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LAES POWERED BY AGN AND THEIR IMPACTS ON COSMIC REIONIZATION SUNGHYE BAEK (SNS, ITALY) COLLABORATION WITH ANDREA FERRARA SKA IN EAST ASIA 2013 NAGOYA UNIVERSITY 5-7 JUNE 2013 2013 MNRAS 432L 6B THE 21 CM SIGNAL AND THE 21 CM SIGNAL AND


  1. LAES POWERED BY AGN AND THEIR IMPACTS ON COSMIC REIONIZATION SUNGHYE BAEK (SNS, ITALY) COLLABORATION WITH ANDREA FERRARA SKA IN EAST ASIA 2013 NAGOYA UNIVERSITY 5-7 JUNE 2013 2013 MNRAS 432L 6B

  2. THE 21 CM SIGNAL AND THE 21 CM SIGNAL AND REIONIZATION REIONIZATION MOST PROMISING PROBE OF THE DARK AGES AND • REIONIZATION SIGNAL REDSHIFTED TO METER WAVE (50-200 MHZ), • DETECTABLE WITH SKA THE INTENSITY OF THE 21CM DEPENDS ON THE • TEMPERATURE OF THE IGM : WE CAN CONSTRAIN SOURCE PROPERTIES (X-RAYS) USING THE 21 CM POWER SPECTRUM X-RAYS HEATING → INCREASE GAS TEMPERATURE (IGM) → REDUCE THE INTENSITY OF THE 21 CM SIGNAL

  3. X-RAYS AND THE IGM X-RAYS AND THE IGM TEMPERATURE TEMPERATURE BAEK+2010

  4. POWER SPECTRUM OF POWER SPECTRUM OF Δ T T B B BAEK+2010

  5. X-RAY SOURCE CANDIDATE AT X-RAY SOURCE CANDIDATE AT HIGH-Z HIGH-Z QSO : THE MOST RECENT RECORD AT Z=7.1 HOSTING 10 9 • M SOL BH THEIR PROGENITORS Z > 7 : AGN HOSTING MINI OR • INTERMEDIATE BH WHERE X-RAY INTENSITY UNDER DETECTION LIMIT THE ROLE OF MINI(INTERMEDIATE) BH IN ACTIVE NUCLEUS • GALAXY : ALTERNATIVE SOURCE FOR LYMAN ALPHA? WHAT IS THE PROPERTIES OF SUCH LAE POWERED BY AGN • WITH RESPECT TO THE ONE POWERED BY STARBURST?

  6. LYMAN APHA EMITTERS LYMAN APHA EMITTERS A PROMINENT LY α (N=2 → N=1 : • 1216 Å) LINE EMITTING GALAXIES (EW ≥ 20 Å) HIGH REDSHIFT, STARBURST • GALAXIES, HIGH HI DENSITY (Z ≅ 2-7) STAR FORMATION → IONIZING • UV → RECOMBINATION → EMITTING LY α SOURCES OF REIONIZATION •

  7. ORIGINS OF LYMAN PHOTON ORIGINS OF LYMAN PHOTON RECOMBINATION • IN THE IONIZED GAS • STAR FORMING HIGH DENSE REGION • STRONG UV FIELD, SHORT RECOMBINATION TIME • VERY EFFICIENT PROCESS • EXCITATION - DEEXCITATION • IN THE NEUTRAL GAS • STELLAR WIND VIA COOLING (LYMAN ALPHA BLOB) • X-RAYS •

  8. MOTIVATION MOTIVATION Galaxies at high redshift (z>6) are compact and contains plenty of neutral gas. When AGN in LAE is faint (X-rays flux under detection limit) and obscured (no broaden emission), How can we distinguish and identify them from LAE powered by starburst?

  9. LAE WITH AGN LAE WITH AGN X-rays detection on LAE • Gawiser et al. 2006 at z~3 • Zheng et al. 2010 at z~4.5 • Broaden emission line • Ouchi et al. 2008 at z~3-4, 800 candidates • 1 % contains AGN • Brightest LAEs with Log(L α ) > 43.4-43.6 erg s -1 • Variable photometry • Shibuya et al. 2012 at z~7.3 • Temporal luminosity enhancement • Shibuya et al. 2012 associated with a QSO, an AGN, or SN

  10. NUMERICAL SIMULATION NUMERICAL SIMULATION Hydrodynamics Gadget2 • Consider both ISM 2 X 512 3 DM and baryon • and IGM to DM : 6.68 X 10 5 M sol • modeling LAE at Baryon : 1.32 X 10 5 M sol • z=6.6 UV, X-ray RT with LICORICE • A Point source at the center • Ly α RT with LICORICE • 10 cMpc/h Source from every cell where • Log(L α ) > 37 [erg s -1 ]

  11. 3 MODELS - DIFFERENT SED 3 MODELS - DIFFERENT SED 1. Starburst model STARBURST99 : 0.02 Z sol , Salpeter IMF, 1-100 M sol cut off Continuous SFR : 10 M sol /yr 2. The Compton thick AGN (Shang et al. 2011) UV and X-rays confined in a cone with opening θ =45° 3. The Compton thin AGN Isotropically emitted for X-rays 100eV < h ν < 500eV AGN composite spectra Normalized to have the same X-rays photoionization rate ˙ Q = 3 × 10 54 s − 1 A halo with M h =1.17X10 11 M sol

  12. TOTAL INTRINSIC LYA TOTAL INTRINSIC LYA X-rays Recombination Lya production : X-rays ➘ ➘ with time • Recombination ➚ ➚ with time • Early : X-ray dominated ★ Later : Recombination ★ dominated

  13. Neutral fraction Ly α radiative transfer Ly α production UV, X-rays RT 1 st post processing Ly α Surface Brightness Ly α RT 60 pkpc/h 2 nd post processing

  14. Nature of LAE powered by AGN

  15. 1. Evolution of skewness S w Early phase Later phase

  16. Lower skewness z~5.7 Ouchi et al. 2008

  17. 2. Evolution of the SB profile (the SB map) Early phase or X-ray effect dominates Later phase or recombination dominates

  18. Skewness vs. FWHM of SB Starburst can not make Parametrized curves with time t = 0.02, 0.04, 0.06, 0.08, 1.00 • Myr from left to right The shaded area denotes AGN-powered LAE identification • criterion S w < 0 and FWHM ≥ 1.5”

  19. Summary Alternative X-ray/Lya source for high-z (z>6) • High redshift (z>6) LAE probably contains obscured and • less powerful AGN For given Q, X-rays can boost Ly α luminosity with several • orders when there is plenty of neutral gas (e.g. when AGN just turns on or large amount of accreting gas) Nature of LAE powered by AGN • The lower skewness S w < 0 • Extended SB profile, having FWHM greater than FWHM • of PSF(seeing size) FWHM ≥ 1.5”

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