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GALAXIES IN DIFFERENT GALAXIES IN DIFFERENT ENVIRONMENTS: ENVIRONMENTS: VOIDS TO CLUSTERS: VOIDS TO CLUSTERS: Simulations will require to model full physics: Cooling, heating, star formation feedbacks… Large dynamical range: resolving galaxies in different density environments. Important problems to address: Excess of small scale structure in CDM models: making small halos invisible?. Hubble sequence (formation of disks) Interactions galaxy -ICM

GALAXIES IN DIFFERENT ENVIRONMENTS: VOIDS TO CLUSTERS:

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GALAXIES IN DIFFERENT ENVIRONMENTS: VOIDS TO CLUSTERS:. Simulations will require to model full physics: Cooling, heating, star formation feedbacks… Large dynamical range: resolving galaxies in different density environments. Important problems to address: - PowerPoint PPT Presentation

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Page 1: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

GALAXIES IN DIFFERENT GALAXIES IN DIFFERENT ENVIRONMENTS: ENVIRONMENTS:

VOIDS TO CLUSTERS:VOIDS TO CLUSTERS: Simulations will require to model full physics:

Cooling, heating, star formation feedbacks… Large dynamical range: resolving galaxies in

different density environments. Important problems to address:

Excess of small scale structure in CDM models: making small halos invisible?.

Hubble sequence (formation of disks) Interactions galaxy -ICM

Page 2: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

GALAXIES IN VOIDSGALAXIES IN VOIDS

M. Hoeft, G. Yepes, S. Gottlober and V. SpringelM. Hoeft, G. Yepes, S. Gottlober and V. Springelastro-ph / 0501394astro-ph / 0501394

Page 3: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Void dwarf dark halos.Void dwarf dark halos.

Gottlöber et al 03Void dwarf galax

Page 4: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Halo Mass function in VoidsHalo Mass function in Voids

Page 5: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

The missing dwarf galaxy problemin VOIDS

● No galaxies brighter than Mb=-15 found.

● What happens with baryons of small halos in voids?– Are they visible but faint?. Magnitude, colors. (Red Dwarfs)

– Are they just baryonless dark halos?

● What are the physical mechanism – Gas evaporation by UV photoionization

– Supernova feedback (e.g Dekel & Silk)

● What is the typical halo mass for this to happen?

Page 6: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

VOIDS FROM A 80/h Mpc Box

1024102433 effective particle in void region effective particle in void region MMgas gas = = 5.5106 M MMdark dark = = 3.4107 M Smoothing= 2-0.8 kpcSmoothing= 2-0.8 kpc

10/h Mpc10/h Mpc Simulations done with GADGET2Simulations done with GADGET2Primordial CoolingPrimordial CoolingPhotoionization Photoionization Multiphase mediumMultiphase mediumStar formationStar formationFeedback Feedback

ThermalThermalKinetic (Winds)Kinetic (Winds)

Page 7: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:
Page 8: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

• 20483 effective particles

• RUN with 10243

– Mgas = 1.5106 M

– Mdark= 8.2106 M

Spatial smoothing= 0.5 kpc

Different feedback params.

• Same void was resimulated

with full resolution 20483 – Mgas 2 105 M

– Mdark 106 M

– Spatial smoothing= 0.5 kpc

(ULTRA)HIGH-RESOLUTION SIMULATIONS OF A VOID IN THE 50/h Mpc Box

10/h Mpc10/h Mpc

Page 9: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

The missing dwarf galaxy problemin VOIDS

● No galaxies brighter than Mb=-15 found.

● What happens with baryons of small halos in voids?– Are they visible but faint?. Magnitude, colors. (Red Dwarfs)

– Are they just baryonless dark halos?

● What are the physical mechanism – Gas evaporation by UV photoionization

– Supernova feedback (e.g Dekel & Silk)

● What is the typical halo mass for this to happen?

Page 10: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Baryon fractionBaryon fraction

Halos belowfew times109 Msun

arebaryon-poor

Characteristicmass scaledepends onredshift

Baryon fract

Page 11: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Characteristic massCharacteristic mass Mc

baryon-rich

baryon-poor

Mc risessignificantlywith z

Halo may startbaryon-richand becomelaterbaryon-poor

Char mass

Page 12: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Tentry

Density temperature phase spaceDensity temperature phase space

Cold modeof galactic gasaccretion:gas creeps alongthe equilibriumline betweenheating and cooling(Keres et al. 04)

Rho T

Page 13: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Max gas temperature

Relate radius to mass

Prediction for Mc

Measurement Mc

Condition for suppression

How to suppress gas condensation?How to suppress gas condensation?How to

Page 14: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Entry temperature versus characteristic massEntry temperature versus characteristic mass

General scaling:factor 1.3

High redshift:empty halos has todevelop

T entry

Page 15: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Mass accretion historyMass accretion historyMass accr hist

