Symbols and notation
Every symbol on this page is used somewhere in the lessons. Each one has its meaning, how to say it, and links to the lessons that use it. Symbols are grouped by the year of the programme in which they first appear. The list is built from the lessons themselves, so it grows as the site grows.
The same letter often means different things in different courses: σ is a velocity spread in one lesson and a cross section in another. Where that happens, each meaning says where it applies. In a lesson, tap or click a symbol in a formula to see its meaning there; every lesson also lists its symbols near the end, under “Symbols on this page”. Under every formula, “In words” spells the whole formula out.
The Greek alphabet
Physics borrows Greek letters when it runs out of Latin ones. Here are all 24, with a guide to saying them (where two are given, both are common). Letters used on the site link to their entry below.
| Capital | Small | Name | Say it |
|---|---|---|---|
| Α | α | alpha | AL-fa |
| Β | β | beta | BAY-ta or BEE-ta |
| Γ | γ | gamma | GAM-a |
| Δ | δ | delta | DEL-ta |
| Ε | ε, ϵ | epsilon | EP-si-lon |
| Ζ | ζ | zeta | ZAY-ta or ZEE-ta |
| Η | η | eta | AY-ta or EE-ta |
| Θ | θ | theta | THAY-ta or THEE-ta |
| Ι | ι | iota | eye-OH-ta |
| Κ | κ | kappa | KAP-a |
| Λ | λ | lambda | LAM-da |
| Μ | μ | mu | MYOO |
| Ν | ν | nu | NEW |
| Ξ | ξ | xi | KSEE or ZYE |
| Ο | ο | omicron | OM-i-kron |
| Π | π | pi | PIE |
| Ρ | ρ | rho | ROW |
| Σ | σ | sigma | SIG-ma |
| Τ | τ | tau | TOW (rhymes with cow) |
| Υ | υ | upsilon | UP-si-lon |
| Φ | φ, ϕ | phi | FYE or FEE |
| Χ | χ | chi | KYE |
| Ψ | ψ | psi | SIGH or PSY |
| Ω | ω | omega | oh-MAY-ga or oh-MEE-ga |
Symbols that look alike
- ν and v
- ν is the Greek letter nu (a frequency, or a neutrino); v is the Latin letter v (a speed). Nu comes to a point at the bottom.
- ρ and p
- ρ (rho) is a density; p is a pressure. Both appear in ρ + 3p/c². Rho has a tail below the line.
- κ and k
- κ (kappa) and k (curvature) even appear together: for an open universe κ = −k.
- χ and x
- χ (chi) has a long stroke below the line; x does not.
- ω and w
- ω (omega) is rounded at the bottom; w is pointed.
- ξ and ζ
- ξ (xi) has three bumps stacked up; ζ (zeta) is a single curl.
- ϕ and φ; ε and ϵ
- Two ways of writing the same letter (phi; epsilon). They mean the same thing.
- ∝ and α
- ∝ means “is proportional to” and sits on the line like =; α is the letter alpha.
- ℓ, l and 1
- ℓ is a script l, used for lengths so that it is not mistaken for the number 1.
- ≈, ∼, ≃ and ∝
- ≈ and ≃: close in value. ∼: the same order of magnitude (within a factor of a few). ∝: the same shape, up to a constant factor.
- Δ and ∇
- Δ (capital delta) means “a change in”; ∇ (nabla, upside down) is the vector derivative “del”.
- d, ∂ and δ
- d: an ordinary derivative or small step (dx). ∂: a partial derivative, other variables held fixed. δ: a small variation, or the density contrast in 8.902.
- ħ and h
- ħ (h-bar) is Planck's constant divided by 2π.
First used in Year I · Mechanics, electromagnetism and calculus
Letters
H H
Say it: H
- In 8.286, 8.902: The Hubble parameter H = ȧ/a: the expansion rate of the universe at a given time.
- On Position and velocity in one dimension and Vectors: The Hubble parameter H = ȧ/a: the expansion rate of the universe.
Used in 29 lessons
- Position and velocity in one dimension (8.01)
- Vectors (8.01)
- The age of a closed universe from H and Ω (8.286)
- The age of the universe and the Big Bang singularity (8.286)
- The age of the universe with vacuum energy (8.286)
- The anthropic argument and the multiverse — and where the course begins (8.286)
- The cosmological constant and vacuum energy (8.286)
- The expanding sphere and the equation for a(t) (8.286)
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- The false vacuum and the mechanism of inflation (8.286)
- The flatness problem (8.286)
- The Friedmann equation (8.286)
- The homogeneous expanding universe (8.286)
- The horizon distance (8.286)
- The horizon problem (8.286)
- How inflation solves the problems of the Big Bang (8.286)
- How bright is a distant supernova? (8.286)
- Topological defects and the magnetic monopole problem (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- Neutrinos and counting particle species (8.286)
- Open, closed and flat universes (8.286)
- The open universe and the age of any matter universe (8.286)
- The radiation-dominated universe (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
- The supernova evidence for acceleration (8.286)
- The puzzle of the vacuum energy, and Einstein's mistake about Friedmann (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- How small ripples grow — linear perturbation theory (8.902)
- When ripples collapse — the spherical collapse model (8.902)
z z
Say it: z
- On Vectors: The z coordinate: the third axis, with x and y.
- On The Doppler effect and special relativity: Redshift: 1 + z = λ_O/λ_S, how much a wave's wavelength is stretched between source and observer (on this page by the source's motion).
- On The Higgs field and spontaneous symmetry breaking: A complex number, z = e^(iθ).
- On The spacetime metric of the universe, The spacetime interval, The metric of a sphere and of a closed universe and The geometry of open universes: A Cartesian coordinate, with x, y (and w on the 3-sphere).
- On Mass, energy and the dilution of radiation: Redshift, 1 + z = a(observed)/a(emitted); in Δz, a coordinate difference.
- In 8.286, 8.902: Redshift: 1 + z = a(observed)/a(emitted), how much the universe has stretched since the light left.
Used in 20 lessons
- Vectors (8.01)
- The age of the universe with vacuum energy (8.286)
- Cosmological redshift (8.286)
- The Doppler effect and special relativity (8.286)
- The Higgs field and spontaneous symmetry breaking (8.286)
- The horizon problem (8.286)
- How bright is a distant supernova? (8.286)
- Mass, energy and the dilution of radiation (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- The geometry of open universes (8.286)
- The spacetime metric of the universe (8.286)
- The spacetime interval (8.286)
- The metric of a sphere and of a closed universe (8.286)
- The supernova evidence for acceleration (8.286)
- The temperature of the early universe and decoupling (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- How many halos? — the Press–Schechter mass function (8.902)
- When ripples collapse — the spherical collapse model (8.902)
- Why structure formation needs cold dark matter (8.902)
G G
Say it: G
- Newton's gravitational constant, G ≈ 6.674 × 10⁻¹¹ m³ kg⁻¹ s⁻².
Used in 26 lessons
- The universal law of gravitation (8.01)
- The age of a closed universe from H and Ω (8.286)
- The age of the universe with vacuum energy (8.286)
- Black-body radiation (8.286)
- The closed universe as a cycloid (8.286)
- The cosmological constant and vacuum energy (8.286)
- Cosmological redshift (8.286)
- The expanding sphere and the equation for a(t) (8.286)
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- Falling into a black hole (8.286)
- The false vacuum and the mechanism of inflation (8.286)
- The flatness problem (8.286)
- The Friedmann equation (8.286)
- How inflation solves the problems of the Big Bang (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- Neutrinos and counting particle species (8.286)
- Why a static universe cannot work (8.286)
- Open, closed and flat universes (8.286)
- The radiation-dominated universe (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
- The temperature of the early universe and decoupling (8.286)
- The puzzle of the vacuum energy, and Einstein's mistake about Friedmann (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- How small ripples grow — linear perturbation theory (8.902)
- When ripples collapse — the spherical collapse model (8.902)
- Why structure formation needs cold dark matter (8.902)
k k
Say it: k
- On Vectors: With a hat, k̂ is the unit vector along the z axis.
- On The puzzle of the vacuum energy, and Einstein's mistake about Friedmann: A wavenumber; k_max is the largest one included (the cut-off).
