4.7 Article

Characterizing dark interactions with the halo mass accretion history and structural properties

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 434, Issue 4, Pages 2982-2998

Publisher

OXFORD UNIV PRESS
DOI: 10.1093/mnras/stt1218

Keywords

methods: numerical; galaxies: haloes; cosmology: theory; dark matter

Funding

  1. European Seventh Framework Programme, Ideas [259349]
  2. European Community
  3. DFG Cluster of Excellence 'Origin and Structure of the Universe'
  4. TRR33 Transregio Collaborative Research Network on the 'DarkUniverse'
  5. PRIN MIUR
  6. [ASI-INAF I/023/12/0]

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We study the halo mass accretion history (MAH) and its correlation with the internal structural properties in coupled dark energy (cDE) cosmologies. To accurately predict all the non-linear effects caused by dark interactions, we use the COupled Dark Energy Cosmological Simulations (CoDECS). We measure the halo concentration at z = 0 and the number of substructures above a mass resolution threshold for each halo. Tracing the halo merging history trees back in time, following the mass of the main halo, we develop a MAH model that accurately reproduces the halo growth in term of M-200 in the Lambda cold dark matter (Lambda CDM) Universe; we then compare the MAH in different cosmological scenarios. For cDE models with a weak constant coupling, our MAH model can reproduce the simulation results, within 10 per cent of accuracy, by suitably rescaling the normalization of the linear matter power spectrum at z = 0, Sigma(8). However, this is not the case for more complex scenarios, like the 'bouncing cDE model, for which the numerical analysis shows a rapid growth of haloes at high redshifts, that cannot be reproduced by simply rescaling the value of Sigma(8). Moreover, at a fixed value of Sigma(8), CDM haloes in these cDE scenarios tend to be more concentrated and have a larger amount of substructures with respect to Lambda CDM predictions. Finally, we present an accurate model that relates the halo concentration to the time at which it assembles half or 4 per cent of its mass. Combining this with our MAH model, we show how halo concentrations change while varying only Sigma(8) in a Lambda CDM Universe, at a fixed halo mass.

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