Nucleus-Nucleus Collisions: Proceedings of the Conference by A. Ventura, G.C. Bonsignori, M. Bruno

By A. Ventura, G.C. Bonsignori, M. Bruno

The convention "Bologna 2000: constitution of the Nucleus on the sunrise of the Century" was once dedicated to a self-discipline which has obvious a powerful revival of analysis actions within the final decade. New experimental effects and theoretical advancements in nuclear physics will surely make vital contributions to our wisdom and knowing of nature's basic development blocks. The curiosity aroused through the convention one of the medical group was once sincerely mirrored within the huge variety of members. those represented crucial nuclear physics laboratories on the earth. The convention lined 5 significant issues of contemporary nuclear physics: nuclear constitution, nucleus-nucleus collisions, hadron dynamics, nuclear astrophysics, and transdisciplinary and peaceable functions of nuclear technological know-how. It reviewed fresh development within the box and supplied a discussion board for the dialogue of present and destiny examine tasks.

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1965 -» Nuclear antimatter is (experimentally) discovered [29]. See also [26]. 1968 -» The discovery [27] at SLAC of Scaling (free quarks inside a nucleon at very high q 2 ) but in violent (pp) collisions no free quarks at the ISR are experimentally found [28]. Theorists consider Scaling as being evidence for RQFT not to be able to describe the Physics of Strong Interactions. The only exception is G. 't Hooft who discovers in 1971 that the p-function has negative sign for non-Abelian theories [30].

M- m the mass of the fundamental antifermion " s". a md | s the QCD-Bag energy needed to confine the pair "d s ". mj^ s the QCD-Bag energy needed to confine the pair "ds". mRad m rat ji a tiye corrections. Formula (4) makes sense if quarks are non-relativistic. If the interaction responsible for the intrinsic mass of a quark is CPT invariant, if the QCD confining effects and the radiative effects are all CPT invariant, the result is expected to be (mKo - mRo) = ArnKR = z ero If there are CPT breaking effects on the fundamental fermion masses and no effects on QCD confining forces and on radiative effects, then, from (4) we see that the only quantities left for CPT breaking are the "intrinsic" quark masses.

For antimatter to exist, the antifundamental fermions, as well as the antiparticles and the antinuclei, are needed. The masses associated with these components of matter are the "intrinsic" (quarks and leptons), the "confinement" (mesons and baryons) and the "binding" [either nuclear (nuclei), or electromagnetic (atoms)]. The first two are positive, the two "binding" ones are negative. These masses have different origins. No one has been able to establish the origin of the "intrinsic" masses (it could be the Higgs mechanism, but this lacks experimental confirmation so far).

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