Spin Acquisition, Violent Disks, Compaction and Quenching

Size: px
Start display at page:

Download "Spin Acquisition, Violent Disks, Compaction and Quenching"

Transcription

1 Spin Acquisition, Violent Disks, Compaction and Quenching Avishai Dekel The Hebrew University of Jerusalem July 2014 stars 5 kpc

2 Three Provocative Questions concerning high-z massive galaxy formation 1. How do galaxies acquire AM? Gas ~ DM? 2. Do we understand violent disk instability? 3. How do galaxies compactify and quench? Hydro simulations cosmological - 25pc, isolated 1pc resolution - ART (Klypin, Kravtsov, Ceverino) - RAMSES (Teyssier, Bournaud+) Combined with toy modeling

3 1. Angular Momentum: from the cosmic web to disks & spheroids Pichon, Devriendt Pichon, Devriendt Stewart, Bullock+ 2011, 2013 Danovich, Dekel+ 2012, 2014

4 Massive halos at high-sigma nodes are fed by relatively thin dense filaments cold streams Typical halos reside in relatively thick filaments, fed from all directions the millenium cosmological simulation

5 Gas streams along the cosmic web AMR RAMSES Teyssier, AD box 300 kpc res 50 pc z = 5 to 2.5

6 Streams Feeding a Hi-z Galaxy Tweed, Dekel, Teyssier RAMSES Res. 50 pc

7 Co-planar ~3 Streams (in a pancake) influx M yr -1 rad R vir Danovich, Dekel, Teyssier, Hahn 12

8 Narrow dense gas streams at high z versus spherical infall at low z high z low z M=10 12 M ʘ >>M PS M=10 12 M ʘ ~M PS Ocvirk, Pichon, Teyssier 08

9 Cold Streams Penetrate through Hot Halos M v > M 100 kpc Agertz et al 09

10 AM Buildup by Cold Gas in 4 Phases III. inner halo extended tilted ring non-linear torques, dissipation AM loss λ cold 0.04 & alignment Danovich, Dekel, Hahn+ 14 II. outer halo AM transport, j~const. λ cold ~3λ dm ~0.1 DM mix V v I. cosmic web linear tidal torques impact parameter λ cold ~1.7λ dm ~ R v 2R v IV. inner disc (+ bulge) disk instability, outflows λ baryons ~0.03 spin parameter λ ~ J / M 2R V V V

11 TTT outside the halo: λ cold ~1.7λ DM due to quadrupole moment of inertia J tε i ijk T jl I lk R v ~100 kpc cold gas dark matter TTT is applied at max-expansion along the streams, after pre-collapse of gas to the filaments cords

12 AM of Cold Gas R v AM is represented by impact parameters <0.3R v Some counter-rotating In outer halo AM transport by straight streams Most of the AM is in one stream (determines the AM plane at R v ) Deep penetration of the streams

13 How do the streams join the disk? Ceverino, Dekel, Bournaud 2010 ART 35-70pc resolution streams disk 30 kpc interface region A messy interface region: breakup due to shocks, hydro and thermal instabilities, collisions between streams and clumps, heating

14 An Extended Tilted Ring about the Disk gas density 30 kpc stream lines expressway entrance

15 A tilted AM transport rotating ring the in outer the inner halo halo radial inflow AM loss circular orbits AM conserved spiral in alignment with disk color indicates mass in each cell impact parameter ~ const. AM not aligned with disk

16 AM Exchange in the Ring: Torques by Disk torques by an idealized disk Torques in the simulated galaxies

17 Extended Ring: HI Column Density Random lines of sight through ( )R v 30% DLAS HI 60% no HI n > 0.01 H cm -3

18 Detection of an Extended Ring? Bouche z=2.3 Low-Z gas 26 kpc from center V=180 km/s Crighton z=2.4, 54 kpc Steidel+ 2002, Kacprzak+ 2010

19 Outflows do not halt the Inflows DeGraf+ 14 Gas density Temperature Velocity dilute hot z=2.6 M v =7x Dense, cold, metal-poor inflows penetrate into the galaxy - Hot, metal-rich, fast outflows fly through the dilute CGM -300 M yr -1 rad -2 - outflows remove low-angular-momentum gas outflows help quenching SFR +50

20 AM Evolution in Disks Gas-rich -> violent disk instability (VDI) (Noguchi 99; Dekel+ 09) -> torques -> AM outflow and mass inflow (Gammie 01) -> massive spheroids (+BHs) with low AM (Genzel+ 08; Bournaud+11; Dekel+ 13) Stellar and AGN feedback -> outflows remove low-am gas from galaxy centers (Maller & Dekel 02; Governato+ 10; Guedes+ 11) λ gal < λ disk ~ 0.03 λ disk is only slightly smaller than λ DM -> naïve model is ~valid despite the different AM evolution

21 2. Violent Disk Instability Clumpy disk galaxies: Elmegreen+ UDF Genzel, Tacconi, Forster-Schreiber+ SINS Guo, Giavallisco+ 12, 14 CANDELS

22 Clumpy Disk Ceverino, Dekel et al. 10 kpc z=4-2.1

23 Violent Disk Instability (VDI) at High z High gas density disk unstable Q σω G Σ 1 Giant clumps and transient features GΣ R rapid evolution on dynamical time clump 2 Ω 5 kpc Toomre 64 Isolated galaxies: Noguchi 99 Immeli+ 04a,b Bournaud, Elmegreen+ 06, 08 Hopkins+ 12 Bournaud+ 13 In cosmology: Dekel, Sari, Ceverino 09 Agertz et al. 09 Ceverino, AD, Bournaud 10 Ceverino+ 11 Cacciato, AD, Genel 12a,b Genel+ 12 Forbes et al. 12, 13, 14 Self-regulated at Q~1 by torques and inflow high σ/v~1/5 Inflow in disk compact bulge and BH Steady state: disk draining and replenishment, bulge ~ disk

24 Violent Disk Instability (VDI) at High z Ceverino+ ART-AMR cosmological simulations at 25pc resolution highly perturbed, clumpy rotating disk: H/R ~ σ/v ~ f cold ~ 0.2

25 Violent Disk Instability (VDI) at High z Ceverino+ ART-AMR cosmological simulations at 25pc resolution H/R ~ σ/v ~ f cold ~ 0.2

26 z=4 Clumpy Disk in a cosmological steady state VDI is robust at z>1 because of high gas density (cosmological density and intense accretion). In some galaxies from z>7 to z<1. z=3 z=2 z=1.5 z=1 Σ gas [M pc -2 ] Dekel, Sari, Ceverino 09; Ceverino, Dekel, Bournaud 10 Mandelker et al. 14

