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General properties of the dual resonance model

โœ Scribed by E Del Giudice; P Di Vecchia; S Fubini


Publisher
Elsevier Science
Year
1972
Tongue
English
Weight
980 KB
Volume
70
Category
Article
ISSN
0003-4916

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โœฆ Synopsis


In this paper we give a general procedure for the construction of the physical states in the case of intercept a(0) = 1. This procedure exhibits in an explicit form the "bootstrap" requirement that the spectrum of the intermediate states, obtained by the factorization of the scattering amplitude, is independent from the particular process used for constructing it. A big advantage of this way is that one avoids the unnecessary introduction of spurious states. The physical states are constructed together with their corresponding operators; this makes it then possible to get scattering amplitudes with the physical states on the external legs.

Using the vertex operator associated with the photon-like particle of the level 01(s) = 1, we can construct an infinite number of orthogonal and positive norm states, growing up exponentially as the partition function of n objects with only two Lorentz components.

The zero mass of the "photon" has been also used to construct operators which transform a physical state belonging to a certain multiplet LX(S) = n into another physical state contained in the same multiplet. These operators should be intimately related to the degeneracy of the multiplets. An interesting by-product of this approach is the universality of the "electric charge" and the "magnetic moment." * This work supported in part through funds provided by the Atomic Energy Commission under contract AT(30-l)-2098.


๐Ÿ“œ SIMILAR VOLUMES


Algebraic treatment of subsidiary condit
โœ S Fubini; G Veneziano ๐Ÿ“‚ Article ๐Ÿ“… 1971 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 714 KB

## WE BOTH REMEMBER AMOS DE-SHALIT A8 A WONDERFUL FRIEND AND TEACHER The Ward-like identities previously proposed in order to eliminate unphysical states (ghosts) from dual amplitudes and generalized by Virasoro, are investigated within the context of the projective operator language. We are able