Star formation and metal enrichment at z~1-2: First multi-object near-infrared spectroscopy with large telescopes and the future with FMOS Andy Bunker.

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Presentation transcript:

Star formation and metal enrichment at z~1-2: First multi-object near-infrared spectroscopy with large telescopes and the future with FMOS Andy Bunker (Oxford)

Big Questions 1) What is the history for star formation - i.e. how rapidly is the Universe converting its gas into stars, and how does this evolve with time? 2) How is this star formation divided up among galaxies of different masses/environments as a function of cosmic time (“downsizing” etc). 3) Is the measured stellar mass density consistent with the integrated past cosmic star formation rate? 4) As heavy elements are made in stars, how does the metal enrichment of the gas & stars proceed?

Background Key problem in observational cosmology: At what epoch did majority of stars form? Star formation rate (SFR) higher in recent past, peaks around z=1-2? Large discrepancies between SFR estimates obtained from different methods Different indicators have uncertain relative calibration and are differently affected by dust extinction * A key

The Star Formation History of the Univese Madau/Lilly diagram

Madau-Lilly diagram ( from Hopkins et al. 2001) Factor of 10 uncertainty at z~1 in star formation history of Universe Madau-Lilly diagram ( from Hopkins et al. 2001)

Ha as an SFR indicator Ha luminosity proportional to ionising flux from massive stars (instantaneous SFR) Relatively immune to metallicity effects Less susceptible to extinction than rest-UV tracing Ha to early epochs forces a move to NIR at z>0.6

Ha in the Infrared Previous Ha spectroscopy in NIR restricted to small samples - long-slit spectroscopy ( inefficient for surveys in terms of telescope time) - e.g. Glazebrook et al. (1999), Tresse et al. (2002) @z~1 , Erb et al. (2003) @z~2 Need a large sample (several hundred to a few thousand!) to address the issue properly. Spectroscopy is key Narrow-band searches, after years of trying (e.g. Bunker et al 1995) finally delivering a few hundred candidates (Geach et al. 2009, Villar et al 2008)

Cambridge InfraRed Panoramic Survey Spectrograph A near infrared fibre-fed spectrograph - prelude to FMOS Built by the IoA with support of Sackler foundation & PPARC Two modes - Integral Field with 490 elements (commissioned Aug ‘02) -Multi-object mode, 150 fibres (commissioned October ‘02) Operates between 0.9-1.67 micron. Can survey galaxies over 40arcmin (AAT) or 17arcmin (WHT) resolving power R~3000-5000, great sensitivity between skylines

Instrument cryostat on dome floor PhD of Michelle Doherty, IoA Cambridge (now ESO) Collaborators: Andy Bunker, Rob Sharp (AAO), Ian Parry, Dave King (IoA), & Gavin Dalton, Ian Lewis, Emily MacDonald, Chris Wolf (Oxford), Hans Hippelein (MPIA) Instrument cryostat on dome floor

Sky "glow" in the near-IR

"Beam switching" between pairs of fibres "Beam switching" between pairs of fibres. Sky lines burn only ~10% - no need for OH suppression at R~5000

Human fibre positioners with CIRPASS 2dF robot fibre positioner on AAT

Star Formation History Currently, different redshift bins use different indicators of star formation rate Uncertain relative calibration & susceptibility to dust At high-redshift, mostly relying on rest-UV By using IR spectrographs, can trace same reliable rest- optical tracers (Hb, Ha etc.) over most of time Until recently, no multi-object capability, until CIRPASS Demonstrated on AAT & WHT with a few galaxies Want many thousand, and go fainter (FMOS/Subaru)

Ha Survey with FMOS huge multiplex advantage over any other IR spectrograph, making it ideal for surveys use the same robust star formation tracers used locally (e.g. Ha) at z>1 to study history of star formation. Pilot study with CIRPASS-MOS. Surveyed~200 galaxies at 0.7<z<1.5

Doherty, Bunker, Sharp et al. MNRAS 2004 354, L7 HDF-N galaxies, observed in Ha with CIRPASS on WHT Doherty, Bunker, Sharp et al. MNRAS 2004 354, L7

Hubble Deep Field North Limiting flux 1.0×10-16erg s-1 cm-2 with CIRPASS-MOS 5 in 3 hours = 5 Msun /yr (M=0.3, =0.7, Ho=70km/s/Mpc) Compare Ha to SFR from UV flux => photometry from GOODS HST/ACS images, B band (4500Å) is rest-frame UV at this redshift Find SFRHa/SFRUV ratio of 2-3, consistent with results found by Glazebrook et al., Tresse et al., at similar z

Stack of HDFN Spectroscopic samples, complete to a mag limit (I~24m) - redshifts known from optical, want true star formation rates: can stack H lines (use e.g. Hubble Deep) & photometric redshifts (e.g. Oxford ODT survey, GOODS) to preselect galaxies with H in near-IR. Less successful.