27 Elmegreen et al Observations vs. Simulations

28 A typical star-forming galaxy at z=2: clumpy, rotating, extended disk & a bulge Hα star-forming regions color-code velocity field Genzel et al 08

29 BzK 6004 (2.4) BzK (2.4) BX 610 (2.2) BX482 (2.2) ZC (2.2) merger merger -160 BX389 (2.2) D3a 6397 (1.51) +50 K20-7 (2.2) BX663 (2.4) MD 41 (2.2) K20-9 (2.0) HDF 242 (2.49) ZC (1.41) BX528 (2.3) (8 kpc) -70 K20-8 (2.2) -170 K20-6 (2.2) K20-5 (2.2) GK2471 (2.43) D3a 4751 (2.27) SA (1.51) 150 HDF 169 (1.2) BX 405 (2.03) GK2252 (2.41) BX 599 (2.33) 100 BzK 4165 (1.7) SMMJ09431 (3.35) H7 H6 HDF 76 (2.20) SA (2.3) BX 502 (2.16) N (2.45) BM 1163 (1.41) GK 167 (2.58) SA (2.2) BX 404 (2.03) (Förster SMMJ Schreiber (3.41) et al. 2006, 2008) SMMJ (1.21) N (2.38) +200 GK 2113 (1.61) (8 kpc) The SINS survey of galaxy kinematics at z~

30 High-z Disks with Giant Clumps Guo et al. 12 CANDELS

31 Simulated hi-z galaxy through Dust SUNRISE low dust RGB colors MW3 z=2.33 Moody+ medium high

32 In-situ (VDI) and Ex-situ (merger) Clumps gas Poster by Nir Mandelker: clump properties, young survival stars under feedback, observable gradients of age/color 10 kpc dark matter stars

33 Clumps in VDI Disks - most hi-z galaxies go through a VDI phase - perturbed by intense inflows including minor mergers - bulge ~ disk in cosmological steady state - giant clumps M~ M R<0.5kpc - in-situ (gaseous, SFR) and ex-situ (stellar, mergers) - half the SFR in clumps - migration to center in ~300 Myr gas+ young stars - clumps >10 8 M survive outflows with mass~constant η~1-2 winds, gas accretion, tidal stripping - less massive clumps disrupt - VDI feed gas & stars to the bulge and BH Expect a weak gradient of clump mass in disks Certain gradient in age/color for in-situ clumps

34 Violent Instability with Q~2-3 Toomre Q Ωσ / Σ 1 Q=1-2 Q=2-5 Q=1-2 Q=5-10 Nonlinear instability - driven by intense inflows with minor mergers, or by the non-linear clumps themselves Compression modes of turbulence r r r σ = σ + σ = r φ + r irrotation solenoid A r

35 Compression Modes of Turbulence: Merger r r r σ = σ + σ = r φ+ r irrotational solenoidal A r Renaud+ 14

36 3. Compaction to Blue Nuggets Quenching to Red Nuggets Cheung+ 12; Fang+13; Barro+ 13,14a,b; Bruce+ 12,14; Williams+ 14; Nelson, van Dokkum+ 14 Dekel & Burkert 2014; Zolotov et al. 2014

37 Inflow in unstable disks Clump migration in ~300 Myr Massive clumps survive feedback Elmegreen, Bournaud+ 07, 08; Genzel+ 06, 08; Dekel, Sari, Ceverino 09; Bournaud+ 14; Dekel+ 14 Inflow in disk, evaluated by torques, dynamical friction, clump encounters, self-regulated instability t 2 inflow f cold t dyn 2 ( V σ) tdyn 10tdyn Gammie 01; Dekel, Sari, Ceverino 09 Wet compaction if 2 tinflow / tsfr εsfr fcold< 1 valid when gas fraction is high (high z) and spin is relatively low Dekel, Burkert 14 Bournaud, Dekel+ 13

38 Red Nuggets and Blue Nuggets Dekel & Burkert 2013; Zolotov et al Compact stellar spheroid dissipative wet inflow to a blue nugget by mergers and/or VDI Inflow is wet if t inflow << t sfr Self-regulated instability Q ~ 1 Wetness parameter M M cold M tot σ δ V tsfr 1 2 w ε sfrδ > 1 ε sfr 0.02 δ 0. 2 t inflow Expect VDI-driven nuggets: - at high z, where f gas is high - for low spin λ, where R gas is low

39 Wet Origin of Bulge: Stellar Birthplace Zolotov, Dekel, Mandelker, Tweed, Ceverino, Primack 2013 Fraction of bulge stars born in different components in bulge 60-30% of the bulge stars form in the bulge wet inflow Driven by wet VDI or wet mergers

40 Compaction and quenching Zolotov ART cosmological simulations, res. 25pc, with radiative fdbk SFR ~outflow ~recycling VDI + merger self-gravitating M stars >M dm wet inflow > SFR

41 Compaction and quenching stars self-gravitating M stars >M dm mergers DM merger gas no mergers VDI outflow inflow wet inflow > SFR SFR ~outflow ~recycling SFR

42 gas + young stars wet compaction max density: blue nugget vdi disk a hole and a ring vela v2 07

43 stars wet compaction max density: blue nugget green nugget red nugget vela v2 07

44 Stellar Component at z=2.3, edge-on Ceverino Overall Sersic n=2-4 Classical bulge n=3-5

45 Blue and Red Nuggets blue nugget Zolotov, AD+ 14 ssfr quenching SFR stars wet compaction z=3.7 central density SFR stars Observed at z~2-3: - compact passive ellipticals - their progenitors: compact star-forming galaxies z=1.2 red nugget

46 Observations: Blue Nuggets > Red Nuggets Barro+ 13 CANDELS z=1-3 Evolution: diffuse compaction quenching

47 Similar Structure for Blue & Red Nuggets Z=2 M * =10 11 M R e =1 kpc σ=300 km s -1 SFR=90 M yr -1 Nelson, vandokkum+ 2014

48 line width evolution in simulated galaxies quenching blue nugget red nugget extended disk compaction Inoue, Zolotov+ Barro+ 14

49 Blue Nuggets by Wet Inflow: Spin and ssfr Simulations confirm model predictions Dekel, Burkert 14; Zolotov+ 14 low-spin disk -> high Σ max 0.7 ssfr 0.5 high-ssfr disk -> high Σ max 0.3 Σ max

50 Two Modes of Evolution: Fast and Slow Barro, Fang, Yesuf, Woo, Faber, Koo, AD quenched ssfr star forming low z Halo quenching Slow: lower Σ gas disk secular inflow halo grows high z Bulge quenching stellar & AGN fdbk morph. quenching Fast: hi Σ gas disk wet VDI or merger inflow starburst diffuse compact Σ

