Conference Summary
Richard Ellis (Caltech)
ITALIA
DEUTSCHLAND
SCHWEIZ
ÖSTERREICH
View from Top Mountain Star
Happiness is an espresso and Jägermeister at the Top Mountain Star…and a redshift 10 galaxy.
Disclaimer
67 talks × 30 slides = 2010 slides
AND 35 posters
All carefully digested, rationalized, inter-compared with results in the literature to give a “lucid, crisp, holistic view of our present understanding of the formation of galaxies…..”
What follows is a brief, personal, selection of key issues
Apologies if your talk/poster (or even entire field!) is not mentioned
Theoretical Progress - I
Support for standard model ΛCDM strengthened (White)
- precision cosmology from CMB
- Cold DM particle vindicated by Lyα forest simulations
- Local Group dwarf discrepancies must relate to baryonic feedback
- Measurement ≠ understanding (DM/DE remain a mystery)
Viel et al (2013)
Zeldovich (1978): “One can be pretty sure that the problem of galaxy formation will be solved in the 1980’s”
Theoretical Progress - II
Numerical simulations incorporating hydrodynamics have as much or more predictive power as semi-analytic models (Schaye, Sparre, Henriques, Popping) matching:
- stellar mass functions; star formation histories; color bimodality
Theoretical Challenges - I
But aren’t there degeneracies in matching integrated properties of galaxies?
Empirical methods for quantifying mass and environmental-dependent processes offer a refreshing complement to detailed simulations (Lilly)
The challenge is to marry the two approaches to agree the details of the physical processes involved
Peng et al 2010, 2011
Theoretical Challenges - II
Understanding the gas-phase metal distribution (that in CGM > galaxies)
Tumlinson et al 2011
COS spectra of 42 galaxies in the vicinity of background QSOs reveals ubiquitous halos of OVI at impact parameters up to 150 kpc
Theoretical Progress
First steps in predicting resolved properties of galaxies with moving mesh AREPO-based simulations (tested against GADGET-based SPH)
Vogelsberger et al 2012, 2013, Torrey et al 2014
Stars
Gas
Metals
Feedback
No feedback
White, Ceverino
Resolved Metal Gradients in Lensed z~2-3 LBGs
HST
The strong magnification for two images of z=2.00 LBG recovers the [O/H] gradient with ~200 pc resolution in the source plane
Outflow properties follow directly from echellette spectroscopy
Jones et al (2010)
AO resolution sans lensing
Abundance Gradients for Larger Samples Coming..
15 systems from catalog of >50 spectroscopically-confirmed examples
Stark et al 2013
Evolution of Cosmic Gas Density
Next observational frontier after SFR and stellar mass histories:
provides SF efficiency (Narayanan, Lagos, Elbaz, Munoz, Hayward, Hodge, Biggs)
Zafar et al 2013
Saintonge et al 2013
Great progress in surveys and resolved data of targeted examples
Big challenges in utilizing observations and interpreting results
conversion from CO to H2, CO excitation (high J to low J)…
HI
H2
The densities of SFR and H2
Lagos et al. (2014)
x20
x8
Difference comes from the contribution from starbursts: they contribute more to the SFR than to H2 (SF more efficient)
Contrasting Star Formation and H2
The densities of SFR and HI
Lagos et al. (2014)
(1) The evolution of total neutral gas: �outflow vs. inflow
(2) The size evolution of galaxies: �gas density
x20
x2
Contrasting Star Formation and HI
No Need For Bimodal XCO?
Narayanan
Modeling gas kinematics/thermal structure, gas-phase metallicity suggests nature is continuous, not bimodal
Continuous XCO improves interpretation of main sequence
First CO Deep Fields
Walter et al 2014, Decarli et al 2014, Chapman..
Narayanan
Consider an input SFH and its implied H2 density as TRUTH, limitations of current methodologies could lead to BIASED MEASURE
Resolving the SMGs
Hayward, Geach, Hodge, Walth, Zavala
SMA (Wang et al 2011) and later ALMA (Karim et al 2013) resolve individual sub-mm galaxies revealing multiple components, often at different redshift.
Typically <65% of the original integrated flux lies in the primary component
ALMA (Karim et al 2013)
SMA (Wang et al 2011)
Correlating FIR emission with LBGs
Geach
Confusion on CII] Detections at High Redshift
The ALMA Story (so far..)
Ouchi, Williams, Munoz
The Most Exciting Development?
Watson
A truly remarkable achievement:
Cosmic Dawn and Reionization
time
baby galaxies
dark hydrogen clouds
ionized gas bubbles
fully ionized gas
Courtesy: Avi Loeb
Huge progress in observations (HST, ground-based spectroscopy) and simulations of first stars and reionization
Bromm, Robertson, McLure, Stark, Ciardi, Ouchi, Dayal, Wilkins
Bromm
Extremely massive (>100 M◉) first stars unlikely
How Did Massive Black Holes in z>6 QSOs Form?
