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Original Title
Utiliser facilement la methode graphique
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Oct 1973; 10 p
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AbstractAbstract
[en] A review of the different approaches of the recoil and finite range effects in heavy-ion transfer reactions is given. One nucleon and two nucleon transfer reactions have been considered. It is shown how phase approaches are related to each other and what results they have yielded
[fr]
On passe en revue les differents traitements proposes pour les effets de portee finie et de recul dans les transferts d'ions lourds. Le transfert d'un ou deux nucleons a ete considere et il a ete montre comment les methodes proposees etaient reliees entre elles et les resultats qu'elles avaient donnesPrimary Subject
Source
Lyon-1 Univ., 69 - Villeurbanne (France). Inst. de Physique Nucleaire; p. 1-37 (pt.C8); nd; 3. Biennial session of nuclear physics; La Toussuire, France; 10 Feb 1975
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[en] We use the rishon structure of the ordinary mesons and the experimentally well established decay modes of these particles to obtain their graphical structure. A remarkable regularity is found and allows a prediction on the decay modes of the eta(c) and eta'(c) charmonium
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May 1980; 13 p
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[en] The quarks is defined as a flavour vector state in the C colour space and the antiquark as a vector in the C* dual space. The observables become scalar in the colour-space built even with a vector and a covector (meson) or with a vector and a pseudo-vector (baryon). The pseudo-vector is responsible of the Pauli principle existence and allows a comprehension of the distinction between baryons and mesons. The investigation of the strong interaction as the exchange of gluons leads to a crossing rule in contradiction with the JOZI rule in the general case. The existence and allowed decay of different sort of baryium is then considered
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Oct 1979; 34 p
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[en] The Graphical Spin Algebra has been shown to be applicable in a cartesian coordinate system without major modification. Then the (G.S.A.) allows a new and very easy approach of the usual vector analysis. Some examples of application are given
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Oct 1979; 19 p
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[en] The Graphical Spin algebra has been shown to be applicable in a cartesian coordinate system without major modification. Then the (G.S.A.) allows a new and very easy approach of the usual vector analysis. Some examples of application are given
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Jun 1978; 26 p
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AbstractAbstract
[en] Starting from the schematic models of Harari and Shupe we propose a geometrical approach of the leptons. The model is extended to consideration of the force mediating bosons
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Mar 1980; 9 p
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Uschersohn, J.; Elbaz, E.
Lyon-1 Univ., 69 - Villeurbanne (France). Inst. de Physique Nucleaire1983
Lyon-1 Univ., 69 - Villeurbanne (France). Inst. de Physique Nucleaire1983
AbstractAbstract
[en] In the rishon model the leptons and the quarks can be classified in either doublets or quadruplets of a SU(2) group. Gauge invariance leads to different charged current interactions in the doublet and the quadruplet cases. Demanding that the neutral currents be the same in the two cases, one obtains relations between the different charged current couplings to leptons and quark; moreover, if these transform as linear combinations of doublets and quadruplets, one can estimate the mass of the gauge boson responsible for baryon decay to be not larger than 105GeV. A SU(2)sub(L) x U(1) model is treated in detail
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1983; 11 p
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Kibler, M.; Elbaz, E.
Lyon-1 Univ., 69 - Villeurbanne (France). Inst. de Physique Nucleaire1978
Lyon-1 Univ., 69 - Villeurbanne (France). Inst. de Physique Nucleaire1978
AbstractAbstract
[en] Some basic relations for the representation theory and the Wigner-Racah algebra of a finite or compact continuous group are discussed and transcribed in terms of diagrams. Special emphasis is placed on the case of a simply reducible group and all the diagrams are applicable to SU2 without any change
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Jun 1978; 41 p
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[en] We propose a concrete representation of leptons and quarks in different generations in the geometrical approach to the rishon model where rishons behave as the fundamental representations of the SU(3)sub(C) x SU(3)sub(H) group. The model allows a unified description of both hadronic and leptonic decays of elementary particles
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Dec 1981; 17 p
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