Lyman-alpha constraints on warm and on warm-plus-cold dark matter models
By Alexey Boyarsky, Julien Lesgourgues, Oleg Ruchayskiy, M. Viel. 2008
384 citations recorded by the source corpus.
We revisit Lyman-alpha bounds on the dark matter mass in Lambda Warm Dark Matter (Lambda-WDM) models, and derive new bounds in the case of mixed Cold plus Warm models (Lambda-CWDM), using a set up which is a good approximation for several theoretically well-motivated dark matter models. We combine WMAP5 results with two different Lyman-alpha data sets, including observations from the Sloan Digital Sky Survey. We pay a special attention to systematics, test various possible sources of error, and compare the results of different statistical approaches. Expressed in terms of the mass of a non-resonantly produced sterile neutrino, our bounds read m_NRP > 8 keV (frequentist 99.7% confidence limit) or m_NRP > 12.1 keV (Bayesian 95% credible interval) in the pure Lambda-WDM limit. For the mixed model, we obtain limits on the mass as a function of the warm dark matter fraction F_WDM. Within the mass range studied here (5 keV < m_NRP < infinity), we find that any mass value is allowed when F_WDM < 0.6 (frequentist 99.7% confidence limit); similarly, the Bayesian joint probability on (F_WDM, 1/m_NRP) allows any value of the mass at the 95% confidence level, provided that F_WDM < 0.35.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/309b32e1e25dda12cb5a1b69280544c6b1b590f6
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In Astronomy and Astrophysics
- Volker Springel
- Simon D. M. White
- P. Hopkins
- Carlos S. Frenk
- M. Boylan-Kolchin
- L. Hernquist
- James S. Bullock
- A. Benson
In Nuclear and High Energy Physics
- M. Drewes
- Julien Lesgourgues
- Z. Xing
- M. Shaposhnikov
- Carlos S. Frenk
- Alexey Boyarsky
- Oleg Ruchayskiy
- James S. Bullock
Citations in the corpus
- “Non-cold” dark matter at small scales: a general approach (2017, background): “In principle, the DM sector may consist of a complicated mixture of different DM particles [60].”
- Neutrino physics with the PTOLEMY project: active neutrino properties and the light sterile case (2019, background): “On the other hand, neutrino states with a mass in the keV range are excellent warm dark matter candidates [26, 27].”
- Erratum: From dwarf spheroidals to cD galaxies: simulating the galaxy population in a ΛCDM cosmology (2010, background): “These place an upper limit on the cut-off wavelength and the corresponding halo mass, which implies a lower limit on the mass of the dark matter particle (Viel et al. 2008; Boyarsky et al. 2009a,b).”
- The Milky Way’s bright satellites as an apparent failure of ΛCDM (2011, background): “The particle mass used by Lovell et al. (2012) is also near the lower limit of what is allowed by observations of Lyman-α absorption features in the spectra of distant quasars (Boyarsky et al. 2009).”
- A facility to search for hidden particles at the CERN SPS: the SHiP physics case (2015, background): “In addition the Lyman-α bound (M & 8 keV [736], marked by the cross) is in tension with the other bounds.”
- The Dawn of FIMP Dark Matter: A Review of Models and Constraints (2017, background): “It is therefore evident that sterile neutrinos produced by the DW mechanism cannot account for all DM, although it has been claimed that they can still comprise O(10)% of the observed abundance [350, 351].”
- New production mechanism for keV sterile neutrino Dark Matter by decays of frozen-in scalars (2013, background): “The constraints from structure formation [7] can then only be realised for relatively large keV sterile neutrino masses, which are in conflict with the constraints from the nonobservation of the decay of the keV neutrino into a light neutrino and a photon [17, 18].”
- The effect of neutrinos on the matter distribution as probed by the intergalactic medium (2010, methodology): “ion of Damped Lyman-α systems to the flux power spectrum. In total a set of 28 parameters are allowed to vary. For a more extensive discussion on the use of the MCMC method in this context we refer to [53, 54, 55]. The main difference to our previous work in this respect is the addition of the effect o”
- Lyman-alpha forests cool warm dark matter (2015, background): “0 30 HIRES + 27 UVES + 23 LRIS (30, 200) hydro BLR09 [14] 2.”
- Detecting superlight dark matter with Fermi-degenerate materials (2015, positive): “Cosmologically, the keV mass scale is significant because it corresponds to the lower bound on the DM mass from the Lyman-α forest [24] and phase space packing [25, 26]; lighter (fermionic and thermalized) DM is inconsistent with cosmological observations (though see ref.”
- Quantifying the effect of baryon physics on weak lensing tomography (2011, background): “…et al. 2005): α = 0.049 (mWDM keV )−1.11(ΩWDM 0.25 )0.11( h 0.7 )1.22 h−1Mpc, (23) whereΩWDM is the WDM density parameter andmWDM is the WDM particles mass. Observations of the power spectrum of the Lyman-α forest suggestmWDM > 4keV (Seljak et al. 2006; Viel et al. 2008; Boyarsky et al. 2009).”
- Constraints on neutrinos and WDM Hints, neutrino bounds and WDM constraints from SDSS DR14 Lyman-$\alpha$ and Planck full-survey data (2019, methodology): “Since it extends the lever arm of other cosmological probes towards smaller scales, it has often been used to constraint the parameters of models affecting only the smallest scales – like warm dark matter (WDM) [1–4] or interacting dark matter [5–7] – or altering the global shape of the power spectr”
- Dark Matter, Baryogenesis and Neutrino Oscillations from Right Handed Neutrinos (2012, background): “Without resonant production, the distribution reconstructed from Lyα forest observations suggests a lower bound on the mass M1 & 8 keV [92], see also [93–95] 19.”