The Main Mode of Galaxy/Star Formation? Avishai Dekel, HU Jerusalem Leiden, September 2008 HU Flow Team Birnboim, Freundlich, Goerdt, Neistein, Zinger.

Slides:



Advertisements
Similar presentations
arvard.edu/phot o/2007/m51/. Confronting Stellar Feedback Simulations with Observations of Hot Gas in Elliptical Galaxies Q. Daniel Wang,
Advertisements

The main growth modes of disks, bulges, and central black holes: Mergers - Violent Instabilities - Secular Evolution Frédéric Bournaud - CEA Saclay with.
Daniel Ceverino (HU) Potsdam, 2009 Avishai Dekel (HU), Reem Sari(HU), Tobias Goerdt(HU), Anatoly Klypin (NMSU) High-Redshift Clumpy Disks & Bulges in Cosmological.
The Thick Disks of Spiral Galaxies as Relics from Gas-Rich, Turbulent, Clumpy Disks at High Redshifts Frédéric Bournaud, Bruce G. Elmegreen, and Marie.
Effects of galaxy formation on dark matter haloes Susana Pedrosa Patricia Tissera, Cecilia Scannapieco Chile 2010.
The Role of Dissipation in Galaxy Mergers Sadegh Khochfar University of Oxford.
GALAXIES IN DIFFERENT ENVIRONMENTS: VOIDS TO CLUSTERS:  Simulations will require to model full physics:  Cooling, heating, star formation feedbacks…
Formation of Globular Clusters in  CDM Cosmology Oleg Gnedin (University of Michigan)
AGN in hierarchical galaxy formation models Nikos Fanidakis and C.M. Baugh, R.G. Bower, S. Cole, C. Done, C. S. Frenk Accretion and ejection in AGN, Como,
Mathieu PUECH GEPI Observatoire de Paris Rebuilding discs with gas-rich major merger ESO 3D2014 – March 2014, R. Delgado, M. Rodrigues, S. Fouquet + J.L.
Forming Early-type galaxies in  CDM simulations Peter Johansson University Observatory Munich Santa Cruz Galaxy Workshop 2010 Santa Cruz, August 17 th,
How Do Galaxies Get Their Gas? astro-ph/ Dušan Kereš University of Massachusetts Collaborators: Neal Katz, Umass David Weinberg, Ohio-State Romeel.
Chania, Crete, August 2004 “The environment of galaxies” Pierre-Alain Duc Recycling in the galaxy environment F. Bournaud J. Braine U. Lisenfeld P. Amram.
Numerical issues in SPH simulations of disk galaxy formation Tobias Kaufmann, Lucio Mayer, Ben Moore, Joachim Stadel University of Zürich Institute for.
Anatoly Klypin New Mexico State University Also: Stefan Gottloeber (Astrophysikalisches Institut Potsdam ) Gustavo Yepes (UAM, Madrid) Andrey Kravtsov.
The two phases of massive galaxy formation Thorsten Naab MPA, Garching UCSC, August, 2010.
How Galaxies Assemble Romeel Davé, Univ. of Arizona With: Dušan Kereš & Neal Katz (U.Mass), and David Weinberg (Ohio State)
Merger Histories of LCDM Galaxies: Disk Survivability and the Deposition of Cold Gas via Mergers Kyle Stewart AAS Dissertation Talk 213 th AAS Meeting.
Simulating the Cooling Flow of Cool-Core Clusters Yuan Li Advisor: Greg Bryan Department of Astronomy, Columbia University July 2011.
June th Birmingham-Nottingham Extragalactic Workshop A NEW STRATEGY WITH UNAVOIDABLE PARAMETERS ONLY Dept. Astronomy & Meteorology Institut.
Bi-modality and Do w n s i z i n g Avishai Dekel HU Jerusalem Bernard ’ s Cosmic Stories, Valencia, June 2006 Origin of E vs S Galaxies.
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.
Dark Matter and Galaxy Formation (Section 3: Galaxy Data vs. Simulations) Joel R. Primack 2009, eprint arXiv: Presented by: Michael Solway.
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,
A.Kravtsov (U.Chicago) D. Ceverino (NMSU) O. Valenzuela (U.Washington) G. Rhee (UNLV) F. Governato, T.Quinn, G.Stinson (U.Washington) J.Wadsley (McMaster,
The Dark Universe Dark Matter Matters! Exploring the Dark Universe June 28-29, 2007 Indiana University.
Cosmological formation of elliptical galaxies * Thorsten Naab & Jeremiah P. Ostriker (Munich, Princeton) T.Naab (USM), P. Johannson (USM), J.P. Ostriker.
TURBULENCE AND HEATING OF MOLECULAR CLOUDS IN THE GALACTIC CENTER: Natalie Butterfield (UIowa) Cornelia Lang (UIowa) Betsy Mills (NRAO) Dominic Ludovici.
Galaxies…. + On the largest scales… they trace the cosmic structure as the “living fossils” of the earliest density fluctuations of the universe They are.
Overview of Astronomy AST 200. Astronomy Nature designs the Experiment Nature designs the Experiment Tools Tools 1) Imaging 2) Spectroscopy 3) Computational.
Superbubble Driven Outflows in Cosmological Galaxy Evolution Ben Keller (McMaster University) James Wadsley, Hugh Couchman CASCA 2015 Paper: astro-ph:
Lecture 3 - Formation of Galaxies What processes lead from the tiny fluctuations which we see on the surface of last scattering, to the diverse galaxies.
