Ch.5 absorption lines they allow to use quasars as cosmological probes to study the Universe at large distances and large look-back times QSO zabs<zem * zem absorption line system: system of absorption lines at the same zabs, presumably associated with the same absorber 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 zem (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 absorption lines “metal” line system “damped” Lyα large column density, probably due to the cross of a galactic disk absorption lines Lyα systems Ly limit system Broad Absorption Lines and BAL QSOs intrinsic to the quasar, not intergalactic ! profiles PCygni-like, absorptions shifted by ~ 30000 km/s probably associated with outflows from nuclear region broad (104 km/s) Gibson et al 2008 BAL QSOs are: •X-ray-weak, lower than for non-BAL •usually radio quiet BAL QSOs ~15-20% of radio-quiet AGNs two classes of models model by Elvis (2000) outflows are evolutionary phenomenon, independent on orientation outflows are present in every quasar, but cover only ~20% of solid angle statistic of absorption lines number of absorbers crossed per unit path length proper length cross section of the absorbers density of the absorbers: constant comoving density n(z)=n0(1+z)3 number of absorption lines per unit redshift it is assumed that comoving density and cross section are both constant more generally, dependence on z is assumed parametrically for the non evolutionary case, no, σo const, we have: q0=0 q0=1/2 implies evolution for Λ≠0 change to: risultati statistici clear evidence of evolution possibly, lower metallicity at high z effects near the QSO number of absorbers can increase for zabs~zem 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 zabs less than the value corresponding to β~0.1 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 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 zem surface brightness falls rapidly, making photometry difficult the apparent sizes of corresponding isophotes shrink fall of the isophotal diameter R25 exponential disk spheroid R1/4 at low z there is a larger effect for the spheroid, at high z for the exponential disk luminosity distance in units of c/H0 A(z) 0 z angular diameter distance in units of c/H0 Aa(z) z K-correction (evolutionary correction) same spectrum shifted in lambda 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 effect for z=0.5 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 K-correction K-correction for ellipticals, Sb spirals, blue irregolar/starburst galaxies, in the bands BJ, I, K evolutionary correction different spectrum at t0 and te 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 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 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 evolution of a galactic spectrum 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 Baldry et al 2004 Hogg et al 2003 color bimodality otherwise, this can be viewed with color distributions in bins of absolute magnitude, approximated by double Gaussians Baldry et al 2004 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. 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 Lilly et al 1995 blue and red luminosity function 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 MB* 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/LB of 1-2 mag, constancy of jB implies that stellar mass of red galaxies is at least doubled from z=1 Faber et al 2007 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 color-stellar mass diagram Bundy et al 2005 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*/LK, M*, chi2, 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* evolution in the color-stellar mass diagram 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: 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” 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 C is intermediate, with contributions by both mechanisms. this scenario is in better agreement with the properties of elliptical galaxies, both distant and local variants of the color-stellar mass diagram Dekel et al 2006 Cattaneo et al 2009 variants of the color-stellar mass diagram Cattaneo et al 2006 green valley Hasinger 2008 Smolcic 2009