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Page 1: 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,
Page 2: 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,

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, Canada)

Galaxy Formation

Page 3: 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,

• Hydrodynamic simulations of galaxies

• Rotation Curves and ISM of Dwarf Galaxies

Page 4: 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,

Numerical simulations: recent progress

• Stellar Disk and Bulge:

•is there a thin disk? Is bulge too massive?

•Angular momentum

•Tully-Fisher relation

• Feedback

• How gas gets to the disk?

• Mbaryons/Mhalo ratio

Page 5: 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,

Robertson et al. 2004

Abadi et al 2003

Hydrodynamical simulations of galaxy Hydrodynamical simulations of galaxy formation in a cosmological context.formation in a cosmological context.

(50.000 DM particles)

(40.000 DM particles)

gasstars

Page 6: 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,

A LCDM galaxy at z=0 Governato et al 04

Age > 10 Gyr

Age < 10 Gyr

Only Stars are shown (brighter colors for younger ages) boxes 40 kpc across

Disk Bulge + Stellar Halo

N>100.000

Page 7: 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,

Increasing Resolution Conserves Angular Momentum in Disks

4000 DM

10.000 DM

100.000 DM

If DM+stellar component not collisionless: Massive halo particles exchange E and J with disk particles ---> disks heat and lose angular momentum

Page 8: 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,

Angular momentum of Stellar Disks increases with resolution. Galaxies still too concentratedAbadi et al. 2003Governato et al. 2004(see also Robertson 05 Okamoto 05)

stars

Page 9: 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,

High Spin Halo(0.05)

Vc =170Km/sec

Low Spin Halo(0.01)

Vc =70Km/sec

Due to sufficient resolution 300pc disks form with the right angular momentum

Credits: Governato

Page 10: 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,

8 10^11 solar masses3 10^12 solar masses

Galaxies too concentrated. B/D 1:3 or higher.

Peak velocity higher than in the real Milky Way. No realistic

feedback yet!

Governato et al. 04 Abadi et al 03

Governato

Page 11: 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 Feedback and satellites:

No Feedback. UV+SN Feedback

Red: starsRed: starsBlue: gasBlue: gas

Total Mass 3e12 Msol Spin Parameter = 0.035 Vrot Max 270 Km/sec Formation time z = 0.75 Last major merger z=3 Frame size ~ 200 Kpc

QuickTime™ and aYUV420 codec decompressor

are needed to see this picture.

QuickTime™ and aYUV420 codec decompressor

are needed to see this picture.

Page 12: 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,

12

F.Governato: simulations with GASOLINE

QuickTime™ and aYUV420 codec decompressor

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Page 13: 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,

13

QuickTime™ and aYUV420 codec decompressor

are needed to see this picture.

Page 14: 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,

14

F.Governato: simulations

with GASOLINE

QuickTime™ and aYUV420 codec decompressor

are needed to see this picture.

Page 15: 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,

How gas gets to the disk

• The old picture is wrong: do not even think about spherical accretion and shocking to virial temperature

• Still not clear what fraction of gas comes with satellites and what comes with filaments

Page 16: 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,

1 Mpc scale

100 kpc scale

Tgas

Gas density

Credits: Kravtsov 100pc resolution Z=4

Page 17: 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,

350kpc

Z=2.5

40pc resolution. Mvir(z=0)=1.e12Msun. Ndm=400K

Page 18: 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,

350kpc

Z=2.5

Page 19: 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,

115kpc

Page 20: 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,

7kpc

Page 21: 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,

7kpc

Page 22: 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,
Page 23: 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,

Isolated galaxies

•Observations•Simulations

Page 24: 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,

Simon etal 04: NGC 4605 Vmax =100km/s

-- Usual problems with NFW.

-- Disk is important: normal M/LR=1 M/LK= 0.5

1arcmin

Page 25: 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,

Simon etal 04 NGC 4605

POSS II

Changes in PA and inclination in central 1kpc are consistent with a weak bar

Page 26: 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,

DDO 47:Vmax = 80km/s

Distance = 4Mpc

HI is very lumpy

Stellar light does not align with HI

Page 27: 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,

• A large fraction of dwarf Galaxies in the central 1kpc has a maximal disk with expected stellar population (judging by colors).

• Signs of a weak bar are frequent.• ISM is very clumpy.

Observations:

Page 28: 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,

LMC HI distribution Venn+Stavely Smith 2003)LMC HI distribution Venn+Stavely Smith 2003)

Cosmological Simulations: feeback, 300pc resolution …

Governato 2004Multiphase ISM is nicely reproduced

Page 29: 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,

Valenzuela et al 05

Isolated Galaxy:

NFW halo 1-2M particles

Exponential disk 200K particles

Gas 100K

Resolution 50-100 pc

Star formation, feedback ….

Stars: phase-on

Two simulations:

dwarf: 60km/s

M33-type: 120km/s

Code: GASOLINE

Page 30: 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,

Stars

YoungStars

T<0.5Gyrs

Cold GasT<1.5e4

Hot GasT=1e5 K

Page 31: 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,

Cold GasT<1.5e4

Hot GasT=1e5 K

Stars

YoungStars

T<0.5Gyrs

Page 32: 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,

• Cold gas hardly shows any traces of the bar.• Filaments and lumps of cold gas • Large bubbles filled by 105K gas• Stellar feedback feeds the multiphase ISM

Page 33: 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,

Rotation Curves:

Cold and Hot gas

Little difference

Page 34: 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,

Gas Rotation

Circular Velocity

Asymmetric drift (aka Asymmetric drift (aka random motions) random motions) cannot help to explain cannot help to explain why gas rotates too why gas rotates too slowslow

Rms Velocities < 20km/s

Page 35: 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,

Recovering total density

Page 36: 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,

Another simulation: dwarf 5

Resolution: 60pc

starsCold gas

dm

baryons

Gas rms velocity

Valenzuela, Rhee, Klypin, Governato et al. 2005

Models of NGC3109 and NGC6822

Page 37: 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,

Cold Gas density in the central 2kpc region:

Clear signs of multiphase medium

Page 38: 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,

Cold/Hot Gas: density

Stars

Cold Gas:velocity

Page 39: 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,

NGC 6822

Observations

Vcirc(total)

Magellanic-type dwarf irregular

0.5Mpc from Milky Way

Page 40: 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,

• -In dwarf galaxies gas does not rotates fast enough: Vgas < Vcirc•-Non-circular velocities are not large enough to account for the difference•-Pressure support from 1e5K gas is one of key ingredients

Core is ‘observed’ where there is a real cusp.

CONCLUSIONS

Page 41: 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,

Structure of the ISM at z= 0.5 (several 10^6 particles per halo, gas clouds resolved down to 10^5 solar masses)

Ram Pressure Stripping

Cold Gas in Disks

High Velocity Clouds Gas Rich Satellites

Hot Halo (Blue)

Page 42: 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,

Bars in galaxies:

Simulations with ART and Gadget.

50-100pc resolution

200K disk particles

2M dm particles.

Dt =1e4 yrs