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Binary Quasars in the Sloan Digital Sky Survey Joseph F. Hennawi Berkeley Hubble Symposium April 7, 2005.

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Presentation on theme: "Binary Quasars in the Sloan Digital Sky Survey Joseph F. Hennawi Berkeley Hubble Symposium April 7, 2005."— Presentation transcript:

1 Binary Quasars in the Sloan Digital Sky Survey Joseph F. Hennawi Berkeley Hubble Symposium April 7, 2005

2 Suspects Naohisa Inada (Tokyo) Masamune Oguri (Princeton) Michael Strauss (Princeton) Gordon Richards (Princeton)

3 Conclusions New sample of 26 binary quasars with separations R < 50 kpc/h more than doubles the number known First measurement of quasar clustering on small scales 10 kpc/h < R < 400 kpc/h (proper) The quasar correlation function gets progressively steeper on sub-Mpc scales Factor of 10-30 excess clustering is detected on scales < 40 kpc/h over extrapolation of large scale power law Is excess clustering the hallmark of mergers and dissipative interactions which trigger quasar activity in rich environments?

4 An Old Problem: Excess Close Pairs Djorgovski (1991) Djorgovski realized that 3 close pairs in sample ~ 3000, implies a pair probability P(R< 200 kpc/h) ~ 10 -3 Binary Quasar Lore –tides/mergers galaxy activated –large R ~ 100 kpc/h no tides –small R ~ 10 kpc/h t DF < t H P(<R) Probability of Having a Companion R [kpc/h] Comoving Transverse Separation Could these be strong lenses? –No corresponding radio population –Requires dark/exotic mass concentration –“We don’t expect splittings this large....”

5 Small Scale Quasar Clustering Fiber Collisions: Optical fibers can only be packed so tightly –For 2dF: No pairs with  < 35” –For SDSS: No pairs with  < 55” Shot Noise –Volume decreases faster than the correlation function increases Proper Mpc/h 0.4 10 1 440 Comoving Mpc/h Solutions 1. Wait for next generation all sky (i < 21) spectroscopic survey of ~ 10 6 quasars –Several years of observing –Need $$ + huge consortium of people n = 35 deg -2 2. Target only ~ 200 close pairs (i < 21) –Use LF to get mean density –Less than 20 nights of observing –Sucker in one graduate student 2dF: Croom et al. (2005)

6 Why Observe at Princeton? Apache Point Observatory (APO) SDSS spectroscopic survey –4000 deg 2 –45,000 low -z quasars i < 19.1 –5,000 z > 3 quasars i < 20.2 –Precise 5 band (u,g,r, i, z) photometry SDSS 2.5m ARC 3.5m ARC 3.5m telescope –Plenty of time available in a department full of theorists –Remote operation from comfort of basement of Peyton Hall –There was little else to do at night in Princeton Jim Gunn

7 3.0 3.3 3.5 4.0 4.5 5.0 low-z qsos A-stars UVX WD 2’ 55” Excluded Area Finding Quasar Pairs  = 14.7” Keck Spectrum taken by Bob Becker & Michael Gregg SDSS quasar @ z =2.17

8 Binary Quasars in the SDSS Statistical Clustering Sample –Subset of full sample with quantifiable selection criteria –38 binaries below fiber collision limit (  < 55”; R< 400 kpc/h) Full Binary Sample Statistical Clustering Sample Pairs found from SDSS Sparse sampling of this region Dense sampling of this region Fiber collision (  = 55”) Barely Resolved (  = 3”) Full Binary Sample –26 new binaries with R < 50 kpc/h (  < 10”) –More than doubles the number of such systems known!

9 Excess Small Scale Clustering Factor ~ 10 excess for R < 40 kpc/h. Rises to ~ 30 for R ~ 10 kpc/h Quasar correlation function progressively steepens for R < 1 Mpc/h Is excess clustering the hallmark of mergers and dissipative interactions? High redshift galaxies (z = 1- 3) show no excess clustering, but measurements don’t yet probe R < 100 kpc/h Hennawi et al. (2005) Projected Correlation Function Extrapolation of larger scale 2dF clustering Ratio of Observed/Extrapolated Uncertain selection function for smallest angles Fiber Collision

10 Future Directions Use photometric selection to measure clustering with better statistics Push to high redshift binary quasars at z > 4 Deep imaging to study the environments of these systems. Proto-clusters at z ~ 2? Measure transverse small scale Ly  forest correlations with quasar pairs with z > 2

11 Excess Galaxy Clustering? Low-z galaxies lie on a single power law down to 10 kpc/h (comoving) High redshift (DEEP2, LBGs) clustering does not probe < 100 kpc/h Quasar-Galaxy correlations do not yet probe relevant scales or redshifts SDSS Galaxies z ~ 0.1 Coil et al. (2004) DEEP2 Galaxies z = 0.7-1.35 Masjedi et al. in prep LBGs at z ~ 3 Adelberger (2003)

12 A B C D G1 Inada et al. (2003) Oguri et al. (2004) Inada et al. (2005) z=1.734 The Widest Lensed Quasar Largest Splitting  = 14.6”! HST ACS HST NICMOS SDSS spectroscopic survey –4000 deg 2 –45,000 low -z quasars i < 19.1 –5,000 z > 3 quasars i < 20.2 –Precise 5 band (u,g,r, i, z) photometry

13 SDSS Spectroscopic Quasars SDSS Photometric Quasars Predict ~ 2 lenses with  > 10” in current (~ 4000 deg 2 ) sample Consistent with discovery of quad lens SDSS 1004+4112 How Many Quasars Lensed by Clusters? Predict ~ 8 lenses with  > 10” in current (~ 7000 deg 2 ) sample ~ 1 should have  > 30” ~ 1 will have z s ~ 4 Hennawi, Dalal, & Bode (2005) From Ray Tracing Simulations through LCDM clusters


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