Modern Physics · Advanced Topics

Cosmology

Cosmology is the study of the universe as a whole — its origin, structure, evolution, and ultimate fate. From the Big Bang to dark energy, from the cosmic microwave background to the large-scale structure, cosmology is one of the most precisely tested areas of physics.

PrerequisitesGeneralrelativity(Ch.GR)Statisticalmechanics(Ch.S)Nuclearphysics(Ch.NP)AGeneral relativity (Ch. GR) \cdot Statistical mechanics (Ch. S) \cdot Nuclear physics (Ch. NP) \cdot Astrophysics (Ch. AS)
Learning Goals
  • Write down the FLRW metric and derive the Friedmann equations from Einstein field equations.
  • ComputetheageoftheuniversebyintegratingtheFriedmannequationforaflat\LambdaCDMmodeCompute the age of the universe by integrating the Friedmann equation for a flat \LambdaCDM model.
  • Describe the sequence of cosmic epochs from inflation through BBN, recombination, and reionization.
  • Interpret CMB acoustic peaks to extract the curvature, baryon density, and matter density of the universe.
  • Quantify the Hubble tension and evaluate proposed resolutions including systematic errors and new physics.

CO.1 The Expanding Universe

Hubble (1929) discovered that galaxies recede with velocity v = H₀ d — the universe is expanding. In general relativity, the FLRW metric describes a homogeneous, isotropic universe:

ds2=c2dt2+a(t)2[dr2/(1kr2)+r2dΩ2](FLRWmetric)ds^{2} = -c^{2}dt^{2} + a(t)^{2}[dr^{2}/(1-kr^{2}) + r^{2}d\Omega^{2}] \qquad (FLRW metric)(CO.1)

where a(t) is the scale factor (a = 1 today) and k = −1, 0, +1 for open, flat, closed geometry. The Hubble parameter H(t) = ȧ/a; today H₀ ≈ 70 km/s/Mpc.

Redshift z relates the observed to emitted wavelength: 1 + z = a_obs/a_emit = 1/a(t_emit). Cosmological redshift is not a Doppler effect but the stretching of photon wavelengths by the expanding space.

CO.2 The Friedmann Equations

Substituting FLRW into Einstein's equations gives the Friedmann equations:

(a˙/a)2=H2=8\piGρtotal/(3)kc2/a2+\Lambdac2/3(Friedmannequation)(ȧ/a)^{2} = H^{2} = 8\piG \rho_total/(3) - kc^{2}/a^{2} + \Lambdac^{2}/3 \qquad (Friedmann equation)(CO.2)
a¨/a=4\piG(ρ+3P/c2)/3+\Lambdac2/3(Raychaudhuriequation)ä/a = -4\piG(\rho + 3P/c^{2})/3 + \Lambdac^{2}/3 \qquad (Raychaudhuri equation)(CO.3)

The cosmological constant Λ (dark energy) drives acceleration (ä > 0) when Λc²/3 > 4πG(ρ + 3P/c²). The critical density (k = 0, Λ = 0):

ρc=3H02/(8\piG)9.47×1027kg/m35.6protons/m3\rho_c = 3H_{0}^{2}/(8\piG) \approx 9.47\times10^{-27} kg/m^{3} \approx 5.6 protons/m^{3}(CO.4)

Density parameters: Ω_i = ρ_i/ρ_c. Current values (Planck 2018): Ω_m ≈ 0.315 (matter: 5% baryonic + 27% dark), Ω_Λ ≈ 0.685 (dark energy), k = 0 (flat).

Definition CO.1ΛCDM — The Standard Model of Cosmology
LambdaColdDarkMatter(\LambdaCDM):flatuniversewithcosmologicalconstantΛ(darkenergy,wLambda-Cold Dark Matter (\LambdaCDM): flat universe with cosmological constant \Lambda (dark energy, w = 1)andcolddarkmatter.Sixfreeparameters:H0,Ωbh2,Ωch2,As,ns,τ.FitsCMB-1) and cold dark matter. Six free parameters: H_{0}, \Omega_b h^{2}, \Omega_c h^{2}, A_{s}, n_{s}, \tau. Fits CMBAO,weaklensing,supernovaetoremarkableprecision.Tensions:Hubble(5σ),S8(matterflAO, weak lensing, supernovae to remarkable precision. Tensions: Hubble (5\sigma), S_{8} (matter fluctuationamplitude,23σ),possiblyhintingatextensions.Despiteitssuccess,\LambdaCDMtelluctuation amplitude, 2–3\sigma), possibly hinting at extensions. Despite its success, \LambdaCDM tells us nothing about what dark matter or dark energy actually are.

