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Test 01 — Age–Temperature Expansion Consistency Test

Does every claimed early-universe "distinction event" in the granularity story land at an age and temperature that standard expansion history actually supports? This is the first of 44 tests in the Early Universe Granularity Test Suite, and it is the load-bearing sanity check that every later test in the suite leans on.

✓ VERDICT: Agrees Early-universe expansion timeline

What we're checking

Observable
The cosmic age at each temperature milestone — the clock reading when the universe passes a given heat
Standard cosmology
Friedmann expansion with the known particle content sets each age, e.g. neutrino decoupling at T ≈ 1 MeV (t ≈ 1 s); recombination at z* = 1089.92 (t* ≈ 3.8×105 yr)
Granularity (consistency reading)
Reads history as records switching on step by step; each milestone lands on the same clock — the same ages, using the same expansion physics
Measured
T0 = 2.7255 ± 0.0006 K; z* = 1089.92 ± 0.25 (Planck 2018)
The epoch
A span, not the compared quantity: ~10−5 s (quark–hadron) → 380,000 yr (recombination)
Verdict
Agrees — by shared physics, not two independent numbers

Run the tape of the early universe forward and it keeps hitting the same marks. About a second in, the neutrinos stop talking to everything else — both roads put that at a temperature near 1 MeV. Three minutes in, the first light nuclei lock into place. And 380,000 years in, the fog clears at redshift z* = 1089.92, leaving the microwave glow we still read today at 2.7255 K. This is the master clock check, and it is the honest place to start.

Two very different ways of telling the story converge here. One is plain hot-Big-Bang cosmology, cooling and expanding on a fixed schedule. The other is this framework's picture, in which cosmic history is the history of what becomes recordable — a free quark isn't a thing you can count, but a proton is; two thermal baths aren't separate until each can be read on its own. Ask each road what time it is at every milestone, and the answers land on the same clock, epoch after epoch.

One point of honesty, kept in the open: this test is passed by agreement, not by a new prediction. The framework does not derive these ages independently — it inherits the same expansion physics and reads the same numbers, so the match confirms that its way of framing the story isn't contradicted by the timeline, rather than forcing the timeline from scratch. That is a consistency reading, and calling it anything stronger would be overclaiming. It is open for everyone to check: the ages, the redshift, and the temperature are all measured, and both roads have to meet them.

Read this before anything else on this page. This is the master timeline check, and it's a genuinely nice place to start: two independent ways of thinking about the early universe — plain hot-Big-Bang cosmology, and this framework's picture of the universe building up recordable distinctions step by step — land on the same clock. Quark confinement at ~20 microseconds, neutrinos going free at ~1 second, the first nuclei at ~3 minutes, atoms and the CMB at 380,000 years: every one of these lines up with the standard age-temperature relation, using the same Planck, HotQCD, and PDG numbers any textbook would cite. That agreement is the whole point of the test, and it earns real confidence — but agreement between two methods is not proof that the "recordable distinction" framing is the right way to read the physics; it only shows the framing isn't contradicted by the timing. Nothing about the sequence itself is in dispute here — the open questions in cosmology (inflation's exact slope, dark matter's identity, the lithium-7 anomaly) live on other pages in this suite, not this one.

1. Verdict

The number, both ways

Number we’re testing
The cosmic age at each temperature milestone — the clock reading when the universe passes a given heat
Standard cosmology & measured
Standard cosmology here is the measurement itself — Friedmann expansion sets each age: neutrino decoupling at T ≈ 1 MeV (t ≈ 1 s); recombination at z* = 1089.92 (t* ≈ 3.8×10⁵ yr); BBN window t ≈ 180–1000 s · T₀ = 2.7255 ± 0.0006 K (Fixsen 2009/COBE-FIRAS); z* = 1089.92 ± 0.25 (Planck 2018 VI)
This framework (granularity)
The independent read: Each milestone lands on the same clock — same ages, same expansion physics; computed t(1 MeV) ≈ 0.73 s, t(155 MeV QCD) ≈ 2.2–2.6×10⁻⁵ s, t(0.08 MeV BBN) ≈ 2.0×10² s
Agreement
"Same timeline, same numbers" — every claimed event quantitatively consistent with the standard age–temperature relation; passed by agreement via shared physics, not two independent numbers (consistency check — shared inputs)

