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Test 23 — Big Bang Nucleosynthesis Light-Element Test

Do the light-element abundances predicted by standard BBN — deuterium, helium-4, helium-3, and lithium-7 — match observation, given the measured baryon-to-photon ratio, neutron lifetime, and effective neutrino number, with the lithium-7 tension named honestly rather than hidden? Part of the 44-test Early Universe Granularity Test Suite, which checks whether the doctrine "cosmic history is the history of increasing recordable distinction" is consistent with standard cosmology and particle physics at each epoch — not whether it uniquely predicts that epoch.

Read this before the verdict: a CLOSED result on this page means the granularity interpretation — "stable nuclear records first form and lock in during the BBN window, not before or after it" — is consistent with established BBN physics and observation. It is not a claim that this framework uniquely predicted the light-element abundances, and it is not a derivation of \(\eta_B\), the neutron lifetime, or the nuclear reaction network from the framework's own geometry. Standard BBN theory, the reaction rates, and the observed abundances are consistent with standard cosmology — inherited directly from nuclear physics and the standard hot big bang, not something specific to this framework's geometry. The lithium-7 discrepancy is a known, unresolved tension in standard BBN itself (not introduced or fixed by this framework) and is reported here as such, not smoothed over.

Verdict: Agrees   consistent with standard cosmology

1. Verdict

The number, both ways

Number we’re testing
Primordial light-element abundances — deuterium (D/H), helium-4 (Y_p), helium-3, lithium-7
Standard cosmology
Standard BBN at Planck η_B = 6.12 × 10^-10, τ_n = 878.4 ± 0.5 s, N_eff = 3.044: D/H = (2.51 ± 0.11) × 10^-5; Y_p = 0.2470 ± 0.0002; ³He/H ≈ 1.0 × 10^-5; ⁷Li/H = (5.1 ± 0.4) × 10^-10
This framework (granularity)
No stable multi-nucleon record exists before this window; the abundances lock into a fixed record as it closes — same nuclear ledger, the framework reads it, it does not re-derive the inputs
Measured
D/H = (2.527 ± 0.030) × 10^-5 (Cooke et al. 2018); Y_p = 0.245 ± 0.003 (Aver et al. 2021); ³He/H ≈ (1.1 ± 0.2) × 10^-5; ⁷Li/H ≈ (1.6 ± 0.3) × 10^-10 (Spite plateau)
Agreement
D/H agrees within ~0.2σ (best-agreeing BBN probe); Y_p within ~0.7σ; ³He consistent (not a clean primordial probe); ⁷Li discrepant by factor ≈2.9–3 (~5σ) — the cosmological lithium problem, named openly (consistency check — shared inputs)

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

Agrees. The framework does not derive the baryon-to-photon ratio \(\eta_B\), the neutron lifetime, the nuclear reaction cross-sections, or the BBN reaction network from its own geometry — those are taken wholesale from particle physics, nuclear physics, and the Planck-measured baryon density. What the test can honestly check, and what does check out numerically for three of the four light elements, is the timing and consistency claim: that stable, recordable nuclear abundances (D, \(^4\)He, \(^3\)He) lock in at the BBN window (\(t\approx 1\)–20 min, \(T\approx 0.06\)–\(0.9\ {\rm MeV}\)) and match observation to within stated uncertainties, using only inputs measured independently of BBN itself. The fourth element, lithium-7, does not match: standard BBN over-predicts \(^7\)Li/H by a factor of \(\approx\)2.9–3 relative to observed metal-poor-star abundances — the long-standing "cosmological lithium problem." This is a known, unresolved tension in standard BBN itself, not a failure introduced or produced by this framework, and it is reported honestly as an open discrepancy rather than concealed. Per the guardrail "lithium tension handled honestly," that is exactly what determines the outcome here: three-out-of-four quantitative agreement plus one openly-flagged, independently-known tension is graded Agrees, not a clean CLOSED and not CONTRADICTED (a dedicated companion test, Test 24, treats the lithium tension itself in depth).

2. Tested Claim

The precise claim under test: "Given the independently-measured baryon-to-photon ratio \(\eta_B\) (from Planck 2018 CMB data), the measured free-neutron lifetime \(\tau_n\), and the Standard-Model value of the effective neutrino number \(N_{\rm eff}\), the standard BBN reaction network run at \(T\approx0.06\)–\(0.9\ {\rm MeV}\) (\(t\approx1\)–20 minutes) predicts light-element abundances (D/H, \(Y_p\), \(^3\)He/H, \(^7\)Li/H) that match observationally inferred primordial abundances, marking the epoch at which stable nuclear records first become locked in and recordable." This is evaluated as a consistency and timing claim, not a derivation claim: the framework does not compute \(\eta_B\), the nuclear cross-sections, or the neutron lifetime from its own geometry. It claims only that its granularity story — "no stable multi-nucleon record before BBN, a fixed nuclear-abundance record locked in by the end of it" — does not conflict with what nuclear physics and cosmology jointly require, and it must report the lithium anomaly honestly rather than hide it.