Galactic Metamorphoses: Role of Structure Christopher J. Conselice.
Radio Jet Disruption in Cooling Cores OR, can radio jets solve the cooling core problem? OR, how do cooling cores disrupt radio jets?
Cosmological Galaxy Formation
Entropy Generation in the ICM Institute for Computational Cosmology University of Durham Michael Balogh.
The co-evolution of massive ellipticals & their black holes Thorsten Naab University Observatory, Munich 8 th Sino-German Workshop on Galaxy Formation.
“Nature and Descendants of Sub-mm and Lyman-break Galaxies in Lambda-CDM” Juan Esteban González Collaborators: Cedric Lacey, Carlton Baugh, Carlos Frenk,
Virial shocks in galaxy and cluster halos
In, Out, and Around: An Overview from Simulations David Weinberg, Ohio State University Collaborators: Amanda Brady Ford, Romeel Davé, Mark Fardal, Neal.
Ben Moore, Institute for Theoretical Physics, University of Zurich +Oscar Agertz, Roman Teyssier+ Galaxy formation: is the end in sight? Obergurgl, December.
Modeling the dependence of galaxy clustering on stellar mass and SEDs Lan Wang Collaborators: Guinevere Kauffmann (MPA) Cheng Li (MPA/SHAO, USTC) Gabriella.
Gas mixing and Star formation by shock waves and turbulence Claudio Melioli Elisabete M. de Gouveia Dal Pino (IAG-USP)
Spiral Triggering of Star Formation Ian Bonnell, Clare Dobbs Tom Robitaille, University of St Andrews Jim Pringle IoA, Cambridge.
BX663 (2.4) MD 41 (2.2) K20-9 (2.0) K20-7 (2.2) K20-8 (2.2) D3a 4751 (2.27) SA (2.3)
Cool Halo Gas in a Cosmological Context Kyle Stewart “Team Irvine” UC Santa Cruz Galaxy Formation Workshop Kyle Stewart “Team Irvine” UC Santa.
Feedback Observations and Simulations of Elliptical Galaxies –Daniel Wang, Shikui Tang, Yu Lu, Houjun Mo (UMASS) –Mordecai Mac-Low (AMNH) –Ryan Joung (Princeton)
野口正史 (東北大学).  Numerical simulation Disk galaxy evolution driven by massive clumps  Analytical model building Hubble sequence.
Population of Dark Matter Subhaloes Department of Astronomy - UniPD INAF - Observatory of Padova Carlo Giocoli prof. Giuseppe Tormen May Blois.
Observing the End of Cold Flow Accretion: Co-rotation of Cool Halo Gas as a Signature of Cosmological Gas Accretion Kyle Stewart NASA Postdoctoral Fellow,
Cosmology and Dark Matter III: The Formation of Galaxies Jerry Sellwood.
Gas Accretion and Secular Processes 1  How much mass assembled in mergers?  How much through gas accretion and secular evolution? Keres et al 2005, Dekel.
How do Galaxies Get Their Gas? Dušan Kereš Institute for Theory and Computation - Harvard-Smithsonian CFA Collaborators: Neal Katz, David Weinberg, Romeel.
The cold component of cluster accretion Yuval Birnboim Jerusalem 2011.
Semi-analytical model of galaxy formation Xi Kang Purple Mountain Observatory, CAS.
OWLS: OverWhelmingly Large Simulations The formation of galaxies and the evolution of the intergalactic medium.
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: )
Preventing Star and Galaxy Formation Michael Balogh Department of Physics and Astronomy University of Waterloo.
The Physics of Galaxy Formation. Daniel Ceverino (NMSU/Hebrew U.) Anatoly Klypin, Chris Churchill, Glenn Kacprzak (NMSU) Socorro, 2008.
Arman Khalatyan AIP 2006 GROUP meeting at AIP. Outline What is AGN? –Scales The model –Multiphase ISM in SPH SFR –BH model Self regulated accretion ?!
ARCCOS Centre of Excellence in Evolutionary Cosmology University of Central Lancashire Galaxies on a Mesh Brad Gibson Stephanie Courty, Chris Brook, Patricia.
BULGE FRACTION AND DISTRIBUTION OF STAR FORMATION IN SAMI GALAXIES Greg Goldstein PhD student, Dept of Physics and Astronomy, Macquarie University Supervisors:
Cooling, AGN Feedback and Star Formation in Simulated Cool-Core Galaxy Clusters Yuan Li University of Michigan Collaborators: Greg L. Bryan (Columbia)
Cold streams as Lyman-alpha blobs Collaborators: Avishai Dekel, Amiel Sternberg, Daniel Ceverino, Romain Teyssier, Joel Primack Tobias Goerdt.
Towards Realistic Modeling of Massive Star Clusters Oleg Gnedin (University of Michigan) graduate student Hui Li.
On the Origin of Galaxy Morphology in a Hierarchical Universe
Lecture On the Origin of Galaxy Bi-modality: Cold Flows, Clustering and Feedback Observed bi-modality Shock heating vs cold flows Cold filaments in hot.
Outline Part II. Structure Formation: Dark Matter
Outline Part II. Structure Formation: Dark Matter
The SINS survey of galaxy kinematics at z~2 : turbulent thick disks and evidence for rapid secular evolution Reinhard Genzel, Natascha Förster Schreiber,
Presentation transcript:

The Main Mode of Galaxy/Star Formation? Avishai Dekel, HU Jerusalem Leiden, September 2008 HU Flow Team Birnboim, Freundlich, Goerdt, Neistein, Zinger Simulations Teyssier, Pichon, Kravtsov Massive Disk Buildup & Breakup by Cold Streams at z=2-3

Outline Massive galaxies at high z: ‘’narrow cold streams through hot halos Inflow rate into the halo and into the disk Smooth flows vs Mergers High-SFR galaxies at z=2-3 Disk breakup and bulge formation

Shock-Heating Scale M vir [M ʘ ] Birnboim & Dekel 03 Dekel & Birnboim 06 stable shock unstable shock typical halos 6x10 11 M ʘ Keres et al 05

Gas through shock: heats to virial temperature compression on a dynamical timescale versus radiative cooling timescale Shock-stability analysis (Birnboim & Dekel 03): post-shock pressure vs. gravitational collapse

The Critical Mass: Cosmological Simulations virial radius SPH Keres et al 2005, AMR Kravtsov et al M<<10 12 M ʘ cold flows M>10 12 M ʘ virial shock heating

Fraction of Cold Gas in Halos: Cosmological simulations (Kravtsov) ‏ Birnboim, Dekel, Neistein 2007 cold hot Zinger, Birnboim, Dekel, Kravtsov

Libeskind, Birnboim, Dekel 08 d(Entropy)/dt A virial shock in a 3D cosmological simulation: at M crit – rapid expansion from the inner halo to R vir

Cold Streams in Hot Massive Halos at High z Dekel & Birnboim 2006 Dekel et al. 2008

At High z, in Massive Halos: Cold Streams in Hot Halos Totally hot at z<1 in M>M shock Cold streams at z>2 shock no shock cooling Dekel & Birnboim 2006

density Temperature adiabatic infall shock- heated cold flows disk Analysis of Eulerian hydro simulations by Birnboim, Zinger, Dekel, Kravtsov Mass Distribution of Halo Gas

M*M* M vir [M ʘ ] all hot redshift z all cold cold filaments in hot medium M shock M shock >>M * M shock ~M * Cold Streams in Big Galaxies at High z Dekel & Birnboim 06 Fig. 7

the millenium cosmological simulation high-sigma halos: fed by relatively thin, dense filaments → cold narrow streams typical halos: reside in relatively thick filaments, fed ~spherically → no cold streams

M s ~M * M s >>M * Large-scale filaments grow self-similarly with M * (t) and always have typical width ~R * ∝M * 1/3 At high z, M shock halos are high-σ peaks: they are fed by a few thinner filaments of higher density Origin of dense filaments in hot halos ( M ≥ M shock ) at high z At low z, M shock halos are typical: they reside in thicker filaments of comparable density

Dark-matter inflow in a shell 1-3R vir M>>M * radial velocity temperature density one thick filament several thin filaments Seleson & Dekel M~M *

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

Gas Density in Massive Halos 2x10 12 M ʘ Ocvirk, Pichon, Teyssier 08 high z low z M=10 12 M ʘ

Critical Mass in Cosmological Simulations Ocvirk, Pichon, Teyssier 08 M stream M shock DB06 cold filaments in hot medium

