Lambda-CDM model

Physical cosmology

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Expanding universe Redshift · Hubble's law Metric expansion of space Friedmann equations FLRW metric
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Components Lambda-CDM model Dark energy · Dark matter Dark fluid · Dark flow
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Experiments Observational cosmology 2dF · SDSS COBE · BOOMERanG · WMAP · Planck
Scientists Isaac Newton · Einstein · Hawking · Friedman · Lemaître · Hubble · Penzias · Wilson · Gamow · Dicke · Zel'dovich · Mather · Rubin · Smoot · others

ΛCDM or Lambda-CDM is an abbreviation for Lambda-Cold Dark Matter, which is also known as the cold dark matter model with dark energy. It is frequently referred to as the standard model of big bang cosmology, since it attempts to explain:

the existence and structure of the cosmic microwave background
the large scale structure of galaxy clusters
the distribution of hydrogen, helium, deuterium and lithium
the accelerating expansion of the universe observed in the light from distant galaxies and supernovae

It is the simplest model that is in general agreement with observed phenomena; however, a significant minority of astrophysicists have challenged the validity of the model.^[1]

1 Overview
2 Parameters
3 Extended models
4 See also
5 References
6 External links

Overview

All modern cosmological models are based on the cosmological principle that our observational location in the universe is in no way unusual or special; on a large enough scale, the universe looks the same in all directions (isotropy) and from every location (homogeneity).^[2]

The model includes an expansion of metric space that is well documented both as the red shift of prominent spectral absorption or emission lines in the light from distant galaxies and as the time dilation in the light decay of supernova luminosity curves. Both effects are attributed to a Doppler shift in electromagnetic radiation as it travels across expanding space. Paradoxically, while this expansion increases the distance between objects that are not under shared gravitational influence, it does not increase the size of the objects in space. It also allows for distant galaxies to recede from each other at speeds greater than the speed of light.

The model assumes a "flat" spatial geometry, which means that the interior angles of a triangle defined by three beams of light will sum to 180°; space is defined by straight lines. (Alternative geometries include a spherical or "closed universe" in which the interior angles of a triangle would sum to more than 180°, and a hyperbolic or "open universe", in which the angles would sum to less than 180°.) The current values of key parameters imply that the universe is either flat or slightly open, the universe will expand forever, and the expansion is accelerating.

Λ (Lambda) stands for the cosmological constant which is currently associated with a vacuum energy or dark energy inherent in empty space that explains the current accelerating expansion of space against the attractive (collapsing) effects of gravity. The cosmological constant is denoted as $\Omega_{\Lambda}$ , which is interpreted as the fraction of the total mass-energy density of a flat universe that is attributed to dark energy. Currently, about 73% of the energy density of the present universe is estimated to be dark energy.

Cold dark matter is a form of matter necessary to account for gravitational effects observed in very large scale structures (anomalies in the rotation of galaxies, the gravitational lensing of light by galaxy clusters, enhanced clustering of galaxies) that cannot be accounted for by the quantity of observed matter. Dark matter is described as being cold (i.e. its velocity is non-relativistic [far below the speed of light] at the epoch of radiation-matter equality), possibly non-baryonic (consisting of matter other than protons and neutrons), dissipationless (cannot cool by radiating photons) and collisionless (i.e., the dark matter particles interact with each other and other particles only through gravity). This component is currently estimated to constitute about 23% of the mass-energy density of the universe.

The remaining 5% comprises all matter and energy observed as subatomic particles, chemical elements and electromagnetic radiation, the stuff of which visible planets, stars and galaxies are made.

The model includes a single originating event, the "Big Bang" or initial singularity, which was not an explosion but the abrupt appearance of expanding space-time containing radiation at temperatures of around 10¹⁵ K. This was immediately (within 10⁻²⁹ seconds) followed by an exponential expansion of space by a scale multiplier of 10²⁷ or more, known as cosmic inflation. The early universe remained hot (above 10,000 K) for several hundred thousand years, a state that is detectable as a residual cosmic microwave background or CMB, a very low energy radiation emanating from all parts of the sky. The "Big Bang" scenario, with cosmic inflation and standard particle physics, is the only current cosmological model consistent with the observed continuing expansion of space, the observed distribution of lighter elements in the universe (hydrogen, helium, and lithium), and the spatial texture of minute irregularities (anisotropies) in the CMB radiation. Cosmic inflation is also necessary to address the "horizon problem" in the CMB. Indeed, it seems likely that the universe is larger than the observable particle horizon.

