Big Bang f(HI) ~ 0 f(HI) ~ 1 f(HI) ~ 10 -5 History of Baryons (mostly hydrogen) Redshift Recombination Reionization z = 1000 (0.4Myr) z = 0 (13.6Gyr) z.

Slides:



Advertisements
Similar presentations
Probing the End of Reionization with High-redshift Quasars Xiaohui Fan University of Arizona Mar 18, 2005, Shanghai Collaborators: Becker, Gunn, Lupton,
Advertisements

The Highest-Redshift Quasars and the End of Cosmic Dark Ages Xiaohui Fan Collaborators: Strauss,Schneider,Richards, Hennawi,Gunn,Becker,White,Rix,Pentericci,
ESO Recent Results on Reionization Chris Carilli (NRAO) Dakota/Berkeley,August 2011 CO intensity mapping during reionization: signal in 3 easy steps Recent.
End of Cosmic Dark Ages: Observational Probes of Reionization History Xiaohui Fan University of Arizona New Views Conference, Dec 12, 2005 Collaborators:
ESO Recent Results on Reionization Chris Carilli (NRAO) LANL Cosmology School, July 2011 Review: constraints on IGM during reionization  CMB large scale.
Molecular Gas, Dense Molecular Gas and the Star Formation Rate in Galaxies (near and far) P. Solomon Molecular Gas Mass as traced by CO emission and the.
Molecular gas in the z~6 quasar host galaxies Ran Wang National Radio Astronomy Observatory Steward Observatory, University of Atrizona Collaborators:
HI Stacking: Past, Present and Future HI Pathfinder Workshop Perth, February 2-4, 2011 Philip Lah.
15 years of science with Chandra– Boston 20141/16 Faint z>4 AGNs in GOODS-S looking for contributors to reionization Giallongo, Grazian, Fiore et al. (Candels.
HI 21cm Signal from Cosmic Reionization IAU 2006, Long Wavelength Astrophysics Chris Carilli (NRAO) Ionized Neutral Reionized.
Dust and Molecules in primordial galaxies F.-Xavier Désert, Lab. Astrophysique, Grenoble Erik Elfgren, Dept. of physics, Lulea, Sweden Early dust in the.
The Dark Age… before the stars, beyond the galaxies…
NEUTRAL HYDROGEN Frank Briggs RSAA and ATNF z = 8 z = 0.
What good are low frequencies? HI, neutral hydrogen, H 0, atomic hydrogen high redshifts and early times…. USS, GPS, … “enabling technologies” …multi-beaming,
Epoch of Reionization Tomography with the CSO Wide-field C+ spectral mapping and correlation with HI Matt Bradford CSO NSF visit: October 12, 2011 CSO.
Star formation at high redshift (2 < z < 7) Methods for deriving star formation rates UV continuum = ionizing photons (dust obscuration?) Ly  = ionizing.
Modeling Cosmic Reionization (Leave No Photon Behind) Nick Gnedin.
Cosmology with the 21 cm Transition Steve Furlanetto Yale University September 25, 2006 Steve Furlanetto Yale University September 25, 2006.
A Primer on SZ Surveys Gil Holder Institute for Advanced Study.
Simona Gallerani Constraining cosmic reionization models with QSOs, GRBs and LAEs observational data In collaboration with: A. Ferrara, X. Fan, T. Choudhury,
Dusty star formation at high redshift Chris Willott, HIA/NRC 1. Introductory cosmology 2. Obscured galaxy formation: the view with current facilities,
Large Scale Simulations of Reionization Garrelt Mellema Stockholm Observatory Collaborators: Ilian Iliev, Paul Shapiro, Marcelo Alvarez, Ue-Li Pen, Hugh.
Matched Filter Search for Ionized Bubbles in 21-cm Maps Kanan K. Datta Dept. of Astronomy Stockholm University Oskar Klein Centre.
Star Formation Research Now & With ALMA Debra Shepherd National Radio Astronomy Observatory ALMA Specifications: Today’s (sub)millimeter interferometers.
Title Here Probing the Epoch of Reionization with the Tomographic Ionized-carbon Mapping Experiment (TIME) Jamie Bock Caltech / JPL CCAT Workshop, Boulder.
ESO Galaxy Formation: The Radio Decade (Dense Gas History of the Universe) Chris Carilli (NRAO) Santa Fe, March 2011 Power of radio astronomy: dust, cool.
130 cMpc ~ 1 o z~ = 7.3 Lidz et al ‘Inverse’ views of evolution of large scale structure during reionization Neutral intergalactic medium via HI.
130 cMpc ~ 1 o z = 7.3 Lidz et al ‘Inverse’ views of evolution of large scale structure during reionization Neutral intergalactic medium via HI 21cm.
Cosmic magnetism ( KSP of the SKA) understand the origin and evolution of magnetism in the Galaxy, extragalactic objects, clusters and inter-galactic/-cluster.
Cosmic Reionization Chris Carilli (M/NRAO) Vatican Summer School June 2014 I. Introduction: Cosmic Reionization  Concept  Cool gas in z > 6 galaxies:
Molecular Gas and Dust in SMGs in COSMOS Left panel is the COSMOS field with overlays of single-dish mm surveys. Right panel is a 0.3 sq degree map at.
ALMA DOES GALAXIES! A User’s Perspective on Early Science Jean Turner UCLA.
