IFU observations of the high-z Universe Constraints on feedback from deep field observations with SAURON and VIMOS Joris Gerssen.

Slides:



Advertisements
Similar presentations
The Highest-Redshift Quasars and the End of Cosmic Dark Ages Xiaohui Fan Collaborators: Strauss,Schneider,Richards, Hennawi,Gunn,Becker,White,Rix,Pentericci,
Advertisements

Lyman-α Galaxies at High Redshift James E. Rhoads (Space Telescope Science Institute) with Sangeeta Malhotra, Steve Dawson, Arjun Dey, Buell Jannuzi, Emily.
Digging into the past: Galaxies at redshift z=10 Ioana Duţan.
Integral Field Spectroscopy on Gemini Andrew Bunker (IoA, Cambridge) Euro3D Meeting July 2002 GMOS Gemini Multi-Object Spectrograph, optical IFU (Durham)
Padova 03 3D Spectrography 3D Spectrography IV – The search for supermassive black holes.
Molecular gas in the z~6 quasar host galaxies Ran Wang National Radio Astronomy Observatory Steward Observatory, University of Atrizona Collaborators:
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.
With a wide-field multi-IFU spectrograph.  Clusters provide large samples of galaxies in a moderate field  Unique perspective on the interaction of.
Kinematics/Dynamics  Chemistry/dust  Stellar populations  Searches for z ~ 6-7 « Hot » scientific researches at VLT in cosmology Mass Galaxy formation/gas.
Ben Maughan (CfA)Chandra Fellows Symposium 2006 The cluster scaling relations observed by Chandra C. Jones, W. Forman, L. Van Speybroeck.
Primeval Starbursting Galaxies: Presentation of “Lyman-Break Galaxies” by Mauro Giavalisco Jean P. Walker Rutgers University.
AGN and Quasar Clustering at z= : Results from the DEEP2 + AEGIS Surveys Alison Coil Hubble Fellow University of Arizona Chandra Science Workshop.
Figure 5: Example of stacked images. Figure 6: Number count plot where the diamonds are the simulated data assuming no evolution from z=3-4 to z=5 and.
Rand (2000) NGC 5775 Hα map. D = 24.8 Mpc It is an interacting galaxy.
Quasar & Black Hole Science for GSMT Central question: Why do quasars evolve?
Dusty star formation at high redshift Chris Willott, HIA/NRC 1. Introductory cosmology 2. Obscured galaxy formation: the view with current facilities,
High Redshift Galaxies: Encircled energy performance budget and IFU spectroscopy Claire Max Sept 14, 2006 NGAO Team Meeting.
Black Holes in Nearby Galaxies Claire Max NGAO Team Meeting March 7, 2007.
1 High-z galaxy masses from spectroastrometry Alessio Gnerucci Department of Physics and Astronomy University of Florence 13/12/2009- Obergurgl Collaborators:
Evolution in Lyman-alpha Emitters and Lyman-break Galaxies Masao Mori Theoretical Astrophysics division, Center for Computational Sciences, University.
Andrew Humphrey INAOE Submitted to MNRAS Letters with M. Villar-Martín, S.F. Sánchez, A. Martínez-Sansigre, R. González Delgado, E. Pérez, C. Tadhunter,
Gamma-ray Bursts in the E-ELT era Rhaana Starling University of Leicester.
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.
Luminosity and Mass functions in spectroscopically-selected groups at z~0.5 George Hau, Durham University Dave Wilman (MPE) Mike Balogh (Waterloo) Richard.
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.
The Evolution of Quasars and Massive Black Holes “Quasar Hosts and the Black Hole-Spheroid Connection”: Dunlop 2004 “The Evolution of Quasars”: Osmer 2004.
Wide Field Imagers in Space and the Cluster Forbidden Zone Megan Donahue Space Telescope Science Institute Acknowledgements to: Greg Aldering (LBL) and.
Large-Scale Winds in Starbursts and AGN David S. Rupke University of Maryland Collaborators: Sylvain Veilleux D. B. Sanders  v = km s -1 Rupke,
RADIO OBSERVATIONS IN VVDS FIELD : PAST - PRESENT - FUTURE P.Ciliegi(OABo), Marco Bondi (IRA) G. Zamorani(OABo), S. Bardelli (OABo) + VVDS-VLA collaboration.
10/14/08 Claus Leitherer: UV Spectra of Galaxies 1 Massive Stars in the UV Spectra of Galaxies Claus Leitherer (STScI)
Next generation redshift surveys with the ESO-VLT
1 VVDS: Towards a complete census of star formation at 1.4
