24.01.2015 Views

MATHEMATICAL TRIPOS Part II PAPER 4 Before you begin read ...

MATHEMATICAL TRIPOS Part II PAPER 4 Before you begin read ...

MATHEMATICAL TRIPOS Part II PAPER 4 Before you begin read ...

SHOW MORE
SHOW LESS
  • No tags were found...

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

5<br />

10E Cosmology<br />

The number density of a species ⋆ of non-relativistic particles of mass m, in<br />

equilibrium at temperature T and chemical potential µ, is<br />

n ⋆ = g ⋆<br />

( 2πmkT<br />

h 2 ) 3/2<br />

e (µ−mc2 )/kT ,<br />

where g ⋆ is the spin degeneracy. During primordial nucleosynthesis, deuterium, D, forms<br />

through the nuclear reaction<br />

p + n ↔ D ,<br />

where p and n are non-relativistic protons and neutrons.<br />

between the chemical potentials in equilibrium.<br />

Write down the relationship<br />

Using the fact that g D = 4, and explaining the approximations <strong>you</strong> make, show that<br />

(<br />

n D h<br />

2<br />

) 3/2 ( )<br />

BD<br />

≈<br />

exp ,<br />

n n n p πm p kT<br />

kT<br />

where B D is the deuterium binding energy, i.e. B D = (m n + m p − m D )c 2 .<br />

Let X ⋆ = n ⋆ /n B where n B is the baryon number density of the universe. Using the<br />

fact that n γ ∝ T 3 , show that<br />

( )<br />

X D<br />

∝ T 3/2 BD<br />

η exp ,<br />

X n X p kT<br />

where η is the baryon asymmetry parameter<br />

η = n B<br />

n γ<br />

.<br />

Briefly explain why primordial deuterium does not form until temperatures well below<br />

kT ∼ B D .<br />

<strong>Part</strong> <strong>II</strong>, Paper 4<br />

[TURN OVER

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!