Lecture 7 Flashcards

1
Q

The CMBR originated at a point when the universe was in

A

thermal equilibrium

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2
Q

photons interact very strongly with electrons and so have a

A

very short mean free path

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3
Q

photons mean free path increases until

A

it matches the size of the universe

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4
Q

a consequence of the photons mean free path matching the size of the universe is that the

A

photons can now travel unimpeded

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5
Q

decoupling

A

photons travelling unimpeded : the photons decouple from matter

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6
Q

CMBR is formed during

A

decoupling

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7
Q

At what temperature T was the CMBR formed

A

we can make a estimate using the Saha equation

Tdec = 3000K at z = 1000

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8
Q

Recombination refers to the period

A

during which electrons and protons first become bound as hydrogen nuclei

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9
Q

Decoupling refers to the point

A

where photons fall out of thermal equilibrium with matter

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10
Q

The surface of Last Scattering

A

the universe as it was just after it become cool enough for photons to travel without being scattered by electrons

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11
Q

CMBR forms at

A

lower temperature than that defined by the epoch of matter-radiation equality

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12
Q

the universe was already

A

matter-dominated when the CMBR formed

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13
Q

the epochs of matter-radiation equality and decoupling occurred

A

very early on in the evolution of the universe and within a few hundred thousand years of each other

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14
Q

For T > Teq the universe is

A

radiation dominated with

a(t) ∝ t^1/2

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15
Q

formula for T

A

T = 1.4x10^10 K / √t

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16
Q

formula for E(typical)

A

E(typical)(t) = 3 MeV/√t

17
Q

Nucleosynthesis

A

the typical nuclear binding energy is 1MeV so at this time the lightest nuclei can begin to form

18
Q

Strongly interacting plasma

A

The universe comprised of strongly interacting plasma of free electrons, protons, neutrons, photons and neutrinos

the neutrinos and other dark matter particles would have already decoupled from the photons at this time

19
Q

Quark-Hadron Phase Transition

A

the universe comprised a strongly interacting soup of quarks and leptons

during this era the quarks became confined which is why we refer to a quark-hadron phase transition

20
Q

We only have indirect evidence

A

of the behaviour of fundamental particles

21
Q

the Planck era

A

need quantum theory of gravity

we believe that quantum fluctuations are the likely origin of the CMBR temperature variations