Introduction to the modern observational cosmology Introduction/Overview.
Surveying the Universe with SNAP Tim McKay University of Michigan Department of Physics Seattle AAS Meeting: 1/03 For the SNAP collaboration.
The cooling-flow problem
The Environmental Effect on the UV Color-Magnitude Relation of Early-type Galaxies Hwihyun Kim Journal Club 10/24/2008 Schawinski et al. 2007, ApJS 173,
Imaging Molecular Gas in a Nearby Starburst Galaxy NGC 3256, a nearby luminous infrared galaxy, as imaged by the SMA. (Left) Integrated CO(2-1) intensity.
Expected progress and break-throughs in ground-based extragalactic astronomy Ralf Bender ESO Council FORS Deep Field.
Naoyuki Tamura (University of Durham) The Universe at Redshifts from 1 to 2 for Early-Type Galaxies ~ Unveiling “Build-up Era” with FMOS ~
The European Extremely Large Telescope Studying the first galaxies at z>7 Ross McLure Institute for Astronomy, Edinburgh University.
Elizabeth Stanway - Obergurgl, December 2009 Lyman Break Galaxies as Markers for Large Scale Structure at z=5 Elizabeth Stanway University of Bristol With.
Simulations of Lyα emission: fluorescence, cooling, galaxies Jordi Miralda Escudé ICREA University of Barcelona, Catalonia Berkeley, Collaborators:
Lyman- Emission from The Intergalactic Medium
Galaxies with Active Nuclei Chapter 14:. Active Galaxies Galaxies with extremely violent energy release in their nuclei (pl. of nucleus).  “active galactic.
From Avi Loeb reionization. Quest to the Highest Redshift.
Probing the Reionization Epoch in the GMT Era Xiaohui Fan (University of Arizona) Seoul/GMT Meeting Oct 5, 2010.
Feedback Observations and Simulations of Elliptical Galaxies –Daniel Wang, Shikui Tang, Yu Lu, Houjun Mo (UMASS) –Mordecai Mac-Low (AMNH) –Ryan Joung (Princeton)
Mark Dijkstra, PSU, June 2010 Seeing Through the Trough: Detecting Lyman Alpha from Early Generations of Galaxies ‘ Mark Dijkstra (ITC, Harvard) based.
RGS observations of cool gas in cluster cores Jeremy Sanders Institute of Astronomy University of Cambridge A.C. Fabian, J. Peterson, S.W. Allen, R.G.
Goals for HETDEX Determine equation of state of Universe and evolutionary history for dark energy from 0
Emission Line Surveys Lecture 1 Mauro Giavalisco Space Telescope Science Institute University of Massachusetts, Amherst 1 1 From January 2007.
Robust identification of distant Compton-thick AGNs IR AGN Optical AGN Need for deep optical-mid-IR spectroscopy: multiple lines of evidence for intrinsic.
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.
Deep Surveys for High-z Galaxies with Hyper Suprime-Cam M. Ouchi (OCIW), K. Shimasaku (U. Tokyo), H. Furusawa (NAOJ), & HSC Consortium ≲ ≳≲ ≳
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: )
Competitive Science with the WHT for Nearby Unresolved Galaxies Reynier Peletier Kapteyn Astronomical Institute Groningen.
Chapter 25 Galaxies and Dark Matter. 25.1Dark Matter in the Universe 25.2Galaxy Collisions 25.3Galaxy Formation and Evolution 25.4Black Holes in Galaxies.
Tools for computing the AGN feedback: radio-loudness and the kinetic luminosity function Gabriele Melini Fabio La Franca Fabrizio Fiore Active Galactic.
Sample expanded template for one theme: Physics of Galaxy Evolution Mark Dickinson.
The Radio Properties of Type II Quasars PLAN Type II quasars Motivations Our sample Radio observations Basic radio properties Compare our results with.
High Redshift Galaxies/Galaxy Surveys ALMA Community Day April 18, 2011 Neal A. Miller University of Maryland.
The Formation of the HE System 胡剑 清华天体物理中心 Apr. 22, 2005.
Galaxy Evolution and WFMOS
A Survey of Starburst Galaxies An effort to help understand the starburst phenomenon and its importance to galaxy evolution Megan Sosey & Duilia deMello.
in a Large-Scale Structure at z=3.1
Constraints on Star Forming Galaxies at z>6.5
High Resolution Spectroscopy of the IGM: How High
Galaxies With Active Nuclei
Galaxies With Active Nuclei
Borislav Nedelchev et al. 2019
Presentation transcript:

