Over the past few decades, cosmological simulations have become
invaluable tools that are helping us to reach a deeper comprehension of
astrophysics, particularly about the formation and evolution of galaxies in the
early Universe (Springel et al., Nature, 2005). The intrinsic multi-scale
nature of astrophysical processes renders the task of comprehending the
functioning of the Universe a challenging endeavor. This is extremely evident
in cosmological simulations, as the reproduction of the behavior of the Universe
necessitates the inclusion of phenomena ranging from atomic physics to galactic
scales.
The advent of sophisticated numerical techniques and an enhanced
computing capacity have enabled modern simulations to follow every fundamental component
of the Cosmos, such as dark matter, dark energy and baryonic matter (Plack
Collaboration, A&A, 2016). The latter, more than the others, is the most
challenging to add in a numeric hydrodynamic simulation, because baryonic
matter is involved in many physical processes. Nevertheless, its presence in a
simulation is indispensable for the formation of stars and black holes, which
represent the main characters in the evolution of the Universe.
The concept of high-performance computing has facilitated the
development of increasingly sophisticated hydrodynamic simulations. Indeed,
while the desire to create more realistic simulations is understandable, it is
also important to consider the time required to obtain results. The
incorporation of additional physics necessitates an increase in the
computational time. The parallel computation has resulted in a significant
acceleration of cosmological hydrodynamic simulations. In our simulations, we
employ a combination of shared memory, message passing techniques and GPUs to
reduce the time-consuming nature of our codes.
Our research group at Sapienza University of Rome is interested in the
formation channels of supermassive black holes (Event Horizon Telescope
Collaboration, ApJL, 2019), which are black holes with masses between 108 ÷ 1010 MΘ situated at the center of galaxies. The
formation of a black hole can occur in several ways, however the maximum mass
estimated is approximately 104 MΘ (Omukai K., ApJ, 2001; Costa et al.,
MNRAS, 2023). Consequently, the key question is how they grow. Furthermore, the
modern space-born James Webb telescope has discovered numerous supermassive
black holes at a few million years after the Big Bang (Inayoshi et al.,
ARA&A, 2020). This challenges our understanding of black hole physics, as
the growth of the first black holes should have been extremely rapid.
In my current PhD research, I am utilizing the hydrodynamic galaxy
evolution code based on the SPH formalism called dustyGadget (Graziani et al.
MNRAS, 2020) to investigate the pristine environments where the first stars are
formed, with the goal of elucidating the conditions under which the first
stellar black holes will be created. Subsequently, the way these “seeds” will
assemble to give rise to the first supermassive black holes will be studied.
The final steps will how these massive objects will coevolve with their own
host galaxy. Indeed, it remains unclear whether the winds and matter accretion
of SMBHs could play an important role in defining the final morphology of their
host galaxy.