The model uses the FLRW metric, the Friedmann equations and the cosmological equations of state to describe the observable universe from right after the inflationary epoch to present and future.

Historically, the dominant cosmological model previous to the now "standard model" was the Steady State theory, proposed independently in 1948 by H. Bondi & T. Gold and by Fred Hoyle. The universe in this model was flat, infinitely large, infinitely old (homogeneity and isotropy were extended in time as well as space) and was continuously creating matter to stabilize the mass-energy density of expanding space. There is currently active research into many aspects of the ΛCDM model, the details of which are very likely to change as new information becomes available. In particular, it is difficult to measure accurately the distance of very far galaxies or supernovae, so that distance related estimates (of stellar or galactic luminosities, or of key parameters such as the Hubble constant) are still uncertain. In addition, ΛCDM has no explicit physical theory for the origin or physical nature of dark matter or dark energy; the nearly scale-invariant spectrum of the CMB perturbations, and their image across the celestial sphere, are believed to result from very small thermal and acoustic irregularities at the point of recombination. The overwhelming majority of astronomers and astrophysicists support the ΛCDM model, but Milgrom, McGaugh, and Kroupa are leading critics.

Parameters

The ΛCDM model is based on six parameters: physical baryon density, physical dark matter density, dark energy density, scalar spectral index, curvature fluctuation amplitude and reionization optical depth. From these the other model values, including the Hubble constant and age of the universe, can be derived.

Parameter values listed below are from the Seven-Year Wilkinson Microwave Anisotropy Probe (WMAP) temperature and polarization observations.^[3] These include estimates based on data from Baryon Acoustic Oscillations^[4] and Type Ia supernova luminosity/time dilation measurements.^[5] Implications of the data for cosmological models are discussed in Komatsu et al. ^[6] and Spergel et al.^[7]

Parameter	Value	Description
t₀	$13.75\pm0.11 \times10^9$ years	Age of the universe
H₀	$70.4^{%2B1.3}_{-1.4}$ km s⁻¹ Mpc⁻¹	Hubble constant
Ω_bh²	$0.0260\pm0.00053$	Physical baryon density
Ω_ch²	$0.1123\pm0.0035$	Physical dark matter density
Ω_b	$0.0456\pm0.0016$	Baryon density
Ω_c	$0.227\pm0.014$	Dark matter density
Ω_Λ	$0.728^{%2B0.015}_{-0.016}$	Dark energy density
Δ_R²	$2.441^{%2B0.088}_{-0.092}\times10^{-9}$ , k₀ = 0.002Mpc⁻¹	Curvature fluctuation amplitude
σ₈	$0.809\pm0.024$	Fluctuation amplitude at 8h⁻¹Mpc
n_s	$0.963\pm0.012$	Scalar spectral index
z_*	$1090.89^{%2B0.68}_{-0.69}$	Redshift at decoupling
t_*	$377730^{%2B3205}_{-3200}$ years	Age at decoupling
τ	$0.087\pm0.014$	Reionization optical depth
z_reion	$10.4\pm1.2$	Redshift of reionization

The "physical baryon density" Ω_bh² differs from the "baryon density" Ω_b in that the baryon density gives the fraction of the critical density made up of baryons (the critical density is the total density of matter/energy needed for the universe to be spatially flat, with measurements indicating that the actual total density Ω_tot is very close if not equal to this value, see below), while the physical baryon density is equal to the baryon density multiplied by the square of the reduced Hubble constant h,^[8] where h is related to the Hubble constant H₀ by the equation H₀ = 100 h (km/s)/Mpc.^[9] Likewise for the difference between "physical dark matter density" and "dark matter density".

