Lecture 4 - Non covariant quantization of EM field Flashcards

1
Q

What is the gauge condition for the Coulomb gauge

A

nabla cdot A(r,t) = 0

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2
Q

For each time t the vector potential A(x,t) is a sum over two variables, what?

A

Sum over k and r, making up the modes.

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3
Q

How is non-covariant quantization of the electromagnetic field done?

A
  1. Introduce a infinitely large volume L^3
  2. Impose periodic boundary conditions for vector potential A
  3. Impose expressions for a and a* in terms of new coordinates p and q.
  4. Impose canonical commutation relations on q and p (these are equivalent to those of a and a-dagger)
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4
Q

Is the number operator definite positive?

A

Yes

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5
Q

What are the eigenvalues of the number operators?

A

Positive integers and zero

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6
Q

For what purpose is Ferm’s golden rule used?

A

To calculate the probability for a transition

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