Polarization of Lambda^0 hyperons as a signature for the Quark-Gluon Plasma
| dc.creator | Berdnikov, A. Ya. | |
| dc.creator | Berdnikov, Ya. A. | |
| dc.creator | Ivanov, A. N. | |
| dc.creator | Ivanova, V. A. | |
| dc.creator | Kosmach, V. F. | |
| dc.creator | Samsonov, V. M. | |
| dc.creator | Troitskaya, N. I. | |
| dc.creator | Vento, V. Thatar | |
| dc.date | 2003-12-14 | |
| dc.date.accessioned | 2026-07-07T11:44:19Z | |
| dc.date.available | 2026-07-07T11:44:19Z | |
| dc.description | The momentum distribution of Lambda^0 hyperons produced from the quark-gluon plasma (QGP) in ultra-relativistic heavy-ion collisions is calculated in dependence on their polarization. The momentum distribution of Lambda^0 hyperons is defined by matrix elements of relativistic quark Wigner operators, which are calculated within the Effective quark model with chiral U(3)xU(3) symmetry and the Quark-Gluon transport theory. We show that the polarization of the Lambda^0 hyperon depends of the spin of the strange quark that agrees well with the DeGrand-Miettinen model. We show that Lambda^0 hyperons, produced from the QGP, are fully unpolarized. This means that a detection of unpolarized Lambda^0 hyperons, produced in ultra-relativistic heavy-ion collisions, should serve as one of the signatures for the existence of the QGP in intermediate states of ultra-relativistic heavy-ion collisions. | |
| dc.description | 17 pages, no figure, latex | |
| dc.identifier | https://arxiv.org/abs/nucl-th/0312045 | |
| dc.identifier | http://arxiv.org/abs/nucl-th/0312045 | |
| dc.identifier | ActaPhys.Hung.A22:139-147,2005 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/201561 | |
| dc.subject | Nuclear Theory | |
| dc.title | Polarization of Lambda^0 hyperons as a signature for the Quark-Gluon Plasma | |
| dc.type | text |