Results The timescale for abiogenesis is bounded above by T_abio ≤ n_{1/2} · ⌈log₂(N/8)⌉, a logarithmic bound from the half-life of the defect complexity budget.
Results · Life Frontier problem Internally addressed

Abiogenesis Timescale Bound from Geometric Decay

The timescale for abiogenesis is bounded above by T_abio ≤ n_{1/2} · ⌈log₂(N/8)⌉, a logarithmic bound from the half-life of the defect complexity budget.

Life High impact frontier problem Origin of Life Book VI
Public Manuscript Life cascade
In plain language

The timescale for abiogenesis is bounded above by T_abio ≤ n_{1/2} · ⌈log₂(N/8)⌉, a logarithmic bound from the half-life of the defect complexity budget.

Overview

VI.T45 proves a timescale bound for abiogenesis: the number of steps required for the Distinction+SelfDesc attractor to be reached is at most n_{1/2} · ⌈log₂(N/T)⌉, where n_{1/2} is the half-life of the complexity budget C(n), N is the initial complexity, and T = 8 is the Distinction threshold. The logarithmic scaling means abiogenesis can occur on geological (rather than astronomical) timescales for any reasonably complex prebiotic system, addressing the apparent timescale paradox.

Detail

A perennial challenge in origin-of-life research is the ‘abiogenesis paradox’: the probability of life arising by pure chance from a prebiotic soup is astronomically small, suggesting it could not have happened in the age of the universe. This is sometimes called the ‘Hoyle fallacy’ (Hoyle’s 747 assembled by a tornado in a junkyard).

VI.T45 internally addresses this paradox through a timescale bound. The key definitions (VI.D74–D77):

  • Complexity budget C(n) = N – D_n : the number of available self-assembly steps minus the number of defects at step n.
  • Distinction threshold T = 8: the minimum complexity required to satisfy all five τ-Distinction conditions.
  • Half-life n_{1/2}: the number of steps for the defect budget to halve (from the geometric decay rate (1–ιτ)^n of defect absorption, V part 3).

VI.L15 and VI.L16 prove that C(n) is monotone (non-decreasing) and the attractor basin is absorbing: once C(n) > T, the system cannot leave the basin without an external perturbation. VI.T44 proves the basin is entered under finite defect budget.

VI.T45 gives the timescale: once C(0) > 0 (any non-zero initial complexity), the attractor is reached in at most n_{1/2} · ⌈log₂(N/T)⌉ steps. For N ≈ 10³ (a few hundred chemical components), T = 8, and n_{1/2} ≈ geological timescale (millions of years), the bound is T_abio ≤ n_{1/2} · ⌈log₂(125)⌉ = 7 · n_{1/2} — well within geological time.

The logarithmic dependence on N/T is the key insight: even for very large initial systems, the timescale grows only logarithmically. This transforms the abiogenesis probability argument from an impossibility claim into an inevitability claim.

Result Statement

VI.T45: Abiogenesis timescale T_abio ≤ n_{1/2} · ⌈log₂(N/8)⌉. Logarithmic bound from geometric defect decay. For any prebiotic system with C(0) > 0, abiogenesis is reached in finite, geologically plausible time.

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