Summary
The simultaneous diagonalization of the residues of the signaturized and unsignaturized propagators is performed. This is done by means of an orthogonal decomposition of the space of the nonspurious states lying on arbitrary daughter trajectories.
Riassunto
Si effettua la diagnonalizzazione simultanea dei residui dei propagatori con segnatura e senza segnatura. Ciò si esegue mediante una decomposizione ortogonale dello spazio degli stati non spuri giacenti su traiettorie figlie arbitrarie.
Резюме
Осуществяется совместная диагонализация вычетов сигнатуризованных и несигнатуризованных пропагаторов. Диагонализация проводится с помощью ортогонального разложения пространства неложных состояний, лежащих на произвольных дочерних траекториях.
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References
J. M. Combes andJ. Soffer:Nuovo Cimento,2A, 279 (1971).
S. Fubini andG. Veneziano:Nuovo Cimento,64A, 811 (1969);K. Bardakçi andS. Mandelstam:Phys. Rev.,184, 1640 (1969).
M. Ida, H. Matsumoto andS. Yazaki:Progr. Theor. Phys.,44, 456 (1970).
J. L. Hopkinson andChan Hong-Mo:Nucl. Phys.,14B, 28 (1969).
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Traduzione a cura della Redasione.
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Ida, M., Soffer, J. General level structure in the dual-resonance model. Nuov Cim A 3, 355–364 (1971). https://doi.org/10.1007/BF02813696
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DOI: https://doi.org/10.1007/BF02813696