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Titlebook: Hadronic Matter at Extreme Energy Density; Nicola Cabibbo,Luigi Sertorio Book 1980 Springer Science+Business Media New York 1980 elementar

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樓主: Daguerreotype
61#
發(fā)表于 2025-4-1 04:47:53 | 只看該作者
978-1-4684-3604-4Springer Science+Business Media New York 1980
62#
發(fā)表于 2025-4-1 09:29:35 | 只看該作者
Lawrence Freedman,Jeffrey Michaelsistance behaviour of this theory has been successfully extracted with the renormalized perturbation techniques and even partly tested with experiment. However the long distance structure of the theory poses a number of yet unsolved questions, owing to the non-perturbative nature of the problem.
63#
發(fā)表于 2025-4-1 12:34:11 | 只看該作者
64#
發(fā)表于 2025-4-1 16:09:50 | 只看該作者
Conclusion and Future Directions,oduction in soft hadronic collisions using the quark recombination model. Finally particle production in hard collisions, in particular large transverse momentum processes and the occurence of gluon jets in deep inelastic processes is discussed within the framework of QCD perturbation theory.
65#
發(fā)表于 2025-4-1 20:46:39 | 只看該作者
https://doi.org/10.1007/978-3-031-23054-7 we obtain an equation of state which yields a quark phase at small and a hadron phase at large values of the resonance coupling constant. Separating these regimes, there is a transition region with a behaviour of the Van der Waals type, providing a negative specific heat and, at the critical point, infinite temperature fluctuations.
66#
發(fā)表于 2025-4-1 23:32:26 | 只看該作者
Duality Transformation and Confinement in Gauge Theoriesistance behaviour of this theory has been successfully extracted with the renormalized perturbation techniques and even partly tested with experiment. However the long distance structure of the theory poses a number of yet unsolved questions, owing to the non-perturbative nature of the problem.
67#
發(fā)表于 2025-4-2 05:36:10 | 只看該作者
Thermodynamics of Nuclear Matter from the Statistical Bootstrap Modelball grows with its mass. We find that the such described nuclear matter can exist in two phases. In particular we consider in a numerical example the high temperature (T ? T. ≈ 150 MeV) regime of the gaseous phase with a density of less than ~ 0.75 of normal nuclear density.
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