The Quark-Gluon Plasma: a Perfect Thermostat and a Perfect Particle Reservoir
| dc.creator | Moretto, L. G. | |
| dc.creator | Bugaev, K. A. | |
| dc.creator | Elliott, J. B. | |
| dc.creator | Phair, L. | |
| dc.date | 2005-11-15 | |
| dc.date.accessioned | 2026-07-07T06:50:01Z | |
| dc.date.available | 2026-07-07T06:50:01Z | |
| dc.description | A system H with a Hagedorn-like mass spectrum imparts its unique temperature T_H to any other system coupled to it. An H system radiates particles in preexisting physical and chemical equilibrium. These particles form a saturated vapor at temperature T_H. This coexistence describes a first order phase transition. An H system is nearly indifferent to fragmentation into smaller H systems. A lower mass cut-off in the spectrum does not significantly alter the general picture. These properties of the Hagedorn thermostats naturally explain a single value of hadronization temperature observed in elementary particle collisions at high energies and lead to some experimental predictions. | |
| dc.description | Contribution to the ``World Consensus Initiative III, Texas A & M University, College Station, Texas, USA, February 11-17, 2005, 15p | |
| dc.identifier | https://arxiv.org/abs/hep-ph/0511180 | |
| dc.identifier | http://arxiv.org/abs/hep-ph/0511180 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/104564 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | The Quark-Gluon Plasma: a Perfect Thermostat and a Perfect Particle Reservoir | |
| dc.type | text |