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

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garrulous

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Baryon Transport Dynamics: From , — , to , — , Collisionsata is significantly under-predicted by models which use diquark-quark (. ? .) hadronic strings for their primary baryon number transport mechanism [6,7] and has thus generated much interest. We therefore study new baryon number transport mechanisms in order to differentiate non-equilibrium multi-pa

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dainty

Dynamics of the Chiral Phase Transitionr, at the unprecedented energy densities now within reach at RHIC, two fundamental phase changes are expected to occur. One is the dissolution of ordinary hadrons into a deconfined quark-gluon plasma phase, which has long been a principal research objective. The other, with which the present discuss

瑪瑙

Filamentation Instability in Ultrarelativistic Heavy-Ion Collisions the system can be unstable with respect to the plasma oscillations driven by the QCD forces. A specific mode, which splits the parton system into the color current filaments parallel to the beam direction, is discussed in detail.

Frisky

Chaos as a Signature of Quark-Hadron Phase Transitionnd is useful for the characterization of the fluctuations of the final states of any hadronic and nuclear collisions. Applying that measure to the Ising model in 2D, it is found that the entropy index exhibits a sharp peak at the critical temperature. The use of the entropy index as a signature of q

Blasphemy

Instinctive

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.

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