| Star Formation in Giant Molecular Clouds | How do cold interstellar gas clouds collapse and fragment into newborn stars? | M_BE = 1.18 c_s⁴ / √(G³ P_ext) ≈ 1.0 M_☉ (T / 10 K)^{3/2} (n_{H2} / 10^4 cm^{−3})^{−1/2}; dN / dM ∝ M^{−2.35} | Strong Observational Evidence |
| Main-Sequence Evolution & the Faint Young Sun | How does a star change during its main-sequence lifetime while fusing hydrogen into helium? | 1 / μ ≈ 2 X + (3/4) Y + (1/2) Z; τ_MS ≈ 10^{10} yr × (M / M_☉) / (L / L_☉) ≈ 10^{10} yr × (M / M_☉)^{−2.5} | Strong Observational Evidence |
| Red Giants, Helium Flash & AGB Evolution | Why does a star swell to 100 times its radius and cool at its surface when its core contracts? | (M_ic / M_★)_SC ≈ 0.37 (μ_env / μ_core)² ≈ 0.08; L_RGB ∝ M_core^7 (Paczyński AGB relation: L_AGB ≈ 59,250 (M_c/M_☉ − 0.52) L_☉) | Strong Observational Evidence |
| Core Collapse, Neutrino Heating & Stellar Death | Why does iron accumulation doom a massive star to catastrophic core collapse in less than a second? | ⁵⁶Fe + γ (≳ 2 MeV) → 13 ⁴He + 4 n − 124.4 MeV; p + e⁻ → n + ν_e; v_infall ≈ 0.23 c | Widely Accepted Model |
| Protoplanetary Disks & Planet Formation | How do microscopic dust grains in a circumstellar disk grow by 14 orders of magnitude into planets? | Δv_gas ≈ (1/2) (c_s / v_K)² v_K ≈ 50 m/s; R_Hill = a (M_proto / (3 M_★))^{1/3} | Widely Accepted Model |
| Planetary Migration, Resonances & Hot Jupiters | How do gas giants end up in 3-day 'hot Jupiter' orbits when they must form beyond the icy snow line? | P_{i+1} / P_i ≈ (p + q) / p; L_z = √(1 − e²) cos i ≈ const (Kozai-Lidov oscillation for i_0 > 39.2°) | Widely Accepted Model |
| Galaxy Formation, Cold Streams & Mergers | How do galaxies form inside dark matter halos and evolve from star-forming disks to quiescent ellipticals? | T_vir = (μ m_p G M_vir) / (2 k_B R_vir) ≈ 3.6 × 10^5 K × (v_circ / 100 km/s)²; t_cool = (3 n k_B T) / (2 n_e n_H Λ(T, Z)) < t_dyn | Widely Accepted Model |
| Galactic Archaeology & Stellar Populations | How do astronomers use stellar chemistry and orbits as fossils to reconstruct our galaxy's past? | [Fe/H] = log_10(N_Fe / N_H)_★ − log_10(N_Fe / N_H)_☉; [α/Fe] = log_10(N_α / N_Fe)_★ − log_10(N_α / N_Fe)_☉ | Strong Observational Evidence |
| Supermassive Black Hole Seeds & Co-Evolution | How did supermassive black holes grow to a billion solar masses less than 700 million years after the Big Bang? | M(t) = M_seed exp(t / t_Sal), t_Sal = [η / (1 − η)] (c σ_T) / (4π G m_p) ≈ 45 Myr (at η = 0.1); M_BH ∝ σ_bulge^{4.4} | Active Research Frontier |
| Stellar & Supernova Nucleosynthesis (B²FH) | Which astrophysical processes forged each element of the periodic table after the Big Bang? | ⁴He + ⁴He ⇌ ⁸Be, ⁸Be + ⁴He → ¹²C* (7.65 MeV) → ¹²C + 2γ; s-process: τ_n ≫ τ_β vs. r-process: τ_n ≪ τ_β | Strong Observational Evidence |
| The r-Process, Kilonovae & Neutron Star Mergers | How do neutron star mergers and kilonovae forge the heaviest elements in the universe like gold and uranium? | Y_e = n_p / (n_p + n_n) ≲ 0.25 (for 3rd-peak Au/Pt/U); t_peak ∝ (κ_lanth M_ej / v_ej)^{1/2} | Strong Observational Evidence |
| Cosmic Dawn, First Stars & Reionization | How did the first stars and galaxies end the Cosmic Dark Ages and reionize the universe? | M_J(Pop III, T≈200 K) ≈ 100× M_J(Pop I, T≈10 K); dQ_{H II} / dt = ṅ_ion / n̄_H − Q_{H II} / t_rec | Active Research Frontier |