51 critical halo mass ~10 12 M ʘ Virial Shock Heating Dekel & Birnboim t cool < t compress Kravtsov+ in hi-z massive hot halos cold streams penetrate slow cooling -> shock fast cooling > no shock

52 Cold Streams in Big Galaxies at High z M vir [M ʘ ] all hot cold filaments in hot medium M shock ~M * M shock >>M * M shock all cold M * redshift z Dekel & Birnboim 06

53 Two Quenching Mechanisms: Bulge & Halo Compact gaseous bulge -> gas removal by high SFR, outflow, AGN, Q-quenching quenched In halos > M -> long-term shutdown of gas supply by virial shock heating Woo, Dekel, Faber, Koo+ 14 star forming Need both bulge and halo quenching

54 Stream-Fed Galaxies at High z cold streams compact spheroid wet inflow to bulge quenching thick disk hot halo clumpy disk In parallel, mergers outflows clumpy disk VDI SFR spheroid late disk The main mode of galaxy formation hot halo

55 Conclusions High-z massive galaxies at cosmic-web nodes Fed by ~3 co-planar streams penetrating hot CGM Angular-momentum: - effective tidal torques on gas streams, AM transport to inner halo - spiral-in through an extended rotating tilted ring (DLAS?) - disk spin halo spin Typical SFGs have perturbed rotating disks at violent instability (VDI) - Massive clumps (>10 8 M ) survive feedback - off-center in-situ young clumps <300 Myr, showing age/gas gradient - older ex-situ clumps Nonlinear instability driven by inflow+mergers. Compressive turbulence? A characteristic sequence of events: - wet compaction by mergers and VDI into compact SFGs (blue nuggets) - high SFR+AGN, outflows, massive self-gravitating bulge fast quenching to compact ellipticals (red nuggets) +gas rings (?) - long-term quenching by hot massive halo

Three comments on High-z Galaxy Formation. Avishai Dekel The Hebrew University of Jerusalem

Three comments on High-z Galaxy Formation. Avishai Dekel The Hebrew University of Jerusalem Three comments on High-z Galaxy Formation Avishai Dekel The Hebrew University of Jerusalem August 2014 Outline 1. Angular momentum: buildup in 4 phases 2. Violent disk instability: Nonlinear, Stimulated

More information

Violent Disk Instability at z=1-4 Outflows; Clump Evolution; Compact Spheroids

Violent Disk Instability at z=1-4 Outflows; Clump Evolution; Compact Spheroids Violent Disk Instability at z=1-4 Outflows; Clump Evolution; Compact Spheroids Avishai Dekel The Hebrew University of Jerusalem Santa Cruz, August 2013 stars 5 kpc Outline 1. Inflows and Outflows 2. Evolution

More information

High-z Galaxy Evolution: VDI and (mostly minor) Mergers

High-z Galaxy Evolution: VDI and (mostly minor) Mergers High-z Galaxy Evolution: VDI and (mostly minor) Mergers Avishai Dekel The Hebrew University of Jerusalem UCSC, August 2012 Outline: in-situ (VDI) and ex-situ (mergers) 1. Cold streams: smooth and clumpy

More information

Nir Mandelker, H.U.J.I.

Nir Mandelker, H.U.J.I. Compressive vs Solenoidal Turbulence and Non-Linear VDI Nir Mandelker, H.U.J.I. IAU Symposium 319, August 11 2015 Collaborators: Avishai Dekel, Shigeki Inoue, Daniel Ceverino, Frederic Bournaud, Joel Primack

More information

The Magic Scale of Galaxy Formation: SNe & Hot CGM --> Compaction & BHs

The Magic Scale of Galaxy Formation: SNe & Hot CGM --> Compaction & BHs The Magic Scale of Galaxy Formation: SNe & Hot CGM --> Compaction & BHs Avishai Dekel The Hebrew University of Jerusalem & UCSC Silk 75, December 2017 A Characteristic Mass for Galaxy Formation Efficiency

More information

Violent Disk Instability Inflow to Spheroid and Black Hole

Violent Disk Instability Inflow to Spheroid and Black Hole Violent Disk Instability Inflow to Spheroid and Black Hole Avishai Dekel The Hebrew University of Jerusalem Jerusalem Winter School 101/13 Lecture stars 5 kpc Outline 1. Violent Disk Instability (VDI):

More information

Galaxy Evolution & Black-Hole Growth (review)

Galaxy Evolution & Black-Hole Growth (review) Galaxy Evolution & Black-Hole Growth (review) Avishai Dekel The Hebrew University of Jerusalem & UCSC Delivered by Fangzhou Jiang Dali, China, November 2018 See also Claude-Andre s talk and Joel s talk

More information

Stream-Driven Galaxy Formation at High Redshift

Stream-Driven Galaxy Formation at High Redshift Stream-Driven Galaxy Formation at High Redshift Avishai Dekel The Hebrew University of Jerusalem KooFest, Santa Cruz, August 2011 Outline 1. Streams in pancakes from the cosmic web (Hahn) 2. Is angular

More information

Feeding High-z Galaxies from the Cosmic Web

Feeding High-z Galaxies from the Cosmic Web Feeding High-z Galaxies from the Cosmic Web Avishai Dekel The Hebrew University of Jerusalem Jerusalem Winter School 2012/13 Lecture 1 z=0 z=2 z=8 Cosmological simulations Toy modeling Oxford Dictionary:

More information

Origin of Bi-modality

Origin of Bi-modality Origin of Bi-modality and Downsizing Avishai Dekel HU Jerusalem Galaxies and Structures Through Cosmic Times Venice, March 2006 Summary Q: z

More information

Unstable Disks: Gas and Stars via an analytic model

Unstable Disks: Gas and Stars via an analytic model Unstable Disks: Gas and Stars via an analytic model Marcello Cacciato in collaboration with Avishai Dekel Minerva Fellow @ HUJI Theoretical studies and hydrodynamical cosmological simulations have shown

More information

Yicheng Guo (UCO/Lick, UCSC)

Yicheng Guo (UCO/Lick, UCSC) Formation and Evolution of Clumpy Galaxies at z=0.5--3 Yicheng Guo (UCO/Lick, UCSC) Collaborators: Henry Ferguson, Eric Bell, David Koo, Chris Conselice, Mauro Giavalisco, Nir Mandelker, Swara Ravindranatch,

More information

Cosmological simulations of galaxy formation. Romain Teyssier

Cosmological simulations of galaxy formation. Romain Teyssier Cosmological simulations of galaxy formation 1 Outline Disc formation in LCDM cosmology Star formation efficiency and morphology connection The baryon fraction problem Star formation at high redshift:

More information

Connecting Galaxy Formation to the Cosmic Web

Connecting Galaxy Formation to the Cosmic Web Connecting Galaxy Formation to the Cosmic Web Andreas Burkert (University of Munich & MPE) Bigiel et al. Properties of the Hubble Sequence Halpha imaging surveys (galaxy assembly in the great wall) (Gavazzi+

More information

Hydro ART simulations sample

Hydro ART simulations sample Hydro ART simulations sample Stellar Merger Trees Dylan Tweed dylan.tweed@googlemail.com Racah Institute of Physics, HUJI, Jerusalem CANDELS Theory Workshop - UCSC - August 8 th 10 th 2012 D. P. Tweed

More information

arxiv: v2 [astro-ph.ga] 6 Mar 2015

arxiv: v2 [astro-ph.ga] 6 Mar 2015 Mon. Not. R. Astron. Soc. 000, 1 30 (2002) Printed 9 March 2015 (MN LATEX style file v2.2) Compaction and quenching of high- galaxies in cosmological simulations: blue and red nuggets arxiv:1412.4783v2

More information

Using Hydro-Simulations to Interpret Observed Kinematic Maps of Star-Forming Galaxies

Using Hydro-Simulations to Interpret Observed Kinematic Maps of Star-Forming Galaxies disk from the VELA simulation suite Ceverino, Dekel, Primack, + z = 1.6, young stars Using Hydro-Simulations to Interpret Observed Kinematic Maps of Star-Forming Galaxies Raymond Simons Johns Hopkins University

More information

Secular Evolution of Galaxies

Secular Evolution of Galaxies Secular Evolution of Galaxies Outline:!Disk size evolution! Bar fraction vs mass & color! AM transfers, radial migrations! Bulges, thick disks Françoise Combes Durham, 19 July 2011 Two modes to assemble

More information

Characterizing z~2 Galaxies in HYDRO-ART Simulations and Observations

Characterizing z~2 Galaxies in HYDRO-ART Simulations and Observations Characterizing z~2 Galaxies in HYDRO-ART Simulations and Observations Mark Mozena (UCSC) Sandra Faber, Avishai Dekel, Daniel Ceverino, Joel Primack, Kamson Lai, David Koo, David Rosario, Dale Kocevski,

More information

Galaxy Hydrodynamic Simulations and Sunrise Visualizations

Galaxy Hydrodynamic Simulations and Sunrise Visualizations Galaxy Hydrodynamic Simulations and Sunrise Visualizations Joel Primack, UCSC Daniel Ceverino, HU Madrid Avishai Dekel, HU & UCSC Sandra Faber, UCSC Anatoly Klypin, NMSU Patrik Jonsson, Harvard CfA Chris

More information

Origin and Evolution of Disk Galaxy Scaling Relations

Origin and Evolution of Disk Galaxy Scaling Relations Origin and Evolution of Disk Galaxy Scaling Relations Aaron A. Dutton (CITA National Fellow, University of Victoria) Collaborators: Frank C. van den Bosch (Utah), Avishai Dekel (HU Jerusalem), + DEEP2

More information

Rotational support of giant clumps in high-z disc galaxies

Rotational support of giant clumps in high-z disc galaxies Mon. Not. R. Astron. Soc. 420, 3490 3520 (2012) doi:10.1111/j.1365-2966.2011.20296.x Rotational support of giant clumps in high-z disc galaxies Daniel Ceverino, 1 Avishai Dekel, 1 Nir Mandelker, 1 Frederic

More information

Elad Zinger Hebrew University Jerusalem Spineto, 12 June Collaborators: Avishai Dekel, Yuval Birnboim, Daisuke Nagai & Andrey Kravtsov

Elad Zinger Hebrew University Jerusalem Spineto, 12 June Collaborators: Avishai Dekel, Yuval Birnboim, Daisuke Nagai & Andrey Kravtsov Elad Zinger Hebrew University Jerusalem IGM@50, Spineto, 12 June 2015 Collaborators: Avishai Dekel, Yuval Birnboim, Daisuke Nagai & Andrey Kravtsov They re still there! Account for most of the accretion.

More information

Galaxy Formation: Overview

Galaxy Formation: Overview Galaxy Formation: Overview Houjun Mo March 30, 2004 The basic picture Formation of dark matter halos. Gas cooling in dark matter halos Star formation in cold gas Evolution of the stellar populaion Metal

More information

Numerical Cosmology & Galaxy Formation

Numerical Cosmology & Galaxy Formation Numerical Cosmology & Galaxy Formation Lecture 13: Example simulations Isolated galaxies, mergers & zooms Benjamin Moster 1 Outline of the lecture course Lecture 1: Motivation & Historical Overview Lecture

More information

Assembly of Galaxies Across Cosmic Time: Formaton of te Hubble Sequence at High Redshift

Assembly of Galaxies Across Cosmic Time: Formaton of te Hubble Sequence at High Redshift Assembly of Galaxies Across Cosmic Time: Formaton of te Hubble Sequence at High Redshift Yicheng Guo University of Massachusetts Collaborator: Mauro Giavalisco (UMASS), Paolo Cassata (Marseille), Henry

More information

Disk Formation and the Angular Momentum Problem. Presented by: Michael Solway

Disk Formation and the Angular Momentum Problem. Presented by: Michael Solway Disk Formation and the Angular Momentum Problem Presented by: Michael Solway Papers 1. Vitvitska, M. et al. 2002, The origin of angular momentum in dark matter halos, ApJ 581: 799-809 2. D Onghia, E. 2008,

More information

Physical properties of galaxies at high redshifts II

Physical properties of galaxies at high redshifts II Physical properties of galaxies at high redshifts II Different galaxies at high z s Luminous Infra Red Galaxies (LIRGs): LFIR > 10 11 L Ultra Luminous Infra Red Galaxies (ULIRGs): LFIR > 10 12 L SubMillimeter-selected

More information

Theoretical ideas About Galaxy Wide Star Formation! Star Formation Efficiency!

