On the Role of Galaxies and AGN in Reionising the IGM: - - PowerPoint PPT Presentation

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On the Role of Galaxies and AGN in Reionising the IGM: - - PowerPoint PPT Presentation

On the Role of Galaxies and AGN in Reionising the IGM: spectroscopic survey of 5<z<7 galaxies in QSO fields s Koki Kakiichi University College London With Richard Ellis, Nicolas Laporte, Adi Zitrin, Anna-Christina Eilers, Emma


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SLIDE 1

Koki Kakiichi

University College London

Sakura CLAW @ Tokyo 2018

s

On the Role of Galaxies and AGN in Reionising the IGM:

spectroscopic survey of 5<z<7 galaxies in QSO fields

With Richard Ellis, Nicolas Laporte, Adi Zitrin, Anna-Christina Eilers, Emma Ryan-Weber, Romain Meyer, Brant Robertson, Dan Stark, Sarah Bosman

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SLIDE 2

z=1100 (CMB) first stars z~20-30

Epoch of Cosmic Dawn & Reionization When did reionization happen? What reionized the Universe?

reionization z~6-18 “Long-standing questions in observational cosmology” assemble to first galaxies

Gunn & Peterson (1965) paper

50 years old problem!

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SLIDE 3

What reionized the universe?

Problem 1

Becker+2015

Robertson+2015

✔ Hubble+Planck

1. HST galaxy demographics can drive reionisation but “Unknown fesc”

Robertson+15

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SLIDE 4

UV background Temperature

Gunn-Peterson trough Transmission spikes

What reionized the universe?

Problem 2

2. Huge variation of the intergalactic Lyman alpha optical depth at z>5.5

Difficult with faint galaxies.. Luminous systems? thermal fluctuations?

Becker+15 Also Bosman & Chardin’s talks

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SLIDE 5

Testing what reionized the universe:

Probing the direct influence of galaxies on the Lyα forest at z>5

Becker+2015

QSO absorption spectra Galaxy spectra Spectroscopic survey of Lyα emitting galaxies in QSO fields Post-reionized IGM

HI HII

Lyα

QSO

z>6

small-scale absorbers

A reionisation-era extension of idea in Keck Baryonic Structure Survey (Steidel et al) e.g. Rudie+12, Turner+14 and Quasar Probing Quasar Survey (Hennawi & Prochaska et al) e.g. Prochaska+13, Schmidt+17

“Lyα probing Lyα”

Lyα emission & absorption

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SLIDE 6

Survey design: DEIMOS spectroscopy of bright LBGs (r- and i-dropouts, z mag < 25.5) in the foreground of well-known QSO z~6 (Keck/ESI QSO spectra)

Keck spectroscopy of 5<z<7 galaxies around the Lyɑ forest of a background QSO field

SDSS J1148+5251 QSO z=6.4189

Kakiichi+2018 (arXiv:1803.02981)

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SLIDE 7

Lyα emitting Lyman-break galaxies in J1148+5251 QSO field

Lyɑ Ly𝛾

“Direct mapping of the physical state of the IGM around galaxies at z~6” Cosmological hydrodynamic simulation + simple radiative transfer

Ionising UV radiation from galaxies → more Lyα transmission spikes around galaxies but the individual associations are “stochastic"

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SLIDE 8

Lyα emitting Lyman-break galaxies in J1148+5251 QSO field

Lyɑ Ly𝛾

“Direct mapping of the physical state of the IGM around galaxies at z~6”

Cross-correlate… ?

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SLIDE 9

Lyα emitting Lyman-break galaxies in J1148+5251 QSO field

“Direct mapping of the physical state of the IGM around galaxies at z~6”

galaxy - Lya forest pixel exp(-𝞄) r

Lya transmitted flux

r

Cross-correlate… ?

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SLIDE 10

Lyα emitting Lyman-break galaxies in J1148+5251 QSO field

“Direct mapping of the physical state of the IGM around galaxies at z~6”

r

galaxy - Lya forest pixel exp(-𝞄) r

Lya transmitted flux

Cross-correlate… ?

