Fetching the paper…
Reading the bibliography…
Dwarf spheroidal galaxies provide well-known challenges to the standard cold and collisionless dark matter scenario: The too-big-to-fail problem, namely the mismatch between the observed mass enclosed within the half-light radius of dwarf spheroidals and cold dark matter N-body predictions; The hints for inner constant-density cores.
\BibitemOpen
1911
Earlier work this paper cites.
\BibitemOpen
1974
Earlier work this paper cites.
\BibitemOpen
1995
Earlier work this paper cites.
\BibitemOpen
1997
Earlier work this paper cites.
\BibitemOpen
2000
Earlier work this paper cites.
\BibitemOpen
2006
Earlier work this paper cites.
\BibitemOpen
2007
Earlier work this paper cites.
\BibitemOpen
2007
Earlier work this paper cites.
\BibitemOpen
2008
Earlier work this paper cites.
For what concerns the outer region of the system, we actually assume that the DM halo of the classical satellites can be extended up to 𝒪 ( 10 ) \mathcal{O}(10) kpc. Such order of magnitude estimate may be easily obtained from the Roche limit of satellite galaxies under the influence of the MW gravitational field Strigari et al. 2008 : 75 (75) r t = ( G N 2 M dSph M MW ( d σ MW ) 2 ) 1 3 ∼ 10 kpc , \@@lbibitem{}\NAT@@wrout{75}{}{}{}{(75)}{}\lx@bibnewblock r_{t}=\left(\frac{G_{N}}{2}\frac{M_{\textrm{dSph}}}{M_{\textrm{MW}}}\left(\frac{d}{\sigma_{\textrm{MW}}}\right)^{2}\right)^{\frac{1}{3}}\sim 10\ \textrm{kpc}\ , (8)
2008
Earlier work this paper cites.
\BibitemOpen
2008
Earlier work this paper cites.
\BibitemOpen
2009
Earlier work this paper cites.
\BibitemOpen
2010
Earlier work this paper cites.
\BibitemOpen
2010
Earlier work this paper cites.
\BibitemOpen
2010
Earlier work this paper cites.
\BibitemOpen
2011
Earlier work this paper cites.
\BibitemOpen
2011
Earlier work this paper cites.
\BibitemOpen
2011
Earlier work this paper cites.
\BibitemOpen
2012
Cited alongside, same era.
\BibitemOpen
2012
Cited alongside, same era.
\BibitemOpen
2012
Cited alongside, same era.
\BibitemOpen
2012
Cited alongside, same era.
\BibitemOpen
2012
Cited alongside, same era.
\BibitemOpen
2013
Cited alongside, same era.
\BibitemOpen
2013
Cited alongside, same era.
\BibitemOpen
2013
Cited alongside, same era.
\BibitemOpen
2015
Later among the works it cites.
\BibitemOpen
2015
Later among the works it cites.
\BibitemOpen
2016
Later among the works it cites.
\BibitemOpen
2016
Later among the works it cites.
\BibitemOpen
2016
Later among the works it cites.
2016
Later among the works it cites.
\BibitemOpen
2016
Later among the works it cites.
\BibitemOpen
alphaXiv searches the wider corpus for related work and actual follow-ups.
alphaXiv is searching for related work…
Acknowledgments:
2013
Cited alongside, same era.
Spherical Jeans analysis
2013
Cited alongside, same era.
Eventually, the most important part of our statistical analysis consists in the Bayesian fit of the 7-parameter SIDM model on the basis of the log ℒ tot \log\mathcal{L}_{\textrm{tot}} discussed above. At the basis of the adopted MCMC algorithm for the present study there is the affine-invariant ensemble sampler algorithm of Goodman & Weare 2010 . We have used the public implementation of it within the package emcee
2013
Cited alongside, same era.
2013
Cited alongside, same era.
2016
Later among the works it cites.
Concentration-mass relation for MW dSphs
2016
Later among the works it cites.
Equipped with such concentration-mass relation, we can estimate the allowed spread on R max R_{\textrm{max}} and V max V_{\textrm{max}} according to the outcome in Vogelsberger et al. 2016 . Varying R max R_{\textrm{max}} for fixed values of V max V_{\textrm{max}} , namely 25, 40, 55 km/s, we end up estimating an overall spread on R max R_{\textrm{max}} of about 0.2 dex in order to span the whole gray band in the right panel of figure 9 in Vogelsberger et al. 2016 . Note that, while our study of the SIDM model importantly depends on the adopted spread and functional form of the concentration-mass relation discussed here, our derivation of the latter may be regarded as “conservative”. Indeed, we are including the spread of the fifteen most massive CDM subhalos as representative of the eight most luminous MW dSph satellites analyzed in our work. Restricting to the spread reported e.g. in Zavala et al. 2013 for the classical satellites (figure 2 of the reference), would have led to a much more restrictive constraint in our analysis and would be translated into a stronger tension for CDM in our inspection of the TBTF problem. In order to stick to what illustrated in Vogelsberger et al. 2016 within a minimal set of assumptions, we do not impose in our study a definite range on V max V_{\textrm{max}} , but rather require V c ( r = 0.5 kpc ) > 19 V_{c}(r=0.5\ \textrm{kpc})>19 km/s, together with 25 km/s < V c ( r = 10 kpc ) < <V_{c}(r=10\ \textrm{kpc})< 60 km/s, consistently with the CDM band in figure 2
2016
Later among the works it cites.
\BibitemOpen
2016
Later among the works it cites.
\BibitemOpen
2017
Closest in time.
\BibitemOpen
2017
Closest in time.
\BibitemOpen
2017
Closest in time.
\BibitemOpen
2017
Closest in time.
\BibitemOpen
2017
Closest in time.
\BibitemOpen
2017
Closest in time.
\BibitemOpen
2018
Closest in time.