The cosmic coincidence problem is one of the most unsettling questions of standard cosmology: while the dark-energy density stays constant, the matter density dilutes as a⁻³. These two quantities, seemingly entirely independent of each other, become comparable only within a brief window of cosmic history — and we sit exactly in that window. This review offers a common-origin solution to the problem from a planckon-based discrete framework and builds the framework self-containedly: the mathematical point is excluded from ontology (the rejection of zero) ; the planckon is the finite physical realization of the point; space is the folding cubic bond lattice of the nodes; time is not a dimensional axis but the measurement record of the occurrence of events (τ = n·tP). The energypotential ledger E (d) = (d+1) εP, U (d) = (3−d) εP is derived from the direction count of this geometry; the budget items are states of a single ledger — dark energy is the closed reserve of nodes that have not yet formed a bond (the d0 pool) ; dark matter is the chain remnant frozen after forming its first bond but failing to complete the climb (d1) ; visible matter is the fraction that finishes the closure and locks in (d3). The solution has four layers. Common origin: the two dark densities are not two independent substances but two fates of a single reservoir — there are no two free constants whose coincidence must be arranged. Common threshold: pairing and climbing are events of the same kind (bond formation) and are subject to the same freeze threshold; a single cooling event releases both dark remnants at once. Quantitative skeleton: the per-node energies are exact from the ledger (pool 3εP, frozen chain exactly one εP per node) ; the observed 68. 3/26. 8 ratio reduces to the proximity fd0/fd1 ≈ 0. 85 of two sibling populations. Magnitude proof: the time principle closes the magnitude component of the “why now” question — in every power-law era λ·n = H·t = O (1) is an identity, and the dark-energy density reduces to the clock-squared law: ρDE/ρP = (3ΩDE/8π) ·λ² ≈ 10⁻¹²³; the order 10⁻¹²² is not a tuned constant but the current reading of the event counter (n ≈ 8. 1×10⁶⁰). The distribution component, in turn, finds its form through the exact solution of the folding kinetics: the population fractions follow the three-axis binomial law (fd = C (3, d) ·a³⁻ᵈ (1−a) ᵈ), the sibling-population ratio reduces to a single parameter, and the stopping scale is derived within the framework by the full integration of the ledger set (Af/Ac = 1. 45–1. 46; Proposition 8; closed form log₂ (11/4) = 1. 4594 — the counting closure of the unified-cycle paper), yielding fd0/fd1 = 0. 8617 — within 1. 4% of the observed 0. 85. The derivation is free of budget circularity: the composite budget→stopping→budget map is a contraction (|dr′/dr| ≈ 0. 03) and converges to the attractor r* = 0. 877 from any initial 1 partition; the observation is also within 3. 2% of the attractor. The framework’s distinguishing prediction is recorded: the equation of state cannot be w = −1; a draining pool carries a w signature that deviates from −1, is strictly decreasing, and evolves in time.
Hamdi Barut (Thu,) studied this question.
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