Observed Maximum Bursts - Optical/UV-selected galaxies at z~ M star ~10 11 M ʘ SFR ~ 200 M ʘ yr -1 - Most of the mass is bursting -> gaseous input - Very rapid SFR: burst ~0.5 Gyr...t SFR < R vir /V vir ~ t cool << t Hubble - Disk morphology & kinematics: no major mergers Genzel et al. 2006, …

Massive high-z disks by cold narrow streams Dekel et al. 2008, Nature MareNostrum AMR simulation 50 Mpc cosmological box 1 kpc resolution Ocvirk, Pichon, Teyssier 2008 M vir =10 12 M ʘ at z=2.5

Gas density following dark-matter filaments

Entropy: virial shock & low-entropy streams

Inward gas flux: all in the streams.

Another example Always 3 streams?

Flux per solid angle

Average Assembly Rate into R vir by EPS Neistein, van den Bosch, Dekel 06; Birnboim, Dekel, Neistein 07; Neistein & Dekel 07, 08 Growth rate of main progenitor (time invariant): Approximate for LCDM ~ M=2x10 12 M ʘ z=2.2  dM/dt ~ 200 M ʘ yr -1 May explain high-SFR galaxies if - a similar flux penetrates to the disk - it is gas rich - SFR follows rapidly

Inflow Rate into the Disk ~~ At z~2-3, M~10 12 M ʘ, the input rate into the disk is comparable to the infall rate into the virial shock, most of it along narrow streams

Conditional Distribution of Gas Inflow Rate mergers >1:10 smooth flows

Assume scaling of P(Mdot|M) ‏ P(M) by Sheth-Tormen Comoving Number Density of Galaxies as a function of gas inflow rate Gas inflow rate > SFR but by a small margin  SFR very efficient! Star-Forming Gal’s Sub-Millimeter Gal’s SFR= prediction, e.g., n=2x10 -4 SFR<200

Contribution of Different Masses <12.5

At Different Redshifts 3 4 similar n(>SFR) at z=2-3

Streams in 3D: partly clumpy

Half the stream mass is in clump >1:10 Birnboim, Zinger, Dekel, Kravtsov

Inflow Rate into the Disk 50% of the flux is in mergers > 1:10 but the duty cycle is < 10%

Fraction of Mergers BzK/BX/BM are mostly mini-minor mergers <1:10, i.e. smooth flows Bright SMG are half-and-half mergers >1:10 and smooth flows SFG: Stream-Fed Galaxies At a given Mdot, 75% of the galaxies are fed by smooth flows

M*M* M vir [M ʘ ] all hot redshift z all cold cold filaments in hot medium M shock Stream Flux in halos of M at z

Streams – Clumpy Disk - Bulge ~ One stream with impact parameter ~ R disk determines the disk spin, while other streams generate turbulence The streams provide continuous rapid gas supply into a disk  Jeans instability At z>2, the streams maintain high dispersion:  Giant clumps. They interact, lose AM, and coalesce into a compact spheroid - “classical bulge” (Noguchi 99; Elmegreen, Bournaud, Elmegreen 08)

merger h halos accretion disk Old Paradigm radiative cooling cold hot cold gas  young stars spheroid  old stars

hot halo spheroid clumpy disk New Paradigm z>2 clumpy disk spheroid cold streams hot halo thick disk M v >10 12 z<1 new disk

Detectable by absorption: External source: c.d.>20 cm -2 at 30% sky coverage Internal source: c.d.>21 cm -2 at 5% sky coverage Column density of cold, in-streaming gas

Here is what it should look like in H α

M*M* M vir [M ʘ ] all hot redshift z all cold cold filaments in hot medium M shock M shock >>M * M shock ~M * When and where did most stars form? Dekel & Birnboim 06 ~ at z=2-3 in galaxies of ~10 11 M ʘ by cold streams

Conclusions: SFG = Stream-Fed Galaxies =2-3,~ At z=2-3, “disks” of ~10 11 M ʘ grow rapidly via narrow cold gas streams through shock-heated halos ~~ 200 M ʘ yr -1 Penetration: disk input rate ~ halo entry rate ~ 200 M ʘ yr -1 Streams are half Streams are half clumps >1:10 and half smooth, merger duty cycle <0.1 ~~ Abundance: SFR>150 at n~3x10 -4, SFR>500 at n~6x10 -5 Most sBzK/BX/BM are fed by smooth streams in halos M ʘ Half the SMG are mergers >1:10 At z>2, streams generate rotation & maintain gas-rich & turbulent disk  giant clumps  (1) SFR & (2) coalescence into a spheroid The cold streams should be detectable at z>2 in absorption and emission (DLAS? Lyman-limit? Lyman-alpha emitters?) ‏ Observed SFGs  SFR must closely follow gas input rate