Theoretical ideas About Galaxy Wide Star Formation! Star Formation Efficiency! Theoretical ideas About Galaxy Wide Star Formation Theoretical predictions are that galaxy formation is most efficient near a mass of 10 12 M based on analyses of supernova feedback and gas cooling times

More information

Phys/Astro 689: Lecture 8. Angular Momentum & the Cusp/Core Problem

Phys/Astro 689: Lecture 8. Angular Momentum & the Cusp/Core Problem Phys/Astro 689: Lecture 8 Angular Momentum & the Cusp/Core Problem Summary to Date We first learned how to construct the Power Spectrum with CDM+baryons. Found CDM agrees with the observed Power Spectrum

More information

Two Phase Formation of Massive Galaxies

Two Phase Formation of Massive Galaxies Two Phase Formation of Massive Galaxies Focus: High Resolution Cosmological Zoom Simulation of Massive Galaxies ApJ.L.,658,710 (2007) ApJ.,697, 38 (2009) ApJ.L.,699,L178 (2009) ApJ.,725,2312 (2010) ApJ.,744,63(2012)

More information

arxiv: v1 [astro-ph.ga] 1 Dec 2016

arxiv: v1 [astro-ph.ga] 1 Dec 2016 Gas Accretion and Angular Momentum Kyle R. Stewart arxiv:1612.00513v1 [astro-ph.ga] 1 Dec 2016 Abstract In this chapter, we review the role of gas accretion to the acquisition of angular momentum, both

More information

Ken-ichi Tadaki (NAOJ, JSPS research fellow)

Ken-ichi Tadaki (NAOJ, JSPS research fellow) Subaru GLAO Science Workshop June 13-14, 2013 Clumpy galaxies and compact star-forming galaxies giant clumps, compact SFGs ~ 1kpc Ken-ichi Tadaki (NAOJ, JSPS research fellow) Tadayuki Kodama (NAOJ), Ichi

More information

Bright Cluster Galaxy formation and the role of AGN feedback. Romain Teyssier

Bright Cluster Galaxy formation and the role of AGN feedback. Romain Teyssier Bright Cluster Galaxy formation and the role of AGN feedback Romain Teyssier KITP 2011: Monster Inc. Romain Teyssier 1 Outline - Feedback and galaxy formation - The role of AGN feedback in Milky Way halos

More information

Gas accretion in Galaxies

Gas accretion in Galaxies Massive Galaxies Over Cosmic Time 3, Tucson 11/2010 Gas accretion in Galaxies Dušan Kereš TAC, UC Berkeley Hubble Fellow Collaborators: Romeel Davé, Mark Fardal, C.-A. Faucher-Giguere, Lars Hernquist,

More information

Cold streams in early massive hot haloes as the main mode of galaxy formation

Cold streams in early massive hot haloes as the main mode of galaxy formation Cold streams in early massive hot haloes as the main mode of galaxy formation arxiv:88.553v3 [astro-ph] 16 Jan 29 A. Dekel 1, Y. Birnboim 1, G. Engel 1, J. Freundlich 1,2, T. Goerdt 1, M. Mumcuoglu 1,

More information

ASTRON 449: Stellar (Galactic) Dynamics. Fall 2014

ASTRON 449: Stellar (Galactic) Dynamics. Fall 2014 ASTRON 449: Stellar (Galactic) Dynamics Fall 2014 In this course, we will cover the basic phenomenology of galaxies (including dark matter halos, stars clusters, nuclear black holes) theoretical tools

More information

How do Black Holes Get Their Gas?

How do Black Holes Get Their Gas? How do Black Holes Get Their Gas? Philip Hopkins Eliot Quataert, Lars Hernquist, T. J. Cox, Kevin Bundy, Jackson DeBuhr, Volker Springel, Dusan Keres, Gordon Richards, Josh Younger, Desika Narayanan, Paul

More information

Galaxy Evolution Workshop Austin, TX, Nov 2008

Galaxy Evolution Workshop Austin, TX, Nov 2008 Galaxy Evolution Workshop Austin, TX, Nov 2008 LCDM is a well-specified theory which makes definite predictions about the way structures in the Universe form and evolve. most (all?) of the mass of the

More information

Star cluster formation in dwarf galaxies

Star cluster formation in dwarf galaxies Star cluster formation in dwarf galaxies Florent Renaud University of Surrey Massive clusters in dwarf outskirts Fornax dwarf galaxy, Larsen et al. High specific frequency Beyond optical radius In situ

More information

Growing and merging massive black holes

Growing and merging massive black holes Growing and merging massive black holes Marta Volonteri Institut d Astrophysique de Paris S. Cielo (IAP) R. Bieri (MPA) Y. Dubois (IAP) M. Habouzit (Flatiron Institute) T. Hartwig (IAP) H. Pfister (IAP)

More information

Galaxy interaction and transformation

Galaxy interaction and transformation Galaxy interaction and transformation Houjun Mo April 13, 2004 A lot of mergers expected in hierarchical models. The main issues: The phenomena of galaxy interaction: tidal tails, mergers, starbursts When

More information

molecular cloud and a

molecular cloud and a A molecular cloud and a Stop me if you ve heard this one before star cluster walk into a bar... Florent Renaud Lund Observatory with E. Emsellem, N. Guillard et al. A complex scale-coupling environment

More information

Gravitational heating, clumps, overheating. Yuval Birnboim (Harvard Smithsonian Center for Astrophysics) Avishai Dekel (Hebrew University)

Gravitational heating, clumps, overheating. Yuval Birnboim (Harvard Smithsonian Center for Astrophysics) Avishai Dekel (Hebrew University) Gravitational heating, clumps, overheating Yuval Birnboim (Harvard Smithsonian Center for Astrophysics) Avishai Dekel (Hebrew University) Basic idea: Cooling flow Clusters need additional energy to reduce

More information

Cosmological formation of slowly rotating massive elliptical galaxies

Cosmological formation of slowly rotating massive elliptical galaxies Cosmological formation of slowly rotating massive elliptical galaxies Thorsten Naab with ATLAS 3D MPA L. Oser, M.Hilz, E. Emsellem, M. Cappellari, D. Krajnovic, R. M. McDermid, N. Scott, P. Serra, G. A.

More information

Gravitational Radiation from Coalescing SMBH Binaries in a Hierarchical Galaxy Formation Model

Gravitational Radiation from Coalescing SMBH Binaries in a Hierarchical Galaxy Formation Model Gravitational Radiation from Coalescing SMBH Binaries in a Hierarchical Galaxy Formation Model Motohiro ENOKI (National Astronomical Observatory of Japan) Kaiki Taro INOUE (Kinki University) Masahiro NAGASHIMA

More information

Gaia Revue des Exigences préliminaires 1

Gaia Revue des Exigences préliminaires 1 Gaia Revue des Exigences préliminaires 1 Global top questions 1. Which stars form and have been formed where? - Star formation history of the inner disk - Location and number of spiral arms - Extent of

More information

Three Major Components

Three Major Components The Milky Way Three Major Components Bulge young and old stars Disk young stars located in spiral arms Halo oldest stars and globular clusters Components are chemically, kinematically, and spatially distinct

More information

What Doesn t Quench Galaxy Formation?