- On Black-body radiation, The spectrum of the cosmic microwave background, Neutrinos and counting particle species, The temperature of the early universe and decoupling, Exponential expansion, de Sitter space and the inflationary scenario and Why structure formation needs cold dark matter: Boltzmann's constant, in kT (the typical thermal energy at temperature T); k ≈ 1.381 × 10⁻²³ J/K.
- On Simplifying the geodesic equation and The geodesic equation: An index running over the coordinates.
- On Eternal inflation, dark energy and the landscape: The half-life of the false vacuum, measured in doubling times.
- On Where dark matter comes from — freeze-out, hot and cold: Boltzmann's constant in kT; in P(k), the wavenumber.
- In 8.286: The curvature constant: k > 0 closed, k = 0 flat, k < 0 open (Guth's units: 1/notch²).
- In 8.902: The (comoving) wavenumber of a Fourier mode: waves of length 2π/k.
Used in 31 lessons
- Vectors (8.01)
- The age of a closed universe from H and Ω (8.286)
- The age of the universe with vacuum energy (8.286)
- Black-body radiation (8.286)
- Simplifying the geodesic equation (8.286)
- The closed universe as a cycloid (8.286)
- The spectrum of the cosmic microwave background (8.286)
- The cosmological constant and vacuum energy (8.286)
- Eternal inflation, dark energy and the landscape (8.286)
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- The flatness problem (8.286)
- The Friedmann equation (8.286)
- The geodesic equation (8.286)
- How inflation solves the problems of the Big Bang (8.286)
- How bright is a distant supernova? (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- Neutrinos and counting particle species (8.286)
- Non-Euclidean geometry (8.286)
- Open, closed and flat universes (8.286)
- The geometry of open universes (8.286)
- The open universe and the age of any matter universe (8.286)
- The radiation-dominated universe (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
- The spacetime metric of the universe (8.286)
- The temperature of the early universe and decoupling (8.286)
- The puzzle of the vacuum energy, and Einstein's mistake about Friedmann (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- How small ripples grow — linear perturbation theory (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- How many halos? — the Press–Schechter mass function (8.902)
- Why structure formation needs cold dark matter (8.902)
Greek letters
capital delta \Delta
Say it: capital delta
- On When ripples collapse — the spherical collapse model: Density of the sphere relative to the background, Δ = 1 + δ; Δ_V is the value for a virialised halo.
- A change or difference in a quantity, e.g. Δx = x₂ − x₁.
Used in 13 lessons
- Acceleration in one dimension (8.01)
- Newton's laws of motion (8.01)
- Position and velocity in one dimension (8.01)
- Black-body radiation (8.286)
- Cosmological redshift (8.286)
- The Doppler effect and special relativity (8.286)
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- The false vacuum and the mechanism of inflation (8.286)
- Mass, energy and the dilution of radiation (8.286)
- The spacetime interval (8.286)
- The supernova evidence for acceleration (8.286)
- How small ripples grow — linear perturbation theory (8.902)
- When ripples collapse — the spherical collapse model (8.902)
theta \theta
Say it: theta
(sounds like “thay-ta or thee-ta”)
- On The closed universe as a cycloid, The age of a closed universe from H and Ω and The open universe and the age of any matter universe: The parameter (development angle) of the parametric solution: it runs from 0 at the Big Bang.
- On The Higgs field and spontaneous symmetry breaking: A phase angle, as in e^(iθ).
- On Simplifying the geodesic equation, Falling into a black hole, How bright is a distant supernova?, The geometry of open universes, Curvature and expansion — the Robertson–Walker metric, The spacetime metric of the universe and The metric of a sphere and of a closed universe: Polar angle: measured from the north pole (0) to the south pole (π).
- An angle.
Used in 13 lessons
- Motion in two dimensions and projectiles (8.01)
- Vectors (8.01)
- The age of a closed universe from H and Ω (8.286)
- Simplifying the geodesic equation (8.286)
- The closed universe as a cycloid (8.286)
- Falling into a black hole (8.286)
- The Higgs field and spontaneous symmetry breaking (8.286)
- How bright is a distant supernova? (8.286)
- The geometry of open universes (8.286)
- The open universe and the age of any matter universe (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
- The spacetime metric of the universe (8.286)
- The metric of a sphere and of a closed universe (8.286)
rho \rho
Say it: rho
- Density: mass (or energy divided by c²) per unit volume. ρ_c is the critical density, ρ̄ the mean density.
Used in 30 lessons
- The universal law of gravitation (8.01)
- The age of a closed universe from H and Ω (8.286)
- The age of the universe with vacuum energy (8.286)
- The anthropic argument and the multiverse — and where the course begins (8.286)
- Black-body radiation (8.286)
- The closed universe as a cycloid (8.286)
- The spectrum of the cosmic microwave background (8.286)
- The cosmological constant and vacuum energy (8.286)
- The expanding sphere and the equation for a(t) (8.286)
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- The false vacuum and the mechanism of inflation (8.286)
- The flatness problem (8.286)
- The Friedmann equation (8.286)
- How inflation solves the problems of the Big Bang (8.286)
- Topological defects and the magnetic monopole problem (8.286)
- Mass, energy and the dilution of radiation (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- Neutrinos and counting particle species (8.286)
- Why a static universe cannot work (8.286)
- Open, closed and flat universes (8.286)
- The radiation-dominated universe (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
- The temperature of the early universe and decoupling (8.286)
- The puzzle of the vacuum energy, and Einstein's mistake about Friedmann (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- How small ripples grow — linear perturbation theory (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- How many halos? — the Press–Schechter mass function (8.902)
- When ripples collapse — the spherical collapse model (8.902)
- Why structure formation needs cold dark matter (8.902)
Named quantities (a letter with a subscript)
Hubble constant H_0
Say it: H nought
- The Hubble constant: today's value of H, about 67–73 km/s/Mpc.
Used in 13 lessons
- Position and velocity in one dimension (8.01)
- The age of the universe with vacuum energy (8.286)
- The cosmological constant and vacuum energy (8.286)
- The flatness problem (8.286)
- The horizon distance (8.286)
- The horizon problem (8.286)
- How bright is a distant supernova? (8.286)
- Topological defects and the magnetic monopole problem (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- Open, closed and flat universes (8.286)
- The supernova evidence for acceleration (8.286)
- The puzzle of the vacuum energy, and Einstein's mistake about Friedmann (8.286)
- When ripples collapse — the spherical collapse model (8.902)
comoving distance \ell_c
Say it: ell c
- A comoving distance: fixed as the universe expands, measured in coordinate units (Guth's notches).
Used in 4 lessons
Constants
pi \pi
Say it: pi
- The ratio of a circle's circumference to its diameter, π ≈ 3.14159.
Used in 34 lessons
- The universal law of gravitation (8.01)
- The age of a closed universe from H and Ω (8.286)
- The age of the universe with vacuum energy (8.286)
- Black-body radiation (8.286)
- The closed universe as a cycloid (8.286)
- The spectrum of the cosmic microwave background (8.286)
- The cosmological constant and vacuum energy (8.286)
- The expanding sphere and the equation for a(t) (8.286)
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- Falling into a black hole (8.286)
- The false vacuum and the mechanism of inflation (8.286)
- The flatness problem (8.286)
- The Friedmann equation (8.286)
- The Standard Model, gauge theories and grand unification (8.286)
- How inflation solves the problems of the Big Bang (8.286)
- How bright is a distant supernova? (8.286)
- Topological defects and the magnetic monopole problem (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- Neutrinos and counting particle species (8.286)
- Why a static universe cannot work (8.286)
- Open, closed and flat universes (8.286)
- The geometry of open universes (8.286)
- The radiation-dominated universe (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
- The metric of a sphere and of a closed universe (8.286)
- The supernova evidence for acceleration (8.286)
- The temperature of the early universe and decoupling (8.286)
- The puzzle of the vacuum energy, and Einstein's mistake about Friedmann (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- How small ripples grow — linear perturbation theory (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- How many halos? — the Press–Schechter mass function (8.902)
- When ripples collapse — the spherical collapse model (8.902)
- Why structure formation needs cold dark matter (8.902)
Other symbols
script l \ell
Say it: ell
- A length or distance; ℓ_p is a physical distance and ℓ_c a comoving one.
