7. Reionization Flashcards

1
Q

What was the redshift at the bigbang and recombination?

A

Infinity at the BB
1100 at recombination

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2
Q

What is recombination?

A

p+e -> H I

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3
Q

What are Stromgren spheres?

A

An ionised bubble for a source emitting N dot photons per second

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4
Q

What is the clumping factor

A

Measure of the density of hydrogen gas
- Compares the density of protons and electrons vs electrons ^2

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5
Q

What is the filling factor?

A

What fraction of the volume of the universe is ionised

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6
Q

What does it mean if we have quantities represented as <x>?</x>

A

They are volume averaged quantities

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7
Q

As the Universe expands, what happens to the number density <n>, clumping factor and recombination timescale? What is a consequence of this with regards to electrons and ionisation?</n>

A

<n> and clumping factor decrease
t_rec increases
- Electrons are far less likely to recombine as time passes (low z)
- Universe stays ionised even after bright hot sources fade
</n>

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8
Q

What is the Gunn-Peterson trough?

A

Occurs when Lyman alpha forest absorption lines merge into continuous absorption
- Light will be scattered or reabsorbed by electrons

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9
Q

What is the optical depth (tau) and how can we measure it?

A

It is a measure of how much light is absorbed when light travels through an absorbing medium
- Measure it by comparing observations to models

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10
Q

When inserting reasonable parameters in the optical depth equation, what conclusion can be drawn?

A

We get that the optical depth, tau, is > > 1 implying total absorption
- Ly alpha absorption is sensitive to v small neutral fractions

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11
Q

What does the presence of total absorption (GP troughs) for distant objects (give examples) tell us about the Universe?

A

Examples: QSOs (z > 6) and GRBs
- Shows that the U has just become ionised with a small neutral fraction left

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12
Q

What is the main assumption which is slightly incorrect that we used in the optical depth equation?

A

Assumed gas is static but it is not
- Ly alpha absorption is never a perfect delta function
To get around this, we can model the effects of dense gas to be slightly wavelength dependent yielding “damping wings”

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13
Q

What are damping wings?

A

When we suppress flux either side of the absorption wavelength

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14
Q

How are damping wings obseved for bright distant sources?

A

As a curved edge to the Ly alpha break
- Can also suppress Ly alpha emission from the original source

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15
Q

How does the GP trough affect the type of galaxies that we observe?

A

Distant galaxies are expected to be Ly alpha emitters
- Fewer will be than expected but we will still see Ly break galaxies

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16
Q

When do CMB photons become polarised?

A

When they scatter from free electrons

17
Q

What does measuring polarisation as a function of frequency tell us?

A

Tells us about ionised hydrogen as a function of redshift
- Sensitive to the start of recombination

18
Q

How many photons did reionizing the Universe need, and what are possible sources of this?

A

10^53.3 ionising photons/s/Mpc
- Candidates are AGN (rare) and star forming galaxies (common but faint)

19
Q

What is the typical magnitude for a galaxy in the UV

A

M_UV = -21

20
Q

What are the best estimates of L_UV and why is this quantity important?

A

between -10 and -16
- Important as it encodes our understanding of how small a galaxy gan be while forming stars

21
Q

What is the maximum wavelength of the ionising photons?

A

912 Angstroms

22
Q

During reionization, up to what wavelength of photons were absorbed?

A

Up to 1216 Angstroms

23
Q

What is the problem we have when trying to see how many ionising photons are produced from a galaxy?

A

We observe longwards of the Ly alpha emission at say 1500 Angstroms
- Ionising photons exist upto 912 Angstroms
- Need to extrapolate what we observe

24
Q

How can we improve our understanding of the sources of reionization

A

Need improved observational constraints on the process to refine models of early G’s and stellar populations
- JWST will do this