IFU observations of the high-z Universe Constraints on feedback from deep field observations with SAURON and VIMOS Joris Gerssen

Overview Until a decade ago only extreme objects were known in the distant universe Since then photometric redshift surveys and narrow band surveys identified ( at z ~2 to ~4) –Lyman Break Galaxies –Ly-alpha galaxies Observational constraints on galaxy formation and evolution –e.g. morphology, star formation history, luminosty functions, etc.

Among the drivers behind this advancement are –The 10m class telescopes and instruments –Hubble Space Telescope –Theoretical understanding of structure formation Integral Field Spectropscopy (IFS) is a recent development with great potential to further galaxy evolution studies

Integral Field Spectroscopy Data cube: f(x, y, lambda) - VIMOS - SINFONI - MUSE - SAURON - PMAS - … Field-of-View few (tens) of arcsec Spectral resolution: R ~200 to ~2500 Typical properties:

High-redshift science with IFUs (e.g. list of MUSE science drivers) Formation and evolution of galaxies: –High-z Ly-  emitters –Feedback –Luminosity functions (PPAK, VIRUS) –Reionization –...

Feedback A longstanding problem in galaxy formation is to understand how gas cools to form galaxies Discrepancy between observed baryon fraction (~8%) and predicted fraction (> 50% ) To solve this “cosmic cooling crisis” the cooling of gas needs to be balanced by the injection of energy (SNe/AGN)

Feedback Galactic outflows driven by AGN and/or SNe –Resolve discrepancy between observed and predicted baryon fraction –Terminate star formation –Enrich IGM NGC 6240 (ULIRG) M82 (starburst)

IFU Deep Field Observations Deep SAURON & VIMOS observations of blank sky But in practice centered on QSOs/high-z galaxies –observe extended Ly-  halo emission –serendipitous detections

SAURON Deep Fields The SAURON IFU is optimized for the study of internal kinematics in early type galaxies DF observations of: SSA22a, SSA22b, HB89 Redshift range ( Angstrom) Texp ~10 hours FoV: 33 x 41 arcsec, R ~ 1500

SSA22a SAURON observations: overview SSA22b HB

SSA22b (z = 3.09) Wilman, Gerssen, Bower, Morris, Bacon, de Zeeuw & Davies (Nature, 14 July 2005) VolView rendering

Ly-  distribution 1.0 arcsec = 7.6 kpc

Line profiles Emission lines ~ 1000 km/s wide Emission peaks shift by a few 100 km/s Absorption minima differ by at most a few tens of km/s Ly alpha is resonant scattered, naturally double peaked Yet, absorption by neutral gas is a more straighforward explanation

Model cartoon

SSA22b results Assuming shock velocities of several 100 km/s Shell travels ~100 kpc in a few 10 8 yr Shell can cool to ~10 4 K in this time – Implied by the Voigt profile b parameter – Required to be in photoionization equilibrium Implied shell mass of M  Kinetic energy of the shell ~10 58 erg About erg available (IMF) Superwind model provides a consistent, and energetically feasible description

Comparison with SSA22a SSA22a –Kinematical structure more irregular –Luminous sub-mm source Suggests that a similar outflow may have just begun Probe a wider range of galaxies: –SCUBA galaxy (observed last year) –Radio galaxy (observed one last week) –LBG (a few hours last week)

SINFONI observations of SSA22b Foerster Schreiber et al. Constrain the stellar properties Link them to the superwind Scheduled for P77 (B)

Serendipitous emitters The correlation of Ly-alpha emitters with the distribution of intergalactic gas provides another route to observationally constrain feedback Based on Adelberger et al (2003) who find that the mean transmission increases close to a QSO –This result is derived from 3 Ly-  sources only

Mean IGM transmission Adelberger et al Adelberger et al z ~ 3 z ~ 2.5

Advantage of IFUs IFUs cover a smaller FOV then narrow band imaging, but –IFUs are better matched to Ly-alpha line width –Do not require spectroscopic follow-up –Directly probe the volume around a central QSO Thus, IFUs should be more efficient than narrow band surveys

IFU observations Search the data cube for emitters Use the QSO spectrum to measure the gas distribution –Likely require the UVES spectra Available: –One SAURON data cube –2 of 4 VIMOS IFU data cubes SAURON example: HB

VIMOS 'QSO2' z = 3.92, Texp = 9 hours LR mode

Search by eye for candidates Need to identify/apply an automated procedure

Detection algorithms Matched kernel search –Many false detections IDL algorithm (van Breukelen & Jarvis 2005) FLEX: X-ray based technique (Braito et al. 2005) ELISE-3D: sextractor based (Foucaud 2005)

van Breukelen & Jarvis (MNRAS 2005) Similar data set: –Radio galaxy at z = 2.9 –same instrumental set up –similar exposure time Yet, they find more (14) and brighter Ly-  emitters –Using an automated source finder

In progress A direct comparison with the van Breukelen results –Obtained their data from ESO archive –And reduced and analyzed it with our procedures Preliminary results are in reasonably good agreement –‘Our’ data appears somwhat more noisy –Find their emitters and their new type-II quasar (Jarvis et al 2005)

Preliminary results Number density of Ly alpha emitters agrees with model predictions (fortuitous) –The VIMOS fields contain emitters –Models (Deliou 2005) predict 9 in a similar volume IFUs are sensitive to at least a few 10E-18 erg/s/cm2

Summary IFUs provide a uniquely powerful way to study the haloes around high redshift proto-galaxies Volumetric data are an efficient way to search for Ly-alpha galaxies –An alternative method to constrain feedback IFUs are a very valuable new tool to study the formation and evolution of galaxies