Used in 13 lessons
- Position and velocity in one dimension (8.01)
- Cosmological redshift (8.286)
- The Doppler effect and special relativity (8.286)
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- The homogeneous expanding universe (8.286)
- The horizon distance (8.286)
- The horizon problem (8.286)
- Topological defects and the magnetic monopole problem (8.286)
- The geometry of open universes (8.286)
- The radiation-dominated universe (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
- The puzzle of the vacuum energy, and Einstein's mistake about Friedmann (8.286)
- Why structure formation needs cold dark matter (8.902)
degree \circ
Say it: degrees
- Degrees of angle (as in 45°).
Used in 4 lessons
- Motion in two dimensions and projectiles (8.01)
- Newton's laws of motion (8.01)
- Vectors (8.01)
- Simplifying the geodesic equation (8.286)
Relations
approximately equal \approx
Say it: is approximately
- Is approximately equal to.
Used in 43 lessons
- Acceleration in one dimension (8.01)
- Motion in two dimensions and projectiles (8.01)
- The universal law of gravitation (8.01)
- Vectors (8.01)
- The age of a closed universe from H and Ω (8.286)
- The age of the universe and the Big Bang singularity (8.286)
- The age of the universe with vacuum energy (8.286)
- The anthropic argument and the multiverse — and where the course begins (8.286)
- Black-body radiation (8.286)
- Simplifying the geodesic equation (8.286)
- The closed universe as a cycloid (8.286)
- The spectrum of the cosmic microwave background (8.286)
- The cosmological constant and vacuum energy (8.286)
- Cosmological redshift (8.286)
- The Doppler effect and special relativity (8.286)
- Eternal inflation, dark energy and the landscape (8.286)
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- Falling into a black hole (8.286)
- The false vacuum and the mechanism of inflation (8.286)
- The flatness problem (8.286)
- The geodesic equation (8.286)
- The homogeneous expanding universe (8.286)
- The horizon problem (8.286)
- The Big Bang and its prequel — an overview of inflation (8.286)
- How bright is a distant supernova? (8.286)
- Topological defects and the magnetic monopole problem (8.286)
- Mass, energy and the dilution of radiation (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- Neutrinos and counting particle species (8.286)
- Why a static universe cannot work (8.286)
- Open, closed and flat universes (8.286)
- The geometry of open universes (8.286)
- The open universe and the age of any matter universe (8.286)
- The radiation-dominated universe (8.286)
- The metric of a sphere and of a closed universe (8.286)
- The temperature of the early universe and decoupling (8.286)
- The puzzle of the vacuum energy, and Einstein's mistake about Friedmann (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- How small ripples grow — linear perturbation theory (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- How many halos? — the Press–Schechter mass function (8.902)
- When ripples collapse — the spherical collapse model (8.902)
- Why structure formation needs cold dark matter (8.902)
proportional to \propto
Say it: is proportional to
- Is proportional to: doubling one doubles the other.
Used in 28 lessons
- The universal law of gravitation (8.01)
- The age of the universe and the Big Bang singularity (8.286)
- The age of the universe with vacuum energy (8.286)
- Black-body radiation (8.286)
- The closed universe as a cycloid (8.286)
- The cosmological constant and vacuum energy (8.286)
- Cosmological redshift (8.286)
- The expanding sphere and the equation for a(t) (8.286)
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- The flatness problem (8.286)
- The Friedmann equation (8.286)
- The horizon distance (8.286)
- How bright is a distant supernova? (8.286)
- Topological defects and the magnetic monopole problem (8.286)
- Mass, energy and the dilution of radiation (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- Neutrinos and counting particle species (8.286)
- Open, closed and flat universes (8.286)
- The radiation-dominated universe (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
- The supernova evidence for acceleration (8.286)
- The temperature of the early universe and decoupling (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- How small ripples grow — linear perturbation theory (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- How many halos? — the Press–Schechter mass function (8.902)
- When ripples collapse — the spherical collapse model (8.902)
- Why structure formation needs cold dark matter (8.902)
identical to \equiv
Say it: is defined as
- Is defined as (or is identically equal to).
Used in 16 lessons
- Newton's laws of motion (8.01)
- Position and velocity in one dimension (8.01)
- The age of the universe with vacuum energy (8.286)
- The closed universe as a cycloid (8.286)
- The Doppler effect and special relativity (8.286)
- The expanding sphere and the equation for a(t) (8.286)
- Falling into a black hole (8.286)
- The flatness problem (8.286)
- The Friedmann equation (8.286)
- The horizon problem (8.286)
- Mass, energy and the dilution of radiation (8.286)
- Open, closed and flat universes (8.286)
- The open universe and the age of any matter universe (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
- The spacetime interval (8.286)
- The metric of a sphere and of a closed universe (8.286)
not equal \neq, \ne
Say it: is not equal to
- Is not equal to.
Used in 4 lessons
arrow \to, \rightarrow
Say it: goes to
- Goes to (tends to), or becomes.
Used in 19 lessons
- Acceleration in one dimension (8.01)
- Position and velocity in one dimension (8.01)
- The age of a closed universe from H and Ω (8.286)
- The age of the universe with vacuum energy (8.286)
- The cosmological constant and vacuum energy (8.286)
- The Doppler effect and special relativity (8.286)
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- Falling into a black hole (8.286)
- The Standard Model, gauge theories and grand unification (8.286)
- The Higgs field and spontaneous symmetry breaking (8.286)
- The horizon distance (8.286)
- How bright is a distant supernova? (8.286)
- Neutrinos and counting particle species (8.286)
- Why a static universe cannot work (8.286)
- Open, closed and flat universes (8.286)
- The geometry of open universes (8.286)
- The open universe and the age of any matter universe (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
- How many halos? — the Press–Schechter mass function (8.902)
implies \Rightarrow, \Longrightarrow
Say it: which gives
- Implies: what follows is a consequence of what came before.
Used in 21 lessons
- The universal law of gravitation (8.01)
- The age of the universe and the Big Bang singularity (8.286)
- The age of the universe with vacuum energy (8.286)
- The cosmological constant and vacuum energy (8.286)
- The Doppler effect and special relativity (8.286)
- The false vacuum and the mechanism of inflation (8.286)
- The homogeneous expanding universe (8.286)
- How bright is a distant supernova? (8.286)
- Topological defects and the magnetic monopole problem (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- Why a static universe cannot work (8.286)
- Open, closed and flat universes (8.286)
- The radiation-dominated universe (8.286)
- The spacetime metric of the universe (8.286)
- The temperature of the early universe and decoupling (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- How small ripples grow — linear perturbation theory (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- How many halos? — the Press–Schechter mass function (8.902)
- When ripples collapse — the spherical collapse model (8.902)
- Why structure formation needs cold dark matter (8.902)
if and only if \Longleftrightarrow, \Leftrightarrow
Say it: is equivalent to
- If and only if: each statement implies the other.
Used in 3 lessons
- Vectors (8.01)
- Falling into a black hole (8.286)
- When ripples collapse — the spherical collapse model (8.902)
Operators and functions
times \times
Say it: times
- Times (multiplication). Between two vectors: the cross product.
Used in 37 lessons
- Motion in two dimensions and projectiles (8.01)
- The universal law of gravitation (8.01)
- The age of the universe and the Big Bang singularity (8.286)
- The age of the universe with vacuum energy (8.286)
- The anthropic argument and the multiverse — and where the course begins (8.286)
- Black-body radiation (8.286)
- The spectrum of the cosmic microwave background (8.286)
- The cosmological constant and vacuum energy (8.286)
- The Doppler effect and special relativity (8.286)
- The expanding sphere and the equation for a(t) (8.286)
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- Falling into a black hole (8.286)
- The flatness problem (8.286)
- The Friedmann equation (8.286)
- The Standard Model, gauge theories and grand unification (8.286)
- The Higgs field and spontaneous symmetry breaking (8.286)
- The homogeneous expanding universe (8.286)
- The horizon problem (8.286)
- The Big Bang and its prequel — an overview of inflation (8.286)
- How bright is a distant supernova? (8.286)
- Topological defects and the magnetic monopole problem (8.286)
- Mass, energy and the dilution of radiation (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- Neutrinos and counting particle species (8.286)
- Why a static universe cannot work (8.286)
- Open, closed and flat universes (8.286)
- The open universe and the age of any matter universe (8.286)
- The radiation-dominated universe (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
- The supernova evidence for acceleration (8.286)
- The temperature of the early universe and decoupling (8.286)
- The puzzle of the vacuum energy, and Einstein's mistake about Friedmann (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- How many halos? — the Press–Schechter mass function (8.902)
- When ripples collapse — the spherical collapse model (8.902)
- Why structure formation needs cold dark matter (8.902)
dot \cdot
Say it: times
- Times (multiplication). Between two vectors: the dot product.