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SLIDE 11

Lyα emitting Lyman-break galaxies in J1148+5251 QSO field

“Direct mapping of the physical state of the IGM around galaxies at z~6”

galaxy - Lya forest pixel exp(-𝞄) r

Lya transmitted flux

Cross-correlate… ?

r

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SLIDE 12

Lyα emitting Lyman-break galaxies in J1148+5251 QSO field

“Direct mapping of the physical state of the IGM around galaxies at z~6”

galaxy - Lya forest pixel exp(-𝞄) r

Lya transmitted flux

Cross-correlate… ?

r

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SLIDE 13

Lyα emitting Lyman-break galaxies in J1148+5251 QSO field

“Direct mapping of the physical state of the IGM around galaxies at z~6”

galaxy - Lya forest pixel exp(-𝞄) r

Lya transmitted flux

Cross-correlate… ?

r

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SLIDE 14

Lyα emitting Lyman-break galaxies in J1148+5251 QSO field

“Direct mapping of the physical state of the IGM around galaxies at z~6”

galaxy - Lya forest pixel exp(-𝞄) r Cross-correlate… well, just take the MEAN Lya transmitted flux around LBGs

r

Lya transmitted flux

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SLIDE 15

Mean Lyα transmitted flux around LBGs at z~5.8

More Lyα forest transmission (=IGM more ionised) Closer to galaxies

“Tentative”, but promising, evidence of “Statistical HI proximity effect” ?

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SLIDE 16

101 100 101 log10 r [pMpc] 1013 1012 1011 hΓHI(r)i 101 100 101 log10 r [pMpc]

1 2 3 4 5 6

r [pMpc]

103 102 101

hexp(τα(r))i

hfesci = 0.02 hfesci = 0.05 hfesci = 0.10 hfesci = 0.20

1 2 3 4 5 6

r [pMpc]

M lim

UV = 10

M lim

UV = 13

M lim

UV = 15

M lim

UV = 18

QSO absorption spectra Galaxy spectra Spectroscopic survey of Lyα emitting galaxies in QSO fields Post-reionized IGM

HI HII

Lyα

QSO

Mean Lyα transmitted flux around LBGs at z~5.8

101 100 101 log10 r [pMpc] 1013 1012 1011 hΓHI(r)i 101 100 101 log10 r [pMpc]

1 2 3 4 5 6

r [pMpc]

103 102 101

hexp(τα(r))i

hfesci = 0.02 hfesci = 0.05 hfesci = 0.10 hfesci = 0.20

1 2 3 4 5 6

r [pMpc]

M lim

UV = 10

M lim

UV = 13

M lim

UV = 15

M lim

UV = 18
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SLIDE 17

101 100 101 log10 r [pMpc] 1013 1012 1011 hΓHI(r)i 101 100 101 log10 r [pMpc]

1 2 3 4 5 6

r [pMpc]

103 102 101

hexp(τα(r))i

hfesci = 0.02 hfesci = 0.05 hfesci = 0.10 hfesci = 0.20

1 2 3 4 5 6

r [pMpc]

M lim

UV = 10

M lim

UV = 13

M lim

UV = 15

M lim

UV = 18

QSO absorption spectra Galaxy spectra Spectroscopic survey of Lyα emitting galaxies in QSO fields Post-reionized IGM

HI HII

Lyα

QSO

Mean Lyα transmitted flux around LBGs at z~5.8

Ionising radiation from the ‘detected’ galaxies is too small to explain the

  • bservation (statistical HI proximity effect)
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SLIDE 18

101 100 101 log10 r [pMpc] 1013 1012 1011 hΓHI(r)i 101 100 101 log10 r [pMpc]

1 2 3 4 5 6

r [pMpc]

103 102 101

hexp(τα(r))i

hfesci = 0.02 hfesci = 0.05 hfesci = 0.10 hfesci = 0.20

1 2 3 4 5 6

r [pMpc]

M lim

UV = 10

M lim

UV = 13

M lim

UV = 15

M lim

UV = 18

QSO absorption spectra Galaxy spectra Spectroscopic survey of Lyα emitting galaxies in QSO fields Post-reionized IGM

HI HII

Lyα

QSO

Ionising radiation from the ‘detected’ galaxies is too small to explain the

  • bservation (statistical HI proximity effect)

