Confinement and Light-Front QCD
| dc.creator | Burkardt, Matthias | |
| dc.date | 1996-08-23 | |
| dc.date.accessioned | 2026-07-07T03:59:50Z | |
| dc.date.available | 2026-07-07T03:59:50Z | |
| dc.description | Numerical results for the (rest-frame) $Q\bar{Q}$ potential in light-front quantized $QCD_{2+1}$ on a $\perp$ lattice are presented. Both in the longitudinal as well as the $\perp$ spatial directions one obtains linear confinement. The confinement mechanism in light-front QCD depends on the orientation of the external charges: for longitudinally (with respect to the boost direction in the infinite momentum frame) separated quarks, confinement arises from the instantaneous interaction piece in the Hamiltonian while for $\perp$ separated quarks, the confinement mechanism is similar to the one in Hamiltonian lattice QCD. Nevertheless, already a very simple ansatz for the effective link-field potential yields an almost rotationally symmetric $Q\bar{Q}$ potential. The momentum carried by the glue strongly depends on the orientation ("polarization") of the $Q\bar{Q}$ pair. | |
| dc.description | Talk given at $3^{rd}$ AUP workshop on "Confinement, Chaos and Collision", Paris, France, June 96. Uses lprocl.sty | |
| dc.identifier | https://arxiv.org/abs/hep-ph/9608428 | |
| dc.identifier | http://arxiv.org/abs/hep-ph/9608428 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/46392 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | Confinement and Light-Front QCD | |
| dc.type | text |