lecture 4: matter-radiation decoupling and the cosmic ...star-kdh1/ce/ce04.pdf · lecture 4:...

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Lecture 4: Matter-Radiation Decoupling and the Cosmic Microwave Background Annihilation (with symmetry breaking) quark soup Baryogenesis (quark confinement) neutrons and protons Nucleosynthesis Plasma of charged nuclei (75% H 25% He) + electrons, photons, neutrinos, traces of Li, Be. Recombination Neutral atoms Matter and radiation decouple (Universe transparent) Origin of the Cosmic Microwave Background

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Page 1: Lecture 4: Matter-Radiation Decoupling and the Cosmic ...star-kdh1/ce/ce04.pdf · Lecture 4: Matter-Radiation Decoupling and the Cosmic Microwave Background • Annihilation ... coupling

Lecture 4: Matter-Radiation Decoupling and the Cosmic Microwave Background

•  Annihilation (with symmetry breaking) –  quark soup

•  Baryogenesis (quark confinement) –  neutrons and protons

•  Nucleosynthesis –  Plasma of charged nuclei (75% H 25% He) + electrons, photons, neutrinos, traces of Li, Be.

•  Recombination –  Neutral atoms –  Matter and radiation decouple (Universe transparent)

•  Origin of the Cosmic Microwave Background

Page 2: Lecture 4: Matter-Radiation Decoupling and the Cosmic ...star-kdh1/ce/ce04.pdf · Lecture 4: Matter-Radiation Decoupling and the Cosmic Microwave Background • Annihilation ... coupling

After Nucleosynthesis: charge-neutral plasma. 12 H+ + He++ + 14 e- + 109 photons

Thompson scattering of photons by electrons:

Electrons and photons exchange energy. Maintains thermal equilibrium and coupling (same T) between radiation and matter.

e+!! e+!

!

"1 e

#•

• e#

"2$ "

1

The Plasma Era

Page 3: Lecture 4: Matter-Radiation Decoupling and the Cosmic ...star-kdh1/ce/ce04.pdf · Lecture 4: Matter-Radiation Decoupling and the Cosmic Microwave Background • Annihilation ... coupling

The Universe is opaque. Photons cannot travel far without scattering on electrons. Photons “random walk”. Like “looking thru fog”. 1. matter-radiation equality ( T ~ 30,000 K t ~ 104 yr ) energy density of photons drops below that of matter Before: After: 2. “recombination” ( T ~ 3000 K t ~ 3x105 yr ) electrons + nuclei --> neutral atoms

!

T "1

R"1

t1/ 2

!

T "1

R"1

t2 / 3

Page 4: Lecture 4: Matter-Radiation Decoupling and the Cosmic ...star-kdh1/ce/ce04.pdf · Lecture 4: Matter-Radiation Decoupling and the Cosmic Microwave Background • Annihilation ... coupling

Plasma

Neutral gas

Recombination

Page 5: Lecture 4: Matter-Radiation Decoupling and the Cosmic ...star-kdh1/ce/ce04.pdf · Lecture 4: Matter-Radiation Decoupling and the Cosmic Microwave Background • Annihilation ... coupling

H ionisation potential I = 13.6 eV. Photons with can ionise H. Mean energy of blackbody photons: Recombination temperature: Too crude, because:

1) ~109 photons per H atom (photons in blackbody tail can ionise H) 2) H has bound states (excited electrons)

!

h " = 3 k T

!

T ~I

3 k=

13.6 eV( ) 11600 K eV-1( )

3" 52,000K

Recombination Temperature

!

h " > I

13.6 eV

!

3 k T ~ I

1/k =11,600 K/eV

Page 6: Lecture 4: Matter-Radiation Decoupling and the Cosmic ...star-kdh1/ce/ce04.pdf · Lecture 4: Matter-Radiation Decoupling and the Cosmic Microwave Background • Annihilation ... coupling

Energy levels: En = - I / n2. Excitation to n = 1 -->2 needs E = E2 - E1 = 13.6 x ( 1 - 1/22 ) = 10.2 eV.

!

Photon/proton ratio : N"

Np

#109

To get ~ 1 photon (with h$ >10.2 eV) per proton.

Np = N" (h$ > E) # N" exp %E /k T( )

E

k T = ln

N"

Np

&

' ( (

)

* + + # ln 109( ) # 20

k T #10.2 eV

ln 109( )# 0.5 eV

T # 5700 K

Refined Calculation

10.2 eV

Ionisation from bound states keeps gas ionised until T

drops further.

