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Effects of early reionization on the formation of galaxies. Hajime Susa Rikkyo University. Impacts of UVB on GF. PHOTO IONIZATION Production of electrons : catalysts of H 2 formation → enhance the fraction of H 2 Momentum Transfer PHOTO DISSOCOATION Dissociation of H 2 → No coolant
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Effects of early reionization on the formation of galaxies Hajime Susa Rikkyo University
Impacts of UVB on GF • PHOTO IONIZATION • Production of electrons : catalysts of H2 formation → enhance the fraction of H2 • Momentum Transfer • PHOTO DISSOCOATION • Dissociation of H2 → No coolant • PHOTO HEATING • Keep the gas temperature 104-105 K • Photo-evaporation • Suppression of SF in gals.
Substructure in Galactic Halo Cluster Halo Moore et al. 1999 Galactic Halo 20 times smaller than expected
Blown away by photo-evaporation Late Reionization, CDM density perturbation, and Radiative cooling..... If Z_reion=7, 1σ density perturbations are not prevented from forming stars. 20 7
Early reionization (WMAP) Spergel et al. 2003 Instantaneous reionization:
Shaded ≒ Blown away by photo-evaporation Early Reionization, CDM density perturbation, and Radiative cooling..... If Z_reion=20, >2σ density perturbations are prevented from forming stars. 20 7
Smaller scale sub-clumps In hierarchical clustering scenario, small clumps evolve faster than the parent system.
Method (RSPH) • SPH • Steinmetz & Muller 1993 • Umemura 1993 • Gravity • HMCS in University of Tsukuba(CCP) • GRAPE6, direct-sum • Radiation transfer of ionizing photons • Kessel-Dynet & Burkurt 2000 • Nakamoto, Umemura & Susa 2001 • Primordial chemistry & Cooling • Susa & Kitayama 2000 • Galli & Palla 1998
Model of SF In order to evaluate the case of maximal star formation rate, we assume
Model of UVB Early Reionization model Put a source outside the simulation box so that the mean intensity is equal to above value at the center.
Maximally Star-forming model (c*=1) “ Evaporated ” >95% halos are photo-evaporated.
Summary 1 • Formation of low mass galaxies are investigated by 3D RHD simulationswith early reionization model. • CDM substructure problem isresolved solely by the early reionization model at dSph scale (<10^8 Msun or Vrot < 20 km/s).
Detection of Reneutralization ? Susa Rikkyo University
GP trough of High-z QSOs Z=5.80 @ z=6 Z=5.82 z>7 ... No flux.... Z=5.99 Z=6.28 Fan et al. 2002 Becker et al., 2001
Top Heavy IMF? +First Stars TOP Heavy Volume fraction of HII region POPII、 Salpeter IMF τe Sokasian et al 2003
High-z Lyα emitter low-z high-z
High-z Lyαemitter 2 Haiman 2002 Broad line emission + high SFR ⇒ large self HII region⇒ Still detectable even at neutral universe. How they look like in double reionization universe ?
A double reionization history Z<6 yh1=0.0001 6<z<9 yh1=0.3 9<z<19 yh1=0.0001 Z>19 yh1=1 Cen like Effects of self-HII region is also taken into account. Haiman like
Emission profile Δv=10km/s, SFR=1Msun/yr Z=15 Z=4 ionized ionized revival Z=23 neutral Z=9 neutral
Flux of Lyα、Hα Detectable by next generation facilities ………….
Summary 2 • It is possible to use F(Lyα)/F(Hα) ratio to probe the reionization history at z > 7. • If double reionization history is assumed, the ratio has characteristic behavior.