Check the source → the calculation shown on this page (Data Used · Calculation Summary)

Agrees. Every claimed granularity/distinction-stabilization event listed below occurs at an age and temperature that is quantitatively consistent with the standard radiation-dominated (and, at late times, matter-dominated) expansion history. No claimed event requires a stability or binding scale that the ambient temperature at that epoch fails to support (in either direction). No claimed event contradicts BBN, CMB, or particle-physics timing constraints.

2. Tested Claim

The doctrine under test states: "Cosmic history is the history of increasing recordable distinction." Applied to timing, the specific claim audited here is: each proposed appearance of a particle, field phase, nucleus, atom, or stable record occurs at an age/temperature consistent with standard expansion history — i.e., the window \(W = \{\text{age}, \text{temperature/redshift}, \text{density/expansion regime}, \text{interactions}\}\) claimed for each transition is a window in which that transition is physically able to occur, per the Friedmann equations and the Standard Model particle content.

3. Data Used

QuantityValueSource
\(T_{\text{CMB},0}\)2.7255 ± 0.0006 KFixsen 2009 (COBE/FIRAS); used as standard reference value, e.g. Planck Collaboration 2018 (Planck 2018 VI, A&A 641, A6, published 2020)
Redshift of recombination \(z_\ast\)1089.92 ± 0.25Planck 2018 VI, Table 2 (base-ΛCDM, TT,TE,EE+lowE+lensing)
Age at recombination≈ 3.8 × 10⁵ yrPlanck 2018 VI, Table 2 (\(t_\ast\))
\(N_{\rm eff}\)3.044 (SM prediction) / 2.99 ± 0.17 (Planck 2018 measured)Bennett et al. 2021 (SM \(N_{\rm eff}\)=3.044); Planck 2018 VI
Neutrino decoupling temperature≈ 0.8–1 MeVStandard weak-interaction freeze-out estimate (Kolb & Turner; Dolgov 2002 review)
QCD confinement / hadronization temperature\(T_c \approx 156.5 \pm 1.5\) MeVHotQCD Collaboration, Bazavov et al. 2019 (lattice QCD crossover)
BBN light-element formation window\(T \approx 0.06\text{–}0.09\) MeV, \(t \approx 180\text{–}1000\) sParticle Data Group 2024, Big-Bang Nucleosynthesis review
Baryon density \(\Omega_b h^2\)0.02237 ± 0.00015Planck 2018 VI, Table 2
Planck time / temperature\(t_{\rm Pl}\approx5.39\times10^{-44}\) s, \(T_{\rm Pl}\approx1.42\times10^{32}\) KCODATA 2018 (Planck units from \(G,\hbar,c\))

4. Calculation Summary

For radiation domination, the standard age–temperature relation (e.g. Kolb & Turner, The Early Universe, eq. 3.36) is:

\[ t(T) \approx \frac{2.4}{\sqrt{g_*(T)}}\left(\frac{1\ \text{MeV}}{T}\right)^2\ \text{seconds} \]

where \(g_*(T)\) is the effective number of relativistic degrees of freedom at temperature \(T\) (in MeV). Applying this relation at three benchmark epochs and comparing to the standard literature values:

EpochT\(g_*\)Computed \(t\)Standard literature valueConsistent?
QCD hadronization155 MeV≈15–20 (crossover)≈ 2.2–2.6 × 10⁻⁵ s≈ 10 μs (order-of-magnitude standard estimate)Yes
Neutrino decoupling1 MeV10.75≈ 0.73 s≈ 1 s (standard textbook value)Yes
BBN (light-element freeze-out)0.08 MeV3.38≈ 2.0 × 10² s (≈ 3.4 min)≈ 3–17 min window (PDG 2024 BBN review)Yes

For recombination, the relation is no longer purely radiation-dominated, so the Planck 2018 fitted ΛCDM value is used directly rather than the radiation-only formula: \(z_\ast = 1089.92\), giving \(T_\ast = T_{\rm CMB,0}(1+z_\ast) \approx 2.7255\,\text{K}\times1090.9 \approx 2973\,\text{K} \approx 0.256\) eV, at age \(t_\ast \approx 3.8\times10^5\) yr — matching the Planck 2018 VI Table 2 value directly (same source, not an independent check, but internally consistent).

