principle

cosmological homogeneity

The assumption that the universe is statistically uniform on large scales, tested observationally.
37 related articles · 4 formulas

Description

Cosmological homogeneity is the assumption that the universe, when viewed on sufficiently large scales, is statistically uniform: every region looks roughly the same in terms of matter density, galaxy distribution, and other properties. This principle, combined with isotropy (the universe looks the same in every direction), forms the cosmological principle, which is a foundational assumption of the standard model of cosmology. It allows cosmologists to describe the universe with simple, uniform solutions to Einstein's equations, such as the Friedmann-Lemaître-Robertson-Walker metric, which underpins our understanding of the expanding universe and the Big Bang.

History

The cosmological principle was articulated in its modern form by Albert Einstein in 1917, when he applied his general theory of relativity to the universe as a whole, assuming a homogeneous and isotropic model. The observational confirmation of homogeneity came much later, with the discovery of the cosmic microwave background in 1965 and subsequent large-scale galaxy surveys.

How it works

Homogeneity is not an exact property but a statistical one: on scales of hundreds of millions of light-years, the distribution of galaxies and matter becomes smooth, with fluctuations averaging out. This is tested by mapping the large-scale structure of the universe, for example through galaxy surveys or measurements of the cosmic microwave background. The observed near-uniformity of the cosmic microwave background radiation, with temperature variations of only one part in 100,000, is strong evidence for homogeneity on the largest scales. However, the assumption is not universally accepted, and some studies explore whether significant inhomogeneities could affect cosmological observations, such as the apparent acceleration of the universe's expansion.

In practice

Homogeneity is used to simplify cosmological models, enabling predictions of the universe's evolution, the formation of large-scale structure, and the interpretation of dark energy and dark matter observations.

Fun fact

The largest known structure in the universe, the Hercules-Corona Borealis Great Wall, spans about 10 billion light-years, yet even it is still smaller than the scale at which the universe becomes homogeneous.

Concept graph →

Formulas

$$K_i(C_r^*(G)) igoplus_{j e 0} H_{2j+i}(G)$$
Relates K-theory of group C*-algebras to group homology.
What is in the formula
ivariableindex for K-theory group (0 or 1) — index
jvariablehomology degree index — index
\bigoplusoperatorcombines multiple abelian groups into one — direct sum
k_i(c_r^*(g))\cong\bigoplus_{j\ge0}h_{2j+i}(g) · 2607.00577
$$\Omega_M + \Omega_\Lambda + \Omega_k = 1$$
The sum of all density parameters equals one in cosmology.
What is in the formula
Ω_MvariableMatter density parameter (including baryonic and dark matter) — density parameter
Ω_ΛvariableCosmological constant (dark energy) density parameter — density parameter
Ω_kvariableCurvature density parameter — density parameter
ω_m^{\mathcal{d}}+ω_\lambda^{\mathcal{d}}+ω_r^{\mathcal{d}}+ω_q^{\mathcal{d}}=1 · 2605.05454v1
$$H(f) = \mathbb{E}[I(Y > \tilde{Y}) I(f(X) > f(\tilde{X}))]$$
Probability that predicted and observed orders agree.
What is in the formula
Hvariableconcordance probability — concordance probability
fvariablescoring function — function
Yvariableobserved response — response variable
Xvariableinput features — feature vector
Ỹvariableindependent copy of observed response — response variable
X̃variableindependent copy of input features — feature vector
Eoperatoraverages over the random variables — expectation operator
Ioperatorreturns 1 if condition true, 0 otherwise — indicator function
h(f_t)=\mathbb{e}_{x,\tilde{x},y,\tilde{y}}[i(y>\tilde{y})i(f_t(x)>f_t(\tilde{x}))] · 2607.00995
$$a(n) = \frac{1}{n!} \sum_{\pi \in S_n} \mathrm{fix}(\pi)$$
The number of unlabeled objects equals the average fixed points over permutations.
What is in the formula
a(n)variableNumber of unlabeled objects — count
nvariableSize parameter (e.g., number of elements) — count
πvariablePermutation in symmetric group — permutation
fix(π)variableNumber of fixed points of permutation π — count
∑operatorSum over all permutations — summation
1/n!operatorAverage over the group — average
a(n)=\frac{1}{n!}\sum_{π\ins_n}{fix}(π) · 2607.02613

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