What Doesn t Quench Galaxy Formation? What Doesn t Quench Galaxy Formation? Phil Hopkins Dusan Keres, Claude Faucher-Giguere, Jose Onorbe, Freeke van de Voort, Sasha Muratov, Xiangcheng Ma, Lena Murchikova, Norm Murray, Eliot Quataert, James

More information

Formation of z~6 Quasars from Hierarchical Galaxy Mergers

Formation of z~6 Quasars from Hierarchical Galaxy Mergers Formation of z~6 Quasars from Hierarchical Galaxy Mergers Yuexing Li et al Presentation by: William Gray Definitions and Jargon QUASAR stands for QUASI-stellAR radio source Extremely bright and active

More information

A new mechanism for the formation of PRGs

A new mechanism for the formation of PRGs A new mechanism for the formation of PRGs Spavone Marilena (INAF-OAC) Iodice Enrica (INAF-OAC), Arnaboldi Magda (ESO-Garching), Longo Giuseppe (Università Federico II ), Gerhard Ortwin (MPE-Garching).

More information

Star formation in interacting and merging galaxies

Star formation in interacting and merging galaxies Antennae Star formation in interacting and merging galaxies Arp 220 Françoise Combes Observatoire de Paris Sapporo, February 2014 M82 N1433 1 Outline 1- How much Star Formation is enhanced in interacting/merging

More information

Compact Starbursts: Extreme Star Formation and Feedback at High Density Aleks Diamond-Stanic Grainger Fellow, University of Wisconsin

Compact Starbursts: Extreme Star Formation and Feedback at High Density Aleks Diamond-Stanic Grainger Fellow, University of Wisconsin Compact Starbursts: Extreme Star Formation and Feedback at High Density Aleks Diamond-Stanic Grainger Fellow, University of Wisconsin Arp 220 (talks by N. Scoville, D. Elbaz) 12 galaxies from our sample

More information

Disc formation and the origin of clumpy galaxies at high redshift

Disc formation and the origin of clumpy galaxies at high redshift Mon. Not. R. Astron. Soc. 397, L64 L68 (2009) doi:10.1111/j.1745-3933.2009.00685.x Disc formation and the origin of clumpy galaxies at high redshift Oscar Agertz, 1 Romain Teyssier 1,2 and Ben Moore 1

More information

The Role of Dissipation in Spheroid Formation

The Role of Dissipation in Spheroid Formation The Role of Dissipation in Spheroid Formation Philip Hopkins 4/08/08 Lars Hernquist, TJ Cox, John Kormendy, Tod Lauer, Suvendra Dutta, Dusan Keres, Volker Springel Ellipticals & Bulges: Formation in Mergers?

More information

Angular Momentum Acquisition in Galaxy Halos

Angular Momentum Acquisition in Galaxy Halos Angular Momentum Acquisition in Galaxy Halos Kyle Stewart NASA Postdoctoral Fellow Jet Propulsion Laboratory, California Institute of Technology Mentor: Leonidas Moustakas The Baryon Cycle, UC Irvine,

More information

AGN/Galaxy Co-Evolution. Fabio Fontanot (HITS)

AGN/Galaxy Co-Evolution. Fabio Fontanot (HITS) AGN/Galaxy Co-Evolution Fabio Fontanot (HITS) 21/11/2012 AGN activity in theoretical models of galaxy formation Represents a viable solution for a number of long-standing theoretical problems Properties

More information

Kinematics and Formation Mechanisms of High-Redshift Galaxies

Kinematics and Formation Mechanisms of High-Redshift Galaxies Kinematics and Formation Mechanisms of High-Redshift Galaxies White Paper Submitted to the Astro 2010 Decadal Survey Science Frontier Panel: Galaxies Across Cosmic Time (GCT) David R. Law (UC Los Angeles;

More information

Two Main Techniques. I: Star-forming Galaxies

Two Main Techniques. I: Star-forming Galaxies p.1/24 The high redshift universe has been opened up to direct observation in the last few years, but most emphasis has been placed on finding the progenitors of today s massive ellipticals. p.2/24 Two

More information

The angular momentum of z=1 star forming galaxies from deep MUSE observations

The angular momentum of z=1 star forming galaxies from deep MUSE observations The angular momentum of z=1 star forming galaxies from deep MUSE observations Nicolas Bouché T. Contini; B. Epinat + MUSE team: R. Bacon (PI); E. Emsellem; J. Brinchman; J. Richard; T. Martinsson; D. Krajnovic;

More information

MASSIVE GALAXIES IN GROUPS vs ISOLATED GALAXIES FROM HYDRODYNAMICAL SIMULATIONS

MASSIVE GALAXIES IN GROUPS vs ISOLATED GALAXIES FROM HYDRODYNAMICAL SIMULATIONS MASSIVE GALAXIES IN GROUPS vs ISOLATED GALAXIES FROM HYDRODYNAMICAL SIMULATIONS Rosa Domínguez Tenreiro (1) Paola Alpresa(1) José Oñorbe (1) Fran Martínez-Serrano (2) Arturo Serna (2) (1) Universidad Autónoma

More information

Morphologies and building blocks of galaxies at high redshift

Morphologies and building blocks of galaxies at high redshift Morphologies and building blocks of galaxies at high redshift Mariko Kubo TMT project office, NAOJ The TMT Science Forum 2016 24-26, May Galaxies in the current Universe NASA, ESA, and The Hubble Heritage

More information

Cosmological simulations of galaxy formation

Cosmological simulations of galaxy formation Cosmological simulations of galaxy formation Modern galaxy formation simulations Mock gri SDSS composite image with dust absorption based on Draine opacity model. NGC4622 as seen from HST Outline - Impact

More information

Supernova Feedback in Low and High Mass Galaxies: Luke Hovey 10 December 2009

Supernova Feedback in Low and High Mass Galaxies: Luke Hovey 10 December 2009 Supernova Feedback in Low and High Mass Galaxies: Luke Hovey 10 December 2009 Galactic Winds: Mathews, W. et al. 1971 Effects of Supernovae on the Early Evolution of Galaxies: Larson, R. 1974 The origin

More information

Orianne ROOS CEA-Saclay Collaborators : F. Bournaud, J. Gabor, S. Juneau

Orianne ROOS CEA-Saclay Collaborators : F. Bournaud, J. Gabor, S. Juneau Orianne ROOS CEA-Saclay Collaborators : F. Bournaud, J. Gabor, S. Juneau Bachelor of Physics, Master of Astrophysics Université de Strasbourg PhD, Université Paris-Diderot Observatoire de Strasbourg Les

