Quasar Absorption Lines Tracing Cosmic Structure Growth & Galaxy Evolution Over Cosmic Time.

Slides:



Advertisements
Similar presentations
Astronomical Solutions to Galactic Dark Matter Will Sutherland Institute of Astronomy, Cambridge.
Advertisements

Metals at Highish Redshift And Large Scale Structures From DLAs to Underdense Regions Patrick Petitjean Institut d’Astrophysique de Paris B. Aracil R.
Dark Matter in Dwarf Galaxies
Matter Content of the Universe David Spergel March 2006 Valencia, Spain.
The Self-Similarity of Galactic Gaseous Halos: Clues to the Evolution of Galaxies Chris Churchill New Mexico State University Collaborators: Nikki Nielsen.
HI Stacking: Past, Present and Future HI Pathfinder Workshop Perth, February 2-4, 2011 Philip Lah.
Tidal Disruption of Globular Clusters in Dwarf Galaxies J. Peñarrubia Santiago 2011 in collaboration with: M.Walker; G. Gilmore & S. Koposov.
SKA Science Measuring Variations in the Fundamental Constants with the SKA Steve Curran School of Physics School of Physics University of New South Wales.
Probing the Universe with QSO Absorption Lines David Turnshek University of Pittsburgh.
The faint end …. …. in neutral gas. “luminous”
C. Churchill (NMSU) D. Ceverino (NMSU) A. Klypin (NMSU) C. Steidel (Caltech) M. Murphy (Swinburne) N. Vogt (NMSU) Glenn G. Kacprzak (NMSU / Swinburne)
Missing Photons that Count: Galaxy Evolution via Absorbing Gas (and a little bit of fundamental physics to boot) Chris Churchill (Penn State)
Mg II & C IV Absorption Kinematics vs. Stellar Kinematics in Galaxies Chris Churchill (Penn State) J. Charlton J. Ding J. Masiero D. Schneider M. Dickinson.
Rand (2000) NGC 5775 Hα map. D = 24.8 Mpc It is an interacting galaxy.
Galactic Gas Kinematics and High Velocity Clouds at z~1 Chris Churchill (Penn State) Mg II 2796,2803 absorption from galaxies and ??? in quasar spectra.
How to Measure Evolution in the Fundamental Constants of Physics with Large Telescopes Chris Churchill (Penn State) …and sneak in astronomical observations.
“Damped Lyman Alpha Systems” by Wolfe, Arthur M., Gawiser, E. and Prochaska, Jason X. Jean P. Walker Rutgers University Galaxy Formation Seminar.
Evolution of the IGM/Galaxy Halo Interface to z=2 Chris Churchill (New Mexico State University) Wal Sargent (Caltech) Michael Rauch (Carnegie)
ON THE RELATION BETWEEN CIRCULAR VELOCITY AND CENTRAL VELOCITY DISPERSION IN HSB AND LSB GALAXIES E.M. Corsini, A. Pizzella, E. Dalla Bontà, F.Bertola.
1 GRB Host Galaxies S. R.Kulkarni, E. J. Berger & Caltech GRB group.
Galaxy Properties and the Kinematics of Gaseous Halos Chris Churchill (NMSU) Glenn Kacprzak (NMSU) Chuck Steidel (Caltech) also see: Poster (G.
Modelling Dwarf Galaxies with a Multi-Phase ISM Stefan Harfst 1,2 with: Ch. Theis 3,2 and G. Hensler 3,2 G. Hensler 3,2 1 Rochester Institute of Technology,
IAP XVII1 Millions of Tiny, Weak Mg II Absorbers: What are They? Chris Churchill (Penn State) Jane Rigby (Steward); Jane Charlton (PSU) Churchill, Rigby,
Quasars Probing Quasars
Molecular absorption in Cen A on VLBI scales Huib Jan van Langevelde, JIVE Ylva Pihlström, NRAO Tony Beasley, CARMA.
Figure 2: H  emission from NGC 1569 (Hunter et al. 1993). Note the numerous filaments extending far into the halo and the prominent H  arm in the west.
Galaxy Formation and Evolution Chris Brook Modulo 15 Room 509
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.
1 Probing the high redshift (2-3) IGM through OVI absorption Sowgat Muzahid (IUCAA, INDIA) Supervisor : R. Srianand (IUCAA, INDIA) Collaborator : P. Petitjean.
Roland DiehlIAU Beijing Aug 2012 The ISM throughout the Galaxy 26 Al Radioactivity Positron Annihilation Roland Diehl MPE Garching, Germany.
The Evolution of Quasars and Massive Black Holes “Quasar Hosts and the Black Hole-Spheroid Connection”: Dunlop 2004 “The Evolution of Quasars”: Osmer 2004.
Star Formation in our Galaxy Dr Andrew Walsh (James Cook University, Australia) Lecture 1 – Introduction to Star Formation Throughout the Galaxy Lecture.
Galaxy Wind IGM Enrichment from Star Forming Galaxies: 1
Missing Photons that Count: Galaxy Evolution via Absorbing Gas (and a little bit of fundamental physics to boot) Chris Churchill (Penn State)
