Ram pressure stripping of halo gas in disk galaxies: Implications on galactic star formation in different environments

We numerically investigate evolution of gaseous halos around disk galaxies in different environments ranging from small groups to rich clusters in order to understand galaxy evolution in these environments. Our simulations self-consistently incorporate effects of ram pressure of intergalactic medium (IGM) on disk and halo gas of galaxies and hydrodynamical interaction between disk and halo gas so that mass fractions of halos gas stripped by ram pressure of IGM (F_strip) can be better estimated. We mainly investigate how F_strip depends on total masses of their host environments (M_host}), galactic masses (M_gal), densities and temperature of IGM (T_IGM and rho_IGM, respectively), relative velocities between IGM and galaxies (V_r), and physical properties of disks (e.g., gas mass fraction). We find that typically 60-80% of halo gas can be efficiently stripped from Milky Way-type disk galaxies by ram pressure in clusters with M_host 10^{14} M_sun We also find that F_strip depends on M_host such that F_strip is higher for larger M_host. Furthermore it is found that F_strip can be higher in disk galaxies with smaller M_gal for a given environment. Our simulations demonstrate that the presence of disk gas can suppress ram pressure stripping of halo gas owing to hydrodynamical interaction between halo and disk gas. Ram pressure stripping of halo gas is found to be efficient (i.e., F_strip>0.5) even in small and/or compact groups, if rho_IGM ~ 10^5 M_sun/kpc^3 and V_r ~ 400 km/s. Based on the derived radial distributions of remaining halo gas after ram pressure stripping, we propose that truncation of star formation after halo gas stripping can occur outside-in in disk galaxies.Comment: 11 pages, 12 figures, accepted by MNRA

Origin of rotational kinematics in the globular cluster system of M31: A new clue to the bulge formation

We propose that the rotational kinematics of the globular cluster system (GCS) in M31 can result from a past major merger event that could have formed its bulge component. We numerically investigate kinematical properties of globular clusters (GCs) in remnants of galaxy mergers between two disks with GCs in both their disk and halo components. We find that the GCS formed during major merging can show strongly rotational kinematics with the maximum rotational velocities of 140 - 170 km/s for a certain range of orbital parameters of merging. We also find that a rotating stellar bar, which can be morphologically identified as a boxy bulge if seen edge-on, can be formed in models for which the GCSs show strongly rotational kinematics. We thus suggest that the observed rotational kinematics of GCs with different metallicities in M31 can be closely associated with the ancient major merger event. We discuss whether the formation of the rotating bulge/bar in M31 can be due to the ancient merger.Comment: 5 pages, 5 figures, accepted in MNRAS Letter

Photometric evolution of dusty starburst mergers:On the nature of ultra-luminous infrared galaxies

By performing N-body simulations of chemodynamical evolution of galaxies with dusty starbursts, we investigate photometric evolution of gas-rich major mergers in order to explore the nature of ultraluminous infrared galaxies (ULIRGs) with the total infrared luminosity ($L_{\rm IR}$ for $8\sim 1000$ $\mu$m) of $\sim$ $10^{12}$ $L_{\odot}$. Main results are the following three. (1) Global colors and absolute magnitudes the during dusty starburst of a major merger do not change with time significantly, because interstellar dust heavily obscures young starburst populations that could cause rapid evolution of photometric properties of the merger. (2) Dust extinction of stellar populations in a galaxy merger with large infrared luminosity ($L_{\rm IR}$ $>$ $10^{11}$ $L_{\odot}$) is selective in the sense that younger stellar populations are preferentially obscured by dust than old ones. This is because younger populations are located in the central region where a larger amount of dusty interstellar gas can be transferred from the outer gas-rich regions of the merger. (3) Both $L_{\rm IR}$ and the ratio of $L_{\rm IR}$ to $B$ band luminosity $(L_{\rm B}$) increases as the star formation rate increase during the starburst of the present merger model, resulting in the positive correlation between $L_{\rm IR}$ and $L_{\rm IR}/L_{\rm B}$.Comment: 32 pages 25 figures,2001,ApJ,in press. For all 25 PS figures (including fig25.ps), see http://newt.phys.unsw.edu.au/~bekki/res.dir/paper.dir/apj06.dir/fig.tar.g

Formation of globular clusters with multiple stellar populations from massive gas clumps in high-z gas-rich dwarf galaxies

One of the currently favored scenarios for the formation of globular clusters (GCs) with multiple stellar populations is that an initial massive stellar system forms (`first generation', FG), subsequently giving rise to gaseous ejecta which is converted into a second generation (SG) of stars to form a GC. We investigate, for the first time, the sequential formation processes of both FG and SG stars from star-forming massive gas clumps in gas-rich dwarf disk galaxies. We adopt a novel approach to resolve the two-stage formation of GCs in hydrodynamical simulations of dwarf galaxies.In the new simulations, new gas particles that are much less massive than their parent star particle are generated around each new star particle when the new star enters into the asymptotic giant branch (AGB) phase. Furthermore, much finer maximum time step width (<10^5 yr) and smaller softening length (<2 pc) are adopted for such AGB gas particles to properly resolve the ejection of gas from AGB stars and AGB feedback effects. Therefore, secondary star formation from AGB ejecta can be properly investigated in galaxy-scale simulations. An FG stellar system can first form from a massive gas clump developing due to gravitational instability within its host gas-rich dwarf galaxy. Initially the FG stellar system is not a single massive cluster, but instead is composed of several irregular stellar clumps (or filaments) with a total mass larger than 10^6 Msun. While the FG system is dynamically relaxing, gaseous ejecta from AGB stars can be gravitationally trapped by the FG system and subsequently converted into new stars to form a compact SG stellar system within the FG system. Interestingly, about 40% of AGB ejecta is from stars that do not belong to the FG system (`external gas accretion'). The mass-density relation for SG stellar systems can be approximated as rho_SG ~ M_SG^1.5.Comment: 23 pages, 16 figures, A&A in pres