1. Ch.5

2. absorption lines * QSO z em z abs <z em they allow to use quasars as cosmological probes to study the Universe at large distances and large look-back times absorption line system: system of absorption lines at the same z abs, presumably associated with the same absorber

3. absorption lines study of great potential interest to investigate the gas distribution in the Universe difficulties: * weak and unresolved lines need high spectral resolution, and high S/N ratio for weak sources need big telescopes * study must be done as a function of redshift need wide spectral range every given QSO can include between 0 and hundreds of absorption lines in his spectrum, depending on (1) redshift z em (2) observed spectral region (3) limit EW (function of spectral resolution and S/N ratio) most common lines: Lyalpha 1216, CIV 1548,1551, MgII 2795,2802 other common lines: CII 1335, Si IV1394,1403, MgI 2852

4. absorption lines “metal” line system “damped” Lyα large column density, probably due to the cross of a galactic disk

5. absorption lines Lyα systems Ly limit system

6. Broad Absorption Lines and BAL QSOs BAL QSOs are: X-ray-weak, lower than for non-BAL usually radio quiet broad (10 4 km/s) profiles PCygni-like, absorptions shifted by ~ 30000 km/s probably associated with outflows from nuclear region Gibson et al 2008 intrinsic to the quasar, not intergalactic !

7. BAL QSOs model by Elvis (2000) ~15-20% of radio-quiet AGNs outflows are evolutionary phenomenon, independent on orientation outflows are present in every quasar, but cover only ~20% of solid angle two classes of models

8. statistic of absorption lines number of absorbers crossed per unit path length proper length number of absorption lines per unit redshift cross section of the absorbers density of the absorbers: constant comoving density n(z)=n 0 (1+z) 3 it is assumed that comoving density and cross section are both constant more generally, dependence on z is assumed parametrically q 0 =0 q 0 =1/2 implies evolution for the non evolutionary case, n o, σ o const, we have: for Λ≠0 change to:

9. risultati statistici clear evidence of evolution possibly, lower metallicity at high z

10. effects near the QSO number of absorbers can increase for z abs ~z em because some absorbers could be physically related to the QSO viceversa in many cases (e.g. Lyα) number of absorption lines decreases due to the higher ionization level (proximity effect or inverse effect) to remove the effect, absorption systems within an appropriate velocity interval from QSO are excluded in the QSO rest-frame, a cloud moving toward the observer produces an absorption line at in the observer frame: the corresponding velocity can be found: typically, bias is removed excluding absorptions with z abs less than the value corresponding to β~0.1

11. high redshift galaxies they appear different from nearby galaxies, both for observational effects and for intrinsic differences main effects: * redshift-dependence of surface brightness * K-correction * passive and active evolution light of distant galaxies comes mainly from massive, young stars: observing at high redshift, we see cosmic epochs of vigorous star formation portion of the Hubble Deep Field galaxies appear more irregular than present day galaxies we see them through the light emitted in UV by the young stars but in UV also nearby galaxies appear less regular

12. cosmic distances and surface brightness like for quasars, also for galaxies we must use luminosity distance moreover, because galaxies have extended images, it is also important the angular diameter distance the different dipendence on redshift has important consequences on surface brightness, and is due to the fact that in one case photons are dispersed on detector’s area at z=0, while in the other we observe photons emitted by an area of the source at z em surface brightness falls rapidly, making photometry difficult the apparent sizes of corresponding isophotes shrink

13. fall of the isophotal diameter R 25 exponential disk spheroid R 1/4 at low z there is a larger effect for the spheroid, at high z for the exponential disk

14. z A(z) luminosity distance in units of c/H 0 0

15. z A a (z) angular diameter distance in units of c/H 0

16. K-correction (evolutionary correction) we cannot measure the spectrum of a distant galaxy like it is now, but we can compute how a galaxy identical to one present day galaxy would appear if placed at a redshift z elliptical, falls rapidly in the rest-frame UV corresponding to observed B starburst, small or no decrease, because of young stars emitting in this band effect in the I band is lower for both spectra same spectrum shifted in lambda effect for z=0.5

17. K-correction K-correction for ellipticals, Sb spirals, blue irregolar/starburst galaxies, in the bands B J, I, K

18. evolutionary correction different spectrum at t 0 and t e 3 possibilities: burst of star formation, and then rapid death of massive stars and progressive dimming of the other stars (passive evolution) further episodes of star formation addition of stars and/or gas in merging episodes approximate expression in terms of the evolutionary luminosity change dL/dt, for small z and Λ=0: Δt being the look-back time

19. Hubble diagram in the K band for some samples of radiogalaxies curves show the effect of two models of passive evolution with star formation burst at z=20