CO.3 Cosmic History

The universe cools as it expands: T ∝ 1/a ∝ (1+z). Key epochs:

t ∼ 10⁻³⁵ s: Inflation — exponential expansion driven by inflaton field. Solves the flatness, horizon, and monopole problems. Generates primordial perturbations with spectrum P(k) ∝ k^(n_s−1), n_s ≈ 0.965 (nearly scale-invariant, Planck 2018).

t ∼ 1 s – 3 min: Big Bang Nucleosynthesis (BBN) — T falls to ∼1 MeV. Free neutrons freeze out (n/p ≈ 1/7). Protons and neutrons fuse: p + n → d + γ, then ²H + ²H → ³He + n → ⁴He + γ. Final abundances: ⁴He: 25% by mass, ²H/H ≈ 2.5×10⁻⁵, ³He/H ≈ 10⁻⁵, ⁷Li/H ≈ 10⁻¹⁰. Predicted from one parameter (baryon-to-photon ratio η): match with observed primordial abundances is a triumph of Big Bang cosmology.

t ∼ 380,000 yr: Recombination — T ≈ 3000 K. Electrons and protons combine to form neutral hydrogen. Universe becomes transparent. Relic photons today: CMB at T₀ = 2.7255 K.

t ∼ 10⁸ yr: Reionization — first stars and quasars reionize the intergalactic medium. Absorption spectra of distant quasars show the Gunn-Peterson trough.

Example CO.1Age of the Universe in ΛCDM

GivenH0=67.4km/s/MpcandΩm=0.315,ΩΛ=0.685,computetheageoftheuniverseGiven H_{0} = 67.4 km/s/Mpc and \Omega_m = 0.315, \Omega_\Lambda = 0.685, compute the age of the universe.

Friedmann:H(a)=H0(Ωm/a3+ΩΛ).Theageist0=(0to1)da/(aH(aH(a) = H_{0} \sqrt(\Omega_m/a^{3} + \Omega_\Lambda). The age is t_{0} = \int(0 to 1) da/(a H(a.
Convert H₀:H0=67.4km/s/Mpc=67.4×103/(3.086×1022)=2.18×1018s1H_{0} = 67.4 km/s/Mpc = 67.4\times10^{3}/(3.086\times10^{22}) = 2.18\times10^{-18} s^{-1}.
Integral:Numerically:t0=(1/H0)(0to1)da/(0.315/a+0.685a2)(1/H0)×0.964=0.964/(2.18×Numerically: t_{0} = (1/H_{0}) \int(0 to 1) da/\sqrt(0.315/a + 0.685a^{2}) \approx (1/H_{0}) \times 0.964 = 0.964/(2.18\times1018)=4.42×1017s10^{-18}) = 4.42\times10^{17} s.
Convert:t0=4.42×1017/(3.156×107)=1.40×1010yr=13.8Gyrt_{0} = 4.42\times10^{17}/(3.156\times10^{7}) = 1.40\times10^{10} yr = 13.8 Gyr.
Check:Consistentwitholdestglobularclusters(13.5Gyr)andstellardating.Amatteronlyuniverse(Ωnt with oldest globular clusters (∼13.5 Gyr) and stellar dating. A matter-only universe (\OmegaΩΛ=0)givest0=2/(3H0)=9.3Gyrtooyoung!Darkenergyisneeded\Omega_\Lambda = 0) gives t_{0} = 2/(3H_{0}) = 9.3 Gyr — too young! Dark energy is needed.

