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STRUCTURE FORMATION MATTEO VIEL INAF and INFN Trieste

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Presentation on theme: "STRUCTURE FORMATION MATTEO VIEL INAF and INFN Trieste"— Presentation transcript:

1 STRUCTURE FORMATION MATTEO VIEL INAF and INFN Trieste
SISSA LECTURE #4 – March 14th 2011

2 OUTLINE: LECTURES Structure formation: tools and the high redshift universe The dark ages and the universe at 21cm IGM cosmology at z=2=6 IGM astrophysics at z=2-6 Low redshift: gas and galaxies 6. Cosmological probes LCDM scenario

3 OUTLINE: LECTURE 4 Galactic winds and metal enrichment
The evolution of the UV background The Warm-Hot Intergalactic Medium

4 GALACTIC WINDS

5 Galactic winds –I Local galactic winds M82 X-ray
Local galactic winds M82 optical and infra-red

6 Galactic winds –II Theory: Galactic winds do they destroy the forest ?
Log overdensity Log Temp Flux Temp. Dens. Theuns, MV, et al, 2002, ApJ, 578, L5

7 Feedback effects: Galactic winds-IV
Line widths distribution Column density distribution function

8 Metal enrichment CIV systems at z=3
Strong Feedback e= Role of the UV background Mori, Ferrara, Madau 2000; Rauch, Haehnelt, Steinmetz 1996; Schaye et al. 2003 Soft background ---- Role of different feedback e=0 e=1 e=0.1

9 Observations: the POD technique
Aguirre,Schaye, Theuns, 2002, ApJ, 576, 1 Cowie & Songaila, 1998, Nature, 394, 44 Pieri & Haehnelt, 2004, MNRAS, 347, 985 Pixel-by-pixel search using higher order transitions

10 Springel & Hernquist 2002,2003

11 Observations: the POD technique-II
NO SCATTER IN THE Z-r relation SCATTER IN THE Z-r relation Good fit to the median but not for the scatter Schaye et al., 2003, ApJ, 596, 768

12 Observations: the POD technique-III
VARIANCE OF THE METALLICITY Lognormal fit Schaye et al., 2003, ApJ, 596, 768

13 When did the IGM become enriched – II ?
Adelberger et al. 2005

14 GALAXY-IGM CONNECTION
- Early or late metal enrichment???? PopIII objects?? Where are the metals? How far can they get? - Search for galactic winds. No definitive proof of galactic winds at high redshift. DEFINITIVE proof will be signatures of outflows in QUASAR PAIRS (within 2yrs)? - Lyman-break proximity effect? Is there still something odd? radiative transfer effects? - Better modelling of the ISM into cosmological hydro simulations ISM-IGM connection

15 UV BACKGROUND

16 Ionizing background – I
t ~ 1/ G -12 With the fluctuating Gunn – Peterson approximation Photoionization rate Bolton, Haehnelt, MV, Springel, 2005, MNRAS, 357, 1178

17 Ionizing background-II
Bolton, Haehnelt, MV, Springel, 2005, MNRAS, 357, 1178

18 Summary Metal enrichment: Significant progress made on the
understanding of the IGM-galaxy connection but still: No proofs of strong galactic winds at high redshfit No clues of who is polluting the IGM and to what extent. PopIII? Lyman-break galaxies? the amplitude, shape of the (fluctuating?) UV background is quite uncertain

19 WHIM

20 WHIM - I Cen & Ostriker 1999, ApJ, 514, 1L
Fukugita, Hogan, Peebles, 1998, ApJ, 503, 518

21 WHIM - II Possibility of detecting the WHIM in absorption with EDGE (Explorer of Diffuse Emission and Gamma-ray burst Explosions) characterize its physical state, spatial clustering and estimate the baryon mass density of the WHIM. - WHIM models and uncertainties. - Probability of WHIM detections. - WWHIM estimate. - Systematic effects. Joint emission+absorption analysis - Spatial distribution of WHIM and its bias

22 WHIM: model uncertainties – I
To asses model (random+systematic) uncertainties we have used different techniques to simulate WHIM

23 WHIM: model uncertainties – II
Semi analytic model (Viel et al. 2003) Hydro-dynamical model by Borgani Hydro-dynamical model (Viel 2006) = 0.7, m = , b = , h = 0.7,  = 0.85 L = 60 h -1 Mpc, , NDM = 4003, NGAS = 4003, = 2.5 h -1 kpc Gadget-2 SPH code. Metallicity model: Z/Zsun=min(0.2,0.025.r–1/3) Simple star formation prescription. No Feedback. Ions: OVI (KLL), OVIIKa, OVII Kb, OVIII, CV, NeIX, MgXI FeXVII. Hybrid collisional ionization + (X+UV) photoionization. Independent spectra drawn by stacking outputs out to z=0.5 (Dz=0.1)

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27 Minimum flux (fluence) for detection
NOVII/Dz = 4–8 NOVIII/Dz=0.6–1.3

28 OVII EW=0.1 eV OVII EW=0.072 OVII OVI EW=0.06 eV

29 WHIM as a mass tracer Galaxy Light: Tully Catalog Biasing hypothesis +
Eulerian Hydro-simulation. Flat LCDM L=25 Mpc/h. l=32.6 Kpc/h. Cen et al. 2003 Biasing hypothesis + ADDING POWER IGM distribution Gas properties OVII distribution CLOUDY

30 But see Kaastra et al. 2006 and Rasmussen et al 2006
WHIM: the observational state of the art Nicastro et al PKS 1 z~0 Nicastro et al Mark-421. 2 z~0.011 and z~0.027 NeX OVIII OVII OVII NeIX NVI CVI OVIII But see Kaastra et al and Rasmussen et al 2006

31 Best bright background sources ? GRBs
Summary - WHIM Best bright background sources ? GRBs Unambiguous WHIM at detection at z>0 ? Yes Measuring WWHIM ? Yes. e~20% Tracing Dark Matter (Wm) ? No WHIM spatial distribution ? Yes. Emission ..alternative observational strategies are also possible

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33 WHIM and feedback - II


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