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Hadronic Electrons? (1975)


Structure of the Electron

By analogy with hadrons, the core of the electron is taken as a collection of 'bitons' bound by a superstrong interaction mediated by neutral massive vector gluons with photon quantum numbers. These will not be restricted to the core, but will tend to form a cloud around it. From a comparison of the expected gradients of strong and weak Regge trajectories, we expect a characteristic weak interaction structure size of order (Greenberg and Yodh 1974). The radius of the electron will be governed primarily by the range of the gluon interaction, so that we will have , that is, .

The most sensitive tests of possible electron structure made to date are measurements on and reactions. Data for elastic scattering set a lower limit of about (Beron et al. 1974; Richter 1974) on the cutoff parameter in the electron form factor

corresponding to an upper bound of about for the electron radius. The contribution of internal structure to is roughly proportional to , so that we expect

if the electron core has similar interactions to those of the nucleon. Hence an extended electron with a radius is consistent with the data.

At low energies, photons couple to the electron via its gluon cloud (Fig. 1a), and appears pointlike because of the high gluon mass and the large superstrong interaction coupling constant. Similarly, photons couple to the nucleon via its vector meson cloud, but here the departure of the form factors from unity is quicker, because of the low mass and the comparative weakness of the strong interaction.


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[ Figure 1 ] Photon-lepton coupling (a) and hadron-lepton coupling (b) via intermediate gluons.

Since gluons interact superstrongly, they should not be immune to the strong interaction (hadrons undergo weak interactions), so that they couple to hadronic states with photon quantum numbers (Fig. 1b). As any gluon-hadron vertex will be strong, it must obey strong interaction selection rules, and thus we should assign more quantum numbers to the gluon. We take and , although and would also have been a possible choice. Hence gluons couple to the one-particle states and , and interactions such as and are forbidden.

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