Spin-dependent interaction in the deconfined phase of QCD
| dc.creator | Simonov, Yu. A. | |
| dc.date | 2005-12-19 | |
| dc.date.accessioned | 2026-07-07T06:54:17Z | |
| dc.date.available | 2026-07-07T06:54:17Z | |
| dc.description | Spin-dependent deconfined interaction in the Q\barQ system is derived from the field correlators known from lattice and analytic calculations. As a result hyperfine splitting is found numerically for charmonium, bottomonium and strangeonium in the range T_c<T<2T_c. Spin-orbit interaction due to magnetic correlators (the Thomas term) is able to produce numerous Q\barQ bound states with accumulation point at M=m_Q+m_\barQ. Possible influence of these effects on the thermodynamics of quark-gluon plasma is discussed. | |
| dc.description | 11 pages,in honor of Adriano Di Giacomo on his 70th birthday, to be published in the Festschrift | |
| dc.identifier | https://arxiv.org/abs/hep-ph/0512242 | |
| dc.identifier | http://arxiv.org/abs/hep-ph/0512242 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/105883 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.subject | High Energy Physics - Lattice | |
| dc.subject | Nuclear Theory | |
| dc.title | Spin-dependent interaction in the deconfined phase of QCD | |
| dc.type | text |