}=A^{-1}c_hcA,h​=A−1ch​, with coordinates πA(x)=((Ax)1,−log⁡(Ax)3,−log⁡(Ax)4)\pi_A(x)=((Ax)_1,-\log (Ax)_3,-\log (Ax)_4)πA​(x)=((Ax)1​,−log(Ax)3​,−log(Ax)4​). At p=−dp=-\sqrt dp=−d​ its flux density and measure are

ρh(y)=p2+v2−2p2∣p∣(1+4(hbc)2/3),dμh=1Uhρh+ dy.\rho_h(y)=\frac{p^2+v^2-2p}{2|p|(1+4(hbc)^{2/3})}, \qquad d\mu_h={\bf1}_{U_h}\rho_h^+\,dy.ρh​(y)=2∣p∣(1+4(hbc)2/3)p2+v2−2p​,dμh​=1Uh​​ρh+​dy.

Write φ\varphiφ for the signed section flux and δˉ\bar\deltaδˉ for the corrected divergence. The three primary frames interchange axis zero with the chosen dominant axis.

For target frames BiB_iBi​, heights kik_iki​, and coordinate sets EiE_iEi​ put c(i,y)=cBi,ki(y)c(i,y)=c_{B_i,k_i}(y)c(i,y)=cBi​,ki​​(y), E⊔={(i,y):y∈Ei}E^\sqcup=\{(i,y):y\in E_i\}E⊔={(i,y):y∈Ei​} and νk=∑i(y↦(i,y))∗μki\nu_k=\sum_i(y\mapsto(i,y))_*\mu_{k_i}νk​=∑i​(y↦(i,y))∗​μki​​. A hit from z=(i,y)z=(i,y)z=(i,y) at time ttt starts with y∈Ukiy\in U_{k_i}y∈Uki​​ at t0t_0t0​, exists in the maximal domain, and reaches a target frame with its first wall at the prescribed height, negative first shear, and coordinates in the corresponding target set. Write H(z)H(z)H(z) for these times t>t0t>t_0t>t0​, and DE={z∈E⊔:H(z)≠∅}D_E=\{z\in E^\sqcup:H(z)\ne\varnothing\}DE​={z∈E⊔:H(z)=∅}. A wall arrival atlas from (A,h)(A,h)(A,h) gives countably many injective C1C^1C1 branches covering each crossing time in each target chart. For a branch q=(i,n)q=(i,n)q=(i,n) with map RqR_qRq​ and time τq\tau_qτq​, put

jq(y)=ρki(Rqy)∣det⁡DRq(y)∣/ρh(y).j_q(y)=\rho_{k_i}(R_qy)|\det DR_q(y)|/\rho_h(y).jq​(y)=ρki​​(Rq​y)∣detDRq​(y)∣/ρh​(y).

Given a time set III, an eligible point lies on the branch, has time in III and target in EiE_iEi​. Its delay is (τq−t0)+(\tau_q-t_0)^+(τq​−t0​)+ there and +∞+\infty+∞ otherwise. The first piece LqL_qLq​ consists of eligible points attaining the infimum of all delays with the least branch encoding.

The first delay is the infimum over eligible branches, and the first time is the initial time plus the real value of this delay. For general initial data at time zero, global hitting times are all existing times in the given time set with endpoint in a target chart image. The first state is the flow evaluated at the real value of the infimum of the nonnegative extended hitting times. A success target removes the corresponding labelled failure slice. Four-coordinate nullity of SSS means λ4(Q(S))=0\lambda_4(Q(S))=0λ4​(Q(S))=0 for every differentiable Q:R5→R4Q:\mathbb R^5\to\mathbb R^4Q:R5→R4.