The Evolution of Quasars and Massive Black Holes “Quasar Hosts and the Black Hole-Spheroid Connection”: Dunlop 2004 “The Evolution of Quasars”: Osmer 2004.
Large-Scale Winds in Starbursts and AGN David S. Rupke University of Maryland Collaborators: Sylvain Veilleux D. B. Sanders  v = km s -1 Rupke,
Nick Gnedin (Once More About Reionization)
Andrea Ferrara SISSA/International School for Advanced Studies, Trieste Cosmic Dawn and IGM Reionization.
After decoupling, overdense regions collapse IF Collapse timefor all sizes. More small ripples than large waves. --> Universe dominated by globular clusters.
SMA [CII] 158um 334GHz, 20hrs BRI z=4.7 Quasar-SMG pair Both HyLIRG Both detected in CO Iono ea 2007 Omont ea ”4” HST 814 Hu ea 96.
Scaling Relations in HI Selected Star-Forming Galaxies Gerhardt R. Meurer The Johns Hopkins University Gerhardt R. Meurer The Johns Hopkins University.
The Dawn of 21 cm Cosmology with EDGES Judd D. Bowman Caltech Alan E. E. Rogers Haystack Observatory.
Mário Santos1 EoR / 21cm simulations 4 th SKADS Workshop, Lisbon, 2-3 October 2008 Epoch of Reionization / 21cm simulations Mário Santos CENTRA - IST.
Molecular Gas (Excitation) at High Redshift Fabian Walter Max Planck Institute for Astronomy Heidelberg Fabian Walter Max Planck Institute for Astronomy.
The Distributions of Baryons in the Universe and the Warm Hot Intergalactic Medium Baryonic budget at z=0 Overall thermal timeline of baryons from z=1000.
Finding z  6.5 galaxies with HST’s WFC3 and their implication on reionization Mark Richardson.
Simulations of Lyα emission: fluorescence, cooling, galaxies Jordi Miralda Escudé ICREA University of Barcelona, Catalonia Berkeley, Collaborators:
ALMA Science Examples Min S. Yun (UMass/ANASAC). ALMA Science Requirements  High Fidelity Imaging  Precise Imaging at 0.1” Resolution  Routine Sub-mJy.
ALMA and the Formation of Galaxies Pierre Cox IAS, Orsay, France.
Mark Dijkstra, PSU, June 2010 Seeing Through the Trough: Detecting Lyman Alpha from Early Generations of Galaxies ‘ Mark Dijkstra (ITC, Harvard) based.
ALMA: Imaging the cold Universe Great observatories May 2006 C. Carilli (NRAO) National Research Council Canada.
Radio Galaxies Part 3 Gas in Radio galaxies. Why gas in radio galaxies? Merger origin of radio galaxies. Evidence: mainly optical characteristics (tails,
Star Formation in Damped Lyman alpha Systems Art Wolfe Collaborators: J.X. Prochaska, J. C. Howk, E.Gawiser, and K. Nagamine.
C.Carilli, AUI Board October 2006 ISAC-run three year process: Quantified ‘experiments’ for future large area cm telescopes 50 chapters, 90 authors, 25%
Lyman Alpha Spheres from the First Stars observed in 21 cm Xuelei Chen (Beijing) Jordi Miralda Escudé (IEEC, Barcelona).
Radiative Transfer Simulations The Proximity Effect of LBGs: Antonella Maselli, OAArcetri, Firenze, Italy Collaborators: A.Ferrara, M. Bruscoli, S. Marri.
KASI Galaxy Evolution Journal Club A Massive Protocluster of Galaxies at a Redshift of z ~ P. L. Capak et al. 2011, Nature, in press (arXive: )
Warm Dust in the Most Distant Quasars Ran Wang Department of Astronomy, Peking University, China.
What is EVLA? Giant steps to the SKA-high ParameterVLAEVLAFactor Point Source Sensitivity (1- , 12 hr.)10  Jy1  Jy 10 Maximum BW in each polarization0.1.
ESO The other side of galaxy formation: radio line and continuum ‘Great Surveys’ Santa Fe November 2008 Chris Carilli NRAO.
Lyα Forest Simulation and BAO Detection Lin Qiufan Apr.2 nd, 2015.
High Redshift Galaxies/Galaxy Surveys ALMA Community Day April 18, 2011 Neal A. Miller University of Maryland.
History of IGM bench-mark in cosmic structure formation indicating the first luminous structures Epoch of Reionization (EoR) C.Carilli (NRAO) NNIW Dec.
The cross-correlation between CMB and 21-cm fluctuations during the epoch of reionization Hiroyuki Tashiro N. Aghanim (IAS, Paris-sud Univ.) M. Langer.
High Redshift QUASAR Spectra as Probe of Reionization of IGM.
Proximity Effect Around High-redshift Galaxies
Nithyanandan Thyagarajan1, Aaron R. Parsons2,
ALMA studies of the first galaxies
What is EVLA? Build on existing infrastructure, replace all electronics (correlator, Rx, IF, M/C) => multiply ten-fold the VLA’s observational capabilities.
HI 21cm Tomography of IGM: freq ~ 100 to 200 MHz
Dense gas history of the Universe  Tracing the fuel for galaxy formation over cosmic time SF Law SFR Millennium Simulations, Obreschkow & Rawlings 2009;
Recovery of The Signal from the Epoch of Reionization
Presentation transcript:

Big Bang f(HI) ~ 0 f(HI) ~ 1 f(HI) ~ History of Baryons (mostly hydrogen) Redshift Recombination Reionization z = 1000 (0.4Myr) z = 0 (13.6Gyr) z ~ 7 to 15 (0.8Gyr) Reionization: Last phase of cosmic evolution to explore Bench-mark in cosmic structure formation indicating the formation of the first galaxies

130 cMpc ~ 1 o z~ = 7.3 Lidz et al ‘Inverse’ views of evolution of large scale structure during reionization Neutral intergalactic medium via HI 21cm line observations = consequence Galaxies which drive reionization = sources 20mK

Inverse Views of the Universe: Neutral IGM vs. galaxies Power  Complete view of physics: sources of reionization and their impact on the IGM  Cross correlation of HI 21cm signal with galaxy distribution mitigates large (but independent) systematic errors (eg. foregrounds) in each measurement Challenge: Problematic to match very (very) large scale of HI measurements with classical galaxy surveys  HI 21cm experiments cover 100 to 1000 deg 2 and z range ~ 6 to 10  Galaxy surveys by eg. JWST/ALMA have FoV ~ arcmin, dz < 0.5 Solution: Intensity mapping of the aggregate CO emission from the galaxies that reionize the Universe

Intensity mapping: image summed signal from aggregates of thousands of galaxies on Mpc scales (tens of arcmin). No need to detect each galaxy individually.