Bromm, Haehnelt
Leo IV abundances c.f. Pop III supernova models
Pop III Phase May Be Very Short-lived
Leo IV star
10 M◉, normal energy
30 M◉, high energy
Simon et al (2011)
Bromm
Progress in Reionization Studies Using 21cm Surveys
Matching simulations with LOFAR, can expect good progress via power spectrum analyses in 7<z<11 shortly
Ciardi, Meisinger, Scobbachi
Lyα visibility decline
Treu et al (2013) – Keck MOSFIRE + BoRG z~8
Finkelstein et al (2013) – Keck MOSFIRE + CANDELS z > 7
Schenker et al (2014) – Keck MOSFIRE + UDF, CLASH 7<z<8.2
Pentericci et al (2014 in prep) – VLT FORS 6<z<7.3
Schenker et al 2014
Konno et al 2014
Stark, Ouchi
~1.5 deg
FoV of HSC
FoV of Suprime
1.7m
Clustering of Lyman α Emitters
The spatial distribution of Lyα emitters over key redshift ranges 5.7, 6.6 and 7.0 contains information on the emerging distribution of ionized bubbles; expect boosting in bias at higher z.
Can explore with Subaru’s unique imager HSC and massive-multiplexed spectrograph PFS
Subaru 8m
HSC corrector
Ouchi et al (2010)
High Redshift Measurements without Lyα?
Spectra of lensed 106-9 M⦿ z~2-3 galaxies with properties similar to those at z~7
CIII] 1909 Å is stronger in such systems (EW~10-30 Å) reflecting larger Te and harder ionizing spectrum expected at low (10% solar) metallicities.
Stark et al (2014a, b)
✖
First Confirmation of z>6 Sources using CIII]
Stark
Hubble WFC3 High z Stampede (2009)
WFC3/IR: 850 - 1170nm
2.1 × 2.3 arcmin field of view
0.13 arcsec pixel-1
10 times survey power of NIC3
UDF 4.7 arcmin2
60 orbits in YJH
Reaches mAB~29 (5σ)
Bouwens et al 0909.1803
Oesch et al 0909.1806
Bunker et al 0909.2255
McLure et al 0909.2437
Bouwens et al 0910.0001
Yan et al 0910.0077
Labbé et al 0910.0838
Bunker et al 0910.1098
Labbé et al 0911.1365
Finkelstein 0912.1338
Progress With Hubble Space Telescope
Ferguson, Robertson, Bouwens, McLure
Ultra Deep Field 2012 (>80 galaxies z>6.5)
Wider Area CANDELS survey
z~7 Luminosity Function (2009)
Ouchi 09 (Subaru)
WFC3 UDF
α = -1.86 ± 0.33 (Oesch)
α = -1.72 ± 0.65 (Ouchi)
NIC UDF
- 10-16 z-band dropouts to YAB~28.5 corresponding to 6.5<z<7.5 - Towards a reliable faint end slope: low star formers ~1 M◉ yr-1 dominant - Abundance decline of ~×2 since z=6
z~7 Luminosity Function (2014)
Bowler
Tail of luminous galaxies detected only in ground-based panoramic surceys (UltraVISTA, UDS) suggests demise of AGN feedback at early times?
Star Formation History
1Byr 800Myr 400Myr 350Myr
UDF12/CANDELS, in agreement with CLASH, smooth decline in SF
history to z~10
Bouwens+(2011), Oesch+(2013) originally claimed a `cliff’ at z~8 but this now seems unlikely
Continuity has important implications for z>10 studies with JWST and models of reionization
Oesch et al 2013
β - wars are over?!
Gonzalez, Smit, Stark, Maseda
Both spectroscopic and ingenious photometric tests confirm increasing nebular emission pollutes broad-band photometry at high z.
Although we can correct this contamination, why are these lines so strong?
Specific Star Formation Rate: Nebular Emission
Bursty Star Formation
Stark
It is not necessary for the nebular contribution to be consistent with the stellar fit to the continuum SED
The Full Monty: Galaxies Ended the Dark Ages
HST star formation
Ionized fraction
Spitzer old stars
WMAP τ
The UDF2012 star formation rate density (N(z) and faint end LF slope) integrates to match the stellar mass density and given ξion ( β) matches the CMB optical depth τ
provided
Robertson et al (2013)
Unique Role of GRBs
Tanvir
GRBs continue to play an independent role in reionization studies:
SF history, HI optical depth etc
Role of Frontier Fields - I
z=5.6
z=6.8
Ellis et al (2001), Kneib et al (2005)
Multiply-imaged sources close to the `critical line’ of maximum magnification offer a number of unique advantages:
But they are RARE because the relevant survey volume is tiny!
Abell 2218
Kawamata
Role of Frontier Fields - II
A singly-imaged source is located in the vicinity of a cluster but away from the critical line. It offers no geometric information. The magnification is less. Such sources are much more common but offer only a modest boosting in flux
Bradley et al arXiv 1308.1692
Abell 1689
z=7.35
Area vs magnification for ~250 lensed sources in 18 CLASH clusters
Accuracy of Magnification Maps (A2744)
Robertson
Cosmic Variance
RMS/mean
For the first Frontier Field cluster, independently submitted magnification maps and the limited survey volume in the source plane allow us to estimate the uncertainties in surveys of faint high redshift galaxies
THE FUTURE (Steve Rawlings 1961-2012)
James Webb ST
ALMA
SKA
LMT
TMT
SVOM
The Era of Extremely Large Telescopes (ca. 2009!)
A new generation of 20-42m ELTs is being designed:
Almost there..ground-breaking Oct 2014
Substantial progress; construction underway
Ground preparation underway, waiting for Brazil
TMT
GMT
E-ELT
Thanks to Conference Organizers!!