Used in 17 lessons
- Acceleration in one dimension (8.01)
- Black-body radiation (8.286)
- Simplifying the geodesic equation (8.286)
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- The Friedmann equation (8.286)
- The geodesic equation (8.286)
- The Standard Model, gauge theories and grand unification (8.286)
- The horizon distance (8.286)
- Topological defects and the magnetic monopole problem (8.286)
- Mass, energy and the dilution of radiation (8.286)
- Neutrinos and counting particle species (8.286)
- Why a static universe cannot work (8.286)
- Open, closed and flat universes (8.286)
- The radiation-dominated universe (8.286)
- How small ripples grow — linear perturbation theory (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- When ripples collapse — the spherical collapse model (8.902)
sine \sin
Say it: sine
- Sine of an angle.
Used in 15 lessons
- Motion in two dimensions and projectiles (8.01)
- Position and velocity in one dimension (8.01)
- Vectors (8.01)
- The age of a closed universe from H and Ω (8.286)
- Simplifying the geodesic equation (8.286)
- The closed universe as a cycloid (8.286)
- Falling into a black hole (8.286)
- How bright is a distant supernova? (8.286)
- The geometry of open universes (8.286)
- The open universe and the age of any matter universe (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
- The spacetime metric of the universe (8.286)
- The metric of a sphere and of a closed universe (8.286)
- The supernova evidence for acceleration (8.286)
- When ripples collapse — the spherical collapse model (8.902)
cosine \cos
Say it: cos
- Cosine of an angle.
Used in 10 lessons
- Motion in two dimensions and projectiles (8.01)
- Position and velocity in one dimension (8.01)
- Vectors (8.01)
- The age of a closed universe from H and Ω (8.286)
- Simplifying the geodesic equation (8.286)
- The closed universe as a cycloid (8.286)
- How bright is a distant supernova? (8.286)
- The open universe and the age of any matter universe (8.286)
- The metric of a sphere and of a closed universe (8.286)
- When ripples collapse — the spherical collapse model (8.902)
tangent \tan
Say it: tan
- Tangent of an angle, sin/cos.
Used in 4 lessons
- Motion in two dimensions and projectiles (8.01)
- Vectors (8.01)
- The age of the universe with vacuum energy (8.286)
- Falling into a black hole (8.286)
natural logarithm \ln
Say it: log
- Natural logarithm (base e ≈ 2.718).
Calculus
integral \int
Say it: the integral of
- Integral: the sum of infinitely many small pieces, such as the area under a curve.
Used in 16 lessons
- Acceleration in one dimension (8.01)
- The age of the universe with vacuum energy (8.286)
- The closed universe as a cycloid (8.286)
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- Falling into a black hole (8.286)
- The geodesic equation (8.286)
- The horizon distance (8.286)
- How bright is a distant supernova? (8.286)
- Topological defects and the magnetic monopole problem (8.286)
- Why a static universe cannot work (8.286)
- The geometry of open universes (8.286)
- The radiation-dominated universe (8.286)
- The supernova evidence for acceleration (8.286)
- Measuring structure — the power spectrum and the correlation function (8.902)
- How many halos? — the Press–Schechter mass function (8.902)
- Why structure formation needs cold dark matter (8.902)
limit \lim
Say it: the limit
- Limit: the value approached as the variable written below approaches its target.
Used in 4 lessons
Accents (marks on a letter)
vector arrow \vec
Say it: vector
- A vector: a quantity with a size and a direction.
Used in 17 lessons
- Acceleration in one dimension (8.01)
- Motion in two dimensions and projectiles (8.01)
- Newton's laws of motion (8.01)
- Position and velocity in one dimension (8.01)
- The universal law of gravitation (8.01)
- Vectors (8.01)
- The expanding sphere and the equation for a(t) (8.286)
- The Standard Model, gauge theories and grand unification (8.286)
- The Higgs field and spontaneous symmetry breaking (8.286)
- Topological defects and the magnetic monopole problem (8.286)
- Mass, energy and the dilution of radiation (8.286)
- Why a static universe cannot work (8.286)
- The radiation-dominated universe (8.286)
- The puzzle of the vacuum energy, and Einstein's mistake about Friedmann (8.286)
- How small ripples grow — linear perturbation theory (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- How many halos? — the Press–Schechter mass function (8.902)
hat \hat
Say it: hat
- In 8.902: A Fourier-transformed quantity, such as δ̂(k) or Ŵ(k).
- A unit vector: a vector of length 1 that only gives a direction (î, r̂).
Used in 10 lessons
- Acceleration in one dimension (8.01)
- Motion in two dimensions and projectiles (8.01)
- Newton's laws of motion (8.01)
- Position and velocity in one dimension (8.01)
- The universal law of gravitation (8.01)
- Vectors (8.01)
- Why a static universe cannot work (8.286)
- How small ripples grow — linear perturbation theory (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- How many halos? — the Press–Schechter mass function (8.902)
dot \dot
Say it: dot
- Rate of change with time: ȧ = da/dt.
Used in 18 lessons
- Position and velocity in one dimension (8.01)
- The age of the universe and the Big Bang singularity (8.286)
- The age of the universe with vacuum energy (8.286)
- The closed universe as a cycloid (8.286)
- The cosmological constant and vacuum energy (8.286)
- The expanding sphere and the equation for a(t) (8.286)
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- The false vacuum and the mechanism of inflation (8.286)
- The Friedmann equation (8.286)
- The homogeneous expanding universe (8.286)
- How bright is a distant supernova? (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- Open, closed and flat universes (8.286)
- The radiation-dominated universe (8.286)
- The spacetime metric of the universe (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- How small ripples grow — linear perturbation theory (8.902)
- When ripples collapse — the spherical collapse model (8.902)
double dot \ddot
Say it: double dot
- Second rate of change with time: ä = d²a/dt².
Used in 10 lessons
- The universal law of gravitation (8.01)
- The age of the universe with vacuum energy (8.286)
- The cosmological constant and vacuum energy (8.286)
- The expanding sphere and the equation for a(t) (8.286)
- The false vacuum and the mechanism of inflation (8.286)
- The Friedmann equation (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- The radiation-dominated universe (8.286)
- How small ripples grow — linear perturbation theory (8.902)
- When ripples collapse — the spherical collapse model (8.902)
First used in Year IV · Cosmology
Letters
a a
Say it: a
- On Why a static universe cannot work: The scale factor a(t); in the integral limits a is just a number, and in d a⃗ (with an arrow) a small piece of surface area.
- On Non-Euclidean geometry: A constant that sets the length scale of the disk.
- On The spacetime interval: A label for an event (events a and b).
- In 8.286: The scale factor a(t): how much the universe has expanded. Physical distance = a × comoving distance (Guth's units: metres per notch).
- In 8.902: The scale factor a(t): how much the universe has expanded (a = 1 today, 1/(1 + z) in the past).
Used in 40 lessons
- The age of a closed universe from H and Ω (8.286)
- The age of the universe and the Big Bang singularity (8.286)
- The age of the universe with vacuum energy (8.286)
- Black-body radiation (8.286)
- Simplifying the geodesic equation (8.286)
- The closed universe as a cycloid (8.286)
- The cosmological constant and vacuum energy (8.286)
- Cosmological redshift (8.286)
- The Doppler effect and special relativity (8.286)
- The expanding sphere and the equation for a(t) (8.286)
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- The false vacuum and the mechanism of inflation (8.286)
- The flatness problem (8.286)
- The Friedmann equation (8.286)
- The homogeneous expanding universe (8.286)
- The horizon distance (8.286)
- The horizon problem (8.286)
- How inflation solves the problems of the Big Bang (8.286)
- How bright is a distant supernova? (8.286)
- Mass, energy and the dilution of radiation (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- Neutrinos and counting particle species (8.286)
- Why a static universe cannot work (8.286)
- Non-Euclidean geometry (8.286)
- Open, closed and flat universes (8.286)
- The geometry of open universes (8.286)
- The open universe and the age of any matter universe (8.286)
- The radiation-dominated universe (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
- The spacetime metric of the universe (8.286)
- The spacetime interval (8.286)
- The supernova evidence for acceleration (8.286)
- The temperature of the early universe and decoupling (8.286)
- The puzzle of the vacuum energy, and Einstein's mistake about Friedmann (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- How small ripples grow — linear perturbation theory (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- How many halos? — the Press–Schechter mass function (8.902)
- When ripples collapse — the spherical collapse model (8.902)
- Why structure formation needs cold dark matter (8.902)
c c
Say it: c
- On Measuring structure — the power spectrum and the correlation function: In r₀^cc the letters cc label cluster–cluster correlations; elsewhere c is the speed of light.