CO intensity mapping: predicted mean brightness temperature in 3 simple steps (Carilli 2011) 1. Cosmic star formation rate density required to reionize the IGM using mean baryon density (Haardt & Madau, Bunker et al.)  f esc uv = ionizing photon escape fraction ~ 0.06 (MW), up to 0.2 for z~3 LBGs  C = IGM clumping factor (recombinations) = 5 to 30 (simulations)  Strong increase with z due to increase in mean cosmic baryon density 2. Conversion of star formation rate to IR luminosity based on known properties of galaxies (eg. Kennicutt 1998 and many others)

Predicted Mean CO Brightness Temperature 3. Conversion of IR luminosity to CO luminosity based on known properties of galaxies (Daddi et al. 2010)  Roughly linear relationship between L’ CO and L FIR for disk galaxies at low and high z  Similar slope for merger driven starbursts, with different normalization  Disks likely dominate cosmic star formation rate density

Doing some cosmic algebra => mean brightness temperature of CO emission from the galaxies that reionize the neutral IGM at a given redshift [Not what we expect to see at all redshifts, but what is required to have reionization occur at that redshift.] z=8 = 1.1 (0.1/f esc ) -1 (C/5) uK (1+z) 3

Major uncertainties: f esc – calibrated with JWST observations of 1 st galaxies C – get handle via HI 21m observations (21cm forest absorption?) Line confusion (30GHz = CO 2-1 z=6.7 or 1-0 at z=2.8): requires dual frequency, cross correlation experiment (eg. 15 and 30GHz). Cross correlation with 21cm will also help (Gong, Visbal) Early production of CO and dust (SFR – FIR – L’CO relationships)

z= km/s +150 km/s 7kpc 1” ~ 5.5kpc CO3-2 VLA ” T B ~ 25K PdBI Early production of dust + CO: detections of 8 quasar host galaxies at z~6 M(dust) ~ 10 8 M o, M(H 2 ) ~ M o SFR – FIR – L’ CO relationships can be calibrated with ALMA/EVLA/JWST observations of representative z>6 galaxy samples.

Gong et al.: numerical prediction of T B Obreschkow & Rawlings CO galaxy catalog based on Millenium simulations z=7 = 0.1 and 0.7uK Fluctuations on 10’ scales are factor few smaller CO auto-power spectrum can be detected at 40σ CO-HI cross power spectrum: errors dominated by HI measurements! CO auto HI-CO cross 7’

COIM: Experimental specs (to match HI 21cm) Observing frequencies: 10 to 45 GHz, BW > 1GHz 0.1 to 1 uK sensitivity Angular resolution ~ 1’ to 10’ spectral resolution ~ 100MHz ~ 1500 km/s FoV > 25 deg 2 (LOFAR) Gong experimental parameters: 1000 elements of 0.7m diameter (area = 385m 2 ; element FoV = 2 o ) BW = 1 GHz, channel = 30MHz Interferometer spacings from 0.7m to 25m (resolution ~ 3’) 20K system at 15 GHz 3000hrs (mosaic?)

END

L FIR vs L’(CO): Star Formation Law Index=1.5 1e11 M o 1e3 M o /yr Further circumstantial evidence for star formation Star formation efficiency (FIR/L’CO) increases with SFR => Gas consumption time (M gas /SFR) decreases with SFR FIR ~ L o /yr => t c > 10 8 yr FIR ~ L o /yr => t c < 10 7 yr SFR M gas MW