Motivation
The Friedmann spacetimes (FLRW spacetimes) are the explicit, spatially homogeneous and isotropic solutions of Einstein's field equations on which standard Big Bang cosmology is built. Under a pressureless (dust, p=0) equation of state they form a family indexed by a curvature parameter k: the critical spacetime k=0, the underdense spacetimes k<0 and the overdense spacetimes k>0. The current ΛCDM model fits supernova data with the critical Friedmann spacetime plus a cosmological constant (dark energy).
Alexander, Temple and Vogler (arXiv:2510.14228) study how stable the pressureless Friedmann spacetimes are under smooth, spherically symmetric (radial) perturbations near the Big Bang. They write the Einstein–Euler equations in self-similar variables (tˉ,ξ), ξ=rˉ/tˉ, a formulation introduced by Smoller, Temple and Vogler (Proc. R. Soc. A, 2017). In these variables the critical Friedmann spacetime is a time-independent solution. They argue that the instability of this rest point causes underdense perturbations to accelerate away from k<0 Friedmann spacetimes at intermediate times, and they propose this as a mechanism for the observed acceleration that needs no cosmological constant.
This mission formalizes the dynamical-systems core of that paper: the STV ODE of orders n=1 and n=2, its rest points and eigenvalues, the exact k<0 Friedmann trajectory, and the order-2 instability theorem.
Setting
Expand a solution that is smooth at the centre of symmetry in even powers of ξ:
z=κρrˉ2=z2(tˉ)ξ2+z4(tˉ)ξ4+… (density) and w=v/ξ=w0(tˉ)+w2(tˉ)ξ2+… (velocity). Collecting like powers of ξ gives, at each order n, a closed 2n×2n system tˉU˙=Fn(U), the STV ODE of order n. At order 1, in the unknowns (z2,w0):
tˉz˙2=2z2−3z2w0,tˉw˙0=−61z2+w0−w02.
At order 2, in (z2,w0,z4,w2), the system adds
tˉz˙4=125z22w0+4z4−5w0z4−5z2w2,tˉw˙2=−241z22+41z2w02−101z4+3w2−4w0w2.
The system is autonomous in log-time τ=lntˉ. Its rest points include the Minkowski point M=(0,1), resp. (0,1,0,0), and the critical Friedmann point SM=(34,32), resp. (34,32,2740,92). The p=0, k=−1 Friedmann spacetime with parameter Δ0>0 is given in parametric form by tˉ=2Δ0(sinh2θ−2θ) and explicit functions z~2,w~0,z~4,w~2 of θ>0 (equations (2.41), (2.43)).
Formalization targets
Goal: Theorem 8 at order n=2
Fix Δ0>0. Let S be the set of solutions of the order-2 STV ODE on tˉ∈(0,∞) that tend to SM as tˉ→0+, tend to M as tˉ→∞, and agree exactly with the k=−1 Friedmann spacetime at leading order, i.e. (z2,w0)(tˉ)=(z~2,w~0)(θ). Then
S={Ub:b∈R},b↦Ub injective,U0=(z~2,w~0,z~4,w~2).
So the k<0 Friedmann spacetime is one member of a one-parameter family of trajectories from SM to M. All members agree with it at leading order, and the others differ from it at order 2.
Milestones
- Corollary 1 at n=1: the rest points U,M,SM; the eigenpairs (32,(−9,23)) and (−1,(4,1)) at SM; M is degenerate stable.
- Corollary 1 at n=2: the rest points; the four eigenpairs (2.30)–(2.33) at SM; −1 is the only eigenvalue at M.
- Equation (2.29): for every k≥1 the block Pk of (2.26) at SM has eigenvalues 32k and 32k−5.
- Theorem 5 at n=1 and n=2: the explicit k=−1 Friedmann curve solves the STV ODE and runs from SM to M.
- Theorem 7: solutions tending to M satisfy z2,z4=O(tˉ−1) and w0−1,w2=O(tˉ−1lntˉ).
- Theorem 9 at n=2: some solutions that agree with Friedmann at leading order and decay to M blow up as tˉ→0+ instead of tending to SM.
Significance
The result. At order 1 every relevant trajectory is a Friedmann spacetime. Order 2 is the first order where the instability of SM (the second positive eigenvalue 34) produces trajectories that agree with a k<0 Friedmann spacetime as tˉ→0 and as tˉ→∞ but differ from it in between. The paper reads this as an acceleration away from Friedmann spacetimes without dark energy. The extra eigenvalue −31 is why some perturbations do not have a self-similar Big Bang.
Formalizing it. The paper is an announcement: most claims are justified by eigenvalue computations and appeals to standard ODE theory (Hartman–Grobman, decay at degenerate nodes). A machine-checked proof of the order-2 statements would turn these appeals into explicit arguments for a concrete polynomial system. None of these results is known to have been formalized.
Difficulty
The eigenvalue milestones are finite computations. The trajectory milestones (Theorem 5) need hyperbolic-function identities and limits at θ→0+, where numerators and denominators both vanish to high order. The goal is harder because it is global. Linearizing at SM only describes trajectories near SM. One must also show that every member of the family exists for all time and reaches M, and that nothing outside the family belongs to S. Theorem 7 needs sharp decay rates at a rest point whose Jacobian is not diagonalizable, which is where the logarithm comes from.
Formalization scope
- Phase-space points are vectors
Fin 2 → ℝ or Fin 4 → ℝ, with coordinates ordered (z2,w0) and (z2,w0,z4,w2).
- A solution is a map U:R→R2n of log-time τ=lntˉ with U′(τ)=Fn(U(τ)) for every τ. Hence tˉ→0+ is τ→−∞, tˉ→∞ is τ→+∞, and tˉ=2Δ0(sinh2θ−2θ) becomes τ=log(Δ0⋅bigBangTime(θ)).
- Jacobians are Fréchet derivatives (
fderiv). Norms on R4 are sup norms.
- The goal requires a family parametrized by R that is injective, has range exactly S, and has U0 equal to the Friedmann curve. Exhibiting a single solution does not prove it.
- Out of scope: the derivation of the STV PDE and STV ODE from the Einstein–Euler equations (Theorems 1–3), the coordinate transformations (Theorems 4 and 6), and the general-order statements of Theorems 8–9. The paper does not write out the order-n system for general n, so these cannot be stated without first formalizing that derivation. Contributions in that direction are welcome.
- Discrepancy with the source: Corollary 1 says RM is the only eigenvector at M. For the explicit order-2 system (2.48)–(2.51) the −1 eigenspace at M is two-dimensional, so the order-2 milestone does not include that uniqueness claim.
Selected references
- C. Alexander, B. Temple, Z. Vogler, The Instability of the Critical Friedmann Spacetime at the Big Bang as an Alternative to Dark Energy, arXiv preprint, 2025. https://arxiv.org/abs/2510.14228
- J. Smoller, B. Temple, Z. Vogler, An instability of the standard model of cosmology creates the anomalous acceleration without dark energy, Proc. R. Soc. A 473 (2017). https://doi.org/10.1098/rspa.2016.0887