Molecular Gas and the Host Galaxies of Infrared-Excess Quasi-Stellar Objects

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Molecular Gas and the Host Galaxies of Infrared-Excess Quasi-Stellar Objects A. S. Evans (Stony Brook) J. A. Surace & D. T. Frayer (Caltech) D. B. Sanders (Hawaii)

Luminous Infrared Galaxies Properties 1. Infrared Excess Infrared Optical (Sanders & Mirabel 1996)

2. Galaxy Mergers with Starburst Activity HST NICMOS HST NICMOS VV 114 (e.g. Scoville et al. 2000)

Simulations of Merging Disk Galaxies Double Nuclei Tidal Features Evolution Toward Galaxies with Elliptical Profiles (e.g. Toomre & Toomre 1972; Barnes & Hernquist 1996; Mihos & Hernquist 1996)

3. Significant Quantities of Star-Forming Molecular Gas 3mm CO(1-0) Emission Line: Collisionally excited by H 2 Few x 10 9-10 M sun of Gas Star-formation Rates = 100s M sun / year Depletion Time = 10 7-8 years (e.g. Sanders, Scoville, & Soifer 1991 Evans, Surace, & Mazzarella 2000; Evans et al. 2002)

4. Increase in AGN Fraction with Increasing Infrared Luminosity (Veilleux et al 1995; Veilleux, Sanders, & Kim 1998)

5. Luminosity Function at High End Similar to QSOs Ultra luminous Infrared Galaxies (ULIGs: L IR [8-1000µm] >~ 10 12 L sun ) (Soifer et al. 1987; Kim & Sanders 1998)

Properties of Nearby QSOs (1988) (e.g. Stockton & MacKenty 1984) (Sanders et al. 1989) (Sanders, Scoville, Soifer 1988)

Dust-Enshrouded Quasar Model: QSOs are the/an Evolutionary By-product of the Ultraluminous Infrared Galaxy Phenomenon Similarities in Luminosity Function Distorted Stellar Morphologies and Large Amounts of Molecular Gas Increased AGN Fraction with Increasing Infrared Luminosity (Sanders et al. 1988)

Possible Evolutionary Sequence Infrared Cool ULIGs (f 25 /f 60 <0.2) Warm ULIGs (f 25 /f 60 > 0.2) UV-Excess QSOs Progression Optical (Sanders et al. 1988)

Warm ULIGs have Bright, Compact Nuclei (Scoville et al. 2000)

Infrared Galaxies at High Redshift Space Density of Infrared Galaxies Higher in the Past Based on SCUBA and ISO Observations SCUBA HDF (Hughes et al. 1998)

Relationship Between Black Hole Mass and Bulge Mass I.e., Black Hole Creation is a Standard Part of Galaxy Formation (e.g. Kormendy & Richstone 1995; Magorrian et al. 1998)

Comparison of LIG-QSO Datasets Observation Type Optical/NIR Imaging Optical/IR Spectroscopy FIR Photometry CO Spectroscopy X-ray, etc Importance L IR (ca. 1998) Galaxy Type/ Age-Dating Ionization Mechanism Fuel for Star Formation and AGN? Local LIGs Lots Lots Lots Lots (i.e. Single Dish) Local QSOs Substantial (AO, HST) N/A Lots Several

CO(1-0) Observations of QSOs Possible Evolutionary Connection with ULIGs Molecular Gas is a Possible Fuel Source for AGN Activity Molecular Gas Present if Stars and Black Hole are Co- evolving (Evans et al. 2001)

An Infrared-Excess Sample - Palomar-Green Quasar Survey L IR / L bbb (0.1-1.0 1.0 µm) > 0.36 Redshift,, z < 0.17 M B < -22.0 17 QSOs Total, 10 Observed in CO(1-0) thus Far Note: For PG QSOs, L IR = 0.2 0.4 L bol

Millimeter (CO) Observations Two Transits/Source Beam Size = 4 Detection Limit of S CO (3σ rms) ) = 8 mjy with 280 km/s Smoothing I.e., M(H 2 ) = 10 9 M sun at z = 0.1 Owens Valley Millimeter Array (α = 4 M sun [Km/s/pc 2 ] 1 )

Previous Detections with Single Dish Telescopes (mostly( mostly) (Sanders et al. 1988; Barvainis et al. 1989; Alloin et al. 1992; Solomon et al. 1997; Schinnerer et al. 1998)

CO Spectra of IR-Excess QSOs v FWHM = 50-500 km/s

Synthesized CO(1-0) Maps Contours = 1σ1 steps Detections = 4.6-8.6σ

Log (L CO) ) vs. Redshift Scatter in L CO Gas Mass > 10 9 M sun

Log (L ) IR vs. Log (L CO CO) I.e., Dust Heating vs. Fuel Reservoir

Star Formation Efficiency or Significant Heating by AGN?

Can the QSOs Account for most/all of the Bolometric Luminosity? PG QSO PG 1226+023 PG 1351+640 PG 1411+442 PG 1613+658 PG 2130+099 M 5x10 8 5x10 7 8x10 7 2x10 8 1x10 8 L bol /L eddington 0.12 0.16 0.04 0.02 0.02 From Reverberation Mapping (Kaspi et al. 2000) Answer: Yes.

If L = L for IR bol QSOs Regions Occupied by Dust-Enshrouded Quasars?

Optical/Near-Infrared Imaging UH 2.2m B, I, H, K-Band K Filters Total Integration Times = 9-549 minutes Typical Seeing: I= 0.4-0.9, 0.9, K=0.25-0.5 0.5 (Surace, Sanders, & Evans 2001)

Diverse Morphology Half are in spiral galaxies. And half of those are barred.

Diverse Morphology A quarter are in major merger systems as evidenced by tidal tails 20-80 kpc in length. A few are extended but don t look like anything. They have no resolvable structure, and could be ellipticals or unresolved spirals. Radial profiles do not produce very meaningful results due to convolution effects with PSF.

Small-Scale Scale Structure In some cases there is resolvable small scale structure similar to the star-forming knots found in ULIRG nuclear regions and tidal structure. In most cases the ages of these knots are probably under 100 Myrs based on 4-color analysis and spectral synthesis models.

Optical Imaging of QSOs IR-Excess QSOs Have Spiral, Merger, and Elliptical Galaxy Hosts 25% - Ongoing Major Mergers

Improvements to CO Work Larger QSO Samples Higher Resolution Observations CO Extent, Column Density Other CO Transitions Density, Temperature HCN Dense Gas (10 5 cm -3 ) Similar Observations of Luminous Infrared Galaxies as a Function of Evolutionary State

Improvements: A Sample of Intermediate Stage ULIGs: Projected Nuclear Separation = 2 5 kpc.

Improvements to Imaging Work 2MASS QSOs (Hines et al. 2002)

Summary Six out of Nine QSOs Detected in CO(1-0) with Molecular Gas Mass > 10 9 M sun High L IR / L CO of QSOs is Indicative of Dust Heating by an AGN and/or Massive Stars (I.e., High Star Formation Efficiency) IR-Excess QSOs have Host Galaxies Which are Spirals, Mergers, and Elliptical Galaxies