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Transporting an original-time variation by the reference clock

Proved
BianchiIX.hasDerivAt_referenceOriginalVariation

by trppppp · Nov 4, 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). For y=(m,u,v,w)∈R4y=(m,u,v,w)\in\mathbb R^4y=(m,u,v,w)∈R4, define

K(u,v,w)=u2+v2+w2−2(uv+vw+wu),κ=u(v+w−u),K(u,v,w)=u^2+v^2+w^2-2(uv+vw+wu),\qquad \kappa=u(v+w-u),K(u,v,w)=u2+v2+w2−2(uv+vw+wu),κ=u(v+w−u), Fm=−v2+w2+u(v−w)−mκ,Fu=12(1−m2−(v−w)2+u2)u,F_m=-v^2+w^2+u(v-w)-m\kappa,\qquad F_u=\tfrac12(1-m^2-(v-w)^2+u^2)u,Fm​=−v2+w2+u(v−w)−mκ,Fu​=21​(1−m2−(v−w)2+u2)u, Fv=(m−1−κ)v,Fw=(−m−1−κ)w,F=(Fm,Fu,Fv,Fw),F_v=(m-1-\kappa)v,\qquad F_w=(-m-1-\kappa)w,\qquad F=(F_m,F_u,F_v,F_w),Fv​=(m−1−κ)v,Fw​=(−m−1−κ)w,F=(Fm​,Fu​,Fv​,Fw​),

and E(m,v)=(m−1)2+v2E(m,v)=(m-1)^2+v^2E(m,v)=(m−1)2+v2.

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

ψ(p,z)=3 z1+p,Π(x)=(ψ(p,s),ψ(p,a),ψ(p,b),ψ(p,c)).\psi(p,z)=\frac{\sqrt3\,z}{1+p},\qquad \Pi(x)=(\psi(p,s),\psi(p,a),\psi(p,b),\psi(p,c)).ψ(p,z)=1+p3​z​,Π(x)=(ψ(p,s),ψ(p,a),ψ(p,b),ψ(p,c)).

For y=(m,u,v,w)y=(m,u,v,w)y=(m,u,v,w), set D(y)=3+m2+K(u,v,w)D(y)=3+m^2+K(u,v,w)D(y)=3+m2+K(u,v,w) and

ΞA(y)=(A−1,Am3,Au3,Av3,Aw3),Ξ(y)=Ξ6/D(y)(y).\Xi_A(y)=\left(A-1,\frac{Am}{\sqrt3},\frac{Au}{\sqrt3}, \frac{Av}{\sqrt3},\frac{Aw}{\sqrt3}\right),\qquad \Xi(y)=\Xi_{6/D(y)}(y).ΞA​(y)=(A−1,3​Am​,3​Au​,3​Av​,3​Aw​),Ξ(y)=Ξ6/D(y)​(y).

Write N(x)=(P,Q,r1a,r2b,r3c)N(x)=(P,Q,r_1a,r_2b,r_3c)N(x)=(P,Q,r1​a,r2​b,r3​c) for the normalized vector field and C(x)=C(p,s,a,b,c)\mathcal C(x)=C(p,s,a,b,c)C(x)=C(p,s,a,b,c) for its constraint.

The normalized and projective state spaces are R5\mathbb R^5R5 and R4\mathbb R^4R4 with their finite-product norms. The maps Π,Ξ,D,F\Pi,\Xi,D,FΠ,Ξ,D,F act on these state spaces.

For real k,tk,tk,t, define the boundary pulse

βk(t)=(mk(t),0,vk(t),0)=(1−ktanh⁡(kt),0,kcosh⁡(kt),0).\beta_k(t)=(m_k(t),0,v_k(t),0) =\left(1-k\tanh(kt),0,\frac{k}{\cosh(kt)},0\right).βk​(t)=(mk​(t),0,vk​(t),0)=(1−ktanh(kt),0,cosh(kt)k​,0).

Set

hk=arcosh⁡kk,Tk=(k2+4)arcosh⁡k3k,dk=k2−1,h_k=\frac{\operatorname{arcosh}k}{k},\qquad T_k=\frac{(k^2+4)\operatorname{arcosh}k}{3k},\qquad d_k=\sqrt{k^2-1},hk​=karcoshk​,Tk​=3k(k2+4)arcoshk​,dk​=k2−1​, Hk(t)=k2+46t−13log⁡cosh⁡(kt).H_k(t)=\frac{k^2+4}{6}t-\frac13\log\cosh(kt).Hk​(t)=6k2+4​t−31​logcosh(kt).

Use the total real conventions x/0=0x/0=0x/0=0, x=max⁡(x,0)\sqrt{x}=\sqrt{\max(x,0)}x​=max(x,0)​, log⁡0=0\log0=0log0=0, and log⁡x=log⁡∣x∣\log x=\log|x|logx=log∣x∣ for x<0x<0x<0, with arcosh⁡x=log⁡(x+x2−1)\operatorname{arcosh}x=\log(x+\sqrt{x^2-1})arcoshx=log(x+x2−1​). Write αx,0\alpha_{x,0}αx,0​ for the maximal normalized solution starting at xxx at time zero, with domain Imax⁡(x,0)I_{\max}(x,0)Imax​(x,0).