Cross-check for BBN abundance: at \(T\approx0.08\) MeV the deuterium photodissociation bottleneck lifts (binding energy 2.22 MeV vs. photon-to-baryon ratio \(\eta\approx6\times10^{-10}\) delays the "deuterium bottleneck" from the naive \(T\sim\)2.2 MeV down to \(T\sim0.07\)–0.09 MeV) — this is the standard mechanism, reproduced here only as a plausibility check, not re-derived.

Assumptions: Standard Model particle content and \(g_*(T)\) table (no new light species beyond \(N_{\rm eff}=3.044\)); flat ΛCDM background for late-time (\(z<3400\)) epochs; natural units (\(\hbar=c=k_B=1\)) converted to seconds/Kelvin via CODATA 2018 constants.

5. Granularity Interpretation

Under the doctrine being tested, each row above corresponds to a proposed step in "increasing recordable distinction": quark–gluon plasma → confined hadrons (QCD transition) is the point past which quarks are no longer separately propagating degrees of freedom but are bound into hadronic records; neutrino decoupling is the point past which the relic neutrino background becomes (in principle) a separately propagating, non-interacting record, distinguishable from the photon bath; BBN is the point past which specific nuclear species (D, ³He, ⁴He, ⁷Li) become long-lived, countable relic abundances; recombination is the point past which neutral atoms form and the photon bath free-streams as the observable CMB — the single most information-rich "recordable distinction" in the early universe. This test does not show that the granularity framing is required by the physics — only that it is not contradicted by the timing of any of these transitions.

6. Gate Routing

Granularity timing gate — this is the gate this entire test suite is anchored to. Because Test 01 closes, it does not by itself block or license any downstream test in the suite; each of the other 43 tests (interaction-rate/Hubble decoupling, \(g_*\) ledger, causal horizon, BBN light-element abundances, CMB acoustic peaks, etc.) carries its own independent numerical check. A closure here means the coarse timeline is sound enough to host those finer-grained tests — it is a necessary consistency floor, not a substitute for them.

7. Failure Mode

Not applicable — this test closed. For completeness, the failure modes that were checked for and not found: (a) no claimed transition requires a binding/stability energy scale that exceeds the ambient thermal energy at the wrong sign (e.g., nucleons binding before nuclear binding energies exceed \(T\)); (b) no field degree of freedom was treated as an already-stable recordable particle before its actual freeze-out/decoupling time; (c) no relic abundance was asserted without pointing to the standard calculation that produces it (BBN abundances and \(N_{\rm eff}\) are treated as measured/standard-computed inputs here, not re-derived — see Data Used); (d) no cross-epoch contradiction with BBN, CMB, or \(N_{\rm eff}\) constraints was introduced.

8. Next Action

Proceed to the more granular tests in the suite that this one licenses as a floor: Test 02 (interaction rate vs. Hubble rate decoupling — the actual freeze-out criterion, of which this test only checked the coarse timing), Test 03 (the full \(g_*(T)\) ledger used here, checked degree-of-freedom by degree-of-freedom), and Test 23 (BBN light-element abundances, checked quantitatively against measured D/H and \(Y_p\) rather than only checked for timing plausibility). No distinctive derivation is claimed or required to close this test — it inherits directly from standard hot-Big-Bang cosmology.

Summary table

FieldValue
Test number01 of 44
VerdictAgrees
Our answer vs standardSame timeline, same numbers — the recordable-distinction sequence lands exactly where standard hot-Big-Bang cosmology puts it.
Gate routeGranularity timing gate
Data vintagePlanck 2018 (2020 publication); HotQCD 2019; PDG 2024; Fixsen 2009

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