Hubble Deep Field North extended compact 1.1arcsec fibres : results heavily seeing dependant affects different morphologies differently

FMOS on Subaru based on CIRPASS design Survey Science We have a spectroscopic sample in HDFN, complete to a mag limit (I~24 mag) - redshifts known from optical, want true star formation rates: can stack Ha lines Next step at z~1-1.5 (H in J & H): move to an 8-m. FMOS on Subaru based on CIRPASS design

Spectra with FMOS on 8-m Subaru; Evolution of Star-formation & Metallicity in the Universe at high Reshift with FMOS Andrew Bunker, Scott Croom, Gavin Dalton, Michelle Doherty, Karl Glazebrook, Rob Kennicutt, Ian Lewis, Ian Parry, Rob Sharp, Chris Wolf et al. [YOUR NAME HERE…] evol SMURF

Emission lines ⇒ Star formation rates, metallicity (oxygen, R23), dust extinction H/H line widths/rot curves ⇒ kinematics/masses

Metallicity Diagnostics “R23” Kewley & Dopita (2002, ApJS, 142, 35)

Why ~>1sq deg? And why >>1000 galaxies? Want not only luminosity function and clustering, but to split galaxies by: (stellar) mass Star formation rate Metallicity Environment Redshift slices To test downsizing, feedback etc Want sufficient numbers, smooth over cosmic variance

Possible survey 10 luminosity bins with 400 galaxies per bin (5% Poisson error) at z=1, and perhaps 100 per bin at z=1.5 (10% error) Two redshift bins, z=1 (J-band), z=1.5 (H-band) 5000 galaxies in all (need multiple high-resolution settings) 30 arcmin field, surveys 30 x 30 Mpc2 and 70 Mpc in redshift space Encompasses 2000 >0.3L* galaxies per field Well-matched to FMOS 400 fibres once crowding accounted for Do 2 repeats on 5 well-separated fields and 2 redshift bins Limiting flux 0.8×10-16erg s-1 cm-2 with FMOS for FWHM~100km/s 5 in 1 hours = 5 Msun /yr (z=1, M=0.3, =0.7, Ho=70km/s/Mpc) Aim for 7×10-16erg s-1 cm-2 with FMOS 5 in 5 hours = 2-4 Msun /yr for z=1-1.5 >100hours, 15+ nights (a useful trial in 4 nights, still world-beating)

Possible Fields Want good multi-waveband imaging (inc HST) Initially test on optical redshifts (e.g. DEEP2) so can do H-alpha “stacking” Extended Groth Strip (AEGIS), GOODS-North & GOODS-South (CDFS) have good spectroscopic redshifts, but smaller than 30arcmin FMOS field (can do “beam-switch”) Mag-limited? Stellar mass selected? (photo-z ultimately?) Narrow-band follow-up? (e.g. UDS)

Conclusions Have performed multi-object, near-infrared spectroscopy of z~1 galaxies in HDFN can detect star formation to 5 solar masses per year (5s in 3 hours) on a 4m telescope We have ~200 galaxies (with at least upper limits to the SFR): already an improvement over previous work BUT: Want several thousand to pin down Ha luminosity function at z~1 . evolSMURF Very feasible with FMOS on subaru Use H-alpha/H-beta for dust, and with [OIII], [OII] and [NII] get metallicity (and weed out the AGN). Determine the mass-metallicity relation. Initally best to target surveys with known redshifts, and determine H-alpha SFR by stacking.

Pushing to Higher Redshifts CIRPASS and FMOS are fibre-fed, do not work well in thermal IR (wavelengths beyond 2microns, K-band) Rules out studying z>1.6 in H => Next step: cold slitmasks rather than fibres, to get K late Sept 2005: used IRIS2 on AAT, 7arcmin field, to observe 100 galaxies in 3 fields at higher redshift

IRIS2 on AAT

Bunker, Sharp & Doherty (in prep)