More information

Steady outflows in giant clumps of high-z disc galaxies during migration and growth by accretion

Steady outflows in giant clumps of high-z disc galaxies during migration and growth by accretion MNRAS 432, 455 467 (2013) Advance Access publication 2013 April 12 doi:10.1093/mnras/stt480 Steady outflows in giant clumps of high-z disc galaxies during migration and growth by accretion Avishai Dekel

More information

quenching and structural & morphological evolution: physics

quenching and structural & morphological evolution: physics quenching and structural & morphological evolution: physics rachel somerville Rutgers University with thanks to: Ryan Brennan, Viraj Pandya, Ena Choi Guillermo Barro, Stijn Wuyts, Dale Kocevski, Arjen

More information

Survey of Astrophysics A110

Survey of Astrophysics A110 Goals: Galaxies To determine the types and distributions of galaxies? How do we measure the mass of galaxies and what comprises this mass? How do we measure distances to galaxies and what does this tell

More information

Angular Momentum Problems in Disk Formation

Angular Momentum Problems in Disk Formation Angular Momentum Problems in Disk Formation MPIA Theory Group Seminar, 07/03/2006 The Standard Picture Disks galaxies are systems in centrifugal equilibrium Structure of disks is governed by angular momentum

More information

The theoretical view of high-z Clusters. Nelson Padilla, PUC, Chile Pucón, November 2009

The theoretical view of high-z Clusters. Nelson Padilla, PUC, Chile Pucón, November 2009 The theoretical view of high-z Clusters Nelson Padilla, PUC, Chile Pucón, November 2009 The Plan: 1) To see what the observations are telling us using models that agree with the cosmology, and with other

More information

ASTR 610 Theory of Galaxy Formation Lecture 18: Disk Galaxies

ASTR 610 Theory of Galaxy Formation Lecture 18: Disk Galaxies ASTR 610 Theory of Galaxy Formation Lecture 18: Disk Galaxies Frank van den Bosch Yale University, spring 2017 The Structure & Formation of Disk Galaxies In this lecture we discuss the structure and formation

More information

The Iguaçu Lectures. Nonlinear Structure Formation: The growth of galaxies and larger scale structures

The Iguaçu Lectures. Nonlinear Structure Formation: The growth of galaxies and larger scale structures April 2006 The Iguaçu Lectures Nonlinear Structure Formation: The growth of galaxies and larger scale structures Simon White Max Planck Institute for Astrophysics z = 0 Dark Matter ROT EVOL Cluster structure

More information

AGN in hierarchical galaxy formation models

AGN in hierarchical galaxy formation models AGN in hierarchical galaxy formation models Nikos Fanidakis and C.M. Baugh, R.G. Bower, S. Cole, C. Done, C. S. Frenk Physics of Galactic Nuclei, Ringberg Castle, June 18, 2009 Outline Brief introduction

More information

Fundamental Planes and Galaxy Formation

Fundamental Planes and Galaxy Formation Fundamental Planes and Galaxy Formation Philip Hopkins, NoviCosmo 2007 Fundamental Planes = Scaling Laws Obeyed by Galaxies vs Origin of scaling laws: Ideally, we d understand every galaxy as an individual:

More information

Summary So Far! M87van der Maerl! NGC4342! van den Bosch! rotation velocity!

Summary So Far! M87van der Maerl! NGC4342! van den Bosch! rotation velocity! Summary So Far Fundamental plane connects luminosity, scale length, surface brightness, stellar dynamics. age and chemical composition Elliptical galaxies are not randomly distributed within the 3D space

More information

Solving. Andrey Kravtsov The University of Chicago Department of Astronomy & Astrophysics Kavli Institute for Cosmological Physics

Solving. Andrey Kravtsov The University of Chicago Department of Astronomy & Astrophysics Kavli Institute for Cosmological Physics Solving Constraining galaxy formation with gaseous halos Andrey Kravtsov The University of Chicago Department of Astronomy & Astrophysics Kavli Institute for Cosmological Physics X-ray Vision workshop:

More information

Mergers and Mass Assembly of Dark Matter Halos & Galaxies

Mergers and Mass Assembly of Dark Matter Halos & Galaxies Mergers and Mass Assembly of Dark Matter Halos & Galaxies Chung-Pei Ma Onsi Fakhouri James McBride (UC Berkeley) Mike Boylan-Kolchin (MPA --> Southern UC) Claude-Andre Faucher-Giguere Dusan Keres (Harvard

More information

Feedback in Galaxy Clusters

Feedback in Galaxy Clusters Feedback in Galaxy Clusters Brian Morsony University of Maryland 1 Not talking about Galaxy-scale feedback Local accretion disk feedback 2 Outline Galaxy cluster properties Cooling flows the need for feedback

More information

Feedback, AGN and galaxy formation. Debora Sijacki

Feedback, AGN and galaxy formation. Debora Sijacki Feedback, AGN and galaxy formation Debora Sijacki Formation of black hole seeds: the big picture Planck data, 2013 (new results 2015) Formation of black hole seeds: the big picture CMB black body spectrum

More information

Dwarf Galaxies as Cosmological Probes

Dwarf Galaxies as Cosmological Probes Dwarf Galaxies as Cosmological Probes Julio F. Navarro The Ursa Minor dwarf spheroidal First Light First Light The Planck Satellite The Cosmological Paradigm The Clustering of Dark Matter The Millennium

More information

modified gravity? Chaire Galaxies et Cosmologie XENON1T Abel & Kaehler

modified gravity? Chaire Galaxies et Cosmologie XENON1T Abel & Kaehler Dark matter or modified gravity? Chaire Galaxies et Cosmologie Françoise Combes 11 December, 2017 XENON1T Abel & Kaehler Why modified gravity? CDM models beautifully account for LSS, CMB, galaxy formation

More information

the self-regulated agn feedback loop: chaotic cold accretion

the self-regulated agn feedback loop: chaotic cold accretion the self-regulated agn feedback loop: chaotic cold accretion Massimo Gaspari Max Planck Institute for Astrophysics the self-regulated agn feedback loop: raining onto black holes Massimo Gaspari Max Planck

More information

Co-Evolution of Central Black Holes and Nuclear Star Clusters

Co-Evolution of Central Black Holes and Nuclear Star Clusters Co-Evolution of Central Black Holes and Nuclear Star Clusters Oleg Gnedin (University of Michigan) Globular clusters in the Galaxy median distance from the center is 5 kpc Resolved star cluster highest