Extended models

Possible extensions of the simplest ΛCDM model are to allow quintessence rather than a cosmological constant. In this case, the equation of state of dark energy is allowed to differ from −1. Cosmic inflation predicts tensor fluctuations (gravitational waves). Their amplitude is parameterized by the tensor-to-scalar ratio, which is determined by the energy scale of inflation. Other modifications allow for spatial curvature (Ω_tot may be different from 1), hot dark matter in the form of neutrinos, or a running spectral index, which are generally viewed as inconsistent with cosmic inflation.

Allowing these parameters will generally increase the errors in the parameters quoted above, and may also shift the observed values somewhat.

Parameter	Value	Description
Ω_tot	$1.0023^{%2B0.0056}_{-0.0054}$	Total density
w	$-0.980\pm0.053$	Equation of state
r	$<0.24$ , k₀ = 0.002Mpc⁻¹ (2σ)	Tensor-to-scalar ratio
d n_s / d ln k	$-0.022\pm0.020$ , k₀ = 0.002Mpc⁻¹	Running of the spectral index
Ω_vh²	$< 0.0062$	Physical neutrino density
Σm_ν	$<0.58$ eV (2σ)	Neutrino mass

Some researchers have suggested that there is a running spectral index, but no statistically significant study has revealed one. Theoretical expectations suggest that the tensor-to-scalar ratio r should be between 0 and 0.3, and the latest results are now within those limits.

References

^ P. Kroupa, B. Famaey, K.S. de Boer, J. Dabringhausen, M. Pawlowski, C.M. Boily, H. Jerjen, D. Forbes, G. Hensler, M. Metz, "Local-Group tests of dark-matter concordance cosmology . Towards a new paradigm for structure formation", A&A 523, 32 (2010).
^ Andrew Liddle. An Introduction to Modern Cosmology (2nd ed.). London: Wiley, 2003.
^ Table 8 on p. 39 of Jarosik, N. et.al. (WMAP Collaboration). "Seven-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Sky Maps, Systematic Errors, and Basic Results" (PDF). nasa.gov. http://lambda.gsfc.nasa.gov/product/map/dr4/pub_papers/sevenyear/basic_results/wmap_7yr_basic_results.pdf. Retrieved 2010-12-04. (from NASA's WMAP Documents page)
^ Percival, W. J. et al. (2010). "Baryon Acoustic Oscillations in the Sloan Digital Sky Survey Data Release 7 Galaxy Sample". Monthly Notices of the Royal Astronomical Society 401 (4): 2148–2168. arXiv:0907.1660. Bibcode 2010MNRAS.401.2148P. doi:10.1111/j.1365-2966.2009.15812.x.
^ Riess, A. G. et.al.. "A Redetermination of the Hubble Constant with the Hubble Space Telescope from a Differential Distance Ladder" (PDF). hubblesite.org. http://hubblesite.org/pubinfo/pdf/2009/08/pdf.pdf. Retrieved 2010-12-04.
^ E. Komatsu et al. 2010 (WMAP Collaboration). Seven-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Cosmological Interpretation (from NASA's WMAP Documents page)
^ Spergel, D. N.; et al. (2003). "First‐YearWilkinson Microwave Anisotropy Probe(WMAP) Observations: Determination of Cosmological Parameters". The Astrophysical Journal Supplement Series 148: 175. arXiv:astro-ph/0302209. Bibcode 2003ApJS..148..175S. doi:10.1086/377226.
^ Appendix A of the LSST Science Book Version 2.0
^ p. 7 of Findings of the Joint Dark Energy Mission Figure of Merit Science Working Group

Rebolo, R.; et al. (2004). "Cosmological parameter estimation using Very Small Array data out to ℓ= 1500". Monthly Notices of the Royal Astronomical Society 353 (3): 747. arXiv:astro-ph/0402466. Bibcode 2004MNRAS.353..747R. doi:10.1111/j.1365-2966.2004.08102.x.
Ostriker, J. P.; Steinhardt, P. J. (1995). "Cosmic Concordance". arXiv:astro-ph/9505066 [astro-ph].

Lambda-CDM model

Contents

Overview

Parameters

Extended models

See also

References

External links