- #1
Nicolasrll
- 2
- 0
Hi everyone! Something has been bothering me lately. Consider the quark propagator:
[tex] \langle 0|\psi_a(x)\psi_a(0) |0\rangle[/tex]
For a given color a. Now let's say we insert [tex] 1 = \sum |n \rangle \langle n| [/tex] between the two quark fields, where the sum is over a complete set of energy eigenstates. We then have a sum over a bunch of terms of the form [tex]\langle n|\psi_a(0)|0\rangle[/tex]
Here then is what I'm worried about: confinement, as I understand it, tells us that all energy eigenstates must be color singlets. But unless I'm mistaken, [tex]\psi_a(0)|0\rangle[/tex] is not at all a color singlet, and therefore I would expect all the terms of the form shown above to be zero. This, obviously, clashes hideously with the quark propagator used in perturbative QCD. So what am I missing?
Thank you for your insight!
[tex] \langle 0|\psi_a(x)\psi_a(0) |0\rangle[/tex]
For a given color a. Now let's say we insert [tex] 1 = \sum |n \rangle \langle n| [/tex] between the two quark fields, where the sum is over a complete set of energy eigenstates. We then have a sum over a bunch of terms of the form [tex]\langle n|\psi_a(0)|0\rangle[/tex]
Here then is what I'm worried about: confinement, as I understand it, tells us that all energy eigenstates must be color singlets. But unless I'm mistaken, [tex]\psi_a(0)|0\rangle[/tex] is not at all a color singlet, and therefore I would expect all the terms of the form shown above to be zero. This, obviously, clashes hideously with the quark propagator used in perturbative QCD. So what am I missing?
Thank you for your insight!