Page 7: Lecture 4: Matter-Radiation Decoupling and the Cosmic ...star-kdh1/ce/ce04.pdf · Lecture 4: Matter-Radiation Decoupling and the Cosmic Microwave Background • Annihilation ... coupling

Detailed calculation gives 3000 K. At T < 3000 K, electrons and nuclei form neutral

atoms, not immediately re-ionised by photons. Photons interact strongly with free charges (i.e. mainly free electrons), but not with neutral atoms. Photons & matter decouple and no longer interact! Universe becomes transparent. Photons now fly uninterrupted across the Universe. (this is the Cosmic Microwave Background)

Page 8: Lecture 4: Matter-Radiation Decoupling and the Cosmic ...star-kdh1/ce/ce04.pdf · Lecture 4: Matter-Radiation Decoupling and the Cosmic Microwave Background • Annihilation ... coupling

Last Scattering Epoch

!

T > 3000K

!

T < 3000K

Page 9: Lecture 4: Matter-Radiation Decoupling and the Cosmic ...star-kdh1/ce/ce04.pdf · Lecture 4: Matter-Radiation Decoupling and the Cosmic Microwave Background • Annihilation ... coupling

Photons, now free of matter, fly freely in all directions. Their temperature decreases as the Universe expands.

Today we see these photons from all directions with T = 3000 K / expansion factor = 2.7 K. expansion factor = ( 1 + z ) = ( 3000 / 2.7 ) = 1100.

Redshift of Last Scattering

Page 10: Lecture 4: Matter-Radiation Decoupling and the Cosmic ...star-kdh1/ce/ce04.pdf · Lecture 4: Matter-Radiation Decoupling and the Cosmic Microwave Background • Annihilation ... coupling

!

"T

T~ 10

#5

1948. Gamow predicts T ~ 5 K. 1965. Penzias & Wilson discover the CMB. T ~ 2.7 K. 1995. COBE measures perfect blackbody spectrum. T = 2.728 K 2004. WMAP resolves the ripples.

!

"# ~ 1o

COBE :

WMAP :

All-sky maps

Page 11: Lecture 4: Matter-Radiation Decoupling and the Cosmic ...star-kdh1/ce/ce04.pdf · Lecture 4: Matter-Radiation Decoupling and the Cosmic Microwave Background • Annihilation ... coupling

!

"T

T~ 10

#5

T = 2.728 K

Dipole anisotropy

Our velocity:

Milky Way sources

+ anisotropies

!

V

c="#

#="T

T$10

%3

Almost isotropic

V ! 400 km/s

CMB

Page 12: Lecture 4: Matter-Radiation Decoupling and the Cosmic ...star-kdh1/ce/ce04.pdf · Lecture 4: Matter-Radiation Decoupling and the Cosmic Microwave Background • Annihilation ... coupling

!

"# ~ 1o

COBE 1994

WMAP 2004

CMB Anisotropies

!

"T

T~ 10

#5

Snapshot of Universe at z = 1100 Seeds of galaxy formation.

Page 13: Lecture 4: Matter-Radiation Decoupling and the Cosmic ...star-kdh1/ce/ce04.pdf · Lecture 4: Matter-Radiation Decoupling and the Cosmic Microwave Background • Annihilation ... coupling

Power Spectrum of CMB anisotropies

Peak at 1o scale => Flat geometry,

Ωtot=1

Temperature ripple ΔT vs angular scale θ = 180o / l

“Acoustic Peaks” arise from sound waves in the plasma era. Sound speed is c/√3. Peak when the duration of plasma era matches a multiple of half a sound wave oscillation period.

Page 14: Lecture 4: Matter-Radiation Decoupling and the Cosmic ...star-kdh1/ce/ce04.pdf · Lecture 4: Matter-Radiation Decoupling and the Cosmic Microwave Background • Annihilation ... coupling

Recap of key physics

Matter: !M = "Mc

2!R

"3

Radiation: !R = "Rc

2=! T 4

!R"4

Observations: TCMB

= 2.7 K # !R$10"31 kg m"3

!M$10"28 kg m"3

#photons

baryons=N!

Nb

~ 109

Mean energy of blackbody photons: h! = 3kT

For <1 photon in the blackbody tail per baryon:

N! (h! > E) $ N! exp "E kT( ) < Nb

# k T <E

ln N! Nb( )=

E

ln 109( )$E

20

Sets p/n ratio, hence H/He ratio and T=3000K at recombination.

Page 15: Lecture 4: Matter-Radiation Decoupling and the Cosmic ...star-kdh1/ce/ce04.pdf · Lecture 4: Matter-Radiation Decoupling and the Cosmic Microwave Background • Annihilation ... coupling

Key stages in the history of our Universe: ~ 1 TeV matter-antimatter annihilation quark soup ~ 1 GeV baryogenesis (quark confinement) neutron proton soup ~ 0.8 MeV neutron – proton freeze-out

neutrons decay ~ 0.1 MeV nucleosynthesis H+He+e Thomson scattering plasma ~ 1 eV Recombination / decoupling neutral atoms + CMB photons ~ 10-3 eV Today Recollapse or Eternal expansion ? R

adiation era M

atter era Galaxy Formation