The shapes of the THINGS HI profiles Presented by : Ianjamasimanana Roger Supervisor : Erwin de Blok UNIVERSITY OF CAPE TOWN.
QSO Absorbers in Radio Selected Samples Sara Ellison - University of Victoria Max Pettini - Cambridge Chris Akerman - Cambridge Chris Churchill - NMSU.
Spatial Probing of Absorbing “Halo” Gas Through  CDM Simulations of Galaxies Chris W. Churchill, Daniel Ceverino, Glenn G. Kacprzak, Jessica L. Evans,
Galaxies and Other Gaseous Structures Through Quasar Absorption Lines Jane Charlton Penn State Collaborators: Chris Churchill (NMSU), Jie Ding (NYU),
Study Mg II quasar absorption line systems in order to understand the kinematics of halos probing distances out to 70 kpcs from the galaxies. Therefore.
In this toy scenario, metal enriched clouds entrained in galactic winds gives rise to absorption lines in quasar spectra, as illustrated in the above panels.
Theoretical Predictions about the Cold- Warm Gas Size around Cluster Galaxies using MgII systems Iván Lacerna VII Reunión Anual, SOCHIAS 2009 January 14.
Complete Ionisation of the Neutral Gas in the Hosts of High Redshift AGN As Traced Through HI and MgII Absorption.
UNM 29-Oct04 Galaxy-Halo Gas Kinematic Connection at 0.3 < z < 1 Collaborators: Chris Churchill (NMSU) Chuck Steidel (Caltech) Alice Shapley (Princeton)
Weipeng Lin (The Partner Group of MPA, SHAO) Collaborators Gerhard Börner (MPA) Houjun Mo (UMASS & MPA) Quasar Absorption line systems: Inside and around.
Spiral Triggering of Star Formation Ian Bonnell, Clare Dobbs Tom Robitaille, University of St Andrews Jim Pringle IoA, Cambridge.
Lyman- Emission from The Intergalactic Medium
Cool Halo Gas in a Cosmological Context Kyle Stewart “Team Irvine” UC Santa Cruz Galaxy Formation Workshop Kyle Stewart “Team Irvine” UC Santa.
Expansion and Collapse in the Cosmic Web Rauch (OCIW), Becker (CIT), Viel (IoA), Sargent (CIT), Smette (ESO),Simcoe (MIT), Barlow (CIT) (based on QSO absorption.
DLA Surveys and Stats Sandhya Rao University of Pittsburgh.
Missing Photons that Count: Galaxy Evolution via Absorbing Gas (and a little bit of fundamental physics to boot) Chris Churchill (Penn State)
Probing quasar outflows with intrinsic narrow absorption lines 1/15 The Central Engine of AGN in Xi’an (Oct. 17, 2006) T. Misawa, M. Eracleous, J. C. Charlton.
A New Perspective on Galaxy Outflows Glenn Kacprzak Kutching - Sept. 19 th 2014 N. Bouché (IRAP) C. Churchill (NMSU) J. Cooke (Swinburne) S. Ho (UCSB)
David R. Law Hubble Fellow, UCLA The Physical Structure of Galaxies at z ~ John McDonald, CFHT Galaxies in the Distant Universe: Ringberg Castle.
Surveying the Highly Ionized HVCs with FUSE and HST Joe Collins (University of Colorado) Mike Shull (University of Colorado) Mark Giroux (East Tennessee.
Jessica Rosenberg Harvard-Smithsonian Center for Astrophysics NSF Astronomy and Astrophysics Postdoctoral Fellow Collaborators: Stephen Schneider, Jennifer.
A deep view of the iron line and spectral variability in NGC 4051 James Reeves Collaborators:- Jane Turner, Lance Miller, Andrew Lobban, Valentina Braito,
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.
Eugenio Ursino on behalf of the UM Astrophysics Group University of Miami, USA Looking for the Missing Baryons.
European X-ray CalorimeterUtrecht, October 2004 (Some) astrophysical drivers for a high-resolution imaging X-ray spectrometer Xavier Barcons Instituto.
Mass Profiles of Galaxy Clusters Drew Newman Newman et al. 2009, “The Distribution of Dark Matter Over Three Decades in Radius in the Lensing Cluster Abell.
The prolate shape of the Galactic halo Amina Helmi Kapteyn Astronomical Institute.
Figure 7 from The Evolution of Dwarf Galaxy Satellites with Different Dark Matter Density Profiles in the ErisMod Simulations. I. The Early Infalls Mihai.
Filamentary Structures Traced by IRDCs
Galaxy Formation and Evolution: Where we are and where we are going.
Biases in Virial Black Hole Masses: an SDSS Perspective
Jill Bechtold (University of Arizona)
Molecular Gas Distribution of our Galaxy: NANTEN Galactic Plane Survey
Churchill (NMSU) – Santa Cruz 2013
High Resolution Spectroscopy of the IGM: How High
Author: Ting-Wen Lan and Houjun Mo.(2018)
Presentation transcript:

Quasar Absorption Lines Tracing Cosmic Structure Growth & Galaxy Evolution Over Cosmic Time

Chris Churchill (PSU)2

3

4

5

6

7 Motivations and Astrophysical Context Mg II arises in environments ranging over five decades of N(HI) DLAs: N(HI)>2 x cm -2 LLSs: N(HI)>2 x cm -2 sub-LLSs: N(HI)<6 x cm -2 Statistical Cross-Sections, n  Giant molecular clouds?; 0.1 L * and LSB galaxies with wide range of morphologies; intergalactic clumps; n  ~15 kpc; black-bottom absorption with  v~200 km s -1 ; average C IV absorption (eg. Le Brun et al 1997; Rao & Turnshek 2000; Bouche’ etal 2000; cwc etal (II) 2000) “Normal” HSB galaxies with >0.1 L * ; n  ~40 kpc; complex kinematics with “high velocity” components with  v~ km s -1 ; range of C IV absorption (eg. Steidel et al 1994; cwc etal 1996; cwc 1997; cwc & Vogt 2000) assuming  * =0.03 h 3 Mpc -3 “forest clouds”? LSB galaxies?; dwarf galaxies?; few associated with HSB galaxies; mostly single unresolved clouds; n  ~70 kpc; sizes ~10 pc to 1 kpc; Z>0.1 solar; [  /Fe]~0 to +0.5; C f ~0.15; range of C IV absorption (eg. cwc & Le Brun 1998; cwc etal ApJS 1999 ; Rigby etal 2001) Sub-LLS Mg II selects a wide range of astrophysical sites, which can be traced from redshift 0 to 5

Chris Churchill (PSU)8 What the sensitivity and resolution buy… Steidel & Sargent (1992) cwc (1997); cwc & Charlton (1999)

Chris Churchill (PSU)9 cwc & Charlton 1999

Chris Churchill (PSU)10

Chris Churchill (PSU)11

Chris Churchill (PSU)12 cwc 2001

Chris Churchill (PSU)13 Statistically, Profiles are Consistent with … (Charlton & cwc 1998) Monte-Carlo Models of Absorbing Galaxies What is probability distribution for such models? Assume  ~r -2 probability distribution of clouds in disk and in halo Assume V rot =V infall kinematics of clouds in disk and in halo

Chris Churchill (PSU)14

Chris Churchill (PSU)15 Voigt Profiles Assume minimum number of components that are statistically significant (MINFIT). Parameterization does not account for asymmetric line-of-sight streaming motion. cwc (1997); cwc, Vogt, & Charlton, ApJ, (2001)

Chris Churchill (PSU)16 “Weak Systems” Single Clouds, W r (MgII)<0.3 , isolated in redshift Unresolved line widths at 6 km s -1 Power law equivalent width distribution down to W r (MgII)=0.02  cwc etal, ApJS (1999) Steidel & Sargent (1992)

Chris Churchill (PSU)17

Chris Churchill (PSU)18

Chris Churchill (PSU)19