3. Data Used

QuantityValueSource
Baryon density (input to BBN) \(\Omega_b h^2 = 0.02237 \pm 0.00015\); equivalently \(\eta_B = n_B/n_\gamma = (6.12\pm0.04)\times10^{-10}\) Planck 2018 (arXiv:1807.06209), TT,TE,EE+lowE+lensing, Table 2
Free-neutron lifetime (input to BBN) \(\tau_n = 878.4 \pm 0.5\ {\rm s}\) Particle Data Group (PDG), Review of Particle Physics 2024
Effective number of neutrino species \(N_{\rm eff} = 3.044\) (Standard Model prediction, includes finite-temperature/QED corrections); Planck 2018 measured \(N_{\rm eff}=2.99\pm0.17\) Bennett, Buldgen, de Salas et al. (2021), arXiv:2012.02726; Planck 2018 (arXiv:1807.06209)
Standard-BBN predicted deuterium abundance D/H \(= (2.51\pm0.11)\times10^{-5}\) (theory, at Planck \(\eta_B\)) Fields, Molaro & Sarkar, PDG 2024 Big-Bang Nucleosynthesis review (and refs. therein, e.g. Pitrou et al. 2018, PRIMAT code)
Observed primordial deuterium abundance D/H \(= (2.527\pm0.030)\times10^{-5}\) (mean of metal-poor damped Ly-α QSO absorbers) Cooke, Pettini & Steidel (2018), ApJ 855, 102; PDG 2024 BBN review
Standard-BBN predicted helium-4 mass fraction \(Y_p = 0.2470 \pm 0.0002\) (theory, at Planck \(\eta_B\), \(N_{\rm eff}=3.044\)) PDG 2024 BBN review; Pitrou et al. (2018), Phys. Rept. 754, 1 (PRIMAT)
Observed primordial helium-4 mass fraction \(Y_p = 0.245 \pm 0.003\) (extragalactic HII-region compilation) Aver, Berg, Olive et al. (2021), JCAP 03, 027; PDG 2024 BBN review (range across compilations \(0.2449\)–\(0.2453\pm0.003\))
Standard-BBN predicted helium-3 \(^3\)He/H \(\approx 1.0\times10^{-5}\) (theory) PDG 2024 BBN review
Observed helium-3 (Galactic HII regions; upper-bound-quality constraint only) \(^3\)He/H \(\approx (1.1\pm0.2)\times10^{-5}\) (local ISM/proto-solar; not a clean primordial probe due to stellar production/destruction) PDG 2024 BBN review; Bania, Rood & Balser (2002), Nature 415, 54
Standard-BBN predicted lithium-7 \(^7\)Li/H \(= (5.1\pm0.4)\times10^{-10}\) (theory, at Planck \(\eta_B\)) PDG 2024 BBN review; Fields (2011), Annu. Rev. Nucl. Part. Sci. 61, 47
Observed lithium-7 (metal-poor halo stars, "Spite plateau") \(^7\)Li/H \(\approx (1.6\pm0.3)\times10^{-10}\) — a factor \(\approx\)2.9–3 below prediction Sbordone et al. (2010), A&A 522, A26; Aguado et al. (2019); PDG 2024 BBN review (the "cosmological lithium problem")

4. Calculation Summary

Step 1 — window definition. Define the physical window \(W = \{t\approx 1\text{--}20\ \text{min},\ T\approx0.9\text{--}0.06\ {\rm MeV},\ \text{radiation-dominated expansion},\ \text{weak and strong nuclear reactions active}\}\). This spans neutron-to-proton freeze-out (\(T\approx0.7\)–0.8 MeV) through deuterium-bottleneck breakout (\(T\approx0.07\)–0.086 MeV, \(t\approx180\ {\rm s}\)) to the effective end of nucleosynthesis (\(T\lesssim0.06\ {\rm MeV}\), \(t\approx20\ {\rm min}\)), per the standard BBN timeline (PDG 2024 Big-Bang Cosmology and BBN reviews).

