Titlebook: Extreme States of Matter in Strong Interaction Physics; An Introduction Helmut Satz Book 2018Latest edition Springer International Publishi

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Centralization and Decentralization,rature and high baryon density, where deconfinement and chiral symmetry restoration need not coincide. Following this, we survey results obtained on the basis of the Nambu-Jona-Lasinio model, and we conclude with a discussion of the present status of finite density lattice QCD.

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Inside the World of Older Spouse Carersthe medium. Subsequently, we note that in a temperature range up to several .., the plasma exhibits strong, non-perturbative interaction effects, which can be described in terms of an ideal gas of massive quasi-particles.

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https://doi.org/10.1007/978-3-642-22857-5versal hadronization temperature found in .... annihilation as well as in hadron-hadron and nucleus-nucleus collisions. In the final part we address deviations from a universal statistical hadronization description.

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https://doi.org/10.1007/978-3-658-28472-5gh energy collisions as the QCD counterpart of Hawking-Unruh radiation, encountered in black holes and for accelerated observers. This is shown to provide a common, “non-kinetic” origin for thermal multihadron production.

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Statistical QCD, of chromodynamics, we develop statistical QCD at finite temperature in the lattice formulation and discuss how it can be evaluated by computer simulation. We then use this method to study the thermodynamics of strongly interacting matter at vanishing baryon number density.

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Broken Symmetries,reaking of a global ZN symmetry. Next we turn to the chiral symmetry of the QCD Lagrangian in case of massless quarks and discuss the spontaneous breaking and eventual restoration of this symmetry. We then consider the relation of the two kinds of symmetry breaking in determining the transition beha

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