Definition code
import Mathlib.MeasureTheory.Integral.Lebesgue.Markov
import Definitions.Def_BianchiIX_Dynamics_Normalized
import Mathlib.Analysis.Calculus.InverseFunctionTheorem.ContDiff
import Mathlib.MeasureTheory.Function.Jacobian
import Mathlib.Topology.Compactness.Lindelof
import Mathlib.Analysis.Calculus.Deriv.Pow
import Mathlib.Analysis.Calculus.Deriv.Mul
import Mathlib.Analysis.Calculus.Deriv.Add
import Mathlib.Analysis.Real.Sqrt
import Mathlib.Tactic.Linarith
import Mathlib.Tactic.Ring
import Mathlib.Analysis.Calculus.ContDiff.Operations
import Mathlib.Analysis.Calculus.Deriv.Prod
import Mathlib.Analysis.Calculus.MeanValue
import Mathlib.Data.Fin.VecNotation
import Mathlib.Tactic.FinCases
import Mathlib.Tactic.FunProp
import Mathlib.MeasureTheory.Constructions.Pi
import Definitions.Def_BianchiIX_AxisAndOrbitData
import Mathlib.Analysis.SpecialFunctions.Pow.Deriv
import Mathlib.Tactic.FieldSimp
import Mathlib.Analysis.SpecialFunctions.Integrals.Basic
import Mathlib.Analysis.ODE.ExistUnique
import Mathlib.Analysis.Calculus.FDeriv.Partial
import Mathlib.Analysis.SpecialFunctions.Sqrt
import Mathlib.Analysis.SpecialFunctions.Log.Deriv
import Mathlib.Topology.Instances.Matrix
import Mathlib.LinearAlgebra.Matrix.Trace
import Mathlib.Analysis.Calculus.FDeriv.Analytic
import Mathlib.Topology.Algebra.Module.Determinant
import Mathlib.Analysis.Calculus.Deriv.Pi
import Mathlib.LinearAlgebra.Determinant
import Mathlib.Data.Real.Basic
import Mathlib.LinearAlgebra.Alternating.Curry
import Mathlib.Analysis.Calculus.ImplicitContDiff
import Mathlib.MeasureTheory.Measure.WithDensity
import Definitions.Def_BianchiIX_Dynamics_MaximalFlow
import Definitions.Def_BianchiIX_Dynamics_AxisSymmetry
import Mathlib.Analysis.Normed.Module.FiniteDimension
import Mathlib.MeasureTheory.MeasurableSpace.Prod
import Mathlib.Analysis.Calculus.Deriv.Slope
import Mathlib.Topology.Compactness.Compact

section

/-! Strict expansion on a finite-measure invariant failure set, Section 7.1. -/

open MeasureTheory Set
open scoped ENNReal

namespace BianchiIX

variable {X : Type*} [MeasurableSpace X] {μ : Measure X}



/-- Iterates outside the return domain are excluded, even if a total extension is used. -/
def permanentFailure (R : X → X) (D E : Set X) : Set X :=
  {x | ∀ n : ℕ, R^[n] x ∈ D ∩ E}











end BianchiIX

end

section

noncomputable section

namespace BianchiIX

open Set MeasureTheory
open scoped Topology ENNReal

abbrev FourCoordinates := Fin 4 → ℝ

/-- Nullity after every differentiable four-dimensional coordinate observation. -/
def NullInFourCoordinates (S : Set NormalizedState) : Prop :=
  ∀ P : NormalizedState → FourCoordinates, Differentiable ℝ P → volume (P '' S) = 0















end BianchiIX

end
end

section

noncomputable section

namespace BianchiIX

open Set MeasureTheory
open scoped ENNReal





def mainWallMeasure (h : ℝ) : Measure SectionCoordinates :=
  (volume.restrict (mainWallChartDomain h)).withDensity (fun y => ENNReal.ofReal (mainWallChartDensity h y))











namespace MainWallArrival













end MainWallArrival



end BianchiIX

end
end

section

noncomputable section

namespace BianchiIX

open Set Filter MeasureTheory
open scoped Topology ENNReal

def transverseAxisWallOrbitPreimage (C : SectionCoordinates → NormalizedState)
    (A : NormalizedSymmetry) (h t₀ : ℝ) (Z : Set SectionCoordinates) : Set SectionCoordinates :=
  {y | ∃ t ∈ normalizedMaxDomain (C y) t₀, ∃ z ∈ Z,
    axisWallChart A h z = normalizedMaxCurve (C y) t₀ t}





end BianchiIX

end
end

section

noncomputable section

namespace BianchiIX

open Set MeasureTheory
open scoped ENNReal

/-- The sum of the verified coordinate flux measures on labelled section charts. -/
def axisFamilyMeasure {ι : Type*} [MeasurableSpace ι] (k : ι → ℝ) : Measure (ι × SectionCoordinates) :=
  Measure.sum (fun i => (mainWallMeasure (k i)).map (Prod.mk i))











