simona gallerani (osservatorio astronomico di roma)
DESCRIPTION
What can we learn from quasar spectra on the high-redshift Universe?. Simona Gallerani (Osservatorio Astronomico di Roma). In collaboration with: T.Choudhury, P. Dayal, X. Fan, A. Ferrara, A. Maselli, R. Maiolino, R. Salvaterra. 21 th July 2009 Roman Young Researchers Meeting. - PowerPoint PPT PresentationTRANSCRIPT
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Simona Gallerani
(Osservatorio Astronomico di Roma)
What can we learn from quasar spectra
on the high-redshift Universe?
In collaboration with: T.Choudhury, P. Dayal, X. Fan, A. Ferrara, A. Maselli, R. Maiolino, R.
Salvaterra
21th July 2009 Roman Young Researchers Meeting
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The early Universe
TodayBig Bang
Recombinationprocess
The Universe is composed by a very hot and dense mix of particles and radiation
The expansion allows the radiation to decouple from matter and the first atoms to form
CosmicMicrowave
Background
THE COSMOLOGICAL PRINCIPLE
The Universe is homogeneous and isotropic
on large scales
~50 kyr
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Cosmic Web
First stars and galaxies originated predominantly in the regions
of intersection of these filaments.They are immersed in the
Intergalactic medium (IGM)
The first stars
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HI
HIIHII
HI
Pre-overlap stage
HII
Overlap stage Post-overlap stage
HII
HII
HIHI
HII
Cosmic reionization
R
O
E
What is the epoch of reionization (EOR)?
~100 Myr ≤1 Gyr ~14 Gyr
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Quasars: a class of very bright Active Galactic Nuclei
Black Hole
Accretion disk
Dust torus
SunQSO LL 1310
SunBH MM 96 1010
Particularly luminous
in the rest frame near ultra-violet,
i.e. close to the Lyα emission line
The quasar spectra we observe are strongly affected by the intervening material along the lines of sight
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The Lyα forest in quasar absorption spectra
Keck telescope
e
obsz
1
REDSHIFT
α=1216 Å )1( ** z
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Becker et al. (2003)
QSOs constraints on cosmic reionization
SDSS
~20 QSOs
@ 5.7<z<6.4
6reiz
Fan et al. (2005)
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Simulating the Ly forest
Coles & Jones (1991)
Log-Normal model
Reionization model Choudhury & Ferrara (2006)
Optical depth
Density field(ΛCDM)
Neutral hydrogen(TIGM; UVB)
(Voigt profile)
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Reionization models
Early Reionization (ERM) Late Reionization (LRM)
7reionz 6reionz
HII
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Models testingERM
LRM
Fan et al. (2006)
Songaila (2004) Fan et al. (2002)
Optical depth evolution Transmitted flux
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Simulated spectra3.67.5 z
GAPSGAPS
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Largest gap width distributionObservations vs Simulations
Low Redshift (zem<6)
ERM LRM
SG, F
erra
ra, F
an, C
houd
hury
(20
07)
High Redshift (zem>6)
LRM
ERM
6.5z3.5z
The Universe is highly ionized at z~6
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Quasars: a class of very bright Active Galactic Nuclei
Black Hole
Accretion disk
Dust torus
SunQSO LL 1310
SunBH MM 96 1010
Particularly luminous
in the rest frame near ultra-violet,
i.e. close to the Lyα emission line
The quasar spectra we observe are strongly affected by the intervening material along the lines of sightAND BY THE DUST SURROUNDING THE AGN!
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Dust extinction on quasar spectra
Intrinsic spectrum
Dust absorbed spectrum
Dust absorbs preferentially bluer photons, thus reddening the spectra
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An example of extincted spectra at z~6
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An empirical extinction law for the high redshift dust
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Conclusions
Quasar absorption spectra provide a huge amount of information both concerning the ionization level of the intergalactic medium
and the amount of dust present in the host galaxy.
The analysis of ~ 20 quasars at z~6 shows that observations are consistent with a highly ionized intergalactic medium at z~6.
The analysis of ~ 30 quasars at 4<z<6 shows that the properties of dust at these epochs differ from the local Universe.