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Physical Review. D, Particles Fields; v. 7(7); p. 2265-2266
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[en] This paper reviews some of the very exciting work on resonances in the past year following the discovery of the J/psi. A number of important few-body aspects are pointed out. Work presented on generalized isobar models used to do resonance analysis are pointed out. The important question of whether the A1 is a true resonance is the focal point of this discussion. Relevant new experiments and dynamical calculations lend support to the existence of the A1. Papers concerning the ΔΔ content of the deuteron are also summarized. This seems to be a difficult question to answer quantitatively. The many new developments in high energy spectroscopy starting with the remarkable simultaneous discovery of the very narrow meson resonance at 3.1 GeV at Brookhaven (the J) and at SLAC, (the psi (3,1)) are reviewed. Most of the phenomena can be explained by the assumption of a new heavy c quark (possibly the charmed quark predicted by Glashow). Some problems in which few body systems play an important role are singled out. (Auth.)
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Mitra, A.N.; Slaus, I.; Bhasin, V.S.; Gupta, V.K. (eds.); p. 659-666; ISBN 0720404819; ; 1976; North-Holland; Amsterdam, The Netherlands; 7. international conference on few body problems in nuclear and particle physics; Delhi, India; 29 Dec 1975
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Shaw, G.L.
International Centre for Theoretical Physics, Trieste (Italy)1972
International Centre for Theoretical Physics, Trieste (Italy)1972
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1972; 5 p
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AbstractAbstract
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Anon; p. 417-426; 1973; Purdue Univ; West Lafayette, IN; Conference on Baryon resonances; West Lafayette, Indiana, USA; 20 Apr 1973
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Physical Review. D, Particles Fields; v. 8(1); p. 353-355
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[en] The glow model of broken QCD allows for free, low-mass, fractionally charged, glow-singlet, color 6, diquarks Q. Although these composite Q's may be difficult to produce at present e+e- and hadronic energies, the situation could be much more favorable in heavy-ion collisions. In contrast to other models, the glow model allows for parameters which could lead to the production of fractional charge at Bevalac energies. A two stage experiment is in progress: The first step consisted of an (initial) exposure of a heavy target configuration to a total of 3 x 1010 Fe ions of 1.9 GeV/nucleon kinetic energy. Fractional charge which escaped the target was stopped in five gallon tanks of CCl4 and collected (and thus concentrated) on thin central wires. The target materials and collection wires were distributed to a number of laboratories conducting experiments designed to look for free fractional charge in bulk matter. The first results from the SFSU automated Millikan droplet experiment found less than one fractional charge produced per 104 Fe-Pb collisions (and with further assumptions, less than one for 2 x 106 collisions). 14 references
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Lawrence Berkeley Lab., CA (USA); p. 567-573; Dec 1983; p. 567-573; 6. high energy heavy ion study and 2. workshop on anomalons; Berkeley, CA (USA); 28 Jun - 1 Jul 1983; Available from NTIS, PC A99/MF A01 as TI84005862
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Original Title
Differential cross sections
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Physical Review. D, Particles Fields; v. 8(1); p. 232-240
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BARYONS, BASIC INTERACTIONS, BEAMS, BOSONS, CROSS SECTIONS, ELEMENTARY PARTICLES, ENERGY RANGE, FERMIONS, HADRONS, INTERACTIONS, MESONS, MEV RANGE, NUCLEONS, PARTICLE INTERACTIONS, PARTICLE PRODUCTION, PHOTON-BARYON INTERACTIONS, PHOTON-HADRON INTERACTIONS, PHOTON-NUCLEON INTERACTIONS, PIONS, PSEUDOSCALAR MESONS
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Physical Review. D, Particles Fields; v. 7(9); p. 2789-2790
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Physical Review Letters; v. 28(17); p. 1143-1144
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[en] The tests and constraints of composite models for fermions are reviewed. Possible indications for composite fermions are listed: families, excitations, actual constituents, moments and transitions, complicated-effective forces, form factors, high spin, and 't Hooft's conditions. A relativistic calculation of a pointlike composite fermion is reviewed. The SO14 unified composite model is examined in light of the enormous difficulty seen in obtaining a full dynamic calculation for a composite electron as constrained by equation 4. The limits of F2 for quarks from e+e- annihilation are also investigated
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Anon; p. 349-364; 1983; p. 349-364; Plenum Press; New York, NY (USA)
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Book
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