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
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.
3
Q
How is non-covariant quantization of the electromagnetic field done?
A
- Introduce a infinitely large volume L^3
- Impose periodic boundary conditions for vector potential A
- Impose expressions for a and a* in terms of new coordinates p and q.
- Impose canonical commutation relations on q and p (these are equivalent to those of a and a-dagger)
4
Q
Is the number operator definite positive?
A
Yes
5
Q
What are the eigenvalues of the number operators?
A
Positive integers and zero
6
Q
For what purpose is Ferm’s golden rule used?
A
To calculate the probability for a transition