Normalisation constant expansion of spinor field

Join the discussion
Ask a follow-up here, or get your own question answered by working scientists, mathematicians and engineers — people, not an autocomplete.
Real named experts · corrections over time · the nuance an AI answer skips
2 replies · 2K views
Josh1079
Messages
45
Reaction score
0
Hi, I'm reading about the wave packet solution to the dirac equation but in the book I'm reading it states that [tex]\int \frac {d^3p} {(2\pi)^3 2E} [a u e^{-ipx} + b^\dagger \bar{v} e^{ipx}[/tex]

The normalisation constant confuses me. I guess the 2pi^3 is reasonalbe. However, the 1/2E seems a bit weird to me. I thought it should always be something of the order of (-1/2) of E. Did I misunderstand something about the normalisation?

Thanks!
 
Physics news on Phys.org
Josh1079 said:
Hi, I'm reading about the wave packet solution to the dirac equation but in the book I'm reading it states that [tex]\int \frac {d^3p} {(2\pi)^3 2E} [a u e^{-ipx} + b^\dagger \bar{v} e^{ipx}[/tex]

The normalisation constant confuses me. I guess the 2pi^3 is reasonalbe. However, the 1/2E seems a bit weird to me. I thought it should always be something of the order of (-1/2) of E. Did I misunderstand something about the normalisation?

Thanks!

This might be the reason:

  • Start with a 4-D Fourier transform: [itex]\int d^4 p A(p_\mu) u e^{- i p_\mu x^\mu}[/itex]
  • Realize that the only values of [itex]p_\mu[/itex] that can contribute satisfy: [itex](p_0)^2 - \vec{p}^2 - m^2 = 0[/itex] (ignoring factors of [itex]c[/itex] and [itex]\hbar[/itex])
  • This implies that [itex]A(p_\mu)[/itex] has the form [itex]a(\vec{p}) \delta((p_0)^2 - \vec{p}^2 - m^2)[/itex]
  • Just a fact about the delta-function: [itex]\int dx Q(x) \delta(f(x)) = \frac{Q(x_0)}{f'(x_0)}[/itex] where [itex]x_0[/itex] is a zero of [itex]f(x)[/itex] and [itex]f'(x)[/itex] means the derivative of [itex]f[/itex] with respect to [itex]x[/itex]. (If [itex]f(x)[/itex] has multiple zeros, then there is a term like that for each zero)
  • So if we let [itex]E[/itex] be the value of [itex]p_0[/itex] satisfying [itex](p_0)^2 - \vec{p}^2 - m^2 = 0[/itex], then integrating over [itex]dp_0[/itex] gives: [itex]\frac{1}{\frac{d}{dp_0}( (p_0)^2 - \vec{p}^2 - m^2)} = \frac{1}{2 p_0} = \frac{1}{2E}[/itex]
 
  • Like
Likes   Reactions: dextercioby
Hi stevendaryl, thanks for the reply! I think I roughly understand what your writing and it seems reasonable. There is just one more question that I'm a bit curious about. So are you trying to say that the reason why there is a factor 1/2E in the expression is because it's doing a 4D Fourier transform? Does this mean that the expressions with 1/√(2E) is doing a 3D Fourier transform? I'm also a bit curious about the difference.

Thanks!