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Lecture 35 The early Universe II: Astrophysics joins particle physics

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Nobel prizes 1979 (theory) and 1984 (experiment) April 13, 2001 ... force and strong nuclear force join to form the GUT (grand unified theories) ... – PowerPoint PPT presentation

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Title: Lecture 35 The early Universe II: Astrophysics joins particle physics


1
Lecture 35The early Universe II Astrophysics
joins particle physics
2
General acceptance of the big bang model
  • Until mid 60ies big bang model very
    controversial, many alternative models
  • After mid 60ies little doubt on validity of the
    big bang model
  • Four pillars on which the big bang theory is
    resting
  • Hubbles law ?
  • Cosmic microwave background radiation ?
  • The origin of the elements
  • Structure formation in the universe

3
Can we see the sound of the universe ?
  • Compressed gas heats up? temperature
    fluctuations

4
The Music of the Universe
5
Measuring the Curvature of the Universe Using the
CMB
6
Abundance of elements
  • Hydrogen and helium most abundant
  • gap around Li, Be, B

7
The structure of matter
8
Nomenclature
or
  • Z number of protons
  • A number of nucleons (protons and neutrons)
  • N number of neutrons (A-Z)
  • X name of the element

9
Transforming hydrogen into helium
  • Hot big bang neutrons and protons
  • Use a multi step procedure
  • p n ? 2H
  • p 2H ? 3He
  • n 2H ? 3H
  • 3He 3He ? 4He 2 p
  • some side reactions
  • 3He 3H ? 7Li
  • 3He 3He ? 7Be

10
Mass gap/stability gap at A5 and 8
  • Reaction chain
  • 4He 4He ? 8B
  • 8B 4He ? 12C
  • so-called 3-body reaction
  • in order to have 3-body reactions, high particle
    densities are required
  • densities are not high enough in the big-bang
  • but they are in the center of evolved stars
  • Conclusion big bang synthesizes elements up to
    7Li. Higher elements are formed in stars

11
Primordial nucleosynthesis
  • Result
  • abundance of H,He and Li is consistent
  • but ?b 0.04

12
Can we understand why 25 He?
  • Before the universe cooled sufficiently to allow
    nucleons to assemble into helium, the neutron to
    proton ratio was 17
  • 4He equal number of protons and neutrons
  • Assume that all neutrons grab a proton to form a
    4He. The left over protons form hydrogen.

13
Can we understand why 25 He?
  • Abundance of hydrogen
  • Abundance of hydrogen
  • Abundance of helium 1-0.75 0.25
  • but why is nn/np 1/7 ?

14
The four forces of nature
  • Gravity
  • weak, long ranged
  • electromagnetism
  • intermediate, long ranged
  • strong nuclear force
  • strong, short ranged
  • weak nuclear force
  • weak, short ranged

15
The weak nuclear force
  • Free neutrons decay into protons
  • Free neutrons decay into protons
  • n neutron
  • p proton
  • e- electron
  • ? neutrino
  • half life time 10 min

n ? p
n ? p e-
? n ? p e-
16
What happened when the universe was even younger?
  • Recall special relativity Emc2
  • If the thermal energy exceeds twice the rest mass
    energy of a particle, particle-antiparticle
    pairs can be created ? Pair creation
  • Matter protons, neutrons, electrons neutrinos
  • Antimatter antiprotons, antineutrons, positrons,
    antineutrino

17
Pair creation
  • Antiparticle same mass as particle, but opposite
    charge.
  • Antimatter has positive mass !!!!!!
  • The inverse process is called annihilation

18
Examples
  • Tgt1010 K creation/annihilation of
    electron-positron pairs
  • Tgt1013 K creation/annihilation of
    proton-antiproton pairs

19
A common theme ...
  • For each reaction there is a temperature Tc
  • For temperature larger than Tc, there is a
    continuous transformation between photons into
    particle-antiparticle pairs and vice versa
  • This state is called thermal equilibrium
  • If the temperature drops below the threshold
    temperature Tc, pair creation freezes out,
    remaining pairs annihilate.

20
The History of the Universe
21
Matter era
  • The energy of matter is nowadays 10000 times
    higher than that of radiation
  • but temperature rises like (1z)
  • 2.7K lt T lt 10000K matter era
  • dominate particles (in order of decreasing
    contribution
  • baryons, photons, neutrinos
  • dominant forces
  • gravity

22
Radiation era
  • As the temperature exceeds 10000K, radiation
    starts dominating
  • 10000K lt T lt 1010K radiation era
  • dominate particles (in order of decreasing
    contribution
  • photons, neutrinos, baryons
  • dominant forces
  • electromagnetism, gravity

23
Electron-positron annihilation
  • As the temperature exceeds 1010K, creation of
    electron-positron pairs
  • T gt 1010K equilibrium between electron-positron
    pair creation and annihilation
  • T lt 1010K freeze-out. Remaining pairs annihilate

24
Lepton era
  • 1010K lt T lt 1012K
  • dominate particles (in order of decreasing
    contribution
  • electrons, positrons, photons, neutrinos,
    antineutrinos, baryons
  • dominant forces
  • electromagnetism, weak nuclear, gravity

25
Hadron annihilation
  • As the temperature exceeds 1012K, creation of
    hadron-antihadron pairs (e.g. proton-antiproton)
  • T gt 1012K equilibrium between hadron pair
    creation and annihilation
  • T lt 1012K freeze-out. Remaining pairs annihilate

26
Hadron era
  • 1012K lt T lt 1013K
  • dominate particles (in order of decreasing
    contribution
  • baryonsantiparticles, mesonsantiparticles,
    electrons, positrons, photons, neutrinos,
    antineutrinos
  • dominant forces
  • electromagnetism, strong nuclear, weak nuclear,
    gravity

27
Still quark era
  • 1013K lt T lt 1015K
  • hadrons (baryons, mesons) break into quarks
  • dominate particles (in order of decreasing
    contribution
  • quarks, antiquarks, electrons, positrons,
    photons, neutrinos, antineutrinos
  • dominant forces
  • electromagnetism, strong nuclear, weak nuclear,
    gravity

28
Electroweak phase transition
  • As the temperature exceeds 1015K,
    electromagnetism and weak nuclear force join to
    form the electroweak force
  • T gt 1015K electroweak force
  • T lt 1015K electromagnetism, weak nuclear force
  • Limit of what we can test in particle
    accelerators.
  • Nobel prizes 1979 (theory) and 1984 (experiment)

29
Quark era
  • 1015K lt T lt 1029K
  • dominate particles (in order of decreasing
    contribution
  • quarks, antiquarks, electrons, positrons,
    photons, neutrinos, antineutrinos
  • dominant forces
  • electroweak, strong nuclear, gravity

30
GUT phase transition
  • As the temperature exceeds 1029K, electroweak
    force and strong nuclear force join to form the
    GUT (grand unified theories)
  • T gt 1029K GUT
  • T lt 1029K electroweak force, strong nuclear
    force
  • relatively solid theoretical framework (but may
    be wrong), but pretty much no constraint by
    experiments

31
GUT era
  • 1029K lt T lt 1032K
  • dominate particles (in order of decreasing
    contribution
  • Zillions of particles, most of them not detected
    yet
  • dominant forces
  • GUT, gravity

32
Planck epoch
  • T gt 1032K unification of GUT and gravity
  • Particles
  • ???
  • Forces
  • TOE (theory of everything)
  • The last frontier ...
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