CO.4 Cosmic Microwave Background

The CMB is a near-perfect blackbody at T₀ = 2.7255 K with tiny anisotropies δT/T ∼ 10⁻⁵. The angular power spectrum C_l (variance per multipole l) shows:

Acoustic peaks: the primordial plasma was a photon-baryon fluid. Pressure waves (sound) oscillated until recombination. Modes caught at maximum compression/rarefaction appear as peaks at l ≈ 200, 500, 800... The first peak location θ ∼ 1° determines the curvature: flat universe. The peak heights determine Ω_b (baryons) and Ω_m (total matter).

Damping tail(l > 1000): photon diffusion erases small-scale fluctuations (Silk damping). Exponential suppression ∝ e^(−(l/l_D)²).

Polarization: CMB is polarized (E and B modes). B-modes from primordial gravitational waves would confirm inflation — not yet detected.

CO.5 Dark Matter and Dark Energy

Dark matter evidence: galaxy rotation curves (flat, not Keplerian decline), galaxy cluster mass vs. temperature/lensing discrepancy, BBN (Ω_b = 0.049 ≪ Ω_m = 0.315), CMB peak heights, large-scale structure formation. Dark matter must be: cold (non-relativistic), non-baryonic, collisionless. Candidates: WIMPs (100 GeV−TeV scale), axions (μeV scale), sterile neutrinos, primordial black holes. No direct detection yet.

Dark energy: Ω_Λ = 0.685, equation of state w = P/(ρc²) ≈ −1 (consistent with Λ). The cosmological constant problem: why is Λ ≈ 10⁻¹²³ × (Planck scale)? The worst prediction in physics. Alternatives: quintessence (w(t) varies), phantom energy (w < −1, leads to Big Rip), modifications of gravity.

Definition CO.2Common Traps
  • Expansion is metric expansion: galaxies are not flying through pre-existing space from a central explosion.
  • Redshift has multiple causes: cosmological, Doppler, and gravitational shifts are conceptually distinct.
  • Critical density is a benchmark: it does not mean the universe is spatially small or large by itself.
  • Lookback time is not distance: cosmology has several useful distance measures.
Exercises — CO.1–CO.5 Cosmology
1.
CalculatetheCMBphotonnumberdensityatT0=2.7255K.WhatisthebaryontophotonratCalculate the CMB photon number density at T_{0} = 2.7255 K. What is the baryon-to-photon ratioηgivenΩb=0.049io \eta given \Omega_b = 0.049?
m⁻³
Straightforward
2.Explain how inflation solves the horizon problem, flatness problem, and monopole problem. What observational signatures of inflation have been confirmed?
Intermediate
3.Explain baryon acoustic oscillations (BAO) as a cosmological standard ruler. What is the BAO scale and how is it used to measure dark energy?
Intermediate
4.Describe the growth of structure from linear perturbation theory to N-body simulations. What determines the shape of the matter power spectrum P(k)?
Challenging
Key Takeaways
  • FLRWmetric:expandinguniversewithscalefactora(t).Redshiftz+1=1/a.HubbleH=a˙/aFLRW metric: expanding universe with scale factor a(t). Redshift z+1 = 1/a. Hubble H = ȧ/a.
  • Friedmann:H2=8\piGρ/3kc2/a2+\Lambdac2/3.Flat\LambdaCDM:Ωm+ΩΛ=1Friedmann: H^{2} = 8\piG\rho/3 - kc^{2}/a^{2} + \Lambdac^{2}/3. Flat \LambdaCDM: \Omega_m + \Omega_\Lambda = 1.
  • Cosmichistory:inflationBBN(4He,2H)recombinationreionizationstructureCosmic history: inflation \to BBN (^{4}He, ^{2}H) \to recombination \to reionization \to structure.
  • CMB:T=2.7255Kblackbody,\deltaT/T105.Acousticpeaksflatgeometry,Ωb,ΩmCMB: T = 2.7255 K blackbody, \deltaT/T ∼ 10^{-5}. Acoustic peaks \to flat geometry, \Omega_b, \Omega_m.
  • Dark matter (27%): cold, non-baryonic. Galaxy rotation curves, lensing, CMB peaks.
  • Darkenergy(68Dark energy (68%): w \approx -1. Drives accelerated expansion. Cosmological constant problem unsolved.