SLIDE 1
H I 21 cm Absorption as a Probe of High-z ISM + Possible Interest for AGNs
Hiroyuki Hirashita
Masanori Nakamura, Keiichi Asada Chiranjib Konar (ASIAA, Taiwan)
See also T.-C. Chang’s review & C.-C. Chiong’s talk
SLIDE 2 Outline
- 1. Introduction to DLAs
- 2. Physical State of the ISM in DLAs
- 3. Interests in AGNs at ASIAA
- 4. Summary
SLIDE 3 QSO Damped Lyα cloud Lyα absorption
Damped Lyα Clouds (DLAs)
- High H I column density (> 2×1020 cm–2)
Reservoir of a large amount of H I ⇒ progenitors of nearby large galaxies?
- Unique objects at high z for detailed study ISM by
using various species.
SLIDE 4 21 cm Observations of DLAs
see also Curran et al. (2010)
Srianand et al. (2012) Kanekar et al. (2009): anticorrelation between metallicity and Ts
SLIDE 5
H2 in DLAs (A Probe of Cold Gas)
Ledoux, Petitjean, & Srianand (2003) log (molecular fraction) metal depletion log (dust/gas) log (molecular fraction)
Paucity of H2 large dispersion
SLIDE 6
DLA Samples are mostly tracing diffuse medium?
Paucity of 21 cm absorption detection ⇒ low τ ⇒ High Ts (warm diffuse medium) Paucity of H2 absorption detection ⇒ H is mostly atomic in the warm diffuse medium. (Hirashita et al. 2003)
SLIDE 7
- 2. Physical State of the ISM in DLAs
Damped Lyman α clouds (DLAs): NH > 2×1020 cm–2
Hirashita et al. (2003) background quasar
Experiment: One simulated galaxy with a background quasar at a random line of sight
SLIDE 8
50 pc log (molecular fraction)
Equilibrium H2 abundance (1) Formation on dust (2) Destruction by UV (1) = (2)
with i21 = 0.1, D = 0.1Dsun
Distribution of H2
Patchy and localized H2 distribution
Hirashita et al. (2003)
SLIDE 9
“Simulation” of Observation
log (dust-to-gas ratio) log (molecular fraction) ×: Ledoux et al. (2003) ◆: our simulation
Choose randomly a line of sight on the simulated galaxy ... positive correlation Molecular fraction increases rapidly at log (D/Dsun) ~ ‒1.5 (←self-shielding) large scatter
Hirashita & Ferrara (2005)
SLIDE 10 Implication for 21 cm Observations
- Detection rate of 21 cm absorption is low (1/10).
Consistent with the small covering fraction of cold gas
Srianand et al. (2012) At least an order of magnitude better S/N ⇒ SKA is suitable.
- Low detection rate of H2, which is localized in
the cold medium.
SLIDE 12 Imaging Re-collimation Process
Dynamic Range of current our EVN image is ~ 2500
- SKA will improve it > 1,000,000
Asada & Nakamura (2012)
HST-1 expansion Re-collimation? Re-ex pansion
- Is the M87 jet re-collimated to form HST-1?
SLIDE 13 Asada et al.
Imaging the counter-jets
Detection of the counter-jets is very important;
- Constraining a proper viewing angle
Jet acceleration dynamics SED analysis for core emission profile Modeling the accretion disk and BH shadow
SLIDE 14 Diffuse emission around FR II radio galaxies: episodic activity
αinn
inj ∼ αout inj : similar jet power
(Konar & Hardcastle, 2013) Newly discovered diffuse halo (Sirothia+, 2013) Hope to discover many such radio haloes with the SKA
Radio Galaxies: Their Dynamics and Episodic Jet Activities – p.17/17
SLIDE 15
(1)Small science group in ASIAA. ⇒ Collaboration is necessary. (2)Paucity of H I 21 cm detection for DLAs can be understood in terms of the prominent warm diffuse medium, consistent with the small H2 detection rate. (3)AGN science in ASIAA
- a. Collimation and dynamics of the M87 jet
- b. Survey of diffuse radio emission around radio galaxies
SLIDE 16
Deadline for abstracts: 24 August 2013