Lecture 10: Cosmology & Particle Physics Flashcards

1
Q

We’re looking at high energies and temperatures things which are relevant on

A

the sub-atomic scale

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2
Q

Electromagnetism, the weak, the strong and gravity are distinct today but the strength of each

A

scales differently with increasing energies

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3
Q

Increase the energies enough and the forces will

A

unify

this means they become of comparable strength

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4
Q

electroweak theory (EW)

A

the EM and weak forces unify at around 300GeV or 10^15K

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5
Q

Quantum chromodynamics (QCD)

A

a description of strong nuclear interactions

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6
Q

standard model

A

includes both EW and QCD

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7
Q

grand unified theory (GUT)

A

would require 10^15 GeV but current particle accelerators are not powerful enough to test this

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8
Q

Theory of everything (TOE)

A

a theory of quantum gravity would require 10^19 GeV but we would also need testable predictions to validate it

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9
Q

The basic difficulty in cosmology is to do with

A

mass

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10
Q

In order to explain cosmological observations (i.e.: the universe appearing flat) we need

A

more mass than we currently observe

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11
Q

the only classes of elementary particle known experimentally

A
  1. matter fermions
  2. bosons
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12
Q

matter fermions

A

leptons and quarks
both of which are spin 1/2 particles

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13
Q

bosons

A

including gauge bosons, which are spin 1 particles and are the force carriers in the standard model

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14
Q

elementary particles

A

something effectively point-like with no size or structure

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15
Q

EM radiation is quantised and can be polarised so the photon has

A

two polarisation or spin states

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16
Q

effective number of degrees of freedom for particles

A

geff = nspin x nanti x npauli

17
Q

nspin

A

either spin up or spin down for photons

18
Q

nanti

A

tells you if the particle has an anti particle

if yes set it to two
else set it to one

19
Q

npauli

A

tells you if the particle obeys the Pauli exclusion principle, integrate over the Fermi-Dirac distribution to get it if true.

20
Q

spin essentially refers to the

A

quanta of angular momentum

21
Q

for photons, nanti=

A

1
light is its own anti-particle

22
Q

for electrons, nanti=

A

2 (electron has the positron)

23
Q

photons are bosons so have npauli=

24
Q

fermions have npauli=

25
Q

s=1/2 and ms=+/- 1/2 for

A

electrons and fermions

26
Q

s=0,1 for

27
Q
  • It turned out that the reason we were not detecting enough neutrinos was
A

that we were essentially digging in the wrong place

28
Q

we did not see neutrinos until the discovery that

A

neutrinos oscillated between type with a small mass difference of 10^-2eV

29
Q

If neutrinos were highly relativistic at decoupling they would be

A

hot dark matter

30
Q

Massive neutrinos would therefore not clump together on small scales (galaxies) and structure
would

A

become washed out

does not match observations of the clustering of galaxies

31
Q

we believe that non-baryonic matter is

A

cold and does not consist of neutrinos

32
Q

Sakharov Conditions for Baryogenesis

A

baryon number violation

cp violation

departure from thermal equilibrium

33
Q

baryon number violation

A

requires the proton to decay

34
Q

cp violation

A

requires reaction rates for particles and anti particles to be different

35
Q

departure from thermal equilibrium

A

departure from thermal equilibrium permits reactions
to proceed preferentially in one direction.

36
Q

There has been some limited evidence of both baryon number and CP violation at the LHCb
experiment

A

but observations of baryon density in the universe cannot currently be explained: we need a new theory.