The positive transverse modes and crossing multipliers are

Mk,r(t)=e−rtcosh⁡(kt),μu(k)=e−karcosh⁡k,μw(k)=e−4arcosh⁡k/k.M_{k,r}(t)=e^{-rt}\cosh(kt),\qquad \mu_u(k)=e^{-k\operatorname{arcosh}k},\qquad \mu_w(k)=e^{-4\operatorname{arcosh}k/k}.Mk,r​(t)=e−rtcosh(kt),μu​(k)=e−karcoshk,μw​(k)=e−4arcoshk/k.

Define the variational velocity with tangent forcing by

Vk(t,ξ,a)=dFβk(t)ξ+aF(βk(t)).V_k(t,\xi,a)=dF_{\beta_k(t)}\xi+aF(\beta_k(t)).Vk​(t,ξ,a)=dFβk​(t)​ξ+aF(βk​(t)).

For ξ=(ξm,ξu,ξv,ξw)\xi=(\xi_m,\xi_u,\xi_v,\xi_w)ξ=(ξm​,ξu​,ξv​,ξw​), set

Jk(t,ξ)=2(mk(t)−1)ξm+2vk(t)ξv−4vk(t)ξu,J_k(t,\xi)=2(m_k(t)-1)\xi_m+2v_k(t)\xi_v-4v_k(t)\xi_u,Jk​(t,ξ)=2(mk​(t)−1)ξm​+2vk​(t)ξv​−4vk​(t)ξu​, Pkξ=(ξm−ξv/dk,ξu,0,ξw).P_k\xi=(\xi_m-\xi_v/d_k,\xi_u,0,\xi_w).Pk​ξ=(ξm​−ξv​/dk​,ξu​,0,ξw​).

Write G(y)=6F(y)/D(y)G(y)=6F(y)/D(y)G(y)=6F(y)/D(y) for the projective vector field in normalized time. At a fixed ttt, suppose

ξ′(c(t))=dGβk(t)ξ(c(t)),c′(t)=D(βk(t))/6.\xi'(c(t))=dG_{\beta_k(t)}\xi(c(t)),\qquad c'(t)=D(\beta_k(t))/6.ξ′(c(t))=dGβk​(t)​ξ(c(t)),c′(t)=D(βk​(t))/6.

Then

ddtξ(c(t))=Vk(t,ξ(c(t)),−dDβk(t)ξ(c(t))D(βk(t))).\frac{d}{dt}\xi(c(t)) =V_k\left(t,\xi(c(t)),-\frac{dD_{\beta_k(t)}\xi(c(t))}{D(\beta_k(t))}\right).dtd​ξ(c(t))=Vk​(t,ξ(c(t)),−D(βk​(t))dDβk​(t)​ξ(c(t))​).
Preamble
import Definitions.Def_BianchiIX_Dynamics_ReferencePulse
import Definitions.Def_BianchiIX_Dynamics_ReferenceScattering
import Definitions.Def_BianchiIX_Dynamics_ProjectiveOriginalTime
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.Analysis.Calculus.Deriv.Inv
import Mathlib.Tactic.FieldSimp
import Mathlib.Tactic.LinearCombination
import Mathlib.Analysis.SpecialFunctions.Arcosh
import Mathlib.MeasureTheory.Integral.IntervalIntegral.FundThmCalculus
import Mathlib.Analysis.Calculus.InverseFunctionTheorem.Deriv
import Mathlib.Analysis.Calculus.Deriv.MeanValue
import Mathlib.Analysis.SpecialFunctions.Pow.Deriv
import Mathlib.Analysis.SpecialFunctions.Integrals.Basic
import Mathlib.Analysis.ODE.ExistUnique

noncomputable section
open BianchiIX

Formal statement
theorem BianchiIX.hasDerivAt_referenceOriginalVariation {k t : ℝ} {xi : ℝ → ProjectiveState}
    {clock : ℝ → ℝ}
    (hxi : HasDerivAt xi
      (fderiv ℝ projectiveOriginalField (referencePulse k t) (xi (clock t))) (clock t))
    (hc : HasDerivAt clock (projectiveStateDenom (referencePulse k t) / 6) t) :
    HasDerivAt (fun s => xi (clock s))
      (referenceVariationVelocity k t (xi (clock t))
        (-fderiv ℝ projectiveStateDenom (referencePulse k t) (xi (clock t)) /
          projectiveStateDenom (referencePulse k t))) t := by sorry
Source
https://github.com/l46430640-del/ERA-STATISTICS-FORMAL/blob/d74c241819f896ab8d050b21ace80c8e90eabd9e/BianchiIX/Dynamics/ProjectiveOriginalTime.lean#L67-L79

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