Research

Numerical Astrophysics / Galaxies / Galaxy Clusters / Large-Scale Structure

Scientific Research

Dark Baryon

It is well known that the baryonic component occupies about 4% of the cosmic energy density. However, the amount of the baryons observationally identified in galaxies, galaxy clusters in nearby universe is at most only half of the cosmic baryonic content. Such unindentified baryonic component is called "missing baryon" or "dark baryon". Based on cosmological hydrodynamic simulations of the large-scale structure in the universe, about 40% of the baryonic component in the current universe is in the form of diffuse plasma with a temperature of 105 K to 107 K associated with the large-scale structure, and a promissing candidate of the dark baryon. Such component is called "Warm-Hot Intergalactic Medium" of WHIM for short.

  • Detectability of WHIM through emission lines of ionized oxygen ions
  • Distribution of WHIM in the local universe
  • Non-equilibrium ionization state of WHIM
  • Galaxy Clusters

    Galaxy clusters are the largest virialized systems in the universe, and their typical dynamical timescale is comparable to the age of the universe. Thus, the abundance of galaxy clusters is an important clue to the cosmological parameters. Recently, galaxy clusters are observed in the radio bands through the Sunyaev-Zel'dovich (SZ) effect as well as in the X-ray bands, and the combinations of X-ray and radio observations of galaxy clusters provide new physical insights to the intracluster medium (ICM). Furthermore, the physical state of the ICM in the outskirts of galaxy clusters which had been beyond the reach of X-ray observation is probed with the observation using Suzaku satellite.

  • Reconstruction of 3D profiles of galaxy clusters with the combinations of X-ray and radio observations
  • Study of the abundance of galaxy clusters using cosmological N-body/SPH simulations
  • Sunyaev-Zel'dovich observation of a galaxy cluster RX J1347-1145
  • Cluster morphology as a test of cosomological parameters
  • Non-equilibrium ionization state of ICM in a merging galaxy cluster system A399 and A401
  • Non-equilibrium ionization and two-temperature states of merging galaxy clusters
  • Non-equilibrium ionization and two-temperature states of the Bullet cluster 1E 0657-56
  • Cosmological Neutrinos

    Neutrinos are the electrically neutral leptons and thought to be detached from photons in the very early phase of our universe. In the standard model of elemetary particle physics, they are assumed to be massless based on the fact that all neutrinos are left-handed. However, the detection of the neutrino oscillation in ground-based experiments turns out that neutrinos are MASSIVE. We can only measure the squared masses differences of neutrinos in different mass eigen states through the detection of neutrino oscillation. Since cosmological neutrinos detached from photons in the early universe are non-relativistic massive component in the present universe, it can make physical impact on the fomation of the large-scale structure in the universe through the gravitational interaction. One of the such physical effects is the collisionless damping (aka free streaming or Landau damping) caused by the large velocity dispersion of the cosmological neutrnios and tends to erase the density fluctuation, which is evolved through the gravitational instability drived by the cold dark matter. The collisionless damping is actually difficult to be handled with conventional N-body simulations. We, instead, explore an alternative approach other than N-body simulations, the Vlasov simulation, which directly solves the collisionless Boltzmann equation or the Vlasov equation.

  • Direct Integration of the Collisionless Boltzmann Equation in Six-dimensional Phase Space: Self-gravitating Systems
  • Cosmological Vlasov-Poisson Simulations of Structure Formation with Relic Neutrinos: Nonlinear Clustering and the Neutrino Mass
  • A 400 trillion-grid Vlasov simulation on Fugaku supercomputer: large-scale distribution of cosmic relic neutrinos in a six-dimensional phase space