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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,

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Presentation on theme: "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,"— Presentation transcript:

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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, Canada) Galaxy Formation

3 Hydrodynamic simulations of galaxies Rotation Curves and ISM of Dwarf Galaxies

4 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

5 Robertson et al. 2004 Abadi et al 2003 Hydrodynamical simulations of galaxy formation in a cosmological context. (50.000 DM particles) (40.000 DM particles) gasstars

6 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

7 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

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

9 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

10 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

11 The Feedback and satellites : No Feedback.UV+SN Feedback Red: stars Blue: 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

12 12 F.Governato: simulations with GASOLINE

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14 14 F.Governato : simulations with GASOLINE

15 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

16 1 Mpc scale 100 kpc scale T gas Gas density Credits: Kravtsov 100pc resolution Z=4

17 350kpc Z=2.5 40pc resolution. Mvir(z=0)=1.e12Msun. Ndm=400K

18 350kpc Z=2.5

19 115kpc

20 7kpc

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23 Isolated galaxies Observations Simulations

24 Simon etal 04: NGC 4605 Vmax =100km/s -- Usual problems with NFW. -- Disk is important: normal M/L R =1 M/L K = 0.5 1arcmin

25 Simon etal 04 NGC 4605 POSS II Changes in PA and inclination in central 1kpc are consistent with a weak bar

26 DDO 47: Vmax = 80km/s Distance = 4Mpc HI is very lumpy Stellar light does not align with HI

27 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:

28 LMC HI distribution Venn+Stavely Smith 2003) Cosmological Simulations: feeback, 300pc resolution … Governato 2004 Multiphase ISM is nicely reproduced

29 Valenzuela et al 05 Isolated Galaxy: NFW halo1-2M particles Exponential disk 200K particles Gas100K Resolution50-100 pc Star formation, feedback …. Stars: phase-on Two simulations: dwarf: 60km/s M33-type: 120km/s Code: GASOLINE

30 Stars Young Stars T<0.5G yrs Cold Gas T<1.5e4 Hot Gas T=1e5 K

31 Cold Gas T<1.5e4 Hot Gas T=1e5 K Stars Young Stars T<0.5G yrs

32 Cold gas hardly shows any traces of the bar. Filaments and lumps of cold gas Large bubbles filled by 10 5 K gas Stellar feedback feeds the multiphase ISM

33 Rotation Curves: Cold and Hot gas Little difference

34 Gas Rotation Circular Velocity Asymmetric drift (aka random motions) cannot help to explain why gas rotates too slow Rms Velocities < 20km/s

35 Recovering total density

36 Another simulation: dwarf 5 Resolution: 60pc stars Cold gas dm baryons Gas rms velocity Valenzuela, Rhee, Klypin, Governato et al. 2005 Models of NGC3109 and NGC6822

37 Cold Gas density in the central 2kpc region: Clear signs of multiphase medium

38 Cold/Hot Gas: density Stars Cold Gas:velocity

39 NGC 6822 Observations Vcirc(total) Magellanic-type dwarf irregular 0.5Mpc from Milky Way

40 -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

41 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)

42 Bars in galaxies: Simulations with ART and Gadget. 50-100pc resolution 200K disk particles 2M dm particles. Dt =1e4 yrs


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