The VLA CO Luminosity Density at High Redshift (COLDz) Survey

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The VLA CO Luminosity Density at High Redshift (COLDz) Survey Dominik A. Riechers Cornell University Developing the ngvla Science Program Workshop June 28, 2017 with the COLDz Survey Team: R. Pavesi (PhD), C. Sharon, F. Walter, C. Carilli, J. Hodge, M. Aravena, R. Decarli, P. Capak, E. da Cunha, E. Daddi, M. Dickinson, R. Ivison, M. Sargent, N. Scoville, I. Smail, V. Smolcic

à What is the cause for this evolution?

Simplest Version of Star Formation Law : Spatially Integrated Observables log LFIR ~ proxy for SFR starbursts main sequence MS galaxies L CO vs. L FIR as a surrogate for M gas vs. SFR One super-linear relation or Two sequences (quiescent/starburst) Bimodal or running conversion factor many subtleties, but: High-z galaxies higher on both axes Quiescent and Starburst Galaxies log L CO ~ proxy for M(H2) Carilli & Walter 2013 ARAA; after Daddi et al. 2010, Genzel et al. 2010

cold gas history of the universe W SFR W M(gas) connection: star formation law (M gas vs. SF rate) Star formation law: SF history of the universe is a reflection of the cold gas history of the universe (gas supply) Ø Studies of galaxy evolution are shifting focus to cold gas (source vs. sink) Problem: populations at high-z so far are highly selected (IR, radio, UV/optical luminosity) Ø may miss cold gas rich, quiescent galaxy populations solution: unbiased census of molecular gas, the fuel for star formation i.e. a molecular deep field (at the same time: continuum deep field)

CO deep field surveys 1) PdBI Survey in Hubble Deep Field North (PI: Walter) -79-115 GHz (3mm), 180hr, ~0.6 arcmin2 -CO 1-0 @ z=0.0-0.4 & CO J=2-5 @ z=1.0-6.2 -L CO > 8 x 109 K km/s pc2 2) VLA Survey in COSMOS & GOODS-North (PI: Riechers) -30-39 GHz (9mm), 320hr (main survey), ~60 arcmin2 -CO 1-0 @ z=1.9-2.8 & CO 2-1 @ z=4.9-6.7 -L CO > 5 x 109 K km/s pc2 (deep) -L CO > 1.5 x 1010 K km/s pc2 (wide) COLDz 3) ALMA Survey in Hubble Ultra Deep Field (PIs: Walter & Aravena) -84-115 GHz (3mm) & 212-272 GHz (1mm), 40hr, ~1 arcmin2 -CO 1-0 @ z=0.0-0.4 & CO J=2-5 @ z=0.0-5.8 -L CO > 3 x 109 K km/s pc2 -[CII] @ z=6.0-8.0 ASPECS-Pilot

COLDz Molecular Deep Field: A Jansky VLA Large Program CO luminosity function is only measured well at z=0 to date. Ø Require very deep, wide-band line survey over substantial cosmic volume to measure CO luminosity function at high redshift Ø CO à H 2 mass: Obtain Cold Gas History of the Universe CO excitation uncertain (e.g., factor 3-8 variation for CO J=3-2): à observe CO J=1-0 Only possible with the fully upgraded Karl G. Jansky VLA Ø VLA Large Program (PI: Riechers) R. Pavesi, PhD Thesis project

Pavesi, Riechers et al. 2017 COSMOS Deep 7-pnt continuum 1.3 µjy/bm rms @35 GHz COSMOS/AzTEC-3 Protocluster Region optical image 19 microjy 9 arcmin2 ( HDF-size field) GOODS-N/CANDELS Wide 56-pnt ~51 arcmin2 continuum 4.5 µjy/bm rms @34 GHz PdBI Hubble Deep Field CO Survey (to scale) ~0.6 arcmin2 @3mm

Pavesi, Riechers et al. 2017 COSMOS/Deep GOODS-N/Wide Ka band One single 8 GHz wide frequency setup covers: CO(1-0) @ z=1.9-2.8 à >50,000 Mpc3 CO(2-1) @ z=4.9-6.7 à >320,000 Mpc3

Pavesi, Riechers et al. 2017 COSMOS/Deep GOODS-N/Wide Approx. flat noise across bandpass (slight increase at sub-band edges) - GN6: deeper; contains original PdBI HDF pointing - GN43-56: observed with upgraded 3-bit samplers

Pavesi, Riechers et al. 2017 COSMOS/Deep CO(J=1-0) CO(J=2-1) GOODS-N/Wide 5s limits Approx. flat noise across bandpass à Resulting in approx. constant CO luminosity limits

Molecular Deep Field: CO Luminosity Function PdBI HDF ALMA ASPECS-Pilot Riechers et al. 2017a

Molecular Deep Field: Comparison to Models/Simulations All models/simulations underpredict SFR in galaxies at z~1-2 à Part of the same problem? compilation from Somerville & Dave 2015

VLA COLDz: Pathfinder for ngvla Science US 2020 Decadal Survey Study: - 10x eff. resolution & collecting area of VLA - 1-115 GHz; multiple times VLA bandwidth à The ideal cosmic CO survey machine! ALMA B1

n COLDz: cosmic H 2 mass density ( cause of SFR density) needs direct molecular gas selection to be unbiased COLDz: VLA directly measures CO(J=1-0) at z=2-3 now can measure CO luminosity function out to at least z~3 high gas fractions at high-z responsible for increase in SFR density n COLDz sources: 54 CO candidates, 7 now confirmed in other CO lines 3 CO(J=2-1) detections in z>5 dusty starburst: high space density! 3.7s stacked detection of optical spec-z sources: below survey limit To date tightest constraints on CO in normal z>5 galaxies n COLDz synergies with ngvla: ngvla: US Astro 2020 study for next large radio observatory VLA & ALMA deep field surveys are a pathfinder for the ngvla