20. passive and active evolution passive evolution is called the change of galactic properties due to the aging of stellar population born initially in the original star formation burst. active evolution indicates instead the effect on galactic properties due to secondary events of star formation, e.g. produced by merging population synthesis: a galactic spectrum can be written simply as sum of the spectra of constituent stars (ignoring complications such as internal absorption by dust or co-evolving binary systems): theoretical stellar spectra can be used, or even empirical stellar spectra, if they can be observed for a grid of values of temperature, luminosity, and chemical composition need to specify the initial mass function (IMF) with which stars are born. at high redshift IMF can be much different than present IMF, probably peaked toward very massive stars most common models use star formation with a single burst, or exponentially decreasing, or constant. results show that much of the initial emission is in the UV. later, a strong characteristic spectral feature is produced, called HK break or 4000Å break, a blend of absorption lines near the HK CaII doublet. the amplitude of the break increases with age and is little dependent on other factors

21. evolution of a galactic spectrum

22. color bimodality luminosity, mass, color, morphology, stellar population of galaxies are strongly related. analysis of such properties in the cosmic time started first with the study of the luminosity function but later included galaxy counts as function of the various parameters however, almost all these properties are unimodal, and galaxies tend to occupy a big cloud in the parameter space, and it is often difficult to distinguish if a change in a particular cell of the parameter space is due to a global number change or to a shift towards/from nearby cells in this sea of unimodal functions, one function appears different for his bimodal character, the color function. bimodality is evident, e.g. in the color-magnitude diagram (CMD), where two populations are clearly distingushed, the BLUE CLOUD and the RED SEQUENCE Hogg et al 2003 Baldry et al 2004

23. color bimodality Baldry et al 2004 otherwise, this can be viewed with color distributions in bins of absolute magnitude, approximated by double Gaussians bimodality is present also for other parameters, morphology, metallicity, SFR, but color bimodality is much more clear, and is observed up to z~1, and partially for z>1.

24. Lilly et al 1995 blue and red luminosity function bimodal behavior is also clear from the luminosity function, where a steepening is observed in the low luminosity part of the LF of blue galaxies for z > ~0.5, and instead a substantial lack of evolution for red galaxies (Lilly et al 1995) these observations were interpreted with the conclusion that red galaxies formed first, in accordance with the so-called “monolithic collapse” scenario (Eggen Lynden-Bell Sandage 1962), and that blue galaxies are still evolving

25. Faber et al 2007 more recent studies based on 39,000 galaxies from surveys DEEP2 and COMBO-17 (Faber et al 2007) have provided evidence also for evolution of the LF of red galaxies, with a decrease of M B * and an increase of φ* (parameters of the Schechter LF) it is found also a substantial constancy of the luminosity density for z<1 as stellar evolution models for red galaxies predict an increase of the ratio M/L B of 1-2 mag, constancy of j B implies that stellar mass of red galaxies is at least doubled from z=1 blue and red luminosity function

26. color-stellar mass diagram besides the color-magnitude diagram, bimodality is represented also with the color-stellar mass diagram e.g. Taylor et al 2009

27. Bundy et al 2005 color-stellar mass diagram estimate of stellar masses uses multiband photometry and redshift to compare the observed SED with a grid of synthetic SEDs depending on star formation history, age, metallicity, dust content. for each grid model the computed quantities are M*/L K, M*, chi 2, and the probability that the model represents the data probabilities are then summed on the grid and probability histograms by stellar mass are produced. so for each galaxy a probability distribution of M* is found, and the median value is adopted as measure of M*

28. evolution in the color-stellar mass diagram Track C is intermediate, with contributions by both mechanisms. this scenario is in better agreement with the properties of elliptical galaxies, both distant and local Track B is the opposite extreme, with a late star formation quenching. in this case, galaxies collect most of their mass in the blue phase, and then are subject to merging and become red, without further “dry merging” Track A represents an early quenching of star formation, when galaxy fragments are still small. in this case, most of the galaxy growth occurs in “dry mergers” Faber et al 2007 assume that galaxies can transit from BLUE CLOUD to RED SEQUENCE when star formation stops during a “major merger” (merging between galaxies with nearly equal masses). the stop of star formation(quenching) is represented by nearly vertical lines. mergers are gas-reach (wet mergers) because progenitor galaxies are blue galaxies with star formation. once on the red sequence, galaxies can be subject to gas-poor mergers (dry mergers), described by the white arrows. three cases are proposed:

29. Dekel et al 2006 variants of the color-stellar mass diagram

30. Cattaneo et al 2006 variants of the color-stellar mass diagram Cattaneo et al 2009

31. Hasinger 2008 Smolcic 2009 green valley