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Quasar Absorption System Current status of QALs (1) Katsuya Okoshi - PowerPoint PPT Presentation

Quasar Absorption System Current status of QALs (1) Katsuya Okoshi Tokyo Univ of Science Kazuyuki Ogura (Bunkyo Univ) 2018/11/24-25 Introduction Ly emission QSO spectra HI absorptions Metal absorptions Classification H


  1. Quasar Absorption System Current status of QALs (1) Katsuya Okoshi � Tokyo Univ of Science � Kazuyuki Ogura (Bunkyo Univ) 2018/11/24-25

  2. Introduction Lyα emission QSO spectra HI absorptions Metal absorptions

  3. Classification • HⅠ absorption Systems Photo-ionization: “Ionized” system � Cross section cm 2 cm -2 n Metal absorption Systems Elements: C, Mg, Fe, Na, Zn, etc.. � Constraints on SF, SN feedback process

  4. Why we focus on absorption systems ? • Physical properties of Intergalactic Medium � IGM) Dominant process in IGM Photo-ionization: UV background radiation at e=13.6 eV Photon vs Baryon

  5. UV background radiation at e=13.6 eV Ø Number densities of Radiation sources QSOs, young galaxies, … Ø Proximity Effect : Decrease Lyα Forest in the vicinity of QSOs

  6. Ionization state of IGM Ionization rate per hydrogen atom Photo-ionization timescale Recombination timescale (+ Timescales of physical & chemical processes gravitational instability, etc)

  7. Hydrogen photoionization rate Galaxiess QSOs Haadt & Madau 2012

  8. Photon vs Baryon Observed photon is enough to ionize the intergalactic medium? Photon number density n γ vs Baryon number density n B at z=3

  9. Ionizing radiation intensity at 912 Å Haadt & Madau 2012

  10. Photo-ionization: UV background radiation at e=13.6 eV Specific Intensity at z~2-3

  11. Low Opacity (Lyα) High Opacity

  12. Single power-law ( ∝ N(HI) � β )

  13. N HI ∝ N HI � β ; β < 2 Prochaska et al. 2010

  14. HI gas reservoir DLA contains a significant fraction of the HI gas in the universe! Ω(HI) � 10 -3 at 0 < z < 4 β = 1.4-1.7 HI gas resides in DLAs �

  15. Rao et al. 2017

  16. Codoreanu et al. 2018

  17. QSO Absorption Systems Types Log N(HI) dN/dz Origin Lyα Forest 13-16.5 ~30 (z<2) Intergalactic density fluctuations ~100 (z=3) Cool CGM (10 4 K) (?) LLS 17-19 ~0.6(z~1) ~1-3 (z=3) Sub-DLA 19-20 ~0.6 (z=3) Extended halo gas, outflows (?) DLA 20-22 ~0.1 (z=1) Galactic disk, Extended halo gas, outflows, inflows, ~0.2 (z=3) tidal gas, etc… halo hot gas (10 5 K) C IV ~ Lyα Forest ~10 (z~0) (?) <10 (z>3) IGM halo warm gas (10 3 K) Mg II 15-20 ~1 (z~1) <5 (z>3) Gas out/inflow O VI ~ LLS(?) ~1-10 (z~0) Warm-hot CGM (?) ~30 (z~2)

  18. Metal abundance N(HI) distribution Incidence Rate QSO Absorption System Correlation (QSO) Gas abundance Correlation (galaxy) dynamics

  19. Incidence rate n : number density σ : cross section

  20. Redshift Distributions (Incidence Rates) of DLA, sub-DLA &LLS LLS (17.2< Log N(HI)/ cm -2 <19.0) Sub-DLA (19.0< Log N(HI)/ cm -2 <20.3) DLA ( Log N(HI) /cm -2 >20.3)

  21. HI absorption systems No evolution

  22. H Lyα 1216 Å Ionizing radiation spectrum CIV 1418 Å MgII 2783 Å OVI 1078 Å LL 912 Å

  23. Low ionization system Mg Ⅱ, Si Ⅱ, Al Ⅱ, O I, etc IP/eV = 15.0, 16.3, 18.8, 13.6, .. Low-temperature/high-density regions High ionization system C Ⅳ, Si Ⅳ, O Ⅳ, etc IP/eV = 64.4, 45.1, 136.1, .. High-temperature/low-density regions

  24. Metal absorption systems Strong MgII traces GALAXIES?

  25. Weak MgII (W<0.3Å) Strong MgII (W>0.3Å) Nestor et al. 2005

  26. HI & Metal absorption systems Trace structure Trace structure formation ? formation ? (e.g., galaxies ?)

  27. Mean proper distance along the line of sight

  28. Mean proper distrance between systems along the line of sight 1000 z = 3 100 L / Mpc 10 1 0 Lya Forest LLS DLA weak MgII strong MgII CIV 1 2 3 4 5 6 7 Metal HI

  29. Incidence rate n : number density σ : cross section

  30. Total cross sections σ at z=3 (n=1.0 � 10 -3 Mpc -3 ) 100 z = 3 Cross section / Mpc 2 10 1 0.1 0 Lya Forest LLS DLA weak MgII strong MgII CIV 1 2 3 4 5 6 7

  31. Total cross sections at z=3 (n=1.0 � 10 -3 Mpc -3 ) 100 z = 3 Cross section / Mpc 2 10 1 0.1 0 Lya Forest LLS DLA weak MgII strong MgII CIV 1 2 3 4 5 6 7

  32. Total cross sections at z=3 (n=1.0 � 10 -3 Mpc -3 ) 100 z = 3 Cross section / Mpc 2 10 1 0.1 0 Lya Forest LLS DLA 1 2 3 weak MgII strong MgII CIV 4 5 6 7

  33. Strong MgII and DLA DLA shows strong MgII MgII Absorption width Rao et al. 2017

  34. DLA-MgII Sub-DLA-CIV LLS-OVI Lyα Forest

  35. Absorbers as a probe of SF in galactic halos SF in galaxctic halos Vs Physical scale R (e.g, cross section σ) radiation e.g., SFR Velocity shifts Metallicity Velocity width ΔV 90 including Outflow DLA Sub-DLA LLS

  36. Summary • QSO Absorption System HI, Metal absorption system & IGM � Incident rates dN/dz (+ Total cross-section ) DLA < LLS < Lyα forest strong MgII < weak MgII < CⅣ ~ OⅥ Galaxy < Halo (virial radius) < CGM < LSS (filaments, voids) • A probe of galaxy, galactic halo, CGM and IGM Galaxy DLA and strong MgII Halo (cloud in/outflow) & CGM DLA~LLS, MgII IGM Lya-forest , CIV

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