end BianchiIX

end
end

section

noncomputable section

namespace BianchiIX

open Set MeasureTheory
open scoped ENNReal

namespace AxisWallArrival

variable {A B : NormalizedSymmetry} {h k t₀ : ℝ} (P : AxisWallArrival A B h k t₀)

def eligible (E : Set SectionCoordinates) (I : Set ℝ) : Set SectionCoordinates :=
  {y | y ∈ P.source ∧ P.coordinateTime y ∈ I ∧ P.map y ∈ E}



def delay (E : Set SectionCoordinates) (I : Set ℝ) : SectionCoordinates → ℝ≥0∞ := by
  classical
  exact (P.eligible E I).piecewise (fun y => ENNReal.ofReal (P.coordinateTime y - t₀)) (fun _ => ∞)







end AxisWallArrival

/-- Actual target hits; labels may overlap and are not identified with disjoint physical sections. -/
def axisFamilyHittingTimes {ι : Type*} (A : NormalizedSymmetry) (B : ι → NormalizedSymmetry)
    (h : ℝ) (k : ι → ℝ) (t₀ : ℝ) (E : ι → Set SectionCoordinates) (I : Set ℝ)
    (y : SectionCoordinates) : Set ℝ :=
  {t | t ∈ I ∧ ∃ i, (y, t) ∈ axisWallArrivalRelation A (B i) h (k i) t₀ ∧
    axisWallCoordinates (B i) (normalizedMaxCurve (axisWallChart A h y) t₀ t) ∈ E i}

def axisFamilyHittingDomain {ι : Type*} (A : NormalizedSymmetry) (B : ι → NormalizedSymmetry)
    (h : ℝ) (k : ι → ℝ) (t₀ : ℝ) (E : ι → Set SectionCoordinates) (I : Set ℝ) : Set SectionCoordinates :=
  {y | (axisFamilyHittingTimes A B h k t₀ E I y).Nonempty}

namespace AxisWallAtlasFamily

variable {ι : Type*} {A : NormalizedSymmetry} {B : ι → NormalizedSymmetry}
  {h t₀ : ℝ} {k : ι → ℝ} (C : AxisWallAtlasFamily A B h k t₀)





def firstDelay (E : ι → Set SectionCoordinates) (I : Set ℝ) (y : SectionCoordinates) : ℝ≥0∞ :=
  ⨅ i, ⨅ n, ((C i).branch n).delay (E i) I y





end AxisWallAtlasFamily



end BianchiIX

end
end

section

noncomputable section

namespace BianchiIX

open Set MeasureTheory
open scoped ENNReal

def globalAxisWallHittingTimes {ι : Type*} (A : ι → NormalizedSymmetry) (h : ι → ℝ)
    (B : ι → Set SectionCoordinates) (I : Set ℝ) (x : NormalizedState) : Set ℝ :=
  {t | t ∈ I ∧ t ∈ normalizedMaxDomain x 0 ∧
    ∃ i, ∃ y ∈ B i, axisWallChart (A i) (h i) y = normalizedMaxCurve x 0 t}

def globalAxisWallHittingDomain {ι : Type*} (A : ι → NormalizedSymmetry) (h : ι → ℝ)
    (B : ι → Set SectionCoordinates) (I : Set ℝ) : Set NormalizedState :=
  {x | (globalAxisWallHittingTimes A h B I x).Nonempty}





def globalAxisWallFirstDelay {ι : Type*} (A : ι → NormalizedSymmetry) (h : ι → ℝ)
    (B : ι → Set SectionCoordinates) (I : Set ℝ) (x : NormalizedState) : ℝ≥0∞ :=
  ⨅ t : globalAxisWallHittingTimes A h B I x, ENNReal.ofReal t.val













end BianchiIX

end
end

section

noncomputable section

namespace BianchiIX

open Set MeasureTheory
open scoped ENNReal





namespace AxisWallAtlasFamily

variable {ι : Type*} {A : NormalizedSymmetry} {B : ι → NormalizedSymmetry}
  {h t₀ : ℝ} {k : ι → ℝ} (C : AxisWallAtlasFamily A B h k t₀)





def firstTime (E : ι → Set SectionCoordinates) (I : Set ℝ) (y : SectionCoordinates) : ℝ :=
  t₀ + (C.firstDelay E I y).toReal