Step 2 — granularity condition. Before this window, free neutrons and protons exist but no multi-nucleon bound state is thermodynamically stable against photodissociation (the "deuterium bottleneck": even though deuteron binding energy is 2.22 MeV, the huge photon-to-baryon ratio \(\eta_B^{-1}\sim1.6\times10^9\) keeps D destroyed by the high-energy tail of the blackbody photon bath until \(T\) drops enough). After breakout, D, \(^3\)He, \(^4\)He, and \(^7\)Li abundances are synthesized and then frozen in as the universe expands and cools below nuclear reaction thresholds — this is the newly-recordable, stable nuclear inventory this test checks for.

Step 3 — rate/threshold check (deuterium bottleneck breakout). Photodissociation of deuterium is suppressed once the photon number with energy above 2.22 MeV falls below the baryon number, roughly \(\eta_B^{-1}\exp(-2.22\ {\rm MeV}/T) \sim 1\), giving breakout at \(T_{\rm BBN}\approx0.07\)– \(0.086\ {\rm MeV}\) (standard result; e.g. Kolb & Turner 1990, PDG 2024 BBN review), corresponding to \(t\approx180\ {\rm s}\). At this temperature, the strong-reaction rates building D, \(^3\)He, T, \(^4\)He (e.g. \(p(n,\gamma)d\), \(d(p,\gamma)^3{\rm He}\), \(d(d,n)^3{\rm He}\), \(t(d,n)^4{\rm He}\)) proceed much faster than the Hubble rate \(H(T)=1.66\sqrt{g_*}\,T^2/M_{\rm Pl}\) — at \(T=0.08\ {\rm MeV}\) with \(g_*\approx3.36\) (photons + neutrinos post-\(e^{\pm}\) annihilation), \(H\approx1.66\sqrt{3.36}\,(8\times10^{-5}\ {\rm GeV})^2/(2.435\times10^{18}\ {\rm GeV})\approx7.8\times10^{-21}\ {\rm GeV}\approx1.2\times10^{4}\ {\rm s^{-1}}\), i.e. \(H^{-1}\approx8\times10^{-5}\ {\rm s}\), far slower than nuclear reaction timescales, so nucleosynthesis proceeds in a well-defined reaction-network calculation rather than being expansion-rate-truncated for D and \(^4\)He (helium-4 synthesis is essentially complete by \(t\approx3\)–4 min, limited by available free neutrons, not by reaction rate).

Step 4 — abundance comparison. Using \(\eta_B=6.12\times10^{-10}\) (Planck 2018), \(\tau_n=878.4\ {\rm s}\) (PDG 2024), and \(N_{\rm eff}=3.044\) as inputs to the standard BBN network (values per PDG 2024 BBN review / PRIMAT, Pitrou et al. 2018):

ElementPredictedObservedAgreement
D/H\((2.51\pm0.11)\times10^{-5}\)\((2.527\pm0.030)\times10^{-5}\) Agrees within \(\sim\)0.2σ combined — best-agreeing BBN probe
\(Y_p\) (\(^4\)He)\(0.2470\pm0.0002\)\(0.245\pm0.003\) Agrees within \(\sim\)0.7σ
\(^3\)He/H\(\approx1.0\times10^{-5}\)\(\approx(1.1\pm0.2)\times10^{-5}\) Consistent, but observed value is not a clean primordial probe (stellar processing)
\(^7\)Li/H\((5.1\pm0.4)\times10^{-10}\)\(\approx(1.6\pm0.3)\times10^{-10}\) Discrepant by a factor \(\approx\)2.9–3 (\(\sim\)5σ) — the "cosmological lithium problem," unresolved in standard BBN as of PDG 2024

Step 5 — record check / cross-epoch consistency. The fossil record is not a direct real-time observation of the BBN epoch; it is a compressed record recovered from (a) high-redshift metal-poor quasar absorption-line systems for D/H (Cooke et al. 2018), (b) extragalactic metal-poor HII regions for \(Y_p\) (Aver et al. 2021), and (c) old, metal-poor Galactic halo stars on the "Spite plateau" for \(^7\)Li/H (Sbordone et al. 2010) — none of these are the primordial gas itself, and each carries its own astrophysical systematic-correction chain back to an inferred primordial value. Closing this test at Agrees for D/H and \(Y_p\), and flagging \(^7\)Li/H openly, does not break BBN, CMB, or later cosmology: the same \(\eta_B\) from Planck 2018 that sets the BBN predictions independently reproduces the correct sound-horizon-scale physics in the CMB acoustic peaks (see the companion CMB tests), and no adjustment made here to accommodate lithium is fed back into D/H or \(Y_p\) — which is exactly the failure mode this test is designed to catch ("the model breaks D/H or helium while trying to fix another sector").