- On Open, closed and flat universes: The speed of light; c′ (with a prime) is a constant of integration.
- In 8.286, 8.902: The speed of light, c ≈ 2.998 × 10⁸ m/s.
Used in 38 lessons
- The age of a closed universe from H and Ω (8.286)
- The age of the universe with vacuum energy (8.286)
- Black-body radiation (8.286)
- Simplifying the geodesic equation (8.286)
- The closed universe as a cycloid (8.286)
- The spectrum of the cosmic microwave background (8.286)
- The cosmological constant and vacuum energy (8.286)
- Cosmological redshift (8.286)
- The Doppler effect and special relativity (8.286)
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- Falling into a black hole (8.286)
- The false vacuum and the mechanism of inflation (8.286)
- The flatness problem (8.286)
- The Friedmann equation (8.286)
- The Standard Model, gauge theories and grand unification (8.286)
- The Higgs field and spontaneous symmetry breaking (8.286)
- The homogeneous expanding universe (8.286)
- The horizon distance (8.286)
- The horizon problem (8.286)
- How inflation solves the problems of the Big Bang (8.286)
- How bright is a distant supernova? (8.286)
- Topological defects and the magnetic monopole problem (8.286)
- Mass, energy and the dilution of radiation (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- Neutrinos and counting particle species (8.286)
- Open, closed and flat universes (8.286)
- The open universe and the age of any matter universe (8.286)
- The radiation-dominated universe (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
- The spacetime metric of the universe (8.286)
- The spacetime interval (8.286)
- The supernova evidence for acceleration (8.286)
- The temperature of the early universe and decoupling (8.286)
- The puzzle of the vacuum energy, and Einstein's mistake about Friedmann (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- How small ripples grow — linear perturbation theory (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- Why structure formation needs cold dark matter (8.902)
T T
Say it: T
- On Measuring structure — the power spectrum and the correlation function: The transfer function T(k): how much each mode's growth was held back.
- On When ripples collapse — the spherical collapse model: Kinetic energy (virial theorem: 2T + V = 0).
- In 8.286, 8.902: Temperature, in kelvin.
Used in 12 lessons
- Black-body radiation (8.286)
- The spectrum of the cosmic microwave background (8.286)
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- The flatness problem (8.286)
- The horizon problem (8.286)
- Neutrinos and counting particle species (8.286)
- The radiation-dominated universe (8.286)
- The temperature of the early universe and decoupling (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- When ripples collapse — the spherical collapse model (8.902)
- Why structure formation needs cold dark matter (8.902)
Greek letters
alpha \alpha
Say it: alpha
- On The closed universe as a cycloid, The age of a closed universe from H and Ω and The open universe and the age of any matter universe: A length constant of the parametric (cycloid) solution, as in ct = α(θ − sin θ).
- On The geodesic equation: The small number that sizes a variation of the path; the geodesic condition is taken at α = 0.
- On Topological defects and the magnetic monopole problem: The fine-structure constant, about 1/137.
Used in 5 lessons
beta \beta
Say it: beta
(sounds like “bay-ta or bee-ta”)
- On The Doppler effect and special relativity and The spacetime interval: Speed as a fraction of the speed of light, β = v/c.
- On Simplifying the geodesic equation: Latitude of the two end points (in the plot).
Used in 3 lessons
- Simplifying the geodesic equation (8.286)
- The Doppler effect and special relativity (8.286)
- The spacetime interval (8.286)
gamma \gamma
Say it: gamma
- On The Doppler effect and special relativity, Mass, energy and the dilution of radiation and The spacetime interval: The Lorentz factor, γ = 1/√(1 − β²).
- On Black-body radiation, Matter–radiation equality and the pressure of light and Neutrinos and counting particle species: As a subscript: photons (u_γ, T_γ, n_γ).
- On Where dark matter comes from — freeze-out, hot and cold: A photon; 2γ means two photons.
- On Measuring structure — the power spectrum and the correlation function: The slope of the correlation function, ξ ∝ r^(−γ).
- On Why structure formation needs cold dark matter: The ratio of specific heats of a gas (adiabatic index).
Used in 9 lessons
- Black-body radiation (8.286)
- The Doppler effect and special relativity (8.286)
- Mass, energy and the dilution of radiation (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- Neutrinos and counting particle species (8.286)
- The spacetime interval (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- Why structure formation needs cold dark matter (8.902)
delta \delta
Say it: delta
- On Simplifying the geodesic equation: The Kronecker delta: δ^i_j is 1 when i = j and 0 otherwise.
- On Measuring structure — the power spectrum and the correlation function: The density contrast, δ = (ρ − ρ̄)/ρ̄; δ_D (with subscript D) is the Dirac delta.
- In 8.902: The density contrast, δ = (ρ − ρ̄)/ρ̄: how much denser than average a region is. δ_c is the critical value for collapse.
Used in 6 lessons
- Simplifying the geodesic equation (8.286)
- How small ripples grow — linear perturbation theory (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- How many halos? — the Press–Schechter mass function (8.902)
- When ripples collapse — the spherical collapse model (8.902)
- Why structure formation needs cold dark matter (8.902)
epsilon \varepsilon, \epsilon
Say it: epsilon
- A small starting time, later taken to zero.
Used in 1 lesson
- The horizon distance (8.286)
zeta \zeta
Say it: zeta
(sounds like “zay-ta or zee-ta”)
- The Riemann zeta function; ζ(3) ≈ 1.202.
Used in 1 lesson
- Black-body radiation (8.286)
kappa \kappa
Say it: kappa
- κ = −k, positive for an open universe.
Used in 1 lesson
lambda \lambda
Say it: lambda
- On Cosmological redshift, The Doppler effect and special relativity and The spectrum of the cosmic microwave background: Wavelength.
- On Simplifying the geodesic equation and The geodesic equation: The parameter along a path; in the spacetime formulas λ is also an index running over 0–3.
- On How small ripples grow — linear perturbation theory and Why structure formation needs cold dark matter: A length; λ_J is the Jeans length, above which perturbations grow.
- On Where dark matter comes from — freeze-out, hot and cold: The free-streaming length.
Used in 8 lessons
- Simplifying the geodesic equation (8.286)
- The spectrum of the cosmic microwave background (8.286)
- Cosmological redshift (8.286)
- The Doppler effect and special relativity (8.286)
- The geodesic equation (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- How small ripples grow — linear perturbation theory (8.902)
- Why structure formation needs cold dark matter (8.902)
capital lambda \Lambda
Say it: lambda
- On The age of the universe with vacuum energy, The cosmological constant and vacuum energy and The supernova evidence for acceleration: Einstein's cosmological constant; Ω_Λ is its share of the critical density.
- On The Standard Model, gauge theories and grand unification and The Higgs field and spontaneous symmetry breaking: The function in a gauge transformation.
mu \mu
Say it: mu
(sounds like “myoo”)
- On Simplifying the geodesic equation, Falling into a black hole, The Standard Model, gauge theories and grand unification, The Higgs field and spontaneous symmetry breaking and Mass, energy and the dilution of radiation: A spacetime index, running over 0 (time) and 1, 2, 3 (space).
- On Black-body radiation and Neutrinos and counting particle species: As a subscript: the muon (ν_μ, m_μ).
- On The spectrum of the cosmic microwave background: Micro-, one millionth: 1 μm = 10⁻⁶ m.