end AxisWallAtlasFamily



end BianchiIX

end
end

section

noncomputable section

namespace BianchiIX

open Set MeasureTheory
open scoped ENNReal



def globalAxisWallFirstTime {ι : Type*} (A : ι → NormalizedSymmetry) (h : ι → ℝ)
    (B : ι → Set SectionCoordinates) (I : Set ℝ) (x : NormalizedState) : ℝ :=
  (globalAxisWallFirstDelay A h B I x).toReal

def globalAxisWallFirstState {ι : Type*} (A : ι → NormalizedSymmetry) (h : ι → ℝ)
    (B : ι → Set SectionCoordinates) (I : Set ℝ) (x : NormalizedState) : NormalizedState :=
  normalizedMaxCurve x 0 (globalAxisWallFirstTime A h B I x)



















end BianchiIX

end
end

section

noncomputable section

namespace BianchiIX

open Set MeasureTheory
open scoped ENNReal

namespace MainWallArrivalAtlas









end MainWallArrivalAtlas





def cumulativeReturnTime {X : Type*} (R : X → X) (τ : X → ℝ) (t₀ : ℝ) (n : ℕ) (y : X) : ℝ :=
  t₀ + ∑ i ∈ Finset.range n, (τ (R^[i] y) - t₀)







end BianchiIX

end
end

section

noncomputable section

namespace BianchiIX

open Set MeasureTheory

def axisFamilyReturnTimes {ι : Type*} (B : ι → NormalizedSymmetry) (k : ι → ℝ) (t₀ : ℝ)
    (E : ι → Set SectionCoordinates) (z : ι × SectionCoordinates) : Set ℝ :=
  axisFamilyHittingTimes (B z.1) B (k z.1) k t₀ E (Ioi t₀) z.2

def axisFamilyReturnDomain {ι : Type*} (B : ι → NormalizedSymmetry) (k : ι → ℝ) (t₀ : ℝ)
    (E : ι → Set SectionCoordinates) : Set (ι × SectionCoordinates) :=
  {z | z.2 ∈ E z.1 ∧ (axisFamilyReturnTimes B k t₀ E z).Nonempty}







end BianchiIX

end
end

section

noncomputable section

namespace BianchiIX

open Set MeasureTheory
open scoped ENNReal

namespace AxisWallAtlasFamily

variable {ι : Type*} [Encodable ι] {A : NormalizedSymmetry} {B : ι → NormalizedSymmetry}
  {h t₀ : ℝ} {k : ι → ℝ} (C : AxisWallAtlasFamily A B h k t₀)

/-- Choose the first encoded target and branch among those attaining the true earliest time. -/
def firstPiece (E : ι → Set SectionCoordinates) (I : Set ℝ) (q : ι × ℕ) : Set SectionCoordinates :=
  {y | y ∈ ((C q.1).branch q.2).eligible (E q.1) I ∧
    ((C q.1).branch q.2).delay (E q.1) I y = C.firstDelay E I y ∧
    ∀ r : ι × ℕ, Encodable.encode r < Encodable.encode q →
      ((C r.1).branch r.2).delay (E r.1) I y ≠ C.firstDelay E I y}











end AxisWallAtlasFamily



end BianchiIX

end
end

section

noncomputable section

namespace BianchiIX

open Set MeasureTheory
open scoped ENNReal

def axisFamilyInfiniteReturns {ι : Type*} (B : ι → NormalizedSymmetry) (k : ι → ℝ) (t₀ : ℝ)
    (E : ι → Set SectionCoordinates) : Set (ι × SectionCoordinates) :=
  {z | z ∈ axisFamilySection E ∧ (axisFamilyReturnTimes B k t₀ E z).Infinite}







end BianchiIX

end
end

section

noncomputable section

namespace BianchiIX

open Set MeasureTheory
open scoped ENNReal

def axisFamilySuccessTargets {ι : Type*} (E : ι → Set SectionCoordinates)
    (F : Set (ι × SectionCoordinates)) (i : ι) : Set SectionCoordinates :=
  E i \ (Prod.mk i ⁻¹' F)









end BianchiIX

end
end
Source
https://github.com/l46430640-del/ERA-STATISTICS-FORMAL/tree/d74c241819f896ab8d050b21ace80c8e90eabd9e/BianchiIX

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