Need “faint unseen galaxies clustering around the detected galaxies” & their collective ionising radiation

(modelled by CLF/HOD framework and joint analysis of luminosity function and angular galaxy clustering, then do RT)

Mean Lyα transmitted flux around LBGs at z~5.8

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SLIDE 19

101 100 101 log10 r [pMpc] 1013 1012 1011 hΓHI(r)i 101 100 101 log10 r [pMpc]

1 2 3 4 5 6

r [pMpc]

103 102 101

hexp(τα(r))i

hfesci = 0.02 hfesci = 0.05 hfesci = 0.10 hfesci = 0.20

1 2 3 4 5 6

r [pMpc]

M lim

UV = 10

M lim

UV = 13

M lim

UV = 15

M lim

UV = 18

QSO absorption spectra Galaxy spectra Spectroscopic survey of Lyα emitting galaxies in QSO fields Post-reionized IGM

HI HII

Lyα

QSO

Ionising radiation from the ‘detected’ galaxies is too small to explain the

  • bservation (statistical HI proximity effect)

Slope is shallower if the IGM is ionised by even fainter galaxies ‘clustering bias of ionising sources’ Need “faint unseen galaxies clustering around the detected galaxies” & their collective ionising radiation

(modelled by CLF/HOD framework and joint analysis of luminosity function and angular galaxy clustering, then do RT)

Mean Lyα transmitted flux around LBGs at z~5.8

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SLIDE 20

101 100 101 log10 r [pMpc] 1013 1012 1011 hΓHI(r)i 101 100 101 log10 r [pMpc]

1 2 3 4 5 6

r [pMpc]

103 102 101

hexp(τα(r))i

hfesci = 0.02 hfesci = 0.05 hfesci = 0.10 hfesci = 0.20

1 2 3 4 5 6

r [pMpc]

M lim

UV = 10

M lim

UV = 13

M lim

UV = 15

M lim

UV = 18

From the mean Lyα transmitted flux around LBGs to the average LyC escape fraction

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SLIDE 21

101 100 101 log10 r [pMpc] 1013 1012 1011 hΓHI(r)i 101 100 101 log10 r [pMpc]

1 2 3 4 5 6

r [pMpc]

103 102 101

hexp(τα(r))i

hfesci = 0.02 hfesci = 0.05 hfesci = 0.10 hfesci = 0.20

1 2 3 4 5 6

r [pMpc]

M lim

UV = 10

M lim

UV = 13

M lim

UV = 15

M lim

UV = 18

From the mean Lyα transmitted flux around LBGs to the average LyC escape fraction

Luminosity function + LBG clustering

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SLIDE 22

101 100 101 log10 r [pMpc] 1013 1012 1011 hΓHI(r)i 101 100 101 log10 r [pMpc]

1 2 3 4 5 6

r [pMpc]

103 102 101

hexp(τα(r))i

hfesci = 0.02 hfesci = 0.05 hfesci = 0.10 hfesci = 0.20

1 2 3 4 5 6

r [pMpc]

M lim

UV = 10

M lim

UV = 13

M lim

UV = 15

M lim

UV = 18

From the mean Lyα transmitted flux around LBGs to the average LyC escape fraction

Luminosity function + LBG clustering Muv

lim

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SLIDE 23

101 100 101 log10 r [pMpc] 1013 1012 1011 hΓHI(r)i 101 100 101 log10 r [pMpc]

1 2 3 4 5 6

r [pMpc]

103 102 101

hexp(τα(r))i

hfesci = 0.02 hfesci = 0.05 hfesci = 0.10 hfesci = 0.20

1 2 3 4 5 6

r [pMpc]

M lim

UV = 10

M lim

UV = 13

M lim

UV = 15

M lim

UV = 18

From the mean Lyα transmitted flux around LBGs to the average LyC escape fraction

Spectral hardness of sources Luminosity function + LBG clustering Muv

lim

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SLIDE 24

101 100 101 log10 r [pMpc] 1013 1012 1011 hΓHI(r)i 101 100 101 log10 r [pMpc]

1 2 3 4 5 6

r [pMpc]

103 102 101

hexp(τα(r))i

hfesci = 0.02 hfesci = 0.05 hfesci = 0.10 hfesci = 0.20

1 2 3 4 5 6

r [pMpc]