Used in 8 lessons
- Black-body radiation (8.286)
- Simplifying the geodesic equation (8.286)
- The spectrum of the cosmic microwave background (8.286)
- Falling into a black hole (8.286)
- The Standard Model, gauge theories and grand unification (8.286)
- The Higgs field and spontaneous symmetry breaking (8.286)
- Mass, energy and the dilution of radiation (8.286)
- Neutrinos and counting particle species (8.286)
nu \nu
Say it: nu
(sounds like “new”)
- On Black-body radiation: Frequency; with a subscript (ν_e, ν_μ, ν_τ) a neutrino.
- On The spectrum of the cosmic microwave background and Mass, energy and the dilution of radiation: Frequency.
- On Neutrinos and counting particle species and The Standard Model, gauge theories and grand unification: A neutrino (T_ν, g_ν); ν̄ is an antineutrino.
- On Simplifying the geodesic equation and Falling into a black hole: A spacetime index, running over 0–3.
- On How many halos? — the Press–Schechter mass function: Peak height, ν = δ_c/(σD): how rare a fluctuation is.
Used in 8 lessons
- Black-body radiation (8.286)
- Simplifying the geodesic equation (8.286)
- The spectrum of the cosmic microwave background (8.286)
- Falling into a black hole (8.286)
- The Standard Model, gauge theories and grand unification (8.286)
- Mass, energy and the dilution of radiation (8.286)
- Neutrinos and counting particle species (8.286)
- How many halos? — the Press–Schechter mass function (8.902)
xi \xi
Say it: xi
(sounds like “ksee or zye”)
- On Topological defects and the magnetic monopole problem: The correlation length of the Higgs field.
- On Measuring structure — the power spectrum and the correlation function: The two-point correlation function ξ(r): the excess chance of finding two galaxies a distance r apart.
- On When ripples collapse — the spherical collapse model: How much denser than the background the sphere is at turnaround, ξ = (3π/4)² ≈ 5.55.
sigma \sigma
Say it: sigma
- On Simplifying the geodesic equation: A spacetime index, running over 0–3.
- On How small ripples grow — linear perturbation theory and Why structure formation needs cold dark matter: The velocity dispersion of dark matter (the spread of particle speeds).
- On Measuring structure — the power spectrum and the correlation function and How many halos? — the Press–Schechter mass function: The rms density fluctuation; σ₈ is its value in spheres of radius 8 h⁻¹ Mpc.
- On Where dark matter comes from — freeze-out, hot and cold: The annihilation cross section; ⟨σv⟩ is its thermal average times speed.
Used in 6 lessons
- Simplifying the geodesic equation (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- How small ripples grow — linear perturbation theory (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- How many halos? — the Press–Schechter mass function (8.902)
- Why structure formation needs cold dark matter (8.902)
tau \tau
Say it: tau
(sounds like “rhymes with cow”)
- On Simplifying the geodesic equation, Falling into a black hole, The spacetime metric of the universe and The spacetime interval: Proper time: the time measured by a clock moving with the object.
- On Black-body radiation and Neutrinos and counting particle species: As a subscript: the tau lepton (ν_τ).
- On Where dark matter comes from — freeze-out, hot and cold and Why structure formation needs cold dark matter: A time scale, e.g. τ_H for expansion and τ_coll between collisions.
- On How small ripples grow — linear perturbation theory: The time scale of exponential growth in a static medium.
- On When ripples collapse — the spherical collapse model: Dimensionless time, τ = H_ta t.
Used in 10 lessons
- Black-body radiation (8.286)
- Simplifying the geodesic equation (8.286)
- Falling into a black hole (8.286)
- Neutrinos and counting particle species (8.286)
- The spacetime metric of the universe (8.286)
- The spacetime interval (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- How small ripples grow — linear perturbation theory (8.902)
- When ripples collapse — the spherical collapse model (8.902)
- Why structure formation needs cold dark matter (8.902)
phi \phi, \varphi
Say it: phi
(sounds like “fye”)
- On The metric of a sphere and of a closed universe, Simplifying the geodesic equation, Falling into a black hole, How bright is a distant supernova?, The geometry of open universes, Curvature and expansion — the Robertson–Walker metric and The spacetime metric of the universe: Azimuthal angle (longitude), running from 0 to 2π around the axis.
- On Why a static universe cannot work and How small ripples grow — linear perturbation theory: The gravitational potential: g = −∇φ.
- On The false vacuum and the mechanism of inflation: The value of a scalar field (such as the Higgs field or the inflaton).
- On The Standard Model, gauge theories and grand unification: A phase angle; in A_μ = (−φ, A) it is the electric potential.
- On The Higgs field and spontaneous symmetry breaking: The electric potential.
Used in 12 lessons
- Simplifying the geodesic equation (8.286)
- Falling into a black hole (8.286)
- The false vacuum and the mechanism of inflation (8.286)
- The Standard Model, gauge theories and grand unification (8.286)
- The Higgs field and spontaneous symmetry breaking (8.286)
- How bright is a distant supernova? (8.286)
- Why a static universe cannot work (8.286)
- The geometry of open universes (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
- The spacetime metric of the universe (8.286)
- The metric of a sphere and of a closed universe (8.286)
- How small ripples grow — linear perturbation theory (8.902)
chi \chi
Say it: chi
(sounds like “kye”)
- On Exponential expansion, de Sitter space and the inflationary scenario and How inflation solves the problems of the Big Bang: The rate of exponential expansion, χ = √(8πGρ_f/3).
- On The geometry of open universes: A real variable used when the angle ψ becomes imaginary, ψ = iχ.
Used in 3 lessons
psi \psi
Say it: psi
(sounds like “sigh”)
- On The metric of a sphere and of a closed universe, How bright is a distant supernova?, The geometry of open universes, Curvature and expansion — the Robertson–Walker metric and The supernova evidence for acceleration: The extra angle of the 3-sphere: how far round the closed universe a point is.
- On The Higgs field and spontaneous symmetry breaking: The electron (Dirac) field.
- On Where dark matter comes from — freeze-out, hot and cold: The rate at which particles are created, per unit volume.
Used in 7 lessons
- The Higgs field and spontaneous symmetry breaking (8.286)
- How bright is a distant supernova? (8.286)
- The geometry of open universes (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
- The metric of a sphere and of a closed universe (8.286)
- The supernova evidence for acceleration (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
omega \omega
Say it: omega
- On Black-body radiation, The Higgs field and spontaneous symmetry breaking and The puzzle of the vacuum energy, and Einstein's mistake about Friedmann: Angular frequency, ω = 2πν.
- On How small ripples grow — linear perturbation theory: The oscillation frequency of a perturbation mode in a static medium.
Used in 4 lessons
capital omega \Omega
Say it: omega
- The density parameter Ω = ρ/ρ_c. Subscripts pick one ingredient: Ω_m matter, Ω_vac (or Ω_Λ) vacuum energy, Ω_r radiation, Ω_k curvature.
Used in 17 lessons
- The age of a closed universe from H and Ω (8.286)
- The age of the universe with vacuum energy (8.286)
- The cosmological constant and vacuum energy (8.286)
- The flatness problem (8.286)
- The horizon problem (8.286)
- The Big Bang and its prequel — an overview of inflation (8.286)
- How inflation solves the problems of the Big Bang (8.286)
- How bright is a distant supernova? (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- Open, closed and flat universes (8.286)
- The open universe and the age of any matter universe (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
- The supernova evidence for acceleration (8.286)
- The temperature of the early universe and decoupling (8.286)
- The puzzle of the vacuum energy, and Einstein's mistake about Friedmann (8.286)
- How many halos? — the Press–Schechter mass function (8.902)
- When ripples collapse — the spherical collapse model (8.902)
capital gamma \Gamma
Say it: gamma
- A Christoffel symbol, Γ^i_jk, built from derivatives of the metric.
Used in 1 lesson
Named quantities (a letter with a subscript)
little h h_0
Say it: h nought
- H₀ in units of 100 km/s/Mpc: h₀ ≈ 0.67–0.7.
Used in 4 lessons
today t_0
Say it: t nought
- Today: the present time, about 13.8 billion years after the Big Bang in the real universe (simple models on some pages give other ages).
