Panoramic Survey of the Deep Universe. Observing Galaxy Formation at High Redshift. Toru Yamada National Astronomical Observatory of Japan Opt/IR Div., Subaru Telescope. Needs for Panoramic Deep Surveys Subaru/XMM-Newton Deep Survey Extensive Study of Lyα Blobs
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Panoramic Survey of the Deep Universe Observing Galaxy Formation at High Redshift Toru Yamada National Astronomical Observatory of Japan Opt/IR Div., Subaru Telescope
Needs for Panoramic Deep Surveys • Subaru/XMM-Newton Deep Survey • Extensive Study of Lyα Blobs • and High Redshift Large-Scale Structure
1. Panoramic Deep Surveys • - Subaru Deep Field Surveys * • - Subaru/XMM-Newton Deep Survey * • - EIS+Subaru Survey • - COSMOS • NEP Deep Survey (+Astro-F) • SSA22 Emission Line Galaxy Survey * • UKIDSS-DXS/Scam 10 deg2 Survey * • etc, etc…… * T.Y. involved
N-body + Semi-analytic treatment 21 Mpc (Comoving) Blue●Young Gals Red ●Old Gals Early (massive) galaxy formation preferentially occurs in the region of large-scale density peaks which will evolve to massive clusters. → Cluster galaxies are old → Spatial distribution of high-z galaxies is much inhomogeneous than that of mass. B&W:mass (CDM) Galaxy Formation occurs in the ‘Biased’ manner due to the collapse of ‘high peak’ of CDM fluctuation and some local physical processes (Feedback; UV/Xray heating, Super-galactic wind). Joerg Colberg and Antonaldo Diaferio http://www.mpa-garching.mpg.de/GIF/ (1999)
z=3 simulation at larger scale (Benson et al. 2001) 141 h-1 Mpc N-body + semi-analytic treatment B&W :CDMColord: Galaxies
Strong clustering of high-z Star-Forming galaxies = bias to the mass (Steidel et al. 1998. Adelberger et al. 1999) Two-Point Correlation Function of ~6000 z~4 ‘B-drop’ Lyman Break Galaxies In the Subaru SXDS Field galaxies mass bias at high-z large scale (~10 Mpc), bias is likely to be treated as ‘linear bias’,σg=bσ
Deep Imaging of High-z Universe Pencil-Beam Surveys are not sufficient. Panoramic Surveys over large comoving volume are needed. Whole picture of structure formation Events with shorter time scale (e.g., QSO) Rare objects + High Statistical Accuracy
3’ ACS F435W (B) F606W (V) F775W (I) F840LP (z) Deepest Image of the Universe we have: Hubble Ultra Deep Field (2004)
Size of HUDF 3 arcmin x 3 arcmin … 9 arcmin2 Vcomoving (z < 1) ~ 1 x 104 Mpc3(Ω0=0.3:ΩΛ=0.7: H0=70 km/s/Mpc) Vcomoving (z < 2) ~ 4 x 104 Mpc3 Local Universe φ* = 5 x 10-3 Mpc-3 (SDSS, r*) If uniform, ~200 L* or brighter galaxies at z~2 /unit redshift Physical dimension~ 1 - 1.5 Mpc (Just twice of the distance between M31 andMW ) M31 d=0.7 Mpc
Subaru/XMM-Newton Deep Survey (SXDS) Galaxy evolution can be studied in sufficiently large volume. 1.2 deg2 Optical (Subaru) X-ray (XMM-Newton) HUDF SXDS is observed in NIR (UKIDSS UDS), radio (VLA), sub-mm (SHADES), etc.
z~1 Evolved Quiescent Galaxies Old Passively-Evolving Galaxies (OPEGs) zf=2-10 3900 OPEGs selected Ri’z’ colors to z’=25
Z>4 Lyman Beake Galaxies Dark Matter Halo z=4 gas 1 < z < 4 OPEGs z=1 ダークマターハロー
Strong clustering of high-z Star-Forming galaxies = bias to the mass (Steidel et al. 1998. Adelberger et al. 1999) Two-Point Correlation Function of ~6000 z~4 ‘B-drop’ Lyman Break Galaxies In the Subaru SXDS Field galaxies mass bias Preliminary results at high-z large scale (~10 Mpc), bias is likely to be treated as ‘linear bias’,σg=bσ
Hamana, TY, et al. Halo Occupation Model bias < Host Mass > Galaxy Density Halo Occupation Number
Our Results Preliminary results Solid line: Halo mass growth curve In CDM Dashed lines:68% interval z~4 LBGs z~1 OPEGs Average host halo mass of galaxies obtained from their clustering properties
Narrow-band imaging (Steidel et al. 2000) SSA22 Proto-cluster at z=3.1 Discovery of the SSA22 proto-cluster of Lyman Break Galaxies at z=3.1 (Steidel et al. 1998)
Extended LyαEmitters: Lyα Blobs (LABs) • Giant LyαEmission-Line Nebulae > 100 kpc (physical scale) (Steidel et al. 1998, Keel et al. 1999) • Internal velocity structure Δv>1000 km/s (Ohyama et al. 2004, Bower et al. 2004) • Not enough UV by the apparent SFR • 4 previous examples of LAB with > 100 kpc at z=2~3 are all in the high density regions of LAE LAB1 LAB2 LABs are mysterious objects… How frequent are they? How they related with galaxy-formation phenomena?
Subaru Narrow-Band Observation of the SSA22 Proto-cluster region Lyα Emitters (LA) • 2 x 10-17erg/s/cm2 • EWobs> 160 Å • 283個 HDR Lyα absorbers Hayashino et al. 2004 LAE average local density Steidel et al. 2000
LAE survey: extension to the North-West area SSA22-Sb2 (2004年8月) 50 Mpc (comoving) • 2 x 10-17erg/s/cm2 • EWobs> 120 Å • Sb1+Sb2 ~600 個 SSA22-Sb1 (Hayashino et al. 2004) HDR (LAE NB497 < 26.0 EW > 120Å)
sub-mm / CO source Subaru 7h image of LAB1 25” = 190 kpc How ordinary these gigantic LABs are ? What are their size, luminosity, and spatial distribution? z=3.1 LBG Lyα image (after continuum subtraction) (before subtraction) Cont. subtracted image B, V, NB. Lyα= green
Lyα Excess LAB: origins of the Lyα (1) Photoionization by massive stars or by AGN (in some cases … may be hidden by dust) by diffuse background UV ? (2) Atomic cooling radiation (early phase of galaxy formation) (3) Superwind (late phase of intense star formation) Plus, scattering.. Lyαexcess is seen for 14/35 objects (in the apparent flux)
53W002 No.18 LAB … Keel et al. (1999) 10” Detected in Sub-mm observation (Smail et al. 2003) Lyα+cont Lyα SCUBA Source SMM 02399-0136 (z=2.8) Slit direction LyαHalo NV LABs in Matsuda et al. Lyα wavelength
LABs in the new survey field A New Gigantic LAB with > 100 kpc in SSA22-Sb2 fielfd, which is comparable with LAB1, LAB2 in the SSA22-Sb1 field 2005/08 3D spextroscopy with VLT VIMOS Matsuda et al. 25”=190 kpc