Page 16: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Baryon poor small halosBaryon poor small halosMAH, several

total mass baryonic (condensed) mass

Page 17: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Age of starsAge of stars

In small halosstars can onlybe formed at highredshift

Age

Page 18: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Thermal feedbackThermal feedback

Strong wind modelStrong wind model

z=0z=0

Luminosity functionLuminosity function

Page 19: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Color evolutionColor evolution

z=0z=0

z=1z=1

Page 20: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

SOME CLUES ABOUT DWARF SOME CLUES ABOUT DWARF GALAXIES IN VOIDSGALAXIES IN VOIDS

Halos below Mlim~ 7x109 M (vc ~27 km/s) are photo-evaporated and have almost no baryon content, either cold gas or stars. This mass scale decreases with redshift. Very small dependence of UV flux.

UV-heating not able to suppress small galaxies: Problem for semianalitical models to explain substructure in the Local Group.

Thermal feedback does not play a significant role in keeping gas out of halos.

Kinetic feedback (winds) can be very efficient in inhibitting star-formation: Z agreement, redder colors,

Page 21: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

WORK IN PROGRESS...

Page 22: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

DWARF GALAXIES IN GROUPS:

Page 23: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:
Page 24: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Group five

Page 25: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Baryonfraction againBaryonfraction again

Baryonfraction again

Page 26: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Metallicity enrichment:Metallicity enrichment:Remove baryons by feedback?Remove baryons by feedback?

Dekel+Woo

Feedback

Page 27: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

GALAXIES IN CLUSTERSGALAXIES IN CLUSTERS

Entropy generation from galactic feedback.

Scaling relations and non-adiabatic physics.

Understanding Intracluster light.

Effect of central Cd-galaxy on ICM radial profiles.

Cold fronts and cold flows.

How many galaxies survive in the cluster environment?

Very demanding simulations:

E.g. Cluster 6 simulated with 4.5 million particles within 3 virial radius took more than 680,000 timesteps to finished.

Page 28: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

STAR FORMATION IN STAR FORMATION IN CLUSTERS CLUSTERS

PhotonisationPhotonisationCoolingCoolingMultiphase mediumMultiphase mediumMetallicity Metallicity Wind modelWind model

Springel & Herquist 2003Springel & Herquist 2003

Obtain observational Obtain observational properties of dark halos from properties of dark halos from stars using BC2003 SSP stars using BC2003 SSP models models

Study Study

Page 29: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

CDM CLUSTER SIMULATIONSCDM CLUSTER SIMULATIONS

m=0.3; =0.7, h=0.7;

8=0.9

● 80/h Mpc box size. (Initial P(k) for 10243)

● Resample to 1283 particles.

● Identify clusters for

resimulation

GADGET (2-5 kpc)

Page 30: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Z=1; =3 A=1

z=0

Page 31: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

LARGE-SCALE SPH SIMULATIONS

m=0.3; =0.7, h=0.7;

8=0.9, b=0.045

500/h Mpc box size. (Initial P(k) for 20483) Runs with up to 5123 particles.

# Halos=4x105 (M>1012 M)

Mdark= 7x1010 M

Identify clusters for

resimulation with 1283

Mass of clusters Mcluster 2.51015 M

Same resolution than

previous simulations 500 h500 h-1-1 Mpc Mpc

Page 32: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Z=1; =3 A=1

z=0

Page 33: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Lx-Tx

TTxx1.91.9

. . MMvirvir > 10 > 1015 15 MM

. 10. 1014 14 < M < Mvirvir < 10 < 101515

.2x10.2x101313 < M < Mvirvir < 10 < 101414

Clusters at 500 Mpc/h

Page 34: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Lx-Tx

. . MMvirvir > 10 > 1015 15 MM

. 10. 1014 14 < M < Mvirvir < 10 < 101515

.2x10.2x101313 < M < Mvirvir < 10 < 101414

TTxx1.91.9

Observations

Clusters at 500 Mpc/h

Page 35: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

Lx-Tx

. . MMvirvir > 10 > 1015 15 MM

. 10. 1014 14 < M < Mvirvir < 10 < 101515

.2x10.2x101313 < M < Mvirvir < 10 < 101414

TTxx1.91.9

Observations

Clusters at 500 Mpc/h

Resimulated clusters at 80 Mpc/h

Page 36: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

X-ray Temperature Function

Page 37: GALAXIES  IN DIFFERENT ENVIRONMENTS:  VOIDS TO CLUSTERS:

LARGE-SCALE SPH SIMULATIONS

The MareNostrum Universe Simulation:

500/h Mpc box size. (Initial P(k) for 20483)

2x10243 particles. # Halos=106 (M>1012 M)

Mdark= 1010 M

Resolution 15 kpc.

500 h500 h-1-1 Mpc Mpc