Abstract
Starting from a phenomenologically successful, numerical solution of the Dyson-Schwinger equation that governs the quark propagator, we reconstruct in detail the interaction kernel that has to enter the instantaneous approximation to the Bethe-Salpeter equation to allow us to describe the lightest pseudoscalar mesons as quark-antiquark bound states exhibiting the (almost) masslessness necessary for them to be interpretable as the (pseudo) Goldstone bosons related to the spontaneous chiral symmetry breaking of quantum chromodynamics.
| Original language | English |
|---|---|
| Article number | 096005 |
| Number of pages | 8 |
| Journal | Physical Review D |
| Volume | 93 |
| Issue number | 9 |
| DOIs | |
| Publication status | Published - 5 May 2016 |
Austrian Fields of Science 2012
- 103024 Quantum field theory
Keywords
- BOUND-STATES
- EQUATION