Cosmology: Origin, ΛCDM & Cosmic Tensions

Big Bang cosmology, the CMB, ΛCDM parameters, the Hubble tension, dark matter, dark energy, inflation, and BBN.

Modern physical cosmology tests general relativity and particle physics across 13.8 billion years of cosmic expansion. Using the Cosmic Microwave Background, Big Bang Nucleosynthesis, Baryon Acoustic Oscillations, weak gravitational lensing, and standard candles, cosmologists constrain the six-parameter flat ΛCDM model—and probe where it may be cracking.

Every cosmology article separates model-independent observables from ΛCDM parameter fits and labels active tensions (H₀ and S₈) and open frontier questions with transparent epistemic badges.

Topics & Explainers in Cosmology (12)

Quantitative Overview & Epistemic Status

ArticleCore Question / MechanismGoverning RelationEpistemic Status
Big Bang Cosmology & The ΛCDM ModelWhat is the standard ΛCDM Big Bang model and what are its six foundational parameters?H²(z) = H₀² [ Ω_r (1 + z)⁴ + Ω_m (1 + z)³ + Ω_Λ ]Widely Accepted Model
The Cosmic Microwave Background (CMB)What is the Cosmic Microwave Background and what do its acoustic peaks measure?T_CMB(z) = T₀ (1 + z) ; θ_* = r_s(z_*) / D_M(z_*) = 0.010411 rad (0.596°)Strong Observational Evidence
Hubble Parameter H(z) & Expansion HistoryHow does the Hubble parameter H(z) change over cosmic time?E(z) ≡ H(z) / H₀ = √[ Ω_m (1 + z)³ + Ω_Λ ] ; q(z) = Ω_m(z)/2 − Ω_Λ(z)Strong Observational Evidence
The Hubble Tension in Modern CosmologyWhat is the Hubble tension and why do early- and late-universe measurements of H₀ disagree?T_σ = |H₀,local − H₀,CMB| / √(σ_local² + σ_CMB²) ≈ |73.04 − 67.36| / √(1.04² + 0.54²) ≈ 4.9σCompeting Interpretations
Dark Matter: Evidence & Particle CandidatesWhat is the astrophysical evidence for dark matter and what are the leading particle candidates?M(<r) = r v_circ² / G ; ρ_NFW(r) = ρ_0 / [ (r/r_s)(1 + r/r_s)² ]Widely Accepted Model
Dark Energy & Cosmic AccelerationWhat is dark energy and why does it cause the expansion of the universe to accelerate?(d²a / dt²) / a = −(4πG / 3) · ρ_total (1 + 3w) ; ρ_DE(z) = ρ_DE,0 (1 + z)^(3(1 + w))Active Research Frontier
Cosmic Inflation & The Horizon ProblemWhat is cosmic inflation and how does it explain the horizon problem and primordial fluctuations?N_e = ln(a_end / a_init) = ∫ H dt ≥ 60 ; P_ℛ(k) = A_s (k / k_* )^(n_s − 1)Widely Accepted Model
Recombination & Surface of Last ScatteringHow did recombination turn the opaque early universe transparent at 380,000 years?[x_e² / (1 − x_e)] = (1 / n_H) (m_e k_B T / 2πℏ²)^(3/2) e^(−E_I / k_B T) ; dτ = n_e σ_T c dtStrong Observational Evidence
Big Bang Nucleosynthesis (BBN)How did Big Bang Nucleosynthesis forge the lightest elements in the first three minutes?Y_p = 2(n / p)_fusion / [ 1 + (n / p)_fusion ] ≈ 0.247Strong Observational Evidence
Baryon Acoustic Oscillations (BAO)What are Baryon Acoustic Oscillations and how do they act as a cosmic standard ruler?r_d = ∫_(z_d)^∞ [ c_s(z) / H(z) ] dz ≈ 147.09 ± 0.26 Mpc ; Δθ_BAO = r_d / D_M(z)Strong Observational Evidence
Baryogenesis & Matter-Antimatter AsymmetryWhy is the observable universe made of matter instead of equal amounts of matter and antimatter?η = (n_B − n_B̄) / n_γ = 2.74 × 10⁻⁸ Ω_b h² = (6.12 ± 0.04) × 10⁻¹⁰Active Research Frontier
The Ultimate Fate of the UniverseHow will the universe end according to modern cosmological observations?a(t) ∝ exp(H₀ √Ω_Λ · t) [for w = −1] ; t_rip − t₀ ≈ (2 / 3|1 + w|) · H₀⁻¹ / √Ω_DE [for w < −1]Active Research Frontier

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