2003
DOI: 10.1098/rsta.2003.1288
|View full text |Cite
|
Sign up to set email alerts
|

Large–scale structure and matter in the Universe

Abstract: This paper summarizes the physical mechanisms that encode the type and quantity of cosmological matter in the properties of large-scale structure, and reviews the application of such tests to current datasets. The key lengths of the horizon size at matter-radiation equality and at last scattering determine the total matter density and its ratio to the relativistic density; acoustic oscillations can diagnose whether the matter is collisionless, and small-scale structure or its absence can limit the mass of any … Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
6
0

Year Published

2004
2004
2020
2020

Publication Types

Select...
6
2
1

Relationship

0
9

Authors

Journals

citations
Cited by 12 publications
(6 citation statements)
references
References 39 publications
0
6
0
Order By: Relevance
“…For instance, a hot dark matter (HDM) particle candidate with mass of a few to 15 eV would have a free-streaming length of about ∼ 100 Mpc, leading to too little power at the small-scale end of the matter power spectrum. The existence of galaxies at redshift z ∼ 6 implies that the coherence length should have been smaller than 100 kpc or so, meaning that even warm dark matter (WDM) particles with masses between 1 and 10 keV are close to being ruled out as well (see, e.g., [349]). ΛCDM thus presently remains the state-of-the-art in Cosmology, although some of the challenges listed below in Sect.…”
Section: Cold Dark Matter (Cdm)mentioning
confidence: 99%
“…For instance, a hot dark matter (HDM) particle candidate with mass of a few to 15 eV would have a free-streaming length of about ∼ 100 Mpc, leading to too little power at the small-scale end of the matter power spectrum. The existence of galaxies at redshift z ∼ 6 implies that the coherence length should have been smaller than 100 kpc or so, meaning that even warm dark matter (WDM) particles with masses between 1 and 10 keV are close to being ruled out as well (see, e.g., [349]). ΛCDM thus presently remains the state-of-the-art in Cosmology, although some of the challenges listed below in Sect.…”
Section: Cold Dark Matter (Cdm)mentioning
confidence: 99%
“…For lighter particle candidates, the damping scale becomes too large: for instance, a hot DM (HDM) particle candidate (m HDM ≈ few eV) would have a free-streaming length of ≈ 100 Mpc leading to too little power at the small-scale end of the matter power spectrum. The existence of galaxies at redshift z ≈ 6 implies that the coherence scale should have been smaller than 100 kpc or so, meaning that warm DM (WDM) particles with mass m WDM ≈ 1 − 10 keV are close to being ruled out (Peacock 2003).…”
Section: Introductionmentioning
confidence: 99%
“…Blind surveys for galaxies and galaxy clusters have been performed in the optical waveband for many years. The most recent galaxy redshift surveys (2dFGRS and SDSS) have yielded significant constraints on cosmological parameters via measurements of the power spectrum and redshift-space distortions, as well as a wealth of understanding of the properties of the individual galaxies (Peacock 2003;Tegmark et al 2004). If deep redshift surveys using H I could be performed they would open up a new window on the Universe which could have some technical advantages (and inevitably some disadvantages) over optical approaches.…”
Section: Introductionmentioning
confidence: 99%