TY - JOUR
T1 - A deeper look into the structure of CDM haloes
T2 - Correlations between halo parameters from Einasto fits
AU - Udrescu, Silviu M.
AU - Dutton, Aaron A.
AU - Macciò, Andrea V.
AU - Buck, Tobias
N1 - Publisher Copyright:
© 2018 The Author(s).
PY - 2019/2/1
Y1 - 2019/2/1
N2 - We used high resolution dark matter only cosmological simulations to investigate the structural properties of Lambda Cold Dark Matter (CDM) haloes over cosmic time. The haloes in our study range in mass from ∼1010 to ∼1012 M, and are resolved with 105 to 107 particles. We fit the spherically averaged density profiles of DM haloes with the three parameter Einasto function. For our sample of haloes, the Einasto shape parameter, α, is uncorrelated with the concentration, c, at fixed halo mass, and at all redshifts. Previous reports of an anticorrelation are traced to fitting degeneracies, which our fits are less sensitive to due to our higher spatial resolution. However, for individual haloes the evolution in α and c is anticorrelated: at redshift z = 7, α 0.4 and decreases with time, while c 3 and increases with time. The evolution in structure is primarily due to accretion of mass at larger radii. We suggest that α traces the evolutionary state of the halo, with dynamically young haloes having high α (closer to a top-hat: α−1 = 0), and dynamically relaxed haloes having low α (closer to isothermal: α = 0). Such an evolutionary dependence reconciles the increase of α versus peak height, ν, with the dependence on the slope of the power spectrum of initial density fluctuations found by previous studies.
AB - We used high resolution dark matter only cosmological simulations to investigate the structural properties of Lambda Cold Dark Matter (CDM) haloes over cosmic time. The haloes in our study range in mass from ∼1010 to ∼1012 M, and are resolved with 105 to 107 particles. We fit the spherically averaged density profiles of DM haloes with the three parameter Einasto function. For our sample of haloes, the Einasto shape parameter, α, is uncorrelated with the concentration, c, at fixed halo mass, and at all redshifts. Previous reports of an anticorrelation are traced to fitting degeneracies, which our fits are less sensitive to due to our higher spatial resolution. However, for individual haloes the evolution in α and c is anticorrelated: at redshift z = 7, α 0.4 and decreases with time, while c 3 and increases with time. The evolution in structure is primarily due to accretion of mass at larger radii. We suggest that α traces the evolutionary state of the halo, with dynamically young haloes having high α (closer to a top-hat: α−1 = 0), and dynamically relaxed haloes having low α (closer to isothermal: α = 0). Such an evolutionary dependence reconciles the increase of α versus peak height, ν, with the dependence on the slope of the power spectrum of initial density fluctuations found by previous studies.
KW - Cosmology: theory
KW - Dark matter
KW - Galaxies: formation
KW - Galaxies: structure
KW - Methods: numerical
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U2 - 10.1093/mnras/sty3112
DO - 10.1093/mnras/sty3112
M3 - Article
AN - SCOPUS:85061094622
SN - 0035-8711
VL - 482
SP - 5259
EP - 5267
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
IS - 4
ER -