Origin of Galaxies

TL;DR

This paper investigates the $ u$HDM cosmological model combining sterile neutrinos and MOND gravity, using hydrodynamical simulations to assess its ability to replicate standard cosmological observations and structure formation.

Contribution

It introduces and tests the opt-$ u$HDM model, optimizing its parameters to fit CMB data and exploring its implications for galaxy formation and high-redshift observations.

Findings

The $ u$HDM model can reproduce the expansion history similar to $ m extLambda$CDM.

Optimized opt-$ u$HDM fits Planck CMB data except the fourth peak.

Early structure formation occurs late, challenging high-redshift galaxy explanations.

Abstract

Milgromian Dynamics (MOND) has been particularly successful in predicting scaling relations for galactic systems, namely the baryonic Tully-Fisher for spirals, the Faber-Jackson for ellipticals and the Radial Acceleration Relation for late-type galaxies. Its essential tenet is the modification of the gravity law at low accelerations. Nevertheless, despite MOND's passed tests, the puzzle of the missing mass on galaxy clusters' scales still persists. One proposed scenario to complete this deficit and apply it further to cosmology is the so-called $\nu$HDM model. It is composed of a sterile neutrino and the MOND gravity. In this Ph.D. thesis, I have put forward this cosmological idea, conducting hydrodynamical simulations to investigate the $\nu$HDM structure formation. In the debut attempt, the $\nu$HDM model was proven capable of reproducing the $\Lambda$CDM cosmology, imitating the same expansion history ($\Omega_m \approx$ 0.3 and $H_0 \approx$ 67.6 km/s/Mpc), reproducing the CMB phenomenology, while the cosmic web is nicely formed. In the next step, I have optimized the $\nu$HDM model using Bayesian statistics, re-branding it to opt-$\nu$HDM. I managed to optimally fit the angular power spectrum of the CMB calculated by \textit{Planck}, except its fourth peak, but the opt-$\nu$HDM cosmological parameters changed significantly with respect to its precursor, resulting in a much heavier cosmos, with $\Omega_m \approx$ 0.5 and $H_0 \approx$ 55.6 km/s/Mpc. Next, I explore the opt-$\nu$HDM expansion history, its structure formation and the resulting mass function. The appearance of the early-time structures, firstly in the $\nu$HDM model, as well as in the opt-$\nu$HDM model occurs quiet late, at $z\approx4$ and at $z\approx 5.5$, respectively. Although the resolution has improved from previous studies, the $\nu$HDM variants cannot explain easily the high-redshift galaxies, observed by JWST.