2. FDs II and QED Flashcards

1
Q

What do FDs mathematically represent?

A

The matrix element for a process going from an initial to a final state

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2
Q

What is scalar QED?

A

Electrodynamics of spin-0 particles

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3
Q

How do we define the particles in scalar QED?

A

Φ^(-) for the particle
Φ^(+) for the antiparticle
Φ is the spin 0 field

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4
Q

What are the steps for dealing with the FD in scalar QED to calculate the matrix element M?

A
  1. Label verticies
  2. Slice diagram into fragments
  3. For each fragment, move against arrows along fermion lines and apply the Feyman rules
  4. Multiply the maths parts together and simplify
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5
Q

What is the Mandelstan variable S for a scattering process 1 + 2 -> 3 + 4

A

S = (P1 + P2)^2 = (P3 + P4)^2 = COM Energy^2

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6
Q

What is the Mandelstan variable t for a scattering process 1 + 2 -> 3 + 4

A

t = (P1 - P3)^2 = (P2 - P4)^2

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7
Q

What is the Mandelstan variable U for a scattering process 1 + 2 -> 3 + 4

A

U = (P1 - P4)^2 = (P2 - P3)^2

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8
Q

Which type of diagram is the S channel diagram related to?

A

The propagator of the of a creation diagram

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9
Q

Which type of diagram is the t channel diagram related to?

A

The standard scattering diagram

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10
Q

Which type of diagram is the U channel diagram related to?

A

The crossed diagram

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11
Q

What is the coupling factor for the EM force?

A

α_EM = 1/137

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12
Q

Can pair production happen in a vacuum?

A

No - Cant conserve E, p, m

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13
Q

Is the QED coupling factor constant?

A

No - it changes on the 4 momentum of the photon at the vertex

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14
Q

What is a consequence of the QED coupling factor not being a constant?

A

The electron charge is no longer constant

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15
Q

What is the QED coupling factor a function of for very small distances?

A

α_EM(-Q^2)

where -Q^2 = q^2 = 4 momentum of the photon

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16
Q

What happens to the structure of the target as we increase -Q^2

A

More detail should be visible if the target has structure

17
Q

What happens when you put a charge in a dielectric?

A

You polarise it locally

- Get polarised dipoles in effect which form a negatively charged “screen” around the positive charge

18
Q

How does the measured charge on a electron change with distance?

A

Exponential type decay from q_vac to q_vac / k and tails off at q_vac / k for large r

19
Q

How is an electron considered classically in a vacuum?

A

As a point source

20
Q

How is an electron considered by QFT in a vacuum?

A

Complicated

  • Electron dresses itself in a foam of virtual photons, electrons and positron pairs
  • In each loop, the virtual positron is attracted to the parent electron forming a positively charged screen
21
Q

Wrt electron foam, how does increasing -Q^2 change the measurement of the electric charge?

A

Increase the resolution of the structure and focus in on the region around the electron
- But it is still an effective charge

22
Q

Can the true charge of an electron be measured?

A

No - can’t throw foam away

- Always measure an effective charge

23
Q

What is -1.602 x10^-19 C equal to?

A

The effective charge of the electron + the foam at the distance scaled by the -Q^2 of the probe

24
Q

What value of the charge does the SM predict when -Q^2 -> infinity (wavelength -> 0)

A

Predicts it goes to infinity

25
Q

Which regimes does the SM break down?

A

For very high energy and very small distances