M lim

UV = 10

M lim

UV = 13

M lim

UV = 15

M lim

UV = 18

From the mean Lyα transmitted flux around LBGs to the average LyC escape fraction

Do radiative transfer calculation… Spectral hardness of sources Luminosity function + LBG clustering Muv

lim

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SLIDE 25

101 100 101 log10 r [pMpc] 1013 1012 1011 hΓHI(r)i 101 100 101 log10 r [pMpc]

1 2 3 4 5 6

r [pMpc]

103 102 101

hexp(τα(r))i

hfesci = 0.02 hfesci = 0.05 hfesci = 0.10 hfesci = 0.20

1 2 3 4 5 6

r [pMpc]

M lim

UV = 10

M lim

UV = 13

M lim

UV = 15

M lim

UV = 18

From the mean Lyα transmitted flux around LBGs to the average LyC escape fraction

Spectral hardness of sources

Measurement of the population-averaged escape fraction!!

Luminosity function + LBG clustering Do radiative transfer calculation… Muv

lim

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SLIDE 26

Constraint on the average escape fraction at z~5.8

MCMC fit

Mlim

UV = 14.53+2.71 2.53

18 16 14 12 10

Mlim

UV

1.4 1.2 1.0 0.8 0.6

log10hfesci

1.4 1.2 1.0 0.8 0.6

log10hfesci

log10hfesci = 1.08+0.16

0.09

Galaxy-Ly훼 forest (fiducial)

  • w. low mean free path
  • w. temperature fluctuation

⟨fesc⟩ = 0.08+0.08

  • 0.02

⟨𝜊ion⟩

1025.2 erg-1 Hz

( )

  • 1
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SLIDE 27

Constraint on the average escape fraction at z~5.8

2 3 4 5 6 7

Redshift

102 101 100

hfesci

hfesci > 10%

Galaxy-Lyα forest Q1148 field (this work) Direct LyC imaging ISM abs. lines GRB NHI-stack

What reionised the Universe? Faint galaxies (Muv<-15) deposit enough ionising radiation to the IGM to drive HI reionisation (fesc>10%)

Robertson+2015

✔ Hubble+Planck

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SLIDE 28

Faint galaxies fesc>10% … What reionised the Universe?

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SLIDE 29

Twist in a story: luminous systems

bright galaxies & faint AGN

Subaru/HSC

Lyɑ Ly𝛾

Luminous?

Faint galaxies

Ono+2017

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SLIDE 30

Twist in a story: luminous systems

bright galaxies & faint AGN

Subaru/HSC

Lyɑ Ly𝛾

Luminous?

Faint galaxies

Ono+2017

luminous Lyα emitting LBG faint AGN

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SLIDE 31

A discovery of an individual transverse proximity effect around z=6.177 luminous LBG

Lyβ transmission spike

luminous Lyα emitting LBG

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SLIDE 32

A discovery of an individual transverse proximity effect around z=6.177 luminous LBG

Evidence that z>6 luminous galaxies preferentially reside in highly ionized environment, but need faint galaxies to produce the HII region!

With cosmo. hydrodynamical simulations

Lyβ transmission spike

luminous Lyα emitting LBG

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SLIDE 33

Evidence that z>6 luminous galaxies preferentially reside in highly ionized environment, but need faint galaxies to produce the HII region!

A discovery of an individual transverse proximity effect around z=6.177 luminous LBG

QSO absorption spectra Galaxy spectra Spectroscopic survey of Lyα emitting galaxies in QSO fields Post-reionized IGM

HI HII

Lyα

RHII>10h-1Mpc

A lower limit to the size of cosmological HII region RHII>dspike≃10h-1Mpc @ z≃6.2

Lyβ transmission spike

luminous Lyα emitting LBG

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SLIDE 34

QSO absorption spectra Galaxy spectra Spectroscopic survey of Lyα emitting galaxies in QSO fields Post-reionized IGM

HI HII

Lyα

RHII>10h-1Mpc

Evidence that z>6 luminous galaxies preferentially reside in highly ionized environment, but need faint galaxies to produce the HII region!