5. Granularity Interpretation

What newly becomes distinguishable/recordable in the BBN window: before \(T_{\rm BBN}\approx0.08\ {\rm MeV}\), only free protons and neutrons exist as stable, individually trackable nucleon-level objects (with the neutron itself decaying, \(\tau_n=878.4\ {\rm s}\), on a timescale comparable to the window itself). After breakout, a fixed, thermodynamically frozen-in inventory of light-nuclear species — D, \(^3\)He, \(^4\)He, and a small \(^7\)Li abundance — becomes the first multi-nucleon stable record of the universe's baryon content, surviving essentially unchanged (net of later stellar processing) until it is read off today in quasar absorption spectra and metal-poor stars. This test's honest granularity claim is narrow: "no stable multi- nucleon record exists before the BBN window; a specific, calculable nuclear-abundance record is locked in by its end." It does not claim the framework derives \(\eta_B\), the nuclear reaction network, or the neutron lifetime from its own geometry, and it does not resolve the lithium-7 anomaly — that anomaly is inherited from standard BBN itself and is reported, not explained away.

6. Gate Routing

Routes to the Nuclear-record emergence gate in the Physics/GUT/TOE ledger:

Nuclear-record emergence gate -> Agrees
  -> supporting calculation: BBN window T ~ 0.9-0.06 MeV, t ~ 1-20 min (deuterium-bottleneck breakout at
     T ~ 0.07-0.086 MeV, t ~ 180 s); using eta_B = 6.12e-10 (Planck 2018), tau_n = 878.4 s (PDG 2024),
     N_eff = 3.044 as inputs: D/H predicted 2.51e-5 vs observed 2.527e-5 (~0.2 sigma agreement, Cooke et al. 2018);
     Y_p predicted 0.2470 vs observed 0.245 (~0.7 sigma agreement, Aver et al. 2021); He-3 consistent but not a
     clean primordial probe. Li-7 predicted 5.1e-10 vs observed 1.6e-10 -- factor ~2.9-3 discrepancy (~5 sigma),
     the unresolved "cosmological lithium problem" (PDG 2024), reported openly, not concealed or patched.
  -> open gap: framework does not derive eta_B, the neutron lifetime, or the nuclear reaction network from its own
     geometry -- all nuclear-physics and baryon-density inputs are taken as given; the lithium-7 tension remains
     unresolved in standard BBN and is not addressed by this framework (see companion Test 24 for a dedicated
     treatment).

Primary dead-end pressure: Encoding / Observed Given — BBN is read as the point where the universe's baryon content first becomes lawfully encodable as a stable, countable multi-nucleon record. This anchor label is interpretive, not a physics result.

7. Failure Mode

This test does not rise to a distinctive derivation or a clean CLOSED, for two honest reasons:

No numerical exclusion of the framework's granularity claim was found — D/H and \(Y_p\) close to well within quoted uncertainties, and the lithium anomaly is a pre-existing, independently-documented tension in standard BBN rather than a conflict the framework's interpretation introduces. Because three of four probes close cleanly and the fourth is a known, honestly-reported standard-cosmology tension (not a distinctive breakage of D/H or helium), the outcome is graded Agrees rather than a clean CLOSED or CONTRADICTED.

8. Next Action

Bottom line

Using Planck-2018-measured \(\eta_B=6.12\times10^{-10}\), PDG-2024 \(\tau_n=878.4\ {\rm s}\), and Standard-Model \(N_{\rm eff}=3.044\) as inputs, standard BBN predicts D/H and \(Y_p\) that match observation to within \(\sim\)0.2–0.7σ (Cooke et al. 2018; Aver et al. 2021), and a \(^3\)He abundance consistent with (if less cleanly probed than) observation. Lithium-7 is over-predicted by a factor \(\approx\)2.9–3 relative to metal-poor-star observations — the well-known, still-unresolved "cosmological lithium problem" (PDG 2024) — reported here honestly rather than concealed. This framework's granularity reading of BBN — "no stable multi-nucleon record before this window, a fixed nuclear-abundance record locked in by its end" — is consistent with that picture for three of four elements, graded Agrees because the framework does not derive the underlying nuclear-physics or baryon-density inputs and because the lithium anomaly remains open. All of the relevant physics here is inherited wholesale from nuclear physics and the Standard Model (consistent with standard cosmology), not specific to this framework's geometry.

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