Titlebook: Nuclear Matter in Different Phases and Transitions; Proceedings of the W Jean-Paul Blaizot,Xavier Campi,Marek Ploszajczak Conference procee

Arthr-

Bose-Einstein Condensation in Trapped Atomic Gases trapped atomic gas, at JILA (Boulder, Colorado) [1], closely followed by a group at MIT [2]. This observation has been now reproduced by more than 10 groups in the world, including the “cold atoms” group at the ENS.

COW

Biguanides

Dynamics of the Chiral Phase Transitionion concerned, is the approximate restoration of chiral symmetry. This topic has gained increasing interest in recent years, especially because of the possibility of forming ., the agitation of coherent oscillations of the pion field as a result of the rapid non-equilibrium dynamics. Reviews are given in refs. [1, 2, 3].

闡釋

Apogee

0168-1222 phase transitions may occur. Thus, for moderate excitation energies, of the order of a few MeV per nucleon, nuclear matter behaves as an ordinary fluid with gaseous and liquid phases, and a coexistence region below a critical temperature. For higher excitation energies, of the order of a few Ge V p

Ringworm

Hadron Multiplicities in High Energy e+e?, pp and pp? Collisions with a Statistical-Thermal Modelf quarks and gluons in a high energy collisions has indeed the characteristics of a pure statistical one, namely a given local set of partons can reach any multi-hadronic state with equal probability, provided that all involved conservation laws are fulfilled.

幻影

minaret

Hadronic Transport Model with A Phase Transitionid increase in the number of degrees of freedom. We show that a softening of the equation of state such as associated with the transition to quark-gluon plasma should be observable in the elliptic-flow excitation function from heavy-ion reactions.

天氣

motor-unit

Probing Thermalizing Nuclear Matter with Hard Photons escape from the nuclear medium without strong interaction, as do electromagnetic particles, and its formation time must decouple from the typical collision time, or, in other words, the probe must be created quasi-instantaneously in a frozen source.