A discovery of an individual transverse proximity effect around z=6.177 luminous LBG

Stark+2017

A lower limit to the size of cosmological HII region RHII>dspike≃10h-1Mpc @ z≃6.2

Accelerated reionization around luminous galaxies… …needs clustered faint galaxies to produce the HII region?

Lyβ transmission spike

luminous Lyα emitting LBG

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SLIDE 35

Lyβ transmission spike

luminous Lyα emitting LBG

QSO absorption spectra Galaxy spectra Spectroscopic survey of Lyα emitting galaxies in QSO fields Post-reionized IGM

HI HII

Lyα

RHII>10h-1Mpc

Evidence that z>6 luminous galaxies preferentially reside in highly ionized environment, but need faint galaxies to produce the HII region!

A discovery of an individual transverse proximity effect around z=6.177 luminous LBG

Stark+2017

A lower limit to the size of cosmological HII region RHII>dspike≃10h-1Mpc @ z≃6.2

Accelerated reionization around luminous galaxies… …needs clustered faint galaxies to produce the HII region?

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SLIDE 36

Unusually(?) broad Lyα transmission spikes near faint AGN…

faint AGN

The role of AGN: reionization of hydrogen & helium

broad Lyα transmission spikes

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SLIDE 37

faint AGN

QSO absorption spectra Galaxy spectra Spectroscopic survey of Lyα emitting galaxies in QSO fields Post-reionized IGM

HI HII

Lyα

QSO

HeIII region

AGN may heat up the IGM through HeII photo-heating across HeIII ionization front

Early z>5 patchy onset

  • f HeII reionization?

broad Lyα transmission spikes

The role of AGN: reionization of hydrogen & helium

Unusually(?) broad Lyα transmission spikes near faint AGN…

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SLIDE 38

QSO absorption spectra Galaxy spectra Spectroscopic survey of Lyα emitting galaxies in QSO fields Post-reionized IGM

HI HII

Lyα

QSO

HeIII region

Early z>5 patchy onset

  • f HeII reionization?

Laporte+2017

Evidence of early onset of HeII reionziation The effect of HeII heating in the proximity zone of bright QSOs

Bolton+2012

AGN may heat up the IGM through HeII photo-heating across HeIII ionization front

The role of AGN: reionization of hydrogen & helium

faint AGN

broad Lyα transmission spikes

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SLIDE 39

Evidence of early onset of HeII reionziation The effect of HeII heating in the proximity zone of bright QSOs

Bolton+2012

z=7.15 galaxy with AGN activity

broad Lyα transmission spikes

faint AGN

QSO absorption spectra Galaxy spectra Spectroscopic survey of Lyα emitting galaxies in QSO fields Post-reionized IGM

HI HII

Lyα

QSO

HeIII region

Early z>5 patchy onset

  • f HeII reionization?

broad Lyα transmission spikes

faint AGN

Bolton+2012

Laporte+2017

z=7.15 galaxy with AGN activity (Laporte+2017) and z=6.6 CR7? (Sobral+2018, but Shibuya+2018)

Galaxy that could drive HeII reionization in its local environment AGN may heat up the IGM through HeII photo-heating across HeIII ionization front

The role of AGN: reionization of hydrogen & helium

Bolton+2012

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SLIDE 40

Multi-frequency radiative transfer simulation of hydrogen & helium reionization with galaxies and AGN

The ‘concerted’ impact of galaxies & AGN on the ionization and thermal state of the IGM in its local ennvironment?

KK+(2017)

AGN+galaxies-driven HII region galaxies-driven HII region AGN-dominated HeIII region

HII HeII HeIII

Kakiichi+2017

The role of AGN: reionization of hydrogen & helium

AGN HeIII I-front Heating of the IGM by AGN AGN

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SLIDE 41

Hypothesis emerging from J1148+5251 QSO field

While faint galaxies with high escape fraction (>10%) primarily drive reionization, luminous galaxies and AGN may play an increasingly important role in sourcing the large-scale fluctuations

  • f the UV background and thermal state of the IGM towards

the tail end of reionisation, possibly via their hard ionising spectra.

What reionised the Universe?