More information

high density low density Rayleigh-Taylor Test: High density medium starts on top of low density medium and they mix (oil+vinegar) Springel (2010)

high density low density Rayleigh-Taylor Test: High density medium starts on top of low density medium and they mix (oil+vinegar) Springel (2010) GAS MIXES high density Springel (2010) low density Rayleigh-Taylor Test: High density medium starts on top of low density medium and they mix (oil+vinegar) HOT HALO highest resolved density nth= 50x10

More information

8.1 Structure Formation: Introduction and the Growth of Density Perturbations

8.1 Structure Formation: Introduction and the Growth of Density Perturbations 8.1 Structure Formation: Introduction and the Growth of Density Perturbations 1 Structure Formation and Evolution From this (Δρ/ρ ~ 10-6 ) to this (Δρ/ρ ~ 10 +2 ) to this (Δρ/ρ ~ 10 +6 ) 2 Origin of Structure

More information

The Impact of Minor Mergers

The Impact of Minor Mergers The Impact of Minor Mergers T. J. Cox (CfA) Phil Hopkins (Berkeley) Lars Hernquist (CfA) Rachel Somerville (STScI) Josh Younger (CfA) NGC 7674 Gurtina Besla (CfA), Avishai Dekel (HU), Tiziana Di Matteo

More information

Modelling star formation in galaxy formation simulations

Modelling star formation in galaxy formation simulations Modelling star formation in galaxy formation simulations Vadim Semenov (U.Chicago) Andrey Kravtsov University of Chicago Carving through the codes Davos, Switzerland 16 February, 2017 Nick Gnedin (Fermilab)

More information

Major Review: A very dense article" Dawes Review 4: Spiral Structures in Disc Galaxies; C. Dobbs and J Baba arxiv "

Major Review: A very dense article Dawes Review 4: Spiral Structures in Disc Galaxies; C. Dobbs and J Baba arxiv The Components of a Spiral Galaxy-a Bit of a Review- See MBW chap 11! we have discussed this in the context of the Milky Way" Disks:" Rotationally supported, lots of gas, dust, star formation occurs in

More information

Galaxy Activity in Semi Analytical Models. Fabio Fontanot (INAF OATs) Ljubljana 05/04/11

Galaxy Activity in Semi Analytical Models. Fabio Fontanot (INAF OATs) Ljubljana 05/04/11 Galaxy Activity in Semi Analytical Models Fabio Fontanot (INAF OATs) Ljubljana 05/04/11 Part I: Theoretical background 1. Baryonic gas falls in the gravitational potential of Dark Matter Halos 2. Baryonic

More information

Gas in and around z > 2 galaxies

Gas in and around z > 2 galaxies Gas in and around z > 2 galaxies Michele Fumagalli August 2010 Santa Cruz Xavier Prochaska Daniel Kasen Avishai Dekel In collaboration with: Daniel Ceverino Joel Primack Gas in galaxies from theory Gas

More information

Peculiar (Interacting) Galaxies

Peculiar (Interacting) Galaxies Peculiar (Interacting) Galaxies Not all galaxies fall on the Hubble sequence: many are peculiar! In 1966, Arp created an Atlas of Peculiar Galaxies based on pictures from the Palomar Sky Survey. In 1982,

More information

Dark matter and galaxy formation

Dark matter and galaxy formation Dark matter and galaxy formation Galaxy rotation The virial theorem Galaxy masses via K3 Mass-to-light ratios Rotation curves Milky Way Nearby galaxies Dark matter Baryonic or non-baryonic A problem with

More information

Galaxy Formation and Evolution

Galaxy Formation and Evolution Galaxy Formation and Evolution Houjun Mo Department of Astronomy, University of Massachusetts 710 North Pleasant Str., Amherst, MA 01003-9305, USA Frank van den Bosch Department of Physics & Astronomy,

More information

Barred Galaxies. Morphology Gas in barred galaxies Dynamics: pattern speed Theory: secular evolution, resonances

Barred Galaxies. Morphology Gas in barred galaxies Dynamics: pattern speed Theory: secular evolution, resonances Barred Galaxies Morphology Gas in barred galaxies Dynamics: pattern speed Theory: secular evolution, resonances NGC1300: SB(s) fig.6 NGC1512: SB(r) fig.3 NGC2523: SB(r) fig.2 Dust lanes NGC 1300 Star formation

More information

The Formation and Evolution of Galaxy Clusters

The Formation and Evolution of Galaxy Clusters IAU Joint Discussion # 10 Sydney, July, 2003 The Formation and Evolution of Galaxy Clusters Simon D.M. White Max Planck Institute for Astrophysics The WMAP of the whole CMB sky Bennett et al 2003 > 105

More information

Formation and growth of galaxies in the young Universe: progress & challenges

Formation and growth of galaxies in the young Universe: progress & challenges Obergurgl. April 2014 Formation and growth of galaxies in the young Universe: progress & challenges Simon White Max Planck Institute for Astrophysics Ly α forest spectra and small-scale initial structure

More information

Astronomy 330 Lecture Dec 2010

Astronomy 330 Lecture Dec 2010 Astronomy 330 Lecture 26 10 Dec 2010 Outline Clusters Evolution of cluster populations The state of HI sensitivity Large Scale Structure Cluster Evolution Why might we expect it? What does density determine?

More information

Astro 358/Spring 2008 (49520) Galaxies and the Universe

Astro 358/Spring 2008 (49520) Galaxies and the Universe Astro 358/Spring 2008 (49520) Galaxies and the Universe Figures + Tables for Lecture 13 on Tu Mar 18 Lectures 9 to 12 1) Evidence for DM ; CDM vs HDM 2) Surface brightness profile and v/σ of Disks, Bulges,

More information

Galaxy Evolution: Emerging Insights and Future Challenges. University of Texas (UT) Austin Nov 11-14

Galaxy Evolution: Emerging Insights and Future Challenges. University of Texas (UT) Austin Nov 11-14 Galaxy Evolution: Emerging Insights and Future Challenges University of Texas (UT) Austin Nov 11-14 Thank You! Department of Astronomy & Mc Donald Observatory Board of Visitors Scientific Organizing Committee

More information

PLANET FORMATION BY GRAVITATIONAL INSTABILITY? Kaitlin Kratter University of Arizona. Sagan Summer Workshop, July 2015

PLANET FORMATION BY GRAVITATIONAL INSTABILITY? Kaitlin Kratter University of Arizona. Sagan Summer Workshop, July 2015 PLANET FORMATION BY GRAVITATIONAL INSTABILITY? Kaitlin Kratter University of Arizona Sagan Summer Workshop, July 2015 PLANET FORMATION BY in GAS! GRAVITATIONAL INSTABILITY? Kaitlin Kratter University of

More information