Used in 11 lessons
- The age of the universe with vacuum energy (8.286)
- The flatness problem (8.286)
- The horizon distance (8.286)
- The horizon problem (8.286)
- The Big Bang and its prequel — an overview of inflation (8.286)
- How bright is a distant supernova? (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- Open, closed and flat universes (8.286)
- The supernova evidence for acceleration (8.286)
- The temperature of the early universe and decoupling (8.286)
- When ripples collapse — the spherical collapse model (8.902)
temperature today T_0
Say it: T nought
- Today's temperature of the cosmic background radiation, 2.7255 K.
Used in 3 lessons
- Black-body radiation (8.286)
- The horizon problem (8.286)
- The temperature of the early universe and decoupling (8.286)
redshift of equality z_eq
Say it: z equality
- The redshift of matter–radiation equality, about 3400.
Used in 2 lessons
time of equality t_eq
Say it: t equality
- The time of matter–radiation equality, some 50 000–75 000 years after the Big Bang.
Used in 1 lesson
critical density \rho_c
Say it: rho c
- The critical density, 3H²/(8πG): the density of a flat universe (about 9 × 10⁻²⁷ kg/m³ today).
Used in 13 lessons
- The age of a closed universe from H and Ω (8.286)
- The age of the universe with vacuum energy (8.286)
- The anthropic argument and the multiverse — and where the course begins (8.286)
- The cosmological constant and vacuum energy (8.286)
- The flatness problem (8.286)
- Topological defects and the magnetic monopole problem (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- Open, closed and flat universes (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
- The puzzle of the vacuum energy, and Einstein's mistake about Friedmann (8.286)
- How many halos? — the Press–Schechter mass function (8.902)
- When ripples collapse — the spherical collapse model (8.902)
- Why structure formation needs cold dark matter (8.902)
matter density \rho_m
Say it: rho m
- On Topological defects and the magnetic monopole problem: Magnetic charge density (in ∇·B = 4πρ_m, Gaussian units) — not the matter density.
- The mass density of matter (dark matter and baryons).
Used in 6 lessons
- The age of the universe with vacuum energy (8.286)
- The cosmological constant and vacuum energy (8.286)
- Topological defects and the magnetic monopole problem (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- Measuring structure — the power spectrum and the correlation function (8.902)
- Why structure formation needs cold dark matter (8.902)
radiation density \rho_r
Say it: rho r
- The mass density of radiation (its energy density divided by c²).
Used in 3 lessons
vacuum density \rho_vac
Say it: rho vac
- The mass density of the vacuum energy (its energy density divided by c²); constant in time.
Used in 2 lessons
false-vacuum density \rho_f
Say it: rho f
- The mass density of the false vacuum during inflation; constant in time.
Used in 3 lessons
initial density \rho_i
Say it: rho i
- The density when a = 1, so that ρ = ρᵢ/a³ for matter.
Used in 3 lessons
normal density \rho_n
Say it: rho n
- The density of everything except the vacuum energy: ρₙ = ρ_m + ρ_r.
Used in 2 lessons
matter density parameter \Omega_m, \Omega_m,0
Say it: omega m
- The matter density as a fraction of the critical density, ρ_m/ρ_c; ',0' means today (about 0.3).
Used in 8 lessons
- The age of the universe with vacuum energy (8.286)
- The cosmological constant and vacuum energy (8.286)
- How bright is a distant supernova? (8.286)
- Matter–radiation equality and the pressure of light (8.286)
- The supernova evidence for acceleration (8.286)
- The temperature of the early universe and decoupling (8.286)
- How many halos? — the Press–Schechter mass function (8.902)
- When ripples collapse — the spherical collapse model (8.902)
vacuum density parameter \Omega_vac, \Omega_vac,0, \Omega_\Lambda
Say it: omega vac
- The vacuum-energy density as a fraction of the critical density; ',0' means today (about 0.7).
Used in 6 lessons
radiation density parameter \Omega_r, \Omega_rad,0
Say it: omega r
- The radiation density as a fraction of the critical density (about 9 × 10⁻⁵ today).
Used in 4 lessons
curvature density parameter \Omega_k,0, \Omega_k
Say it: omega k
- The curvature term written like a density parameter, −kc²/(a²H²); ',0' means today. Zero for a flat universe.
Used in 5 lessons
Omega today \Omega_0
Say it: omega nought
- Today's value of Ω, the total density as a fraction of the critical density.
Used in 1 lesson
- The flatness problem (8.286)
physical distance \ell_p
Say it: ell p
- A physical (proper) distance: what a ruler would measure at one moment, ℓ_p = a(t) ℓ_c.
Used in 4 lessons
- Cosmological redshift (8.286)
- The homogeneous expanding universe (8.286)
- The horizon problem (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
horizon distance \ell_p,horizon
Say it: ell horizon
- The horizon distance: how far light could have travelled since the Big Bang, as a physical distance.
Used in 2 lessons
- The horizon distance (8.286)
- The radiation-dominated universe (8.286)
Planck length \ell_P
Say it: ell P
- The Planck length, √(ħG/c³) ≈ 1.6 × 10⁻³⁵ m: where quantum gravity should matter.
Used in 1 lesson
spectral index n_s
Say it: n s
- The spectral index (tilt) of the primordial power spectrum, P ∝ kⁿ; measured n_s ≈ 0.965.
photon temperature T_\gamma
Say it: T gamma
- The temperature of the photons (the CMB).
Used in 1 lesson
neutrino temperature T_\nu
Say it: T nu
- The temperature of the neutrinos, (4/11)^(1/3) of the photon temperature after electron–positron annihilation.
Used in 1 lesson
photon energy density u_\gamma
Say it: u gamma
- The energy density of the photons, proportional to T⁴.
Used in 3 lessons
photon number density n_\gamma
Say it: n gamma
- The number of photons per unit volume, proportional to T³.
Used in 2 lessons
- Black-body radiation (8.286)
- Mass, energy and the dilution of radiation (8.286)
electron mass m_e
Say it: m e
- The electron mass; m_e c² ≈ 0.511 MeV.
Used in 3 lessons
luminosity distance d_L
Say it: d L
- The luminosity distance: the distance that would make the observed brightness obey the inverse-square law.
Used in 2 lessons
Schwarzschild radius r_s
Say it: r s
- The Schwarzschild radius, 2GM/c²: the horizon of a black hole.
Used in 1 lesson
- Falling into a black hole (8.286)
vacuum pressure p_vac
Say it: p vac
- The pressure of the vacuum energy, p_vac = −ρ_vac c²: negative.
Used in 2 lessons
vacuum expansion rate H_vac
Say it: H vac
- The expansion rate a universe dominated by vacuum energy settles to, √(8πGρ_vac/3).
Used in 2 lessons
maximum wavenumber k_max
Say it: k max
- The largest wavenumber included: a cut-off at the smallest length scale.
Constants
h-bar \hbar
Say it: h bar
- The reduced Planck constant, ħ = h/2π ≈ 1.055 × 10⁻³⁴ J·s.
Used in 9 lessons
- Black-body radiation (8.286)
- The spectrum of the cosmic microwave background (8.286)
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- Falling into a black hole (8.286)
- The Higgs field and spontaneous symmetry breaking (8.286)
- Neutrinos and counting particle species (8.286)
- The temperature of the early universe and decoupling (8.286)
- The puzzle of the vacuum energy, and Einstein's mistake about Friedmann (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
Other symbols
infinity \infty
Say it: infinity
- Infinity: larger than any number.
Used in 9 lessons
- The age of a closed universe from H and Ω (8.286)
- The age of the universe with vacuum energy (8.286)
- The cosmological constant and vacuum energy (8.286)
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- Falling into a black hole (8.286)
- The horizon problem (8.286)
- Why a static universe cannot work (8.286)
- Curvature and expansion — the Robertson–Walker metric (8.286)
- How many halos? — the Press–Schechter mass function (8.902)
Relations
tilde (similar) \sim
Say it: is of order
- Is of the order of: roughly equal, to within a factor of a few.
Used in 7 lessons
- Exponential expansion, de Sitter space and the inflationary scenario (8.286)
- The horizon problem (8.286)
- Topological defects and the magnetic monopole problem (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- When ripples collapse — the spherical collapse model (8.902)
- Why structure formation needs cold dark matter (8.902)
much less than \ll
Say it: is much less than
- Is much less than.
