Cosmic Dawn and IGM Reionization

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Andrea Ferrara SISSA/International School for Advanced Studies, Trieste Cosmic Dawn and IGM Reionization

description

Cosmic Dawn and IGM Reionization. Andrea Ferrara. SISSA/International School for Advanced Studies, Trieste. At z=1000 the Universe has cooled down to 3000 K. Hydrogen becomes neutral (“ Recombination ”). At z < 20 the first “ PopIII ” star (clusters)/small galaxies form. - PowerPoint PPT Presentation

Transcript of Cosmic Dawn and IGM Reionization

Page 1: Cosmic Dawn and           IGM Reionization

Andrea FerraraSISSA/International School for Advanced Studies, Trieste

Cosmic Dawn and IGM Reionization

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Seq

uenc

e of

Eve

nts

At z=1000 the Universe has cooled down to 3000 K. Hydrogen becomes

neutral (“Recombination”).

At z < 20 the first “PopIII” star (clusters)/small galaxies form.

At z ~ 6-15 these gradually photo-ionize the hydrogen in the IGM

(“Reionization”).

At z<6 galaxies form most of their stars and grow by merging.

At z<1 massive galaxy clusters are assembled.

Tim

e

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Infall Rate: 0.01 Mo/yr

Envelope: 103 Mo

Core:10-2 Mo

density temperature

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Salvaterra & AF 2002;

Best fit model to NIR data

zend = 8.8f 30%

IR Background Data Points

Pop III stars can explain observed NIRB excess

ifVMS dominate IMF

~ (1+zend ) λLyα

PopIII Stars+Galaxies

First Light at Cosmic Dawn: Very Massive Stars Magliocchetti, Salvaterra & AF 2003

Galaxies

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Reionization by Very Massive Stars ?

z = 17

NIRB - fittingevolution

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WMAP results: reionization at z > 10 ?

Reionization TestsTem

pera

ture

-Pola

riza

tion C

ross

Pow

er

Sp

ect

rum

τe = 0.17± 0.04

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Inhomogeneous Reionization Choudhury & AF 2005Choudhury & AF 2005

Self-consistent treatment of the evolution of ionized regions and thermal history

Follow evolution of neutral, HII and HeIII regions; treat IGM as multiphase gas

Inhomogeneous density distribution: log-normal model

Three sources of ionizing radiation:

PopIII stars: early redshifts, high mass, zero metallicity PopII stars: Salpeter IMF, transition from PopIII @ z < 9 Quasars: significant @ z < 6, using -MBH relation

Radiative feedback suppressing SF in low-mass halos, set by:

Molecular cooling in neutral regions Photoionization temperature in ionized regions

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Experimental constraints

Ionized regionsfilling factor

Photo-rates

HI

HeII

LLS statistics

GP optical depth

e.s. optical depth

Mean density temperature

log

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Inhomogeneous Reionization

Additional hints from CMB+21cm line

(T/T0)CMB

(Tb/T0)21CM

late reionization early reionization

115 MHz 90 MHz

CROSS CORRELATE

Salvaterra, Ciardi, AF & Baccigalupi 2005

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Inhomogeneous Reionization Salvaterra, Ciardi, AF & Baccigalupi 2005

early

late

Size of HII region(Mpc) from zeroof correlation fct.

HII regions: size evolution

Bandwidth

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Miniati, AF, White & Bianchi 2004

The UVB in the Post-Reionization Epoch

Ionizing photons from structure formation

Mass range: log M = 11 – 13 Virial temperatures: log T 6 Bremsstrahlung + line emission Escape fraction 1

Galaxies

QSOs

Thermal

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Miniati et al 2004

The UVB in the Post-Reionization Epoch

Ionizing photons from structure formation

Photoionization rates

Total

QSOs

Galaxies Thermal

Thermal, no feedback

Thermal

Thermal, no feedback

QSOsGalaxies

Fan 2002

HI HeII

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Maselli & AF, in prep

Radiative Transfer Effects on the Ly Forest

UVB fluctuationsSee Maselli’s poster

Photoionization rates fluctuations through a box at z=3.27

HI HeII

Power spectrum Temperature Elemental abundances Eta parameter

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Brief Summary

• Photoionization rate fluctuations (10%, 60%) for (HI, HeII) induced by RT effects

• Massive first stars likely responsible for NIRB excess can reionize the IGM at z15

• Early reionization not in contrast with any constraint from QSO absorption line data

• Detailed reionization history from coupled CMB/21cm experiments

• HeII reionization more complex; affected by thermal radiation from structure formation

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Want to know more ?

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