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SLIDE 42

Next step forward…

two-tiered spectroscopic survey of galaxies in QSO fields + full radiation hydrodynamical simulations

  • More DEIMOS multi-object spectroscopy of
  • ther z~6 QSO fields are coming.
  • MUSE integral field spectroscopy program for

blind search of faint LAEs in the QSO fields.

  • >2021- Subaru/Prime Focus Spectrograph (~1.3deg FoV

& 2400 multi-object spectroscopy) @ 8.2m telescope!

  • Joint theoretical Lyα in emission x absorption framework
  • Fully-coupled radiation hydrodynamical simulations of

galaxy formation and the IGM

Observational… Theoretical…

How to tackle: what reionized the Universe?

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SLIDE 43

Next step forward…

two-tiered spectroscopic survey of galaxies in QSO fields + full radiation hydrodynamical simulations

  • More DEIMOS multi-object spectroscopy of
  • ther z~6 QSO fields are coming.
  • MUSE integral field spectroscopy program for

blind search of faint LAEs in the QSO fields.

  • >2021- Subaru/Prime Focus Spectrograph (~1.3deg FoV

& 2400 multi-object spectroscopy) @ 8.2m telescope!

  • Joint theoretical Lyα in emission x absorption framework
  • Fully-coupled radiation hydrodynamical simulations of

galaxy formation and the IGM

Observational… Theoretical…

How to tackle: what reionized the Universe?

slide-44
SLIDE 44

Next step forward…

two-tiered spectroscopic survey of galaxies in QSO fields + full radiation hydrodynamical simulations

  • More DEIMOS multi-object spectroscopy of
  • ther z~6 QSO fields are coming.
  • MUSE integral field spectroscopy program for

blind search of faint LAEs in the QSO fields.

  • >2021- Subaru/Prime Focus Spectrograph (~1.3deg FoV

& 2400 multi-object spectroscopy) @ 8.2m telescope!

  • Joint theoretical Lyα in emission x absorption framework
  • Fully-coupled radiation hydrodynamical simulations of

galaxy formation and the IGM

Observational… Theoretical…

How to solve: what reionized the Universe?

QSO absorption spectra Spectra of Lyα emitting galaxies Lyα haloes

CGM IGM vr v║ r r║ r┴

Connecting Lyα absorption with emission as a probe of CGM

Lyα scattering as a origin of Lyα haloes, but cold neutral gas in CGM produces a extended tail as ‘ r -2.4 ’

z=3 arXiv:1710.10053

Impact on Lyα escape

⇒ fesc,CGM=80%

Turner+2014 Lyα Model

slide-45
SLIDE 45

Next step forward…

two-tiered spectroscopic survey of galaxies in QSO fields + full radiation hydrodynamical simulations

  • More DEIMOS multi-object spectroscopy of
  • ther z~6 QSO fields are coming.
  • MUSE integral field spectroscopy program for

blind search of faint LAEs in the QSO fields.

  • >2021- Subaru/Prime Focus Spectrograph (~1.3deg FoV

& 2400 multi-object spectroscopy) @ 8.2m telescope!

  • Joint theoretical Lyα in emission x absorption framework
  • Fully-coupled radiation hydrodynamical simulations of

galaxy formation and the IGM

Observational… Theoretical…

How to solve: what reionized the Universe?

Ramses-RT simulation Credit: Harley Katz (see Katz et al 2018)

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SLIDE 46

We are mapping a full 3D distribution of galaxies ⨉ the intergalactic medium (using “Lyα in emission and absorption”) to understand the Epoch of Reionization.

Summary “Lyα probing Lyα”

What reionised the Universe?

Becker+

QSO absorption spectra Galaxy spectra Spectroscopic survey of Lyα emitting galaxies in QSO fields Post-reionized IGM

HI HII

Lyα

QSO

z>6

Ly𝛃 halo

CGM small-scale absorbers

“While faint galaxies (Muv<-15) with high escape fraction (>10%) primarily drive reionization, luminous galaxies and AGN may play an increasingly important role in sourcing the large-scale fluctuations of the UV background and thermal state of the IGM towards the tail end of reionisation”

1) A new route to escape fraction. 2) Role of luminous galaxies and AGN. 3) … more!

Kakiichi+2018 (arXiv:1803.02981)