Used in 8 lessons
- The spectrum of the cosmic microwave background (8.286)
- Neutrinos and counting particle species (8.286)
- The metric of a sphere and of a closed universe (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- How many halos? — the Press–Schechter mass function (8.902)
- When ripples collapse — the spherical collapse model (8.902)
- Why structure formation needs cold dark matter (8.902)
much greater than \gg
Say it: is much greater than
- Is much greater than.
Used in 6 lessons
- Black-body radiation (8.286)
- Neutrinos and counting particle species (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- Measuring structure — the power spectrum and the correlation function (8.902)
- How many halos? — the Press–Schechter mass function (8.902)
- Why structure formation needs cold dark matter (8.902)
less than about \lesssim
Say it: is less than about
- Is less than, or roughly equal to.
Used in 5 lessons
greater than about \gtrsim
Say it: is greater than about
- Is greater than, or roughly equal to.
Used in 3 lessons
less than or equal \le, \leq
Say it: is less than or equal to
- Is less than or equal to.
Used in 6 lessons
- The closed universe as a cycloid (8.286)
- The flatness problem (8.286)
- The geodesic equation (8.286)
- The geometry of open universes (8.286)
- The spacetime metric of the universe (8.286)
- The metric of a sphere and of a closed universe (8.286)
element of \in
Say it: is in
- Is an element of (belongs to) a set.
Used in 2 lessons
Operators and functions
plus or minus \pm
Say it: plus or minus
- Plus or minus: both signs, or an uncertainty (67.3 ± 1.2).
Used in 12 lessons
- The age of a closed universe from H and Ω (8.286)
- The age of the universe and the Big Bang singularity (8.286)
- Black-body radiation (8.286)
- The spectrum of the cosmic microwave background (8.286)
- The flatness problem (8.286)
- The Friedmann equation (8.286)
- The Big Bang and its prequel — an overview of inflation (8.286)
- How inflation solves the problems of the Big Bang (8.286)
- Neutrinos and counting particle species (8.286)
- The open universe and the age of any matter universe (8.286)
- Measuring structure — the power spectrum and the correlation function (8.902)
- When ripples collapse — the spherical collapse model (8.902)
minus or plus \mp
Say it: minus or plus
- Minus or plus: the opposite sign to a ± in the same formula.
Used in 2 lessons
dagger \dagger
Say it: dagger
- Conjugate transpose of a matrix: transpose it and take complex conjugates (U†).
Used in 2 lessons
maximum \max
Say it: max
- Maximum: the largest value.
Used in 4 lessons
determinant \det
Say it: the determinant of
- Determinant of a matrix.
Used in 1 lesson
cotangent \cot
Say it: cot
- Cotangent of an angle, cos/sin.
Used in 1 lesson
arcsine \arcsin
Say it: arc sine
- Inverse sine: the angle whose sine is the given number.
Used in 2 lessons
arccosine \arccos
Say it: arc cos
- Inverse cosine: the angle whose cosine is the given number.
Used in 1 lesson
hyperbolic sine \sinh
Say it: sinh
(sounds like “shine or sinch”)
- Hyperbolic sine, (eˣ − e⁻ˣ)/2.
Used in 4 lessons
hyperbolic cosine \cosh
Say it: cosh
(sounds like “kosh”)
- Hyperbolic cosine, (eˣ + e⁻ˣ)/2.
Used in 2 lessons
hyperbolic tangent \tanh
Say it: tanh
(sounds like “tanch”)
- Hyperbolic tangent, sinh/cosh.
Used in 1 lesson
logarithm \log
Say it: log
- Logarithm; log₁₀ is the base-10 logarithm.
Used in 6 lessons
- The flatness problem (8.286)
- The Big Bang and its prequel — an overview of inflation (8.286)
- How inflation solves the problems of the Big Bang (8.286)
- The supernova evidence for acceleration (8.286)
- Where dark matter comes from — freeze-out, hot and cold (8.902)
- Why structure formation needs cold dark matter (8.902)
Calculus
partial \partial
Say it: partial
- Partial derivative: the rate of change with one variable, holding the others fixed.
Used in 8 lessons
- Simplifying the geodesic equation (8.286)
- Falling into a black hole (8.286)
- The geodesic equation (8.286)
- The Standard Model, gauge theories and grand unification (8.286)
- The puzzle of the vacuum energy, and Einstein's mistake about Friedmann (8.286)
- How small ripples grow — linear perturbation theory (8.902)
- How many halos? — the Press–Schechter mass function (8.902)
- Why structure formation needs cold dark matter (8.902)
nabla (del) \nabla
Say it: del
- Del: ∇f is the gradient, ∇·v the divergence, ∇×v the curl, ∇² the Laplacian.
Used in 4 lessons
loop integral \oint
Say it: the loop integral of
- An integral around a closed loop.
Used in 1 lesson
sum \sum
Say it: the sum of
- Sum: add up the terms over the range written below and above.
Used in 2 lessons
- Black-body radiation (8.286)
- The geodesic equation (8.286)
Accents (marks on a letter)
bar \bar, \overline
Say it: bar
- On The Standard Model, gauge theories and grand unification and Where dark matter comes from — freeze-out, hot and cold: An antiparticle (ν̄, x̄).
- A mean (average) value, such as ρ̄; in 8.902 also a smoothed field (δ̄).
Used in 5 lessons
tilde \tilde
Say it: tilde
- A modified version of a quantity (ã, k̃); its meaning is given where it is introduced.
Used in 7 lessons
- The age of a closed universe from H and Ω (8.286)
- The closed universe as a cycloid (8.286)
- The geodesic equation (8.286)
- How bright is a distant supernova? (8.286)
- The open universe and the age of any matter universe (8.286)
- The supernova evidence for acceleration (8.286)
- How small ripples grow — linear perturbation theory (8.902)
First used in Year V · Graduate year: astrophysics and general relativity
Named quantities (a letter with a subscript)
solar mass M_\odot
Say it: solar masses
- One solar mass, about 1.99 × 10³⁰ kg.
Used in 3 lessons
Jeans length \lambda_J
Say it: lambda J
- The Jeans length: perturbations larger than this grow under gravity, smaller ones oscillate.
Used in 2 lessons
Jeans mass M_J
Say it: M J
- The Jeans mass: the mass inside a sphere whose radius is the Jeans length, (4/3)πρ̄λ_J³.
Used in 2 lessons
speed of sound c_s
Say it: c s
- The speed of sound in the gas.
Used in 2 lessons
sound or dispersion speed v_s
Say it: v s
- The speed that resists collapse: the sound speed for baryons, the velocity dispersion for dark matter, c/√3 for radiation.
Used in 1 lesson
collapse threshold \delta_c
Say it: delta c
- The critical linear density contrast: a region has collapsed when linear theory gives it δ ≈ 1.69.
Used in 2 lessons
sigma eight \sigma_8
Say it: sigma 8
- The rms density fluctuation in spheres of radius 8 h⁻¹ Mpc: the standard measure of how clumpy matter is (about 0.8).
Used in 2 lessons
sigma R \sigma_R
Say it: sigma R
- The rms density fluctuation after smoothing over spheres of radius R(M).
Used in 1 lesson
Hubble time \tau_H
Say it: tau H
- The expansion time scale, 1/H.
Used in 1 lesson
collision time \tau_coll
Say it: tau collision
- The mean time between annihilations, 1/(n_eq⟨σv⟩).
Used in 1 lesson
equilibrium density n_eq, n_c,eq
Say it: n equilibrium
- The number density in thermal equilibrium (n_c,eq: the same, comoving).
Used in 1 lesson
Constants
Sun symbol \odot
Say it: solar
- The Sun: M_⊙ is one solar mass, about 1.99 × 10³⁰ kg.
Used in 3 lessons
Relations
congruent \cong
Say it: is approximately
- Is approximately equal to (written ≅ in the source).
Used in 1 lesson
greater than or equal \ge, \geq
Say it: is greater than or equal to
- Is greater than or equal to.
Used in 1 lesson
equilibrium arrows \rightleftharpoons
Say it: goes both ways to
- A reaction that runs in both directions (equilibrium).
Used in 1 lesson
Operators and functions
angle brackets \langle, \rangle
Say it: the average of
- The average (mean value) of what is inside, ⟨…⟩.